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$: INTERNATIONAL BULLETIN ON ATOMIC AND MOLECULAR … · The International Bulletin on Atomic and Molecular Data for Fusion (\the Bulletin") is prepared by the Atomic and Molecular (A+M)$
INTERNATIONAL BULLETINON

ATOMIC AND MOLECULARDATA

FOR FUSION

Number 70

November 2016

Contributors:

M. Imai, A. Kramida, D.-H. Kwon, A. Lasa Esquisabel,

H. Lee, W.-W. Lee, K.-M. Lim, I. Murakami,

M.-Y. Song and U. von Toussaint

Editor:

H. K. Chung

Atomic and Molecular Data Unit

Nuclear Data Section, NAPC Division

IAEA

Editorial Board:

B. J. Braams, International Atomic Energy Agency

D.-H. Kwon, Korea Atomic Energy Research Institute, Republic of Korea

I. Murakami, National Institute for Fusion Science, Japan

Yu. Ralchenko, National Institute for Standards and Technology, USA

J. S. Yoon, National Fusion Research Institute, Republic of Korea

INTERNATIONAL ATOMIC ENERGY AGENCYVIENNA, 2016

Copies of the Bulletin may be obtained from

Nuclear Data SectionInternational Atomic Energy Agency

Vienna International CentreP.O. Box 100

A-1400 Vienna, Austria

INTERNATIONAL BULLETINON ATOMIC AND MOLECULAR DATA FOR FUSION

IAEA, VIENNA, 2016

IBAMD/70ISSN 0258-8048

Printed by the IAEA in AustriaNovember 2016

FOREWORD

The International Bulletin on Atomic and Molecular Data for Fusion (“the Bulletin”) isprepared by the Atomic and Molecular (A+M) Data Unit of the International Atomic EnergyAgency (IAEA) and published and distributed free of charge by the IAEA to assist in the developmentof fusion research and technology. Each issue of the Bulletin contains additions to AMBDAS since theprevious issue.

The Bulletin and AMBDAS provide an indexed guide to papers that contain data for atomic structure,spectral lines and intensities (or transition probabilities), atomic and molecular collisions andparticle–surface interactions.

The references and indices included in the Bulletin have been provided by atomic data centres of DataCentre network (DCN), collaborators and IAEA interns:

• National Institute of Standards and Technology (NIST), Gaithersburg, USA;

• Korea Atomic Energy Research Institute, Daejeon, Republic of Korea;

• National Fusion Research Institute, Gunsan, Republic of Korea;

• National Institute of Fusion Science, Toki, Japan;

• Max Planck Institute of Plasma Physics, Garching, Germany;

• University of Helsinki, Helsinki, Finland.

The present edition of the Bulletin contains data mainly on atomic structure, spectra and transitionprobabilities published in the years 2013–2014, electron collisions and surface interaction that appearedin the years 2009–2014. Data for heavy particle and photon collisions will be considered for the nextBulletin.

Information in this Bulletin is presented in four chapters. The Atomic and Molecular Data InformationSystem (AMDIS) of the International Atomic Energy Agency is briefly presented in Chapter 1.

The indexed papers are listed separately for structure and spectra, atomic and molecular collisions, andsurface interactions in Chapter 2. The structure and spectra index lines are grouped by process. Thefirst column gives the reactants, the second one the process and then the character of the datacontained (Th for theoretical, Ex for experimental, and E/T for both experimental and theoretical).The number in the last column is the reference number in Chapter 3 of the Bulletin.

The atomic and molecular index lines are grouped by one collision partner (photon, electron or heavyparticle). The first column gives the reactants, the second column gives the process, the third columngives the energy range with the appropriate units, and the last two columns are the same as in thestructure and spectra index lines. The particle–surface interactions index lines are grouped by process.The first column gives the reactants, the second the energy range with the appropriate units, and thelast two columns are the same as in the structure and spectra index lines.

Chapter 3 contains the bibliographic data for both the indexed and non-indexed references. Under eachentry in Chapter 3 index lines (if any) refer back to the classified entries in Chapter 2.

Chapter 4 contains the Author Index with references to bibliographic entries contained in Chapter 3.

iii

Contributions are solicited on data generation work in progress and on new data in the course ofpublication. Contributions should include an explanation of their applicability to fusion research andshould be sent to:

Atomic and Molecular Data UnitNuclear Data Section, NAPC DivisionInternational Atomic Energy AgencyVienna International CentreP.O. Box 100A-1400 Vienna, Austria

e-mail: [email protected]: https://www-amdis.iaea.org/

All data published in the Bulletin are included in AMBDAS, the IAEA Atomic and Molecular Data Unitbibliographic database. AMBDAS is freely available on-line at

https://www-amdis.iaea.org/AMBDAS/

DISCLAIMER

This Bulletin has not been edited by the editorial staff of the IAEA. The views expressed remain theresponsibility of the contributors and do not necessarily represent the views of the IAEA or its MemberStates. The use of particular designations of countries or territories does not imply any judgement bythe publisher, the IAEA, as to the legal status of such countries or territories, of their authorities andinstitutions or of the delimitation of their boundaries

v

NEWS ON THE ATOMIC AND MOLECULAR DATA UNIT

Coordinated Reasearch Projects (CRP) are the main tool by which the Atomic and Molecular DataUnit collects and evaluates data for the establishment of recommended numerical databases for use infusion energy research. A CRP is a three to five-year joint project involving approximately 7 to 12laboratories, research teams or institutes performing coordinated research to achieve a well defined goal(establishment of a particular database, data generation, compilation and assessment for specific typesof atomic and molecular (A+M) collision processes, particle surface interaction (PSI) or classes of suchprocesses, etc.).

In the years of 2013–2016, two CRPs have concluded and two CRPs have started. The final reportsof completed CRPs on Light Element Atom, Molecule and Radical Behaviour in the Divertor and EdgePlasma Regions and on Spectroscopic and Collisional Data for Tungsten from 1 eV to 20 keV are publishedin Journal of Physics: Conference Series, Vol 576 (2015) and Atoms, Vol 3 (2015). The CRP on Atomicand Molecular Data for State-Resolved Modelling of Hydrogen and Helium and Their Isotopes in FusionPlasma held its second RCM in July 2013 and the final RCM in March 2016. The CRP on Data forErosion and Tritium Retention in Beryllium Plasma-Facing Materials held the second RCM in August2014. The new CRP on Plasma-Wall Interaction with Irradiated Tungsten and Tungsten Alloys in FusionDevices held the first and second RCMs in November 2013 and September 2015 and the new CRP onPlasma-wall Interaction with Reduced-activation Steel Surfaces in Fusion Devices held the first RCM onDecember 2015. More information about the CRPs is available on the A+M Data Unit web site.

https://www-amdis.iaea.org/CRP/

The 22nd and 23rd meetings of the Data Centre Network on Technical Aspects of Atomic and MolecularData Processing and Exchange were held on 4–6 September 2013 and 2–4 November 2015. Currently theData Centre Network (DCN) includes about 10 national data centres for collection, critical assessment(evaluation) and partly for generation of A+M, PSI and bulk material properties data for fusion andother applications. More information on the DCN activities is available on the A+M Data Unit web site.

https://www-amdis.iaea.org/DCN/

Upon recommendations of the Data Centre Network, the A+M Data Unit organized a series of meetingsto address the needs of critical assessment of atomic, molecular and particle-surface interaction data. The3rd TM of the Code Centre Network (CCN) on General Guidelines for Uncertainty Assessments was heldin May 2013 in order to discuss the uncertainty quantification (UQ) of theoretical A+M data. The CMon Evaluation of Data for Collisions of Electrons with Nitrogen Molecule and Nitrogen Molecular Ionwasheld in December 2013 in cooperation with the eMOL project to provide evaluated data for electron-molecule collisions. Following the recommendation from the 3rd TM of CCN, a TM on UncertaintyAssessment for Theoretical Atomic Molecular Scattering Data was held in Cambridge, MA, USA at theHarvard-Smithsonian Center for Astrophysics in collaboration with the Institute of Theoretical Atomic,Molecular and Optical Physics (ITAMP), where more than 20 participants discussed the UQ issues oftheoretical A+M data. In 2015, three CMs were held on the data evaluation topics: CM on Guidelines forUncertainty Quantification of Theoretical Atomic and Molecular Datain June 2015, CM on Evaluation& Uncertainty Assessment for Be, C, Nein July 2015 and a joint IAEA-KAERI CM on RecommendedData for Processes of Tungsten, September 2015. More information on the data evaluation activities isavailable on the A+M Data Unit web site.

https://www-amdis.iaea.org/DCN/Evaluation/

The A+M Data Unit organized two joint ICTP-IAEA workshops: Joint ICTP-IAEA Conference onModels and Data for Plasma-Material Interaction in Fusion Devices, Trieste, Italy, 03-07 November 2014and Joint ICTP-IAEA Advanced School and Workshop on Modern Methods in Plasma Spectroscopy,Trieste, Italy, 16-27 March 2015. Additional information may be found on the A+M Data Unit web site.

vii

https://www-amdis.iaea.org/Workshops/ICTP2012/

The A+M Data Unit cooperated to host the second and third Spectral Line Shapes in Plasmas (SLSP)Code Comparison Workshop on 5-9 August 2013 and 2-6 March 2015.

The A+M Data Unit now provides access to two widely used atomic physics codes, the Flexible AtomicCode and GRASP2K codes.

https://www-amdis.iaea.org/FAC and https://www-amdis.iaea.org/GRASP2K

CONTENTS

FOREWORD iii

DISCLAIMER v

NEWS ON THE ATOMIC AND MOLECULAR DATA UNIT vii

1 The Atomic and Molecular Data Information System . . . . . . . . . . . . . . . . . . 1

2 Process Index . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 32.1 Structure and Spectra . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 32.2 Atomic and Molecular Collisions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23

2.2.1 Electron Collisions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 232.2.2 Heavy Particles Collisions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 66

2.3 Surface Interactions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 672.4 Data Collection, Bibliographic and Progress Report . . . . . . . . . . . . . . . . . . . . . 962.5 Interactions of Atomic Particles with Fields . . . . . . . . . . . . . . . . . . . . . . . . . . 98

3 Bibliography . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 993.1 Structure and Spectra . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 993.2 Atomic and Molecular Collisions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 164

3.2.1 Electron Collisions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1643.2.2 Heavy Particles Collisions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 287

3.3 Surface Interactions . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 2903.4 Data Collection, Bibliographic and Progress Report . . . . . . . . . . . . . . . . . . . . . 3463.5 Interactions of Atomic Particles with Fields . . . . . . . . . . . . . . . . . . . . . . . . . . 348

Author Index . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 349

Chapter 1

The Atomic and Molecular DataInformation System

AMDIS is the Atomic and Molecular Data Information System of the International Atomic EnergyAgency, established and maintained by the Atomic and Molecular Data Unit, Nuclear Data Section.AMDIS contains two main databases: AMBDAS, a bibliographic database for atomic and moleculardata for fusion research and ALADDIN, a numerical database of recommended and evaluated atomic,molecular and plasma-surface interaction data.

AMBDAS, Atomic and Molecular Bibliographic Data System, is an on-line bibliographic databasehttps://www-amdis.iaea.org/AMBDAS that contains more than 47,000 bibliographic entries withatomic, molecular and plasma-surface interaction data of interest to fusion research, and dating back to1918. Entries may be retrieved by author, process, reactants, type of reference, year of publication anddata source (theoretical or experimental). The interface is a web-based application, easy to use with norequired registration. AMBDAS data are regularly published in the International Bulletin on Atomicand Molecular Data for Fusion.

ALADDIN is the online numerical database of the Atomic and Molecular Data Unit of the IAEAhttps://www-amdis.iaea.org/ALADDIN, providing atomic, molecular and plasma-materialinteraction data of interest to fusion research. ALADDIN provides two similar interfaces, one forcollisional data and one for particle surface interactions. An ALADDIN entry consists of searchablelabels that characterize the process and reactants; the source of the data, date, laboratory or datacentre, and reference; comment lines and the numerical data. When possible all requested data aredisplayed in the same units to permit easy comparison. A unit conversion tool is available and allresults can be displayed in tabular and graphical mode.

In addition to AMBDAS and ALADDIN databases, AMDIS distributes atomic physics codes and codegenerated data, provides an access to online codes and database search engine and hosts meeting pagesand presentations which contain most recent datasets.

1

2

Chapter 2

Process Index

2.1 Structure and Spectra

H-Cu0+ 28+ Th 66H-Rn Th 132H + Si4+ Th 219H + Si5+ Th 219H + Si6+ Th 219H + Si7+ Th 219H + Si8+ Th 219H + Si9+ Th 219H + Si10+ Th 219H + Si11+ Th 219H + Si12+ Th 219H + Si4+ Th 219H + Si5+ Th 219H + Si6+ Th 219H + Si7+ Th 219H + Si8+ Th 219H + Si9+ Th 219H + Si10+ Th 219H + Si11+ Th 219H + Si12+ Th 219H− + W47+ Th 221H− + W48+ Th 221H− + W49+ Th 221H− + W50+ Th 221H− + W51+ Th 221H− + W52+ Th 221H− + W53+ Th 221H− + W54+ Th 221H− + W55+ Th 221H− + W56+ Th 221H− + W57+ Th 221H− + W58+ Th 221H− + W59+ Th 221H− + W60+ Th 221H− + W61+ Th 221H− + W47+ Th 221H− + W48+ Th 221H− + W49+ Th 221H− + W50+ Th 221H− + W51+ Th 221H− + W52+ Th 221H− + W53+ Th 221H− + W54+ Th 221H− + W55+ Th 221H− + W56+ Th 221H− + W57+ Th 221H− + W58+ Th 221H− + W59+ Th 221H− + W60+ Th 221H− + W61+ Th 221

3

H Th 269H− Th 269He Th 7He-Fe Th 78He0+ + Exp 144He0+ + Exp 145He Th 315He Th 340He Th 466Li Th 7Li+ Th 7Li0+ + Exp 17Li E/T 24Li E/T 26Li Th 32Li Th 34Li E/T 51Li Th 62Li Th 79Li Th 88Li E/T 89Li Exp 95Li Th 96Li Exp 123Li Th 192Li Th 200Li Th 210Li+ Th 233Li Th 234Li Th 269Li− Th 269Li Th 315Li Exp 322Li Th 340Li Th 349Li0+ + Th 350Li+ Th 352Li− Th 374Li0+ + Th 389Li+ Th 389Li Th 390Li Th 391Li Th 435Li Th 466Be Th 6Be0+ 2+ Th 7Be+ Th 79Be+ Th 97Be Th 122Be+ Th 163Be Th 183Be+ Th 191Be Th 200Be Th 239Be Th 264Be+ Th 287Be Exp 293Be+ Th 316Be+ Th 340

4

Be2+ Th 352Be+ Th 359Be Th 374Be E/T 382Be Th 390Be+ Th 484B0+ 3+ Th 7B Th 57B− Th 81B E/T 261B+ Exp 337B Th 390B Th 422B+ Th 479C0+ 4+ Th 7C+ Th 43C+ Th 57C+ 3+ Exp 144C+ 3+ Exp 145C+ Th 165C3+ Th 186C4+ Th 209C4+ Th 282C3+ Th 287C5+ Exp 320C+ 2+ Exp 321C4+ 5+ Exp 363C2+ Th 374C5+ Th 455C2+ Th 486N0+ 5+ Th 7N E/T 51N3+ 4+ E/T 108N0+ + Exp 142N+ 3+ Exp 144N0+ 2+ Exp 145N4+ Th 186N4+ Exp 235N4+ Exp 297N Th 307N− Th 307N+ 2+ Exp 321N2+ Exp 344N5+ 6+ Exp 387N+ Th 440N Th 452O0+ 6+ Th 7O Exp 9O Th 53O3+ E/T 102O0+ 3+ Exp 144O0+ 4+ Exp 145O5+ Th 186O3+ Th 194O6+ Th 209O3+ 4+ Exp 235O3+ 6+ Exp 235O3+ 7+ Exp 248O4+ 6+ Exp 253

5

O5+ Th 287O+ 3+ Exp 321O7+ Exp 355O6+ 7+ Exp 387O6+ 7+ Exp 388O Th 390O Th 411O2+ Th 411O3+ Th 464O4+ 5+ Th 482F0+ 7+ Th 7F Th 67F Th 111F3+ Exp 145F4+ Exp 235F4+ 8+ Exp 235F6+ Th 238F4+ 7+ Exp 248F5+ 6+ Exp 253F Th 309F− Th 309F3+ Exp 386F Th 454Ne0+ 8+ Th 7Ne Th 37Ne5+ E/T 102Ne7+ Th 113Ne+ 4+ Exp 144Ne2+ 4+ Exp 145Ne5+ Th 194Ne8+ Th 209Ne3+ Exp 235Ne3+ 8+ Exp 235Ne5+ 8+ Exp 248Ne4+ 6+ Exp 253Ne0+ + Exp 254Ne7+ Th 287Ne Th 288Ne8+ Th 315Ne7+ Th 315Ne Exp 329Ne6+ Th 374Ne Exp 386Ne Th 390Ne Exp 413Ne3+ Th 431Ne6+ Th 486Ne Exp 488Na E/T 51Na3+ Exp 144Na Th 192Na E/T 247Na Th 269Na− Th 269Na Exp 322Na Th 340Na0+ + Th 350Mg Exp 12Mg7+ E/T 102

6

Mg0+ + Exp 144Mg Exp 145Mg Th 152Mg2+ Th 154Mg+ Th 163Mg Th 183Mg2+ Th 184Mg7+ Th 194Mg10+ Th 209Mg+ E/T 247Mg E/T 247Mg Th 288Mg2+ Th 291Mg Th 318Mg2+ Th 327Mg+ Th 340Mg9+ Exp 370Mg9+ 11+ Exp 370Mg Th 392Mg2+ Th 448Mg2+ Th 463Al11+ Th 99Al Exp 133Al11+ Th 193Al2+ E/T 247Al+ E/T 247Al4+ Th 265Al11+ 12+ Th 282Al9+ Th 285Al3+ Th 327Al3+ Th 463Si12+ E/T 33Si11+ E/T 41Si3+ Th 56Si11+ Th 59Si Exp 61Si9+ E/T 102Si+ Exp 144Si+ 2+ Exp 145Si11+ Th 175Si4+ Th 184Si9+ Th 194Si12+ Th 209Si6+ Th 237Si8+ Th 241Si+ E/T 247Si3+ E/T 247Si4+ 6+ Exp 253Si11+ Th 268Si11+ Th 287Si Th 31029Si− Th 310Si− Th 310Si9+ Th 358Si11+ Th 364Si13+ Exp 377Si6+ Th 400Si8+ Th 403Si9+ Th 481

7

P4+ Th 56P + Fe16+ Th 492S14+ E/T 33S5+ Th 56S12+ 14+ Exp 76S+ 2+ Exp 144S0+ 2+ Exp 145S6+ Th 184S Th 199S14+ Th 209S7+ Exp 235S9+ 11+ Exp 235S7+ 14+ Exp 235S7+ 11+ Exp 248S14+ 15+ Exp 292S14+ E/T 353S10+ 13+ Exp 387S12+ E/T 449S12+ E/T 480Cl15+ E/T 33Cl6+ Th 56Cl E/T 58Cl0+ + E/T 58Cl13+ Exp 76Cl14+ Exp 76Cl Th 112Cl− Th 112Cl2+ 3+ Exp 145Cl Th 169Cl7+ 15+ Th 267Cl13+ Th 300Cl3+ Th 384Cl7+ 15+ Th 424Cl13+ Th 446Cl3+ Th 490Ar14+ 16+ Exp 8Ar16+ E/T 39Ar2+ Exp 40Ar7+ Th 56Ar15+ Th 59Ar+ Exp 75Ar14+ 16+ Exp 76Ar Th 92Ar13+ Th 98Ar9+ Th 109Ar14+ 16+ E/T 114Ar Exp 117Ar16+ Exp 125Ar0+ + Exp 135Ar2+ 4+ Exp 143Ar2+ 4+ Exp 144Ar2+ 4+ Exp 145Ar15+ Th 175Ar8+ Th 184Ar8+ Th 197Ar14+ 16+ Th 201Ar16+ Th 201Ar5+ Th 212Ar8+ E/T 227

8

Ar11+ 12+ Exp 235Ar11+ 16+ Exp 235Ar10+ 13+ Exp 248Ar14+ 16+ Exp 281Ar16+ 17+ Th 282Ar15+ Th 287Ar Th 288Ar16+ 17+ Exp 292Ar16+ Exp 303Ar+ Th 306Ar Th 314Ar+ Th 324Ar14+ Th 328Ar16+ Exp 342Ar16+ Exp 360Ar13+ Th 366Ar16+ 17+ Exp 371Ar13+ Exp 372Ar14+ Th 374Ar5+ E/T 381Ar+ Exp 409Ar Exp 413Ar14+ Th 465Ar+ Exp 468K E/T 51K8+ Th 56K3+ 5+ Exp 143K3+ Exp 144K3+ 5+ Exp 145K Th 192K Th 269K− Th 269K15+ Th 300K Exp 322K Th 340K0+ + Th 350K15+ Th 446Ca Exp 12Ca9+ Th 56Ca17+ Th 59Ca4+ 6+ Exp 143Ca+ Exp 144Ca4+ 5+ Exp 144Ca4+ Exp 145Ca6+ Exp 145Ca Th 152Ca17+ Th 159Ca+ Th 163Ca17+ Th 175Ca Th 183Ca10+ Th 184Ca+ E/T 247Ca9+ 17+ Exp 253Ca12+ 13+ Exp 253Ca17+ Th 268Ca Th 288Ca Th 318Ca17+ Th 335Ca+ Th 340

9

Ca16+ 19+ Exp 342Ca17+ Th 470Sc10+ Th 56Sc+ Exp 144Sc15+ E/T 258Ti20+ Exp 38Ti11+ Th 56Ti19+ Th 59Ti9+ E/T 72Ti5+ Th 73Ti+ Th 86Ti Exp 110Ti2+ Th 140Ti2+ Th 141Ti+ Exp 144Ti Exp 158Ti19+ Th 175Ti9+ Th 178Ti5+ Th 179Ti12+ Th 184Ti13+ Th 245Ti+ E/T 247Ti+ Th 256Ti19+ Th 287Ti20+ Exp 303Ti18+ Th 323Ti19+ Exp 334Ti20+ Exp 334Ti19+ Th 335Ti20+ Exp 351Ti21+ Exp 351Ti+ Th 419Ti12+ E/T 434Ti18+ E/T 449Ti19+ Th 470Ti18+ E/T 480Ti+ Exp 483V+ Exp 18V+ Exp 19V E/T 51V12+ Th 56V11+ Th 74V Exp 110V3+ Th 140V3+ Th 141V+ 3+ Exp 144V+ Th 155V11+ Th 180V14+ Th 245V Exp 249V17+ E/T 258V E/T 415Cr Exp 15Cr0+ + Exp 129Cr+ Th 140Cr3+ 4+ Exp 143Cr+ 4+ Exp 144Cr14+ Th 184Cr15+ Th 245

10

Cr+ E/T 247Cr+ Exp 250Cr11+ Th 319Cr11+ Th 460Mn+ Exp 21Mn Exp 64Mn2+ 5+ Th 140Mn2+ Th 141Mn4+ Th 141Mn2+ 5+ Exp 143Mn+ Exp 144Mn3+ 4+ Exp 144Mn4+ 5+ Exp 145Mn+ E/T 157Mn0+ + Exp 217Mn16+ Th 245Mn+ E/T 247Mn11+ Th 276Mn E/T 332Mn11+ Th 432Mn Th 469Fe17+ 18+ Exp 10Fe10+ E/T 13Fe15+ Th 20Fe+ Exp 22Fe17+ 22+ E/T 35Fe17+ 24+ E/T 35Fe4+ Exp 36Fe10+ Th 42Fe21+ Th 46Fe23+ Th 59Fe4+ Th 60Fe24+ Th 84Fe Exp 106Fe16+ Th 109Fe+ Exp 115Fe16+ E/T 121Fe Exp 133Fe+ 5+ Th 140Fe2+ 5+ Th 141Fe+ 6+ Exp 143Fe+ 7+ Exp 144Fe2+ Exp 145Fe4+ 6+ Exp 145Fe Exp 150Fe10+ Th 153Fe15+ Th 156Fe23+ Th 159Fe10+ Th 164Fe21+ Th 168Fe23+ Th 175Fe16+ Th 184Fe24+ Th 187Fe16+ Th 197Fe+ E/T 205Fe14+ Th 208Fe16+ Exp 211Fe22+ Th 232Fe6+ 13+ Exp 235

11

Fe16+ 17+ Exp 235Fe6+ 17+ Exp 235Fe6+ Th 236Fe8+ E/T 243Fe17+ Th 245Fe E/T 247Fe+ E/T 247Fe6+ 16+ Exp 248Fe20+ Exp 248Fe4+ E/T 251Fe6+ 7+ Exp 253Fe19+ 20+ Exp 253Fe22+ Exp 253Fe10+ Th 280Fe23+ Th 287Fe24+ 25+ Exp 292Fe22+ Th 294Fe13+ E/T 295Fe14+ E/T 295Fe24+ Exp 351Fe25+ Exp 351Fe8+ 14+ Exp 357Fe7+ 13+ Exp 363Fe13+ 15+ E/T 369Fe23+ Exp 386Fe3+ 16+ Exp 388Fe22+ Th 398Fe6+ Th 399Fe7+ Th 401Fe8+ Th 405Fe+ Th 408Fe Exp 410Fe4+ Th 414Fe E/T 425Fe10+ Th 436Fe4+ Th 476Fe13+ E/T 477Fe22+ Th 486Co+ Exp 18Co25+ Th 84Co+ Th 140Co3+ Th 140Co4+ Th 140Co+ 2+ Exp 143Co5+ 6+ Exp 143Co+ Th 155Co18+ Th 245Ni16+ Th 31Ni4+ Exp 36Ni14+ Th 52Ni4+ Th 60Ni22+ Th 77Ni26+ Th 80Ni26+ Th 84Ni20+ Th 100Ni18+ E/T 121Ni3+ 5+ Th 140Ni3+ Th 141Ni4+ Th 141

12

Ni2+ 4+ Exp 143Ni6+ Exp 143Ni+ Exp 144Ni3+ Exp 144Ni14+ Th 172Ni18+ Th 184Ni26+ Th 185Ni10+ Exp 235Ni13+ 16+ Exp 235Ni10+ 17+ Exp 235Ni14+ E/T 240Ni10+ E/T 242Ni19+ Th 245Ni+ E/T 247Ni9+ 17+ Exp 248Ni9+ Exp 253Ni9+ 26+ Exp 253Ni14+ E/T 258Ni22+ E/T 258Ni20+ Th 283Ni+ Th 341Ni14+ Th 402Ni10+ Th 404Ni Exp 417Ni20+ Th 437Cu E/T 51Cu27+ Th 84Cu19+ E/T 121Cu Exp 128Cu Exp 133Cu3+ 5+ Th 140Cu+ Exp 143Cu3+ Exp 143Cu+ Exp 144Cu20+ Th 245Cu Th 252Cu Th 269Cu− Th 269Cu27+ Exp 351Cu28+ Exp 351Cu25+ 26+ Exp 386Cu Th 416Cu E/T 462Zn16+ Th 52Zn27+ Th 59Zn28+ Th 84Zn Exp 133Zn3+ 5+ Th 140Zn27+ Th 159Zn+ Th 163Zn16+ Th 172Zn27+ Th 175Zn20+ Th 184Zn9+ Th 245Zn+ E/T 247Zn27+ Th 287Ga26+ Th 46Ga E/T 51Ga17+ Th 52

13

Ga3+ 5+ Th 140Ga26+ Th 168Ga17+ Th 172Ga Th 373Ge18+ Th 52Ge29+ Th 59Ge4+ 5+ Th 140Ge18+ Th 172Ge29+ Th 175Ge18+ Th 276Ge28+ Th 300Ge30+ Exp 351Ge31+ Exp 351Ge30+ E/T 353Ge Th 373Ge18+ Th 432Ge28+ Th 446As19+ Th 52As5+ Th 140As19+ Th 172As Th 373Se2+ E/T 258Se Th 373Br E/T 51Br27+ E/T 258Br Th 373Kr+ E/T 3Kr+ Th 14Kr5+ Th 14Kr6+ Th 14Kr10+ Th 14Kr15+ Th 14Kr17+ Th 14Kr2+ Th 14Kr11+ Th 14Kr16+ Th 14Kr6+ Th 54Kr33+ Th 59Kr32+ Th 85Kr33+ Th 85Kr Exp 105Kr+ 3+ Th 107Kr26+ Th 109Kr34+ Th 119Kr31+ Th 126Kr6+ Th 173Kr33+ Th 175Kr26+ Th 197Kr26+ Th 203Kr34+ Th 207Kr6+ E/T 259Kr31+ E/T 277Kr31+ Th 278Kr33+ Th 287Kr Th 288Kr Th 314Kr20+ 21+ Exp 339Kr24+ Exp 339Kr26+ 33+ Exp 339

14

Kr34+ E/T 353Kr32+ Th 365Kr Th 373Kr Exp 413Kr17+ E/T 459Kr23+ Th 472Kr2+ Exp 485Rb E/T 51Rb34+ Th 59Rb34+ Th 175Rb23+ E/T 258Rb Th 269Rb− Th 269Rb Exp 322Rb Th 340Rb0+ + Th 350Sr35+ Th 59Sr+ Th 163Sr35+ Th 175Sr Th 183Sr24+ E/T 258Sr Th 288Sr3+ Th 298Sr Th 318Sr+ Th 340Sr3+ Th 444Y36+ Th 59Y36+ Th 175Y4+ Th 298Y4+ Th 444Zr37+ Th 59Zr+ Exp 144Zr37+ Th 175Zr-Sn2+ Th 246Zr Th 290Zr2+ Th 290Zr5+ Th 298Zr0+ + Exp 378Zr5+ Th 444Nb+ E/T 90Nb+ Th 91Nb12+ Th 104Nb12+ Th 195Nb Th 230Nb Exp 231Nb6+ Th 298Nb11+ Th 433Nb6+ Th 444Mo E/T 51Mo39+ Th 59Mo39+ Th 159Mo39+ Th 175Mo Exp 204Mo2+ Th 228Mo33+ Th 245Mo37+ E/T 277Mo35+ E/T 277Mo37+ Th 278Mo35+ Th 278

15

Mo39+ Th 287Mo7+ Th 298Mo32+ Exp 342Mo40+ Exp 379Mo41+ Exp 379Mo2+ Th 396Mo33+ Th 407Mo12+ Th 433Mo40+ Th 442Mo41+ Th 442Mo7+ Th 444Ru E/T 51Ru41+ Th 59Ru41+ Th 175Ag E/T 51Ag Exp 128Ag Th 269Ag− Th 269Ag E/T 462Cd E/T 51Cd45+ Th 59Cd+ Th 163Cd45+ Th 175In3+ E/T 25In E/T 28In+ E/T 29In2+ E/T 29In E/T 51In+ E/T 161In E/T 188In2+ Th 313In Exp 347In Exp 376In2+ Th 458In Th 474Sn E/T 51Sn47+ Th 59Sn+ Exp 139Sn47+ Th 159Sn47+ Th 175Sn Th 290Sn+ E/T 301Sn13+ Th 311Sn13+ 14+ Th 311Sn4+ 19+ Exp 355Sn+ E/T 447Sb E/T 51Te2+ E/T 258Te Th 290Te3+ E/T 301I+ Th 290Xe51+ Th 59Xe43+ E/T 83Xe44+ Th 109Xe Exp 116Xe49+ Th 126Xe51+ Th 175Xe44+ Th 197Xe Th 199

16

Xe49+ Th 214Xe51+ Th 287Xe Th 288Xe2+ Th 290Xe Th 314Xe Exp 317Xe7+ E/T 331Xe Th 345Xe52+ E/T 353Xe8+ 18+ Exp 355Xe Exp 413Xe Th 457Xe50+ Th 486Xe17+ 20+ Exp 487Xe22+ 24+ Exp 487Cs E/T 51Cs Th 269Cs− Th 269Cs Exp 322Cs Th 340Cs0+ + Th 350Ba E/T 51Ba45+ E/T 83Ba+ Th 163Ba Th 183Ba Th 318Ba+ Th 340La E/T 51La-Lu Th 314Nd E/T 51Nd57+ Th 287Sm51+ E/T 83Eu E/T 51Eu Exp 329Eu Exp 468Gd E/T 51Gd53+ E/T 83Gd59+ Th 126Gd59+ Th 214Gd33+ 35+ Exp 357Gd18+ 27+ Exp 367Gd30+ Exp 367Gd31+ Exp 367Gd32+ Exp 367Dy E/T 51Dy55+ E/T 83Er57+ E/T 83Er Th 290Er2+ Th 290Tm66+ Th 159Tm3+ Th 290Yb E/T 51Yb67+ Th 159Yb Th 183Yb67+ Th 287Yb23+ E/T 333Lu E/T 51Lu+ Th 290Hf44+ 54+ E/T 127

17

Hf44+ 55+ E/T 127Hf44+ Th 198Hf Th 290Hf12+ Th 290Ta E/T 16Ta45+ 56+ E/T 127Ta45+ 57+ E/T 127Ta+ Exp 255Ta6+ E/T 299Ta45+ 57+ Exp 361Ta6+ Th 445W42+ 51+ E/T 1W48+ 50+ E/T 1W62+ Th 27W36+ Th 45W24+ 30+ Th 49W39+ Th 55W47+ 61+ Exp 82W63+ E/T 83W27+ 37+ Th 103W0+ 3+ Th 130W0+ 73+ Th 131W42+ 51+ Th 146W62+ Th 160W36+ Th 167W39+ Th 174W13+ E/T 177W46+ Th 198W3+ Th 202W65+ 71+ Th 215W42+ 46+ Th 262W25+ Th 266W57+ Th 270W35+ E/T 271W39+ Th 272W67+ E/T 277W67+ Th 278W57+ Th 284W57+ Th 286W26+ E/T 289W14+ Th 290W14+ 45+ Exp 302W62+ 66+ Th 304W Exp 320W5+ Exp 321W43+ Th 325W44+ Th 330W28+ E/T 336W Exp 338W65+ Th 348W39+ Th 354W24+ 33+ Exp 356W26+ Exp 356W22+ 26+ Exp 357W42+ 45+ Exp 357W26+ Exp 362W27+ 29+ Exp 367W26+ Exp 368W28+ Exp 368

18

W7+ E/T 375W45+ Th 383W20+ 37+ Exp 385W25+ Th 423W57+ Th 426W35+ Th 427W39+ Th 428W57+ Th 438W57+ Th 439W26+ Th 441W62+ 66+ Th 451W43+ Th 461W44+ Th 467W28+ Th 471W65+ Th 475W39+ Th 478W45+ Th 489Re E/T 51Re+ Exp 196Re47+ Th 198Os48+ Th 198Os13+ Th 290Ir E/T 51Ir49+ Th 198Pt67+ E/T 83Pt50+ Th 198Pt20+ Th 290Au66+ 67+ Th 44Au E/T 51Au71+ 76+ Th 63Au41+ 53+ Th 120Au62+ 67+ Th 124Au74+ Th 126Au51+ 60+ E/T 127Au51+ 62+ E/T 127Au Exp 128Au0+ 78+ Th 131Au41+ 51+ Exp 134Au44+ 51+ Exp 136Au47+ 53+ Exp 137Au47+ 52+ Exp 138Au66+ 67+ Th 166Au18+ E/T 177Au51+ Th 198Au62+ 67+ Th 213Au74+ Th 214Au47+ 50+ Th 229Au67+ Th 260Au Th 269Au− Th 269Au45+ 52+ Th 273Au19+ 42+ E/T 343Au20+ 42+ E/T 343Au32+ 33+ E/T 343Au32+ 34+ E/T 343Au47+ 50+ Th 397Au67+ Th 421Au45+ 52+ Th 429Au77+ Th 442

19

Au78+ Th 442Hg E/T 51Hg+ Th 163Hg77+ Th 287Hg22+ Th 290Tl E/T 51Pb79+ Th 268Pb24+ Th 290Bi72+ E/T 83Bi78+ Th 126Bi78+ Th 214Bi80+ Th 287Bi80+ Th 364Bi82+ Th 364Po Th 290Po26+ Th 290Fr E/T 51Fr Th 269Fr− Th 269Fr84+ Th 287Fr0+ + Th 350Ra30+ Th 290Ra Th 318Ac-NO Th 314Th0+ + Exp 135Th0+ 2+ Exp 254Th87+ Th 287Th Th 290Th32+ Th 290Pa88+ Th 287Pa2+ 3+ Th 290U E/T 51U87+ Th 126U87+ Th 214U89+ Th 268U89+ Th 287U33+ Th 290U89+ Th 315U90+ Th 315U90+ E/T 353U90+ Th 442U91+ Th 442U88+ Th 486e + Li+ 1E4−1E6 K Th 218e + Be2+ 1E4−1E6 K Th 218e + B3+ 1E4−1E6 K Th 218e + C4+ 1E4−1E6 K Th 218e + Li+ 1E4−1E6 K Th 218e + Be2+ 1E4−1E6 K Th 218e + B3+ 1E4−1E6 K Th 218e + C4+ 1E4−1E6 K Th 218e + W26+ Th 220e + W26+ Th 220e + HD Th 222e + e Th 223e + W71+ Th 224e + W72+ Th 224e + W73+ Th 224e + W37+ Th 224

20

e + W71+ Th 224e + W72+ Th 224e + W73+ Th 224e + W37+ Th 224e + Ca8+ 0−60 RYD Th 491e + Fe16+ Th 492e + Ni10+ threshold−1000 eV Th 493e + Ni10+ threshold−1000 eV Th 493e + Ni16+ threshold−1700 eV Th 494e + Ni16+ threshold−1700 eV Th 494e + Fe14+ threshold−1670 eV Th 495e + Fe14+ threshold−1670 eV Th 495He Z= 1-3 Th 87He Z= 2-3 Th 87He Z= 2-10 Th 225He Z= 6-8 Exp 305He Z= 18-24 E/T 353He Z= 26-27 E/T 353He Z= 2-10 Th 380He Z= 3-54 E/T 477Li Z= 3-13 Th 23Li Z= 12-20 Th 50Li Z= 41-50 Th 65Li Z= 12-20 Th 171Li Z= 3-9 Th 238Li Z= 3-7 Th 238Li Z= 7-30 Th 274Li Z= 6-8 Exp 305Li Z= 21-30 Th 346Li Z= 7-30 Th 430Be Z= 8-28 step 2 Th 30Be Z= 26-92 Th 48Be Z= 8-18 E/T 68Be Z= 8-28 step 2 Th 162Be Z= 5-92 Th 182Be Z= 4-110 Th 263Be Z= 5-74 E/T 277Be Z= 5-74 Th 278Be Z= 4-54 E/T 449Be Z= 4-92 Th 450Be Z= 4-36 E/T 477Be Z= 6-92 E/T 480B Z= 6-10 Th 4B Z= 5-19 Th 23B Z= 17-100 Th 70B Z= 6-10 step 2 E/T 93B Z= 6-14 step 2 E/T 93B Z= 14-35 Th 126B Z= 6-10 Th 148B Z= 6-14 Th 189B Z= 14-36 Th 214B Z= 8-30 E/T 277B Z= 8-30 Th 278B Z= 26-92 Th 279B Z= 22-29 Th 358B Z= 6-54 Th 393B Z= 18-22 E/T 477B Z= 22-29 Th 481C Z= 7-92 Th 118

21

C Z= 7-92 Th 206C Z= 7-10 Exp 216C Z= 26-92 Th 226C Z= 18-30 Th 244C Z= 7-28 E/T 277C Z= 7-28 Th 278C Z= 26-92 Th 394C Z= 18-30 Th 406C Z= 6-8 Th 418C Z= 14-16 E/T 477e + C Z= 9-28 Th 496e + C Z= 9-28 Th 496N Z= 9-36 Th 2N Z= 9-36 Th 147N Z= 26-92 Th 275N Z= 7-36 E/T 277N Z= 7-36 Th 278N Z= 7-100 Th 312N Z= 7-80 Th 412N Z= 7-100 Th 456O Z= 9-36 Th 11O Z= 9-36 Th 151O Z= 14-16 E/T 477F Z= 14-74 Th 47F Z= 14-74 Th 170F Z= 22-30 Th 245F Z= 22-30 Th 407F Z= 17-22 E/T 477Ne Z= 12-36 Th 5Ne Z= 12-36 Th 149Ne Z= 12-30 Th 184Ne Z= 18-36 E/T 227Ne Z= 18-36 Th 395Ne Z= 10-35 Th 450Na Z= 11-18 Th 23Na Z= 18-92 E/T 83Mg Z= 19-92 Th 257Mg Z= 13-100 Th 296Mg Z= 19-92 Th 420Mg Z= 13-100 Th 443P Z= 22-36 E/T 449Cl Z= 18-29 E/T 477K Z= 19-36 Th 23Ni Z= 72-79 Th 198Cu Z= 64-66 Exp 302Zn Z= 50-92 E/T 101e + Ga Z= 33-41 Th 223As Z= 38-92 Th 326Br Z= 38-42 Th 69Br Z= 38-42 Th 176Rb Z= 37-54 Th 23Sr Z= 50-92 Th 181Mo Z= 50-92 Th 181Rh Z= 50-92 Th 181Ag Z= 64-66 Exp 302Ag Z= 50-94 Th 308Ag Z= 62-74 E/T 333Ag Z= 50-94 Th 453Cs Z= 55-86 Th 23

22

Pm Z= 74-100 Th 71Pm Z= 74-100 E/T 177Sm Z= 74-100 Th 94Sm Z= 74-100 Th 190Tm Z= 70-88 Th 473Fr Z= 87-105 Th 23

2.2 Atomic and Molecular Collisions

2.2.1 Electron Collisions

H+ + U91+ 1−15 threshold unit, 1−2000 keVTh 768P + H2 16−3000eV Th 958P + D2 16−3000eV Th 958P + Kr 1E1−1E8 K Th 1344P + Kr+ 1E1−1E8 K Th 1344P + Kr2+ 1E1−1E8 K Th 1344P + Kr3+ 1E1−1E8 K Th 1344P + Kr4+ 1E1−1E8 K Th 1344P + Kr5+ 1E1−1E8 K Th 1344P + Kr6+ 1E1−1E8 K Th 1344hν + He 1keV,100MeV Th 991hν + He 1keV,100MeV Th 991e + Es ned Th 497e + Cf ned Th 497e + Bk ned Th 497e + Cm ned Th 497e + Am ned Th 497e + Pu ned Th 497e + Np ned Th 497e + U ned Th 497e + Pa ned Th 497e + Th ned Th 497e + Ac ned Th 497e + Ra ned Th 497e + Fr ned Th 497e + Rn ned Th 497e + At ned Th 497e + Po ned Th 497e + Bi ned Th 497e + Pb ned Th 497e + Tl ned Th 497e + Hg ned Th 497e + Au ned Th 497e + Pt ned Th 497e + Ir ned Th 497e + Os ned Th 497e + Re ned Th 497e + W ned Th 497e + Ta ned Th 497e + Hf ned Th 497e + Lu ned Th 497e + Yb ned Th 497e + Tm ned Th 497e + Er ned Th 497e + Ho ned Th 497e + Dy ned Th 497e + Tb ned Th 497

23

e + Gd ned Th 497e + Eu ned Th 497e + Sm ned Th 497e + Pm ned Th 497e + Nd ned Th 497e + Pr ned Th 497e + Ce ned Th 497e + La ned Th 497e + Ba ned Th 497e + Cs ned Th 497e + Xe ned Th 497e + I ned Th 497e + Te ned Th 497e + Sb ned Th 497e + Sn ned Th 497e + In ned Th 497e + Cd ned Th 497e + Ag ned Th 497e + Pd ned Th 497e + Rh ned Th 497e + Ru ned Th 497e + Tc ned Th 497e + Mo ned Th 497e + Nb ned Th 497e + Zr ned Th 497e + Y ned Th 497e + Sr ned Th 497e + Rb ned Th 497e + Kr ned Th 497e + Br ned Th 497e + Se ned Th 497e + As ned Th 497e + Ge ned Th 497e + Ga ned Th 497e + Zn ned Th 497e + Cu ned Th 497e + Ni ned Th 497e + Co ned Th 497e + Fe ned Th 497e + Mn ned Th 497e + Cr ned Th 497e + V ned Th 497e + Ti ned Th 497e + Sc ned Th 497e + Ca ned Th 497e + K ned Th 497e + Ar ned Th 497e + Cl ned Th 497e + S ned Th 497e + P ned Th 497e + Si ned Th 497e + Al ned Th 497e + Mg ned Th 497e + Na ned Th 497e + Ne ned Th 497e + F ned Th 497e + O ned Th 497e + N ned Th 497e + C ned Th 497

24

e + B ned Th 497e + Be ned Th 497e + Li ned Th 497e + He ned Th 497e + H ned Th 497e + C2H6 0−12 eV Th 498e + Pb threshold−10000 eV Th 499e + I threshold−10000 eV Th 499e + Te threshold−10000 eV Th 499e + Sb threshold−10000 eV Th 499e + Sn threshold−10000 eV Th 499e + Se threshold−10000 eV Th 499e + As threshold−10000 eV Th 499e + Cu threshold−10000 eV Th 499e + N threshold−10000 eV Th 499e + N2 0−10 eV Th 500e + N2 0−10 eV Th 500e + He 0−25 eV Th 501e + Au49+ 100−1E4 eV Th 502e + Au50+ 100−1E4 eV Th 502e + Au51+ 100−1E4 eV Th 502e + H2 1−10 eV Th 503e + CH2O 50−85 eV Exp 504e + Ar7+ 0−1E6 eV Th 505e + Ar6+ 0−1E6 eV Th 505e + Ar5+ 0−1E6 eV Th 505e + Ar4+ 0−1E6 eV Th 505e + Ar3+ 0−1E6 eV Th 505e + Ar2+ 0−1E6 eV Th 505e + Ar+ 0−1E6 eV Th 505e + Ar 0−1E6 eV Th 505e + S 0−1E6 eV Th 505e + Al3+ 0−1E6 eV Th 505e + Mg 0−1E6 eV Th 505e + Na 0−1E6 eV Th 505e + Ne2+ 0−1E6 eV Th 505e + Ne+ 0−1E6 eV Th 505e + Ne 0−1E6 eV Th 505e + O3+ 0−1E6 eV Th 505e + O2+ 0−1E6 eV Th 505e + O 0−1E6 eV Th 505e + C3+ 0−1E6 eV Th 505e + C+ 0−1E6 eV Th 505e + B+ 0−1E6 eV Th 505e + Li+ 0−1E6 eV Th 505e + Li 0−1E6 eV Th 505e + H 0−1E6 eV Th 505e + Gd36+ 100−5000 eV Th 506e + Sc+ 40−1000 eV Th 507e + CD2

+ 0−2.5 keV Exp 508e + CD2

+ 0−2.5 keV Exp 508e + CD2

+ 0−2.5 keV Exp 508e + CD3

+ 0−2.5 keV Exp 509e + CD3

+ 0−2.5 keV Exp 509e + CD3

+ 0−2.5 keV Exp 509e + C2H4 0−1000 eV Exp 510e + U 0−2E9 eV Th 511e + Bi 0−2E9 eV Th 511e + Pb 0−2E9 eV Th 511

25

e + Au 0−2E9 eV Th 511e + Ta 0−2E9 eV Th 511e + Ba 0−2E9 eV Th 511e + Sn 0−2E9 eV Th 511e + In 0−2E9 eV Th 511e + Ag 0−2E9 eV Th 511e + Pd 0−2E9 eV Th 511e + Mo 0−2E9 eV Th 511e + Y 0−2E9 eV Th 511e + Sr 0−2E9 eV Th 511e + Ga 0−2E9 eV Th 511e + Rb 0−2E9 eV Th 511e + Zn 0−2E9 eV Th 511e + Se 0−2E9 eV Th 511e + Cu 0−2E9 eV Th 511e + Ni 0−2E9 eV Th 511e + Co 0−2E9 eV Th 511e + Cr 0−2E9 eV Th 511e + V 0−2E9 eV Th 511e + Ar 0−2E9 eV Th 511e + Si 0−2E9 eV Th 511e + Al 0−2E9 eV Th 511e + Ne 0−2E9 eV Th 511e + N 0−2E9 eV Th 511e + C 0−2E9 eV Th 511e + He 0−2E9 eV Th 511e + H 0−2E9 eV Th 511e + U 0−2E9 eV Th 512e + Bi 0−2E9 eV Th 512e + Pb 0−2E9 eV Th 512e + Au 0−2E9 eV Th 512e + Ba 0−2E9 eV Th 512e + Sb 0−2E9 eV Th 512e + Sn 0−2E9 eV Th 512e + In 0−2E9 eV Th 512e + Ag 0−2E9 eV Th 512e + Pd 0−2E9 eV Th 512e + Mo 0−2E9 eV Th 512e + Y 0−2E9 eV Th 512e + Sr 0−2E9 eV Th 512e + Se 0−2E9 eV Th 512e + Ge 0−2E9 eV Th 512e + Zn 0−2E9 eV Th 512e + Ni 0−2E9 eV Th 512e + Co 0−2E9 eV Th 512e + Fe 0−2E9 eV Th 512e + Mn 0−2E9 eV Th 512e + Cr 0−2E9 eV Th 512e + V 0−2E9 eV Th 512e + Ca 0−2E9 eV Th 512e + Ar 0−2E9 eV Th 512e + Si 0−2E9 eV Th 512e + Al 0−2E9 eV Th 512e + Ne 0−2E9 eV Th 512e + C 0−2E9 eV Th 512e + He 0−2E9 eV Th 512e + H 0−2E9 eV Th 512e + Au 0−30 keV Th 513e + Ag 0−30 keV Th 513

26

e + Cu 0−30 keV Th 513e + Si 0−30 keV Th 513e + Al 0−30 keV Th 513e + N2O 15−200 eV Exp 514e + C2N2 300−800 eV Th 515e + C2 300−800 eV Th 515e + Ar2+ 113 eV Th 516e + Li+ 0−1000 eV E/T 517e + Kr 0−18 eV E/T 518e + Cs 0−18 eV E/T 518e + H2 8 keV Exp 519e + Be 0−500 keV Th 520e + D3

+ 0−2.5 keV Exp 521e + D3

+ 0−2.5 keV Exp 521e + D3

+ 0−2.5 keV Exp 521e + N2 5−20 eV Exp 522e + SiO 0−10 eV Th 523e + H4O2 0−10 eV Th 524e + Xe 14−40 eV Exp 525e + Ne 14−40 eV Exp 525e + BF+ 0−20 eV Th 526e + He 102 eV Th 527e + He 23.5−35 eV E/T 528e + CH4 500 eV E/T 529e + Kr 12.3−16.6 eV E/T 530e + Cs 12.3−16.6 eV E/T 530e + H2 33.6 eV−64.6 eV E/T 531e + He 33.6 eV−64.6 eV E/T 531e + H 33.6 eV−64.6 eV E/T 531e + N2 0−10 eV Th 532e + N2 0−10 eV Th 532e + N2 0−10 eV Th 532e + Ne 0−100 eV Th 533e + B3+ 0−2000 eV E/T 534e + H2 13.5−1000 eV Th 535e + H2O 0−120 eV Exp 536e + OH 0−120 eV Exp 536e + H2O 0−120 eV Exp 536e + OH 0−120 eV Exp 536e + Mg 0−100 eV Th 537e + N2 13−100 eV Exp 538e + O2 0−1000 eV E/T 539e + O2 0−1000 eV E/T 539e + O2 0−1000 eV E/T 539e + O2 0−1000 eV E/T 539e + O2 0−1000 eV E/T 539e + O2 0−1000 eV E/T 539e + O2 0−1000 eV E/T 539e + N2 0−1 keV E/T 540e + N 0−1 keV E/T 540e + N2 0−1 keV E/T 540e + N 0−1 keV E/T 540e + N2 0−1 keV E/T 540e + N 0−1 keV E/T 540e + CH 0−30 eV Th 541e + H+ 0−100 eV Th 542e + He 0−100 eV Th 542e + H 0−100 eV Th 542e + Li2 0−2.5 eV Th 543

27

e + N2 13−100 eV Exp 544e + N2 13−100 eV Exp 545e + Al 0−25 keV Exp 546e + NO2 1−12 eV Th 547e + NO2 1−12 eV Th 547e + Al+ 1−1000 eV Th 548e + Mg 1−1000 eV Th 548e + Zn 0−300 eV E/T 549e + H2S 0−300 eV Exp 550e + H2S 0−300 eV Exp 550e + Hg 0−80 eV E/T 551e + Hg 0−200 eV E/T 552e + CH3

+ 0−100 eV Exp 553e + CD3

+ 0−100 eV Exp 553e + H2 35.4 eV Th 554e + Si 3−25 keV Exp 555e + H2O 0−100 eV E/T 556e + CF4 0−1.5 eV Th 557e + H2 2−18 eV Th 558e + H2 2−18 eV Th 558e + SO 1−500 eV Th 559e + Cu 0−100 eV E/T 560e + Cs 5−15 eV Th 561e + Cs 5−15 eV Th 561e + AlH Th 562e + AlH Th 562e + AlH Th 562e + U91+ 0−600 eV Th 563e + N2 75, 150 eV E/T 564e + Xe Exp 565e + H2O 0.1−10 eV Th 566e + CH2O 0.1−10 eV Th 566e + H2 4081 eV Th 567e + W 50 eV Exp 568e + W6+ 0−5000 eV Exp 569e + W4+ 0−5000 eV Exp 569e + W2+ 0−5000 eV Exp 569e + W 0−5000 eV Exp 569e + Mg+ 0−1000 K Th 570e + Na+ 0−1000 K Th 570e + O+ 0−1000 K Th 570e + N+ 0−1000 K Th 570e + C+ 0−1000 K Th 570e + He+ 0−1000 K Th 570e + Ta46+ 1−1E5 eV Th 571e + Kr30+ 8.6−9.6 keV Exp 572e + Kr31+ 8.6−9.6 keV Exp 572e + Kr32+ 8.6−9.6 keV Exp 572e + Kr33+ 8.6−9.6 keV Exp 572e + Kr34+ 8.6−9.6 keV Exp 572e + He 9.5 eV Th 573e + Ar 8−10.5 eV Th 574e + Ar16+ 1e2−1e5 eV E/T 575e + O6+ 1e2−1e5 eV E/T 575e + N5+ 1e2−1e5 eV E/T 575e + B3+ 1e2−1e5 eV E/T 575e + Na 50?150 eV Th 576e + Li 50?150 eV Th 576e + Xe 750−7000 eV Th 577

28

e + H 750−7000 eV Th 577e + Ar 5−300 eV E/T 578e + CO2 0−25 eV Th 579e + H2 0−25 eV Th 579e + U65+ 0.5Et − 15Et Th 580e + At58+ 0.5Et − 15Et Th 580e + Au52+ 0.5Et − 15Et Th 580e + W47+ 0.5Et − 15Et Th 580e + Dy39+ 0.5Et − 15Et Th 580e + Pr32+ 0.5Et − 15Et Th 580e + Xe27+ 0.5Et − 15Et Th 580e + Ag20+ 0.5Et − 15Et Th 580e + Mo15+ 0.5Et − 15Et Th 580e + Kr9+ 0.5Et − 15Et Th 580e + Xe E/T 581e + Kr E/T 581e + Ar E/T 581e + Ne2

+ 300−10000K Th 582e + Ne2

+ 300−10000K Th 582e + Au 50−2000 eV Th 583e + Nd 50−2000 eV Th 583e + Ag 50−2000 eV Th 583e + Cu 50−2000 eV Th 583e + Al 50−2000 eV Th 583e + H 50−2000 eV Th 583e + K 6−60 eV Th 584e + CS2 30 eV to 500 eV Exp 585e + SF6 30 eV to 500 eV Exp 585e + CS2 30 eV to 500 eV Exp 585e + SF6 30 eV to 500 eV Exp 585e + Xe 150 eV E/T 586e + Ne 150 eV E/T 586e + HD+ 0.0001−1 eV Th 587e + HD+ 0.0001−1 eV Th 587e + HeD 0.0001−1 eV Th 588e + HeH 0.0001−1 eV Th 588e + HeD 0.0001−1 eV Th 588e + HeH 0.0001−1 eV Th 588e + Ar 39, 23, and 16.5 eV Th 589e + CF2 2?20 eV, Exp 590e + C6H5CH3 1.5−200 eV Exp 591e + C6H6 1.5−200 eV Exp 591e + Tm 0−1 eV Th 592e + Dy 0−1 eV Th 592e + Gd 0−1 eV Th 592e + Eu 0−1 eV Th 592e + Nd 0−1 eV Th 592e + Pr 0−1 eV Th 592e + Ce 0−1 eV Th 592e + La 0−1 eV Th 592e + BeH+ 0−5 eV Th 593e + BeH+ 0−5 eV Th 593e + C2D2 0−10 eV Exp 594e + C2H2 0−10 eV Exp 594e + C2D2 0−10 eV Exp 594e + C2H2 0−10 eV Exp 594e + HNC 0−7 eV Th 595e + HCN 0−7 eV Th 595e + HNC 0−7 eV Th 595

29

e + HCN 0−7 eV Th 595e + C2D2 0−7 eV Th 596e + C2H2 0−7 eV Th 596e + C2D2 0−7 eV Th 596e + C2H2 0−7 eV Th 596e + Hg76+ 49.0−50.2 eV Th 597e + HCO+ 0.001−1 eV E/T 598e + HCO+ 0.001−1 eV E/T 598e + D3

+ 0.001−1 eV E/T 599e + D2H 0.001−1 eV E/T 599e + H2D

+ 0.001−1 eV E/T 599e + H3

+ 0.001−1 eV E/T 599e + D3

+ 0.001−1 eV E/T 599e + D2H 0.001−1 eV E/T 599e + H2D

+ 0.001−1 eV E/T 599e + H3

+ 0.001−1 eV E/T 599e + Ca 10.11− 24.6 eV E/T 600e + HCNH+ 100−700 K E/T 601e + HCNH+ 100−700 K E/T 601e + Ne2

+ 200−700 K E/T 602e + Ne2

+ 200−700 K E/T 602e + Ca16+ 15−225 Ry Th 603e + Na 0.5− 6.5 eV Th 604e + CS 1−100 eV Th 605e + CS 1−100 eV Th 605e + SF6 30−5000 eV Th 606e + SF4 30−5000 eV Th 606e + SO2 30−5000 eV Th 606e + N2 0.1?1.0 eV E/T 607e + N2 0.1?1.0 eV E/T 607e + N2

− 10 eV E/T 608e + N2 10 eV E/T 608e + N2

− 10 eV E/T 608e + N2 10 eV E/T 608e + N2

− 10 eV E/T 608e + N2 10 eV E/T 608e + C4H6 200−4500 eV Exp 609e + C4H8 200−4500 eV Exp 609e + C3H6 200−4500 eV Exp 609e + C2H4 200−4500 eV Exp 609e + C2H4O 0.7−20 eV Th 610e + C2H4O 0.7−20 eV Th 610e + U82+ 150 eV, 30000 eV Th 611e + SiH4 1e−3 − 1e3 eV Exp 612e + CH4 1e−3 − 1e3 eV Exp 612e + CF4 1e−3 − 1e3 eV Exp 612e + N2O 1e−3 − 1e3 eV Exp 612e + SF6 1e−3 − 1e3 eV Exp 612e + Xe 1e−3 − 1e3 eV Exp 612e + Kr 1e−3 − 1e3 eV Exp 612e + Ar 1e−3 − 1e3 eV Exp 612e + He 102 eV E/T 613e + Cl2 300−1100 K Exp 614e + Cl2 300−1100 K Exp 614e + HCOOH 0.5−2.5 eV Th 615e + HCOOH 0.5−2.5 eV Th 615e + CH3Cl 300−1200K Exp 616e + NF3 300−1200K Exp 616e + CH3Cl 300−1200K Exp 616

30

e + NF3 300−1200K Exp 616e + K+ 1000−1000000K Th 617e + Ni+ 10−100000K Th 618e + Cr+ 1000−100000K Th 619e + Zn29+ 1E−6/Z2-10/Z2K Th 620e + Cu28+ 1E−6/Z2-10/Z2K Th 620e + Ni 1E−6/Z2-10/Z2K Th 620e + Co26+ 1E−6/Z2-10/Z2K Th 620e + Fe25+ 1E−6/Z2-10/Z2K Th 620e + Mn24+ 1E−6/Z2-10/Z2K Th 620e + Cr23+ 1E−6/Z2-10/Z2K Th 620e + V22+ 1E−6/Z2-10/Z2K Th 620e + Ti21+ 1E−6/Z2-10/Z2K Th 620e + Sc20+ 1E−6/Z2-10/Z2K Th 620e + Ca19+ 1E−6/Z2-10/Z2K Th 620e + K18+ 1E−6/Z2-10/Z2K Th 620e + Ar17+ 1E−6/Z2-10/Z2K Th 620e + Cl16+ 1E−6/Z2-10/Z2K Th 620e + S15+ 1E−6/Z2-10/Z2K Th 620e + P14+ 1E−6/Z2-10/Z2K Th 620e + Si13+ 1E−6/Z2-10/Z2K Th 620e + Al12+ 1E−6/Z2-10/Z2K Th 620e + Mg11+ 1E−6/Z2-10/Z2K Th 620e + Na10+ 1E−6/Z2-10/Z2K Th 620e + Ne9+ 1E−6/Z2-10/Z2K Th 620e + F8+ 1E−6/Z2-10/Z2K Th 620e + O7+ 1E−6/Z2-10/Z2K Th 620e + N6+ 1E−6/Z2-10/Z2K Th 620e + C5+ 1E−6/Z2-10/Z2K Th 620e + B4+ 1E−6/Z2-10/Z2K Th 620e + Be 1E−6/Z2-10/Z2K Th 620e + Li2+ 1E−6/Z2-10/Z2K Th 620e + He+ 1E−6/Z2-10/Z2K Th 620e + Mg7+ 200−1800eV Exp 621e + S+ 5000−100000K Th 622e + N+ 2−12eV Th 623e + Li 0−25eV Th 624e + CH 10−90eV Exp 625e + H2 10−100eV Th 626e + H2 10−100eV Th 626e + CO 0−50eV Th 627e + CO 0−50eV Th 627e + C2D2

+ 6.5−2498.5eV Exp 628e + C2H2

+ 6.5−2498.5eV Exp 628e + C2D2

+ 6.5−2498.5eV Exp 628e + C2H2

+ 6.5−2498.5eV Exp 628e + C2D2

+ 6.5−2498.5eV Exp 629e + C2H2

+ 6.5−2498.5eV Exp 629e + C2D2

+ 6.5−2498.5eV Exp 630e + C2H2

+ 6.5−2498.5eV Exp 630e + Ti21+ 5400−24000eV Th 631e + NH3 15−2000eV Th 632e + NO 15−2000eV Th 632e + F 15−2000eV Th 632e + O 15−2000eV Th 632e + N 15−2000eV Th 632e + C 15−2000eV Th 632e + C2D2

+ 2.1− 2495.1eV Exp 633e + C2H2

+ 2.1− 2495.1eV Exp 633

31

e + C2D2+ 2.1− 2495.1eV Exp 633

e + C2H2+ 2.1− 2495.1eV Exp 633

e + HI 15 − 2000eV Th 634e + HBr 15 − 2000eV Th 634e + HCl 15 − 2000eV Th 634e + HF 15 − 2000eV Th 634e + I 15 − 2000eV Th 634e + Br 15 − 2000eV Th 634e + Cl 15 − 2000eV Th 634e + F 15 − 2000eV Th 634e + K 0−2000eV Th 635e + Na 0−2000eV Th 635e + Li 0−2000eV Th 635e + K 0−2000eV Th 635e + Na 0−2000eV Th 635e + Li 0−2000eV Th 635e + CH3Br 50,100,200eV 636e + CH3Cl 50,100,200eV 636e + CH3I 50,100,200eV 636e + CH3F 50,100,200eV 636e + CH3Br 50,100,200eV 636e + CH3Cl 50,100,200eV 636e + CH3I 50,100,200eV 636e + CH3F 50,100,200eV 636e + N2O 6−5000eV Exp 637e + S2 15−5000eV Th 638e + OCS 15−5000eV Th 638e + CS2 15−5000eV Th 638e + CS 15−5000eV Th 638e + CO2 15−5000eV Th 638e + CO 15−5000eV Th 638e + Xe24+ 750−1250eV Th 639e + He 0−200eV Th 640e + C2 0− 50eV Th 641e + CH3I 6.5eV, 5.9eV, 5.5eV, 4.7eV Exp 642e + CH3Br 6.5eV, 5.9eV, 5.5eV, 4.7eV Exp 642e + CH3Cl 6.5eV, 5.9eV, 5.5eV, 4.7eV Exp 642e + CH3F 6.5eV, 5.9eV, 5.5eV, 4.7eV Exp 642e + S4+ 10−16eV Th 643e + Xe 0−12.5eV Th 644e + Kr 0−12.5eV Th 644e + NH+ 2.1−2495.1eV Exp 645e + NH+ 2.1−2495.1eV Exp 645e + Be 0−500eV Th 646e + Pu 10−1E9eV Th 647e + Np 10−1E9eV Th 647e + U 10−1E9eV Th 647e + Pa 10−1E9eV Th 647e + Th 10−1E9eV Th 647e + Ac 10−1E9eV Th 647e + Ra 10−1E9eV Th 647e + Fr 10−1E9eV Th 647e + Rn 10−1E9eV Th 647e + At 10−1E9eV Th 647e + Po 10−1E9eV Th 647e + Bi 10−1E9eV Th 647e + Pb 10−1E9eV Th 647e + Tl 10−1E9eV Th 647e + Hg 10−1E9eV Th 647

32

e + Au 10−1E9eV Th 647e + Pt 10−1E9eV Th 647e + Ir 10−1E9eV Th 647e + Os 10−1E9eV Th 647e + Re 10−1E9eV Th 647e + W 10−1E9eV Th 647e + Ta 10−1E9eV Th 647e + Hf 10−1E9eV Th 647e + Lu 10−1E9eV Th 647e + Yb 10−1E9eV Th 647e + Tm 10−1E9eV Th 647e + Er 10−1E9eV Th 647e + Ho 10−1E9eV Th 647e + Dy 10−1E9eV Th 647e + Tb 10−1E9eV Th 647e + Gd 10−1E9eV Th 647e + Eu 10−1E9eV Th 647e + Sm 10−1E9eV Th 647e + Pm 10−1E9eV Th 647e + Nd 10−1E9eV Th 647e + Pr 10−1E9eV Th 647e + Ce 10−1E9eV Th 647e + La 10−1E9eV Th 647e + Ba 10−1E9eV Th 647e + Cs 10−1E9eV Th 647e + Xe 10−1E9eV Th 647e + I 10−1E9eV Th 647e + Te 10−1E9eV Th 647e + Sb 10−1E9eV Th 647e + Sn 10−1E9eV Th 647e + In 10−1E9eV Th 647e + Cd 10−1E9eV Th 647e + Ag 10−1E9eV Th 647e + Pd 10−1E9eV Th 647e + Rh 10−1E9eV Th 647e + Ru 10−1E9eV Th 647e + Tc 10−1E9eV Th 647e + Mo 10−1E9eV Th 647e + Nb 10−1E9eV Th 647e + Zr 10−1E9eV Th 647e + Y 10−1E9eV Th 647e + Sr 10−1E9eV Th 647e + Rb 10−1E9eV Th 647e + Kr 10−1E9eV Th 647e + Br 10−1E9eV Th 647e + Se 10−1E9eV Th 647e + As 10−1E9eV Th 647e + Ge 10−1E9eV Th 647e + Ga 10−1E9eV Th 647e + Zn 10−1E9eV Th 647e + Cu 10−1E9eV Th 647e + Ni 10−1E9eV Th 647e + Co 10−1E9eV Th 647e + Fe 10−1E9eV Th 647e + Mn 10−1E9eV Th 647e + Cr 10−1E9eV Th 647e + V 10−1E9eV Th 647e + Ti 10−1E9eV Th 647e + Sc 10−1E9eV Th 647

33

e + Ca 10−1E9eV Th 647e + K 10−1E9eV Th 647e + Ar 10−1E9eV Th 647e + Cl 10−1E9eV Th 647e + S 10−1E9eV Th 647e + P 10−1E9eV Th 647e + Si 10−1E9eV Th 647e + Al 10−1E9eV Th 647e + Mg 10−1E9eV Th 647e + Na 10−1E9eV Th 647e + Ne 10−1E9eV Th 647e + F 10−1E9eV Th 647e + O 10−1E9eV Th 647e + N 10−1E9eV Th 647e + C 10−1E9eV Th 647e + B 10−1E9eV Th 647e + Be 10−1E9eV Th 647e + Li 10−1E9eV Th 647e + He 10−1E9eV Th 647e + H 10−1E9eV Th 647e + W 9keV−40keV Exp 648e + Gd 9keV−40keV Exp 648e + H2 Th 649e + H2 Th 649e + Mg Th 650e + Mg Th 650e + Ni13+ 0−100eV Th 651e + In+ 33−120eV Exp 652e + Ar+ 25−2495eV Exp 653e + Be 10−50eV Exp 654e + Be 10−50eV Exp 654e + Ar 113.5 eV − 600 eV E/T 655e + Ne 113.5 eV − 600 eV E/T 655e + GeH4 20eV− 100eV 656e + Si2H6 20eV− 100eV 656e + SiH4 20eV− 100eV 656e + SF6 20eV− 100eV 656e + NF3 20eV− 100eV 656e + CF3I 20eV− 100eV 656e + F 20eV− 100eV 656e + CH3 20eV− 100eV 656e + CH2F2 20eV− 100eV 656e + CHF3 20eV− 100eV 656e + C6F6 20eV− 100eV 656e + C4F8 20eV− 100eV 656e + C3F8 20eV− 100eV 656e + C3F6 20eV− 100eV 656e + F6 20eV− 100eV 656e + C2 20eV− 100eV 656e + C2F4 20eV− 100eV 656e + CF4 20eV− 100eV 656e + CF2 20eV− 100eV 656e + C 5−5000K Th 657e + C 5−5000K Th 657e + H3

+ 1−7000K Th 658e + Kr 10−3000eV Th 659e + Fe 10−3000eV Th 659e + Ne 10−3000eV Th 659e + H 10−3000eV Th 659

34

e + Bi 7−30keV Exp 660e + Zn 7−30keV Exp 661e + Ca 7−30keV Exp 661e + S 7−30keV Exp 661e + C6H6 1−1000eV Th 662e + SF6 1−1000eV Th 662e + CF4 1−1000eV Th 662e + CO2 1−1000eV Th 662e + Na 0−5.5eV Th 663e + He 10−500eV Th 664e + He 10−500eV Th 664e + He 20−500eV Th 665e + He 20−500eV Th 665e + C+ 5−20000eV Th 666e + C 5−20000eV Th 666e + H 10−80eV Th 667e + H 0−12eV Th 668e + CO 0−5eV Exp 669e + CO 0−5eV Exp 669e + Mo41+ 1−15u(scaled unit) Exp 670e + Dy65+ 1−15u(scaled unit) Exp 670e + Fe25+ 1−15u(scaled unit) Exp 670e + Ar17+ 1−15u(scaled unit) Exp 670e + Ne9+ 1−15u(scaled unit) Exp 670e + Na 0−6eV Th 671e + He Th 672e + Cu 1−5eV 673e + H2 1−5eV Exp 674e + N2 400−1500eV Exp 675e + H 0−150eV Th 676e + C4H4O 0.6−400eV Exp 677e + C4H4O 0.6−400eV Exp 677e + SO 1−10eV Th 678e + SO 1−10eV Th 678e + H2O 10−10000eV Th 679e + O2 5.9−5000eV Exp 680e + FD2

+ 2−100eV Exp 681e + OD2

+ 2−100eV Exp 681e + ND2

+ 2−100eV Exp 681e + BD2

+ 2−100eV Exp 681e + CH2

+ 2−100eV Exp 681e + FD2

+ 2−100eV Exp 681e + OD2

+ 2−100eV Exp 681e + ND2

+ 2−100eV Exp 681e + BD2

+ 2−100eV Exp 681e + CH2

+ 2−100eV Exp 681e + B2+ 0−40eV Th 682e + B+ 0−40eV Th 682e + B 0−40eV Th 682e + CO2 10−26keV Exp 683e + CO2 10−26keV Exp 683e + H 0−250eV Th 684e + H 0−250eV Th 684e + NH 0−10eV Th 685e + NH 0−10eV Th 685e + BH2 0−10eV Th 686e + BH2 0−10eV Th 686e + O3

+ 3−100eV Exp 687e + H 9.52−10.26eV Th 688

35

e + H2 1−10eV Th 689e + He 10−4000eV 690e + He 10−4000eV 690e + D2 0.1−100eV 691e + H2 0.1−100eV 691e + HD 0.1−100eV 691e + D2 0.1−100eV 691e + H2 0.1−100eV 691e + HD 0.1−100eV 691e + Zn12+ 0.1−10000eV Th 692e + Cu11+ 0.1−10000eV Th 692e + Ni10+ 0.1−10000eV Th 692e + Co9+ 0.1−10000eV Th 692e + Fe8+ 0.1−10000eV Th 692e + Mn7+ 0.1−10000eV Th 692e + Cr6+ 0.1−10000eV Th 692e + V5+ 0.1−10000eV Th 692e + Ti4+ 0.1−10000eV Th 692e + Sc3+ 0.1−10000eV Th 692e + Ca2+ 0.1−10000eV Th 692e + K+ 0.1−10000eV Th 692e + Ca 20−500eV Th 693e + Ca 20−500eV Th 693e + Ba48+ 8.7−24keV Th 694e + Ba49+ 8.7−24keV Th 694e + Ba50+ 8.7−24keV Th 694e + Ba51+ 8.7−24keV Th 694e + Ba52+ 8.7−24keV Th 694e + Ba53+ 8.7−24keV Th 694e + Ba54+ 8.7−24keV Th 694e + I45+ 8.7−24keV Th 694e + I46+ 8.7−24keV Th 694e + I47+ 8.7−24keV Th 694e + I48+ 8.7−24keV Th 694e + I49+ 8.7−24keV Th 694e + I50+ 8.7−24keV Th 694e + I51+ 8.7−24keV Th 694e + Kr28+ 8.7−24keV Th 694e + Kr29+ 8.7−24keV Th 694e + Kr30+ 8.7−24keV Th 694e + Kr31+ 8.7−24keV Th 694e + Kr32+ 8.7−24keV Th 694e + Kr33+ 8.7−24keV Th 694e + Kr34+ 8.7−24keV Th 694e + H2O 6−50eV Th 695e + U64+ 5−69000eV Th 696e + At57+ 5−69000eV Th 696e + Pb54+ 5−69000eV Th 696e + Au51+ 5−69000eV Th 696e + W46+ 5−69000eV Th 696e + Yb42+ 5−69000eV Th 696e + Gd36+ 5−69000eV Th 696e + Nd32+ 5−69000eV Th 696e + Xe26+ 5−69000eV Th 696e + Sn22+ 5−69000eV Th 696e + Ag19+ 5−69000eV Th 696e + Mo14+ 5−69000eV Th 696e + Kr8+ 5−69000eV Th 696e + Eu 10eV, 20eV Th 697

36

e + Mn 10eV, 20eV Th 697e + Sb 10eV, 20eV Th 697e + Ag 10eV, 20eV Th 697e + Fr 2−300eV Th 698e + Cs 2−300eV Th 698e + Rb 2−300eV Th 698e + CF3H 1.5−30eV Exp 699e + CF3I 1.5−30eV Exp 699e + W35+ 5−3000eV Th 700e + Sb 6−1000eV Th 701e + Sb 6−1000eV Th 701e + Kr 5−10eV Exp 702e + CF3I 10−50eV Exp 703e + Er 0−1eV Th 704e + Ho 0−1eV Th 704e + Sm 0−1eV Th 704e + Dy 0−1eV Th 704e + Hf 0−1eV Th 704e + Tm 0−1eV Th 704e + Pr 0−1eV Th 704e + CD5

+ 0.0001− 1eV Exp 705e + CH5

+ 0.0001− 1eV Exp 705e + D2H

+ 0.0001 − 10eV Exp 706e + U91+ 1−700MeV/nucleon Th 707e + C4H4O 1−50eV Exp 708e + C4H4O 1−50eV Exp 708e + DCN 1.2−3.1eV Exp 709e + HCN 1.2−3.1eV Exp 709e + N2 400−1600eV Exp 710e + Hg 0−200eV Th 711e + H3

+ 0.00001−30eV Exp 712e + Ne 0−200eV Th 713e + Ni5+ 10−1000000eV Th 714e + Ar5+ 10−1000000eV Th 714e + Ti2+ 10−1000000eV Th 714e + S4+ 10−1000000eV Th 714e + Cr8+ 10−1000000eV Th 714e + Si3+ 10−1000000eV Th 714e + U82+ 10−1000000eV Th 714e + N3+ 10−1000000eV Th 714e + Ne3+ 10−1000000eV Th 714e + Ne8+ 10−1000000eV Th 714e + U89+ 10−1000000eV Th 714e + C5+ 10−1000000eV Th 714e + CNN 0−10eV Th 715e + NCN 0−10eV Th 715e + HBr 0−1000eV Th 716e + HBr 0−1000eV Th 716e + CH4 5−1000eV Th 717e + CH3 5−1000eV Th 717e + CH2 5−1000eV Th 717e + CH 5−1000eV Th 717e + CH4 5−1000eV Th 717e + CH3 5−1000eV Th 717e + CH2 5−1000eV Th 717e + CH 5−1000eV Th 717e + CH4 5−1000eV Th 717e + CH3 5−1000eV Th 717e + CH2 5−1000eV Th 717

37

e + CH 5−1000eV Th 717e + C2H5OH 60−500eV Exp 718e + CH3OH 60−500eV Exp 718e + C4H4N2 0.1−1000eV Th 719e + C2H6 40−100eV 720e + C2H6 40−100eV 720e + C4H10 10−1000eV Th 721e + C3H8 10−1000eV Th 721e + C2H6 10−1000eV Th 721e + C4H8 10−1000eV Th 721e + C3H6 10−1000eV Th 721e + C2H4 10−1000eV Th 721e + C3H4 200−4500eV Exp 722e + C2H2 200−4500eV Exp 722e + CS2 1−1000eV Th 723e + CS2 1−1000eV Th 723e + HCl 0−4eV Th 724e + C3H8 40−500eV 725e + C3H8 40−500eV 725e + Kr 0.014− 20eV Exp 726e + C4H9OH 1−50eV Th 727e + C4H9OH 1−50eV Th 727e + S8+ 2E2−2E6 (Z+1)2 K Th 730e + S9+ 2E2−2E6 (Z+1)2 K Th 730e + S10+ 2E2−2E6 (Z+1)2 K Th 730e + S11+ 2E2−2E6 (Z+1)2 K Th 730e + Kr27+ 1E7−1E9 K Th 731e + Se24+ 100−10000 eV Th 732e + Ni+ 30 − 1E6 K Th 733e + Fe7+ 5E3−5E6 K Th 734e + N+ 500 − 1E5 K Th 735e + Cr+ 2E3−1E5 K Th 736e + H 50−300 eV Th 737e + H 50−300 eV Th 737e+ + U91+ 1−10 threshold unit Th 738e + H 50−300 eV Th 739e + H 50−300 eV Th 739e + Ar 2500 eV Exp 740e + N2 5−30 eV Th 741e + N2 5−30 eV Th 741e + HD+ 1−12 eV Th 742e + CH4 0.01−2E3 eV Th 743e + SiH4 0.01−2E3 eV Th 743e + H2O 0.01−2E3 eV Th 743e + Xe threshold−200 eV Th 744e + Ar 4−12 eV, 50−400 eV Th 745e + Nd+ threshold−2.5 keV E/T 746e + H 150, 250 eV Th 747e + H 150, 250 eV Th 747e threshold−1 keV Th 748e + e 0−300 eV Exp 749e + H2S 20−200 eV Exp 750e threshold−2 keV Th 751e + e threshold−2 keV Th 751e + e threshold−2 keV Th 752e + HCOOH threshold−2 keV Th 752e + PH3 threshold−2 keV Th 752e + H2S threshold−2 keV Th 752e + Ba46+ 5.69, 8.2 keV Th 753

38

e + U threshold−200 MeV, −1GeV Th 754e + Bi threshold−200 MeV, −1GeV Th 754e + Pb threshold−200 MeV, −1GeV Th 754e + Au threshold−200 MeV, −1GeV Th 754e + Ta threshold−200 MeV, −1GeV Th 754e + Ni4+ threshold−200 MeV, −1GeV Th 754e + Ni7+ threshold−200 MeV, −1GeV Th 754e + Fe5+ threshold−200 MeV, −1GeV Th 754e + Ni8+ threshold−200 MeV, −1GeV Th 754e + Fe6+ threshold−200 MeV, −1GeV Th 754e + Ti2+ threshold−200 MeV, −1GeV Th 754e + e+ threshold−200 MeV, −1GeV Th 754e + Ar3+ threshold−200 MeV, −1GeV Th 754e + Cr10+ threshold−200 MeV, −1GeV Th 754e + Ar4+ threshold−200 MeV, −1GeV Th 754e + Ar5+ threshold−200 MeV, −1GeV Th 754e + Cl4+ threshold−200 MeV, −1GeV Th 754e + Ar6+ threshold−200 MeV, −1GeV Th 754e + Cl5+ threshold−200 MeV, −1GeV Th 754e + S4+ threshold−200 MeV, −1GeV Th 754e + Mg2+ threshold−200 MeV, −1GeV Th 754e + Si5+ threshold−200 MeV, −1GeV Th 754e + Ne+ threshold−200 MeV, −1GeV Th 754e + Si6+ threshold−200 MeV, −1GeV Th 754e + Ne2+ threshold−200 MeV, −1GeV Th 754e + F2+ threshold−200 MeV, −1GeV Th 754e + O+ threshold−200 MeV, −1GeV Th 754e + O2+ threshold−200 MeV, −1GeV Th 754e + N+ threshold−200 MeV, −1GeV Th 754e + O3+ threshold−200 MeV, −1GeV Th 754e + N2+ threshold−200 MeV, −1GeV Th 754e + C+ threshold−200 MeV, −1GeV Th 754e + U88+ threshold−200 MeV, −1GeV Th 754e + Ne6+ threshold−200 MeV, −1GeV Th 754e + C2+ threshold−200 MeV, −1GeV Th 754e + Li+ threshold−200 MeV, −1GeV Th 754e + B3+ threshold−200 MeV, −1GeV Th 754e + C4+ threshold−200 MeV, −1GeV Th 754e + N5+ threshold−200 MeV, −1GeV Th 754e + O6+ threshold−200 MeV, −1GeV Th 754e + U90+ threshold−200 MeV, −1GeV Th 754e + Be+ threshold−200 MeV, −1GeV Th 754e + B2+ threshold−200 MeV, −1GeV Th 754e + N4+ threshold−200 MeV, −1GeV Th 754e + O5+ threshold−200 MeV, −1GeV Th 754e + Ne7+ threshold−200 MeV, −1GeV Th 754e + U89+ threshold−200 MeV, −1GeV Th 754e + Ne threshold−200 eV Th 755e + CH4 30−200 eV Exp 756e + SiCl4 30−200 eV Exp 757e + C6H6 10−200 eV E/T 758e + C6H6 10−200 eV E/T 758e + C4H8O 15−50 eV Exp 759e + C4H8O 15−50 eV Exp 759e + e threshold−360 eV Exp 760e + e 0.4−20 eV Exp 761e + e 0.4−20 eV Exp 761e + e 0.4−20 eV Exp 761e + CF4 Th 762

39

e + C4H8O 5.5−10 eV Exp 763e + C4H4N2 0−20 eV Th 764e + CCl4 1.5−100 eV Exp 765e + e threshold−2 keV Th 766e + P(CH3)3 threshold−2 keV Th 766e+ + H 20 eV Th 767e+ + H 20 eV Th 767e + U91+ 1−15 threshold unit, 1−2000 keVTh 768e + Yb 20 eV E/T 769e + Yb 20 eV E/T 769e+ + H 250 eV Th 770e + H 250 eV Th 770e+ + H 250 eV Th 770e + H 250 eV Th 770e+ + H2 0−10 eV Th 771e + Ar threshold−100 eV Exp 772e + Ar threshold−100 eV Exp 772e + He 80, 100, 120 eV E/T 773e + He 80, 100, 120 eV E/T 773e + He 500 eV E/T 774e + He 500 eV E/T 774e + C4H8O 5−150 eV Exp 775e + Mg 10, 15, 20, 40, 60 eV Exp 776e + Mg 10, 15, 20, 40, 60 eV Exp 776e + He threshold−1 keV Th 777e + Kr 10−15 eV E/T 778e + Kr 10−15 eV E/T 778e + He 28.6 eV Th 779e + He 28.6 eV Th 779e + D2H

+ 5 eV−2.5 keV Exp 780e + Ar 20−100 eV Th 781e + Ne 20−100 eV Th 781e + Ar 20−100 eV Th 781e + Ne 20−100 eV Th 781e + H2

+ 1−12 eV Th 782e + B+ 63−750 eV Th 783e + Ca 10−12 eV Exp 784e + Ca 10−12 eV Exp 784e + Xe threshold−2000 eV Th 785e + I threshold−2000 eV Th 785e + Te threshold−2000 eV Th 785e + Sb threshold−2000 eV Th 785e + Sn threshold−2000 eV Th 785e + In threshold−2000 eV Th 785e + N2 600−700 eV Exp 786e + Ar 600−700 eV Exp 786e + Ne 600−700 eV Exp 786e + N2 600−700 eV Exp 786e + Ar 600−700 eV Exp 786e + Ne 600−700 eV Exp 786e + W+ threshold−500 eV Th 787e + W threshold−500 eV Th 787e threshold−2000 eV Th 788e + Cs 10−600 eV Exp 789e + H Ea/E = 0.1, 0.3 (ratio of outgoing electron energy to incident electron energy)Th 790e + W17+ threshold−1000 eV E/T 791e + Ar 13 eV Exp 792e + Ar 13 eV Exp 792e+ + H 10−200 eV Th 793

40

e + Ne2+ 1E3−1E6 K Th 794e + H2O 100 eV Exp 795e + C8H16 10−200 eV Exp 796e + C6H12 10−200 eV Exp 796e+ + C2H2 0−5 eV Th 797e + N2 0−250 meV E/T 798e + N2 500−600 eV Th 799e + N2 500−600 eV Th 799e + N2O 0.65−4.55 eV Exp 800e + N2O 0.65−4.55 eV Exp 800e + e 1−400 eV E/T 801e + e 1−400 eV E/T 801e + Xe10+ threshold−1000 eV E/T 802e + S2 threshold−370 eV E/T 803e + C2H2CL2 0−20 eV Th 804e + N2 18.8−300 eV Exp 806e + D2 1−12 eV Th 808e + Ba 6−30 keV Exp 809e + Cl 6−30 keV Exp 809e + He 500, 1240−4260 eV Th 810e + He 500, 1240−4260 eV Th 810e + Hf 0−1.0 eV Th 811e + Lu 0−1.0 eV Th 811e + Tm 0−1.0 eV Th 811e + CH4 threshold−1000 eV Th 812e + NH3 threshold−1000 eV Th 812e + H2O threshold−1000 eV Th 812e + Hf threshold−1000 eV Th 812e + He 1000 eV Th 813e + He 1000 eV Th 813e + In 10−100 eV Th 814e + In 10−100 eV Th 814e + Hg 4−10 eV Exp 815e + Na 10−65 eV Th 816e + Na 10−65 eV Th 816e + Cs2 100 eV E/T 817e + H2O 2055 eV E/T 818e + H2O 2055 eV E/T 818e + H2O 1 keV Th 819e + H2O 1 keV Th 819e + Bi threshold−50 keV Th 820e + Pb threshold−50 keV Th 820e + Au threshold−50 keV Th 820e + Os threshold−50 keV Th 820e + Re threshold−50 keV Th 820e + W threshold−50 keV Th 820e + Ta threshold−50 keV Th 820e + Hf threshold−50 keV Th 820e + Pd threshold−18 keV Exp 821e + Kr 0.3−9.8 eV Th 822e + Na 6−60 eV Th 823e + Na 6−60 eV Th 823e + H 11.2−12.1 eV Th 824e + Zn 6.5−8.5 eV Exp 825e + I 1−50 eV E/T 826e + PH3 0.01−2000 eV Th 827e + H2S 0.01−2000 eV Th 827e + NH3 0.01−2000 eV Th 827e + Kr 15−30 eV Exp 828

41

e + Ar 15−30 eV Exp 828e + Kr 15−30 eV Exp 828e + Ar 15−30 eV Exp 828e + Co threshold−10 eV Exp 829e + Co threshold−10 eV Exp 829e + C4H2 1−10 eV Exp 830e + C4H2 1−10 eV Exp 830e + CH4 54 eV Exp 831e + He 5500−5600 eV Th 832e + He 5500−5600 eV Th 832e + Yb threshold−200 eV Th 833e + Yb threshold−200 eV Th 833e + He 70.6 eV E/T 834e + He 70.6 eV E/T 834e + Ar 195 eV E/T 835e + Ar 195 eV E/T 835e + Ba+ threshold−300 eV Th 836e + Cd+ threshold−300 eV Th 836e + Zn+ threshold−300 eV Th 836e + Ca+ threshold−300 eV Th 836e + Mg+ threshold−300 eV Th 836e + C4H2 1−15 eV E/T 837e + C3+ threshold−50 eV Th 838e + e 500−30000 K Th 839e + e 500−30000 K Th 839e + e 500−30000 K Th 839e + H2O 310−340 eV Th 840e + H2O 310−340 eV Th 840e + Fe16+ 820−1150 eV Th 841e + H2 1−1000 eV Th 842e + Ne3+ 1E4−1E6, 1E7 K Th 843e + Ne6+ 1E4−1E6, 1E7 K Th 843e + He 250 eV E/T 844e + He 250 eV E/T 844e + e 0−10 eV Th 845e + e 0−10 eV Th 845e + Ne threshold−100 eV Th 846e + Ar threshold−100 eV Th 846e + Ne threshold−100 eV Th 846e + Ar threshold−100 eV Th 846e + He 40.84−45.60 eV Th 847e + SO2 100−1000 eV E/T 848e+ + H2O 250 eV Th 849e + H2O 250 eV Th 849e+ + H2O 250 eV Th 849e + H2O 250 eV Th 849e + Nd56+ (1−5)?threshold Th 850e + Mo38+ (1−5)?threshold Th 850e + Bi79+ (1−5)?threshold Th 850e + N2D

+ 5−100 eV Exp 851e + H2 4087 eV Th 852e + CO2 12 keV Exp 853e + C3H7OH 1.5−30 eV E/T 854e + S2 0−10 eV Th 855e + S2 0−10 eV Th 855e + S2 0−10 eV Th 855e + H2CO 1−1000 eV Th 856e + HCOOH 1−1000 eV Th 856e + CF3Cl 0.4−2.4 eV Th 857

42

e + He 112−319 eV Th 858e + He 112−319 eV Th 858e + He 112−319 eV Th 858e + SiBR4 1−10 eV Th 859e + SiI4 1−10 eV Th 859e + SiCl4 1−10 eV Th 859e + C4H4O 5−15 eV Exp 860e + C+ threshold−25 eV Th 861e + C+ threshold−25 eV Th 861e 1−6 eV Th 862e + e 1−6 eV Th 862e + Mg 47.65 eV Exp 863e + Mg 47.65 eV Exp 863e + He 70 − 150 eV Th 864e + He 70 − 150 eV Th 864e + He 70 − 150 eV Th 864e + Li+ 1E4−1E6 K Th 865e + Be2+ 1E4−1E6 K Th 865e + B3+ 1E4−1E6 K Th 865e + C4+ 1E4−1E6 K Th 865e + Co3+ 40−70 eV Th 866e + C60 threshold−1000 eV Th 867e + Ca9+ 1−5000 eV Th 868e + Ti11+ 1−5000 eV Th 868e + Cr13+ 1−5000 eV Th 868e + Fe15+ 1−5000 eV Th 868e + Ni17+ 1−5000 eV Th 868e + Zn19+ 1−5000 eV Th 868e + Fe12+ 1E5−1E8 K Exp 869e + Ne2+ 100−700 K Exp 870e + Ne2+ 100−700 K Exp 870e + H3

+ 10−2000 K Th 871e + CH4 8−12 eV Exp 872e + Ar2+ 3E3−1E4 K Exp 873e + C2H2 threshold−1000 eV Th 874e + C2H4 threshold−1000 eV Th 874e + C3H6 threshold−1000 eV Th 874e + Mg6+ 1E5 K Th 875e + Na6+ 1E5 K Th 875e + Al7+ 1E5 K Th 875e + Na7+ 1E5 K Th 875e + Mg8+ 1E5 K Th 875e + Al9+ 1E5 K Th 875e + Mg9+ 1E5 K Th 875e + Al10+ 1E5 K Th 875e + Si10+ 1E5 K Th 875e + Ti10+ 1E5 K Th 875e + Cr12+ 1E5 K Th 875e + Cr13+ 1E5 K Th 875e + Fe14+ 1E5 K Th 875e + Fe15+ 1E5 K Th 875e + Ni17+ 1E5 K Th 875e + Fe22+ 1E5 K Th 875e + e 0−30 eV Exp 876e + N2H 300−500 K Exp 877e + e+ 300 K Exp 878e + GeH4 6−11 eV Exp 879e + CH4 6−11 eV Exp 879e + SiH4 6−11 eV Exp 879

43

e + e 300 K Exp 880e + CF3 300−600 K E/T 881e + CH2Cl2 0−2.0 eV Th 882e + C2H4Cl2 0−2.0 eV Th 882e + e 0−2.0 eV Th 882e + W28+ 0.1−10000 eV Th 883e + CH3I 5−50 eV Exp 884e + Ar 80−220 eV Exp 885e + Ar17+ (2−28)*threshold, threshold−100 eVTh 886e + Ti21+ (2−28)*threshold, threshold−100 eVTh 886e + Fe25+ (2−28)*threshold, threshold−100 eVTh 886e + Hg (2−28)*threshold, threshold−100 eVTh 886e + Sn4+ 1−1000 eV Th 887e + Sn5+ 1−1000 eV Th 887e + Sn6+ 1−1000 eV Th 887e + Sn7+ 1−1000 eV Th 887e + Sn8+ 1−1000 eV Th 887e + Sn9+ 1−1000 eV Th 887e + Sn10+ 1−1000 eV Th 887e + Sn11+ 1−1000 eV Th 887e + Sn12+ 1−1000 eV Th 887e + Sn13+ 1−1000 eV Th 887e + Y 0−7 eV Th 888e + Ru 0−7 eV Th 888e + Pd 0−7 eV Th 888e + Ag 0−7 eV Th 888e + Pt 0−7 eV Th 888e + CO2 8.2 eV E/T 889e + Ni10+ 0.1−5000 eV Th 890e + S2 threshold−100 eV E/T 891e + Ar 100−500 eV Th 892e+ + Ar 100−500 eV Th 892e + Ar 100−500 eV Th 892e+ + Ar 100−500 eV Th 892e + Fe15+ 300−900 eV Th 893e + C4H4N2O2 0.7−2.3 eV Th 894e + e 0.7−2.3 eV Th 894e + W20+ 0−140 eV Exp 895e + U91+ 63−90 keV E/T 896e + HCN 0−4 eV Th 897e + DCN 0−4 eV Th 897e + H3+ 1E−5−1E0 eV E/T 898e + C3+ threshold Th 899e + Mn 0−1 eV Th 900e + Ni 0−1 eV Th 900e + Cu 0−1 eV Th 900e + Zn 0−1 eV Th 900e + Ag 0−1 eV Th 900e + Cd 0−1 eV Th 900e + Sn12+ 1−1000 eV Th 901e+ + Mg 0.01−100 eV Th 902e + e 0−10 eV Th 903e + HD+ 1E−4−20 eV E/T 904e + H2O 11.3 eV E/T 905e + HeH+ 0.01−1 eV Th 906e + C4H5N3O 60−500 eV E/T 907e + e 60−500 eV E/T 907e + Cl2

+ 1E1−1E5 K Th 908e + H2 200−600 eV Th 909

44

e + N2 200−600 eV Th 909e + e 100−1000 eV E/T 910e + H2O 8.5,9.5 eV Th 911e + H2O 8.5,9.5 eV Th 911e + H2 0−20 eV Exp 912e + D2 0−20 eV Exp 912e + H+ 362,687 eV Exp 913e + D+ 362,687 eV Exp 913e + Cd 0.3−9.0 eV Th 914e + U91+ 63−73.5, 0−31.3 keV Th 915e + Gd63+ 63−73.5, 0−31.3 keV Th 915e + Kr35+ 9.22, 9.24 keV E/T 916e + Ni16+ 1E4.5−1E8 K Th 917e + Si7+ 1E4−1E6.5 K Th 918e + Kr31+ 0−−400 Ryd Th 919e + Fe21+ 0−−400 Ryd Th 919e + Ar13+ 0−−400 Ryd Th 919e + Ne5+ 0−−400 Ryd Th 919e + Mg5+ 10000−200000 K Th 920e + Ne6+ 1E5.8−1E7 K Th 921e + Ni13+ 1E5 1E8 K Th 922e + S2+ 0−2 RYD Th 923e + S15+ 1.4−3.0 keV Exp 924e + S14+ 1.4−3.0 keV Exp 924e + S15+ 1.4−3.0 keV Exp 924e + S14+ 1.4−3.0 keV Exp 924e + Fe10+ 250−1200 eV Exp 925e + Fe9+ 250−1200 eV Exp 925e + Cl2+ 5E3−1E6 K Th 926e + He 1keV Th 927e + He 50, 102eV Th 928e + Ar 37,74,205eV Th 929e + H2 8−18eV Th 930e + Co 0−17eV Th 931e + N2 4−15eV Th 932e + C4H4N2 10−150eV Exp 933e + H2O 250eV Th 934e + H2O 250eV Th 934e + BeH+ 0−24eV Th 935e + H2 0.01−1000eV Exp 936e + H2O 0.01−1000eV Exp 936e + N2O 0.01−1000eV Exp 936e + CO2 0.01−1000eV Exp 936e + Co 0.01−1000eV Exp 936e + O2 0.01−1000eV Exp 936e + H2 0.01−1000eV Exp 936e + H2O 0.01−1000eV Exp 936e + N2O 0.01−1000eV Exp 936e + CO2 0.01−1000eV Exp 936e + Co 0.01−1000eV Exp 936e + O2 0.01−1000eV Exp 936e + H2 0.01−1000eV Exp 936e + H2O 0.01−1000eV Exp 936e + N2O 0.01−1000eV Exp 936e + CO2 0.01−1000eV Exp 936e + Co 0.01−1000eV Exp 936e + O2 0.01−1000eV Exp 936e + C3H3NO 8−3000eV Exp 937e + C3H3NO 8−3000eV Exp 937

45

e + C3H8 0−20eV Exp 938e + C2H6 0−20eV Exp 938e + C2H4 0−20eV Exp 938e + C2H2 0−20eV Exp 938e + CH4 0−20eV Exp 938e + C3H8 0−20eV Exp 938e + C2H6 0−20eV Exp 938e + C2H4 0−20eV Exp 938e + C2H2 0−20eV Exp 938e + CH4 0−20eV Exp 938e + HBr 0.1−2000 eV Th 939e + HCl 0.1−2000 eV Th 939e + Mg+ 100−1000 eV Th 940e + Ne6+ 450−5000 eV Th 941e + Ne5+ 450−5000 eV Th 941e + C2H5OH 0−10 eV Th 942e + C2H5OH 0−10 eV Th 942e + OD+ 20−2500 eV Th 943e + OH+ 20−2500 eV Th 943e + OD+ 20−2500 eV Th 943e + OH+ 20−2500 eV Th 943e + Zn 0.1−1E6 keV Th 944e + Fe 0.1−1E6 keV Th 944e + Cr 0.1−1E6 keV Th 944e + V 0.1−1E6 keV Th 944e + Ti 0.1−1E6 keV Th 944e + Sc 0.1−1E6 keV Th 944e + Si 0.1−1E6 keV Th 944e + Ne 0.1−1E6 keV Th 944e + C 0.1−1E6 keV Th 944e + Bi 0.1−1E6 keV Th 944e + Pb 0.1−1E6 keV Th 944e + Ba 0.1−1E6 keV Th 944e + Xe 0.1−1E6 keV Th 944e + Sb 0.1−1E6 keV Th 944e + Ag 0.1−1E6 keV Th 944e + Kr 0.1−1E6 keV Th 944e + Se 0.1−1E6 keV Th 944e + Sr 0.1−1E6 keV Th 944e + Co 0.1−1E6 keV Th 944e + W(CO)6 0−150eV Exp 945e + NF3 20−500eV E/T 946e + BF 10−2000eV Th 947e + HNC 10−2000eV Th 947e + HCN 10−2000eV Th 947e + C2N2 10−2000eV Th 947e + CN 10−2000eV Th 947e + GeF4 3−200eV Exp 948e + C2H2 1−5000eV Th 949e + C2H4 5−50eV Exp 950e + CH4 10−30eV Th 951e + CH4 10−30eV Th 951e + N2O 0.1−2000eV Th 952e + H2 0−360 Deg. Th 953e + CN 0−10eV Th 954e + CN 0−10eV Th 954e + H2O 0−360 Deg. Th 955e + H2O 0−360 Deg. Th 955e + Al 0−30eV Th 956

46

e + H2O 0−360 Deg. Th 957e + H2O 0−360 Deg. Th 957e + D2 16−3000eV Th 958e + H2 16−3000eV Th 958e + SiF4 1.5−200eV Th 959e + SiF4 1.5−200eV Th 959e + Xe 20−1E4 keV Th 960e + Kr 20−1E4 keV Th 960e + Ar 20−1E4 keV Th 960e + Ne 20−1E4 keV Th 960e + N2 0−360 Deg. Th 961e + N2 0−360 Deg. Th 961e + CN 0.1−4eV Th 962e + H2O 9−20eV Th 963e + He 9eV Th 964e + He 9eV Th 964e + Xe 1−35eV Th 965e + C2H4O 0−300eV E/T 966e + H2 0.01−1000eV Th 967e + Si3+ 0−20E4 K Th 968e + Sc+ 1E1−1E5 K Th 969e + NOCl 200 eV Th 970e + H2 200 eV Th 971e + H2 200 eV Th 971e + H 0−20eV Th 972e + Ag 10−100eV Th 973e + Ag 10−100eV Th 973e + HBr 0.2−1eV Th 974e + HCl 0.2−1eV Th 974e + Li 6−10eV,0−2eV Th 975e + H 6−10eV,0−2eV Th 975e + N2 250eV Exp 976e + N 3000−20000 K Th 977e + C 3000−20000 K Th 977e + Ar 3000−20000 K Th 977e + O 3000−20000 K Th 977e + N 3000−20000 K Th 977e + C 3000−20000 K Th 977e + Ar 3000−20000 K Th 977e + O 3000−20000 K Th 977e + Na 6−60eV Th 978e + BeH+ 1−1E4 eV Th 979e + Li2 5−25eV Th 980e + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVTh 981e + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVTh 981e + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVTh 981e + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVTh 981e + Al2+ 20−200eV Th 982e + Na 5−50eV Th 983e + Ar 5−50eV Th 983e + Ne 5−50eV Th 983e + Na 5−50eV Th 983e + Ar 5−50eV Th 983e + Ne 5−50eV Th 983e + Ar 3−15eV Th 984e + Ar 3−15eV Th 984e + Ar 195eV Th 985e + Ar 195eV Th 985e + N2O 10−25keV Exp 986

47

e + He+ 40−46eV Th 987e + Cd 3−85eV Th 988e + Ne 25eV E/T 989e + NCO 0−10eV,10−5000eV,0−10eV Th 990e + NCO 0−10eV,10−5000eV,0−10eV Th 990e + NCO 0−10eV,10−5000eV,0−10eV Th 990e + He 1keV,100MeV Th 991e + He 1keV,100MeV Th 991e + He 250−2000eV Exp 992e + N2 17.5−100eV Th 993e + C4H4O 0−30eV E/T 994e + C4H4O 0−30eV E/T 994e + C4H4O 0−30eV E/T 994e + He 20−500eV Th 995e + He 20−500eV Th 995e + Ne 0.1−200eV Th 996e + Ne 0.1−200eV Th 996e + Ne 0.1−200eV Th 996e + Ne 0.1−200eV Th 996e + Cs2 0−20eV Th 997e + Fe11+ 300−2500eV Th 998e + C3H3NO 2−20eV Exp 999e + C3H3NO 2−20eV Exp 999e + C3H3NO 2−20eV Exp 999e + Yb 10−100eV Th 1000e + Zn 10−100eV Th 1000e + Yb 10−100eV Th 1000e + Zn 10−100eV Th 1000e + Au49+ 100−10000eV Th 1001e + Au48+ 100−10000eV Th 1001e + Au47+ 100−10000eV Th 1001e + Au46+ 100−10000eV Th 1001e + Au45+ 100−10000eV Th 1001e + Au50+ 100−10000eV Th 1001e + Ne 10−300eV Th 1002e + Ne 10−300eV Th 1002e + B2 300−30000K Th 1003e + B2 300−30000K Th 1003e + B2 300−30000K Th 1003e + Ti 2.5−25keV Exp 1004e + Si 2.5−25keV Exp 1004e + Al 2.5−25keV Exp 1004e + O 2.5−25keV Exp 1004e + C 2.5−25keV Exp 1004e + He 19−24eV,25−60eV Th 1005e + He 19−24eV,25−60eV Th 1005e + C3H6 5.5eV Exp 1006e + C3H6 5.5eV Exp 1006e + H2 18eV Th 1007e + H2 18eV Th 1007e + He 1−1000eV Th 1008e + H 1−1000eV Th 1008e + He 1−1000eV Th 1008e + H 1−1000eV Th 1008e + U 10−1E6eV Th 1009e + Ba2+ 10−1E6eV Th 1009e + Cs+ 10−1E6eV Th 1009e + Xe4+ 10−1E6eV Th 1009e + In 10−1E6eV Th 1009

48

e + Sb+ 10−1E6eV Th 1009e + Bi+ 10−1E6eV Th 1009e + Ag 10−1E6eV Th 1009e + Mo3+ 10−1E6eV Th 1009e + Rb+ 10−1E6eV Th 1009e + Kr4+ 10−1E6eV Th 1009e + Ga 10−1E6eV Th 1009e + Pb 10−1E6eV Th 1009e + Ni3+ 10−1E6eV Th 1009e + Fe6+ 10−1E6eV Th 1009e + Ti5+ 10−1E6eV Th 1009e + Sc+ 10−1E6eV Th 1009e + Hg 10−1E6eV Th 1009e + W6+ 10−1E6eV Th 1009e + Sm6+ 10−1E6eV Th 1009e + Pr3+ 10−1E6eV Th 1009e + S14+ 130−550 RYD Th 1010e + P13+ 130−550 RYD Th 1010e + Al11+ 130−550 RYD Th 1010e + Mg10+ 130−550 RYD Th 1010e + Ca18+ 359−900 RYD Th 1011e + K17+ 359−900 RYD Th 1011e + Cl15+ 359−900 RYD Th 1011e + Sc19+ 359−900 RYD Th 1011e + Mn23+ 500−1200 RYD Th 1012e + Cr22+ 500−1200 RYD Th 1012e + V21+ 500−1200 RYD Th 1012e + Ti20+ 500−1200 RYD Th 1012e + S6+ 20−120 RYD Th 1013e + W44+ 0−50keV Th 1014e + W47+ 0−50keV Th 1014e + W46+ 0−50keV Th 1014e + W45+ 0−50keV Th 1014e + Kr34+ 1E5.4−1E8.1 K Th 1015e + Ti18+ 100−1100 RYD Th 1016e + Co 1−10eV Th 1017e + NO 0.1−100eV Th 1018e + N2 0.1−100eV Th 1018e + S3+ 0.1−1000eV Th 1019e + Zn17+ 0.1−1000eV Th 1019e + Cu16+ 0.1−1000eV Th 1019e + Ni15+ 0.1−1000eV Th 1019e + Co14+ 0.1−1000eV Th 1019e + Mn12+ 0.1−1000eV Th 1019e + Cr11+ 0.1−1000eV Th 1019e + V10+ 0.1−1000eV Th 1019e + Ti9+ 0.1−1000eV Th 1019e + Sc8+ 0.1−1000eV Th 1019e + Ca7+ 0.1−1000eV Th 1019e + K6+ 0.1−1000eV Th 1019e + Ar5+ 0.1−1000eV Th 1019e + Cl4+ 0.1−1000eV Th 1019e + P2+ 0.1−1000eV Th 1019e + Si+ 0.1−1000eV Th 1019e + N2H

+ 10−1000 K Exp 1020e + CH3

+ 1E−1−10eV Exp 1021e + Mg7+ 250−1500eV Exp 1022e + Fe11+ 300−2000eV Exp 1023e + Fe12+ 350−1910eV Exp 1024

49

e + Xe52+ 20−22.4keV Th 1025e + Xe51+ 20−22.4keV Th 1025e + Xe50+ 20−22.4keV Th 1025e + Xe49+ 20−22.4keV Th 1025e + Xe48+ 20−22.4keV Th 1025e + Xe47+ 20−22.4keV Th 1025e + Xe46+ 20−22.4keV Th 1025e + K 6−60eV Th 1026e + Ag+ 50−1000eV Th 1027e + Kr34+ 8−13keV Th 1028e + HBr 0.001−1E4eV Th 1029e + HBr 0.001−1E4eV Th 1029e + HBr 0.001−1E4eV Th 1029e + CF3Cl 300−800K Th 1030e + H2O 300−800K Th 1030e + SF6 1−2eV Th 1031e + NH3 0−20eV Exp 1032e + C2F5 300−600K Exp 1033e + N2

+ 0.001−0.1eV Th 1034e + D3O 0.0001−1eV Exp 1035e + H3O 0.0001−1eV Exp 1035e + ND4

+ 0.0001−1eV Exp 1035e + NH4

+ 0.0001−1eV Exp 1035e + N2D

+ 0.0001−1eV Exp 1035e + N2H

+ 0.0001−1eV Exp 1035e + C4H4N2 3−50eV Exp 1036e + N2 500−600eV Th 1037e + H2 500−600eV Th 1037e + Au20+ 1−1000eV Th 1038e + At 0.01−10eV Th 1039e + Ga 0.01−10eV Th 1039e + Tl 0.01−10eV Th 1039e + In 0.01−10eV Th 1039e + He 110−270eV Th 1040e + He 110−270eV Th 1040e + He 110−270eV Th 1040e + W4+ 0.1−5000eV Th 1041e + Hg 0.1−2000eV Th 1042e + Hg 0.1−2000eV Th 1042e + Hg 0.1−2000eV Th 1042e + U 20−200MeV Th 1043e + Pb 20−200MeV Th 1043e + Zn 20−200MeV Th 1043e + H2O 0.01−1E4eV Th 1044e + Al10+ 0−0.1 RYD Th 1045e + Gd18+ 1−50000eV Th 1046e + Se 0.4-0.8 cm−1 Exp 1047e + W6+ 0.1−575eV Th 1048e + HOC+ 0−10eV Th 1049e + HCO+ 0−10eV Th 1049e + S12+ 500−3000eV Exp 1050e + Gd19+ 1−5000eV Th 1051e + W29+ 1−5000eV Th 1051e + W20+ 1−1000eV E/T 1052e + Hg 1−14eV Th 1053e + Zn 1−14eV Th 1053e + C 1−6eV Exp 1054e + Ta 4−180eV Th 1055e + NO2

+ 0−10eV Th 1056

50

e + CH3+ 0.0001−1eV Th 1057

e + H3O+ 0.0001−1eV Th 1057

e + Au76+ 45eV Exp 1058e + Kr2

+ 300−19000K Exp 1059e + F2

− 0.01−1.4eV Th 1060e + F2 0.01−1.4eV Th 1060e + F2

− 0.01−1.4eV Th 1060e + F2 0.01−1.4eV Th 1060e + H3

+ 0.00001−1000eV Exp 1061e + H3

+ 0.00001−10eV Exp 1062e + Ar 9.5−19.5eV Th 1063e + Fe8+ 0−80 RYD Th 1064e + Fe7+ 0−80 RYD Th 1064e + Fe9+ 10−60 RYD Th 1065e + Fe11+ 10−60 RYD Th 1066e + Fe12+ 10−50 RYD Th 1067e + PH3 10−5000eV Th 1068e + SiH4 10−5000eV Th 1068e + CH3F 1E2−2E3 eV Th 1069e + CH2F2 1E2−2E3 eV Th 1069e + CF3H 1E2−2E3 eV Th 1069e + CF4 1E2−2E3 eV Th 1069e + C6H6 20−500eV Th 1070e + Ar 40−1000Td Th 1071e + He 20−1000eV Th 1072e + He 20−1000eV Th 1072e + He 20−1000eV Th 1072e + He 20−1000eV Th 1072e + C4H4N2 15−30eV Exp 1073e + C4H4N2 15−30eV Exp 1073e + C4H4N2 15−30eV Exp 1073e + Xe 0.005−20eV Exp 1074e + Kr 0.005−20eV Exp 1074e + Ar 0.005−20eV Exp 1074e + Xe 0.005−20eV Exp 1074e + Kr 0.005−20eV Exp 1074e + Ar 0.005−20eV Exp 1074e + C2H5OH 1−1000eV E/T 1075e + CH3OH 1−1000eV E/T 1075e + HCN 0.1−10000eV Th 1076e + HCN 0.1−10000eV Th 1076e + He 0.1−1000eV Th 1077e + HeH2+ 10−150eV Th 1078e + H2

+ 10−150eV Th 1078e + Si 0−60eV Th 1079e + Si 0−60eV Th 1079e + Si 0−60eV Th 1079e + Xe 500,750eV E/T 1080e + C3H7NO2 0−8eV Th 1081e + C2H5NO2 0−8eV Th 1081e + C2H3NO2 0−8eV Th 1081e + SO2 0.1−2000eV Th 1082e + U91+ 100−120eV Th 1083e + Ar Th 1084e + Kr34+ 1000−3500eV Th 1085e + Ne 0.5−50eV E/T 1086e + CH4 0.5−50eV E/T 1086e + CF3Cl 0−2.5 eV Th 1087e + CF2Cl2 0−2.5 eV Th 1087

51

e + CH4 10−20eV E/T 1088e + CH4 10−20eV E/T 1088e + CF3Br 100−20000K Th 1089e + C3F5 300−550K Exp 1090e + C2F3 300−550K Exp 1090e + CF2 300−550K Exp 1090e + Xe 5−40eV Exp 1091e + Xe 5−40eV Exp 1091e + C4 0−220 eV E/T 1092e + C2 0−220 eV E/T 1092e + He 100−600eV Th 1093e + W2+ 10−1000 eV Th 1094e + W+ 10−1000 eV Th 1094e + H2

+ 0−1000eV Th 1095e + Ni10+ 0−450eV Th 1096e + D2 178 eV E/T 1097e + D2 178 eV E/T 1097e + H2 0−100eV Th 1098e + Fe 5−2000eV Th 1099e + Ti 5−2000eV Th 1099e + B 5−2000eV Th 1099e + Be 5−2000eV Th 1099e + Li 5−2000eV Th 1099e + O5+ 1−140 RYD Th 1100e + O4+ 1−140 RYD Th 1100e + H 1E−6−10 A.U. Th 1101e + He+ 40−1000eV Th 1102e + C5+ 40−1000eV Th 1102e + C3+ 40−1000eV Th 1102e + Ni 50 eV Exp 1103e + Rb 0−400eV Th 1104e + GeO 45−55eV Exp 1105e + HfO 45−55eV Exp 1105e + YO 45−55eV Exp 1105e + VO2 45−55eV Exp 1105e + VO 45−55eV Exp 1105e + TiO2 45−55eV Exp 1105e + TiO 45−55eV Exp 1105e + Ne 20−300eV Exp 1106e + Li 10−600eV Exp 1107e + Cs 10−600eV Exp 1107e + Rb 10−600eV Exp 1107e + K 10−600eV Exp 1107e + Na 10−600eV Exp 1107e + Li 10−600eV Exp 1107e + Cs 10−600eV Exp 1107e + Rb 10−600eV Exp 1107e + K 10−600eV Exp 1107e + Na 10−600eV Exp 1107e + Xe12+ 100−1000eV Th 1108e + Xe11+ 100−1000eV Th 1108e + Xe17+ 100−1000eV Th 1108e + Xe10+ 100−1000eV Th 1108e + Xe16+ 100−1000eV Th 1108e + Xe15+ 100−1000eV Th 1108e + Xe14+ 100−1000eV Th 1108e + Xe13+ 100−1000eV Th 1108e + CN 0−1000 K Th 1109e + Kr2 0−2000eV Th 1110

52

e + He2 0−2000eV Th 1110e + Ar2 0−2000eV Th 1110e + Ne2 0−2000eV Th 1110e + He2 0−2000eV Th 1110e + Kr2 0−2000eV Th 1110e + Ar2 0−2000eV Th 1110e + Ne2 0−2000eV Th 1110e + C3H8 10−10000eV Th 1111e + N2 10−10000eV Th 1111e + N+ 10−10000eV E/T 1112e + C+ 10−10000eV E/T 1112e + O+ 10−10000eV E/T 1112e + H2O 50−500eV Th 1113e + Ne 20−300eV Exp 1114e + He 5.5−570eV Th 1115e + He 5.5−570eV Th 1115e + He 645−676eV Th 1116e + He 645−676eV Th 1116e + Ne4+ 0−2.5 RYD Th 1117e + Au 0−1E8 keV Th 1118e + Ne8+ 0−1E8 keV Th 1118e + Ne7+ 0−1E8 keV Th 1118e + Be+ 0−1E8 keV Th 1118e + Li+ 0−1E8 keV Th 1118e + Ag 0−1E8 keV Th 1118e + Ne6+ 0−1E8 keV Th 1118e + O6+ 0−1E8 keV Th 1118e + Li 0−1E8 keV Th 1118e + He+ 0−1E8 keV Th 1118e + Cu 0−1E8 keV Th 1118e + O4+ 0−1E8 keV Th 1118e + N6+ 0−1E8 keV Th 1118e + He 0−1E8 keV Th 1118e + H 0−1E8 keV Th 1118e + Ar 0−1E8 keV Th 1118e + N4+ 0−1E8 keV Th 1118e + N3+ 0−1E8 keV Th 1118e + U90+ 0−1E8 keV Th 1118e + U91+ 0−1E8 keV Th 1118e + C4+ 0−1E8 keV Th 1118e + C2+ 0−1E8 keV Th 1118e + U89+ 0−1E8 keV Th 1118e + U88+ 0−1E8 keV Th 1118e + C 0−1E8 keV Th 1118e + B4+ 0−1E8 keV Th 1118e + U 0−1E8 keV Th 1118e + Mo41+ 0−1E8 keV Th 1118e + B2+ 0−1E8 keV Th 1118e + B+ 0−1E8 keV Th 1118e + Xe 540eV Th 1119e + Mo 540eV Th 1119e + Ca 540eV Th 1119e + NF3 1−5keV Th 1120e + NF3 1−5keV Th 1120e + Co 0−1000 Td Th 1121e + In+ 0−120eV Exp 1122e + Sn7+ 0−1000eV E/T 1123e + Sn13+ 0−1000eV E/T 1123e + Sn6+ 0−1000eV E/T 1123

53

e + Sn12+ 0−1000eV E/T 1123e + Sn5+ 0−1000eV E/T 1123e + Sn11+ 0−1000eV E/T 1123e + Sn4+ 0−1000eV E/T 1123e + Sn10+ 0−1000eV E/T 1123e + Sn9+ 0−1000eV E/T 1123e + Sn8+ 0−1000eV E/T 1123e + I 0−10eV Th 1124e + Ar 0−10eV Th 1124e + Ne 0−10eV Th 1124e + He 0−10eV Th 1124e + He 0−10eV Th 1124e + Hg 0−10eV Th 1124e + Kr 0−10eV Th 1124e + I 0−10eV Th 1124e + Ar 0−10eV Th 1124e + Ne 0−10eV Th 1124e + He 0−10eV Th 1124e + Hg 0−10eV Th 1124e + Kr 0−10eV Th 1124e + I 0−10eV Th 1124e + Ar 0−10eV Th 1124e + Ne 0−10eV Th 1124e + Hg 0−10eV Th 1124e + He 0−10eV Th 1124e + Hg 0−10eV Th 1124e + Kr 0−10eV Th 1124e + Kr 0−10eV Th 1124e + I 0−10eV Th 1124e + Ar 0−10eV Th 1124e + Ne 0−10eV Th 1124e + Ar6+ 0−1000keV Th 1125e + Ar5+ 0−1000keV Th 1125e + Ar4+ 0−1000keV Th 1125e + Ar3+ 0−1000keV Th 1125e + Ar2+ 0−1000keV Th 1125e + Ar7+ 0−1000keV Th 1125e + CH3I 20−5000 eV Th 1126e + CH3Br 20−5000 eV Th 1126e + CH3Cl 20−5000 eV Th 1126e + CH3F 20−5000 eV Th 1126e + Mg8+ 1E4−1E7 K Th 1127e + S12+ 1E4−1E8 K Th 1128e + N2 0−40 eV Th 1129e + N2 0−40 eV Th 1129e + H 250eV Th 1130e + He 64−600eV Th 1131e + U91+ 0−160eV Th 1132e + Xe53+ 0−160eV Th 1132e + Ni27+ 0−160eV Th 1132e + O2 30−400eV Exp 1133e + H2O 0−30eV Th 1134e + Ar 4−200eV Th 1135e + Ne 4−200eV Th 1135e + N2 550−600eV Th 1136e + He 550−600eV Th 1136e + H2 550−600eV Th 1136e + H2 20−30eV Th 1137e + H2 20−30eV Th 1137

54

e + Ni22+ 100−500 RYD Th 1138e + U89+ 0−150 keV Th 1139e + Xe51+ 0−150 keV Th 1139e + H2O 9−20eV E/T 1140e + Pb 3−38keV E/T 1141e + H2O 52−107eV Th 1142e + Xe 20−40eV Th 1143e + Ar 200eV E/T 1144e + Xe 2−500eV Th 1145e + Kr 2−500eV Th 1145e + Ar 2−500eV Th 1145e + Ne 2−500eV Th 1145e + He 2−500eV Th 1145e + Xe 2−500eV Th 1145e + Kr 2−500eV Th 1145e + Ar 2−500eV Th 1145e + Ne 2−500eV Th 1145e + He 2−500eV Th 1145e + Xe 2−500eV Th 1145e + Kr 2−500eV Th 1145e + Ar 2−500eV Th 1145e + Ne 2−500eV Th 1145e + He 2−500eV Th 1145e + PO2 0−10eV Th 1146e + PO2 0−10eV Th 1146e + PO2 0−10eV Th 1146e + PO2 0−10eV Th 1146e + C3H4 0.1−2000eV Th 1147e + Ho63+ 0−5 TH Th 1148e + Mo38+ 0−5 TH Th 1148e + U88+ 0−5 TH Th 1148e + SO2 0−200eV Exp 1149e + Zn18+ 700−1300 RYD Th 1150e + Cu17+ 700−1300 RYD Th 1150e + Ni16+ 700−1300 RYD Th 1150e + Co15+ 700−1300 RYD Th 1150e + Fe14+ 700−1300 RYD Th 1150e + He 500−5600eV Th 1151e + Fe17+ 0−3000eV Th 1152e + Fe16+ 0−3000eV Th 1152e + Fe13+ 0−3000eV Th 1152e + Ne 100eV E/T 1153e + Gd 0−200eV E/T 1154e + O2 0−18eV Th 1155e + As31+ 1E5.2−1E7.7 K Th 1156e + Ge30+ 1E5.2−1E7.7 K Th 1156e + Ga29+ 1E5.2−1E7.7 K Th 1156e + Br33+ 1E5.2−1E7.7 K Th 1156e + Se32+ 1E5.2−1E7.7 K Th 1156e + W3+ 0−100eV Th 1157e + W3+ 0−100eV Th 1157e + U91+ 0−500keV Th 1158e + Bi80+ 0−500keV Th 1158e + Xe53+ 0−500keV Th 1158e + Er67+ 0−500keV Th 1158e + Ni27+ 0−500keV Th 1158e + Ca17+ 1E4.5−1E7.5 K Th 1159e + K16+ 1E4.5−1E7.5 K Th 1159e + Ar15+ 1E4.5−1E7.5 K Th 1159

55

e + Cl14+ 1E4.5−1E7.5 K Th 1159e + S13+ 1E4.5−1E7.5 K Th 1159e + P12+ 1E4.5−1E7.5 K Th 1159e + Al10+ 1E4.5−1E7.5 K Th 1159e + Mg9+ 1E4.5−1E7.5 K Th 1159e + BF3 0.1−200eV Th 1160e + BF3 0.1−200eV Th 1160e + BeH+ 0.001−3eV Th 1161e + He 1.2−200eV Th 1162e + Xe 1.2−200eV Th 1162e + Kr 1.2−200eV Th 1162e + Ne 1.2−200eV Th 1162e + C 0−60eV Th 1163e + C4+ 20−130eV Th 1164e + C3+ 20−130eV Th 1164e + C4+ 20−130eV Th 1164e + C3+ 20−130eV Th 1164e + Pb 9−10eV Th 1165e + Cl 0.01−100eV Th 1166e + Cl 0.01−100eV Th 1166e + Co 2−10eV Th 1167e + H2O 10−25keV Exp 1168e + He 100−300eV Exp 1169e + H2 9.2−3000eV Th 1170e + H2 9.2−3000eV Th 1170e + BeH 1−1000eV Th 1171e + CH3Br 13−1000eV Th 1172e + CH3Cl 13−1000eV Th 1172e + CH3F 13−1000eV Th 1172e + Rb 15−50eV E/T 1173e + C 0−100eV Th 1174e + C 0−100eV Th 1174e + C 0−100eV Th 1174e + CH3OH 0.1−2000eV Th 1175e + CH3OH 0.1−2000eV Th 1175e + CH3OH 0.1−2000eV Th 1175e + CH3OH 0.1−2000eV Th 1175e + CH4 200−250 eV Exp 1176e + H2 200−250 eV Exp 1176e + Ar 200−250 eV Exp 1176e + He 200−250 eV Exp 1176e + Co3+ 3−5 RYD Th 1177e + He 1−8eV Th 1178e + Be2H4 0−1000eV Th 1179e + Be2H2 0−1000eV Th 1179e + BeH2 0−1000eV Th 1179e + BeH 0−1000eV Th 1179e + Be 0−1000eV Th 1179e + Si2C 10−2000eV Th 1180e + SiC2 10−2000eV Th 1180e + SiC 10−2000eV Th 1180e + Si3 10−2000eV Th 1180e + Si2 10−2000eV Th 1180e + C3 10−2000eV Th 1180e + C2 10−2000eV Th 1180e + Pb 5−30keV Exp 1181e + C4H6 1000 eV E/T 1182e + OCS 1.2−200eV E/T 1183e + Cs2 1.2−200eV E/T 1183

56

e + NO2 1−1000eV Exp 1184e + C2H2 1−1000eV E/T 1185e + C2H2 1−1000eV E/T 1185e + CF3 7−50eV E/T 1186e + Ne 300−2500eV E/T 1187e + He 56−60eV E/T 1188e + He 56−60eV E/T 1188e + Fe10+ 1E5−1E7 K Th 1189e + Mn 0−25eV Th 1190e + Mn 0−25eV Th 1190e + CF3Br 300−890K Exp 1191e + CF3 300−890K Exp 1191e + HCOOH 1−3.5eV Exp 1192e + CH4 11−28eV E/T 1193e + NH3 11−28eV E/T 1193e + CH4 11−28eV E/T 1193e + NH3 11−28eV E/T 1193e + HCl+ 1E−5−5eV Exp 1194e + C+ 1E3−1E4.8 K Th 1195e + Mg 10−60eV Th 1196e + Na 10−60eV Th 1196e + SF6 0.−3000eV Exp 1197e + CO2 10−30eV Th 1198e + N2

+ 0.001−1eV Th 1199e + W42+ 100−10000eV Th 1200e + W41+ 100−10000eV Th 1200e + W46+ 100−10000eV Th 1200e + W45+ 100−10000eV Th 1200e + W44+ 100−10000eV Th 1200e + W436+ 100−10000eV Th 1200e + W42+ 100−10000eV Th 1200e + W41+ 100−10000eV Th 1200e + W46+ 100−10000eV Th 1200e + W45+ 100−10000eV Th 1200e + W44+ 100−10000eV Th 1200e + W436+ 100−10000eV Th 1200e + K35+ E/T 1201e + C3+ 0.01−30eV Th 1202e + H2O 1−100eV Exp 1203e + HD+ 0−14eV Th 1204e + H2

+ 0−14eV Th 1204e + LiHe+ 0.02−500eV Th 1205e + HCl+ 1E−5−4.06eV Exp 1206e + H2 9.2−3000eV Th 1207e + He 200eV Exp 1208e + CH4 25−300eV Exp 1209e + Fe8+ 1E5−1E6.4 K Th 1210e + Fe7+ 1E5−1E6.4 K Th 1211e + Ni14+ 1E5.6−1E6.7 K Th 1212e + Ni10+ 1E5−1E7 K Th 1213e + Mg7+ 1E4−1E7 K Th 1214e + Ne6+ 1−1E9 K Th 1215e + C2+ 1−1E9 K Th 1215e + Fe22+ 1−1E9 K Th 1215e + Mg8+ 1−1E9 K Th 1215e + S12+ 0−150 RYD Th 1216e + Sn− 0−10eV Exp 1217e + U88+ 0−1E5 eV Th 1218e + Xe50+ 0−1E5 eV Th 1218

57

e + Ca8+ 0−60 RYD Th 1219e + CH4 300−350eV E/T 1220e + Co 0−1000 Td Th 1221e + PH3 14−1000eV Th 1222e + Ne 20−300eV Th 1223e + CF3 7−50eV E/T 1224e + O5+ 8−17eV Th 1225e + N4+ 8−17eV Th 1225e + C3+ 8−17eV Th 1225e + Xe 0−200eV Th 1226e + Fe24+ 0−100 eV Th 1227e + Ar 50−200eV Th 1228e + Ne 50−200eV Th 1228e + SO2 0−3000eV Th 1229e + SO 0−3000eV Th 1229e + Bi 9−40 keV Exp 1230e + Pb 9−40 keV Exp 1230e + Fr Th 1231e + Cs Th 1231e + Rb Th 1231e + K Th 1231e + Na Th 1231e + Li Th 1231e + Ar 2−10eV Th 1232e + Mg 3−10eV Th 1233e + H2 20−30eV Th 1234e + H2 20−30eV Th 1234e + U88+ 0−5eV Th 1235e + Ho63+ 0−5eV Th 1235e + Mo38+ 0−5eV Th 1235e + O2 E/T 1236e + Ni20+ 1E6.4−1E7.4 Th 1237e + Au− Th 1238e + Ag− Th 1238e + Cu− Th 1238e + Fr− Th 1238e + Cs− Th 1238e + Rb− Th 1238e + K− Th 1238e + Na− Th 1238e + Li− Th 1238e + H− Th 1238e + C2H6 0.01−100eV Th 1239e + C2H4 0.01−100eV Th 1239e + CH4 0.01−100eV Th 1239e + C-C4F8 0.01−100eV Th 1239e + C3F8 0.01−100eV Th 1239e + CF3I 0.01−100eV Th 1239e + CF3Cl 0.01−100eV Th 1239e + C2F6 0.01−100eV Th 1239e + Si2H6 0.1−100eV E/T 1240e + CF4 0.1−100eV E/T 1240e + CCl4 0.1−100eV E/T 1240e + H2O 0.1−100eV E/T 1240e + HCl 0.1−100eV E/T 1240e + BCl3 0.1−100eV E/T 1240e + BF3 0.1−100eV E/T 1240e + CO2 0.1−100eV E/T 1240e + NO 0.1−100eV E/T 1240

58

e + CF3Br 0.1−100eV E/T 1240e + CH4 0.1−100eV E/T 1240e + WF6 0.1−100eV E/T 1240e + H2O 0.1−100eV E/T 1240e + CH3Br 0.1−100eV E/T 1240e + CCl2F2 0.1−100eV E/T 1240e + SF6 0.1−100eV E/T 1240e + C2F6 0.1−100eV E/T 1240e + HCl 0.1−100eV E/T 1240e + BCl3 0.1−100eV E/T 1240e + BF3 0.1−100eV E/T 1240e + Si2H6 0.1−100eV E/T 1240e + CF4 0.1−100eV E/T 1240e + CCl4 0.1−100eV E/T 1240e + CH4 0.1−100eV E/T 1240e + CO2 0.1−100eV E/T 1240e + NO 0.1−100eV E/T 1240e + CF3Br 0.1−100eV E/T 1240e + WF6 0.1−100eV E/T 1240e + H2O 0.1−100eV E/T 1240e + HCl 0.1−100eV E/T 1240e + BCl3 0.1−100eV E/T 1240e + CH3Br 0.1−100eV E/T 1240e + CCl2F2 0.1−100eV E/T 1240e + SF6 0.1−100eV E/T 1240e + BF3 0.1−100eV E/T 1240e + CO2 0.1−100eV E/T 1240e + NO 0.1−100eV E/T 1240e + CF3Br 0.1−100eV E/T 1240e + C2F6 0.1−100eV E/T 1240e + Si2H6 0.1−100eV E/T 1240e + CF4 0.1−100eV E/T 1240e + CH3Br 0.1−100eV E/T 1240e + CCl2F2 0.1−100eV E/T 1240e + SF6 0.1−100eV E/T 1240e + C2F6 0.1−100eV E/T 1240e + CCl4 0.1−100eV E/T 1240e + CH4 0.1−100eV E/T 1240e + WF6 0.1−100eV E/T 1240e + Ar15+ 800−1200eV Th 1241e + Fe16+ 800−1200eV Th 1241e + Ar4+ 10eV−5E3keV Th 1242e + Kr5+ 10eV−5E3keV Th 1242e + Kr+ 10eV−5E3keV Th 1242e + Fe 10eV−5E3keV Th 1242e + Ar 10eV−5E3keV Th 1242e + Ar3+ 10eV−5E3keV Th 1242e + Kr 10eV−5E3keV Th 1242e + Ar2+ 10eV−5E3keV Th 1242e + Kr17+ 10eV−5E3keV Th 1242e + Kr15+ 10eV−5E3keV Th 1242e + Fe13+ 10eV−5E3keV Th 1242e + Fe11+ 10eV−5E3keV Th 1242e + Fe9+ 10eV−5E3keV Th 1242e + Fe6+ 10eV−5E3keV Th 1242e + Kr10+ 10eV−5E3keV Th 1242e + Fe5+ 10eV−5E3keV Th 1242e + Fe2+ 10eV−5E3keV Th 1242e + Ar7+ 10eV−5E3keV Th 1242

59

e + Ar6+ 10eV−5E3keV Th 1242e + Ar5+ 10eV−5E3keV Th 1242e + Kr6+ 10eV−5E3keV Th 1242e + CF4 10−1000 eV Exp 1243e + CHF3 10−1000 eV Exp 1243e + CH2F2 10−1000 eV Exp 1243e + CH3F 10−1000 eV Exp 1243e + CF2Cl2 0−4E19 mole/cm3 Exp 1244e + CH3Br 330−1100 K Exp 1245e + CH2O 85eV Th 1246e + C60 Exp 1247e + N2

+ 100−3000 K Th 1248e + Pt 5−1E6 keV Th 1249e + Os 5−1E6 keV Th 1249e + Re 5−1E6 keV Th 1249e + Hf 5−1E6 keV Th 1249e + Dy 5−1E6 keV Th 1249e + I 5−1E6 keV Th 1249e + U 5−1E6 keV Th 1249e + Pb 5−1E6 keV Th 1249e + Au 5−1E6 keV Th 1249e + W 5−1E6 keV Th 1249e + Ta 5−1E6 keV Th 1249e + Y 5−1E6 keV Th 1249e + Tm 5−1E6 keV Th 1249e + Er 5−1E6 keV Th 1249e + Ho 5−1E6 keV Th 1249e + Gd 5−1E6 keV Th 1249e + Eu 5−1E6 keV Th 1249e + Sm 5−1E6 keV Th 1249e + Nd 5−1E6 keV Th 1249e + Pr 5−1E6 keV Th 1249e + Ce 5−1E6 keV Th 1249e + La 5−1E6 keV Th 1249e + Te 5−1E6 keV Th 1249e + Xe 5−1E6 keV Th 1249e + Sb 5−1E6 keV Th 1249e + Sn 5−1E6 keV Th 1249e + In 5−1E6 keV Th 1249e + Cd 5−1E6 keV Th 1249e + Pd 5−1E6 keV Th 1249e + Mo 5−1E6 keV Th 1249e + Nb 5−1E6 keV Th 1249e + Zr 5−1E6 keV Th 1249e + Sr 5−1E6 keV Th 1249e + Rb 5−1E6 keV Th 1249e + Kr 5−1E6 keV Th 1249e + Br 5−1E6 keV Th 1249e + Se 5−1E6 keV Th 1249e + As 5−1E6 keV Th 1249e + Ge 5−1E6 keV Th 1249e + Ga 5−1E6 keV Th 1249e + Zn 5−1E6 keV Th 1249e + Cu 5−1E6 keV Th 1249e + Ni 5−1E6 keV Th 1249e + Co 5−1E6 keV Th 1249e + Mn 5−1E6 keV Th 1249e + Cr 5−1E6 keV Th 1249e + V 5−1E6 keV Th 1249

60

e + Ti 5−1E6 keV Th 1249e + Sc 5−1E6 keV Th 1249e + Ca 5−1E6 keV Th 1249e + K 5−1E6 keV Th 1249e + Ar 5−1E6 keV Th 1249e + Cl 5−1E6 keV Th 1249e + S 5−1E6 keV Th 1249e + Al 5−1E6 keV Th 1249e + Mg 5−1E6 keV Th 1249e + Na 5−1E6 keV Th 1249e + O 5−1E6 keV Th 1249e + H 5−1E6 keV Th 1249e + C 5−1E6 keV Th 1249e + Bi 5−1E6 keV Th 1249e + Ag 5−1E6 keV Th 1249e + Fe 5−1E6 keV Th 1249e + Si 5−1E6 keV Th 1249e + N 5−1E6 keV Th 1249e + Ne 20−300eV Exp 1250e + O2 30−400eV Exp 1251e + CFCl3 1.5−100eV E/T 1252e + CF2Cl2 1.5−100eV E/T 1252e + CF3Cl 1.5−100eV E/T 1252e + CH3I 20−5000eV Th 1253e + CH3Br 20−5000eV Th 1253e + CH3Cl 20−5000eV Th 1253e + CH3F 20−5000eV Th 1253e + CH3F 15−500eV Th 1254e + CHCl3 20−5000eV Th 1255e + CH2Cl2 20−5000eV Th 1255e + Cl2O 0.1−2000eV Th 1256e + N2D

+ 5−3000eV Exp 1257e + N2H

+ 5−3000eV Exp 1257e + Pb 3−38keV E/T 1258e + Rb 15−50eV E/T 1259e + W3+ 0.2−100eV Th 1260e + W3+ 0.2−100eV Th 1260e + CF3 7−50eV Exp 1261e + Na 30−400eV Exp 1262e + Sn13+ 40−1000eV Exp 1263e + Sn12+ 40−1000eV Exp 1263e + Sn11+ 40−1000eV Exp 1263e + Sn10+ 40−1000eV Exp 1263e + Sn9+ 40−1000eV Exp 1263e + Sn8+ 40−1000eV Exp 1263e + Sn7+ 40−1000eV Exp 1263e + Sn6+ 40−1000eV Exp 1263e + Sn5+ 40−1000eV Exp 1263e + Sn4+ 40−1000eV Exp 1263e + HeH+ 10−3000eV Exp 1264e + Ge+ 0−200eV Exp 1265e + U 4−40keV Exp 1266e + Bi 80−100keV Exp 1267e + Au 80−100keV Exp 1267e + Se3+ 30−1000eV Exp 1268e + Se2+ 30−500eV Exp 1269e + Ar 0.1−10keV Th 1270e + Ne 0.1−10keV Th 1270e + Xe 0.1−10keV Th 1270

61

e + Kr 0.1−10keV Th 1270e + CH4 500eV E/T 1271e + Ne 500eV E/T 1271e + Xe 0.01−400eV E/T 1272e + Kr 0.01−400eV E/T 1272e + Xe 0.01−400eV E/T 1272e + Kr 0.01−400eV E/T 1272e + Xe 0.01−400eV E/T 1272e + Kr 0.01−400eV E/T 1272e + Xe 0.01−400eV E/T 1272e + Kr 0.01−400eV E/T 1272e + He 20−1000eV E/T 1273e + Ne 20−1000eV E/T 1273e + He 20−1000eV E/T 1273e + Ne 20−1000eV E/T 1273e + He 20−1000eV E/T 1273e + Ne 20−1000eV E/T 1273e + He 20−1000eV E/T 1273e + Ne 20−1000eV E/T 1273e + Ar 0.01−200eV E/T 1274e + Ar 0.01−200eV E/T 1274e + Ar 0.01−200eV E/T 1274e + W46+ 0−12 keV Th 1275e + W45+ 0−12 keV Th 1275e + W44+ 0−12 keV Th 1275e + W43+ 0−12 keV Th 1275e + W42+ 0−12 keV Th 1275e + Ne 0.06−20eV Exp 1276e + He 0.06−20eV Exp 1276e + Cd+ 20−200eV Th 1277e + N5+ 100−1000eV Exp 1278e + Fe14+ 0.5−1000eV Exp 1279e + Fe14+ 0.5−1000eV Exp 1279e + LiH2

+ 0.001−20eV E/T 1280e + W5+ 50−10000eV Th 1281e + Ar2+ 50−10000eV Th 1281e + C+ 50−10000eV Th 1281e + O3+ 50−10000eV Th 1281e + O2+ 50−10000eV Th 1281e + O+ 50−10000eV Th 1281e + Ar 200 eV E/T 1282e + H2O 0−50eV Th 1283e + CH4 500 eV Th 1284e + Mg 10−25eV Th 1285e + H 25−250eV Th 1286e + Cs 7−12eV Th 1287e + Ar 195eV E/T 1288e + CH3CHO 1−50eV E/T 1289e + Kr+ 0−5eV Th 1290e + H2O 4−40eV Th 1291e + N2 0.088−10 A.U. Th 1292e + O− 0.088−10 A.U. Th 1292e + CN− 0.088−10 A.U. Th 1292e + HD+ 0−1000eV Th 1293e + T2

+ 0−1000eV Th 1293e + D2

+ 0−1000eV Th 1293e + H2

+ 0−1000eV Th 1293e + T2

+ 0−1000eV Th 1293e + D2

+ 0−1000eV Th 1293

62

e + H2+ 0−1000eV Th 1293

e + He+ 0−1000eV Th 1293e + D2

+ 0−1000eV Th 1293e + H2

+ 0−1000eV Th 1293e + He+ 0−1000eV Th 1293e + H2

+ 0−1000eV Th 1293e + He+ 0−1000eV Th 1293e + HT+ 0−1000eV Th 1293e + He+ 0−1000eV Th 1293e + HT+ 0−1000eV Th 1293e + HD+ 0−1000eV Th 1293e + HT+ 0−1000eV Th 1293e + HD+ 0−1000eV Th 1293e + T2

+ 0−1000eV Th 1293e + HT+ 0−1000eV Th 1293e + HD+ 0−1000eV Th 1293e + T2

+ 0−1000eV Th 1293e + D2

+ 0−1000eV Th 1293e + Br33+ 900−2100 RYD Th 1294e + Se32+ 900−2100 RYD Th 1294e + As31+ 900−2100 RYD Th 1294e + Ge30+ 900−2100 RYD Th 1294e + Ga29+ 900−2100 RYD Th 1294e + C3H4 0.1−2000eV Th 1295e + C 0−100eV Th 1296e + C 0−100eV Th 1296e + C 0−100eV Th 1296e + C 0−100eV Th 1296e + CH3OH 0.1−2000eV Th 1297e + CH3OH 0.1−2000eV Th 1297e + CH3OH 0.1−2000eV Th 1297e + Ar16+ 1−1000eV Th 1298e + Ne8+ 1−1000eV Th 1298e + O6+ 1−1000eV Th 1298e + N5+ 1−1000eV Th 1298e + C4+ 1−1000eV Th 1298e + B3+ 1−1000eV Th 1298e + Li+ 1−1000eV Th 1298e + He 1−1000eV Th 1298e + H2

+ 0−1000eV Th 1299e + D2 178eV E/T 1300e + D2 178eV E/T 1300e + H2 0−100eV Th 1301e + U 0−160 keV Th 1302e + Xe 0−160 keV Th 1302e + Ni 0−160 keV Th 1302e + H2O 9−20eV Th 1303e + Al12+ 100 eV Th 1304e + Ar 0.01−300eV Th 1305e + Ar 0.01−300eV Th 1305e + Ar 0.01−300eV Th 1305e + U 0−1000eV Th 1306e + N 0.01−140eV Th 1307e + N 0.01−140eV Th 1307e + N 0.01−140eV Th 1307e + F 0.01−120eV Th 1308e + F 0.01−120eV Th 1308e + F 0.01−120eV Th 1308e + Sn13+ 0−4000eV Th 1309

63

e + Sn13+ 0−4000eV Th 1309e + N2

+ 0.1−1eV Th 1310e + Si9+ 1330−1550eV E/T 1311e + Si8+ 1330−1550eV E/T 1311e + Si7+ 1330−1550eV E/T 1311e + Si6+ 1330−1550eV E/T 1311e + Si12+ 1330−1550eV E/T 1311e + Si11+ 1330−1550eV E/T 1311e + Si10+ 1330−1550eV E/T 1311e + HDO+ 10−2500eV Exp 1312e + Bi79+ Th 1313e + Ho53+ Th 1313e + Ag43+ Th 1313e + W39+ 1−50000eV Th 1314e + N2 0−22eV Th 1315e + O2 0−100eV Th 1316e + BeH 0−1000eV Th 1317e + N2 0−100eV Th 1318e + N2 0−100eV Th 1318e + SF6 0.1−5000eV Th 1319e + SF6 0.1−5000eV Th 1319e + S 0−10eV Exp 1320e + NH+ 1.71E−5−2EeV Exp 1321e + Fe6+ 0.01−40eV Th 1322e + Fe2+ 1E3−1E5 K Th 1323e + Zn15+ 1E4−1E7 K Th 1324e + Cu14+ 1E4−1E7 K Th 1324e + Ni13+ 1E4−1E7 K Th 1324e + Co12+ 1E4−1E7 K Th 1324e + Fe11+ 1E4−1E7 K Th 1324e + Mn10+ 1E4−1E7 K Th 1324e + Cr9+ 1E4−1E7 K Th 1324e + V8+ 1E4−1E7 K Th 1324e + Ti7+ 1E4−1E7 K Th 1324e + Sc6+ 1E4−1E7 K Th 1324e + Ca5+ 1E4−1E7 K Th 1324e + K4+ 1E4−1E7 K Th 1324e + Ar3+ 1E4−1E7 K Th 1324e + Cl2+ 1E4−1E7 K Th 1324e + P+ 1E4−1E7 K Th 1324e + S+ 1E4−1E7 K Th 1324e + Ar 0.01−1000eV Th 1325e + Xe 0.01−1000eV Th 1325e + Xe 0.01−1000eV Th 1325e + Kr 0.01−1000eV Th 1325e + Kr 0.01−1000eV Th 1325e + Ar 0.01−1000eV Th 1325e + Ar 0.01−1000eV Th 1325e + Xe 0.01−1000eV Th 1325e + Xe 0.01−1000eV Th 1325e + Kr 0.01−1000eV Th 1325e + Kr 0.01−1000eV Th 1325e + Ar 0.01−1000eV Th 1325e + BF3 0−10eV Th 1326e + H2O 2−20eV Th 1327e + H2O 30−100eV Th 1328e + Zn28+ 450−1300 RYD Th 1329e + Cu27+ 450−1300 RYD Th 1329e + Ni26+ 450−1300 RYD Th 1329

64

e + Co25+ 450−1300 RYD Th 1329e + Fe24+ 450−1300 RYD Th 1329e + Al9+ 0−350 RYD Th 1330e + Si+ 1E3.7−1E5.5 K Th 1331e + Be 1E−7−1E1 eV Th 1332e + He 10−10000eV Th 1333e + H 10−10000eV Th 1333e + O2+ 0−40eV Th 1334e + S+ 0−20000K Th 1335e + N+ 0−20000K Th 1335e + He+ 40−70eV Th 1336e + He+ 0−1000eV Th 1337e + C 1801eV Th 1338e + Kr+ 3.3eV Th 1339e + Ho64+ 20−40keV Th 1340e + Ho65+ 20−40keV Th 1340e + Pr56+ 20−40keV Th 1340e + Pr57+ 20−40keV Th 1340e + W28+ 0−4000eV Th 1341e + Yb24+ 0−4000eV Th 1341e + Tb19+ 0−4000eV Th 1341e + Nd14+ 0−4000eV Th 1341e + Ba10+ 0−4000eV Th 1341e + Sn4+ 0−4000eV Th 1341e + Gd18+ 0−4000eV Th 1341e + U 0−40keV Exp 1342e + Bi 0−40keV Exp 1342e + Pb 0−40keV Exp 1342e + Au 0−40keV Exp 1342e + Ar2

+ 300−10400 K E/T 1343e + Kr2+ 1E1−1E8 K Th 1344e + Kr+ 1E1−1E8 K Th 1344e + Kr 1E1−1E8 K Th 1344e + Kr4+ 1E1−1E8 K Th 1344e + Kr3+ 1E1−1E8 K Th 1344e + Kr5+ 1E1−1E8 K Th 1344e + Kr6+ 1E1−1E8 K Th 1344e + Ni10+ threshold−1000 eV Th 1345e + Ni16+ threshold−1700 eV Th 1346e + Fe14+ threshold−1670 eV Th 1347e + K 4−100 eV Th 1348e+ + K 4−100 eV Th 1348e + K 4−100 eV Th 1348e+ + K 4−100 eV Th 1348e + CH3Cl 5, 10, 20 eV Exp 1349e + CH3Cl 5, 10, 20 eV Exp 1349e + Rb 10−100 eV Th 1350e + Ar 0−9 eV E/T 1351e + Xe 0−9 eV E/T 1351e+ + Ar 0−9 eV E/T 1351e+ + Xe 0−9 eV E/T 1351e + Ar 0−9 eV E/T 1351e + Xe 0−9 eV E/T 1351e+ + Ar 0−9 eV E/T 1351e+ + Xe 0−9 eV E/T 1351e + CH2O 0.26−50.3 eV E/T 1352e+ + CH2O 0.26−50.3 eV E/T 1352e + CH3OH 10−1000 eV Th 1353e + e 10−1000 eV Th 1353

65

e + e 0.15−50.15 eV E/T 1354e+ + e 0.15−50.15 eV E/T 1354e+ + N2 0.2−40 eV Exp 1355e+ + Co 0.2−40 eV Exp 1355e+ + C2H2 0.2−40 eV Exp 1355e+ + Ne 0.3−60 eV E/T 1356e+ + Ar 0.3−60 eV E/T 1356e + CH3OH 100−1000 eV E/T 1357e + CH3OH 100−1000 eV E/T 1357e+ + Ne 0−200 eV Th 1358e+ + Ar 0−200 eV Th 1358e+ + Be 0−200 eV Th 1358e+ + Mg 0−200 eV Th 1358e+ + Ne 0−200 eV Th 1358e+ + Ar 0−200 eV Th 1358e+ + Be 0−200 eV Th 1358e+ + Mg 0−200 eV Th 1358e + He 0.1−1000 eV Th 1359e + He 0.1−1000 eV Th 1359e + He 0.1−1000 eV Th 1359e + He threshold−1000 eV Th 1360e + He threshold−1000 eV Th 1360e + Ar 7 meV− 20 eV Exp 1361e + Kr 7 meV− 20 eV Exp 1361e + Xe 7 meV− 20 eV Exp 1361e + Ar 100 eV Exp 1362e + Ar 100 eV Exp 1362e+ + H 20−300 eV Th 1363e+ + H 20−300 eV Th 1363e + Ne threshold−20 eV Th 1364e + Ar threshold−20 eV Th 1364e + Kr threshold−20 eV Th 1364e + Xe threshold−20 eV Th 1364e + Ne threshold−20 eV Th 1364e + Ar threshold−20 eV Th 1364e + Kr threshold−20 eV Th 1364e + Xe threshold−20 eV Th 1364e+ + He 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + C 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + Ne 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + Na 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + Ar 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + He 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + C 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + Ne 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + Na 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e+ + Ar 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh 1365e + e 0−15 eV Exp 1366e + H Z= 24-28 7E5−1E9 K Th 728e + Li Z= 4-36 2E2−2E6 (Z+1)2 K Th 729e + Li Z= 3-6 1−1.5 threshold unit Th 805e + Li Z= 3-6 1−1.5 threshold unit Th 805e + Na Z= 12-14 threshold−20 eV Th 807

2.2.2 Heavy Particles Collisions

H+ + He 1−100keV/u Th 1368H+ + H2 5−600eV Th 1369H+ + Kr 10 − 1000keV/amu Th 1371

66

H+ + Xe 10 − 1000keV/amu Th 1371H+ + Ar 10 − 1000keV/amu Th 1371H+ + Ne 10 − 1000keV/amu Th 1371H+ + U91+ 1−15 threshold unit, 1−2000 keVTh 1372H− + Li 0−100 keV Th 1374H− + He 0−100 keV Th 1374H− + H 0−100 keV Th 1374H+ + H2 75 keV Th 1376H+ + H2 75 keV Th 1376H+ + He 100−1000 eV Th 1377H− + He 700−1000 keV Th 1378H+ + He 700−1000 keV Th 1378H− + He 700−1000 keV Th 1378H+ + He 700−1000 keV Th 1378H+ + H 1−100 keV Th 1379H2+ + H 1−100 keV Th 1379H+ + H2O 100−1000 keV Th 1380H+ + H 1.0 MeV Exp 1381H+ + H 1.0 MeV Exp 1381H− + He 1−1000 keV Th 1386H + H2 0.5−1.4 eV Th 1389H− + H 30−500, 30−200 keV Th 1391H− + H 30−500, 30−200 keV Th 1391H+ + Li 0−50 keV Th 1392He+ + Kr 10 − 1000keV/amu Th 1371He+ + Xe 10 − 1000keV/amu Th 1371He+ + Ar 10 − 1000keV/amu Th 1371He+ + Ne 10 − 1000keV/amu Th 1371He2+ + He 700−1000 keV Th 1378He2+ + He 700−1000 keV Th 1378He2+ + H2 0.3−4.6 keV E/T 1383He2+ + He 0.3−4.6 keV E/T 1383He2+ + H2 0.01−25 keV Th 1385Li3+ + He 700−1000 keV Th 1378Li3+ + He 700−1000 keV Th 1378B5+ + H 0.1− 200keV/amu Th 1370C3+ + H 0−700keV/u Th 1367C6+ + He 100 MeV Th 1373C6+ + He 100 MeV Th 1373C6+ + He 700−1000 keV Th 1378C6+ + He 700−1000 keV Th 1378Ne4+ + CO2 60−1200 eV E/T 1387Ne6+ + CO2 450−2400 eV E/T 1388Ne6+ + H2O 450−2400 eV E/T 1388P + P 0.5−2 MeV E/T 1384Ar18+ + Ar 5−4000 eV Th 1375e + U91+ 1−15 threshold unit, 1−2000 keVTh 1372N2 + U91+ 300−1000 MeV Th 1382N2 + Fe25+ 300−1000 MeV Th 1382N2 + Xe53+ 300−1000 MeV Th 1382O2 + O2 4−34 K E/T 1390

2.3 Surface Interactions

H + W 30−85eV(Te), T: 420K Exp 1408H + C 30−85eV(Te), T: 420K Exp 1408H + W ¡100eV, T: undef Exp 1413H + W ¡100eV, T: undef Exp 1413

67

H + W ¡100eV, T: undef Exp 1413H + W ¡100eV, T: undef Exp 1413H + W ¡100eV, T: undef Exp 1413H+ + C 25−200eV, T: 300−1000K Th 1419H + SiC 20eV(Te), T: undef Th 1420H + C 20eV(Te), T: undef Th 1420H + SiC 20eV(Te), T: undef Th 1420H + C 20eV(Te), T: undef Th 1420H+ + W 50−250eV, T: 320−370K Exp 1421H + H 1−100eV, T: undef Th 1424H + C 1−100eV, T: undef Th 1424H + H 1−100eV, T: undef Th 1424H + C 1−100eV, T: undef Th 1424H + H 1−100eV, T: undef Th 1424H + C 1−100eV, T: undef Th 1424H + H 1−100eV, T: undef Th 1424H + C 1−100eV, T: undef Th 1424H + H 1−100eV, T: undef Th 1424H + C 1−100eV, T: undef Th 1424H + B 1−75eV, T: 900−2000K Exp 1435H + C 1−75eV, T: 900−2000K Exp 1435H + C 1000−4000eV, T: undef Exp 1437H + W 333−1000eV, T: 1000−1050K E/T 1439H + W 333−1000eV, T: 1000−1050K E/T 1439H + C 0.35−200eV, T: undef Th 1441H + C 0.35−200eV, T: undef Th 1441H + C 0.35−200eV, T: undef Th 1441H + H undef, T: 300−830K Exp 1442H + C undef, T: 300−830K Exp 1442H + C 0.2−2eV(Te), T: 400−1200K Exp 1444H + C undef, T: 300−1200K Exp 1448H + C undef, T: 300−1200K Exp 1448H + C undef, T: 300−1200K Exp 1448H + C undef, T: 300−1200K Exp 1448H + C undef, T: 300−1200K Exp 1448H + C undef, T: 300−1200K Exp 1448H + W 2.8−10eV(Te), T: 350−600K Exp 1456H + W 2.8−10eV(Te), T: 350−600K Exp 1456H + W undef, T: 330−470K Exp 1459H + W undef, T: 330−470K Exp 1459H + W undef, T: 330−470K Exp 1459H + W undef, T: 330−470K Exp 1459H + Si 0.1−3eV(Te), T: 500−1700K Exp 1460H + C 0.1−3eV(Te), T: 500−1700K Exp 1460H + Be undef, T: 300K Exp 1461H + C 30eV, T: 300−1500K Th 1466H + W undef, T: undef Exp 1469H + W 333−1000eV, T: 453−1050K Th 1470H + W 333−1000eV, T: 453−1050K Th 1470H + W 333−1000eV, T: 453−1050K Th 1470H + W 333−1000eV, T: 453−1050K Th 1470H + W 333−1000eV, T: 453−1050K Th 1470H + WC undef, T: undef Th 1474H + EUROFER97 undef, T: 673K E/T 1476H + W undef, T: 673K E/T 1476H + Be undef, T: undef Th 1478H + W undef, T: undef Th 1479H + C undef, T: undef Th 1479H + Ni undef, T: 285−1000K Exp 1482

68

H + W undef, T: 285−1000K Exp 1482H + Fe undef, T: undef Th 1487H + W undef, T: undef Th 1487H + Mo undef, T: undef Th 1487H + Cr undef, T: undef Th 1487H + Ta undef, T: undef Th 1487H + Nb undef, T: undef Th 1487H + V undef, T: undef Th 1487H + W undef, T: 300−1000K Th 1489H + Mo undef, T: 273−323K Exp 1490H + W undef, T: 273−323K Exp 1490H + W undef, T: undef Th 1492H + EUROFER97 undef, T: 1323K Exp 1495H + W undef, T: undef Th 1498H + W undef, T: ¿300K Th 1500H + Be undef, T: 673K Exp 1503H + C 1−75eV, T: undef Exp 1510H + H 10−10000eV, T: 300−1300K Th 1511H + C 10−10000eV, T: 300−1300K Th 1511H+ + C 10−10000eV, T: 300−1300K Th 1511H+ + C 10−1000eV, T: 200−1000K Th 1516H+ + C 10−1000eV, T: 200−1000K Th 1516H + W 38eV, T: 285−1000K E/T 1526H + W 2.8−10eV(Te), T: 573K Exp 1527H + W 2.8−10eV(Te), T: 573K Exp 1527H + W 2.8−10eV(Te), T: 573K Exp 1527H + W 2.8−10eV(Te), T: 573K Exp 1527H + W undef, T: 373−1073K Exp 1528H + O undef, T: 373−1073K Exp 1528H + W undef, T: 373−1073K Exp 1528H + O undef, T: 373−1073K Exp 1528H + O undef, T: 373−1073K Exp 1528H + W undef, T: 373−1073K Exp 1528H + O undef, T: 373−1073K Exp 1528H + W undef, T: 373−1073K Exp 1528H + WC ¡25eV, T: 400−1000K Exp 1535H + WC ¡25eV, T: 400−1000K Exp 1535H + WC ¡25eV, T: 400−1000K Exp 1535H + WC ¡25eV, T: 400−1000K Exp 1535H+ + H undef, T: undef Exp 1541H+ + C undef, T: undef Exp 1541H+ + H undef, T: undef Exp 1541H+ + C undef, T: undef Exp 1541H+ + H undef, T: undef Exp 1541H+ + C undef, T: undef Exp 1541H+ + H undef, T: undef Exp 1541H+ + C undef, T: undef Exp 1541H + C 50−1000eV, T: 300K Exp 1555H + C 50−1000eV, T: 300K Exp 1555H + C 50−1000eV, T: 300K Exp 1555H + C 50−1000eV, T: 300K Exp 1555H + Mo undef, T: 600−2000K Th 1563H + H undef, T: undef Th 1566H + Be undef, T: undef Th 1566H + W 38−200eV, T: 300−750K Exp 1567H + W 38−200eV, T: 300−750K Exp 1567H + W 38−200eV, T: 300−750K Exp 1567H + W 38−200eV, T: 300−750K Exp 1567H + W undef, T: 673−873K Exp 1568

69

H+ + W 700−2000eV, T: undef Th 1570H+ + H 700−2000eV, T: undef Th 1570H+ + C 700−2000eV, T: undef Th 1570H + W 0.5−50eV, T: 298K Th 1571H + W 0.5−50eV, T: 298K Th 1571H + H undef, T: undef Th 1573H + Be undef, T: undef Th 1573H + W undef, T: undef Th 1575H + W undef, T: undef Th 1576H + W undef, T: undef Th 1578H + Fe undef, T: undef Th 1581H + W undef, T: undef Th 1581H + W undef, T: undef Exp 1582H + C 200−1500eV, T: 300−1000K E/T 1594H + W 200−1500eV, T: 300−1000K E/T 1594H + C 200−1500eV, T: 300−1000K E/T 1594H + W 200−1500eV, T: 300−1000K E/T 1594H + W 200−1500eV, T: 300−1000K E/T 1594H + C 200−1500eV, T: 300−1000K E/T 1594H + W 200−1500eV, T: 300−1000K E/T 1594H + C 200−1500eV, T: 300−1000K E/T 1594H + W undef, T: 273−2000K Exp 1597H + W undef, T: 500−1450K Th 1598H + W undef, T: undef Th 1600H+ + W 15−25eV, T: 450−900K Exp 1612H+ + W 15−25eV, T: 450−900K Exp 1612H+ + W 15−25eV, T: 450−900K Exp 1612H+ + W 15−25eV, T: 450−900K Exp 1612H + W undefined 1614H + W 200−300eV, T: 373−773K 1621H + SS 200−300eV, T: 373−773K 1621H + W 200−300eV, T: 373−773K 1621H + SS 200−300eV, T: 373−773K 1621H + W 200−300eV, T: 373−773K 1621H + SS 200−300eV, T: 373−773K 1621H + W 200−300eV, T: 373−773K 1621H + SS 200−300eV, T: 373−773K 1621H + W 200−300eV, T: 373−773K 1621H + SS 200−300eV, T: 373−773K 1621H + W 20000eV, T: undef 1625H + C undef, T: undef 1629H + C undef, T: undef 1629H + C undef, T: undef 1629H + C undef, T: undef 1629H + Mo undef, T: 50−1500K 1637H + W undef, T: 50−1500K 1637H + Mo undef, T: 50−1500K 1637H + W undef, T: 50−1500K 1637H + Mo undef, T: 50−1500K 1637H + W undef, T: 50−1500K 1637H + Mo undef, T: 50−1500K 1637H + W undef, T: 50−1500K 1637H + Mo undef, T: 50−1500K 1637H + W undef, T: 50−1500K 1637H + SS 10−1000eV, T: undef 1640H + C 10−1000eV, T: undef 1640H + SS 10−1000eV, T: undef 1640H + C 10−1000eV, T: undef 1640H + SS 10−1000eV, T: undef 1640

70

H + C 10−1000eV, T: undef 1640H + SS 10−1000eV, T: undef 1640H + C 10−1000eV, T: undef 1640H + Be undef, T: 673K 1642H + BeO undef, T: 673K 1642H + Be undef, T: 673K 1642H + BeO undef, T: 673K 1642H + Be undef, T: 673K 1642H + BeO undef, T: 673K 1642H + Be undef, T: 673K 1642H + BeO undef, T: 673K 1642H + Be undef, T: 673K 1642H + BeO undef, T: 673K 1642H + W 1000eV, T: ¡373K 1646H + W 1000eV, T: ¡373K 1646H + W 1000eV, T: ¡373K 1646H + W 1000eV, T: ¡373K 1646H + W 200eV, T: 320−450K 1647H + W 200eV, T: 320−450K 1647H + W 200eV, T: 320−450K 1647H + W 200eV, T: 320−450K 1647H + W 200eV, T: 320−450K 1647He + W 60eV, T: 1123K Exp 1394He + W 2−2000eV, T: undef Th 1405He + W 160−320eV, T: 570−1070K Exp 1407He + W 160−320eV, T: 570−1070K Exp 1407He + W 160−320eV, T: 570−1070K Exp 1407He + W 160−320eV, T: 570−1070K Exp 1407He + W 160−320eV, T: 570−1070K Exp 1407He + WC 100−300eV, T: 600K Th 1410He + C 30−126eV, T: 700K Exp 1416He + W 15−70eV, T: 293−1100K Exp 1422He + W 15−70eV, T: 293−1100K Exp 1422He + W 15−70eV, T: 293−1100K Exp 1422He + W 15−70eV, T: 293−1100K Exp 1422He + W 10−1000eV, T: undef Th 1430He + C 1000−4000eV, T: undef Exp 1437He + H 3eV(Te), T: undef Exp 1445He + C 3eV(Te), T: undef Exp 1445He + Li 10−5000eV, T: undef Exp 1452He + C 10−5000eV, T: undef Exp 1452He + W 10−500eV, T: 300−500K Exp 1464He + O 10−500eV, T: 300−500K Exp 1464He + C 10−500eV, T: 300−500K Exp 1464He + W 10−500eV, T: 300−500K Exp 1464He + O 10−500eV, T: 300−500K Exp 1464He + C 10−500eV, T: 300−500K Exp 1464He + O 10−500eV, T: 300−500K Exp 1464He + C 10−500eV, T: 300−500K Exp 1464He + W 10−500eV, T: 300−500K Exp 1464He + W 10−500eV, T: 300−500K Exp 1464He + C 10−500eV, T: 300−500K Exp 1464He + O 10−500eV, T: 300−500K Exp 1464He + W 320−6000eV, T: 1873K Exp 1473He + W 30−1500eV, T: 300−873K Th 1475He + Be undef, T: undef Th 1478He + W undef, T: 1−1000K Th 1494He + W ¡75eV, T: 1070−1320K Exp 1501He + WC 100−300eV, T: 600K Th 1507

71

He + WC 100−300eV, T: 600K Th 1507He + W 20−60eV, T: 320−593K Exp 1508He + W 20−60eV, T: 320−593K Exp 1508He + W 20−60eV, T: 320−593K Exp 1508He + W 20−60eV, T: 320−593K Exp 1508He + Be 10−10000eV, T: 300−1300K Th 1511He+ + W 100−6000eV, T: 300−2000K E/T 1513He + W undef, T: undef Th 1515He+ + W undef, T: 298−823K Exp 1518He + W 170−340eV, T: 300−700K Exp 1522He + W 170−340eV, T: 300−700K Exp 1522He + W 170−340eV, T: 300−700K Exp 1522He + W 170−340eV, T: 300−700K Exp 1522He+ + W 30−60eV, T: 300−700K Exp 1525He+ + W 30−60eV, T: 300−700K Exp 1525He+ + W 30−60eV, T: 300−700K Exp 1525He+ + W 30−60eV, T: 300−700K Exp 1525He + W 38eV, T: 285−1000K E/T 1526He + W 38eV, T: 285−1000K E/T 1526He + W 38eV, T: 285−1000K E/T 1526He + W 38eV, T: 285−1000K E/T 1526He + W undef, T: 200−2000K Exp 1529He + He undef, T: 200−2000K Exp 1529He + W undef, T: 200−2000K Exp 1529He + He undef, T: 200−2000K Exp 1529He + WC ¡25eV, T: 400−1000K Exp 1535He + WC ¡25eV, T: 400−1000K Exp 1535He + WC ¡25eV, T: 400−1000K Exp 1535He + WC ¡25eV, T: 400−1000K Exp 1535He+ + W 76eV, T: 400−750K Exp 1538He+ + W 76eV, T: 400−750K Exp 1538He+ + W 76eV, T: 400−750K Exp 1538He+ + W 76eV, T: 400−750K Exp 1538He + W undef, T: 300−1873K Exp 1539He + W undef, T: 300−1873K Exp 1539He + W undef, T: 300−1873K Exp 1539He + W undef, T: 300−1873K Exp 1539He+ + W 76eV, T: 300−800K Exp 1545He+ + W 76eV, T: 300−800K Exp 1545He+ + W 76eV, T: 300−800K Exp 1545He+ + W 76eV, T: 300−800K Exp 1545He + Be undef, T: 1123−1273K Exp 1565He+ + W 30000eV, T: 1273−1423K Exp 1569He+ + W 30000eV, T: 1273−1423K Exp 1569He+ + W 30000eV, T: 1273−1423K Exp 1569He+ + W 30000eV, T: 1273−1423K Exp 1569He + He undef, T: undef Th 1573He + Be undef, T: undef Th 1573He + W 30−1000eV, T: 837−873K Th 1574He + W undef, T: undef Th 1576He+ + W undef, T: 773−1173K Exp 1577He+ + W undef, T: 773−1173K Exp 1577He+ + W undef, T: 773−1173K Exp 1577He+ + W 60−250eV, T: 1120−1320K Exp 1585He+ + Be 20−160eV, T: undef E/T 1586He + W 1000−5000eV, T: 300−873K E/T 1599He + W 1000−5000eV, T: 300−873K E/T 1599He + W 1000−5000eV, T: 300−873K E/T 1599He + W 1000−5000eV, T: 300−873K E/T 1599

72

He + W undef, T: undef Th 1600He + W 30−200eV, T: 420−1100K Exp 1601He + W 30−200eV, T: 420−1100K Exp 1601He + W 30−200eV, T: 420−1100K Exp 1601He + W 30−200eV, T: 420−1100K Exp 1601He+ + Mo undef, T: undef Exp 1602He+ + W undef, T: undef Exp 1602He+ + Mo undef, T: undef Exp 1602He+ + W undef, T: undef Exp 1602He+ + Mo undef, T: undef Exp 1602He+ + W undef, T: undef Exp 1602He+ + Mo undef, T: undef Exp 1602He+ + W undef, T: undef Exp 1602He + W 40−70eV, T: ¡573K Exp 1603He + W 40−70eV, T: ¡573K Exp 1603He + W 40−70eV, T: ¡573K Exp 1603He + W 40−70eV, T: ¡573K Exp 1603He + W undef, T: 314−773K Exp 1607He + W undef, T: 314−773K Exp 1607He + W undef, T: 314−773K Exp 1607He + W undef, T: 314−773K Exp 1607He+ + W undef, T: 1123−1273K Exp 1611He+ + W undef, T: 1123−1273K Exp 1611He+ + W undef, T: 1123−1273K Exp 1611He+ + W undef, T: 1123−1273K Exp 1611He+ + W 15−25eV, T: 450−900K Exp 1612He+ + W 15−25eV, T: 450−900K Exp 1612He+ + W 15−25eV, T: 450−900K Exp 1612He+ + W 15−25eV, T: 450−900K Exp 1612He + W T: 50−3000K 1616He + W 300−1000eV, T: 298K 1623He + Cd 210eV, T: 300−773K 1627He + Cd 210eV, T: 300−773K 1627He + Cd 210eV, T: 300−773K 1627He + Cd 210eV, T: 300−773K 1627He + WC undef, T: undef 1631He + WC undef, T: undef 1631He + WC undef, T: undef 1631He + WC undef, T: undef 1631He + WC undef, T: undef 1631He + W 320eV, T: undef 1638He + W 320eV, T: undef 1638He + W 320eV, T: undef 1638He + W 320eV, T: undef 1638He + W undef, T: 700−1600K 1643He + He undef, T: 700−1600K 1643He + W undef, T: 700−1600K 1643He + He undef, T: 700−1600K 1643He + W undef, T: 700−1600K 1643He + He undef, T: 700−1600K 1643He + W undef, T: 700−1600K 1643He + He undef, T: 700−1600K 1643He + Be undef, T: undef 1644He + Be undef, T: 570−1333K 1649He + W 60eV, T: 500−2000K 1658He+ + W 10−10000eV, T: 298−1600K 1665He+ + W 10−10000eV, T: 298−1600K 1665He+ + W 10−10000eV, T: 298−1600K 1665He+ + W 10−10000eV, T: 298−1600K 1665

73

He + W 200eV, T: 1223K 1668He + W 60eV, T: 573K 1672He + W 60eV, T: 573K 1672He + W 60eV, T: 573K 1672He + W 60eV, T: 573K 1672He + W 60eV, T: 573−1603K 1673He + W undef, T: undef 1679He + Be undef, T: undef 1679He + C undef, T: undef 1679He + N undef, T: undef 1679He + O undef, T: undef 1679He + Re undef, T: undef 1679He + Ta undef, T: undef 1679He + Nb undef, T: undef 1679He + V undef, T: undef 1679He + Ti undef, T: undef 1679He + Si undef, T: undef 1679He + Zr undef, T: undef 1679He + Y undef, T: undef 1679He + Sc undef, T: undef 1679He + W undef, T: undef 1679He + Be undef, T: undef 1679He + C undef, T: undef 1679He + N undef, T: undef 1679He + O undef, T: undef 1679He + Re undef, T: undef 1679He + Ta undef, T: undef 1679He + Nb undef, T: undef 1679He + V undef, T: undef 1679He + Os undef, T: undef 1679He + Ti undef, T: undef 1679He + Si undef, T: undef 1679He + Zr undef, T: undef 1679He + Y undef, T: undef 1679He + Sc undef, T: undef 1679He + W undef, T: undef 1679He + Be undef, T: undef 1679He + C undef, T: undef 1679He + N undef, T: undef 1679He + O undef, T: undef 1679He + Re undef, T: undef 1679He + Ta undef, T: undef 1679He + Nb undef, T: undef 1679He + V undef, T: undef 1679He + Os undef, T: undef 1679He + Ti undef, T: undef 1679He + Si undef, T: undef 1679He + Zr undef, T: undef 1679He + Y undef, T: undef 1679He + Sc undef, T: undef 1679He + W undef, T: undef 1679He + Be undef, T: undef 1679He + C undef, T: undef 1679He + N undef, T: undef 1679He + O undef, T: undef 1679He + Re undef, T: undef 1679He + Ta undef, T: undef 1679He + Nb undef, T: undef 1679He + V undef, T: undef 1679

74

He + Os undef, T: undef 1679He + Ti undef, T: undef 1679He + Si undef, T: undef 1679He + Zr undef, T: undef 1679He + Y undef, T: undef 1679He + Sc undef, T: undef 1679He + W undef, T: undef 1679He + Be undef, T: undef 1679He + C undef, T: undef 1679He + N undef, T: undef 1679He + O undef, T: undef 1679He + Re undef, T: undef 1679He + Ta undef, T: undef 1679He + Nb undef, T: undef 1679He + V undef, T: undef 1679He + Ti undef, T: undef 1679He + Si undef, T: undef 1679He + Zr undef, T: undef 1679He + Y undef, T: undef 1679He + Sc undef, T: undef 1679Be + W 60eV, T: 1123K Exp 1394Be + C 10−250eV, T: undef Th 1396Be + Be 10−250eV, T: undef Th 1396Be + C 10−250eV, T: undef Th 1396Be + Be 10−250eV, T: undef Th 1396Be + Be 10−250eV, T: undef Th 1396Be + C 10−250eV, T: undef Th 1396Be + C 10−250eV, T: undef Th 1396Be + Be 10−250eV, T: undef Th 1396Be + C 10−250eV, T: undef Th 1396Be + Be 10−250eV, T: undef Th 1396Be + C 10−250eV, T: undef Th 1396Be + Be 10−250eV, T: undef Th 1396Be + W undef, T: 670−1470K E/T 1397Be + W undef, T: 670−1470K E/T 1397Be + Be 10−1000eV, T: undef E/T 1400Be + Be 10−100eV, T: 300K Th 1401Be + C 30−126eV, T: 700K Exp 1416Be + W 15−70eV, T: 293−1100K Exp 1422Be + H 1−100eV, T: undef Th 1424Be + C 1−100eV, T: undef Th 1424Be + H 1−100eV, T: undef Th 1424Be + C 1−100eV, T: undef Th 1424Be + H 1−100eV, T: undef Th 1424Be + C 1−100eV, T: undef Th 1424Be + H 1−100eV, T: undef Th 1424Be + C 1−100eV, T: undef Th 1424Be + H 1−100eV, T: undef Th 1424Be + C 1−100eV, T: undef Th 1424Be + C 7eV(Te), T: undef Th 1425Be + C 7eV(Te), T: undef Th 1425Be + Be 20−500eV, T: 320−670K E/T 1433Be + Be 20−500eV, T: 320−670K E/T 1433Be + W undef, T: undef Th 1471Be + W undef, T: undef Th 1472Be + W ¡75eV, T: 1070−1320K Exp 1501Be + C 13.3−48.5eV, T: undef Th 1502Be + Be 200eV, T: 300−1023K Exp 1506Be + O 200eV, T: 300−1023K Exp 1506

75

Be + C 200eV, T: 300−1023K Exp 1506Be + Be 50−60eV, T: 573K Exp 1519Be + W 50−60eV, T: 573K Exp 1519Be + Be 50−60eV, T: 573K Exp 1519Be + W 50−60eV, T: 573K Exp 1519Be + Be 50−60eV, T: 573K Exp 1519Be + W 50−60eV, T: 573K Exp 1519Be + Be 50−60eV, T: 573K Exp 1519Be + W 50−60eV, T: 573K Exp 1519Be + Be undef, T: 1123−1273K Exp 1565Be + H undef, T: undef Th 1566Be + Be undef, T: undef Th 1566Be + Be 20−160eV, T: undef E/T 1586Be + C undefined 1615Be + BeC undefined 1615Be + C undefined 1615Be + BeC undefined 1615Be + C undefined 1615Be + BeC undefined 1615Be + C undefined 1615Be + BeC undefined 1615Be + C undefined 1615Be + BeC undefined 1615Be + Be 300−500eV, T: undef 1662Be + Be 300−500eV, T: undef 1662Be + Be 300−500eV, T: undef 1662Be + Be 300−500eV, T: undef 1662Be + Be 300−500eV, T: undef 1662Be + Be 5−100eV, T: 300K 1671Be + W 60eV, T: 573K 1672Be + W 60eV, T: 573K 1672Be + W 60eV, T: 573K 1672Be + W 60eV, T: 573K 1672B + W undef, T: undef Exp 1531B + W undef, T: undef Exp 1531B + W undef, T: undef Exp 1531B + W undef, T: undef Exp 1531C + Be 10−250eV, T: undef Th 1396C + C 10−250eV, T: undef Th 1396C + C 10−250eV, T: undef Th 1396C + Be 10−250eV, T: undef Th 1396C + C 10−250eV, T: undef Th 1396C + Be 10−250eV, T: undef Th 1396C + Be 10−250eV, T: undef Th 1396C + C 10−250eV, T: undef Th 1396C + Be 10−250eV, T: undef Th 1396C + C 10−250eV, T: undef Th 1396C + Be 10−250eV, T: undef Th 1396C + C 10−250eV, T: undef Th 1396C + W undef, T: 670−1470K E/T 1397C + W undef, T: 670−1470K E/T 1397C + W 2−2000eV, T: undef Th 1405C + WC 100−300eV, T: 600K Th 1410C + W 1−100eV, T: undef Th 1424C + C 1−100eV, T: undef Th 1424C + C 1−100eV, T: undef Th 1424C + W 1−100eV, T: undef Th 1424C + C 1−100eV, T: undef Th 1424C + W 1−100eV, T: undef Th 1424

76

C + W 1−100eV, T: undef Th 1424C + C 1−100eV, T: undef Th 1424C + W 1−100eV, T: undef Th 1424C + C 1−100eV, T: undef Th 1424C + W 333−1000eV, T: 1000−1050K E/T 1439C + W 333−1000eV, T: 1000−1050K E/T 1439C + W 1−200eV, T: 300K E/T 1468C + W 333−1000eV, T: 453−1050K Th 1470C + W 333−1000eV, T: 453−1050K Th 1470C + W 333−1000eV, T: 453−1050K Th 1470C + W 333−1000eV, T: 453−1050K Th 1470C + W 333−1000eV, T: 453−1050K Th 1470C + WC undef, T: undef Th 1477C + Be undef, T: undef Th 1478C + W undef, T: 300−1000K Th 1480C + W undef, T: undef Th 1485C + W undef, T: 100−1200K Th 1491C + He undef, T: 300−573K Th 1493C + Fe undef, T: 300−573K Th 1493C + EUROFER97 undef, T: 1323K Exp 1495C + ZrO2 undef, T: 1173−1273K Exp 1497C + C 13.3−48.5eV, T: undef Th 1502C + W 1000eV, T: 550−1050K Exp 1505C + Be 200eV, T: 300−1023K Exp 1506C + O 200eV, T: 300−1023K Exp 1506C + C 200eV, T: 300−1023K Exp 1506C + WC 100−300eV, T: 600K Th 1507C+ + W 100−6000eV, T: 300−2000K E/T 1513C + WC 100−6000eV, T: 300−2000K E/T 1513C + C 100−6000eV, T: 300−2000K E/T 1513C + W 100−6000eV, T: 300−2000K E/T 1513C + C undef, T: 1073K Exp 1523C + W undef, T: 1073K Exp 1523C + C undef, T: undef Exp 1524C + W undef, T: undef Exp 1524C + C undef, T: undef Exp 1524C + W undef, T: undef Exp 1524C + C undef, T: undef Exp 1524C + W undef, T: undef Exp 1524C + C undef, T: undef Exp 1524C + W undef, T: undef Exp 1524C + W undef, T: undef Exp 1531C + W undef, T: undef Exp 1531C + W undef, T: undef Exp 1531C + W undef, T: undef Exp 1531C + C 1−200eV, T: undef Th 1562C + Be 1−200eV, T: undef Th 1562C + H 1−200eV, T: undef Th 1562C + W undef, T: undef Th 1572C + W undef, T: 300−1000K Th 1580C + C 0.1−1000eV, T: 400−1400K E/T 1587C + W 0.1−1000eV, T: 400−1400K E/T 1587C + C 0.1−1000eV, T: 400−1400K E/T 1587C + W 0.1−1000eV, T: 400−1400K E/T 1587C + W 1−250eV, T: 300−1500K 1619C + WC 1−250eV, T: 300−1500K 1619C + W 60eV, T: 573−1603K 1673N + W 2−2000eV, T: undef Th 1405N + W undef, T: undef Th 1485

77

N + W undef, T: 300−1000K Exp 1496N + C undef, T: 300−1000K Exp 1496N + N undef, T: 300−1000K Exp 1496N + W 20−500V, T: 350K E/T 1591N + W 20−500V, T: 350K E/T 1591N + W 20−500V, T: 350K E/T 1591N + W 20−500V, T: 350K E/T 1591O + WC undef, T: 800K Exp 1428O + C undef, T: 800K Exp 1428O + W undef, T: 330−470K Exp 1459O + W undef, T: 330−470K Exp 1459O + W undef, T: 330−470K Exp 1459O + W undef, T: 330−470K Exp 1459O + Be undef, T: undef Th 1478O + W undef, T: 300−1000K Th 1499O + Be 200eV, T: 300−1023K Exp 1506O + O 200eV, T: 300−1023K Exp 1506O + C 200eV, T: 300−1023K Exp 1506O + W 700−2000eV, T: undef Th 1570O + CH undef, T: 473−623K 1617O + W undef, T: undef 1635O + W undef, T: undef 1635O + W undef, T: undef 1635O + W undef, T: undef 1635O + W undef, T: undef 1635O + SS 10−1000eV, T: undef 1640O + C 10−1000eV, T: undef 1640O + SS 10−1000eV, T: undef 1640O + C 10−1000eV, T: undef 1640O + SS 10−1000eV, T: undef 1640O + C 10−1000eV, T: undef 1640O + SS 10−1000eV, T: undef 1640O + C 10−1000eV, T: undef 1640Ne + W 2−2000eV, T: undef Th 1405Ne + WC 100−300eV, T: 600K Th 1410Ne + Fe 30−300eV, T: ¡373K Exp 1463Ne + W 1−200eV, T: 300K E/T 1468Ne + WC 100−300eV, T: 600K Th 1507P + EUROFER97 undef, T: 1323K Exp 1495S + EUROFER97 undef, T: 1323K Exp 1495Ar + C 300eV, T: 400K Exp 1402Ar + W 300eV, T: 400K Exp 1402Ar + W 300eV, T: 400K Exp 1402Ar + C 300eV, T: 400K Exp 1402Ar + W undef, T: undef Exp 1403Ar + W undef, T: undef Exp 1403Ar + C undef, T: undef Exp 1403Ar + H undef, T: undef Exp 1403Ar + H undef, T: undef Exp 1403Ar + C undef, T: undef Exp 1403Ar + W 2−2000eV, T: undef Th 1405Ar + WC 100−300eV, T: 600K Th 1410Ar + C 30−126eV, T: 700K Exp 1416Ar + W 30−120eV, T: undef Exp 1427Ar + W 1−1000eV, T: 300−900K E/T 1429Ar + C undef, T: undef Exp 1454Ar + W undef, T: undef Exp 1454Ar + Fe 30−300eV, T: ¡373K Exp 1463Ar + W 30−300eV, T: ¡373K Exp 1463

78

Ar + Mo 30−300eV, T: ¡373K Exp 1463Ar + W 1−200eV, T: 300K E/T 1468Ar + WC 100−300eV, T: 600K Th 1507Ar + WC 100−300eV, T: 600K Th 1507Ar + W 10−10000eV, T: 300−1300K Th 1511Ar + Be 10−10000eV, T: 300−1300K Th 1511Ar+ + H 10−1000eV, T: 200−1000K Th 1516Ar+ + C 10−1000eV, T: 200−1000K Th 1516Ar+ + H 10−1000eV, T: 200−1000K Th 1516Ar+ + C 10−1000eV, T: 200−1000K Th 1516Ar + W 170−340eV, T: 300−700K Exp 1522Ar + W 170−340eV, T: 300−700K Exp 1522Ar + W 170−340eV, T: 300−700K Exp 1522Ar + W 170−340eV, T: 300−700K Exp 1522Ar + W 20−180eV, T: undef Exp 1595Ar + W 30−200eV, T: 420−1100K Exp 1601Ar + W 30−200eV, T: 420−1100K Exp 1601Ar + W 30−200eV, T: 420−1100K Exp 1601Ar + W 30−200eV, T: 420−1100K Exp 1601Ar + W 200−300eV, T: 373−773K 1621Ar + SS 200−300eV, T: 373−773K 1621Ar + W 200−300eV, T: 373−773K 1621Ar + SS 200−300eV, T: 373−773K 1621Ar + W 200−300eV, T: 373−773K 1621Ar + SS 200−300eV, T: 373−773K 1621Ar + W 200−300eV, T: 373−773K 1621Ar + SS 200−300eV, T: 373−773K 1621Ar + W 200−300eV, T: 373−773K 1621Ar + SS 200−300eV, T: 373−773K 1621Ar + Be 300−500eV, T: undef 1662Ar + Be 300−500eV, T: undef 1662Ar + Be 300−500eV, T: undef 1662Ar + Be 300−500eV, T: undef 1662Ar + Be 300−500eV, T: undef 1662Ar+ + Be 15−70eV, T: 298−573K 1670Ar+ + W 15−70eV, T: 298−573K 1670Ar+ + BeW 15−70eV, T: 298−573K 1670Ca + EUROFER97 undef, T: 1323K Exp 1495Cr + EUROFER97 undef, T: 1323K Exp 1495Fe + EUROFER97 undef, T: 1323K Exp 1495Cu + W undef, T: 300−1000K Exp 1496Cu + C undef, T: 300−1000K Exp 1496Cu + N undef, T: 300−1000K Exp 1496Kr + W 2−2000eV, T: undef Th 1405Kr + CuBe 2000−10000eV, T: undef E/T 1434Kr + W 1−200eV, T: 300K E/T 1468W + WC 100−300eV, T: 600K Th 1410W + W 5000eV, T: 300K Th 1418W + Be undef, T: undef Th 1472W + WC undef, T: undef Th 1477W + Re undef, T: 1373−1673K Exp 1484W + W undef, T: 1373−1673K Exp 1484W + EUROFER97 undef, T: 1323K Exp 1495W + WC 100−300eV, T: 600K Th 1507W + W undefined 1613W + W undef, T: undef 1669Re + Re undef, T: 1373−1673K Exp 1484Re + W undef, T: 1373−1673K Exp 1484Re + W undef, T: 673−873K Exp 1568

79

H2 + C 300eV, T: 400K Exp 1402H2 + W 300eV, T: 400K Exp 1402H2 + C 300eV, T: 400K Exp 1402H2 + W 300eV, T: 400K Exp 1402H2 + W undef, T: undef Exp 1403H2 + C undef, T: undef Exp 1403H2 + H undef, T: undef Exp 1403H2 + H undef, T: undef Exp 1403H2 + C undef, T: undef Exp 1403H2 + W undef, T: undef Exp 1403H2 + C undef, T: 300−600K Exp 1411H2 + D undef, T: 300−600K Exp 1411H2 + B undef, T: 300−600K Exp 1411H2 + C 0.1−2.4eV(Te), T: ¡1000K Exp 1440H2

+ + W 700−2000eV, T: undef Th 1570H2 + C 5−8eV 1632H2 + C 5−8eV 1632H2 + C 5−8eV 1632H2 + C 5−8eV 1632H2

+ + W 110eV, T: ¡373K 1657H2

+ + W 110eV, T: ¡373K 1657H2

+ + W 110eV, T: ¡373K 1657H2

+ + W 110eV, T: ¡373K 1657HD + C 5−8eV 1632HD + C 5−8eV 1632HD + C 5−8eV 1632HD + C 5−8eV 1632D+ + W 30−100 eV, T: 350K Exp 1393D+ + C 30−100 eV, T: 350K Exp 1393D + W 60eV, T: 1123K Exp 1394D + WC 10−1000eV, T: 300−600K Th 1395D + W 10−1000eV, T: 300−600K Th 1395D + W2C 10−1000eV, T: 300−600K Th 1395D + W2C 10−1000eV, T: 300−600K Th 1395D + WC 10−1000eV, T: 300−600K Th 1395D + W 10−1000eV, T: 300−600K Th 1395D + W2C 10−1000eV, T: 300−600K Th 1395D + WC 10−1000eV, T: 300−600K Th 1395D + W 10−1000eV, T: 300−600K Th 1395D + W2C 10−1000eV, T: 300−600K Th 1395D + WC 10−1000eV, T: 300−600K Th 1395D + W 10−1000eV, T: 300−600K Th 1395D + W2C 10−1000eV, T: 300−600K Th 1395D + WC 10−1000eV, T: 300−600K Th 1395D + W 10−1000eV, T: 300−600K Th 1395D + C 10−250eV, T: undef Th 1396D + C 10−250eV, T: undef Th 1396D + Be 10−250eV, T: undef Th 1396D + Be 10−250eV, T: undef Th 1396D + Be 10−250eV, T: undef Th 1396D + C 10−250eV, T: undef Th 1396D + C 10−250eV, T: undef Th 1396D + C 10−250eV, T: undef Th 1396D + Be 10−250eV, T: undef Th 1396D + Be 10−250eV, T: undef Th 1396D + C 10−250eV, T: undef Th 1396D + Be 10−250eV, T: undef Th 1396D + W 10−1000eV, T: undef Th 1398D + Be 10−1000eV, T: undef Th 1398

80

D + Be ¡80eV, T: 800−2000K Exp 1399D + Be 10−1000eV, T: undef E/T 1400D + Be 10−100eV, T: 300K Th 1401D + Be2C 10−100eV, T: 300K Th 1401D+ + W 30−300eV, T: 300K Exp 1404D+ + C 30−300eV, T: 300K Exp 1404D + W 2−2000eV, T: undef Th 1405D + W 160−320eV, T: 570−1070K Exp 1407D + W 160−320eV, T: 570−1070K Exp 1407D + W 160−320eV, T: 570−1070K Exp 1407D + W 160−320eV, T: 570−1070K Exp 1407D + W 160−320eV, T: 570−1070K Exp 1407D + W 30−85eV(Te), T: 420K Exp 1408D + C 30−85eV(Te), T: 420K Exp 1408D + Be 30eV, T: 700−900K Exp 1409D + WC 100−300eV, T: 600K Th 1410D + Be 2−200eV, T: 300K Th 1412D + Be2C 2−200eV, T: 300K Th 1412D + WC 2−200eV, T: 300K Th 1412D + C 2−200eV, T: 300K Th 1412D + Be 7−3000eV, T: 373K E/T 1415D + C 30−126eV, T: 700K Exp 1416D+ + W 50−250eV, T: 320−370K Exp 1421D + W 15−70eV, T: 293−1100K Exp 1422D + Be 15−70eV, T: 293−1100K Exp 1422D + W 15−70eV, T: 293−1100K Exp 1422D + Be 15−70eV, T: 293−1100K Exp 1422D + W 15−70eV, T: 293−1100K Exp 1422D + Be 15−70eV, T: 293−1100K Exp 1422D + W 15−70eV, T: 293−1100K Exp 1422D + Be 15−70eV, T: 293−1100K Exp 1422D + Be 15−70eV, T: 293−1100K Exp 1422D + W 1−100eV, T: undef Th 1424D + C 1−100eV, T: undef Th 1424D + C 1−100eV, T: undef Th 1424D + W 1−100eV, T: undef Th 1424D + W 1−100eV, T: undef Th 1424D + C 1−100eV, T: undef Th 1424D + C 1−100eV, T: undef Th 1424D + W 1−100eV, T: undef Th 1424D + W 1−100eV, T: undef Th 1424D + C 1−100eV, T: undef Th 1424D + C 7eV(Te), T: undef Th 1425D + C 7eV(Te), T: undef Th 1425D + C 1−100eV, T: 300−900K Th 1426D + Be 1−100eV, T: 300−900K Th 1426D + C 1−100eV, T: 300−900K Th 1426D + Be 1−100eV, T: 300−900K Th 1426D + C 1−100eV, T: 300−900K Th 1426D + Be 1−100eV, T: 300−900K Th 1426D + C 1−100eV, T: 300−900K Th 1426D + Be 1−100eV, T: 300−900K Th 1426D + C 1−100eV, T: 300−900K Th 1426D + Be 1−100eV, T: 300−900K Th 1426D + C 1−100eV, T: 300−900K Th 1426D + Be 1−100eV, T: 300−900K Th 1426D + Be 1−1000eV, T: 300−900K E/T 1429D + W 1−1000eV, T: 300−900K E/T 1429D + C 1−1000eV, T: 300−900K E/T 1429

81

D + W 1−1000eV, T: 300−900K E/T 1429D + Be 1−1000eV, T: 300−900K E/T 1429D + C 1−1000eV, T: 300−900K E/T 1429D + BeC 1−1000eV, T: 300−900K E/T 1429D + W 1−1000eV, T: 300−900K E/T 1429D + Be 1−1000eV, T: 300−900K E/T 1429D + C 1−1000eV, T: 300−900K E/T 1429D + WC 1−1000eV, T: 300−900K E/T 1429D + BeO 1−1000eV, T: 300−900K E/T 1429D + BeC 1−1000eV, T: 300−900K E/T 1429D + BeO 1−1000eV, T: 300−900K E/T 1429D + BeC 1−1000eV, T: 300−900K E/T 1429D + W 1−1000eV, T: 300−900K E/T 1429D + Be 1−1000eV, T: 300−900K E/T 1429D + C 1−1000eV, T: 300−900K E/T 1429D + WC 1−1000eV, T: 300−900K E/T 1429D + BeO 1−1000eV, T: 300−900K E/T 1429D + Be 1−1000eV, T: 300−900K E/T 1429D + C 1−1000eV, T: 300−900K E/T 1429D + WC 1−1000eV, T: 300−900K E/T 1429D + BeO 1−1000eV, T: 300−900K E/T 1429D + BeC 1−1000eV, T: 300−900K E/T 1429D + W 1−1000eV, T: 300−900K E/T 1429D + WC 1−1000eV, T: 300−900K E/T 1429D + W 10−1000eV, T: undef Th 1430D + W 100−250eV, T: 300K Exp 1432D + C 100−250eV, T: 300K Exp 1432D + C 15−200eV, T: 300−1000K Exp 1436D + C 1000−4000eV, T: undef Exp 1437D + W 250eV, T: 400K Exp 1438D + W 250eV, T: 400K Exp 1438D + W 250eV, T: 400K Exp 1438D + W 250eV, T: 400K Exp 1438D + W 250eV, T: 400K Exp 1438D + Zr 30−200eV Exp 1443D + Ti 30−200eV Exp 1443D + C 30−200eV Exp 1443D + C 0.1−0.4eV(Te), T: 600−1000K Exp 1446D + C undef, T: undef Exp 1447D + C undef, T: undef Exp 1447D + C undef, T: 300−1200K Exp 1448D + C undef, T: 300−1200K Exp 1448D + C undef, T: 300−1200K Exp 1448D + C undef, T: 300−1200K Exp 1448D + C undef, T: 300−1200K Exp 1448D + C undef, T: 300−1200K Exp 1448D + C 100eV, T: ¡340K Exp 1449D + C 100eV, T: ¡340K Exp 1449D + B 44eV(Te), T: 1050−1250K Exp 1450D + C 44eV(Te), T: 1050−1250K Exp 1450D + B 44eV(Te), T: 1050−1250K Exp 1450D + C 44eV(Te), T: 1050−1250K Exp 1450D + B 44eV(Te), T: 1050−1250K Exp 1450D + C 44eV(Te), T: 1050−1250K Exp 1450D + B 44eV(Te), T: 1050−1250K Exp 1450D + C 44eV(Te), T: 1050−1250K Exp 1450D + C undef, T: 470K Exp 1451D + C undef, T: 470K Exp 1451D + C undef, T: 470K Exp 1451

82

D + C undef, T: 470K Exp 1451D + C undef, T: 470K Exp 1451D + Li undef, T: 523−673K Exp 1453D + Li undef, T: 523−673K Exp 1453D + Li undef, T: 523−673K Exp 1453D + Li undef, T: 523−673K Exp 1453D + C 200eV, T: 300K Exp 1455D + Be 200eV, T: 300K Exp 1455D + O 200eV, T: 300K Exp 1455D + C 200eV, T: 300K Exp 1455D + Be 200eV, T: 300K Exp 1455D + O 200eV, T: 300K Exp 1455D + C 200eV, T: 300K Exp 1455D + Be 200eV, T: 300K Exp 1455D + O 200eV, T: 300K Exp 1455D + C 200eV, T: 300K Exp 1455D + Be 200eV, T: 300K Exp 1455D + O 200eV, T: 300K Exp 1455D + W 2.8−10eV(Te), T: 350−600K Exp 1456D + W 2.8−10eV(Te), T: 350−600K Exp 1456D + W 250eV, T: undef Exp 1457D + W 250eV, T: undef Exp 1457D + W 250eV, T: undef Exp 1457D + W 250eV, T: undef Exp 1457D + C 100−250eV, T: ¡400K Exp 1458D + W 100−250eV, T: ¡400K Exp 1458D + C 100−250eV, T: ¡400K Exp 1458D + W 100−250eV, T: ¡400K Exp 1458D + C 100−250eV, T: ¡400K Exp 1458D + W 100−250eV, T: ¡400K Exp 1458D + C 100−250eV, T: ¡400K Exp 1458D + W 100−250eV, T: ¡400K Exp 1458D + C 100−250eV, T: ¡400K Exp 1458D + W 100−250eV, T: ¡400K Exp 1458D + W undef, T: 330−470K Exp 1459D + W undef, T: 330−470K Exp 1459D + W undef, T: 330−470K Exp 1459D + W undef, T: 330−470K Exp 1459D+ + Mo 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + W 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + Mo 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + W 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + Mo 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + W 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + Mo 0.1−3eV(Te), T: 500−1700K Exp 1460D+ + W 0.1−3eV(Te), T: 500−1700K Exp 1460D + W 1000eV, T: 300K Exp 1462D + W 1000eV, T: 300K Exp 1462D + W 1000eV, T: 300K Exp 1462D + W 1000eV, T: 300K Exp 1462D + O 10−500eV, T: 300−500K Exp 1464D + C 10−500eV, T: 300−500K Exp 1464D + W 10−500eV, T: 300−500K Exp 1464D + O 10−500eV, T: 300−500K Exp 1464D + C 10−500eV, T: 300−500K Exp 1464D + W 10−500eV, T: 300−500K Exp 1464D + O 10−500eV, T: 300−500K Exp 1464D + C 10−500eV, T: 300−500K Exp 1464D + W 10−500eV, T: 300−500K Exp 1464

83

D + W 10−500eV, T: 300−500K Exp 1464D + C 10−500eV, T: 300−500K Exp 1464D + O 10−500eV, T: 300−500K Exp 1464D + Ti 30−200eV, T: 630−820K Exp 1465D + C 30−200eV, T: 630−820K Exp 1465D + D 25eV, T: 1000K Th 1467D + C 25eV, T: 1000K Th 1467D + D 25eV, T: 1000K Th 1467D + C 25eV, T: 1000K Th 1467D + D 25eV, T: 1000K Th 1467D + C 25eV, T: 1000K Th 1467D + D 25eV, T: 1000K Th 1467D + C 25eV, T: 1000K Th 1467D + W 1−200eV, T: 300K E/T 1468D + Mo 1−200eV, T: 300K E/T 1468D + W 1−200eV, T: 300K E/T 1468D + Mo 1−200eV, T: 300K E/T 1468D + W 1−200eV, T: 300K E/T 1468D + Mo 1−200eV, T: 300K E/T 1468D + W 1−200eV, T: 300K E/T 1468D + Mo 1−200eV, T: 300K E/T 1468D + W 1−200eV, T: 300K E/T 1468D + O 1000eV, T: 300−1000K Exp 1481D + Be 1000eV, T: 300−1000K Exp 1481D + O 1000eV, T: 300−1000K Exp 1481D + Be 1000eV, T: 300−1000K Exp 1481D + O 1000eV, T: 300−1000K Exp 1481D + Be 1000eV, T: 300−1000K Exp 1481D + O 1000eV, T: 300−1000K Exp 1481D + Be 1000eV, T: 300−1000K Exp 1481D + O 1000eV, T: 300−1000K Exp 1481D + Be 1000eV, T: 300−1000K Exp 1481D + W undef, T: 426−654K Exp 1483D + Ta 50eV, T: undef Exp 1486D + W 50eV, T: undef Exp 1486D+ + C 13.3−48.5eV, T: undef Th 1502D+ + W 1000eV, T: 550−1050K Exp 1505D + Be 200eV, T: 300−1023K Exp 1506D + O 200eV, T: 300−1023K Exp 1506D + C 200eV, T: 300−1023K Exp 1506D + Be 200eV, T: 300−1023K Exp 1506D + O 200eV, T: 300−1023K Exp 1506D + C 200eV, T: 300−1023K Exp 1506D + Be 200eV, T: 300−1023K Exp 1506D + O 200eV, T: 300−1023K Exp 1506D + C 200eV, T: 300−1023K Exp 1506D + Be 200eV, T: 300−1023K Exp 1506D + O 200eV, T: 300−1023K Exp 1506D + C 200eV, T: 300−1023K Exp 1506D + WC 100−300eV, T: 600K Th 1507D + WC 100−300eV, T: 600K Th 1507D+ + W 20−60eV, T: 320−593K Exp 1508D+ + W 20−60eV, T: 320−593K Exp 1508D+ + W 20−60eV, T: 320−593K Exp 1508D+ + W 20−60eV, T: 320−593K Exp 1508D + W 100eV, T: 300−1000K E/T 1509D + W 100eV, T: 300−1000K E/T 1509D + W 100eV, T: 300−1000K E/T 1509D + W 100eV, T: 300−1000K E/T 1509

84

D + Be 10−10000eV, T: 300−1300K Th 1511D + W 10−10000eV, T: 300−1300K Th 1511D+ + C 10−10000eV, T: 300−1300K Th 1511D + W 38−500eV, T: 473−673K Exp 1512D + W 38−500eV, T: 473−673K Exp 1512D + W 38−500eV, T: 473−673K Exp 1512D + W 38−500eV, T: 473−673K Exp 1512D+ + C 130−150eV, T: 473K Exp 1514D+ + C 130−150eV, T: 473K Exp 1514D+ + C 130−150eV, T: 473K Exp 1514D+ + C 130−150eV, T: 473K Exp 1514D + W 70eV, T: 420−927K Exp 1517D + W 70eV, T: 420−927K Exp 1517D + W 70eV, T: 420−927K Exp 1517D + W 70eV, T: 420−927K Exp 1517D + Be 50−60eV, T: 573K Exp 1519D + W 50−60eV, T: 573K Exp 1519D + W 50−60eV, T: 573K Exp 1519D + Be 50−60eV, T: 573K Exp 1519D + W 50−60eV, T: 573K Exp 1519D + Be 50−60eV, T: 573K Exp 1519D + W 50−60eV, T: 573K Exp 1519D + Be 50−60eV, T: 573K Exp 1519D + W 170−340eV, T: 300−700K Exp 1522D + W 170−340eV, T: 300−700K Exp 1522D + W 170−340eV, T: 300−700K Exp 1522D + W 170−340eV, T: 300−700K Exp 1522D + W undef, T: undef Exp 1524D + C undef, T: undef Exp 1524D + W undef, T: undef Exp 1524D + C undef, T: undef Exp 1524D + W undef, T: undef Exp 1524D + C undef, T: undef Exp 1524D + C undef, T: undef Exp 1524D + W undef, T: undef Exp 1524D+ + W 30−60eV, T: 300−700K Exp 1525D+ + W 30−60eV, T: 300−700K Exp 1525D+ + W 30−60eV, T: 300−700K Exp 1525D+ + W 30−60eV, T: 300−700K Exp 1525D + W 38eV, T: 285−1000K E/T 1526D + W 38eV, T: 285−1000K E/T 1526D + W 38eV, T: 285−1000K E/T 1526D + W 38eV, T: 285−1000K E/T 1526D + W 2.8−10eV(Te), T: 573K Exp 1527D + W 2.8−10eV(Te), T: 573K Exp 1527D + W 2.8−10eV(Te), T: 573K Exp 1527D + W 2.8−10eV(Te), T: 573K Exp 1527D + W undef, T: 373−1073K Exp 1528D + O undef, T: 373−1073K Exp 1528D + W undef, T: 373−1073K Exp 1528D + W undef, T: 373−1073K Exp 1528D + O undef, T: 373−1073K Exp 1528D + W undef, T: 373−1073K Exp 1528D + O undef, T: 373−1073K Exp 1528D + O undef, T: 373−1073K Exp 1528D + W undef, T: undef Exp 1531D + W undef, T: undef Exp 1531D + W undef, T: undef Exp 1531D + W undef, T: undef Exp 1531

85

D + W undef, T: 360−950K Th 1532D + W undef, T: 360−950K Th 1532D + W ¡100eV, T: 300−900K Exp 1533D + W ¡100eV, T: 300−900K Exp 1533D + W ¡100eV, T: 300−900K Exp 1533D + W ¡100eV, T: 300−900K Exp 1533D+ + Mo 3eV(Te), T: undef Exp 1534D+ + W 3eV(Te), T: undef Exp 1534D+ + Mo 3eV(Te), T: undef Exp 1534D+ + W 3eV(Te), T: undef Exp 1534D+ + Mo 3eV(Te), T: undef Exp 1534D+ + W 3eV(Te), T: undef Exp 1534D+ + Mo 3eV(Te), T: undef Exp 1534D+ + W 3eV(Te), T: undef Exp 1534D+ + W 38−60eV, T: 300−800K E/T 1536D+ + W 38−60eV, T: 300−800K E/T 1536D+ + W 38−60eV, T: 300−800K E/T 1536D+ + W 38−60eV, T: 300−800K E/T 1536D+ + W 38−60eV, T: 300−800K E/T 1536D + C 200eV, T: 300K Exp 1537D + Be 200eV, T: 300K Exp 1537D + C 200eV, T: 300K Exp 1537D + Be 200eV, T: 300K Exp 1537D + C 200eV, T: 300K Exp 1537D + Be 200eV, T: 300K Exp 1537D + C 200eV, T: 300K Exp 1537D + Be 200eV, T: 300K Exp 1537D+ + Mo 70eV, T: 300−900K Exp 1540D+ + W 70eV, T: 300−900K Exp 1540D+ + Mo 70eV, T: 300−900K Exp 1540D+ + W 70eV, T: 300−900K Exp 1540D+ + Mo 70eV, T: 300−900K Exp 1540D+ + W 70eV, T: 300−900K Exp 1540D+ + Mo 70eV, T: 300−900K Exp 1540D+ + W 70eV, T: 300−900K Exp 1540D + W 2eV(Te), T: ¡1600K Exp 1543D + W 2eV(Te), T: ¡1600K Exp 1543D + W 2eV(Te), T: ¡1600K Exp 1543D + W 2eV(Te), T: ¡1600K Exp 1543D + WO3 20−250eV, T: 300K Exp 1546D + W 20−250eV, T: 300K Exp 1546D + WO3 20−250eV, T: 300K Exp 1546D + W 20−250eV, T: 300K Exp 1546D + WO3 20−250eV, T: 300K Exp 1546D + W 20−250eV, T: 300K Exp 1546D + W 20−250eV, T: 300K Exp 1546D + WO3 20−250eV, T: 300K Exp 1546D + W 30000eV,T: 298K Th 1548D + W 30000eV,T: 298K Th 1548D + W 30000eV,T: 298K Th 1548D + W 30000eV,T: 298K Th 1548D + Be undef, T: undef Exp 1549D + Be undef, T: undef Exp 1549D + C undef, T: undef Exp 1549D + C undef, T: undef Exp 1549D + Be undef, T: undef Exp 1549D + C undef, T: undef Exp 1549D + Be undef, T: undef Exp 1549D + C undef, T: undef Exp 1549

86

D + W 17−28eV, T: 497−1000K Exp 1550D + C 17−28eV, T: 497−1000K Exp 1550D + W 17−28eV, T: 497−1000K Exp 1550D + C 17−28eV, T: 497−1000K Exp 1550D + W 17−28eV, T: 497−1000K Exp 1550D + C 17−28eV, T: 497−1000K Exp 1550D + W 17−28eV, T: 497−1000K Exp 1550D + C 17−28eV, T: 497−1000K Exp 1550D + W 40−140eV, T: 323−903K Exp 1551D + W 40−140eV, T: 323−903K Exp 1551D + W 40−140eV, T: 323−903K Exp 1551D + W 40−140eV, T: 323−903K Exp 1551D + W undef, T: 473−773K Exp 1553D + W undef, T: 473−773K Exp 1553D + W undef, T: 473−773K Exp 1553D + W undef, T: 473−773K Exp 1553D + C 50−1000eV, T: 300K Exp 1555D + C 50−1000eV, T: 300K Exp 1555D + C 50−1000eV, T: 300K Exp 1555D + C 50−1000eV, T: 300K Exp 1555D+ + W 200−3000eV, T: 300−600K Th 1556D+ + W 200−3000eV, T: 300−600K Th 1556D+ + W 200−3000eV, T: 300−600K Th 1556D+ + W 200−3000eV, T: 300−600K Th 1556D+ + W 38−500eV, T: 300−643K Exp 1557D+ + W 38−500eV, T: 300−643K Exp 1557D+ + W 38−500eV, T: 300−643K Exp 1557D+ + W 38−500eV, T: 300−643K Exp 1557D+ + W 38−68eV, T: 300−800K Exp 1558D+ + W 38−68eV, T: 300−800K Exp 1558D+ + W 38−68eV, T: 300−800K Exp 1558D+ + W 38−68eV, T: 300−800K Exp 1558D+ + W 3−200eV, T: 320−500K Exp 1559D+ + W 3−200eV, T: 320−500K Exp 1559D+ + W 3−200eV, T: 320−500K Exp 1559D+ + W 3−200eV, T: 320−500K Exp 1559D + W undef, T: undef E/T 1561D + Mo undef, T: undef E/T 1561D + W undef, T: undef E/T 1561D + Mo undef, T: undef E/T 1561D + W undef, T: undef E/T 1561D + Mo undef, T: undef E/T 1561D + W undef, T: undef E/T 1561D + Mo undef, T: undef E/T 1561D + Mo undef, T: 600−2000K Th 1563D + W 100−200eV, T: 298K Exp 1564D + Mo 100−200eV, T: 298K Exp 1564D + W 100−200eV, T: 298K Exp 1564D + W 100−200eV, T: 298K Exp 1564D + Mo 100−200eV, T: 298K Exp 1564D + Mo 100−200eV, T: 298K Exp 1564D + W 100−200eV, T: 298K Exp 1564D + Mo 100−200eV, T: 298K Exp 1564D + W 38−200eV, T: 300−750K Exp 1567D + W 38−200eV, T: 300−750K Exp 1567D + W 38−200eV, T: 300−750K Exp 1567D + W 38−200eV, T: 300−750K Exp 1567D + W 0.5−50eV, T: 298K Th 1571D + W 0.5−50eV, T: 298K Th 1571

87

D+ + W 200eV, T: 300−573K E/T 1579D+ + W 200eV, T: 300−573K E/T 1579D+ + W 200eV, T: 300−573K E/T 1579D+ + W 200eV, T: 300−573K E/T 1579D+ + Li 20−10000eV, T: 473−693K Th 1583D+ + Be 20−160eV, T: undef E/T 1586D+ + Be 0.1−1000eV, T: 400−1400K E/T 1587D+ + Be 0.1−1000eV, T: 400−1400K E/T 1587D + WC undef, T: 273−873K Exp 1588D + BeO undef, T: 273−873K Exp 1588D + BeC undef, T: 273−873K Exp 1588D + W undef, T: 273−873K Exp 1588D + Be undef, T: 273−873K Exp 1588D + C undef, T: 273−873K Exp 1588D + N 2000eV, T: undef Exp 1589D + Be 2000eV, T: undef Exp 1589D + C 100eV, T: ¡313K Exp 1590D + Be 10−100eV, T: undef E/T 1592D + Be 10−100eV, T: 273−1073K E/T 1593D + W 10−100eV, T: 273−1073K E/T 1593D + C 10−100eV, T: 273−1073K E/T 1593D + Be 10−100eV, T: 273−1073K E/T 1593D + W 10−100eV, T: 273−1073K E/T 1593D + C 10−100eV, T: 273−1073K E/T 1593D + Be 10−100eV, T: 273−1073K E/T 1593D + W 10−100eV, T: 273−1073K E/T 1593D + C 10−100eV, T: 273−1073K E/T 1593D + Be 10−100eV, T: 273−1073K E/T 1593D + W 10−100eV, T: 273−1073K E/T 1593D + C 10−100eV, T: 273−1073K E/T 1593D + C 200−1500eV, T: 300−1000K E/T 1594D + W 200−1500eV, T: 300−1000K E/T 1594D + C 200−1500eV, T: 300−1000K E/T 1594D + W 200−1500eV, T: 300−1000K E/T 1594D + W 200−1500eV, T: 300−1000K E/T 1594D + C 200−1500eV, T: 300−1000K E/T 1594D + W 200−1500eV, T: 300−1000K E/T 1594D + C 200−1500eV, T: 300−1000K E/T 1594D + C 50eV, T: 473−973K Th 1596D + W undef, T: 500−1450K Th 1598D+ + Mo undef, T: undef Exp 1602D+ + W undef, T: undef Exp 1602D+ + Mo undef, T: undef Exp 1602D+ + W undef, T: undef Exp 1602D+ + Mo undef, T: undef Exp 1602D+ + W undef, T: undef Exp 1602D+ + Mo undef, T: undef Exp 1602D+ + W undef, T: undef Exp 1602D + W 40−70eV, T: ¡573K Exp 1603D + W 40−70eV, T: ¡573K Exp 1603D + W 40−70eV, T: ¡573K Exp 1603D + W 40−70eV, T: ¡573K Exp 1603D + W ¡50eV, T: ¡480K Exp 1605D + Ta ¡50eV, T: ¡480K Exp 1605D + W ¡50eV, T: ¡480K Exp 1605D + Ta ¡50eV, T: ¡480K Exp 1605D + W ¡50eV, T: ¡480K Exp 1605D + Ta ¡50eV, T: ¡480K Exp 1605D + W ¡50eV, T: ¡480K Exp 1605

88

D + Ta ¡50eV, T: ¡480K Exp 1605D + W 0.5−5eV(Te), T: ¡525K Exp 1606D + W 0.5−5eV(Te), T: ¡525K Exp 1606D + W 0.5−5eV(Te), T: ¡525K Exp 1606D + W 0.5−5eV(Te), T: ¡525K Exp 1606D + W undef, T: 314−773K Exp 1607D + W undef, T: 314−773K Exp 1607D + W undef, T: 314−773K Exp 1607D + W undef, T: 314−773K Exp 1607D + Mo ¡5eV(Te), T: 600−1600K Exp 1608D + W ¡5eV(Te), T: 600−1600K Exp 1608D + Mo ¡5eV(Te), T: 600−1600K Exp 1608D + W ¡5eV(Te), T: 600−1600K Exp 1608D + Mo ¡5eV(Te), T: 600−1600K Exp 1608D + W ¡5eV(Te), T: 600−1600K Exp 1608D + Mo ¡5eV(Te), T: 600−1600K Exp 1608D + W ¡5eV(Te), T: 600−1600K Exp 1608D + Mo ¡5eV(Te), T: 600−1600K Exp 1609D + W ¡5eV(Te), T: 600−1600K Exp 1609D + Mo ¡5eV(Te), T: 600−1600K Exp 1609D + W ¡5eV(Te), T: 600−1600K Exp 1609D + Mo ¡5eV(Te), T: 600−1600K Exp 1609D + W ¡5eV(Te), T: 600−1600K Exp 1609D + Mo ¡5eV(Te), T: 600−1600K Exp 1609D + W ¡5eV(Te), T: 600−1600K Exp 1609D + W undef, T: undef Exp 1610D + W undef, T: undef Exp 1610D + W undef, T: undef Exp 1610D + W undef, T: undef Exp 1610D + W ¡2000eV, T: 1173−1223K 1618D + W 1−250eV, T: 300−1500K 1619D + WC 1−250eV, T: 300−1500K 1619D+ + Be 10−140eV, T: ¡330K 1620D+ + BeD 10−140eV, T: ¡330K 1620D + W 1−100eV(Te), T: undef 1622D + W 1−50eV(Te), T: undef 1624D+ + BeD 5−100eV, T: 300−725K 1626D+ + BeW 5−100eV, T: 300−725K 1626D + W 3000eV, T: 384−673K 1628D + W 3000eV, T: 384−673K 1628D + W 3000eV, T: 384−673K 1628D + W 3000eV, T: 384−673K 1628D + W 1eV, T: 300−850K 1630D + W 1eV, T: 300−850K 1630D + W 1eV, T: 300−850K 1630D + W 1eV, T: 300−850K 1630D + W undef, T: 673−973K 1633D + W undef, T: 673−973K 1633D + W undef, T: 673−973K 1633D + W undef, T: 673−973K 1633D + W 1−400eV, T: 473−773K 1634D + W 1−400eV, T: 473−773K 1634D + W 1−400eV, T: 473−773K 1634D + W 1−400eV, T: 473−773K 1634D + W 5−100eV, T: 600−2000K 1636D + W 200eV, T: 300−623K 1639D + W 200eV, T: 300−623K 1639D + W 200eV, T: 300−623K 1639D + W 200eV, T: 300−623K 1639

89

D + W 200eV, T: 300−623K 1639D + W ¡1.6eV, T: ¡1250K 1641D + W ¡1.6eV, T: ¡1250K 1641D + W ¡1.6eV, T: ¡1250K 1641D + W ¡1.6eV, T: ¡1250K 1641D + W 200eV, T: 320−450K 1647D + W 200eV, T: 320−450K 1647D + W 200eV, T: 320−450K 1647D + W 200eV, T: 320−450K 1647D + W 200eV, T: 320−450K 1647D + W 20eV, T: 300−1200K 1648D + Be undef, T: 570−1333K 1649D + W 1−150eV, T: 403−550K 1653D + W 1−150eV, T: 403−550K 1653D + W 1−150eV, T: 403−550K 1653D + W 1−150eV, T: 403−550K 1653D + W 30eV, T: 500K 1655D + W 30eV, T: 500K 1655D + W 30eV, T: 500K 1655D + W 30eV, T: 500K 1655D+ + Be 1−300eV, T: 273−523K 1656D+ + Be 1−300eV, T: 273−523K 1656D+ + Be 1−300eV, T: 273−523K 1656D+ + Be 1−300eV, T: 273−523K 1656D + W 38−350eV, T: 370−700K 1660D + W 38−350eV, T: 370−700K 1660D + W 38−350eV, T: 370−700K 1660D + W 38−350eV, T: 370−700K 1660D + W 1−150eV, T: 423−1073K 1661D + W 1−150eV, T: 423−1073K 1661D + W 1−150eV, T: 423−1073K 1661D + W 1−150eV, T: 423−1073K 1661D + Be 300−500eV, T: undef 1662D + Be 300−500eV, T: undef 1662D + Be 300−500eV, T: undef 1662D + Be 300−500eV, T: undef 1662D + Be 300−500eV, T: undef 1662D+ + ReW 76eV, T: 350−750K 1663D+ + ReW 76eV, T: 350−750K 1663D+ + ReW 76eV, T: 350−750K 1663D+ + ReW 76eV, T: 350−750K 1663D + W 1000eV, T: 473−873K 1664D + W 1000eV, T: 473−873K 1664D + W 1000eV, T: 473−873K 1664D + W 1000eV, T: 473−873K 1664D+ + W 10−10000eV, T: 298−1600K 1665D+ + W 10−10000eV, T: 298−1600K 1665D+ + W 10−10000eV, T: 298−1600K 1665D+ + W 10−10000eV, T: 298−1600K 1665D + W 5eV, T: 470−560K 1666D + W 100−1500eV, T: 300−473K 1667D + W 100−1500eV, T: 300−473K 1667D + W 100−1500eV, T: 300−473K 1667D + W 100−1500eV, T: 300−473K 1667D + Be 5−100eV, T: 300K 1671D+ + W 60eV, T: 573K 1672D+ + W 60eV, T: 573K 1672D+ + W 60eV, T: 573K 1672D+ + W 60eV, T: 573K 1672

90

D + W 250eV, T: ¡373K 1674D + WC 30−100eV, T: undef 1675D + WC 30−100eV, T: undef 1675D + WC 30−100eV, T: undef 1675D + WC 30−100eV, T: undef 1675D + W 100eV, T: 373−773K 1676D + W 100eV, T: 373−773K 1676D + W 100eV, T: 373−773K 1676D + W 100eV, T: 373−773K 1676D + W 100eV, T: 373−773K 1676D + Be 200eV, T: 398−623K 1678D + BeW 200eV, T: 398−623K 1678D + BeC 200eV, T: 398−623K 1678D + Be 200eV, T: 398−623K 1678D + BeW 200eV, T: 398−623K 1678D + BeC 200eV, T: 398−623K 1678D + Be 200eV, T: 398−623K 1678D + BeW 200eV, T: 398−623K 1678D + BeC 200eV, T: 398−623K 1678D + Be 200eV, T: 398−623K 1678D + BeW 200eV, T: 398−623K 1678D + BeC 200eV, T: 398−623K 1678D + W 50eV, T: 460−510K 1680D + Ta 50eV, T: 460−510K 1680D + W 50eV, T: 460−510K 1680D + Ta 50eV, T: 460−510K 1680D + W 50eV, T: 460−510K 1680D + Ta 50eV, T: 460−510K 1680D + W 50eV, T: 460−510K 1680D + Ta 50eV, T: 460−510K 1680D2

+ + W 30−100 eV, T: 350K Exp 1393D2

+ + C 30−100 eV, T: 350K Exp 1393D2

+ + W 30−300eV, T: 300K Exp 1404D2

+ + C 30−300eV, T: 300K Exp 1404D2 + Be 30−95eV, T: 310−420K Exp 1406D2 + Be 30−95eV, T: 310−420K Exp 1406D2 + Be 30−95eV, T: 310−420K Exp 1406D2 + Be 30−95eV, T: 310−420K Exp 1406D2 + Be 30−95eV, T: 310−420K Exp 1406D2 + C 2−60eV, T: undef E/T 1417D2 + C 2−60eV, T: undef E/T 1417D2 + C 2−60eV, T: undef E/T 1417D2 + C 2−60eV, T: undef E/T 1417D2 + C 2−60eV, T: undef E/T 1417D2 + W ¡75eV, T: 1070−1320K Exp 1501D2

+ + C 13.3−48.5eV, T: undef Th 1502D2

+ + Be 400−3000eV, T: 300K Exp 1504D2

+ + Be 400−3000eV, T: 300K Exp 1504D2

+ + Be 400−3000eV, T: 300K Exp 1504D2

+ + Be 400−3000eV, T: 300K Exp 1504D2

+ + W 1000eV, T: 550−1050K Exp 1505D2

+ + W 20−60eV, T: 320−593K Exp 1508D2

+ + W 20−60eV, T: 320−593K Exp 1508D2

+ + W 20−60eV, T: 320−593K Exp 1508D2

+ + W 20−60eV, T: 320−593K Exp 1508D2

+ + W 30−60eV, T: 300−700K Exp 1525D2

+ + W 30−60eV, T: 300−700K Exp 1525D2

+ + W 30−60eV, T: 300−700K Exp 1525D2

+ + W 30−60eV, T: 300−700K Exp 1525

91

D2+ + W 76eV, T: 400−750K Exp 1538

D2+ + W 76eV, T: 400−750K Exp 1538

D2+ + W 76eV, T: 400−750K Exp 1538

D2+ + W 76eV, T: 400−750K Exp 1538

D2+ + W 38eV, T: 340−1300K Exp 1544

D2+ + W 38eV, T: 340−1300K Exp 1544

D2+ + W 38eV, T: 340−1300K Exp 1544

D2+ + W 38eV, T: 340−1300K Exp 1544

D2+ + W 76eV, T: 300−800K Exp 1545

D2+ + W 76eV, T: 300−800K Exp 1545

D2+ + W 76eV, T: 300−800K Exp 1545

D2+ + W 76eV, T: 300−800K Exp 1545

D2+ + W 38−68eV, T: 300−800K Exp 1558

D2+ + W 38−68eV, T: 300−800K Exp 1558

D2+ + W 38−68eV, T: 300−800K Exp 1558

D2+ + W 38−68eV, T: 300−800K Exp 1558

D2+ + W 3−200eV, T: 320−500K Exp 1559

D2+ + W 3−200eV, T: 320−500K Exp 1559

D2+ + W 3−200eV, T: 320−500K Exp 1559

D2+ + W 3−200eV, T: 320−500K Exp 1559

D2+ + Be 20−160eV, T: undef E/T 1586

D2 + W 30−200eV, T: 420−1100K Exp 1601D2 + W 30−200eV, T: 420−1100K Exp 1601D2 + W 30−200eV, T: 420−1100K Exp 1601D2 + W 30−200eV, T: 420−1100K Exp 1601D2

+ + Be 10−140eV, T: ¡330K 1620D2

+ + BeD 10−140eV, T: ¡330K 1620D2

+ + BeD 5−100eV, T: 300−725K 1626D2

+ + BeW 5−100eV, T: 300−725K 1626D2 + Cd 210eV, T: 300−773K 1627D2 + Cd 210eV, T: 300−773K 1627D2 + Cd 210eV, T: 300−773K 1627D2 + Cd 210eV, T: 300−773K 1627D2 + C 5−8eV 1632D2 + C 5−8eV 1632D2 + C 5−8eV 1632D2 + C 5−8eV 1632D2

+ + W 1000eV, T: ¡373K 1646D2

+ + W 1000eV, T: ¡373K 1646D2

+ + W 1000eV, T: ¡373K 1646D2

+ + W 1000eV, T: ¡373K 1646D2

+ + W 500eV, T: 298K 1650D2

+ + W 500eV, T: 298K 1650D2

+ + W 500eV, T: 298K 1650D2

+ + W 500eV, T: 298K 1650D2

+ + W 500eV, T: 298K 1650D2

+ + Be 1−300eV, T: 273−523K 1656D2

+ + Be 1−300eV, T: 273−523K 1656D2

+ + Be 1−300eV, T: 273−523K 1656D2

+ + Be 1−300eV, T: 273−523K 1656D2

+ + W 110eV, T: ¡373K 1657D2

+ + W 110eV, T: ¡373K 1657D2

+ + W 110eV, T: ¡373K 1657D2

+ + W 110eV, T: ¡373K 1657D2 + W 1−150eV, T: 423−1073K 1661D2 + W 1−150eV, T: 423−1073K 1661D2 + W 1−150eV, T: 423−1073K 1661D2 + W 1−150eV, T: 423−1073K 1661D2

+ + ReW 76eV, T: 350−750K 1663

92

D2+ + ReW 76eV, T: 350−750K 1663

D2+ + ReW 76eV, T: 350−750K 1663

D2+ + ReW 76eV, T: 350−750K 1663

D2+ + W 100−1500eV, T: 300−473K 1667

D2+ + W 100−1500eV, T: 300−473K 1667

D2+ + W 100−1500eV, T: 300−473K 1667

D2+ + W 100−1500eV, T: 300−473K 1667

D3+ + W 30−100 eV, T: 350K Exp 1393

D3+ + C 30−100 eV, T: 350K Exp 1393

D3+ + W 30−300eV, T: 300K Exp 1404

D3+ + C 30−300eV, T: 300K Exp 1404

D3+ + C 13.3−48.5eV, T: undef Th 1502

D3+ + Be 400−3000eV, T: 300K Exp 1504

D3+ + Be 400−3000eV, T: 300K Exp 1504

D3+ + Be 400−3000eV, T: 300K Exp 1504

D3+ + Be 400−3000eV, T: 300K Exp 1504

D3+ + W 1000eV, T: 550−1050K Exp 1505

D3+ + W 20−60eV, T: 320−593K Exp 1508

D3+ + W 20−60eV, T: 320−593K Exp 1508

D3+ + W 20−60eV, T: 320−593K Exp 1508

D3+ + W 20−60eV, T: 320−593K Exp 1508

D3+ + Be 600eV, T: 623K Exp 1521

D3+ + C 600eV, T: 623K Exp 1521

D3+ + W 600eV, T: 623K Exp 1521

D3+ + Be 600eV, T: 623K Exp 1521

D3+ + C 600eV, T: 623K Exp 1521

D3+ + W 600eV, T: 623K Exp 1521

D3+ + Be 600eV, T: 623K Exp 1521

D3+ + C 600eV, T: 623K Exp 1521

D3+ + W 600eV, T: 623K Exp 1521

D3+ + Be 600eV, T: 623K Exp 1521

D3+ + W 600eV, T: 623K Exp 1521

D3+ + C 600eV, T: 623K Exp 1521

D3+ + W 30−60eV, T: 300−700K Exp 1525

D3+ + W 30−60eV, T: 300−700K Exp 1525

D3+ + W 30−60eV, T: 300−700K Exp 1525

D3+ + W 30−60eV, T: 300−700K Exp 1525

D3+ + W 100eV, T: ¿298K Th 1530

D3+ + W 100eV, T: ¿298K Th 1530

D3+ + W 100eV, T: ¿298K Th 1530

D3+ + W 100eV, T: ¿298K Th 1530

D3+ + W 20−200eV, T: 320−593K Exp 1547

D3+ + W 20−200eV, T: 320−593K Exp 1547

D3+ + W 20−200eV, T: 320−593K Exp 1547

D3+ + W 20−200eV, T: 320−593K Exp 1547

D3+ + W 38−800eV, T: 320−470K Exp 1554

D3+ + W 38−800eV, T: 320−470K Exp 1554

D3+ + W 38−800eV, T: 320−470K Exp 1554

D3+ + W 38−800eV, T: 320−470K Exp 1554

D3+ + W 3−200eV, T: 320−500K Exp 1559

D3+ + W 3−200eV, T: 320−500K Exp 1559

D3+ + W 3−200eV, T: 320−500K Exp 1559

D3+ + W 3−200eV, T: 320−500K Exp 1559

D3+ + W 38eV, T: 300K Exp 1560

D3+ + W 38eV, T: 300K Exp 1560

D3+ + W 38eV, T: 300K Exp 1560

D3+ + W 38eV, T: 300K Exp 1560

D3+ + Be 20−160eV, T: undef E/T 1586

D3+ + Be 10−140eV, T: ¡330K 1620

93

D3+ + BeD 10−140eV, T: ¡330K 1620

D3+ + BeD 5−100eV, T: 300−725K 1626

D3+ + BeW 5−100eV, T: 300−725K 1626

D3+ + W 38eV, T: 370−600K 1652

D3+ + W 38eV, T: 370−600K 1652

D3+ + W 38eV, T: 370−600K 1652

D3+ + W 38eV, T: 370−600K 1652

D3+ + Be 1−300eV, T: 273−523K 1656

D3+ + Be 1−300eV, T: 273−523K 1656

D3+ + Be 1−300eV, T: 273−523K 1656

D3+ + Be 1−300eV, T: 273−523K 1656

D3+ + Be 20000−75000eV, T: ¡340K 1677

D3+ + Be 20000−75000eV, T: ¡340K 1677

D3+ + Be 20000−75000eV, T: ¡340K 1677

D3+ + Be 20000−75000eV, T: ¡340K 1677

T + C undef, T: undef Th 1423T + Be undef, T: undef Th 1423T + C undef, T: undef Th 1423T + Be undef, T: undef Th 1423T + C undef, T: undef Th 1423T + Be undef, T: undef Th 1423T + C undef, T: undef Th 1423T + Be undef, T: undef Th 1423T + W 10−1000eV, T: undef Th 1430T + C 1000−4000eV, T: undef Exp 1437T + Ni undef, T: 285−1000K Exp 1482T + W undef, T: 285−1000K Exp 1482T + W 1000eV, T: 473−873K Th 1488T + Mo undef, T: 273−323K Exp 1490T + W undef, T: 273−323K Exp 1490T + C 13.3−48.5eV, T: undef Th 1502T + C 10−10000eV, T: 300−1300K Th 1511T + C undef, T: undef Th 1520T + C undef, T: undef Th 1520T + C undef, T: undef Th 1520T + C undef, T: undef Th 1520T + Be undef, T: undef Exp 1549T + Be undef, T: undef Exp 1549T + W undef, T: undef Exp 1549T + C undef, T: undef Exp 1549T + W undef, T: undef Exp 1549T + Be undef, T: undef Exp 1549T + C undef, T: undef Exp 1549T + C undef, T: undef Exp 1549T + Be undef, T: undef Exp 1549T + W undef, T: undef Exp 1549T + C undef, T: undef Exp 1549T + W undef, T: undef Exp 1549T + W undef, T: 300−750K Th 1552T + W undef, T: 300−750K Th 1552T + W undef, T: 300−750K Th 1552T + W undef, T: 300−750K Th 1552T + W undef, T: 300−750K Th 1552T + Be undef, T: undef E/T 1561T + W undef, T: undef E/T 1561T + C undef, T: undef E/T 1561T + Be undef, T: undef E/T 1561T + W undef, T: undef E/T 1561T + C undef, T: undef E/T 1561

94

T + Be undef, T: undef E/T 1561T + W undef, T: undef E/T 1561T + C undef, T: undef E/T 1561T + Be undef, T: undef E/T 1561T + W undef, T: undef E/T 1561T + C undef, T: undef E/T 1561T + Mo undef, T: 600−2000K Th 1563T + W 200−1500eV, T: 300−1000K E/T 1594T + C 200−1500eV, T: 300−1000K E/T 1594T + W 200−1500eV, T: 300−1000K E/T 1594T + C 200−1500eV, T: 300−1000K E/T 1594T + W 200−1500eV, T: 300−1000K E/T 1594T + C 200−1500eV, T: 300−1000K E/T 1594T + W 200−1500eV, T: 300−1000K E/T 1594T + C 200−1500eV, T: 300−1000K E/T 1594T + W undef, T: 500−1450K Th 1598T + F82H undef, T: undef Th 1604T + Be undef, T: undef Th 1604T + W 200eV, T: 300−623K 1639T + W 200eV, T: 300−623K 1639T + W 200eV, T: 300−623K 1639T + W 200eV, T: 300−623K 1639T + W 200eV, T: 300−623K 1639T + W 140eV, T: 573K 1645T + W 140eV, T: 573K 1645T + W 140eV, T: 573K 1645T + W 140eV, T: 573K 1645T + Be undef, T: 570−1333K 1649T + Be undef, T: 298−1373K 1651T + He undef, T: 298−1373K 1651T + Be undef, T: 298−1373K 1651T + He undef, T: 298−1373K 1651T + Be undef, T: 298−1373K 1651T + He undef, T: 298−1373K 1651T + Be undef, T: 298−1373K 1651T + He undef, T: 298−1373K 1651T + W 400eV, T: 453−573K 1659T + W 400eV, T: 453−573K 1659T + W 400eV, T: 453−573K 1659T + W 400eV, T: 453−573K 1659T + C undef, T: 1273K 1681T + C undef, T: 1273K 1681T + C undef, T: 1273K 1681T + C undef, T: 1273K 1681CH + Be 1−200eV, T: undef Th 1562CH + H 1−200eV, T: undef Th 1562CH + C 1−200eV, T: undef Th 1562CH2 + Be 1−200eV, T: undef Th 1562CH2 + H 1−200eV, T: undef Th 1562CH2 + C 1−200eV, T: undef Th 1562CH3 + Be 1−200eV, T: undef Th 1562CH3 + H 1−200eV, T: undef Th 1562CH3 + C 1−200eV, T: undef Th 1562CH4 + W undef, T: undef Exp 1403CH4 + C undef, T: undef Exp 1403CH4 + H undef, T: undef Exp 1403CH4 + H undef, T: undef Exp 1403CH4 + C undef, T: undef Exp 1403CH4 + W undef, T: undef Exp 1403

95

CH4 + C 3−100eV, T: undef Th 1414CH4 + W 3−100eV, T: undef Th 1414CH4 + H 3−100eV, T: undef Th 1414CH4 + C 3−100eV, T: undef Th 1414CH4 + W 3−100eV, T: undef Th 1414CH4 + H 3−100eV, T: undef Th 1414CH4 + C 1−100eV, T: undef Th 1424CH4 + C 1−100eV, T: undef Th 1424CH4 + W 1−100eV, T: undef Th 1424CH4 + H 1−100eV, T: undef Th 1424CH4 + W 1−100eV, T: undef Th 1424CH4 + H 1−100eV, T: undef Th 1424CH4 + W 1−100eV, T: undef Th 1424CH4 + H 1−100eV, T: undef Th 1424CH4 + C 1−100eV, T: undef Th 1424CH4 + H 1−100eV, T: undef Th 1424CH4 + C 1−100eV, T: undef Th 1424CH4 + W 1−100eV, T: undef Th 1424CH4 + C 1−100eV, T: undef Th 1424CH4 + W 1−100eV, T: undef Th 1424CH4 + H 1−100eV, T: undef Th 1424CH4 + W 1−100eV, T: 1−50eV Th 1542CH4 + H 1−100eV, T: 1−50eV Th 1542CH4 + C 1−100eV, T: 1−50eV Th 1542CH4 + W undef, T: undef E/T 1584CH4 + C undef, T: undef E/T 1584CH4 + C 0.1−1000eV, T: 400−1400K E/T 1587CH4 + C 0.1−1000eV, T: 400−1400K E/T 1587N2 + Be 30−95eV, T: 310−420K Exp 1406N2 + Be 30−95eV, T: 310−420K Exp 1406N2 + Be 30−95eV, T: 310−420K Exp 1406N2 + Be 30−95eV, T: 310−420K Exp 1406N2 + Be 30−95eV, T: 310−420K Exp 1406N2 + C undef, T: 300−600K Exp 1411N2 + D undef, T: 300−600K Exp 1411N2 + B undef, T: 300−600K Exp 1411N2 + H 500−1000eV, T: 460K Exp 1431N2 + C 500−1000eV, T: 460K Exp 1431N2

+ + Be 15−70eV, T: 298−573K 1670N2

+ + W 15−70eV, T: 298−573K 1670N2

+ + BeW 15−70eV, T: 298−573K 1670O2 + H 3eV(Te), T: undef Exp 1445O2 + C 3eV(Te), T: undef Exp 1445C2H4 + W undef, T: undef E/T 1584C2H4 + C undef, T: undef E/T 1584C2H6 + C 3−100eV, T: undef Th 1414C2H6 + H 3−100eV, T: undef Th 1414C2H6 + C 3−100eV, T: undef Th 1414C2H6 + H 3−100eV, T: undef Th 1414undef + W undef, T: undef 1654

2.4 Data Collection, Bibliographic and Progress Report

e + ND4+ 0.001−1eV 1682

e + NH4+ 0.001−1eV 1682

e + CH5+ 0.001−1eV 1682

e + NO+ 0.001−1eV 1682e + H3O

+ 0.001−1eV 1682

96

e + Cl2 0.01 − 100 eV Exp 1683e + Cl2 0.01−100eV E/T 1684e + Cl 5−1E6 keV Th 1685e + S 5−1E6 keV Th 1685e + Al 5−1E6 keV Th 1685e + Mg 5−1E6 keV Th 1685e + Na 5−1E6 keV Th 1685e + O 5−1E6 keV Th 1685e + H 5−1E6 keV Th 1685e + C 5−1E6 keV Th 1685e + Bi 5−1E6 keV Th 1685e + Ta 5−1E6 keV Th 1685e + Xe 5−1E6 keV Th 1685e + Au 5−1E6 keV Th 1685e + Ag 5−1E6 keV Th 1685e + Y 5−1E6 keV Th 1685e + Fe 5−1E6 keV Th 1685e + Si 5−1E6 keV Th 1685e + N 5−1E6 keV Th 1685e + Pt 5−1E6 keV Th 1685e + Os 5−1E6 keV Th 1685e + Re 5−1E6 keV Th 1685e + Hf 5−1E6 keV Th 1685e + Dy 5−1E6 keV Th 1685e + I 5−1E6 keV Th 1685e + U 5−1E6 keV Th 1685e + Pb 5−1E6 keV Th 1685e + W 5−1E6 keV Th 1685e + Tm 5−1E6 keV Th 1685e + Er 5−1E6 keV Th 1685e + Ho 5−1E6 keV Th 1685e + Gd 5−1E6 keV Th 1685e + Eu 5−1E6 keV Th 1685e + Sm 5−1E6 keV Th 1685e + Nd 5−1E6 keV Th 1685e + Pr 5−1E6 keV Th 1685e + Ce 5−1E6 keV Th 1685e + La 5−1E6 keV Th 1685e + Te 5−1E6 keV Th 1685e + Sb 5−1E6 keV Th 1685e + Sn 5−1E6 keV Th 1685e + In 5−1E6 keV Th 1685e + Cd 5−1E6 keV Th 1685e + Pd 5−1E6 keV Th 1685e + Mo 5−1E6 keV Th 1685e + Nb 5−1E6 keV Th 1685e + Zr 5−1E6 keV Th 1685e + Sr 5−1E6 keV Th 1685e + Rb 5−1E6 keV Th 1685e + Kr 5−1E6 keV Th 1685e + Br 5−1E6 keV Th 1685e + Se 5−1E6 keV Th 1685e + As 5−1E6 keV Th 1685e + Ge 5−1E6 keV Th 1685e + Ga 5−1E6 keV Th 1685e + Zn 5−1E6 keV Th 1685e + Cu 5−1E6 keV Th 1685e + Ni 5−1E6 keV Th 1685e + Co 5−1E6 keV Th 1685

97

e + Mn 5−1E6 keV Th 1685e + Cr 5−1E6 keV Th 1685e + V 5−1E6 keV Th 1685e + Ti 5−1E6 keV Th 1685e + Sc 5−1E6 keV Th 1685e + Ca 5−1E6 keV Th 1685e + K 5−1E6 keV Th 1685e + Ar 5−1E6 keV Th 1685e + Xe 0.01−400eV E/T 1686e + Kr 0.01−400eV E/T 1686e + Ne 20−1000eV E/T 1687e + He 20−1000eV E/T 1687e + Ar 0.01−200eV E/T 1688

2.5 Interactions of Atomic Particles with Fields

B5+ + NO 399 −401eV 1689P + He 80−240 eV Th 1690P + He 65−71 eV Th 1691P + Kr 1E1−1E8 K Th 1692P + Kr+ 1E1−1E8 K Th 1692P + Kr2+ 1E1−1E8 K Th 1692P + Kr3+ 1E1−1E8 K Th 1692P + Kr4+ 1E1−1E8 K Th 1692P + Kr5+ 1E1−1E8 K Th 1692P + Kr6+ 1E1−1E8 K Th 1692e + Kr 1E1−1E8 K Th 1692e + Kr+ 1E1−1E8 K Th 1692e + Kr2+ 1E1−1E8 K Th 1692e + Kr3+ 1E1−1E8 K Th 1692e + Kr4+ 1E1−1E8 K Th 1692e + Kr5+ 1E1−1E8 K Th 1692e + Kr6+ 1E1−1E8 K Th 1692

98

Chapter 3

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Configurations in Fluorine-like Ions Between Si VI and W LXVIAt. Data Nucl. Data Tables 99, 431-446 (2013)

F Z= 14-74 Th

48. H. L. Zhang, C. J. FontesRelativistic Distorted-Wave Collision Strengths for the 16 ∆n = 0 Optically AllowedTransitions with n = 2 in the 67 Be-like Ions with 26≤Z≤92At. Data Nucl. Data Tables 99, 416-430 (2013)

Be Z= 26-92 Th

49. M. B. Trzhaskovskaya, V. K. NikulinRadiative Recombination Data for Tungsten Ions: I. W24+–W45+


104

W24+ 30+ Th

50. K. M. Aggarwal, F. P. KeenanEnergy Levels, Radiative Rates, and Electron Impact Excitation Rates for Transitionsin Li-like Ions with 12≤Z≤20At. Data Nucl. Data Tables 99, 156-248 (2013)

Li Z= 12-20 Th

51. J. R. PerssonTable of Hyperfine Anomaly in Atomic SystemsAt. Data Nucl. Data Tables 99, 62-68 (2013)

Ru E/TAg E/TCd E/TIn E/TSn E/TSb E/TCs E/TBa E/TLa E/TNd E/TEu E/TN E/TGd E/TDy E/TYb E/TLu E/TRe E/TIr E/THg E/TAu E/TTl E/TFr E/TU E/TNa E/TK E/TV E/TCu E/TGa E/TLi E/TBr E/TRb E/TMo E/T

52. A. Abou El-Maaref, M. A. M. Uosif, S. H. Allam, Th. M. El-SherbiniThe 4d-4p Transitions and Soft X-ray Laser Wavelengths in Si-like IonsCan. J. Phys. 91, 981-993 (2013)

As19+ ThGa17+ ThGe18+ ThNi14+ ThZn16+ Th

53. E. Giner, A. Scemama, M. CaffarelUsing Perturbatively Selected Configuration Interaction in Quantum Monte CarloCalculationsCan. J. Chem. 91, 879-885 (2013)

105

O Th

54. L. Liang, W.-J. Gao, C. ZhouEnergy Levels, Oscillator Strengths, Radiative Decay Rates, and Fine StructureCollision Strengths for Kr VII LinesCan. J. Phys. 91, 554-559 (2013)

Kr6+ Th

55. S. Aggarwal, A. K. S. Jha, M. MohanMulticonfigurational Dirac-Fock Energy Levels and Radiative Rates for Br-likeTungstenCan. J. Phys. 91, 394-400 (2013)

W39+ Th

56. N. N. Dutta, S. MajumderElectron-Correlation Trends in the Hyperfine A and B Constants of the NaIsoelectronic SequencePhys. Rev. A 88, 062507 (2013)

Si3+ ThP4+ ThS5+ ThCl6+ ThAr7+ ThK8+ ThCa9+ ThSc10+ ThTi11+ ThV12+ Th

57. C. Froese Fischer, S. Verdebout, M. Godefroid, P. Rynkun, P. Jonsson, G. GaigalasDoublet-Quartet Energy Separation in Boron: A Partitioned-Correlation-Function-Interaction MethodPhys. Rev. A 88, 062506 (2013)

B ThC+ Th

58. W. C. Stolte, Z. Felfli, R. Guillemin, G. Ohrwall, S.-W. Yu, J. A. Young, D. W. Lindle, T. W.Gorczyca, N. C. Deb, S. T. Manson, A. Hibbert, A. Z. MsezaneInner-Shell Photoionization of Atomic ChlorinePhys. Rev. A 88, 053425 (2013)

Cl E/TCl0+ + E/T

59. L. NatarajanTwo-Electron One-Photon Transitions in Li-like IonsPhys. Rev. A 88, 052522 (2013)

Ar15+ ThCa17+ ThCd45+ ThFe23+ ThGe29+ ThKr33+ ThMo39+ ThRb34+ Th

106

Ru41+ ThSi11+ ThSn47+ ThSr35+ ThTi19+ ThXe51+ ThY36+ ThZn27+ ThZr37+ Th

60. A. Ong, J. C. Berengut, V. V. FlambaumMeasuring Chemical Evolution and Gravitational Dependence of α Using UltravioletFe V and Ni V Transitions in White-Dwarf SpectraPhys. Rev. A 88, 052517 (2013)

Fe4+ ThNi4+ Th

61. K. Wendt, C. Mattolat, T. Gottwald, T. Kron, S. Raeder, S. Rothe, F. Schwellnus, H. TomitaHyperfine Structure and Isotope Shift in the 3s23p2 3P0,1,2 → 3s23p4p 3P0,1,2 Transitionsin Silicon by Doppler-Free In-Source Two-Photon Resonance-Ionization SpectroscopyPhys. Rev. A 88, 052510 (2013)

Si Exp

62. C. ChenTerm Energies of 1s2nf High Rydberg States for the Lithium AtomPhys. Scr. 88, 045303 (2013)

Li Th

63. G. Xiong, J.-Y. Zhang, Z.-M. Hu, N. Nakamura, Y.-M. Li, X.-Y. Han, J.-M. Yang, B.-H. ZhangKLL Dielectronic-Recombination Measurement for Li-like to O-like GoldPhys. Rev. A 88, 042704 (2013)

Au71+ 76+ Th

64. A. Klose, K. Minamisono, P. F. ManticaCollinear Laser Spectroscopy on the Ground State and an Excited State in Neutral55MnPhys. Rev. A 88, 042701 (2013)

Mn Exp

65. J.-Y. Li, D.-J. Ding, Z.-W. WangExcited-State Energies and Fine Structure of Highly Charged Lithiumlike IonsPhys. Rev. A 88, 042511 (2013)

Li Z= 41-50 Th

66. U. Argaman, G. Makov, E. KraislerHigher Ionization Energies of Atoms in Density-Functional TheoryPhys. Rev. A 88, 042504 (2013)

H-Cu0+ 28+ Th

67. Th. Carette, M. Nemouchi, J.-G. Li, M. GodefroidRelativistic Effects on the Hyperfine Structures of 2p4(3P)3p 2D◦, 4D◦, and 4P◦ in 19F IPhys. Rev. A 88, 042501 (2013)

F Th

107

68. I. Sakho, M. Tine, M. Dieng, M. Sow, M. Faye, B. Diop, M. Gueye, A. WagueEnergy Resonances and Widths of the (2pns)1P◦ and (2pnd) 1P◦ Rydberg Series ofBe-like IonsPhys. Scr. 88, 035302 (2013)

Be Z= 8-18 E/T

69. A. K. Singh, S. Aggarwal, M. MohanLevel Energies, Lifetimes and Radiative Rates in the 4p44d Configurations of Bromine-like IonsPhys. Scr. 88, 035301 (2013)

Br Z= 38-42 Th

70. A. N. Artemyev, V. M. Shabaev, I. I. Tupitsyn, G. Plunien, A. Surzhykov, S. FritzscheAb Initio Calculations of the 2p3/2-2p1/2 Fine-Structure Splitting in Boronlike IonsPhys. Rev. A 88, 032518 (2013)

B Z= 17-100 Th

71. U. I. Safronova, A. S. Safronova, P. BeiersdorferContribution of the 4f-Core-Excited States in Determination of Atomic Properties inthe Promethium Isoelectronic SequencePhys. Rev. A 88, 032512 (2013)

Pm Z= 74-100 Th

72. K. M. Aggarwal, F. P. KeenanEnergy Levels and Radiative Rates for Transitions in Ti XPhys. Scr. 88, 025303 (2013)

Ti9+ E/T

73. K. M. Aggarwal, F. P. Keenan, A. Z. MsezaneEnergy Levels and Radiative Rates for Transitions in Ti VIPhys. Scr. 88, 025302 (2013)

Ti5+ Th

74. G. P. Gupta, A. Z. MsezaneExcitation Energies, Oscillator Strengths and Lifetimes in Mg-like VanadiumPhys. Scr. 88, 025301 (2013)

V11+ Th

75. Y. Hikosaka, M. Fushitani, A. Matsuda, T. Endo, Y. Toida, E. Shigemasa, M. Nagasono, K. Tono,T. Togashi, M. Yabashi, T. Ishikawa, A. HishikawaResonances in Three-Photon Double Ionization of Ar in Intense Extreme-UltravioletFree-Electron Laser Fields Studied by Shot-By-Shot Photoelectron SpectroscopyPhys. Rev. A 88, 023421 (2013)

Ar+ Exp

76. S. Schlesser, S. Boucard, D. S. Covita, J. M. F. dos Santos, H. Fuhrmann, D. Gotta, A. Gruber,M. Hennebach, A. Hirtl, P. Indelicato, E.-O. Le Bigot, L. M. Simons, L. Stingelin, M. Trassinelli,J. F. C. A. Veloso, A. Wasser, J. ZmeskalHigh-Accuracy X-ray Line Standards in the 3-keV RegionPhys. Rev. A 88, 022503 (2013)

108

Ar14+ 16+ ExpCl13+ ExpCl14+ ExpS12+ 14+ Exp

77. Q.-P. Fan, G. Jiang, L.-F. Cao, B.-L. DengCollision Strength Calculations of Ni XXIIIPhys. Scr. 88, 015302 (2013)

Ni22+ Th

78. C. Schimeczek, S. Boblest, D. Meyer, G. WunnerAtomic Ground States in Strong Magnetic Fields: Electron Configurations and EnergyLevelsPhys. Rev. A 88, 012509 (2013)

He-Fe Th

79. M. B. Ruiz, J. T. Margraf, A. M. FrolovHylleraas-Configuration-Interaction Analysis of the Low-Lying States in the Three-Electron Li Atom and Be+ IonPhys. Rev. A 88, 012505 (2013)

Be+ ThLi Th

80. L. Natarajan, R. KadrekarRadiative Decay from Doubly and Singly Excited States of He-like NickelPhys. Rev. A 88, 012501 (2013)

Ni26+ Th

81. J.-L. Liu, Y.-Q. Li, J.-H. Wu, J.-M. YuanNear-Threshold Photodetachment Cross Section of Negative Atomic Boron IonsPhys. Rev. A 87, 065402 (2013)

B− Th

82. T. Lennartsson, J. Clementson, P. BeiersdorferExperimental Wavelengths for Intrashell Transitions in Tungsten Ions with PartiallyFilled 3p and 3d SubshellsPhys. Rev. A 87, 062505 (2013)

W47+ 61+ Exp

83. J. D. Gillaspy, D. Osin, Yu. Ralchenko, J. Reader, S. A. BlundellTransition Energies of the D Lines in Na-like IonsPhys. Rev. A 87, 062503 (2013)

Na Z= 18-92 E/TBa45+ E/TBi72+ E/TDy55+ E/TEr57+ E/TGd53+ E/TPt67+ E/TSm51+ E/TW63+ E/TXe43+ E/T

109

84. K. M. Aggarwal, F. P. KeenanEnergy Levels, Radiative Rates and Electron Impact Excitation Rates for Transitionsin He-like Fe XXV, Co XXVI, Ni XXVII, Cu XXVIII and Zn XXIXPhys. Scr. 87, 055302 (2013)

Co25+ ThCu27+ ThFe24+ ThNi26+ ThZn28+ Th

85. Z.-M. Hu, Y.-M. Li, N. NakamuraResonance Strength for KLL Dielectronic Recombination of Hydrogenlike KryptonPhys. Rev. A 87, 052706 (2013)

Kr32+ ThKr33+ Th

86. S. BouazzaHyperfine Structure and Isotope Shift Analysis of Singly Ionized TitaniumPhys. Scr. 87, 045301 (2013)

Ti+ Th

87. A. K. BhatiaHybrid Theory of P-Wave Electron-Li2+ Elastic Scattering and Photoabsorption inTwo-Electron SystemsPhys. Rev. A 87, 042705 (2013)

He Z= 1-3 ThHe Z= 2-3 Th

88. Y. Tang, L.-M. Wang, X.-Y. Song, X.-F. Wang, Z.-C. Yan, H.-X. QiaoBound-State Energies of Lithium in Magnetic Fields Using Hylleraas Basis FunctionsPhys. Rev. A 87, 042518 (2013)

Li Th

89. S. Bubin, L. AdamowiczPrediction of 2S Rydberg Energy Levels of 6Li and 7Li Based on Quantum-MechanicalCalculations Performed with Explicitly Correlated Gaussian FunctionsPhys. Rev. A 87, 042510 (2013)

Li E/T

90. S. BouazzaThe Second Spectrum of Niobium: II. Accurate Fine Structure Study of Odd-ParityLevelsPhys. Scr. 87, 035303 (2013)

Nb+ E/T

91. S. BouazzaThe Second Spectrum of Niobium: I. Accurate Fine Structure Study of Even-ParityLevelsPhys. Scr. 87, 035302 (2013)

Nb+ Th

110

92. Jiaolong Zeng, P.-F. Liu, W.-J. Xiang, J.-M. YuanLevel-To-Level and Total Probability for Auger Decay Including Direct DoubleProcesses of Ar 2p−1 Hole StatesPhys. Rev. A 87, 033419 (2013)

Ar Th

93. Y. Sun, B. C. Gou, C. ChenEnergies and the Radiative and Auger Transition Rates of 1s2p4 Resonances of B-likeIonsPhys. Rev. A 87, 032509 (2013)

B Z= 6-10 step 2 E/TB Z= 6-14 step 2 E/T

94. U. I. Safronova, A. S. Safronova, P. BeiersdorferRelativistic Many-Body Calculations of Excitation Energies, Oscillator Strengths,Transition Rates, and Lifetimes in Samariumlike IonsPhys. Rev. A 87, 032508 (2013)

Sm Z= 74-100 Th

95. R. C. Brown, S.-J. Wu, J. V. Porto, C. J. Sansonetti, C. E. Simien, S. M. Brewer, J. N. Tan, J. D.GillaspyQuantum Interference and Light Polarization Effects in Unresolvable Atomic Lines:Application to a Precise Measurement of the 6,7Li D2 LinesPhys. Rev. A 88, 069902 (2013)

Li Exp

96. M. Puchalski, D. Kedziera, K. PachuckiD1 and D2 Lines in 6Li and 7Li Including QED EffectsPhys. Rev. A 87, 032503 (2013)

Li Th

97. U. I. Safronova, M. S. SafronovaRelativistic Many-Body Calculation of Energies, Lifetimes, Polarizabilities, andHyperpolarizabilities in Li-like Be+

Phys. Rev. A 87, 032502 (2013)

Be+ Th

98. D. von Lindenfels, M. Wiesel, D. A. Glazov, A. V. Volotka, M. M. Sokolov, V. M. Shabaev, G.Plunien, W. Quint, G. Birkl, A. Martin, M. VogelExperimental Access to Higher-Order Zeeman Effects by Precision Spectroscopy ofHighly Charged Ions in a Penning TrapPhys. Rev. A 87, 023412 (2013)

Ar13+ Th

99. F. B. Rosmej, B. Deschaud, K. Bennadji, P. Indelicato, J. P. MarquesFine-Structure Electric-Dipole Matrix Elements of He-like Ions for X-ray Line-ShapeCalculationsPhys. Rev. A 87, 022515 (2013)

Al11+ Th

100. Q.-P. Fan, G. Jiang, L.-F. Cao, W.-H. Wang, S. DuCollision Strengths for Transitions of Ni XXIEur. Phys. J. D 67, 255 (2013)

111

Ni20+ Th

101. J. C. Aguiar, M. Raineri, H. O. Di RoccoThe Study of the 4s4p Configuration of the Zn Isoelectronic Sequence Using theRelativistic jj-Coupling ApproachEur. Phys. J. D 67, 158 (2013)

Zn Z= 50-92 E/T

102. Y. Sun, F. Chen, C. Chen, B. C. GouRadiative and Auger Transitions of Core-Excited States for the Boron IsoelectronicSequenceEur. Phys. J. D 67, 88 (2013)

Mg7+ E/TNe5+ E/TO3+ E/TSi9+ E/T

103. T. I. Madeira, P. Amorim, F. Parente, P. Indelicato, J. P. MarquesAnalysis of the Quasicontinuum Band Emitted by Highly Ionised Tungsten Atoms inthe 4–7 nm RangeEur. Phys. J. D 67, 12 (2013)

W27+ 37+ Th

104. Z.-D. Mu, Q.-Y. WeiTheoretical Study of Level Structure and Transitions of Configurations 3d94s2, 3d94s4p,3d94p2 for Nb XIIIActa Phys. Sin. 62, 103101 (2013)

Nb12+ Th

105. C.-Y. Li, T.-T. Wang, J.-F. Zhen, Y. ChenLine-Profile Analysis of Excitation Spectroscopy in the Even 4p5(2P1/2)nl′ [K′]J(l′ = 1,3) Autoionizing Resonances of KrSci. China Chemistry 56, 1623-1632 (2013)

Kr Exp

106. Y. Liu, T. Gottwald, C. C. Havener, C. Mattolat, C. R. Vane, K. WendtResonant Three-Photon Ionization Spectroscopy of Atomic FeJ. Phys. B 46, 245003 (2013)

Fe Exp

107. J. L. Zeng, P. F. Liu, W. J. Xiang, J. M. YuanComplete Auger Decay Pathways of Kr 3d−1 Hole Levels Including Direct DoubleProcessesJ. Phys. B 46, 215002 (2013)

Kr+ 3+ Th

108. M. M. Al Shorman, M. F. Gharaibeh, J. M. Bizau, D. Cubaynes, S. Guilbaud, N. El Hassan, C.Miron, C. Nicolas, E. Robert, I. Sakho, C. Blancard, B. M. McLaughlinK-Shell Photoionization of Be-like and Li-like Ions of Atomic Nitrogen: Experimentand TheoryJ. Phys. B 46, 195701 (2013)

N3+ 4+ E/T

112

109. L. C. Gao, D. H. Zhang, L. Y. Xie, J. G. Wang, Y. L. Shi, C. Z. DongTheoretical Study of the Photoionization Process of Ne-like Ar, Fe, Kr and Xe IonsJ. Phys. B 46, 175402 (2013)

Ar9+ ThFe16+ ThKr26+ ThXe44+ Th

110. C. T. Chantler, L. F. Smale, J. A. Kimpton, D. N. Crosby, M. N. Kinnane, A. J. IlligCharacterization of the Titanium Kβ Spectral ProfileJ. Phys. B 46, 145601 (2013)

Ti ExpV Exp

111. O. Zatsarinny, K. BartschatThe B-Spline R-Matrix Method for Atomic Processes: Application to AtomicStructure, Electron Collisions and PhotoionizationJ. Phys. B 46, 112001 (2013)

F Th

112. T. Carette, M. R. GodefroidIsotope Shift on the Chlorine Electron Affinity Revisited by an MCHF/CI ApproachJ. Phys. B 46, 095003 (2013)

Cl ThCl− Th

113. O. Zabaydullin, J. DubauPhotoionization and Photoabsorption of Li-like Neon Near 1s2p(1P)2s 2P AutoionizingStatesJ. Phys. B 46, 075005 (2013)

Ne7+ Th

114. M. Guerra, P. Amaro, C. I. Szabo, A. Gumberidze, P. Indelicato, J. P. SantosAnalysis of the Charge State Distribution in an ECRIS Ar Plasma UsingHigh-Resolution X-ray SpectraJ. Phys. B 46, 065701 (2013)

Ar14+ 16+ E/T

115. N. G. Shchukina, I. E. Vasil’evaOscillator Strengths for Selected Fe II Lines in the Range λλ 300–400 nmKinemat. Phys. Celest. Bodies 29, 53-65 (2013)

Fe+ Exp

116. C.-Y. Li, T.-T. Wang, J.-F. Zhen, Y. Chen, Z.-W. HeLine-Profile Analysis of Excitation Spectroscopy in Even 5p5(2P1/2)nl′ [K′]J (l′ = 1, 3)Autoionizing Resonances of XeChin. J. Chem. Phys. 26, 374-380 (2013)

Xe Exp

117. C.-Y. Li, Z.-W. He, T.-T. Wang, J.-F. Zhen, Y. Chen, J.-S. ZhangResonance-Enhanced Photon Excitation Spectroscopy of the Even-Parity 3p5(2P1/2)nl′

[K′]J (l′ = 1, 3) Autoionizing Rydberg States of ArChin. J. Chem. Phys. 26, 259-264 (2013)

113

Ar Exp

118. H. Liu, G. Jiang, F. Hu, C.-K. Wang, Z.-B. Wang, J.-M. YangIntercombination Transitions of the Carbon-like Isoelectronic SequenceChin. Phys. B 22, 073202 (2013)

C Z= 7-92 Th

119. S. Aggarwal, J. Singh, M. MohanNew Atomic Data for Kr XXXV Useful in Fusion PlasmaChin. Phys. B 22, 033201 (2013)

Kr34+ Th

120. C. Gao, F.-T. Jin, J.-L. Zeng, J.-M. YuanPopulation Kinetics and M Band Emission Spectra of Gold Plasmas in Non-LocalThermodynamic Equilibrium by Using a Detailed Relativistic Configuration ApproachNew J. Phys. 15, 015022 (2013)

Au41+ 53+ Th

121. A. Dasgupta, R. W. Clark, A. Giuliani, N. D. Ouart, B. Jones, D. J. Ampleford, S. B. HansenK-α Emission Spectroscopic Analysis from a Cu Z-PinchHigh En. Dens. Phys. 9, 347-353 (2013)

Cu19+ E/TFe16+ E/TNi18+ E/T

122. C. ChenEnergies, Fine Structures, and Hyperfine Structures of the 1s22snp 3P (n = 2–4) Statesfor the Beryllium AtomJ. At. Mol. Opt. Phys. (Hindawi) 2012, 569876 (2012)

Be Th

123. S. Civis, M. Ferus, P. Kubelık, V. E. Chernov, E. M. ZanozinaLi I Spectra in the 4.65–8.33 Micron Range: High-L States and Oscillator StrengthsAstron. Astrophys. 545, p.A61 (2012)

Li Exp

124. S. Hamasha, R. AlshaiubConstructing Theoretical M-Shell Spectra for Mg-like Au through Cl-like Au Ions inGold Plasma DiagnosticsPhys. Scr. 86, 065302 (2012)

Au62+ 67+ Th

125. K. Kubicek, J. Braun, H. Bruhns, J. R. Crespo Lopez-Urrutia, P. H. Mokler, J. UllrichHigh-Precision Laser-Assisted Absolute Determination of X-ray Diffraction AnglesRev. Sci. Instrum. 83, 013102 (2012)

Ar16+ Exp

126. J. P. Marques, P. Indelicato, F. ParenteRelativistic Multiconfiguration Calculations of the 2s22p 2P3/2 Level Lifetime Alongthe Boron Isoelectronic SequenceEur. Phys. J. D 66, 324 (2012)

114

Au74+ ThBi78+ ThGd59+ ThKr31+ ThB Z= 14-35 ThU87+ ThXe49+ Th

127. D. Osin, J. D. Gillaspy, J. Reader, Yu. RalchenkoEUV Magnetic-Dipole Lines from Highly-Charged High-Z Ions with an Open 3d ShellEur. Phys. J. D 66, 286 (2012)

Au51+ 60+ E/TAu51+ 62+ E/THf44+ 54+ E/THf44+ 55+ E/TTa45+ 56+ E/TTa45+ 57+ E/T

128. S. Civis, I. Matulkova, J. Cihelka, P. Kubelık, K. Kawaguchi, V. E. ChernovLow-Excited f-, g- and h-States in Au, Ag and Cu Observed by Fourier-TransformInfrared Spectroscopy in the 1000–7500 cm−1 RegionJ. Phys. B 44, 105002 (2012)

Ag ExpAu ExpCu Exp

129. E. B. SalomanEnergy Levels and Observed Spectral Lines of Neutral and Singly Ionized Chromium,Cr I and Cr IIJ. Phys. Chem. Ref. Data 41, 043103 (2012)

Cr0+ + Exp

130. X.-N. Cao, M.-G. Su, D.-X. Sun, Y.-B. Fu, C.-Z. DongTheoretical Analysis of 4f and 5p Inner-Shell Excitations of W–W3+ IonsChin. Phys. Lett. 29, 113202 (2012)

W0+ 3+ Th

131. P. Beiersdorfer, M. J. May, J. H. Scofield, S. B. HansenAtomic Physics and Ionization Balance of High-Z Ions: Critical Ingredients forCharacterizing and Understanding High-Temperature PlasmasHigh En. Dens. Phys. 8, 271-283 (2012)

Au0+ 78+ ThW0+ 73+ Th

132. E. Kraisler, G. Makov, I. KelsonEnsemble v-Representable Ab Initio Density-Functional Calculation of Energy andSpin in Atoms: A Test of Exchange-Correlation ApproximationsPhys. Rev. A 82, 042516 (2010)

H-Rn Th

133. K. Kawaguchi, N. Sanechika, Y. Nishimura, R. Fujimori, T. N. Oka, Y. Hirahara, A. I. Jaman, S.CivisTime-Resolved Fourier Transform Infrared Emission Spectroscopy of Laser AblationProductsChem. Phys. Lett. 463, 38-41 (2008)

115

Al ExpCu ExpFe ExpZn Exp

134. R. F. Heeter, S. B. Hansen, K. B. Fournier, M. E. Foord, D. H. Froula, A. J. Mackinnon, M. J.May, M. B. Schneider, B. K. F. YoungBenchmark Measurements of the Ionization Balance of Non-Local-Thermodynamic-Equilibrium Gold PlasmasPhys. Rev. Lett. 99, 195001 (2007)

Au41+ 51+ Exp

135. F. Kerber, G. Nave, C. J. Sansonetti, P. Bristow, A. Rosa, H.-U. Kaufl, M. R. RosaThe Spectrum of Th-Ar Hollow Cathode Lamps in the 900–4500 nm Region:Establishing Wavelength Standards for the Calibration of VLT SpectrographsProc. SPIE 6269, p.62692O (2006)

Ar0+ + ExpTh0+ + Exp

136. K. L. Wong, M. J. May, P. Beiersdorfer, K. B. Fournier, B. Wilson, G. V. Brown, P. Springer, P.A. Neill, C. L. HarrisDetermination of the Charge State Distribution of a Highly Ionized Coronal Au PlasmaPhys. Rev. Lett. 90, 235001 (2003)

Au44+ 51+ Exp

137. S. H. Glenzer, K. B. Fournier, B. G. Wilson, R. W. Lee, L. J. SuterIonization Balance in Inertial Confinement Fusion HohlraumsPhys. Rev. Lett. 87, 045002 (2001)

Au47+ 53+ Exp

138. M. E. Foord, S. H. Glenzer, R. S. Thoe, K. L. Wong, K. B. Fournier, B. G. Wilson, P. T. SpringerIonization Processes and Charge-State Distribution in a Highly Ionized High-Z Laser-Produced PlasmaPhys. Rev. Lett. 85, 992-995 (2000)

Au47+ 52+ Exp

139. A. Alonso-Medina, C. ColonInterpretation of the Spectrum of Sn II: Experimental and Theoretical TransitionProbabilitiesPhys. Scr. 61, 646-651 (2000)

Sn+ Exp

140. A. J. J. Raassen, P. H. M. UylingsCritical Evaluation of Calculated and Experimental Transition Probabilities andLifetimes for Singly Ionized Iron Group ElementsJ. Phys. B 31, 3137-3146 (1998)

As5+ ThCo+ ThCo3+ ThCo4+ ThCr+ ThCu3+ 5+ ThFe+ 5+ Th

116

Ga3+ 5+ ThGe4+ 5+ ThMn2+ 5+ ThNi3+ 5+ ThTi2+ ThV3+ ThZn3+ 5+ Th

141. A. J. J. Raassen, P. H. M. UylingsThe Use of Complete Sets of Orthogonal Operators in Spectroscopic StudiesPhys. Scr. T65, 84-87 (1996)

Fe2+ 5+ ThMn2+ ThMn4+ ThNi3+ ThNi4+ ThTi2+ ThV3+ Th

142. S. Bashkin, E. Trabert, D. A. Thiede, P. C. Sercel, P.-C. Lin, M.-L. Li, D. G. Jenkins, D. E.Shemansky, K. Wells, R. Bruch, S. Fulling, D. DeWittExcitation of Nitrogen by Fast H+

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N0+ + Exp

143. A. D. ThackerayThe Evolution of the Nebular Spectrum of the Slow Nova RR TelescopiiMem. R. Astron. Soc. 83, 1-68 (1977)

Ar2+ 4+ ExpCa4+ 6+ ExpCo+ 2+ ExpCo5+ 6+ ExpCr3+ 4+ ExpCu+ ExpCu3+ ExpFe+ 6+ ExpK3+ 5+ ExpMn2+ 5+ ExpNi2+ 4+ ExpNi6+ Exp

144. L. H. Aller, R. S. Polidan, E. J. Rhodes Jr., G. W. WaresThe Spectrum of RR Telescopii in 1968Astrophys. Space Sci. 20, 93-110 (1973)

Ar2+ 4+ ExpC+ 3+ ExpCa+ ExpCa4+ 5+ ExpCr+ 4+ ExpCu+ ExpFe+ 7+ ExpHe0+ + ExpK3+ ExpMg0+ + ExpMn+ ExpMn3+ 4+ Exp

117

N+ 3+ ExpNa3+ ExpNe+ 4+ ExpNi+ ExpNi3+ ExpO0+ 3+ ExpS+ 2+ ExpSc+ ExpSi+ ExpTi+ ExpV+ 3+ ExpZr+ Exp

145. L. H. Aller, I. S. Bowen, R. MinkowskiThe Spectrum of NGC 7027Astrophys. J. 122, 62-71 (1955)

Ar2+ 4+ ExpC+ 3+ ExpCa4+ ExpCa6+ ExpCl2+ 3+ ExpF3+ ExpFe2+ ExpFe4+ 6+ ExpHe0+ + ExpK3+ 5+ ExpMg ExpMn4+ 5+ ExpN0+ 2+ ExpNe2+ 4+ ExpO0+ 4+ ExpS0+ 2+ ExpSi+ 2+ Exp

146. J. Clementson, P. Beiersdorfer, T. Brage, M. F. GuAtomic data and theoretical X-ray spectra of Ge-like through V-like W ionsAt. Data Nucl. Data Tables 100, 577-649 (2014)

W42+ 51+ Th

147. P. Rynkun, P. Jonsson, G. Gaigalas, C. Froese FischerEnergies and E1, M1, E2, and M2 transition rates for states of the 2s22p3, 2s2p4, and2p5 configurations in nitrogen-like ions between F III and Kr XXXAt. Data Nucl. Data Tables 100, 315-402 (2014)

N Z= 9-36 Th

148. Y. Sun, F. Chen, C. Chen, B. C. GouEnergies, fine structure, and radiative transitions of the high-lying core-excited states6Se,o(n) and 6Pe,o(n) (n = 1–5) for the boron isoelectronic sequenceAt. Data Nucl. Data Tables 100, 286-296 (2014)

B Z= 6-10 Th

149. P. Jonsson, P. Bengtsson, J. Ekman, S. Gustafsson, L. B. Karlsson, G. Gaigalas, C. Froese Fischer,D. Kato, I. Murakami, H. A. Sakaue, H. Hara, T. Watanabe, N. Nakamura, N. YamamotoRelativistic CI calculations of spectroscopic data for the 2p6 and 2p53l configurationsin Ne-like ions between Mg III and Kr XXVIIAt. Data Nucl. Data Tables 100, 1-154 (2014)

118

Ne Z= 12-36 Th

150. M. P. Ruffoni, C. Allende Prieto, G. Nave, J. C. PickeringInfrared laboratory oscillator strengths of Fe I in the H-bandAstrophys. J. 779, 17 (2013)

Fe Exp

151. P. Rynkun, P. Jonsson, G. Gaigalas, C. Froese FischerEnergies and E1, M1, E2, and M2 transition rates for states of the 2s22p4, 2s2p5, and2p6 configurations in oxygen-like ions between F II and Kr XXIXAstron. Astrophys. 557, p.A136 (2013)

O Z= 9-36 Th

152. S. Civis, M. Ferus, V. E. Chernov, E. M. ZanozinaInfrared transitions and oscillator strengths of Ca and MgAstron. Astrophys. 554, p.A24 (2013)

Ca ThMg Th

153. G. Del Zanna, P. J. StoreyAtomic data for astrophysics: Fe XI soft X-ray linesAstron. Astrophys. 549, p.A42 (2013)

Fe10+ Th

154. C. Colon, C. Moreno-Dıaz, A. Alonso-MedinaTheoretical Stark broadening parameters for spectral lines arising from the 2p5ns,2p5np and 2p5nd electronic configurations of Mg IIIMon. Not. R. Astron. Soc. 435, 1749-1757 (2013)

Mg2+ Th

155. M. P. Ruffoni, J. C. PickeringAccurate Ritz wavelengths of parity-forbidden [Co II] and [V II] lines of astrophysicalinterestAstrophys. J., Suppl. Ser. 207, 20 (2013)

Co+ ThV+ Th

156. F. Dıaz, M. J. Vilkas, Y. Ishikawa, P. BeiersdorferHigh-Accuracy MR-MP perturbation theory energy and radiative rates calculationsfor core-excited transitions in Fe XVIAstrophys. J., Suppl. Ser. 207, 11 (2013)

Fe15+ Th

157. A. Kramida, J. E. SansonettiEnergy levels and spectral lines of singly ionized manganese (Mn II)Astrophys. J., Suppl. Ser. 205, 14 (2013)

Mn+ E/T

158. J. E. Lawler, A. Guzman, M. P. Wood, C. Sneden, J. J. CowanImproved log(gf) values for lines of Ti I and abundance determinations in thephotospheres of the sun and metal-poor star HD 84937 (accurate transitionprobabilities for Ti I)Astrophys. J., Suppl. Ser. 205, 11 (2013)

119

Ti Exp

159. O. Yu. Khetselius, T. A. Florko, A. A. Svinarenko, T. B. TkachRadiative and collisional spectroscopy of hyperfine lines of the Li-like heavy ions andTl atom in an atmosphere of inert gasesPhys. Scr. T153, 014037 (2013)

Ca17+ ThFe23+ ThMo39+ ThSn47+ ThTm66+ ThYb67+ ThZn27+ Th

160. L. Ozdemir, G. G. Konan, S. KabakciEnergies and radiative transition parameters for Mg-like tungstenActa Phys. Pol. A 124, 649-657 (2013)

W62+ Th

161. A. KramidaCritically evaluated energy levels and spectral lines of singly ionized indium (In II)J. Res. Nat. Inst. Stand. Technol. 118, 52-104 (2013)

In+ E/T

162. C. C. Sang, B. C. Gou, F. WangDecay processes of the core-excited states 1s2s2p2 for Be-like systemsJ. Quant. Spectrosc. Radiat. Transfer 116, 17-23 (2013)

Be Z= 8-28 step 2 Th

163. I. L. Glukhov, E. A. Nikitina, V. D. OvsiannikovLifetimes of Rydberg states in ions of the group II elementsOpt. Spectrosc. 115, 9-17 (2013)

Ba+ ThBe+ ThCa+ ThCd+ ThHg+ ThMg+ ThSr+ ThZn+ Th

164. S. Aggarwal, J. Singh, M. MohanBreit-Pauli atomic structure calculations for Fe XIAt. Data Nucl. Data Tables 99, 704-732 (2013)

Fe10+ Th

165. T. Sochi, P. J. StoreyDielectronic recombination lines of C+


C+ Th

166. S. HamashaEnergy levels, wavelengths, and transition rates of multipole transitions (E1, E2, M1,M2) in Au67+ and Au66+ ionsAt. Data Nucl. Data Tables 99, 595-632 (2013)

120

Au66+ 67+ Th

167. P. Bogdanovich, R. KisieliusTheoretical energy level spectra and transition data for 4p64d2, 4p64d4f, and 4p54d3

configurations of W36+


W36+ Th

168. F. El-SayedEnergies, wavelengths, and multipole transition probabilities for B-like Fe and Ga ionsAt. Data Nucl. Data Tables 99, 545-579 (2013)

Fe21+ ThGa26+ Th

169. P. Oliver, A. HibbertE1 oscillator strengths and transition rates among levels of Cl IAt. Data Nucl. Data Tables 99, 459-496 (2013)

Cl Th

170. P. Jonsson, A. Alkauskas, G. GaigalasEnergies and E1, M1, E2 transition rates for states of the 2s22p5 and 2s2p6

configurations in fluorine-like ions between Si VI and W LXVIAt. Data Nucl. Data Tables 99, 431-446 (2013)

F Z= 14-74 Th

171. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates, and electron impact excitation rates for transitions inLi-like ions with 12≤Z≤20At. Data Nucl. Data Tables 99, 156-243 (2013)

Li Z= 12-20 Th

172. A. Abou El-Maaref, M. A. M. Uosif, S. H. Allam, Th. M. El-SherbiniThe 4d-4p transitions and soft X-ray laser wavelengths in Si-like ionsCan. J. Phys. 91, 981-993 (2013)

As19+ ThGa17+ ThGe18+ ThNi14+ ThZn16+ Th

173. L. Liang, W.-J. Gao, C. ZhouEnergy levels, oscillator strengths, radiative decay rates, and fine structure collisionstrengths for Kr VII linesCan. J. Phys. 91, 554-559 (2013)

Kr6+ Th

174. S. Aggarwal, A. K. S. Jha, M. MohanMulticonfigurational Dirac-Fock energy levels and radiative rates for Br-like tungstenCan. J. Phys. 91, 394-400 (2013)

W39+ Th

175. L. NatarajanTwo-Electron one-photon transitions in Li-like ionsPhys. Rev. A 88, 052522 (2013)

121

Ar15+ ThCa17+ ThCd45+ ThFe23+ ThGe29+ ThKr33+ ThMo39+ ThRb34+ ThRu41+ ThSi11+ ThSn47+ ThSr35+ ThTi19+ ThXe51+ ThY36+ ThZn27+ ThZr37+ Th

176. A. K. Singh, S. Aggarwal, M. MohanLevel energies, lifetimes and radiative rates in the 4p44d configurations of bromine-likeionsPhys. Scr. 88, 035301 (2013)

Br Z= 38-42 Th

177. U. I. Safronova, A. S. Safronova, P. BeiersdorferContribution of the 4f-core-excited states in determination of atomic properties in thepromethium isoelectronic sequencePhys. Rev. A 88, 032512 (2013)

Au18+ E/TW13+ E/TPm Z= 74-100 E/T

178. K. M. Aggarwal, F. P. KeenanEnergy levels and radiative rates for transitions in Ti XPhys. Scr. 88, 025303 (2013)

Ti9+ Th

179. K. M. Aggarwal, F. P. Keenan, A. Z. MsezaneEnergy levels and radiative rates for transitions in Ti VIPhys. Scr. 88, 025302 (2013)

Ti5+ Th

180. G. P. Gupta, A. Z. MsezaneExcitation energies, oscillator strengths and lifetimes in Mg-like vanadiumPhys. Scr. 88, 025301 (2013)

V11+ Th

181. R. Karpuskiene, P. Bogdanovich, R. KisieliusSignificance of M2 and E3 transitions for 4p54dN+1- and 4p64dN−14f-configurationmetastable-level lifetimesPhys. Rev. A 88, 022519 (2013)

Mo Z= 50-92 ThRh Z= 50-92 ThSr Z= 50-92 Th

122

182. J. Grumer, W.-X. Li, D. Bernhardt, J.-G. Li, S. Schippers, T. Brage, P. Jonsson, R. Hutton, Y.-M.ZouEffect of an external magnetic field on the determination of E1M1 two-photon decayrates in Be-like ionsPhys. Rev. A 88, 022513 (2013)

Be Z= 5-92 Th

183. Y.-J. Cheng, J. Jiang, J. MitroyTune-out wavelengths for the alkaline-earth-metal atomsPhys. Rev. A 88, 022511 (2013)

Ba ThBe ThCa ThMg ThSr ThYb Th

184. J.-G. Li, J. Grumer, W.-X. Li, M. Andersson, T. Brage, R. Hutton, P. Jonsson, Y. Yang, Y.-M.ZouTheoretical investigation of magnetic-field-induced 2p53s 3P0,2 – 2p6 1S0 transitions inNe-like ions without nuclear spinPhys. Rev. A 88, 013416 (2013)

Mg2+ ThSi4+ ThS6+ ThAr8+ ThCa10+ ThTi12+ ThCr14+ ThFe16+ ThNi18+ ThZn20+ ThNe Z= 12-30 Th

185. L. Natarajan, R. KadrekarRadiative decay from doubly and singly excited states of He-like nickelPhys. Rev. A 88, 012501 (2013)

Ni26+ Th

186. P. K. Mondal, N. N. Dutta, G. Dixit, S. MajumderEffect of screening on spectroscopic properties of Li-like ions in a plasma environmentPhys. Rev. A 87, 062502 (2013)

C3+ ThN4+ ThO5+ Th

187. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Fe XXV, Co XXVI, Ni XXVII, Cu XXVIII and Zn XXIXPhys. Scr. 87, 055302 (2013)

Fe24+ Th

188. M. S. Safronova, U. I. Safronova, S. G. PorsevPolarizabilities, Stark shifts, and lifetimes of the In atomPhys. Rev. A 87, 032513 (2013)

123

In E/T

189. Y. Sun, B. C. Gou, C. ChenEnergies and the radiative and Auger transition rates of 1s2p4 resonances of B-likeionsPhys. Rev. A 87, 032509 (2013)

B Z= 6-14 Th

190. U. I. Safronova, A. S. Safronova, P. BeiersdorferRelativistic many-body calculations of excitation energies, oscillator strengths,transition rates, and lifetimes in samariumlike ionsPhys. Rev. A 87, 032508 (2013)

Sm Z= 74-100 Th

191. U. I. Safronova, M. S. SafronovaRelativistic many-body calculation of energies, lifetimes, polarizabilities, andhyperpolarizabilities in Li-like Be+

Phys. Rev. A 87, 032502 (2013)

Be+ Th

192. B. K. Sahoo, B. AroraMagic wavelengths for trapping the alkali-metal atoms with circularly polarized lightPhys. Rev. A 87, 023402 (2013)

K ThLi ThNa Th

193. F. B. Rosmej, B. Deschaud, K. Bennadji, P. Indelicato, J. P. MarquesFine-Structure electric-dipole matrix elements of He-like ions for x-ray line-shapecalculationsPhys. Rev. A 87, 022515 (2013)

Al11+ Th

194. Y. Sun, F. Chen, C. Chen, B. C. GouRadiative and Auger transitions of core-excited states for the boron isoelectronicsequenceEur. Phys. J. D 67, 88 (2013)

Mg7+ ThNe5+ ThO3+ ThSi9+ Th

195. Z.-D. Mu, Q.-Y. WeiTheoretical study of level structure and transitions of configurations 3d94s2, 3d94s4p,3d94p2 for Nb XIIIActa Phys. Sin. 62, 103101 (2013)

Nb12+ Th

196. M. Ortiz, C. Aragon, J. A. Aguilera, J. Rodrıguez-Garcıa, R. Mayo-GarcıaExperimental transition probabilities for spectral lines of Re IIJ. Phys. B 46, 185702 (2013)

Re+ Exp

124

197. L. C. Gao, D. H. Zhang, L. Y. Xie, J. G. Wang, Y. L. Shi, C. Z. DongTheoretical study of the photoionization process of Ne-like Ar, Fe, Kr and Xe ionsJ. Phys. B 46, 175402 (2013)

Ar8+ ThFe16+ ThKr26+ ThXe44+ Th

198. W.-J. Du, M. Andersson, K. Yao, T. Brage, R. Hutton, Y.-M. ZouLifetimes of the hyperfine levels of 3d94s 3D3 in high-Z Ni-like ionsJ. Phys. B 46, 145001 (2013)

Hf44+ ThW46+ ThRe47+ ThOs48+ ThIr49+ ThPt50+ ThAu51+ ThNi Z= 72-79 Th

199. O. Zatsarinny, K. BartschatThe B-spline R-matrix method for atomic processes: Application to atomic structure,electron collisions and photoionizationJ. Phys. B 46, 112001 (2013)

S ThXe Th

200. S. Verdebout, P. Rynkun, P. Jonsson, G. Gaigalas, C. Froese Fischer, M. GodefroidA partitioned correlation function interaction approach for describing electroncorrelation in atomsJ. Phys. B 46, 085003 (2013)

Be ThLi Th

201. M. Guerra, P. Amaro, C. I. Szabo, A. Gumberidze, P. Indelicato, J. P. SantosAnalysis of the charge state distribution in an ECRIS Ar plasma using high-resolutionx-ray spectraJ. Phys. B 46, 065701 (2013)

Ar14+ 16+ ThAr16+ Th

202. C. P. Ballance, S. D. Loch, M. S. Pindzola, D. C. GriffinElectron-Impact excitation and ionization of W3+ for the determination of tungsteninflux in a fusion plasmaJ. Phys. B 46, 055202 (2013)

W3+ Th

203. W. S. AbdelazizEnergy levels, transition probabilities, collision strength, and reduced populationcalculations for high gain predictions in neon-like kryptonJ. Russ. Laser Res. 34, 488-495 (2013)

Kr26+ Th

125

204. L.-Y. Jiang, Q. Wang, X. Shang, Y.-S. Tian, J.-R. Yin, Z.-K. Jiang, S.-H. Pei, Z.-W. DaiExperimental radiative lifetimes, branching fractions, and oscillator strengths of odd-parity levels in Mo IJ. Opt. Soc. Am. B 30, 489-493 (2013)

Mo Exp

205. N. G. Shchukina, I. E. Vasil’evaOscillator strengths for selected Fe II lines in the range λλ 300–400 nmKinemat. Phys. Celest. Bodies 29, 53-65 (2013)

Fe+ E/T

206. H. Liu, G. Jiang, F. Hu, C.-K. Wang, Z.-B. Wang, J.-M. YangIntercombination transitions of the carbon-like isoelectronic sequenceChin. Phys. B 22, 073202 (2013)

C Z= 7-92 Th

207. S. Aggarwal, J. Singh, M. MohanNew atomic data for Kr XXXV useful in fusion plasmaChin. Phys. B 22, 033201 (2013)

Kr34+ Th

208. S. N. NaharFine structure transitions in Fe XIVNew Astron. 21, 8-16 (2013)

Fe14+ Th

209. J. K. Saha, T. K. Mukherjee, P. K. Mukherjee, B. FrickeEffect of strongly coupled plasma on the magnetic dipolar and quadrupolar transitionsof two-electron ionsPhys. Plasmas 20, 042703 (2013)

C4+ ThMg10+ ThNe8+ ThO6+ ThS14+ ThSi12+ Th

210. S. Civis, M. Ferus, P. Kubelık, V. E. Chernov, E. M. ZanozinaLi I spectra in the 4.65–8.33 micron range: High-L states and oscillator strengthsAstron. Astrophys. 545, p.A61 (2012)

Li Th

211. S. Bernitt, G. V. Brown, J. K. Rudolph, R. Steinbrugge, A. Graf, M. Leutenegger, S. W. Epp, S.Eberle, K. Kubicek, V. Mackel, M. C. Simon, E. Trabert, E. W. Magee, C. Beilmann, N. Hell, S.Schippers, A. Muller, S. M. Kahn, A. Surzhykov, Z. Harman, C. H. Keitel, J. Clementson, F. S.Porter, W. Schlotter, J. J. Turner, J. Ullrich, P. Beiersdorfer, J. R. Crespo Lopez-UrrutiaAn unexpectedly low oscillator strength as the origin of the Fe VII emission problemNature 492, 225-228 (2012)

Fe16+ Exp

212. H. ElabidiElectron impact excitation for Ar VIJ. Phys.: Conf. Ser. 397, 012055 (2012)

126

Ar5+ Th

213. S. Hamasha, R. AlshaiubConstructing theoretical M-shell spectra for Mg-like Au through Cl-like Au ions ingold plasma diagnosticsPhys. Scr. 86, 065302 (2012)

Au62+ 67+ Th

214. J. P. Marques, P. Indelicato, F. ParenteRelativistic multiconfiguration calculations of the 2s22p 2P3/2 level lifetime along theboron isoelectronic sequenceEur. Phys. J. D 66, 324 (2012)

Au74+ ThBi78+ ThGd59+ ThB Z= 14-36 ThU87+ ThXe49+ Th

215. X.-Y. Ma, C.-Z. Dong, Z.-W. Wu, J. Jiang, L.-Y. XieTheoretical study on electron-impact excitation processes and the relevant polarizationof radiation of 2s1/2-2p3/2 in W65+ through W71+

Acta Phys. Sin. 61, 213401 (2012)

W65+ 71+ Th

216. E. Trabert, M. Grieser, R. von Hahn, C. Krantz, R. Repnow, A. WolfM1 and E2 decay-dependent lifetime of the lowest 1S0 level in C-like ions up to Ne4+

measured at a heavy-ion storage ringNew J. Phys. 14, 023061 (2012)

C Z= 7-10 Exp

217. E. A. Den Hartog, J. E. Lawler, J. S. Sobeck, C. Sneden, J. J. CowanImproved log(gf) values of selected lines in Mn I and Mn II for abundancedeterminations in FGK dwarfs and giantsAstrophys. J., Suppl. Ser. 194, 35 (2011)

Mn0+ + Exp

218. K. M. Aggarwal, T. Kato, F. P. Keenan, I. MurakamiEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Li II, Be III, B IV and C VPhys. Scr. 83, 015302 (2011)

e + Li+ 1E4−1E6 K The + Be2+ 1E4−1E6 K The + B3+ 1E4−1E6 K The + C4+ 1E4−1E6 K The + Li+ 1E4−1E6 K The + Be2+ 1E4−1E6 K The + B3+ 1E4−1E6 K The + C4+ 1E4−1E6 K Th

219. X. Wang, G. Jiang, L. H. Hao, L. Zhang, B. DengSystematic multi-configuration Dirac-Fock calculations of the K alpha and K beta X-ray spectra of silicon ionsEur. Phys. J. D 65, 505 (2011)

127

H + Si4+ ThH + Si5+ ThH + Si6+ ThH + Si7+ ThH + Si8+ ThH + Si9+ ThH + Si10+ ThH + Si11+ ThH + Si12+ ThH + Si4+ ThH + Si5+ ThH + Si6+ ThH + Si7+ ThH + Si8+ ThH + Si9+ ThH + Si10+ ThH + Si11+ ThH + Si12+ Th

220. Xiao-Bin Ding, Fumihiro Koike, Izumi Murakami, Daiji Kato, Hiroyuki A. Sakaue, Chen-ZhongDong, Nobuyuki Nakamura, Akihiro Komatsu, Junpei SakodaAb initio multi-configuration Dirac-Fock calculation of M1 visible transitions amongthe ground state multiplets of the W26+ ionJ. Phys. B 44, 145004 (2011)

e + W26+ The + W26+ Th

221. Quinet, PascalDirac-Fock calculations of forbidden transitions within the 3p(k) and 3d(k) groundconfigurations of highly charged tungsten ions (W47+-W61+)J. Phys. B 44, 195007 (2011)

H− + W47+ ThH− + W48+ ThH− + W49+ ThH− + W50+ ThH− + W51+ ThH− + W52+ ThH− + W53+ ThH− + W54+ ThH− + W55+ ThH− + W56+ ThH− + W57+ ThH− + W58+ ThH− + W59+ ThH− + W60+ ThH− + W61+ ThH− + W47+ ThH− + W48+ ThH− + W49+ ThH− + W50+ ThH− + W51+ ThH− + W52+ ThH− + W53+ ThH− + W54+ ThH− + W55+ ThH− + W56+ ThH− + W57+ ThH− + W58+ Th

128

H− + W59+ ThH− + W60+ ThH− + W61+ Th

222. Sergiy Bubin, Monika Stanke, Ludwik AdamowiczComplete pure vibrational spectrum of HD calculated without the Born-Oppenheimerapproximation and including relativistic correctionsPhys. Rev. A 83, 042520 (2011)

e + HD Th

223. Feng Hu, Jiamin Yang, Chuanke Wang, Longfei Jing, Shubo Chen, Gang Jiang, Hao Liu,Lianghuan HaoMulticonfiguration Dirac-Fock calculations on multi-valence-electron systems:Benchmarks on Ga-like ionsPhys. Rev. A 84, 042506 (2011)

e + Ga Z= 33-41 The + e Th

224. Feng Hu, Chuangke Wang, Jiamin Yang, Gang Jiang, Lianghuan HaoMulticonfiguration Dirac-Fock calculations of transition probabilities of some tungstenionsPhys. Scr. 84, 015302 (2011)

e + W71+ The + W72+ The + W73+ The + W37+ The + W71+ The + W72+ The + W73+ The + W37+ Th

225. Y. Gning, M. Sow, A. Traore, M. Dieng, B. Diakhate, M. Biaye, A. WagueCalculations of Resonances Parameters for the ((2s2) 1Se, (2s2p) 1,3P◦) and ((3s2) 1Se,(3s3p) 1,3P◦) Doubly Excited States of Helium-like Ions with Z≤10 Using a ComplexRotation Method Implemented in ScilabRadiat. Phys. Chem. 106, 1-6 (2015)

He Z= 2-10 Th

226. H. L. Zhang, C. J. FontesRelativistic Distorted-Wave Collision Strengths and Oscillator Strengths for the 185∆n = 0 Transitions with n = 2 in the 67 C-like Ions with 26≤Z≤92At. Data Nucl. Data Tables 101, 41-142 (2015)

C Z= 26-92 Th

227. J. A. Santana, J. K. Lepson, E. Trabert, P. BeiersdorferElectron-Correlation Effects on the 3C to 3D Line-Intensity Ratio in the Ne-like IonsAr8+ to Kr26+

Phys. Rev. A 91, 012502 (2015)

Ar8+ E/TNe Z= 18-36 E/T

228. P. QuinetAtomic Structure, Radiative Lifetime and Oscillator Strength Calculations in DoublyIonized Molybdenum (Mo III)Phys. Scr. 90, 015404 (2015)

129

Mo2+ Th

229. G.-J. Bian, F. He, G. Jiang, Q.-P. Fan, F. HuInfluence of Electron Correlation on Transition Energy of Gold IonsPhys. Scr. 90, 015403 (2015)

Au47+ 50+ Th

230. J. Dembczynski, M. Elantkowska, J. Ruczkowski, I. K. Ozturk, A. Er, F. Guzelcimen, Go. Basar,S. KrogerParametric Study of the Fine and Hyperfine Structure for the Even ParityConfigurations of Atomic NiobiumJ. Phys. B 48, 015006 (2015)

Nb Th

231. I. K. Ozturk, Go. Basar, A. Er, F. Guzelcimen, Gu. Basar, S. KrogerNew Energy Levels of Atomic Niobium by Laser Induced Fluorescence Spectroscopyin the Near InfraredJ. Phys. B 48, 015005 (2015)

Nb Exp

232. A. Abou El-Maaref, S. Schippers, A. MullerAb-Initio Calculations of Level Energies, Oscillator Strengths and Radiative Rates forE1 Transitions in Beryllium-like IronAtoms 3, 2-52 (2015)

Fe22+ Th

233. S. Kar, M. Z. M. Kamali, K. RatnaveluDynamic Dipole Polarizability of Li+ Embedded in PlasmasAIP Conf. Proc. 1588, 87-93 (2014)

Li+ Th

234. K. Sowmya, K. N. Nagendra, M. Sampoorna, J. O. StenfloPolarized Light Scattering with the Paschen-Back Effect, Level-Crossing of FineStructure States, and Partial Frequency RedistributionAstrophys. J. 793, 71 (2014)

Li Th

235. P. Beiersdorfer, E. Trabert, J. K. Lepson, N. S. Brickhouse, L. GolubHigh-Resolution Laboratory Measurements of Coronal Lines in the 198–218 A RegionAstrophys. J. 788, 25 (2014)

Ar11+ 12+ ExpAr11+ 16+ ExpF4+ ExpF4+ 8+ ExpFe6+ 13+ ExpFe16+ 17+ ExpFe6+ 17+ ExpN4+ ExpNe3+ ExpNe3+ 8+ ExpNi10+ ExpNi13+ 16+ ExpNi10+ 17+ Exp

130

O3+ 4+ ExpO3+ 6+ ExpS7+ ExpS9+ 11+ ExpS7+ 14+ Exp

236. S. S. Tayal, O. ZatsarinnyElectron Impact Excitation Collision Strengths for Extreme Ultraviolet Lines of Fe VIIAstrophys. J. 788, 24 (2014)

Fe6+ Th

237. A. M. Sossah, S. S. TayalEffective Collision Strengths for Fine-Structure Transitions in Si VIIAstrophys. J. 787, 2 (2014)

Si6+ Th

238. A. M. Frolov, M. B. Ruiz, D. M. WardlawBound State Spectra and Properties of the Doublet States in Three-Electron AtomicSystemsChem. Phys. Lett. 608, 191-200 (2014)

F6+ ThLi Z= 3-9 ThLi Z= 3-7 Th

239. A. M. Frolov, M. B. RuizBound State Spectrum of the Triplet States in the Be AtomChem. Phys. Lett. 595-596, 197-202 (2014)

Be Th

240. G. Del Zanna, P. J. Storey, H. E. MasonAtomic Data for Astrophysics: Ni XVAstron. Astrophys. 567, p.A18 (2014)

Ni14+ E/T

241. H. G. Wei, J. R. Shi, F. L. Wang, J. Y. Zhong, G. Y. Liang, G. ZhaoK-Shell Energy Levels and Radiative Rates for Transitions in Si IXAstron. Astrophys. 566, p.A105 (2014)

Si8+ Th

242. G. Del Zanna, P. J. Storey, N. R. BadnellAtomic Data for Astrophysics: Ni XIAstron. Astrophys. 566, p.A123 (2014)

Ni10+ E/T

243. G. Del Zanna, P. J. Storey, N. R. Badnell, H. E. MasonAtomic Data for Astrophysics: Fe IXAstron. Astrophys. 565, p.A77 (2014)

Fe8+ E/T

244. J. Ekman, P. Jonsson, S. Gustafsson, H. Hartman, G. Gaigalas, M. R. Godefroid, C. Froese FischerCalculations with Spectroscopic Accuracy: Energies, Transition Rates, and Lande gJ -Factors in the Carbon Isoelectronic Sequence from Ar XIII to Zn XXVAstron. Astrophys. 564, p.A24 (2014)

131

C Z= 18-30 Th

245. D. K. Nandy, B. K. SahooSpectral Properties of a Few F-like IonsAstron. Astrophys. 563, p.A25 (2014)

Ti13+ ThV14+ ThCr15+ ThMn16+ ThFe17+ ThCo18+ ThNi19+ ThCu20+ ThZn9+ ThMo33+ ThF Z= 22-30 Th

246. R. Kendurkar, B. D. ShrivastavaOrigin of the Satellites Lα3, Lα4 and Lα5 in the Elements from 40Zr to 50SnJ. Phys.: Conf. Ser. 534, 012037 (2014)

Zr-Sn2+ Th

247. M. T. Murphy, J. C. BerengutLaboratory Atomic Transition Data for Precise Optical Quasar AbsorptionSpectroscopyMon. Not. R. Astron. Soc. 438, 388-411 (2014)

Na E/TMg+ E/TAl2+ E/TCa+ E/TMn+ E/TZn+ E/TAl+ E/TCr+ E/TFe E/TFe+ E/TMg E/TNi+ E/TSi+ E/TSi3+ E/TTi+ E/T

248. E. Trabert, P. Beiersdorfer, N. S. Brickhouse, L. GolubHigh-Resolution Laboratory Spectra of the λ193 Channel of the Atmospheric ImagingAssembly Instrument on Board Solar Dynamics ObservatoryAstrophys. J., Suppl. Ser. 215, 6 (2014)

Ar10+ 13+ ExpF4+ 7+ ExpFe6+ 16+ ExpFe20+ ExpNe5+ 8+ ExpNi9+ 17+ ExpO3+ 7+ ExpS7+ 11+ Exp

132

249. F. Guzelcimen, B. Yapıcı, G. Demir, A. Er, I. K. Ozturk, Go. Basar, S. Kroger, M. Tamanis, R.Ferber, D. Docenko, Gu. BasarHyperfine Structure Constants of Energetically High-Lying Levels of Odd Parity ofAtomic VanadiumAstrophys. J., Suppl. Ser. 214, 9 (2014)

V Exp

250. C. J. Sansonetti, G. NaveExtended Analysis of the Spectrum of Singly Ionized Chromium (Cr II)Astrophys. J., Suppl. Ser. 213, 28 (2014)

Cr+ Exp

251. A. KramidaEnergy Levels and Spectral Lines of Quadruply Ionized Iron (Fe V)Astrophys. J., Suppl. Ser. 212, 11 (2014)

Fe4+ E/T

252. Y. P. Liu, C. Gao, J. L. Zeng, J. M. Yuan, J. R. ShiAtomic Data of Cu I for the Investigation of Element AbundanceAstrophys. J., Suppl. Ser. 211, 30 (2014)

Cu Th

253. E. Trabert, P. Beiersdorfer, N. S. Brickhouse, L. GolubHigh-Resolution Laboratory Spectra on the λ131 Channel of the AIA Instrument onBoard the Solar Dynamics ObservatoryAstrophys. J., Suppl. Ser. 211, 14 (2014)

Ca9+ 17+ ExpCa12+ 13+ ExpF5+ 6+ ExpFe6+ 7+ ExpFe19+ 20+ ExpFe22+ ExpNe4+ 6+ ExpNi9+ ExpNi9+ 26+ ExpO4+ 6+ ExpSi4+ 6+ Exp

254. S. L. Redman, G. Nave, C. J. SansonettiThe Spectrum of Thorium from 250 nm to 5500 nm: Ritz Wavelengths and OptimizedEnergy LevelsAstrophys. J., Suppl. Ser. 211, 4 (2014)

Ne0+ + ExpTh0+ 2+ Exp

255. Z. Uddin, L. WindholzNew Levels of Ta II with Energies Higher Than 72,000 cm−1

J. Quant. Spectrosc. Radiat. Transfer 149, 204-210 (2014)

Ta+ Exp

256. J. Ruczkowski, M. Elantkowska, J. DembczynskiSemi-Empirical Calculations of Oscillator Strengths and Hyperfine Constants for Ti IIJ. Quant. Spectrosc. Radiat. Transfer 149, 168-183 (2014)

133

Ti+ Th

257. F. Hu, M.-F. Mei, C. Han, B.-P. Han, G. Jiang, J.-M. YangAccurate Multiconfiguration Dirac-Hartree-Fock Calculations of TransitionProbabilities for Magnesium-like IonsJ. Quant. Spectrosc. Radiat. Transfer 149, 158-167 (2014)

Mg Z= 19-92 Th

258. J. C. Aguiar, H. O. Di RoccoAn Examination of the Consistency of the Published Levels of the p2, p3 and p4

Isoelectronic Sequences Using jj-Relativistic ExpressionsJ. Quant. Spectrosc. Radiat. Transfer 149, 1-7 (2014)

Br27+ E/TNi14+ E/TNi22+ E/TRb23+ E/TSc15+ E/TSe2+ E/TSr24+ E/TTe2+ E/TV17+ E/T

259. M. Raineri, E. E. Farıas, J. O. Souza, E. Amorim, M. Gallardo, J. Reyna AlmandosRevised and Extended Analysis of the Zn-like Kr IonJ. Quant. Spectrosc. Radiat. Transfer 148, 90-98 (2014)

Kr6+ E/T

260. G. G. Konan, L. Ozdemir, G. UrerEnergy Levels and Strong Electric Dipole Transitions in Magnesium-like GoldJ. Quant. Spectrosc. Radiat. Transfer 145, 110-120 (2014)

Au67+ Th

261. C. Chen, Y. Sun, B. C. GouEnergies, Radiative and Auger Transitions of the Core-Excited States for the BoronAtomJ. Quant. Spectrosc. Radiat. Transfer 145, 1-8 (2014)

B E/T

262. L. Y. Xie, X. Y. Ma, C. Z. Dong, Z. W. Wu, Y. L. Shi, J. JiangPolarization of the nf→ 3d (n = 4, 5, 6) X-rays from Tungsten Ions Following Electron-Impact Excitation and Dielectronic Recombination ProcessesJ. Quant. Spectrosc. Radiat. Transfer 141, 31-39 (2014)

W42+ 46+ Th

263. J. S. Sims, S. A. HagstromHylleraas-Configuration-Interaction Nonrelativistic Energies for the 1S Ground Statesof the Beryllium Isoelectronic SequenceJ. Chem. Phys. 140, 224312 (2014)

Be Z= 4-110 Th

264. S. Bubin, L. AdamowiczPrediction of 1P Rydberg Energy Levels of Beryllium Based on Calculations withExplicitly Correlated GaussiansJ. Chem. Phys. 140, 024301 (2014)

134

Be Th

265. L. Liang, X.-Y. Liu, C. ZhouAutoionization Resonances in the Partial Photoionization Cross Sections of Al VJ. Quant. Spectrosc. Radiat. Transfer 137, 51-56 (2014)

Al4+ Th

266. A. Alkauskas, P. Rynkun, G. Gaigalas, A. Kyniene, R. Kisielius, S. Kucas, S. Masys, G. Merkelis,V. JonauskasTheoretical Investigation of Spectroscopic Properties of W25+


W25+ Th

267. C. Jiang, F. Hu, Y. Zang, G. JiangProperties of the Kα X-ray Transitions in Highly Ionized ChlorineActa Phys. Pol. A 126-3, 694-699 (2014)

Cl7+ 15+ Th

268. A. V. Volotka, D. A. Glazov, V. M. Shabaev, I. I. Tupitsyn, G. PlunienMany-Electron QED Corrections to the g Factor of Lithiumlike IonsPhys. Rev. Lett. 112, 253004 (2014)

Pb79+ ThU89+ ThSi11+ ThCa17+ Th

269. J.-Q. Li, Z. Zhao, X.-M. ZhangMCDHF Calculation of Electron Affinities of Group I and Group IB Atomic AnionsEurophys. Lett. 107, 33001 (2014)

Ag ThAg− ThAu ThAu− ThCs ThCs− ThCu ThCu− ThFr ThFr− ThH ThH− ThK ThK− ThLi ThLi− ThNa ThNa− ThRb ThRb− Th

270. K. M. Aggarwal, F. P. KeenanEnergy Levels, Radiative Rates, and Lifetimes for Transitions in W LVIIIAt. Data Nucl. Data Tables 100, 1603-1767 (2014)

W57+ Th

135

271. P. Bogdanovich, R. KisieliusEnergy Level Properties of 4p64d3, 4p64d24f, and 4p54d4 Configurations of the W35+

IonAt. Data Nucl. Data Tables 100, 1593-1602 (2014)

W35+ E/T

272. K. M. Aggarwal, F. P. KeenanEnergy Levels, Radiative Rates, and Lifetimes for Transitions in W XLAt. Data Nucl. Data Tables 100, 1399-1518 (2014)

W39+ Th

273. M. Xu, G. Jiang, B.-L. Deng, G.-J. BianWavelengths, Transition Probabilities, and Oscillator Strengths for M-Shell Transitionsin Co-, Ni-, Cu-, Zn-, Ga-, Ge-, and Se-like Au IonsAt. Data Nucl. Data Tables 100, 1357-1398 (2014)

Au45+ 52+ Th

274. B.-L. Deng, G. Jiang, C. ZhangRelativistic Configuration-Interaction Calculations of Electric Dipole n = 2 – n = 3Transitions for Medium-Charge Li-like IonsAt. Data Nucl. Data Tables 100, 1337-1355 (2014)

Li Z= 7-30 Th

275. C. J. Fontes, H. L. ZhangRelativistic Distorted-Wave Collision Strengths for the 49 ∆n = 0 Optically AllowedTransitions with n = 2 in the 67 N-like Ions with 26≤Z≤92At. Data Nucl. Data Tables 100, 1292-1321 (2014)

N Z= 26-92 Th

276. F. El-SayedEnergy Levels, Lifetimes, and Transition Probabilities for Mn XII and Ge XIXAt. Data Nucl. Data Tables 100, 1250-1276 (2014)

Ge18+ ThMn11+ Th

277. C. Naze, S. Verdebout, P. Rynkun, G. Gaigalas, M. Godefroid, P. JonssonIsotope Shifts in Beryllium-, Boron-, Carbon-, and Nitrogen-like Ions from RelativisticConfiguration Interaction CalculationsAt. Data Nucl. Data Tables 100, 1197-1249 (2014)

Be Z= 5-74 E/TKr31+ E/TMo37+ E/TMo35+ E/TN Z= 7-36 E/TC Z= 7-28 E/TB Z= 8-30 E/TW67+ E/T

278. S. Verdebout, C. Naze, P. Jonsson, P. Rynkun, M. Godefroid, G. GaigalasHyperfine Structures and Lande gJ -Factors for n = 2 States in Beryllium-, Boron-,Carbon-, and Nitrogen-like Ions from Relativistic Configuration InteractionCalculationsAt. Data Nucl. Data Tables 100, 1111-1155 (2014)

136

Be Z= 5-74 ThKr31+ ThMo37+ ThMo35+ ThN Z= 7-36 ThC Z= 7-28 ThB Z= 8-30 ThW67+ Th

279. C. J. Fontes, H. L. ZhangRelativistic Distorted-Wave Collision Strengths for the 49 ∆n = 0 Optically AllowedTransitions with n = 2 in the 67 B-like Ions with 26≤Z≤92At. Data Nucl. Data Tables 100, 802-832 (2014)

B Z= 26-92 Th

280. A. Abou El-Maaref, M. Ahmad, S. H. AllamFine-Structure Calculations of Energy Levels, Oscillator Strengths, and TransitionProbabilities for Sulfur-like Iron, Fe XIAt. Data Nucl. Data Tables 100, 781-791 (2014)

Fe10+ Th

281. P. Amaro, C. I. Szabo, S. Schlesser, A. Gumberidze, E. G. Kessler Jr., A. Henins, E. O. Le Bigot,M. Trassinelli, J. M. Isac, P. Travers, M. Guerra, J. P. Santos, P. IndelicatoA Vacuum Double-Crystal Spectrometer for Reference-Free X-ray Spectroscopy ofHighly Charged IonsRadiat. Phys. Chem. 98, 132-149 (2014)

Ar14+ 16+ Exp

282. H.-W. Hu, Z.-B. Chen, F.-L. Li, C.-Z. Dong, L.-Y. Xie, W.-C. ChenRelativistic Energy Levels for Ions in PlasmaCan. J. Phys. 92, 1609-1613 (2014)

Al11+ 12+ ThAr16+ 17+ ThC4+ Th

283. S. Aggarwal, N. Verma, A. K. Singh, N. Singh, R. Sharma, M. MohanMulticonfigurational Dirac-Fock Energy Levels and Radiative Rates for Ni XXICan. J. Phys. 92, 1285-1296 (2014)

Ni20+ Th

284. K. M. Aggarwal, F. P. KeenanRadiative Rates for E1, E2, M1, and M2 Transitions Among the 3s23p5, 3s3p6, and3s23p43d Configurations of Cl-like W LVIIICan. J. Phys. 92, 1166-1177 (2014)

W57+ Th

285. L. Liang, X.-Y. Liu, C. ZhouPhotoionization of Al X from Ground State Using the Relativistic R-Matrix Close-Coupling MethodCan. J. Phys. 92, 241-245 (2014)

Al9+ Th

286. M. Mohan, S. Aggarwal, N. SinghMulticonfigurational Dirac-Fock Atomic Structure Calculations for Cl-like TungstenCan. J. Phys. 92, 177-183 (2014)

137

W57+ Th

287. N. A. Zubova, Y. S. Kozhedub, V. M. Shabaev, I. I. Tupitsyn, A. V. Volotka, G. Plunien, C.Brandau, Th. StohlkerRelativistic Calculations of the Isotope Shifts in Highly Charged Li-like IonsPhys. Rev. A 90, 062512 (2014)

Ar15+ ThBe+ ThBi80+ ThC3+ ThFe23+ ThFr84+ ThHg77+ ThKr33+ ThMo39+ ThNd57+ ThNe7+ ThO5+ ThPa88+ ThSi11+ ThTh87+ ThTi19+ ThU89+ ThXe51+ ThYb67+ ThZn27+ Th

288. C. T. Chantler, T. V. B. Nguyen, J. A. Lowe, I. P. GrantConvergence of the Breit Interaction in Self-Consistent and Configuration-InteractionApproachesPhys. Rev. A 90, 062504 (2014)

Ar ThCa ThKr ThMg ThNe ThSr ThXe Th

289. Z. Fei, W. Li, J. Grumer, Z. Shi, R. Zhao, T. Brage, S. Huldt, K. Yao, R. Hutton, Y. ZouForbidden-Line Spectroscopy of the Ground-State Configuration of Cd-like WPhys. Rev. A 90, 052517 (2014)

W26+ E/T

290. A. Kozlov, V. A. Dzuba, V. V. FlambaumOptical Atomic Clocks with Suppressed Blackbody-Radiation ShiftPhys. Rev. A 90, 042505 (2014)

Er ThEr2+ ThHf ThHf12+ ThHg22+ ThI+ ThLu+ ThOs13+ ThPa2+ 3+ Th

138

Pb24+ ThPo ThPo26+ ThPt20+ ThRa30+ ThSn ThTe ThTh ThTh32+ ThTm3+ ThU33+ ThW14+ ThXe2+ ThZr ThZr2+ Th

291. J.-G. Li, T. Brage, P. Jonsson, Y. YangMagnetic-Field-Dependent Angular Distributions and Linear Polarizations ofEmissions from the 2p53s 3P◦2 State in Ne-like IonsPhys. Rev. A 90, 035404 (2014)

Mg2+ Th

292. K. Kubicek, P. H. Mokler, V. Mackel, J. Ullrich, J. R. Crespo Lopez-UrrutiaTransition Energy Measurements in Hydrogenlike and Heliumlike Ions StronglySupporting Bound-State QED CalculationsPhys. Rev. A 90, 032508 (2014)

Ar16+ 17+ ExpFe24+ 25+ ExpS14+ 15+ Exp

293. S. Hasegawa, S. Obara, F. Yoshida, Y. Azuma, F. Koike, T. NagataK-Shell Photoionization Spectra of Atomic Beryllium Between 1s2s2 and 1s(2s2p 3P)4sPhys. Rev. A 90, 032503 (2014)

Be Exp

294. V. A. Yerokhin, A. Surzhykov, S. FritzscheRelativistic Configuration-Interaction Calculation of Kα Transition Energies inBerylliumlike IronPhys. Rev. A 90, 022509 (2014)

Fe22+ Th

295. D. Bernhardt, A. Becker, M. Grieser, M. Hahn, C. Krantz, M. Lestinsky, O. Novotny, R. Repnow,D. W. Savin, K. Spruck, A. Wolf, A. Muller, S. SchippersAbsolute Rate Coefficients for Photorecombination and Electron-Impact Ionization ofMagnesiumlike Iron Ions from Measurements at a Heavy-Ion Storage RingPhys. Rev. A 90, 012702 (2014)

Fe13+ E/TFe14+ E/T

296. U. I. Safronova, A. S. Safronova, P. BeiersdorferMultipole Transitions to Determine Lifetimes and Polarizabilities in Mg-like Ions fromSi2+ to Fm88+

Phys. Rev. A 90, 012519 (2014)

Mg Z= 13-100 Th

139

297. A. Muller, A. Borovik Jr., K. Huber, S. Schippers, D. V. Fursa, I. BrayDouble-K-Vacancy States in Electron-Impact Single Ionization of Metastable Two-Electron N5+(1s2s 3S1) IonsPhys. Rev. A 90, 010701 (2014)

N4+ Exp

298. K. M. Aggarwal, F. P. KeenanEnergy Levels, Radiative Rates and Lifetimes for Transitions in Br-like Ions with38 ≤ Z ≤ 42Phys. Scr. 89, 125404 (2014)

Mo7+ ThNb6+ ThSr3+ ThY4+ ThZr5+ Th

299. A. N. Ryabtsev, E. Ya. Kononov, R. R. Kildiyarova, W.-U L. Tchang-Brillet, J.-F. Wyart, N.Champion, C. BlaessSpectra of the W VIII Isoelectronic Sequence: II. Ta VIIPhys. Scr. 89, 125403 (2014)

Ta6+ E/T

300. K. M. Aggarwal, F. P. KeenanEnergy Levels, Radiative Rates and Electron Impact Excitation Rates for Transitionsin Be-like Cl XIV, K XVI and Ge XXIXPhys. Scr. 89, 125401 (2014)

Cl13+ ThGe28+ ThK15+ Th

301. K. Haris, A. Kramida, A. TauheedExtended and Revised Analysis of Singly Ionized Tin: Sn IIPhys. Scr. 89, 115403 (2014)

Sn+ E/TTe3+ E/T

302. C. Suzuki, F. Koike, I. Murakami, N. Tamura, S. Sudo, H. A. Sakaue, N. Nakamura, S. Morita, M.Goto, D. Kato, T. Nakano, T. Higashiguchi, C. S. Harte, G. O’SullivanEUV Spectroscopy of Highly Charged High Z Ions in the Large Helical Device PlasmasPhys. Scr. 89, 114009 (2014)

Ag Z= 64-66 ExpCu Z= 64-66 ExpW14+ 45+ Exp

303. J. D. GillaspyPrecision Spectroscopy of Trapped Highly Charged Heavy Elements: Pushing theLimits of Theory and ExperimentPhys. Scr. 89, 114004 (2014)

Ar16+ ExpTi20+ Exp

304. Dipti, T. Das, L. Sharma, R. SrivastavaL-Shell Electron Excitations of Mg- through O-like Tungsten IonsPhys. Scr. 89, 085403 (2014)

140

W62+ 66+ Th

305. G. Xiong, J.-Y. Zhang, G.-H. Yang, J.-M. Yang, H. Li, Z.-M. Hu, Y. Zhao, M.-X. Wei, T. YiDifferent Approaches to Precise Wavelength Calibration of a Flat-Field GratingSpectrometer for Laser-Produced PlasmasPhys. Scr. 89, 065005 (2014)

He Z= 6-8 ExpLi Z= 6-8 Exp

306. A. O. G. Wallis, L. Lodi, A. EmmanouilidouAuger Spectra Following Inner-Shell Ionization of Argon by a Free-Electron LaserPhys. Rev. A 89, 063417 (2014)

Ar+ Th

307. Y. Wang, O. Zatsarinny, K. BartschatB-Spline R-Matrix-With-Pseudostates Calculations for Electron-Impact Excitationand Ionization of NitrogenPhys. Rev. A 89, 062714 (2014)

N ThN− Th

308. J. Grumer, R.-F. Zhao, T. Brage, W.-X. Li, S. Huldt, R. Hutton, Y.-M. ZouCoronal Lines and the Importance of Deep-Core-Valence Correlation in Ag-like IonsPhys. Rev. A 89, 062511 (2014)

Ag Z= 50-94 Th

309. V. Gedeon, S. Gedeon, V. Lazur, E. Nagy, O. Zatsarinny, K. BartschatB-Spline R-Matrix-With-Pseudostates Calculations for Electron-Impact Excitationand Ionization of FluorinePhys. Rev. A 89, 052713 (2014)

F ThF− Th

310. T. Carette, M. R. GodefroidTheoretical Study of the Isotope Effects on the Detachment Thresholds of Si−

Phys. Rev. A 89, 052513 (2014)

Si Th29Si− ThSi− Th

311. P. F. Liu, Y. P. Liu, J. L. Zeng, J. M. YuanElectron-Impact Excitation and Single- and Multiple-Ionization Cross Sections ofHeavy Ions: Sn13+ As an ExamplePhys. Rev. A 89, 042704 (2014)

Sn13+ ThSn13+ 14+ Th

312. X.-Y. Han, X. Gao, D.-L. Zeng, R. Jin, J. Yan, J.-M. LiScaling Law for Transition Probabilities in 2p3 Configuration from LS Coupling to jjCouplingPhys. Rev. A 89, 042514 (2014)

N Z= 7-100 Th

141

313. S. Roy, N. N. Dutta, S. MajumderRelativistic Coupled-Cluster Calculations on Hyperfine Structures andElectromagnetic Transition Amplitudes of In IIIPhys. Rev. A 89, 042511 (2014)

In2+ Th

314. V. A. Dzuba, A. Kozlov, V. V. FlambaumScalar Static Polarizabilities of Lanthanides and ActinidesPhys. Rev. A 89, 042507 (2014)

Ac-NO ThAr ThKr ThLa-Lu ThXe Th

315. L. G lowacki, J. Migda lekRelativistic Configuration Interaction Calculations for Some Two- and Three-ElectronSystems with Screened Hydrogenic Spin OrbitalsPhys. Rev. A 89, 042503 (2014)

He ThLi ThNe8+ ThNe7+ ThU89+ ThU90+ Th

316. M. Puchalski, K. PachuckiGround-State Hyperfine Splitting in the Be+ IonPhys. Rev. A 89, 032510 (2014)

Be+ Th

317. B. Bernhardt, A. R. Beck, X. Li, E. R. Warrick, M. J. Bell, D. J. Haxton, C. M. McCurdy, D. M.Neumark, S. R. LeoneHigh-Spectral-Resolution Attosecond Absorption Spectroscopy of Autoionization inXenonPhys. Rev. A 89, 023408 (2014)

Xe Exp

318. S. Chattopadhyay, B. K. Mani, D. AngomElectric Dipole Polarizability of Alkaline-Earth-Metal Atoms from PerturbedRelativistic Coupled-Cluster Theory with TriplesPhys. Rev. A 89, 022506 (2014)

Ba ThCa ThMg ThRa ThSr Th

319. G. P. Gupta, A. Z. MsezaneFine-Structure Energy Levels, Oscillator Strengths and Lifetimes in Al-like ChromiumIndian J. Phys. 88, 11-18 (2014)

Cr11+ Th

142

320. S. Menmuir, C. Giroud, T. M. Biewer, I. H. Coffey, E. Delabie, N. C. Hawkes, M. Sertoli, JETEFDA ContributorsCarbon Charge Exchange Analysis in the ITER-like Wall EnvironmentRev. Sci. Instrum. 85, p.11E412 (2014)

C5+ ExpW Exp

321. T. Oishi, S. Morita, X. L. Huang, H. M. Zhang, M. GotoLine Spectrum and Ion Temperature Measurements from Tungsten Ions at LowIonization Stages in Large Helical Device Based on Vacuum Ultraviolet Spectroscopyin Wavelength Range of 500–2200 ARev. Sci. Instrum. 85, p.11E415 (2014)

C+ 2+ ExpN+ 2+ ExpO+ 3+ ExpW5+ Exp

322. P. V. Kiran Kumar, M. V. SuryanarayanaPrecision Two-Photon Spectroscopy of Alkali ElementsPramana 83, 189-219 (2014)

Cs ExpNa ExpK ExpLi ExpRb Exp

323. L. Liang, X.-Y. Liu, C. ZhouPhotoionization Processes of Ti XIX with J = 1J. Appl. Spectrosc. 81, 483-487 (2014)

Ti18+ Th

324. P.-F. Liu, Y.-P. Liu, Jiaolong Zeng, Jianmin YuanAuger Decay and the Direct Double Ionization Probability of a 2p Inner-Shell Hole ina Singly Charged Ar+ IonEur. Phys. J. D 68, 214 (2014)

Ar+ Th

325. L.-H. Hao, X.-P. KangEnergy Levels and Spectral Lines in the X-ray Spectra of Highly Charged W XLIVEur. Phys. J. D 68, 203 (2014)

W43+ Th

326. M. Cohen, P. MandelbaumIonization Cross Sections and Rate Coefficients for the Ground State of As I-like IonsEur. Phys. J. D 68, 2 (2014)

As Z= 38-92 Th

327. H. ElabidiStructural and Collisional Data for Mg III and Al IVAdv. Space Res. 54, 1203-1222 (2014)

Al3+ ThMg2+ Th

143

328. H. Elabidi, S. Sahal-Brechot, M. S. DimitrijevicQuantum Stark Broadening of Ar XV Lines. Strong Collision and QuadrupolarPotential ContributionsAdv. Space Res. 54, 1184-1189 (2014)

Ar14+ Th

329. V. K. Saini, P. Kumar, S. K. Dixit, S. V. NakheStudies on Pulsed Optogalvanic Effect in Eu/Ne Hollow Cathode DischargeAppl. Opt. 53, 4320-4326 (2014)

Eu ExpNe Exp

330. S. Spencer, A. Hibbert, C. A. RamsbottomOscillator Strengths and Transition Probabilities for the W XLV IonJ. Phys. B 47, 245001 (2014)

W44+ Th

331. A. Muller, S. Schippers, D. Esteves-Macaluso, M. Habibi, A. Aguilar, A. L. D. Kilcoyne, R. A.Phaneuf, C. P. Ballance, B. M. McLaughlinValence-Shell Photoionization of Ag-like Xe7+ Ions: Experiment and TheoryJ. Phys. B 47, 215202 (2014)

Xe7+ E/T

332. T. Nagata, K. Kawajiri, S. Kosugi, N. Suzuki, M. Kemmotsu, T. Nandi, E. Sokell, Y. Azuma, F.KoikePhotoion Spectroscopy on Isolated Mn Atoms in the 2p → 3d Excitation Region:I. Total Photoion-Yield SpectrumJ. Phys. B 47, 185006 (2014)

Mn E/T

333. R. Zhao, J. Grumer, W. Li, J. Xiao, T. Brage, S. Huldt, R. Hutton, Y. ZouThe M1 Ground State Fine Structure Transition in Ag-like YbJ. Phys. B 47, 185004 (2014)

Ag Z= 62-74 E/TYb23+ E/T

334. A. T. Payne, C. T. Chantler, M. N. Kinnane, J. D. Gillaspy, L. T. Hudson, L. F. Smale, A. Henins,J. A. Kimpton, E. TakacsHelium-like Titanium X-ray Spectrum As a Probe of QED ComputationJ. Phys. B 47, 185001 (2014)

Ti19+ ExpTi20+ Exp

335. Madhulita Das, B. K. Sahoo, S. PalRelativistic Spectroscopy of Plasma-Embedded Li-like Systems with Screening Effectsin Two-Body Debye PotentialsJ. Phys. B 47, 175701 (2014)

Ca17+ ThTi19+ Th

336. M. L. Qiu, R. F. Zhao, X. L. Guo, Z. Z. Zhao, W. X. Li, S. Y. Du, J. Xiao, K. Yao, C. Y. Chen,R. Hutton, Y. ZouInvestigation of Transitions Between Metastable Levels of the First ExcitedConfiguration of Palladium-like TungstenJ. Phys. B 47, 175002 (2014)

144

W28+ E/T

337. A. Muller, S. Schippers, R. A. Phaneuf, S. W. J. Scully, A. Aguilar, C. Cisneros, M. F. Gharaibeh,A. S. Schlachter, B. M. McLaughlinK-Shell Photoionization of Be-like Boron (B+) Ions: Experiment and TheoryJ. Phys. B 47, 135201 (2014)

B+ Exp

338. J. Seely, J. L. Glover, L. Hudson, Yu. Ralchenko, N. Pereira, U. FeldmanMeasurement of the O2O3O4 and O3O4O5 Super Coster-Kronig Rates in Tungstenvia Asymmetric Diffraction SpectrometryJ. Phys. B 47, 115004 (2014)

W Exp

339. Y. A. Podpaly, J. D. Gillaspy, J. Reader, Yu. RalchenkoEUV Measurements of Kr XXI–Kr XXXIV and the Effect of a Magnetic-Dipole Lineon Allowed TransitionsJ. Phys. B 47, 095702 (2014)

Kr20+ 21+ ExpKr24+ ExpKr26+ 33+ Exp

340. A. A. Kamenski, V. D. OvsiannikovFormal Approach to Deriving Analytically Asymptotic Formulas for StaticPolarizabilities of Atoms and Ions in Rydberg StatesJ. Phys. B 47, 095002 (2014)

Ba+ ThBe+ ThCa+ ThCs ThHe ThK ThLi ThMg+ ThNa ThRb ThSr+ Th

341. M. H. Abdalmoneam, D. R. BeckDipole and Quadrupole Polarizabilities of Ni II and Parameters of an EffectivePotential for Ni I Rydberg StatesJ. Phys. B 47, 085003 (2014)

Ni+ Th

342. J. E. Rice, M. L. Reinke, J. M. A. Ashbourn, C. Gao, M. M. Victora, M. A. Chilenski, L.Delgado-Aparicio, N. T. Howard, A. E. Hubbard, J. W. HughesX-ray Observations of Ca19+, Ca18+ and Satellites from Alcator C-Mod TokamakPlasmasJ. Phys. B 47, 075701 (2014)

Ar16+ ExpCa16+ 19+ ExpMo32+ Exp

343. B.-W. Li, T. Higashiguchi, T. Otsuka, N. Yugami, P. Dunne, D. Kilbane, E. Sokell, G. O’SullivanAnalysis of Laser Produced Plasmas of Gold in the 1–7 nm RegionJ. Phys. B 47, 075001 (2014)

145

Au19+ 42+ E/TAu20+ 42+ E/TAu32+ 33+ E/TAu32+ 34+ E/T

344. M. F. Gharaibeh, N. El Hassan, M. M. Al Shorman, J. M. Bizau, D. Cubaynes, S. Guilbaud, I.Sakho, C. Blancard, B. M. McLaughlinK-Shell Photoionization of B-like Atomic Nitrogen Ions: Experiment and TheoryJ. Phys. B 47, 065201 (2014)

N2+ Exp

345. I. D. Petrov, B. M. Lagutin, V. L. Sukhorukov, A. Ehresmann, H. SchmoranzerStrong Impact of the Giant Resonance on the Radiationless Decay of the 4d-Vacancyin Xe: II. N4,5OO Auger EffectJ. Phys. B 47, 055001 (2014)

Xe Th

346. J. Cai, W.-W. Yu, N. ZhangThe Scaling Law in the Fine-Structure Splitting of 1s2np States for the LithiumIsoelectronic SequenceChin. Phys. Lett. 31, 093101 (2014)

Li Z= 21-30 Th

347. S. Civis, P. Kubelık, M. Ferus, V. E. Chernov, E. M. Zanozina, L. JuhaLaser Ablation of an Indium Target: Time-Resolved Fourier-Transform InfraredSpectra of In I in the 700–7700 cm−1 RangeJ. Anal. At. Spectrom. 29, 2275-2283 (2014)

In Exp

348. S. AggarwalAtomic Structure Calculations for F-like TungstenChin. Phys. B 23, 093203 (2014)

W65+ Th

349. H.-J. Dong, K.-S. Huang, C.-Y. Li, J.-M. Zhao, L.-J. Zhang, S.-T. JiaElectric Dipole Moments of Lithium Atoms in Rydberg StatesChin. Phys. B 23, 093202 (2014)

Li Th

350. Y.-B. Tang, C.-B. Li, H.-X. QiaoCalculations on Polarization Properties of Alkali Metal Atoms Using Dirac-Fock PlusCore Polarization MethodChin. Phys. B 23, 063101 (2014)

Cs0+ + ThFr0+ + ThK0+ + ThLi0+ + ThNa0+ + ThRb0+ + Th

351. P. Hakel, G. A. Kyrala, P. A. Bradley, N. S. Krasheninnikova, T. J. Murphy, M. J. Schmitt, I. L.Tregillis, R. J. Kanzleieter, S. H. Batha, C. J. Fontes, M. E. Sherrill, D. P. Kilcrease, S. P. ReganX-ray Spectroscopic Diagnostics and Modeling of Polar-Drive Implosion Experimentson the National Ignition FacilityPhys. Plasmas 21, 063306 (2014)

146

Cu27+ ExpCu28+ ExpFe24+ ExpFe25+ ExpGe30+ ExpGe31+ ExpTi20+ ExpTi21+ Exp

352. S. Kar, Y. Wang, Z.-S. Jiang, S.-X. Li, K. RatnaveluDoubly-Excited 1,3De Resonance States of Two-Electron Positive Ions Li+ and Be2+ inDebye PlasmasPhys. Plasmas 21, 012105 (2014)

Be2+ ThLi+ Th

353. C. T. Chantler, A. T. Payne, J. D. Gillaspy, L. T. Hudson, L. F. Smale, A. Henins, J. A.Kimpton, E. TakacsX-ray Measurements in Helium-like Atoms Increased Discrepancy BetweenExperiment and Theoretical QEDNew J. Phys. 16, 123037 (2014)

He Z= 18-24 E/THe Z= 26-27 E/TGe30+ E/TKr34+ E/TS14+ E/TU90+ E/TXe52+ E/T

354. C. Froese FischerEvaluation and Comparison of the Configuration Interaction Calculations for ComplexAtomsAtoms 2, 1-14 (2014)

W39+ Th

355. H. TanumaCharge Exchange Spectroscopy of Multiply Charged Ions of Industrial andAstrophysical InterestAIP Conf. Proc. 1545, 196-201 (2013)

O7+ ExpSn4+ 19+ ExpXe8+ 18+ Exp

356. S. Morita, C. F. Dong, M. Goto, D. Kato, I. Murakami, H. A. Sakaue, M. Hasuo, F. Koike, N.Nakamura, T. Oishi, A. Sasaki, E. H. WangA Study of Tungsten Spectra Using Large Helical Device and Compact Electron BeamIon Trap in NIFSAIP Conf. Proc. 1545, 143-152 (2013)

W24+ 33+ ExpW26+ Exp

357. N. Nakamura, X.-B. Ding, C.-Z. Dong, H. Hara, D. Kato, F. Koike, I. Murakami, T. Nakano, H.Ohashi, H. A. Sakaue, H. Watanabe, T. Watanabe, N. YamamotoEBIT Spectroscopy of Highly Charged Heavy Ions Relevant to Hot PlasmasAIP Conf. Proc. 1545, 62-71 (2013)

147

Fe8+ 14+ ExpGd33+ 35+ ExpW22+ 26+ ExpW42+ 45+ Exp

358. P. Jonsson, J. Ekman, S. Gustafsson, H. Hartman, L. B. Karlsson, R. du Rietz, G. Gaigalas, M.R. Godefroid, C. Froese FischerEnergy Levels and Transition Rates for the Boron Isoelectronic Sequence: Si X,Ti XVIII – Cu XXVAstron. Astrophys. 559, p.A100 (2013)

Si9+ ThB Z= 22-29 Th

359. I. L. Glukhov, E. A. Nikitina, V. D. OvsiannikovThermal Shifts and Broadening of Rydberg Levels in Be II IonsPhys. Scr. T157, 014014 (2013)

Be+ Th

360. P. Amaro, S. Schlesser, M. Guerra, E. Le Bigot, J. P. Santos, C. I. Szabo, A. Gumberidze, P.IndelicatoAbsolute Measurements and Simulations of X-ray Line Energies of Highly ChargedIons with a Double-Crystal SpectrometerPhys. Scr. T156, 014104 (2013)

Ar16+ Exp

361. Yu. Ralchenko, J. D. Gillaspy, J. Reader, D. Osin, J. J. Curry, Y. A. PodpalyMagnetic-Dipole Lines in 3dn Ions of High-Z Elements: Identification, DiagnosticPotential and Dielectronic ResonancesPhys. Scr. T156, 014082 (2013)

Ta45+ 57+ Exp

362. D. Kato, M. Goto, S. Morita, I. Murakami, H. A. Sakaue, X. B. Ding, S. Sudo, C. Suzuki, N.Tamura, N. Nakamura, H. Watanabe, F. KoikeObservation of Visible Forbidden Lines from Highly Charged Tungsten Ions at theLarge Helical DevicePhys. Scr. T156, 014081 (2013)

W26+ Exp

363. J. K. Lepson, P. Beiersdorfer, M. Bitter, A. L. Roquemore, R. KaitaEmission Lines of Iron in the 150–250 A Region on National Spherical TorusExperimentPhys. Scr. T156, 014075 (2013)

C4+ 5+ ExpFe7+ 13+ Exp

364. A. V. Volotka, D. A. Glazov, O. V. Andreev, V. M. Shabaev, I. I. Tupitsyn, G. PlunienProbing Many-Electron QED Effects in the Presence of Magnetic FieldsPhys. Scr. T156, 014017 (2013)

Bi80+ ThBi82+ ThSi11+ Th

365. J. M. Sampaio, F. Parente, C. Naze, M. Godefroid, P. Indelicato, J. P. MarquesRelativistic Calculations of 1s22s2p Level Splitting in Be-like KrPhys. Scr. T156, 014015 (2013)

148

Kr32+ Th

366. D. A. Glazov, A. V. Volotka, A. A. Schepetnov, M. M. Sokolov, V. M. Shabaev, I. I. Tupitsyn, G.Plunieng Factor of Boron-like Ions: Ground and Excited StatesPhys. Scr. T156, 014014 (2013)

Ar13+ Th

367. D. Kilbane, J. D. Gillaspy, Yu. Ralchenko, J. Reader, G. O’SullivanExtreme Ultraviolet Spectra from N-Shell Ions of Gd, Dy and WPhys. Scr. T156, 014012 (2013)

Gd18+ 27+ ExpGd30+ ExpGd31+ ExpGd32+ ExpW27+ 29+ Exp

368. M. Minoshima, J. Sakoda, A. Komatsu, H. A. Sakaue, X.-B. Ding, D. Kato, I. Murakami, C.-Z.Dong, F. Koike, H. Watanabe, N. NakamuraVisible Transitions of Highly Charged Tungsten Ions Observed with a CompactElectron Beam Ion TrapPhys. Scr. T156, 014010 (2013)

W26+ ExpW28+ Exp

369. P. Beiersdorfer, J. K. Lepson, F. Dıaz, Y. Ishikawa, E. TrabertMeasurement and Calculation of L-Shell Transitions in M-Shell Iron IonsPhys. Scr. T156, 014007 (2013)

Fe13+ 15+ E/T

370. M. A. Leutenegger, G. L. Betancourt-Martinez, P. Beiersdorfer, G. V. Brown, R. L. Kelley, C. A.Kilbourne, F. S. PorterCharge Exchange Measurements with an X-ray Calorimeter at an Electron Beam IonTrapPhys. Scr. T156, 014006 (2013)

Mg9+ ExpMg9+ 11+ Exp

371. K. Kubicek, P. H. Mokler, J. Ullrich, J. R. Crespo Lopez-UrrutiaA Step toward Probing Higher-Order Feynman Diagrams in Few-Electron HighlyCharged IonsPhys. Scr. T156, 014005 (2013)

Ar16+ 17+ Exp

372. V. Mackel, R. Klawitter, G. Brenner, J. R. Crespo Lopez-Urrutia, J. UllrichLaser Spectroscopy of Highly Charged Argon at the Heidelberg Electron Beam IonTrapPhys. Scr. T156, 014004 (2013)

Ar13+ Exp

373. N. J. DeYonker, K. A. PetersonIs Near-”Spectroscopic Accuracy” Possible for Heavy Atoms and Coupled ClusterTheory? an Investigation of the First Ionization Potentials of the Atoms Ga–KrJ. Chem. Phys. 138, 164312 (2013)

149

As ThBr ThGa ThGe ThKr ThSe Th

374. J. Komasa, R. S lupski, K. Jankowski, J. Wasilewski, A. M. TealeHigh Accuracy Ab Initio Studies of Electron-Densities for the Ground State of Be-likeAtomic SystemsJ. Chem. Phys. 138, 164306 (2013)

Ar14+ ThBe ThC2+ ThLi− ThNe6+ Th

375. A. N. Ryabtsev, E. Ya. Kononov, R. R. Kildiyarova, W.-U L. Tchang-Brillet, J.-F. WyartThe Spectrum of Seven Times Ionized Tungsten (W VIII) Relevant to TokamakDivertor PlasmasPhys. Scr. 87, 045303 (2013)

W7+ E/T

376. G. Ranjit, N. A. Schine, A. T. Lorenzo, A. E. Schneider, P. K. MajumderMeasurement of the Scalar Polarizability within the 5P1/2-6S1/2 410-nm Transition inAtomic IndiumPhys. Rev. A 87, 032506 (2013)

In Exp

377. S. Sturm, A. Wagner, M. Kretzschmar, W. Quint, G. Werth, K. Blaumg-Factor Measurement of Hydrogenlike 28Si13+ as a Challenge to QED CalculationsPhys. Rev. A 87, 030501 (2013)

Si13+ Exp

378. M. Gaft, L. Nagli, I. GornushkinLaser-Induced Breakdown Spectroscopy of Zr in Short Ultraviolet Wavelength RangeSpectrochimica Acta, Part B 85, 93-99 (2013)

Zr0+ + Exp

379. C. I. Szabo, P. Indelicato, L. T. Hudson, J. F. Seely, T. MaHigh-Resolution K-Shell Spectra from Laser Excited Molybdenum PlasmasEPJ Web Conf. 59, 13007 (2013)

Mo40+ ExpMo41+ Exp

380. M. Dieng, M. Biaye, Y. Gning, A. WagueThe Inter-Shell Doubly Excited 1,3Se, 1,3Po, 1,3De, 1,3Fo, and 1,3Ge States EnergiesCalculations of Helium-like Ions Using Special Forms of Hylleraas-Type WaveFunctionsChin. J. Phys. 51, 674-691 (2013)

He Z= 2-10 Th

381. C.-Y. Li, X.-Y. Han, J.-G. Wang, Y.-Z. QuRelativistic R-Matrix Studies of Photoionization Processes of Ar5+

Chin. Phys. B 22, 123201 (2013)

150

Ar5+ E/T

382. S. Bubin, L. AdamowiczAssessment of the Accuracy the Experimental Energies of the 1P◦ 1s22s6p and 1s22s7pStates of 9Be Based on Variational Calculations with Explicitly Correlated GaussiansJ. Chem. Phys. 137, 104315 (2012)

Be E/T

383. U. I. Safronova, A. S. Safronova, P. BeiersdorferRelativistic Atomic Data for Cu-like TungstenPhys. Rev. A 86, 042510 (2012)

W45+ Th

384. G. P. Gupta, V. Tayal, A. Z. MsezaneFine-Structure Energy Levels and Radiative Rates in Si-like ChlorineIndian J. Phys. 86, 1-8 (2012)

Cl3+ Th

385. C. S. Harte, T. Higashiguchi, T. Otsuka, R. D’Arcy, D. Kilbane, G. O’SullivanAnalysis of Tungsten Laser Produced Plasmas in the Extreme Ultraviolet (EUV)Spectral RegionJ. Phys. B 45, 205002 (2012)

W20+ 37+ Exp

386. S. W. Epp, J. R. Crespo Lopez Urrutia, M. C. Simon, T. Baumann, G. Brenner, R. Ginzel, N.Guerassimova, V. Mackel, P. H. Mokler, B. L. Schmitt, H. Tawara, J. UllrichX-ray Laser Spectroscopy of Highly Charged Ions at FLASHJ. Phys. B 43, 194008 (2010)

Cu25+ 26+ ExpF3+ ExpFe23+ ExpNe Exp

387. M. Frankel, P. Beiersdorfer, G. V. Brown, M. F. Gu, R. L. Kelley, C. A. Kilbourne, F. S. PorterX-ray Signature of Charge Exchange in L-Shell Sulfur IonsAstrophys. J. 702, 171-177 (2009)

N5+ 6+ ExpO6+ 7+ ExpS10+ 13+ Exp

388. T. Holczer, E. Behar, S. KaspiIs the Fe M-Shell Absorber Part of the Outflow in Active Galactic Nuclei?Astrophys. J. 632, 788-792 (2005)

Fe3+ 16+ ExpO6+ 7+ Exp

389. K. T. ChungAuger Decay of Multiply Excited Atomic SystemsPhys. Rev. A 59, 2065-2070 (1999)

Li0+ + ThLi+ Th

151

390. A. K. Roy, B. M. DebAtomic Inner-Shell Transitions: A Density Functional ApproachPhys. Lett. A 234, 465-471 (1997)

B ThBe ThLi ThNe ThO Th

391. P. Jonsson, C. Froese Fischer, J. BieronMulticonfiguration Hartree-Fock Calculations of Low-Lying Excited 2S States inLithiumPhys. Rev. A 52, 4262-4265 (1995)

Li Th

392. C. Froese Fischer, H. P. SahaPhotoionization of MagnesiumCan. J. Phys. 65, 772-776 (1987)

Mg Th

393. M. H. Chen, B. CrasemannAuger and Radiative Decay Rates of 1s Vacancy States in the Boron IsoelectronicSequence: Effects of Relativity and Configuration InteractionPhys. Rev. A 35, 4579-4585 (1987)

B Z= 6-54 Th

394. H. L. Zhang, C. J. FontesRelativistic distorted-wave collision strengths and oscillator strengths for the 185∆n = 0 transitions with n = 2 in the 67 C-like ions with 26≤Z≤92At. Data Nucl. Data Tables 101, 41-142 (2015)

C Z= 26-92 Th

395. J. A. Santana, J. K. Lepson, E. Trabert, P. BeiersdorferElectron-Correlation effects on the 3C to 3D line-intensity ratio in the Ne-like ionsAr8+ to kr26+

Phys. Rev. A 91, 012502 (2015)

Ne Z= 18-36 Th

396. P. QuinetAtomic structure, radiative lifetime and oscillator strength calculations in doublyionized molybdenum (Mo III)Phys. Scr. 90, 015404 (2015)

Mo2+ Th

397. G.-J. Bian, F. He, G. Jiang, Q.-P. Fan, F. HuInfluence of electron correlation on transition energy of gold ionsPhys. Scr. 90, 015403 (2015)

Au47+ 50+ Th

398. A. Abou El-Maaref, S. Schippers, A. MullerAb-Initio calculations of level energies, oscillator strengths and radiative rates for E1transitions in beryllium-like ironAtoms 3, 2-52 (2015)

152

Fe22+ Th

399. S. S. Tayal, O. ZatsarinnyElectron impact excitation collision strengths for extreme ultraviolet lines of Fe VIIAstrophys. J. 788, 24 (2014)

Fe6+ Th

400. A. M. Sossah, S. S. TayalEffective collision strengths for fine-structure transitions in Si VIIAstrophys. J. 787, 2 (2014)

Si6+ Th

401. G. Del Zanna, N. R. BadnellAtomic data for astrophysics: Improved collision strengths for Fe VIIIAstron. Astrophys. 570, p.A56 (2014)

Fe7+ Th

402. G. Del Zanna, P. J. Storey, H. E. MasonAtomic data for astrophysics: Ni XVAstron. Astrophys. 567, p.A18 (2014)

Ni14+ Th

403. H. G. Wei, J. R. Shi, F. L. Wang, J. Y. Zhong, G. Y. Liang, G. ZhaoK-Shell energy levels and radiative rates for transitions in Si IXAstron. Astrophys. 566, p.A105 (2014)

Si8+ Th

404. G. Del Zanna, P. J. Storey, N. R. BadnellAtomic data for astrophysics: Ni XIAstron. Astrophys. 566, p.A123 (2014)

Ni10+ Th

405. G. Del Zanna, P. J. Storey, N. R. Badnell, H. E. MasonAtomic data for astrophysics: Fe IXAstron. Astrophys. 565, p.A77 (2014)

Fe8+ Th

406. J. Ekman, P. Jonsson, S. Gustafsson, H. Hartman, G. Gaigalas, M. R. Godefroid, C. Froese FischerCalculations with spectroscopic accuracy: Energies, transition rates, and Lande gJ -factors in the carbon isoelectronic sequence from Ar XIII to Zn XXVAstron. Astrophys. 564, p.A24 (2014)

C Z= 18-30 Th

407. D. K. Nandy, B. K. SahooSpectral properties of a few F-like ionsAstron. Astrophys. 563, p.A25 (2014)

Mo33+ ThF Z= 22-30 Th

408. N. C. Deb, A. Hibbertlog gf values for astrophysically important transitions Fe IIAstron. Astrophys. 561, p.A32 (2014)

153

Fe+ Th

409. M. T. Belmonte, S. Djurovic, R. J. Pelaez, J. A. Aparicio, S. MarImproved and expanded measurements of transition probabilities in UV Ar II spectrallinesMon. Not. R. Astron. Soc. 445, 3345-3351 (2014)

Ar+ Exp

410. M. P. Ruffoni, E. A. Den Hartog, J. E. Lawler, N. R. Brewer, K. Lind, G. Nave, J. C. PickeringFe I oscillator strengths for the Gaia-ESO surveyMon. Not. R. Astron. Soc. 441, 3127-3136 (2014)

Fe Exp

411. T. V. B. Nguyen, C. T. Chantler, J. A. Lowe, I. P. GrantAdvanced ab initio relativistic calculations of transition probabilities for some O I andO III emission linesMon. Not. R. Astron. Soc. 440, 3439-3443 (2014)

O ThO2+ Th

412. X. Gao, X.-Y. Han, D.-L. Zeng, R. Jin, J.-M. LiBroken scaling laws of the transition probabilities from jj to LS coupling transitionsPhys. Lett. A 378, 1514-1519 (2014)

N Z= 7-80 Th

413. N. K. Piracha, K. V. Duncan-Chamberlin, J. Kaminsky, D. Delanis, M. A. BaigOn the relative transition probabilities of rare gases in the 1si-2pj regionOpt. Commun. 329, 200-205 (2014)

Ar ExpKr ExpNe ExpXe Exp

414. A. KramidaEnergy levels and spectral lines of quadruply ionized iron (Fe V)Astrophys. J., Suppl. Ser. 212, 11 (2014)

Fe4+ Th

415. Q. Wang, L. Y. Jiang, P. Quinet, P. Palmeri, W. Zhang, X. Shang, Y. S. Tian, Z. W. DaiTR-LIF lifetime measurements and HFR+CPOL calculations of radiative parametersin vanadium atom (V I)Astrophys. J., Suppl. Ser. 211, 31 (2014)

V E/T

416. Y. P. Liu, C. Gao, J. L. Zeng, J. M. Yuan, J. R. ShiAtomic data of Cu I for the investigation of element abundanceAstrophys. J., Suppl. Ser. 211, 30 (2014)

Cu Th

417. M. P. Wood, J. E. Lawler, C. Sneden, J. J. CowanImproved Ni I log(gf) values and abundance determinations in the photospheres ofthe sun and metal-poor star HD 84937Astrophys. J., Suppl. Ser. 211, 20 (2014)

154

Ni Exp

418. J. MusielokRecently published line strengths for the transition array 3s-3p in C I, N II and O III:A critical reviewPhys. Scr. T161, 014057 (2014)

C Z= 6-8 Th

419. J. Ruczkowski, M. Elantkowska, J. DembczynskiSemi-Empirical calculations of oscillator strengths and hyperfine constants for Ti IIJ. Quant. Spectrosc. Radiat. Transfer 149, 168-183 (2014)

Ti+ Th

420. F. Hu, M.-F. Mei, C. Han, B.-P. Han, G. Jiang, J.-M. YangAccurate multiconfiguration Dirac-Hartree-Fock calculations of transition probabilitiesfor magnesium-like ionsJ. Quant. Spectrosc. Radiat. Transfer 149, 158-167 (2014)

Mg Z= 19-92 Th

421. G. G. Konan, L. Ozdemir, G. UrerEnergy levels and strong electric dipole transitions in magnesium-like goldJ. Quant. Spectrosc. Radiat. Transfer 145, 110-120 (2014)

Au67+ Th

422. C. Chen, Y. Sun, B. C. GouEnergies, radiative and Auger transitions of the core-excited states for the boron atomJ. Quant. Spectrosc. Radiat. Transfer 145, 1-8 (2014)

B Th

423. A. Alkauskas, P. Rynkun, G. Gaigalas, A. Kyniene, R. Kisielius, S. Kucas, S. Masys, G. Merkelis,V. JonauskasTheoretical investigation of spectroscopic properties of W25+


W25+ Th

424. C. Jiang, F. Hu, Y. Zang, G. JiangProperties of the Kα X-ray transitions in highly ionized chlorineActa Phys. Pol. A 126-3, 694-699 (2014)

Cl7+ 15+ Th

425. S. J. AdelmanElemental abundance analyses with DAO spectrograms. XXXV. On the ironabundances of B and A starsPubl. Astron. Soc. Pac. 126, 505-508 (2014)

Fe E/T

426. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates, and lifetimes for transitions in W LVIIIAt. Data Nucl. Data Tables 100, 1603-1767 (2014)

W57+ Th

155

427. P. Bogdanovich, R. KisieliusEnergy level properties of 4p64d3, 4p64d24f, and 4p54d4 configurations of the W35+ ionAt. Data Nucl. Data Tables 100, 1593-1602 (2014)

W35+ Th

428. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates, and lifetimes for transitions in W XLAt. Data Nucl. Data Tables 100, 1399-1518 (2014)

W39+ Th

429. M. Xu, G. Jiang, B.-L. Deng, G.-J. BianWavelengths, transition probabilities, and oscillator strengths for M-shell transitionsin Co-, Ni-, Cu-, Zn-, Ga-, Ge-, and Se-like Au ionsAt. Data Nucl. Data Tables 100, 1357-1398 (2014)

Au45+ 52+ Th

430. B.-L. Deng, G. Jiang, C. ZhangRelativistic configuration-interaction calculations of electric dipole n = 2 – n = 3transitions for medium-charge Li-like ionsAt. Data Nucl. Data Tables 100, 1337-1355 (2014)

Li Z= 7-30 Th

431. S. N. NaharOscillator strengths and transition probabilities from the Breit-Pauli R-matrix method:Ne IVAt. Data Nucl. Data Tables 100, 1322-1336 (2014)

Ne3+ Th

432. F. El-SayedEnergy levels, lifetimes, and transition probabilities for Mn XII and Ge XIXAt. Data Nucl. Data Tables 100, 1250-1276 (2014)

Ge18+ ThMn11+ Th

433. L. Liang, X.-Y. Liu, C. ZhouEnergy levels, oscillator strengths, radiative decay rates, and fine-structure collisionstrengths for the Zn-like ions Nb XII and Mo XIIIAt. Data Nucl. Data Tables 100, 1059-1109 (2014)

Mo12+ ThNb11+ Th

434. Y. Gokce, G. Celik, M. YildizElectric quadrupole transition probabilities and line strengths of Ti11+


Ti12+ E/T

435. G. Celik, Y. Gokce, M. YildizElectric quadrupole transition probabilities for atomic lithiumAt. Data Nucl. Data Tables 100, 792-801 (2014)

Li Th

156

436. A. Abou El-Maaref, M. Ahmad, S. H. AllamFine-Structure calculations of energy levels, oscillator strengths, and transitionprobabilities for sulfur-like iron, Fe XIAt. Data Nucl. Data Tables 100, 781-791 (2014)

Fe10+ Th

437. S. Aggarwal, N. Verma, A. K. Singh, N. Singh, R. Sharma, M. MohanMulticonfigurational Dirac-Fock energy levels and radiative rates for Ni XXICan. J. Phys. 92, 1285-1296 (2014)

Ni20+ Th

438. K. M. Aggarwal, F. P. KeenanRadiative rates for E1, E2, M1, and M2 transitions among the 3s23p5, 3s3p6, and3s23p43d configurations of Cl-like W LVIIICan. J. Phys. 92, 1166-1177 (2014)

W57+ Th

439. M. Mohan, S. Aggarwal, N. SinghMulticonfigurational Dirac-Fock atomic structure calculations for Cl-like tungstenCan. J. Phys. 92, 177-183 (2014)

W57+ Th

440. M. Yildiz, Y. GokceLifetimes for singly ionized nitrogenCan. J. Phys. 92, 82-85 (2014)

N+ Th

441. Z. Fei, W. Li, J. Grumer, Z. Shi, R. Zhao, T. Brage, S. Huldt, K. Yao, R. Hutton, Y. ZouForbidden-Line spectroscopy of the ground-state configuration of Cd-like WPhys. Rev. A 90, 052517 (2014)

W26+ Th

442. Z. B. Chen, C. Z. Dong, L. Y. Xie, J. JiangInfluence of quantum interference on the polarization and angular distribution of x-ray radiation following electron-impact excitation of highly charged H-like and He-likeionsPhys. Rev. A 90, 012703 (2014)

Au77+ ThAu78+ ThMo40+ ThMo41+ ThU90+ ThU91+ Th

443. U. I. Safronova, A. S. Safronova, P. BeiersdorferMultipole transitions to determine lifetimes and polarizabilities in Mg-like ions fromSi2+ to Fm88+

Phys. Rev. A 90, 012519 (2014)

Mg Z= 13-100 Th

444. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and lifetimes for transitions in Br-like ions with38 ≤ Z ≤ 42Phys. Scr. 89, 125404 (2014)

157

Mo7+ ThNb6+ ThSr3+ ThY4+ ThZr5+ Th

445. A. N. Ryabtsev, E. Ya. Kononov, R. R. Kildiyarova, W.-U L. Tchang-Brillet, J.-F. Wyart, N.Champion, C. BlaessSpectra of the W VIII isoelectronic sequence: II. Ta VIIPhys. Scr. 89, 125403 (2014)

Ta6+ Th

446. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inBe-like Cl XIV, K XVI and Ge XXIXPhys. Scr. 89, 125401 (2014)

Cl13+ ThGe28+ ThK15+ Th

447. K. Haris, A. Kramida, A. TauheedExtended and revised analysis of singly ionized tin: Sn IIPhys. Scr. 89, 115403 (2014)

Sn+ E/T

448. C. Moreno-Dıaz, A. Alonso-Medina, C. ColonTheoretical Stark widths and shifts of spectral lines of 2p5nf and 2p55g configurationsof Mg IIIPhys. Scr. 89, 115401 (2014)

Mg2+ Th

449. E. TrabertE1-forbidden transition rates in ions of astrophysical interestPhys. Scr. 89, 114003 (2014)

S12+ E/TTi18+ E/TBe Z= 4-54 E/TP Z= 22-36 E/T

450. J. Grumer, T. Brage, M. Andersson, J.-G. Li, P. Jonsson, W.-X. Li, Y. Yang, R. Hutton, J.-M.ZhaoUnexpected transitions induced by spin-dependent, hyperfine and external magnetic-field interactionsPhys. Scr. 89, 114002 (2014)

Be Z= 4-92 ThNe Z= 10-35 Th

451. Dipti, T. Das, L. Sharma, R. SrivastavaL-Shell electron excitations of Mg- through O-like tungsten ionsPhys. Scr. 89, 085403 (2014)

W62+ 66+ Th

158

452. Y. Wang, O. Zatsarinny, K. BartschatB-spline R-matrix-with-pseudostates calculations for electron-impact excitation andionization of nitrogenPhys. Rev. A 89, 062714 (2014)

N Th

453. J. Grumer, R.-F. Zhao, T. Brage, W.-X. Li, S. Huldt, R. Hutton, Y.-M. ZouCoronal lines and the importance of deep-core-valence correlation in Ag-like ionsPhys. Rev. A 89, 062511 (2014)

Ag Z= 50-94 Th

454. V. Gedeon, S. Gedeon, V. Lazur, E. Nagy, O. Zatsarinny, K. BartschatB-spline R-matrix-with-pseudostates calculations for electron-impact excitation andionization of fluorinePhys. Rev. A 89, 052713 (2014)

F Th

455. M. Fogle, D. Wulf, K. Morgan, D. McCammon, D. G. Seely, I. N. Draganic, C. C. HavenerX-Ray-Emission measurements following charge exchange between C6+ and H2

Phys. Rev. A 89, 042705 (2014)

C5+ Th

456. X.-Y. Han, X. Gao, D.-L. Zeng, R. Jin, J. Yan, J.-M. LiScaling law for transition probabilities in 2p3 configuration from LS coupling to jjcouplingPhys. Rev. A 89, 042514 (2014)

N Z= 7-100 Th

457. L. Bougas, G. E. Katsoprinakis, D. Sofikitis, T. P. Rakitzis, P. C. Samartzis, T. N. Kitsopoulos, J.Sapirstein, D. Budker, V. A. Dzuba, V. V. Flambaum, M. G. KozlovStark shift and parity nonconservation for near-degenerate states of xenonPhys. Rev. A 89, 042513 (2014)

Xe Th

458. S. Roy, N. N. Dutta, S. MajumderRelativistic coupled-cluster calculations on hyperfine structures and electromagnetictransition amplitudes of In IIIPhys. Rev. A 89, 042511 (2014)

In2+ Th

459. N. D. Guise, J. N. Tan, S. M. Brewer, C. F. Fischer, P. JonssonMeasurement of the Kr XVIII 3d 2D5/2 lifetime at low energy in a unitary PenningtrapPhys. Rev. A 89, 040502 (2014)

Kr17+ E/T

460. G. P. Gupta, A. Z. MsezaneFine-Structure energy levels, oscillator strengths and lifetimes in Al-like chromiumIndian J. Phys. 88, 11-18 (2014)

Cr11+ Th

159

461. L.-H. Hao, X.-P. KangEnergy levels and spectral lines in the X-ray spectra of highly charged W XLIVEur. Phys. J. D 68, 203 (2014)

W43+ Th

462. I. L. Babich, V. F. Boretskij, A. N. Veklich, R. V. SemenyshynSpectroscopic data and Stark broadening of Cu I and Ag I spectral lines: Selectionand analysisAdv. Space Res. 54, 1254-1263 (2014)

Ag E/TCu E/T

463. H. ElabidiStructural and collisional data for Mg III and Al IVAdv. Space Res. 54, 1203-1222 (2014)

Al3+ ThMg2+ Th

464. N. Ben Nessib, N. Alonizan, R. Qindeel, S. Sahal-Brechot, M. S. DimitrijevicThe O IV 1407.3 A/1401.1 A emission-line ratio in a plasmaAdv. Space Res. 54, 1190-1194 (2014)

O3+ Th

465. H. Elabidi, S. Sahal-Brechot, M. S. DimitrijevicQuantum Stark broadening of Ar XV lines. Strong collision and quadrupolar potentialcontributionsAdv. Space Res. 54, 1184-1189 (2014)

Ar14+ Th

466. P. Bogdanovich, R. Kisielius, D. StonysMethods, algorithms, and computer codes for calculation of electron-impact excitationparametersLithuanian Phys. J. 54, 67-79 (2014)

He ThLi Th

467. S. Spencer, A. Hibbert, C. A. RamsbottomOscillator strengths and transition probabilities for the W XLV ionJ. Phys. B 47, 245001 (2014)

W44+ Th

468. S. Fan, Q. Wang, X. Shang, Y.-S. Tian, Z.-W. DaiExperimental branching fractions, transition probabilities and oscillator strengths inEu IJ. Phys. B 47, 215004 (2014)

Ar+ ExpEu Exp

469. T. Nagata, K. Kawajiri, S. Kosugi, N. Suzuki, M. Kemmotsu, T. Nandi, E. Sokell, Y. Azuma, F.KoikePhotoion spectroscopy on isolated Mn atoms in the 2p → 3d excitation region: I. Totalphotoion-yield spectrumJ. Phys. B 47, 185006 (2014)

160

Mn Th

470. Madhulita Das, B. K. Sahoo, S. PalRelativistic spectroscopy of plasma-embedded Li-like systems with screening effects intwo-body Debye potentialsJ. Phys. B 47, 175701 (2014)

Ca17+ ThTi19+ Th

471. M. L. Qiu, R. F. Zhao, X. L. Guo, Z. Z. Zhao, W. X. Li, S. Y. Du, J. Xiao, K. Yao, C. Y. Chen,R. Hutton, Y. ZouInvestigation of transitions between metastable levels of the first excited configurationof palladium-like tungstenJ. Phys. B 47, 175002 (2014)

W28+ Th

472. Y. A. Podpaly, J. D. Gillaspy, J. Reader, Yu. RalchenkoEUV measurements of Kr XXI–Kr XXXIV and the effect of a magnetic-dipole line onallowed transitionsJ. Phys. B 47, 095702 (2014)

Kr23+ Th

473. J. Migdalek, W. SiegelRelativistic effects in E1 transition oscillator strengths along the Yb+ isoelectronicsequenceJ. Phys. B 47, 075003 (2014)

Tm Z= 70-88 Th

474. S. Civis, P. Kubelık, M. Ferus, V. E. Chernov, E. M. Zanozina, L. JuhaLaser ablation of an indium target: Time-resolved Fourier-transform infrared spectraof In I in the 700–7700 cm−1 rangeJ. Anal. At. Spectrom. 29, 2275-2283 (2014)

In Th

475. S. AggarwalAtomic structure calculations for F-like tungstenChin. Phys. B 23, 093203 (2014)

W65+ Th

476. A. KramidaAssessing uncertainties of theoretical atomic transition probabilities with Monte Carlorandom trialsAtoms 2, 86-122 (2014)

Fe4+ Th

477. E. TrabertCritical assessment of theoretical calculations of atomic structure and transitionprobabilities: An experimenter’s viewAtoms 2, 15-85 (2014)

Cl Z= 18-29 E/TB Z= 18-22 E/TBe Z= 4-36 E/TF Z= 17-22 E/TFe13+ E/THe Z= 3-54 E/TC Z= 14-16 E/TO Z= 14-16 E/T

161

478. C. Froese FischerEvaluation and comparison of the configuration interaction calculations for complexatomsAtoms 2, 1-14 (2014)

W39+ Th

479. P. Jonsson, M. Godefroid, G. Gaigalas, J. Bieron, T. BrageAccurate transition probabilities from large-scale multiconfiguration calculations – Atribute to Charlotte Froese FischerAIP Conf. Proc. 1545, 266-278 (2013)

B+ Th

480. S. SchippersStorage-ring measurements of hyperfine induced transition rates in berylliumlike ionsAIP Conf. Proc. 1545, 7-16 (2013)

S12+ E/TTi18+ E/TBe Z= 6-92 E/T

481. P. Jonsson, J. Ekman, S. Gustafsson, H. Hartman, L. B. Karlsson, R. du Rietz, G. Gaigalas, M. R.Godefroid, C. Froese FischerEnergy levels and transition rates for the boron isoelectronic sequence: Si X, Ti XVIII– Cu XXVAstron. Astrophys. 559, p.A100 (2013)

Si9+ ThB Z= 22-29 Th

482. H. Elabidi, S. Sahal-BrechotExcitation cross-sections by electron impact for O V and O VI levelsMon. Not. R. Astron. Soc. 436, 1452-1464 (2013)

O4+ 5+ Th

483. M. P. Wood, J. E. Lawler, C. Sneden, J. J. CowanImproved Ti II log(gf) values and abundance determinations in the photospheres ofthe Sun and metal-poor star HD 84937Astrophys. J., Suppl. Ser. 208, 27 (2013)

Ti+ Exp

484. I. L. Glukhov, E. A. Nikitina, V. D. OvsiannikovThermal shifts and broadening of Rydberg levels in Be II ionsPhys. Scr. T157, 014014 (2013)

Be+ Th

485. S. Itoi, H. Kai, M. Saito, Y. HaruyamaRadiative lifetime measurement of the 1S0 metastable state of Kr2+ using anelectrostatic ion trapPhys. Scr. T156, 014023 (2013)

Kr2+ Exp

486. J. P. Santos, J. P. Marques, A. M. Costa, M. C. Martins, P. Indelicato, F. ParenteTransition probability values of the 1s22s3p 3P0 level in Be-like ionsPhys. Scr. T156, 014020 (2013)

162

C2+ ThFe22+ ThNe6+ ThU88+ ThXe50+ Th

487. J. K. Rudolph, S. Bernitt, S. W. Epp, R. Steinbrugge, C. Beilmann, G. V. Brown, S. Eberle, A.Graf, Z. Harman, N. Hell, M. Leutenegger, A. Muller, K. Schlage, H.-C. Wille, H. Yavas, J. Ullrich,J. R. Crespo Lopez-UrrutiaX-Ray resonant photoexcitation: Linewidths and energies of Kα transitions in highlycharged Fe ionsPhys. Rev. Lett. 111, 103002 (2013)

Xe17+ 20+ ExpXe22+ 24+ Exp

488. H. Asghar, R. Ali, M. A. BaigDetermination of transition probabilities for the 3p → 3s transition array in neon usinglaser induced breakdown spectroscopyPhys. Plasmas 20, 123302 (2013)

Ne Exp

489. U. I. Safronova, A. S. Safronova, P. BeiersdorferRelativistic atomic data for Cu-like tungstenPhys. Rev. A 86, 042510 (2012)

W45+ Th

490. G. P. Gupta, V. Tayal, A. Z. MsezaneFine-structure energy levels and radiative rates in Si-like chlorineIndian J. Phys. 86, 1-8 (2012)

Cl3+ Th

491. E. Landi, A. K BhatiaAtomic data and spectral line intensities for Ca IXAt. Data Nucl. Data Tables 100, 1519 (2014)

e + Ca8+ 0−60 RYD Th

492. Zanna Del, G.Benchmarking atomic data for astrophysics: Fe XVII X-ray linesAstron. Astrophys. 536, A59 (2011)

e + Fe16+ ThP + Fe16+ Th

493. A. K. Bhatia, E. LandiAtomic data and spectral line intensities for Ni XIAt. Data Nucl. Data Tables 97, 50 (2011)

e + Ni10+ threshold−1000 eV The + Ni10+ threshold−1000 eV Th

494. A. K. Bhatia, E. LandiAtomic data and spectral line intensities for Ni XVIIAt. Data Nucl. Data Tables 97, 189 (2011)

e + Ni16+ threshold−1700 eV The + Ni16+ threshold−1700 eV Th

163

495. Landi, E.Atomic data and spectral line intensities for Fe XVAt. Data Nucl. Data Tables 97, 587 (2011)

e + Fe14+ threshold−1670 eV The + Fe14+ threshold−1670 eV Th

496. P. Jonsson, P. Rynkun, G. GaigalasEnergies, E1, M1, and E2 transition rates, hyperfine structures, and Lande g(J)factors for states of the 2s(2)2p(2), 2s2p(3), and 2p(4) configurations in carbon-likeions between F IV and Ni XXIIIAt. Data Nucl. Data Tables 97, 648 (2011)

e + C Z= 9-28 The + C Z= 9-28 Th

3.2 Atomic and Molecular Collisions

3.2.1 Electron Collisions

497. David Bote, Francesc Salvat, Aleksander Jablonski, Cedric J. PowellCross sections for ionization of K, L and M shells of atoms by impact of electrons andpositrons with energies up to 1 GeV: Analytical formulasAt. Data Nucl. Data Tables 95, 871 (2009)

e + Es ned The + Cf ned The + Bk ned The + Cm ned The + Am ned The + Pu ned The + Np ned The + U ned The + Pa ned The + Th ned The + Ac ned The + Ra ned The + Fr ned The + Rn ned The + At ned The + Po ned The + Bi ned The + Pb ned The + Tl ned The + Hg ned The + Au ned The + Pt ned The + Ir ned The + Os ned The + Re ned The + W ned The + Ta ned The + Hf ned The + Lu ned The + Yb ned The + Tm ned The + Er ned The + Ho ned The + Dy ned Th

164

e + Tb ned The + Gd ned The + Eu ned The + Sm ned The + Pm ned The + Nd ned The + Pr ned The + Ce ned The + La ned The + Ba ned The + Cs ned The + Xe ned The + I ned The + Te ned The + Sb ned The + Sn ned The + In ned The + Cd ned The + Ag ned The + Pd ned The + Rh ned The + Ru ned The + Tc ned The + Mo ned The + Nb ned The + Zr ned The + Y ned The + Sr ned The + Rb ned The + Kr ned The + Br ned The + Se ned The + As ned The + Ge ned The + Ga ned The + Zn ned The + Cu ned The + Ni ned The + Co ned The + Fe ned The + Mn ned The + Cr ned The + V ned The + Ti ned The + Sc ned The + Ca ned The + K ned The + Ar ned The + Cl ned The + S ned The + P ned The + Si ned The + Al ned The + Mg ned The + Na ned The + Ne ned The + F ned The + O ned The + N ned Th

165

e + C ned The + B ned The + Be ned The + Li ned The + He ned The + H ned Th

498. M. H. F. Bettega, R. F. daCosta, M. A. P. LimaLow-energy electron collisions with ethaneBraz. J. Phys. 39, 69 (2009)

e + C2H6 0−12 eV Th

499. Yu-Jun Hou, Xin-Lu Cheng, Heng-Jie ChenCalculated cross sections for the single ionization of atoms (N, Cu, As, Se, Sn, Sb, Te,I, Pb) by electron impactChin. Phys. B 18, 553 (2009)

e + Pb threshold−10000 eV The + I threshold−10000 eV The + Te threshold−10000 eV The + Sb threshold−10000 eV The + Sn threshold−10000 eV The + Se threshold−10000 eV The + As threshold−10000 eV The + Cu threshold−10000 eV The + N threshold−10000 eV Th

500. Hao Feng, Wei-Guo Sun, Yang-Yang ZengHigh order correlation-polarization potential for vibrational excitation scattering ofdiatomic molecules by low-energy electronsChin. Phys. B 18, 4846 (2009)

e + N2 0−10 eV The + N2 0−10 eV Th

501. Yuan-Cheng Wang, Ya-Jun Zhou, Yong-Jun Cheng, Jia MaCoupled-Channels Optical Calculation for Electron Scattering from Metastable HeliumChin. Phys. Lett. 26, 083401 (2009)

e + He 0−25 eV Th

502. Ning-Xuan Yang, Chen-Zhong Dong, Jun JiangRelativistic Distorted-Wave Collision Strengths of Ni-, Cu- and Zn-like Au IonsChin. Phys. Lett. 26, 053401 (2009)

e + Au49+ 100−1E4 eV The + Au50+ 100−1E4 eV The + Au51+ 100−1E4 eV Th

503. Yang-Yang Zeng, Hao Feng, Wei-Guo Sun, Bin WangDifferential Cross Sections for High-Lying Vibrational Excitations (upsilon=0 -¿upsilon’=1, 2,..., 9, 10) of e-H-2 ScatteringChin. Phys. Lett. 26, 023402 (2009)

e + H2 1−10 eV Th

504. J. R. Vacher, F. Jorand, N. Blin-Simiand, S. PasquiersElectron impact ionization of formaldehydeChem. Phys. Lett. 476, 178 (2009)

166

e + CH2O 50−85 eV Exp

505. M. R. Talukder, A. K. F. Haque, M. A. UddinElectron impact double ionization cross sections of light elementsEur. Phys. J. D 53, 133 (2009)

e + Ar7+ 0−1E6 eV The + Ar6+ 0−1E6 eV The + Ar5+ 0−1E6 eV The + Ar4+ 0−1E6 eV The + Ar3+ 0−1E6 eV The + Ar2+ 0−1E6 eV The + Ar+ 0−1E6 eV The + Ar 0−1E6 eV The + S 0−1E6 eV The + Al3+ 0−1E6 eV The + Mg 0−1E6 eV The + Na 0−1E6 eV The + Ne2+ 0−1E6 eV The + Ne+ 0−1E6 eV The + Ne 0−1E6 eV The + O3+ 0−1E6 eV The + O2+ 0−1E6 eV The + O 0−1E6 eV The + C3+ 0−1E6 eV The + C+ 0−1E6 eV The + B+ 0−1E6 eV The + Li+ 0−1E6 eV The + Li 0−1E6 eV The + H 0−1E6 eV Th

506. T. -M. Shen, C. -Y. Chen, Y. -S. Wang, Y. -M. ZouElectron impact excitation rate coefficients for Ni-like gadoliniumEur. Phys. J. D 53, 179 (2009)

e + Gd36+ 100−5000 eV Th

507. S. Kumari, L. K. Jha, B. N. RoyDouble ionization of Sc+ ions by electron impactEur. Phys. J. D 55, 93 (2009)

e + Sc+ 40−1000 eV Th

508. J. Lecointre, D. S. Belic, J. J. Jureta, R. K. Janev, P. DefranceAbsolute cross-sections and kinetic-energy-release distributions for electron-impactionization and dissociation of CD (2) (+)Eur. Phys. J. D 55, 557 (2009)

e + CD2+ 0−2.5 keV Exp



509. J. Lecointre, D. S. Belic, J. J. Jureta, R. K. Janev, P. DefranceAbsolute cross-sections and kinetic-energy-release distributions for electron-impactionization and dissociation of CD3+Eur. Phys. J. D 55, 569 (2009)




167

510. N. Endstrasser, F. Zappa, A. Mauracher, A. Bacher, S. Feil, D. K. Bohme, P. Scheier, M. Probst,T. D. MaerkAbsolute partial cross sections and kinetic energy analysis for the electron impactionization of ethyleneInt. J. Mass Spectrom. 280, 65 (2009)

e + C2H4 0−1000 eV Exp

511. M. A. R. Patoary, M. Alfaz Uddin, A. K. F. Haque, M. Shahjahan, A. K. Basak, M. R. Talukder,B. C. SahaEmpirical Model for the Electron Impact K-Shell Ionization Cross Section of AtomsInt. J. Quantum Chem. 109, 897 (2009)

e + U 0−2E9 eV The + Bi 0−2E9 eV The + Pb 0−2E9 eV The + Au 0−2E9 eV The + Ta 0−2E9 eV The + Ba 0−2E9 eV The + Sn 0−2E9 eV The + In 0−2E9 eV The + Ag 0−2E9 eV The + Pd 0−2E9 eV The + Mo 0−2E9 eV The + Y 0−2E9 eV The + Sr 0−2E9 eV The + Ga 0−2E9 eV The + Rb 0−2E9 eV The + Zn 0−2E9 eV The + Se 0−2E9 eV The + Cu 0−2E9 eV The + Ni 0−2E9 eV The + Co 0−2E9 eV The + Cr 0−2E9 eV The + V 0−2E9 eV The + Ar 0−2E9 eV The + Si 0−2E9 eV The + Al 0−2E9 eV The + Ne 0−2E9 eV The + N 0−2E9 eV The + C 0−2E9 eV The + He 0−2E9 eV The + H 0−2E9 eV Th

512. A. K. F. Haque, M. S. I. Sarker, M. A. R. Patoary, M. Shahjahan, M. Ismail Hossain, M. AlfazUddin, A. K. Basak, B. C. SahaModified Version of Revised Deutsch-Mark Model for Electron Impact K-ShellIonization Cross-Sections of Atoms at Relativistic EnergiesInt. J. Quantum Chem. 109, 1442 (2009)

e + U 0−2E9 eV The + Bi 0−2E9 eV The + Pb 0−2E9 eV The + Au 0−2E9 eV The + Ba 0−2E9 eV The + Sb 0−2E9 eV The + Sn 0−2E9 eV The + In 0−2E9 eV The + Ag 0−2E9 eV The + Pd 0−2E9 eV Th

168

e + Mo 0−2E9 eV The + Y 0−2E9 eV The + Sr 0−2E9 eV The + Se 0−2E9 eV The + Ge 0−2E9 eV The + Zn 0−2E9 eV The + Ni 0−2E9 eV The + Co 0−2E9 eV The + Fe 0−2E9 eV The + Mn 0−2E9 eV The + Cr 0−2E9 eV The + V 0−2E9 eV The + Ca 0−2E9 eV The + Ar 0−2E9 eV The + Si 0−2E9 eV The + Al 0−2E9 eV The + Ne 0−2E9 eV The + C 0−2E9 eV The + He 0−2E9 eV The + H 0−2E9 eV Th

513. A. Jablonski, F. Salvat, C. J. PowellPractical formulas for inner-shell ionization cross sections by electron impact:Applications in quantitative Auger electron spectroscopyJ. Appl. Phys. 106, 053706 (2009)

e + Au 0−30 keV The + Ag 0−30 keV The + Cu 0−30 keV The + Si 0−30 keV The + Al 0−30 keV Th

514. H. Kawahara, D. Suzuki, H. Kato, M. Hoshino, H. Tanaka, O. Ingolfsson, L. Campbell, M. J.BrungerCross sections for electron impact excitation of the C (II)-I-1 and D (1)Sigma(+)electronic states in N2OJ. Chem. Phys. 131, 114307 (2009)

e + N2O 15−200 eV Exp

515. S. E. Michelin, K. T. Mazon, F. Arretche, W. Tenfen, H. L. Oliveira, A. S. Falck, M. A. Scopel, L.S. S. daSilva, M. M. Fujimoto, I. Iga, M. -T. LeeComparative study of electron-impact C(1s) core-excitation processes in C-2 and C2N2moleculesJ. Electron Spectrosc. Relat. Phenom. 171, 30 (2009)

e + C2N2 300−800 eV The + C2 300−800 eV Th

516. G. Purohit, Vinod Patidar, K. K. SudImportance of polarization effects in electron impact single ionization of argon atomJ. Electron Spectrosc. Relat. Phenom. 175, 1 (2009)

e + Ar2+ 113 eV Th

517. A., Jr. Borovik, A. Mueller, S. Schippers, I. Bray, D. V. FursaElectron impact ionization of ground-state and metastable Li+ ionsJ. Phys. B 42, 025203 (2009)

e + Li+ 0−1000 eV E/T

169

518. A. Borovik, O. Zatsarinny, K. BartschatResonance effects in electron and photon impact excitation of the p(6) subvalencesubshell in alkali atomsJ. Phys. B 42, 044010 (2009)

e + Kr 0−18 eV E/Te + Cs 0−18 eV E/T

519. S. Chatterjee, S. Kasthurirangan, A. H. Kelkar, C. R. Stia, O. A. Fojon, R. D. Rivarola, L. C.TribediFast-electron impact ionization of molecular hydrogen: energy and angular distributionof double and single differential cross sections and Young-type interferenceJ. Phys. B 42, 065201 (2009)

e + H2 8 keV Exp

520. M. Becher, B. JoulakianK-shell (e, 3e) double ionization of beryllium by relativistic electronsJ. Phys. B 42, 065206 (2009)

e + Be 0−500 keV Th

521. J. Lecointre, M. O. Abdellahi ElGhazaly, J. J. Jureta, D. S. Belic, X. Urbain, P. DefranceAbsolute cross-sections and kinetic energy release distributions for electron-impactdissociation of D-3(+)J. Phys. B 42, 075201 (2009)

e + D3+ 0−2.5 keV Exp

e + D3+ 0−2.5 keV Exp

e + D3+ 0−2.5 keV Exp

522. Ireneusz Linert, Mariusz ZubekDifferential cross sections for electron elastic scattering and vibrational upsilon=1excitation in nitrogen in the energy range from 5 to 20 eV measured over an angularrange of 10 degrees-180 degreesJ. Phys. B 42, 085203 (2009)

e + N2 5−20 eV Exp

523. Hemal N. Varambhia, Monika Gupta, Alexandre Faure, K. L. Baluja, Jonathan TennysonElectron collision with the silicon monoxide (SiO) molecule using the R-matrix methodJ. Phys. B 42, 095204 (2009)

e + SiO 0−10 eV Th

524. S. Caprasecca, J. D. Gorfinkiel, D. Bouchiha, L. G. CaronMultiple scattering approach to elastic electron collisions with molecular clustersJ. Phys. B 42, 095205 (2009)

e + H4O2 0−10 eV Th

525. Brent R. Yates, Kyle Keane, Murtadha A. KhakooNear-threshold electron impact doubly differential cross sections for the ionization ofneon and xenonJ. Phys. B 42, 095206 (2009)

e + Xe 14−40 eV Expe + Ne 14−40 eV Exp

526. K. Chakrabarti, Jonathan TennysonR-matrix calculation of electron collisions with the BF+ molecular ionJ. Phys. B 42, 105204 (2009)

170

e + BF+ 0−20 eV Th

527. J. Colgan, M. Foster, M. S. Pindzola, I. Bray, A. T. Stelbovics, D. V. FursaTriple differential cross sections for the electron-impact ionization of helium at 102 eVincident energyJ. Phys. B 42, 145002 (2009)

e + He 102 eV Th

528. M. Hoshino, H. Kato, H. Tanaka, I. Bray, D. V. Fursa, S. J. Buckman, O. Ingolfsson, M. J. BrungerBenchmark differential cross sections for electron impact excitation of the n=2 statesin helium at near-ionization-threshold energiesJ. Phys. B 42, 145202 (2009)

e + He 23.5−35 eV E/T

529. A. Lahmam-Bennani, A. Naja, E. M. Staicu Casagrande, N. Okumus, C. DalCappello, I.Charpentier, S. HouamerDynamics of electron impact ionization of the outer and inner valence (1t(2) and2a(1)) molecular orbitals of CH4 at intermediate and large ion recoil momentumJ. Phys. B 42, 165201 (2009)

e + CH4 500 eV E/T

530. A. Borovik, A. KupliauskieneThe 5p(6) autoionization cross section of cesium atoms: contribution to singleionization by electron impactJ. Phys. B 42, 165202 (2009)

e + Kr 12.3−16.6 eV E/Te + Cs 12.3−16.6 eV E/T

531. J. Colgan, O. Al-Hagan, D. H. Madison, A. J. Murray, M. S. PindzolaDeep interference minima in non-coplanar triple differential cross sections for theelectron-impact ionization of small atoms and moleculesJ. Phys. B 42, 171001 (2009)

e + H2 33.6 eV−64.6 eV E/Te + He 33.6 eV−64.6 eV E/Te + H 33.6 eV−64.6 eV E/T

532. Hao Feng, Weiguo Sun, Michael A. Morrison, Andrew N. FeldtExact inclusion of exchange in calculations of cross sections for vibrational excitationof N-2 by low-energy electronsJ. Phys. B 42, 175201 (2009)

e + N2 0−10 eV The + N2 0−10 eV The + N2 0−10 eV Th

533. C. P. Ballance, J. A. Ludlow, M. S. Pindzola, S. D. LochElectron-impact ionization of ground and metastable neonJ. Phys. B 42, 175202 (2009)

e + Ne 0−100 eV Th

534. A. C. Renwick, I. Bray, D. V. Fursa, J. Jacobi, H. Knopp, S. Schippers, A. MuellerElectron-impact ionization of B3+ ionsJ. Phys. B 42, 175203 (2009)

e + B3+ 0−2000 eV E/T

171

535. Xianming Liu, Paul V. Johnson, Charles P. Malone, Jason A. Young, Donald E. Shemansky, IsikKanikElectron-impact excitation and emission cross sections of the H-2 B ’ (1)Sigma(+)(u)and D (1)Pi(u) states and rotational dependence of photodissociation cross sections ofthe B ’ (1)Sigma(+)(u) and D (1)Pi(u) continuaJ. Phys. B 42, 185203 (2009)

e + H2 13.5−1000 eV Th

536. M. A. Khodorkovskii, S. V. Murashov, T. O. Artamonova, L. P. Rakcheeva, A. A. Beliaeva, A. L.Shakhmin, D. Michael, N. A. Timofeev, A. S. Mel’nikov, I. A. Shevkunov, G. ZissisExcitation of water molecules by electron impact with formation of OH-radicals in theA(2)Sigma(+) stateJ. Phys. B 42, 215201 (2009)

e + H2O 0−120 eV Expe + OH 0−120 eV Expe + H2O 0−120 eV Expe + OH 0−120 eV Exp

537. M. S. Pindzola, J. A. Ludlow, F. Robicheaux, J. Colgan, D. C. GriffinElectron-impact double ionization of magnesiumJ. Phys. B 42, 215204 (2009)

e + Mg 0−100 eV Th

538. C. P. Malone, P. V. Johnson, J. A. Young, X. Liu, B. Ajdari, M. A. Khakoo, I. KanikIntegral cross sections for electron-impact excitation of the C-3 Pi(u), E-3 Sigma(+)(g)and a ” (1)Sigma(+)(g) states of N-2J. Phys. B 42, 225202 (2009)

e + N2 13−100 eV Exp

539. Yukikazu ItikawaCross Sections for Electron Collisions with Oxygen MoleculesJ. Phys. Chem. Ref. Data 38, 1 (2009)

e + O2 0−1000 eV E/Te + O2 0−1000 eV E/Te + O2 0−1000 eV E/Te + O2 0−1000 eV E/Te + O2 0−1000 eV E/Te + O2 0−1000 eV E/Te + O2 0−1000 eV E/T

540. K. N. Joshipura, Sumona S. Gangopadhyay, Harshit N. Kothari, Foram A. ShelatTotal electron scattering and ionization of N, N-2 and metastable excitedN-2*(A(3)Sigma u(+)): Theoretical cross sectionsPhys. Lett. A 373, 2876 (2009)

e + N2 0−1 keV E/Te + N 0−1 keV E/Te + N2 0−1 keV E/Te + N 0−1 keV E/Te + N2 0−1 keV E/Te + N 0−1 keV E/T

541. R. Celiberto, R. K. Janev, D. ReiterBasic molecular processes for hydrocarbon spectroscopy in fusion edge plasmas:vibrationally state-selective excitation of A (2)Delta, B (2)Sigma(-) and C(2)Sigma(+) states of CH by electron impactPlasma Phys. and Controlled Fusion 51, 085012 (2009)

172

e + CH 0−30 eV Th

542. S. D. Loch, C. P. Ballance, M. S. Pindzola, D. P. StotlerThe role of excited state ionization data on H and He generalized collisional-radiativecoefficientsPlasma Phys. and Controlled Fusion 51, 105006 (2009)

e + H+ 0−100 eV The + He 0−100 eV The + H 0−100 eV Th

543. Michal Tarana, Bernd M. Nestmann, Jiri HoracekR-matrix calculations of the (2)A(g) elastic electron scattering off the Li-2 moleculePhys. Rev. A 79, 012716 (2009)

e + Li2 0−2.5 eV Th

544. C. P. Malone, P. V. Johnson, I. Kanik, B. Ajdari, M. A. KhakooElectron-impact excitation of molecular nitrogen. I. Excitation of the C (3)Pi(u), E(3)Sigma(+)(g), and a(’) (1)Sigma(+)(g) statesPhys. Rev. A 79, 032704 (2009)

e + N2 13−100 eV Exp

545. C. P. Malone, P. V. Johnson, I. Kanik, B. Ajdari, S. S. Rahman, S. S. Bata, A. Emigh, M. A.KhakooElectron-impact excitation of molecular nitrogen. II. Vibrationally resolved excitationof the C (3)Pi(u)(v(’)) statePhys. Rev. A 79, 032705 (2009)

e + N2 13−100 eV Exp

546. K. Fennane, J. -Cl. Dousse, J. Hoszowska, M. Berset, W. Cao, Y. -P. Maillard, J. Szlachetko, M.Szlachetko, M. KavcicDouble K-shell ionization of Al induced by photon and electron impactPhys. Rev. A 79, 032708 (2009)

e + Al 0−25 keV Exp

547. Hema Munjal, K. L. Baluja, Jonathan TennysonElectron collisions with the NO2 radical using the R-matrix methodPhys. Rev. A 79, 032712 (2009)

e + NO2 1−12 eV The + NO2 1−12 eV Th

548. J. A. Ludlow, C. P. Ballance, S. D. Loch, M. S. Pindzola, D. C. GriffinElectron-impact single ionization of Mg and Al+Phys. Rev. A 79, 032715 (2009)

e + Al+ 1−1000 eV The + Mg 1−1000 eV Th

549. S. A. Napier, D. Cvejanovic, J. F. Williams, L. Pravica, D. Fursa, I. Bray, O. Zatsarinny, K.BartschatEmission cross sections for electron-impact excitation of zinc atomsPhys. Rev. A 79, 042702 (2009)

e + Zn 0−300 eV E/T

173

550. S. J. Brotton, E. Vyskocil, W. Kedzierski, J. W. McConkeyDissociative excitation of H2S by electron impactPhys. Rev. A 79, 042709 (2009)

e + H2S 0−300 eV Expe + H2S 0−300 eV Exp

551. F. Juettemann, G. F. Hanne, O. Zatsarinny, K. BartschatSpin-resolved electron-impact excitation of the 6s6p (J=1) states in mercuryPhys. Rev. A 79, 042712 (2009)

e + Hg 0−80 eV E/T

552. O. Zatsarinny, K. BartschatFully relativistic B-spline R-matrix calculations for electron collisions with mercuryPhys. Rev. A 79, 042713 (2009)

e + Hg 0−200 eV E/T

553. E. M. Bahati, M. Fogle, C. R. Vane, M. E. Bannister, R. D. Thomas, V. ZhaunerchykElectron-impact dissociation of CD3+ and CH3+ ions producing CD2+, CH+ andC+ fragment ionsPhys. Rev. A 79, 052703 (2009)

e + CH3+ 0−100 eV Exp

e + CD3+ 0−100 eV Exp

554. J. Colgan, O. Al-Hagan, D. H. Madison, C. Kaiser, A. J. Murray, M. S. PindzolaTriple differential cross sections for the electron-impact ionization of H-2 molecules forequal and unequal outgoing electron energiesPhys. Rev. A 79, 052704 (2009)

e + H2 35.4 eV Th

555. Jingjun Zhu, Zhu An, Mantian Liu, Lixia TianMeasurements of the K-shell ionization cross sections of Si by 3-25-keV electron impactusing the thick-target methodPhys. Rev. A 79, 052710 (2009)

e + Si 3−25 keV Exp

556. M. A. Khakoo, C. Winstead, V. McKoyVibrational excitation of water by electron impactPhys. Rev. A 79, 052711 (2009)

e + H2O 0−100 eV E/T

557. J. Franz, I. Baccarelli, S. Caprasecca, F. A. GianturcoComputed vibrational excitation of CF4 by low-energy electrons and positrons:Comparing calculations and experimentsPhys. Rev. A 80, 012709 (2009)

e + CF4 0−1.5 eV Th

558. R. Celiberto, R. K. Janev, J. M. Wadehra, A. LaricchiutaCross sections for 14-eV e-H-2 resonant collisions: Dissociative electron attachmentPhys. Rev. A 80, 012712 (2009)

e + H2 2−18 eV The + H2 2−18 eV Th

174

559. M. -T. Lee, I. Iga, L. E. Machado, L. M. BrescansinTheoretical investigation of electron collisions with sulfur monoxide in the low- andintermediate-energy rangePhys. Rev. A 80, 022706 (2009)

e + SO 1−500 eV Th

560. V. Suvorov, P. J. O. Teubner, V. Karaganov, K. Ratnavelu, Y. Zhou, M. J. BrungerIntegral cross sections for electron-impact excitation of the 4 P-2 state in copperPhys. Rev. A 80, 022711 (2009)

e + Cu 0−100 eV E/T

561. Dmitry V. Fursa, Christopher J. Bostock, Igor BrayRelativistic convergent close-coupling method: Calculations of electron scattering fromcesiumPhys. Rev. A 80, 022717 (2009)

e + Cs 5−15 eV The + Cs 5−15 eV Th

562. Savinder Kaur, K. L. BalujaElectron-impact study of AlH using the R-matrix methodPhys. Rev. A 80, 042701 (2009)

e + AlH The + AlH The + AlH Th

563. Christopher J. Bostock, Dmitry V. Fursa, Igor BrayRelativistic convergent close-coupling method: Calculation of electron scattering fromhydrogenlike ionsPhys. Rev. A 80, 052708 (2009)

e + U91+ 0−600 eV Th

564. L. R. Hargreaves, C. Colyer, M. A. Stevenson, B. Lohmann, O. Al-Hagan, D. H. Madison, C. G.Ning(e, 2e) study of two-center interference effects in the ionization of N-2Phys. Rev. A 80, 062704 (2009)

e + N2 75, 150 eV E/T

565. R. O. Jung, John B. Boffard, L. W. Anderson, Chun C. LinExcitation into 5p(5)7p levels from the ground level and the J=2 metastable level ofXePhys. Rev. A 80, 062708 (2009)

e + Xe Exp

566. T. C. Freitas, M. A. P. Lima, S. Canuto, M. H. F. BettegaElectron collisions with the CH2O-H2O complexPhys. Rev. A 80, 062710 (2009)

e + H2O 0.1−10 eV The + CH2O 0.1−10 eV Th

567. Vladislav V. Serov, Boghos B. JoulakianImplementation of the external complex scaling method in spheroidal coordinates:Impact ionization of molecular hydrogenPhys. Rev. A 80, 062713 (2009)

175

e + H2 4081 eV Th

568. Yu. M. SmirnovElectron impact excitation cross sections of tungsten atomHigh Temperature 47, 13 (2009)

e + W 50 eV Exp

569. V. Jonauskas, S. Kucas, R. KarazijaELECTRON-IMPACT DOUBLE IONIZATION OF TUNGSTEN ATOMS ANDIONS AT LOW IONIZATION STAGESLithuanian Phys. J. 49, 415 (2009)

e + W6+ 0−5000 eV Expe + W4+ 0−5000 eV Expe + W2+ 0−5000 eV Expe + W 0−5000 eV Exp

570. P. Bryans, H. Kreckel, E. Roueff, V. Wakelam, D. W. SavinMOLECULAR CLOUD CHEMISTRY AND THE IMPORTANCE OFDIELECTRONIC RECOMBINATIONAstrophys. J. 694, 286 (2009)

e + Mg+ 0−1000 K The + Na+ 0−1000 K The + O+ 0−1000 K The + N+ 0−1000 K The + C+ 0−1000 K The + He+ 0−1000 K Th

571. Li Zhou, Fan-Chang Meng, Min Huang, Chong-Yang Chen, Yan-Sen WangDielectronic recombination of Co-like tantalumChin. Phys. B 18, 3409 (2009)

e + Ta46+ 1−1E5 eV Th

572. Zhi-Min Hu, Jia-Min Yang, Ji-Yan Zhang, Tuo Zhu, Bao-Han Zhang, Yao-Nan Ding, Zhi-JianZheng, Bin Duan, Yue-Ming Li, Jun YanMeasurement of the KLL Dielectronic Recombination Resonances in He-like to C-likeKr IonsChin. Phys. Lett. 26, 033401 (2009)

e + Kr30+ 8.6−9.6 keV Expe + Kr31+ 8.6−9.6 keV Expe + Kr32+ 8.6−9.6 keV Expe + Kr33+ 8.6−9.6 keV Expe + Kr34+ 8.6−9.6 keV Exp

573. Bin Zhou, Shu-Min LiElectron-Helium Scattering in a Bichromatic Laser Field in the Second-Order BornApproximationChin. Phys. Lett. 26, 043401 (2009)

e + He 9.5 eV Th

574. Qiu-Bo Hu, Jin-Feng SunLaser-Assisted Elastic Electron Scattering from ArgonCommun. Theor. Phys. 51, 131 (2009)

e + Ar 8−10.5 eV Th

176

575. V. A. Bernshtam, Yu. Ralchenko, Y. MaronElectron impact ionization of helium isoelectronic systemsEur. Phys. J. D 51, 319 (2009)

e + Ar16+ 1e2−1e5 eV E/Te + O6+ 1e2−1e5 eV E/Te + N5+ 1e2−1e5 eV E/Te + B3+ 1e2−1e5 eV E/T

576. S. P. Purohit, K. C. MathurResonant laser assisted elastic scattering of electrons by lithium and sodium atomsEur. Phys. J. D 53, 173 (2009)

e + Na 50?150 eV The + Li 50?150 eV Th

577. M. Vos, M. R. WentElastic electron scattering from hydrogen molecules at high-momentum transferJ. Phys. B 42, 065204 (2009)

e + Xe 750−7000 eV The + H 750−7000 eV Th

578. R. P. McEachran, A. D. StaufferAn optical potential method for elastic electron and positron scattering from argonJ. Phys. B 42, 075202 (2009)

e + Ar 5−300 eV E/T

579. A. G. Harvey, J. TennysonElectron re-scattering from aligned linear molecules using the R-matrix methodJ. Phys. B 42, 095101 (2009)

e + CO2 0−25 eV The + H2 0−25 eV Th

580. Fan-Chang Meng, Li Zhou, Min Huang, Chong-Yang Chen, Yan-Sen Wang, Ya-Ming ZouDielectronic recombination rate coefficients for the CoI isoelectronic sequenceJ. Phys. B 42, 105203 (2009)

e + U65+ 0.5Et − 15Et The + At58+ 0.5Et − 15Et The + Au52+ 0.5Et − 15Et The + W47+ 0.5Et − 15Et The + Dy39+ 0.5Et − 15Et The + Pr32+ 0.5Et − 15Et The + Xe27+ 0.5Et − 15Et The + Ag20+ 0.5Et − 15Et The + Mo15+ 0.5Et − 15Et The + Kr9+ 0.5Et − 15Et Th

581. Toru Morishita, Misaki Okunishi, Kozo Shimada, Georg Pruemper, Zhangjin Chen, ShinichiWatanabe, Kiyoshi Ueda, C. D. LinRetrieval of experimental differential electron-ion elastic scattering cross sectionsfrom high-energy ATI spectra of rare gas atoms by infrared lasersJ. Phys. B 42, 105205 (2009)

e + Xe E/Te + Kr E/Te + Ar E/T

177

582. L’ Malinovsky, P. Lukac, V. Foltin, I. Morva, M. MorvovaOn the electron temperature dependence of the dissociative recombination of Ne-2(+)ions with electronsJ. Phys. B 42, 105701 (2009)

e + Ne2+ 300−10000K Th

e + Ne2+ 300−10000K Th

583. Z. Rouabah, N. Bouarissa, C. ChampionImproved expression for calculating electron transport cross sectionsPhys. Lett. A 373, 282 (2009)

e + Au 50−2000 eV The + Nd 50−2000 eV The + Ag 50−2000 eV The + Cu 50−2000 eV The + Al 50−2000 eV The + H 50−2000 eV Th

584. Y. Khajuria, S. Sunil Kumar, P. C. DeshmukhTriple differential cross section in (e, 2e) collisions for atomic potassiumPhys. Lett. A 373, 4442 (2009)

e + K 6−60 eV Th

585. K. G. Bhushan, K. C. Rao, S. C. Gadkari, J. V. Yakhmi, S. K. GuptaElastic differential cross sections for electron scattering from SF6 and CS2Phys. Rev. A 79, 012702 (2009)

e + CS2 30 eV to 500 eV Expe + SF6 30 eV to 500 eV Expe + CS2 30 eV to 500 eV Expe + SF6 30 eV to 500 eV Exp

586. M. A. Stevenson, L. R. Hargreaves, B. Lohmann, I. Bray, D. V. Fursa, K. Bartschat, A. KheifetsFully differential cross-section measurements for electron-impact ionization of neonand xenonPhys. Rev. A 79, 012709 (2009)

e + Xe 150 eV E/Te + Ne 150 eV E/T

587. H. Takagi, S. Hara, H. SatoOff-the-energy-shell effect in the dissociative recombination of HD+Phys. Rev. A 79, 012715 (2009)

e + HD+ 0.0001−1 eV The + HD+ 0.0001−1 eV Th

588. Daniel J. Haxton, Chris H. GreeneAb initio frame-transformation calculations of direct and indirect dissociativerecombination rates of HeH++e(-)Phys. Rev. A 79, 022701 (2009)

e + HeD 0.0001−1 eV The + HeH 0.0001−1 eV The + HeD 0.0001−1 eV The + HeH 0.0001−1 eV Th

589. A. Cerkic, E. Hasovic, D. B. Milosevic, W. BeckerHigh-order above-threshold ionization beyond the first-order Born approximationPhys. Rev. A 79, 033413 (2009)

178

e + Ar 39, 23, and 16.5 eV Th

590. J. R. Francis-Staite, T. M. Maddern, M. J. Brunger, S. J. Buckman, C. Winstead, V. McKoy, M.A. Bolorizadeh, H. ChoDifferential and integral cross sections for elastic electron scattering from CF2Phys. Rev. A 79, 052705 (2009)

e + CF2 2?20 eV, Exp

591. H. Kato, M. C. Garcia, T. Asahina, M. Hoshino, C. Makochekanwa, H. Tanaka, F. Blanco, G.GarciaAbsolute elastic differential cross sections for electron scattering by C6H5CH3 andC6H5CF3 at 1.5-200 eV: A comparative experimental and theoretical study with C6H6Phys. Rev. A 79, 062703 (2009)

e + C6H5CH3 1.5−200 eV Expe + C6H6 1.5−200 eV Exp

592. Z. Felfli, A. Z. Msezane, D. SokolovskiDifferential cross sections for low-energy electron elastic scattering by lanthanideatoms: La, Ce, Pr, Nd, Eu, Gd, Dy, and TmPhys. Rev. A 79, 062709 (2009)

e + Tm 0−1 eV The + Dy 0−1 eV The + Gd 0−1 eV The + Eu 0−1 eV The + Nd 0−1 eV The + Pr 0−1 eV The + Ce 0−1 eV The + La 0−1 eV Th

593. J. B. Roos, M. Larsson, A. Larson, A. E. OrelDissociative recombination of BeH+Phys. Rev. A 80, 012501 (2009)

e + BeH+ 0−5 eV The + BeH+ 0−5 eV Th

594. O. May, J. Fedor, M. AllanIsotope effect in dissociative electron attachment to acetylenePhys. Rev. A 80, 012706 (2009)

e + C2D2 0−10 eV Expe + C2H2 0−10 eV Expe + C2D2 0−10 eV Expe + C2H2 0−10 eV Exp

595. S. T. Chourou, A. E. OrelDissociative electron attachment to HCN and HNCPhys. Rev. A 80, 032709 (2009)

e + HNC 0−7 eV The + HCN 0−7 eV The + HNC 0−7 eV The + HCN 0−7 eV Th

596. S. T. Chourou, A. E. OrelImproved calculation on the isotope effect in dissociative electron attachment toacetylenePhys. Rev. A 80, 034701 (2009)

179

e + C2D2 0−7 eV The + C2H2 0−7 eV The + C2D2 0−7 eV The + C2H2 0−7 eV Th

597. X. M. Tong, N. Nakamura, S. Ohtani, T. Watanabe, N. ToshimaGreen’s function for multielectron ions and its application to radiative recombinationinvolving dielectronic recombinationsPhys. Rev. A 80, 042502 (2009)

e + Hg76+ 49.0−50.2 eV Th

598. Nicolas Douguet, Viatcheslav Kokoouline, Chris H. GreeneTheory of dissociative recombination of a linear triatomic ion with permanent electricdipole moment: Study of HCO+Phys. Rev. A 80, 062712 (2009)

e + HCO+ 0.001−1 eV E/Te + HCO+ 0.001−1 eV E/T

599. Ch. Jungen, S. T. PrattJahn-Teller Interactions in the Dissociative Recombination of H-3(+)Phys. Rev. Lett. 102, 023201 (2009)

e + D3+ 0.001−1 eV E/T

e + D2H 0.001−1 eV E/Te + H2D

+ 0.001−1 eV E/Te + H3

+ 0.001−1 eV E/Te + D3

+ 0.001−1 eV E/Te + D2H 0.001−1 eV E/Te + H2D

+ 0.001−1 eV E/Te + H3

+ 0.001−1 eV E/T

600. G. Purohit, Vinod Patidar, K. K. Sud(e, 2e) triple differential cross sections of Ca atoms at low energiesPhys. Scr. 80, 065301 (2009)

e + Ca 10.11− 24.6 eV E/T

601. J. L. McLain, N. G. AdamsFlowing afterglow studies of temperature dependencies for electron dissociativerecombination of HCNH+, CH3CNH+ and CH3CH2CNH+ and their symmetricalproton-bound dimersPlanet. Space Sci. 57, 1642 (2009)

e + HCNH+ 100−700 K E/Te + HCNH+ 100−700 K E/T

602. O. Mikus, P. Lukac, I. Morva, Z. Zabudla, J. Trnovec, M. MorvovaElectron and gas temperature dependences of the dissociative recombination coefficientof molecular ions Ne-2(+) with electronsPlasma Sources Sci. Technol. 18, 025031 (2009)

e + Ne2+ 200−700 K E/T

e + Ne2+ 200−700 K E/T

603. E. Landi, A. K. BhatiaAtomic data and spectral line intensities for Ca XVIIAt. Data Nucl. Data Tables 95, 155 (2009)

e + Ca16+ 15−225 Ry Th

180

604. Li-Guang Jiao, Ya-Jun Zhou, Rong-Mei YuLow Energy Scattering of Electrons by SodiumChin. Phys. Lett. 26, 023401 (2009)

e + Na 0.5− 6.5 eV Th

605. F. Sebastianelli, F. A. Gianturco, T. Stoecklin, I. BaccarelliScattering of electrons by gaseous CS((1)Sigma): The role of short-range forces on thevery-low energy (2)Pi resonanceChem. Phys. Lett. 476, 182 (2009)

e + CS 1−100 eV The + CS 1−100 eV Th

606. D. H. Shi, J. F. Sun, Y. F. Liu, Z. L. Zhu, H. MaTotal cross sections of electron scattering by several sulfur-containing molecules OCS,SO2, SF4, SF6, SF5CF3, SO2Cl2 and SO2ClF at 30-5000 eVEur. Phys. J. D 54, 43 (2009)

e + SF6 30−5000 eV The + SF4 30−5000 eV The + SO2 30−5000 eV Th

607. Z. Idziaszek, G. KarwaszModified effective-range theory for low energy e-N-2 scatteringEur. Phys. J. D 57, 347 (2009)

e + N2 0.1?1.0 eV E/Te + N2 0.1?1.0 eV E/T

608. T. H. Hoffmann, M. Allan, K. Franz, M-W Ruf, H. Hotop, G. Sauter, W. MeyerResonance structure in electron-N-2 scattering around 11.5 eV: high-resolutionmeasurements, ab initio calculations and line shape analysesJ. Phys. B 42, 215202 (2009)

e + N2− 10 eV E/T

e + N2 10 eV E/Te + N2

− 10 eV E/Te + N2 10 eV E/Te + N2

− 10 eV E/Te + N2 10 eV E/T

609. P. Wickramarachchi, P. Palihawadana, G. Villela, W. M. AriyasingheElectron scattering from alkenes in the energy range 200-4500 eVNucl. Instrum. Methods Phys. Res. B 267, 3391 (2009)

e + C4H6 200−4500 eV Expe + C4H8 200−4500 eV Expe + C3H6 200−4500 eV Expe + C2H4 200−4500 eV Exp

610. T. C. Freitas, M. H. F. BettegaScattering of low-energy electrons by C2H4OPhys. Rev. A 79, 042714 (2009)

e + C2H4O 0.7−20 eV The + C2H4O 0.7−20 eV Th

611. Douglas H. Sampson, Hong Lin Zhang, Christopher J. FontesA fully relativistic approach for calculating atomic data for highly charged ionsPhys. Rep. 477, 111 (2009)

181

e + U82+ 150 eV, 30000 eV Th

612. Gorur Govinda RajuScaling of Resonance in Total Scattering Cross Section in GasesIEEE Transactions on Dielectrics and Electrical Insulation 16, 1199 (2009)

e + SiH4 1e−3 − 1e3 eV Expe + CH4 1e−3 − 1e3 eV Expe + CF4 1e−3 − 1e3 eV Expe + N2O 1e−3 − 1e3 eV Expe + SF6 1e−3 − 1e3 eV Expe + Xe 1e−3 − 1e3 eV Expe + Kr 1e−3 − 1e3 eV Expe + Ar 1e−3 − 1e3 eV Exp

613. Shi-Yan Sun, Xiang-Fu Jia, Xiang-Yang Miao, Jun-Fang Zhang, Yi Xie, Xiong-Wei Li, Wen-QiangShiThe effect of dynamical screening on helium (e, 2e) fully differential cross-sectionsChin. Phys. B 18, 2744 (2009)

e + He 102 eV E/T

614. Jeffrey F. Friedman, Thomas M. Miller, Linda C. Schaffer, A. A. Viggiano, Ilya I. FabrikantElectron attachment to Cl-2 from 300 to 1100 K: Experiment and theoryPhys. Rev. A 79, 032707 (2009)

e + Cl2 300−1100 K Expe + Cl2 300−1100 K Exp

615. Gordon A. Gallup, Paul D. Burrow, Ilya I. FabrikantElectron-induced bond breaking at low energies in HCOOH and glycine: The role ofvery short-lived sigma(*) anion statesPhys. Rev. A 79, 042701 (2009)

e + HCOOH 0.5−2.5 eV The + HCOOH 0.5−2.5 eV Th

616. Thomas M. Miller, Jeffrey F. Friedman, John S. Williamson, Linda C. Schaffer, A. A. ViggianoA new instrument for thermal electron attachment at high temperature: NF3 andCH3Cl attachment rate constants up to 1100 KRev. Sci. Instrum. 80, 034104 (2009)

e + CH3Cl 300−1200K Expe + NF3 300−1200K Expe + CH3Cl 300−1200K Expe + NF3 300−1200K Exp

617. S. S. Tayal, O. ZatsarinnyElectron excitation collision strengths for transitions in K IIAstron. Astrophys. 510, A79 (2010)

e + K+ 1000−1000000K Th

618. C. M. Cassidy, C. A. Ramsbottom, M. P. Scott, al. etElectron-impact excitation of Ni II Collision strengths and effective collision strengthsfor low-lying fine-structure forbidden transitionsAstron. Astrophys. 513, A55 (2010)

e + Ni+ 10−100000K Th

182

619. I. R. Wasson, C. A. Ramsbottom, P. H. NorringtonElectron-impact excitation of Cr II A theoretical calculation of collision and effectivecollision strengths for forbidden transitionsAstron. Astrophys. 524, A35 (2010)

e + Cr+ 1000−100000K Th

620. K. Hamada, K. M. Aggarwal, K. Akita, al. etEffective collision strengths for optically allowed transitions among degenerate levelsof hydrogenic ions with 2 ¡= Z ¡= 30At. Data Nucl. Data Tables 96, 481 (2010)

e + Zn29+ 1E−6/Z2-10/Z2K The + Cu28+ 1E−6/Z2-10/Z2K The + Ni 1E−6/Z2-10/Z2K The + Co26+ 1E−6/Z2-10/Z2K The + Fe25+ 1E−6/Z2-10/Z2K The + Mn24+ 1E−6/Z2-10/Z2K The + Cr23+ 1E−6/Z2-10/Z2K The + V22+ 1E−6/Z2-10/Z2K The + Ti21+ 1E−6/Z2-10/Z2K The + Sc20+ 1E−6/Z2-10/Z2K The + Ca19+ 1E−6/Z2-10/Z2K The + K18+ 1E−6/Z2-10/Z2K The + Ar17+ 1E−6/Z2-10/Z2K The + Cl16+ 1E−6/Z2-10/Z2K The + S15+ 1E−6/Z2-10/Z2K The + P14+ 1E−6/Z2-10/Z2K The + Si13+ 1E−6/Z2-10/Z2K The + Al12+ 1E−6/Z2-10/Z2K The + Mg11+ 1E−6/Z2-10/Z2K The + Na10+ 1E−6/Z2-10/Z2K The + Ne9+ 1E−6/Z2-10/Z2K The + F8+ 1E−6/Z2-10/Z2K The + O7+ 1E−6/Z2-10/Z2K The + N6+ 1E−6/Z2-10/Z2K The + C5+ 1E−6/Z2-10/Z2K The + B4+ 1E−6/Z2-10/Z2K The + Be 1E−6/Z2-10/Z2K The + Li2+ 1E−6/Z2-10/Z2K The + He+ 1E−6/Z2-10/Z2K Th

621. M. Hahn, D. Bernhardt, M. Lestinsky, al. etSTORAGE RING MEASUREMENT OF ELECTRON IMPACT IONIZATION FORMg7+ FORMING Mg8+Astrophys. J. 712, 1166 (2010)

e + Mg7+ 200−1800eV Exp

622. S. S. Tayal, O ZatsarinnyBREIT-PAULI TRANSITION PROBABILITIES AND ELECTRON EXCITATIONCOLLISION STRENGTHS FOR SINGLY IONIZED SULFURAstrophys. J., Suppl. Ser. 188, 32 (2010)

e + S+ 5000−100000K Th

623. Ning-Xuan Yang, Chen-Zhong Dong, Jun Jiang, al. etElectron impact excitation rate coefficients of N II ionChin. Phys. B 19, 093101 (2010)

e + N+ 2−12eV Th

183

624. Ning-Xuan Yang, Jun Jiang, Chen-Zhong DongDifferential and Integral Cross Sections for Electron Impact Excitation of LithiumChin. Phys. Lett. 27, 113401 (2010)

e + Li 0−25eV Th

625. Ireneusz Linert, Izabela Lachowicz, Tomasz J. Wasowicz, al. etFragmentation of isoxazole molecules by electron impact in the energy range 10-85 eVChem. Phys. Lett. 498, 27 (2010)

e + CH 10−90eV Exp

626. R. Riahi, Ph. Teulet, Z. BenLakhdar, al. etCross section and rate coefficient calculations for electron impact excitation,ionisation and dissociation of the X (1)Sigma(+)(g), c (3)Pi(u), a (3)Sigma(+)(g), e(3)Sigma(+)(u) and B ’ (1)Sigma(+)(u) states of H-2Eur. Phys. J. D 56, 61 (2010)

e + H2 10−100eV The + H2 10−100eV Th

627. R. Riahi, Ph. Teulet, N. Jaidane, al. etCross section and rate coefficient calculations for electron impact excitation of the a(3)Pi, a ’ (3)Sigma(+), d (3)Delta, e (3)Sigma(-), I (1)Sigma(+) and D (1)Delta statesof COEur. Phys. J. D 56, 67 (2010)

e + CO 0−50eV The + CO 0−50eV Th

628. H. Cherkani-Hassani, S. Cherkani-Hassani, D. S. Belic, al. etI. Electron-impact ionization and dissociation of C2H2+ and C2D2+Eur. Phys. J. D 58, 75 (2010)

e + C2D2+ 6.5−2498.5eV Exp

e + C2H2+ 6.5−2498.5eV Exp

e + C2D2+ 6.5−2498.5eV Exp

e + C2H2+ 6.5−2498.5eV Exp

629. H. Cherkani-Hassani, D. S. Belic, J. J. Jureta, al etII. Electron-impact dissociative excitation of C2H2+ and C2D2+Eur. Phys. J. D 58, 85 (2010)

e + C2D2+ 6.5−2498.5eV Exp

e + C2H2+ 6.5−2498.5eV Exp

630. H. Cherkani-Hassani, D. S. Belic, J. J. Jureta, al. etIII. Electron-impact dissociative ionization of C2H2+ and C2D2+Eur. Phys. J. D 58, 95 (2010)

e + C2D2+ 6.5−2498.5eV Exp

e + C2H2+ 6.5−2498.5eV Exp

631. B. W. Li, C. Z. Dong, J. Jiang, al. etElectron-impact excitation of Ti21+ in Debye plasmasEur. Phys. J. D 59, 201 (2010)

e + Ti21+ 5400−24000eV Th

184

632. M. Vinodkumar, K. Korot, P. C. VinodkumarComplex scattering potential - ionization contribution (CSP-ic) method for calculatingtotal ionization cross sections on electron impactEur. Phys. J. D 59, 379 (2010)

e + NH3 15−2000eV The + NO 15−2000eV The + F 15−2000eV The + O 15−2000eV The + N 15−2000eV The + C 15−2000eV Th

633. J. Lecointre, H. Cherkani-Hassani, S. Cherkani-Hassani, al. etElectron-impact ionization and dissociation of C2D+Eur. Phys. J. D 60, 331 (2010)

e + C2D2+ 2.1− 2495.1eV Exp

e + C2H2+ 2.1− 2495.1eV Exp

e + C2D2+ 2.1− 2495.1eV Exp

e + C2H2+ 2.1− 2495.1eV Exp

634. Minaxi Vinodkumar, Rucha Dave, Harshad Bhutadia, al. etElectron impact total ionization cross sections for halogens and their hydridesInt. J. Mass Spectrom. 292, 7 (2010)

e + HI 15 − 2000eV The + HBr 15 − 2000eV The + HCl 15 − 2000eV The + HF 15 − 2000eV The + I 15 − 2000eV The + Br 15 − 2000eV The + Cl 15 − 2000eV The + F 15 − 2000eV Th

635. Minaxi Vinodkumar, Kirti Korot, Harshad BhutadiaCalculations of total and ionization cross-sections on electron impact for alkali metals(Li, Na, K) from threshold to 2 keVInt. J. Mass Spectrom. 294, 54 (2010)

e + K 0−2000eV The + Na 0−2000eV The + Li 0−2000eV The + K 0−2000eV The + Na 0−2000eV The + Li 0−2000eV Th

636. H. Kato, T. Asahina, H. Masui, al. etSubstitution effects in elastic electron collisions with CH3X (X=F, Cl, Br, I) moleculesJ. Chem. Phys. 132, 074309 (2010)

e + CH3Br 50,100,200eVe + CH3Cl 50,100,200eVe + CH3I 50,100,200eVe + CH3F 50,100,200eVe + CH3Br 50,100,200eVe + CH3Cl 50,100,200eVe + CH3I 50,100,200eVe + CH3F 50,100,200eV

185

637. You-Yan Wang, Jian-Min Sun, Lin-Fan ZhuCross sections for the valence shell excitations of nitrous oxide studied by fast electronimpactJ. Chem. Phys. 132, 124301 (2010)

e + N2O 6−5000eV Exp

638. Minaxi Vinodkumar, Chetan Limbachiya, Harshad BhutadiaElectron impact calculations of total ionization cross sections for environmentallysensitive diatomic and triatomic molecules from threshold to 5 keVJ. Phys. B 43, 015203 (2010)

e + S2 15−5000eV The + OCS 15−5000eV The + CS2 15−5000eV The + CS 15−5000eV The + CO2 15−5000eV The + CO 15−5000eV Th

639. M. S. Pindzola, C. P. Ballance, J. A. Ludlow, al. etElectron-impact ionization of Xe24+J. Phys. B 43, 025201 (2010)

e + Xe24+ 750−1250eV Th

640. Y. C. Wang, Y. Zhou, Y. Cheng, al. etCoupled channels optical method of electron impact on excited helium 2(1)SJ. Phys. B 43, 045201 (2010)

e + He 0−200eV Th

641. M. S. Pindzola, C. P. Ballance, J. A. Ludlow, al. etElectron-impact ionization of C2J. Phys. B 43, 065201 (2010)

e + C2 0− 50eV Th

642. H. Kato, M. Hoshino, Y. Nagai, al. etResonant vibrational excitation of CH3X (X = F, Cl, Br and I) by low-energy electronimpactJ. Phys. B 43, 065205 (2010)

e + CH3I 6.5eV, 5.9eV, 5.5eV, 4.7eV Expe + CH3Br 6.5eV, 5.9eV, 5.5eV, 4.7eV Expe + CH3Cl 6.5eV, 5.9eV, 5.5eV, 4.7eV Expe + CH3F 6.5eV, 5.9eV, 5.5eV, 4.7eV Exp

643. Juan A. Santana, Yasuyuki IshikawaRelativistic R-matrix close-coupling method based on the effective many-bodyHamiltonian: electron-impact excitation of electric dipole-allowed and spin-forbiddentransitions of the S4+ ionJ. Phys. B 43, 074030 (2010)

e + S4+ 10−16eV Th

644. Oleg Zatsarinny, Klaus BartschatBenchmark calculations for near-threshold electron-impact excitation of krypton andxenon atomsJ. Phys. B 43, 074031 (2010)

186

e + Xe 0−12.5eV The + Kr 0−12.5eV Th

645. J. Lecointre, J. J. Jureta, P. DefranceElectron-impact dissociation and ionization of NH+: formation of N+ and N2+J. Phys. B 43, 105202 (2010)

e + NH+ 2.1−2495.1eV Expe + NH+ 2.1−2495.1eV Exp

646. M. S. Pindzola, C. P. Ballance, F. Robicheaux, al. etElectron-impact double ionization of berylliumJ. Phys. B 43, 105204 (2010)

e + Be 0−500eV Th

647. A. K. F. Haque, M. R. Talukder, M. Shahjahan, al. etAn extended empirical formula for inner-shell ionization of atomsJ. Phys. B 43, 115201 (2010)

e + Pu 10−1E9eV The + Np 10−1E9eV The + U 10−1E9eV The + Pa 10−1E9eV The + Th 10−1E9eV The + Ac 10−1E9eV The + Ra 10−1E9eV The + Fr 10−1E9eV The + Rn 10−1E9eV The + At 10−1E9eV The + Po 10−1E9eV The + Bi 10−1E9eV The + Pb 10−1E9eV The + Tl 10−1E9eV The + Hg 10−1E9eV The + Au 10−1E9eV The + Pt 10−1E9eV The + Ir 10−1E9eV The + Os 10−1E9eV The + Re 10−1E9eV The + W 10−1E9eV The + Ta 10−1E9eV The + Hf 10−1E9eV The + Lu 10−1E9eV The + Yb 10−1E9eV The + Tm 10−1E9eV The + Er 10−1E9eV The + Ho 10−1E9eV The + Dy 10−1E9eV The + Tb 10−1E9eV The + Gd 10−1E9eV The + Eu 10−1E9eV The + Sm 10−1E9eV The + Pm 10−1E9eV The + Nd 10−1E9eV The + Pr 10−1E9eV The + Ce 10−1E9eV The + La 10−1E9eV The + Ba 10−1E9eV The + Cs 10−1E9eV Th

187

e + Xe 10−1E9eV The + I 10−1E9eV The + Te 10−1E9eV The + Sb 10−1E9eV The + Sn 10−1E9eV The + In 10−1E9eV The + Cd 10−1E9eV The + Ag 10−1E9eV The + Pd 10−1E9eV The + Rh 10−1E9eV The + Ru 10−1E9eV The + Tc 10−1E9eV The + Mo 10−1E9eV The + Nb 10−1E9eV The + Zr 10−1E9eV The + Y 10−1E9eV The + Sr 10−1E9eV The + Rb 10−1E9eV The + Kr 10−1E9eV The + Br 10−1E9eV The + Se 10−1E9eV The + As 10−1E9eV The + Ge 10−1E9eV The + Ga 10−1E9eV The + Zn 10−1E9eV The + Cu 10−1E9eV The + Ni 10−1E9eV The + Co 10−1E9eV The + Fe 10−1E9eV The + Mn 10−1E9eV The + Cr 10−1E9eV The + V 10−1E9eV The + Ti 10−1E9eV The + Sc 10−1E9eV The + Ca 10−1E9eV The + K 10−1E9eV The + Ar 10−1E9eV The + Cl 10−1E9eV The + S 10−1E9eV The + P 10−1E9eV The + Si 10−1E9eV The + Al 10−1E9eV The + Mg 10−1E9eV The + Na 10−1E9eV The + Ne 10−1E9eV The + F 10−1E9eV The + O 10−1E9eV The + N 10−1E9eV The + C 10−1E9eV The + B 10−1E9eV The + Be 10−1E9eV The + Li 10−1E9eV The + He 10−1E9eV The + H 10−1E9eV Th

648. Y. Wu, Z. An, Y. M. Duan, al. etMeasurements of L-shell x-ray production cross-sections of Gd and W by low energyelectron impactJ. Phys. B 43, 135206 (2010)

188

e + W 9keV−40keV Expe + Gd 9keV−40keV Exp

649. K. N. Joshipura, Harshit N. Kothari, Foram A. Shelat, al. etElectron scattering with metastable H-2*(c(3)Pi(u)) molecules: ionization and othertotal cross sectionsJ. Phys. B 43, 135207 (2010)

e + H2 The + H2 Th

650. Klaus Bartschat, Anatoli S. Kheifets, Dmitry V. Fursa, al. etBenchmark calculations for electron impact ionization and ionization-excitation ofmagnesiumJ. Phys. B 43, 165205 (2010)

e + Mg The + Mg Th

651. K. Wang, C. Y. Chen, M. Huang, al. etElectron impact excitation for P-like Ni XIVJ. Phys. B 43, 175202 (2010)

e + Ni13+ 0−100eV Th

652. E. V. Ovcharenko, A. I. Imre, A. N. Gomonai, al. etEmission cross-sections of the In2+ ion VUV laser transitions at electron-In+ ioncollisionsJ. Phys. B 43, 175206 (2010)

e + In+ 33−120eV Exp

653. D. S. Belic, J. Lecointre, P. DefranceElectron impact multiple ionization of argon ionsJ. Phys. B 43, 185203 (2010)

e + Ar+ 25−2495eV Exp

654. J. D. Hein, C. Ududec, D. K. Sasaki, al. etIntegral cross sections for electron-impact ionization-excitation of laser-excited bariumJ. Phys. B 43, 185206 (2010)

e + Be 10−50eV Expe + Be 10−50eV Exp

655. L. R. Hargreaves, M. A. Stevenson, B. LohmannAbsolute triple-differential cross sections for intermediate energy electron impactionization of neon and argonJ. Phys. B 43, 205202 (2010)

e + Ar 113.5 eV − 600 eV E/Te + Ne 113.5 eV − 600 eV E/T

656. J. -S. Yoon, M. -Y. Song, H. Kato, al. etElastic Cross Sections for Electron Collisions with Molecules Relevant to PlasmaProcessingJ. Phys. Chem. Ref. Data 39, 033106 (2010)

189

e + GeH4 20eV− 100eVe + Si2H6 20eV− 100eVe + SiH4 20eV− 100eVe + SF6 20eV− 100eVe + NF3 20eV− 100eVe + CF3I 20eV− 100eVe + F 20eV− 100eVe + CH3 20eV− 100eVe + CH2F2 20eV− 100eVe + CHF3 20eV− 100eVe + C6F6 20eV− 100eVe + C4F8 20eV− 100eVe + C3F8 20eV− 100eVe + C3F6 20eV− 100eVe + F6 20eV− 100eVe + C2 20eV− 100eVe + C2F4 20eV− 100eVe + CF4 20eV− 100eVe + CF2 20eV− 100eV

657. Hemal N. Varambhia, Alexandre Faure, K. Graupner, al. etElectron-impact rotational excitation of the carbon monosulphide (CS) moleculeMon. Not. R. Astron. Soc. 403, 1409 (2010)

e + C 5−5000K The + C 5−5000K Th

658. Viatcheslav Kokoouline, Alexandre Faure, Jonathan Tennyson, al. etCalculation of rate constants for vibrational and rotational excitation of the H+(3)ion by electron impactMon. Not. R. Astron. Soc. 405, 1195 (2010)

e + H3+ 1−7000K Th

659. Philip L. Bartlett, Andris T. StelbovicsIonization of atoms by electron impactNucl. Instrum. Methods Phys. Res. A 619, 1 (2010)

e + Kr 10−3000eV The + Fe 10−3000eV The + Ne 10−3000eV The + H 10−3000eV Th

660. Y. Wu, Z. An, Y. M. Duan, al. etMeasurements of L-alpha, L-beta X-ray production cross sections of Bi by 17-40 keVelectron impactNucl. Instrum. Methods Phys. Res. B 268, 2473 (2010)

e + Bi 7−30keV Exp

661. Y. Wu, Z. An, Y. M. Duan, al. etMeasurements of K-shell ionization cross-sections of S, Ca and Zn by 7-30 keV electronimpactNucl. Instrum. Methods Phys. Res. B 268, 2820 (2010)

e + Zn 7−30keV Expe + Ca 7−30keV Expe + S 7−30keV Exp

190

662. F. Blanco, J. Rosado, A. Illana, al. etComparison of two screening corrections to the additivity rule for the calculation ofelectron scattering from polyatomic moleculesPhys. Lett. A 374, 4420 (2010)

e + C6H6 1−1000eV The + SF6 1−1000eV The + CF4 1−1000eV The + CO2 1−1000eV Th

663. Xiang Gao, Xiao-Ying Han, Lan Voky, al. etPrecision calculation of low-energy electron-impact excitation cross sections of sodiumPhys. Rev. A 81, 022703 (2010)

e + Na 0−5.5eV Th

664. Philip L. Bartlett, Andris T. StelbovicsElectron-helium S-wave model benchmark calculations. I. Single ionization and singleexcitationPhys. Rev. A 81, 022715 (2010)

e + He 10−500eV The + He 10−500eV Th

665. Philip L. Bartlett, Andris T. StelbovicsElectron-helium S-wave model benchmark calculations. II. Double ionization, singleionization with excitation, and double excitationPhys. Rev. A 81, 022716 (2010)

e + He 20−500eV The + He 20−500eV Th

666. Takeshi KaiSingle-differential and integral cross sections for electron-impact ionization for thedamage of carbon clusters irradiated with x-ray free-electron lasersPhys. Rev. A 81, 023201 (2010)

e + C+ 5−20000eV The + C 5−20000eV Th

667. Robin ShakeshaftEnergy partitioning in S-1-wave electron-impact ionization of atomic hydrogenPhys. Rev. A 81, 032705 (2010)

e + H 10−80eV Th

668. Song Bin Zhang, Jian Guo Wang, R. K. JanevElectron-hydrogen-atom elastic and inelastic scattering with screened Coulombinteraction around the n=2 excitation thresholdPhys. Rev. A 81, 032707 (2010)

e + H 0−12eV Th

669. M. AllanElectron collisions with CO: Elastic and vibrational excitation cross sectionsPhys. Rev. A 81, 042706 (2010)

e + CO 0−5eV Expe + CO 0−5eV Exp

191

670. Hsiao-Ling Sun, Jyh-Ching Chang, Ju-Tang Hsiao, al. etElectron-impact ionization of hydrogenlike ions in QED theoryPhys. Rev. A 81, 042711 (2010)

e + Mo41+ 1−15u(scaled unit) Expe + Dy65+ 1−15u(scaled unit) Expe + Fe25+ 1−15u(scaled unit) Expe + Ar17+ 1−15u(scaled unit) Expe + Ne9+ 1−15u(scaled unit) Exp

671. L. Jiao, Y. Zhou, Y. WangNegative-ion resonances in total cross sections for slow electron-sodium collisionsPhys. Rev. A 81, 042713 (2010)

e + Na 0−6eV Th

672. I. Bray, D. V. Fursa, A. S. Kadyrov, al. etSingle ionization of helium by electron impactPhys. Rev. A 81, 062704 (2010)

e + He Th

673. O. Zatsarinny, K. Bartschat, V. Suvorov, al. etElectron-impact excitation of the (3d(10)4s)S-2(1/2) -¿ ( 3d(9)4s(2))D-2(5/2,3/2)transitions in copper atomsPhys. Rev. A 81, 062705 (2010)

e + Cu 1−5eV

674. G. B. Poparie, D. S. BelieResonant vibrational excitation of H-2 by electron impact: Full-range differential crosssectionsPhys. Rev. A 82, 012706 (2010)

e + H2 1−5eV Exp

675. Malkhaz R. Gochitashvili, Roman Ya. Kezerashvili, Ramaz A. LomsadzeExcitation of Meinel and the first negative band system at the collision of electronsand protons with the nitrogen moleculePhys. Rev. A 82, 022702 (2010)

e + N2 400−1500eV Exp

676. D. A. Konovalov, I. BrayCalculation of electron-impact ionization using the J-matrix methodPhys. Rev. A 82, 022708 (2010)

e + H 0−150eV Th

677. Czeslaw Szmytkowski, Pawel Mozejko, Elzbieta Ptasinska-Denga, al. etCross sections for electron scattering from furan molecules: Measurements andcalculationsPhys. Rev. A 82, 032701 (2010)

e + C4H4O 0.6−400eV Expe + C4H4O 0.6−400eV Exp

678. Jasmeet Singh Rajvanshi, K. L. BalujaElectron-impact study of the SO radical using the R-matrix methodPhys. Rev. A 82, 032706 (2010)

192

e + SO 1−10eV The + SO 1−10eV Th

679. C. Champion, R. D. RivarolaOrientation and alignment effects in electron-induced ionization of a single orientedwater moleculePhys. Rev. A 82, 042704 (2010)

e + H2O 10−10000eV Th

680. Wei-Qing Xu, Jian-Min Sun, You-Yan Wang, al. etGeneralized oscillator strengths and integral cross sections for the valence-shellexcitations of oxygen studied by fast electron impactPhys. Rev. A 82, 042716 (2010)

e + O2 5.9−5000eV Exp

681. M. Fogle, E. M. Bahati, M. E. Bannister, al. etElectron-impact dissociation of XH2+ (X = B, C, N, O, F): Absolute cross sectionsfor production of XH+ and X+ fragment ionsPhys. Rev. A 82, 042720 (2010)

e + FD2+ 2−100eV Exp

e + OD2+ 2−100eV Exp

e + ND2+ 2−100eV Exp

e + BD2+ 2−100eV Exp

e + CH2+ 2−100eV Exp

e + FD2+ 2−100eV Exp

e + OD2+ 2−100eV Exp

e + ND2+ 2−100eV Exp

e + BD2+ 2−100eV Exp

e + CH2+ 2−100eV Exp

682. Teck-Ghee Lee, S. D. Loch, C. P. Ballance, al. etElectron-impact-ionization cross sections for excited states of Bq+ (q=0-2) and aninvestigation into n scaling of ionization cross sectionsPhys. Rev. A 82, 042721 (2010)

e + B2+ 0−40eV The + B+ 0−40eV The + B 0−40eV Th

683. Pragya Bhatt, Raj Singh, Namita Yadav, al. etPartial-ionization cross sections of a CO2 molecule due to impact of 10-26-keV electronsPhys. Rev. A 82, 044702 (2010)

e + CO2 10−26keV Expe + CO2 10−26keV Exp

684. Mark C. Zammit, Dmitry V. Fursa, Igor BrayConvergent-close-coupling calculations for excitation and ionization processes ofelectron-hydrogen collisions in Debye plasmasPhys. Rev. A 82, 052705 (2010)

e + H 0−250eV The + H 0−250eV Th

685. Jasmeet Singh Rajvanshi, K. L. BalujaElectron-impact study of the NH radical using the R-matrix methodPhys. Rev. A 82, 062710 (2010)

193

e + NH 0−10eV The + NH 0−10eV Th

686. Song Bin Zhang, Jian Guo Wang, R. K. Janev, al etElectron collisions with the BH2 radical using the R-matrix methodPhys. Rev. A 82, 062711 (2010)

e + BH2 0−10eV The + BH2 0−10eV Th

687. S. H. M. Deng, C. R. Vane, M. E. Bannister, al. etElectron-impact dissociation of ozone cations O-3(+)Phys. Rev. A 82, 062715 (2010)

e + O3+ 3−100eV Exp

688. Song Bin Zhang, Jian Guo Wang, R. K. JanevCrossover of Feshbach Resonances to Shape-Type Resonances in Electron-HydrogenAtom Excitation with a Screened Coulomb InteractionPhys. Rev. Lett. 104, 023203 (2010)

e + H 9.52−10.26eV Th

689. Jonathan TennysonElectron molecule collision calculations using the R-matrix methodPhys. Rep. 491, 29 (2010)

e + H2 1−10eV Th

690. M. Hoshino, H. Kato, D. Suzuki, al. etBenchmark Integral Cross Sections for Electron Impact Excitation of the n=2 Statesin HeliumPlasma Sci. Technol. 12, 348 (2010)

e + He 10−4000eVe + He 10−4000eV

691. Jung-Sik Yoon, Young-Woo Kim, Deuk-Chul Kwon, al. etElectron-impact cross sections for deuterated hydrogen and deuterium moleculesRep. Prog. Phys. 73, 116401 (2010)

e + D2 0.1−100eVe + H2 0.1−100eVe + HD 0.1−100eVe + D2 0.1−100eVe + H2 0.1−100eVe + HD 0.1−100eV

692. D. Nikolic, T. W. Gorczyca, K. T. Korista, N. R. BadnellDielectronic recombination of argon-like ionsAstron. Astrophys. 516, A97 (2010)

e + Zn12+ 0.1−10000eV The + Cu11+ 0.1−10000eV The + Ni10+ 0.1−10000eV The + Co9+ 0.1−10000eV The + Fe8+ 0.1−10000eV The + Mn7+ 0.1−10000eV The + Cr6+ 0.1−10000eV The + V5+ 0.1−10000eV The + Ti4+ 0.1−10000eV The + Sc3+ 0.1−10000eV The + Ca2+ 0.1−10000eV The + K+ 0.1−10000eV Th

194

693. C. V. Pandya, P. M. Patel, K. L. BalujaDifferential Scattering Cross Sections for Elastic Electron Scattering by a CalciumAtomChin. J. Phys. 48, 451 (2010)

e + Ca 20−500eV The + Ca 20−500eV Th

694. Jian-Hui Yang, Hong Zhang, Xin-Lu ChengThe KLL dielectronic recombination processes for highly charged krypton, iodine andbarium ionsChin. Phys. B 19, 063201 (2010)

e + Ba48+ 8.7−24keV The + Ba49+ 8.7−24keV The + Ba50+ 8.7−24keV The + Ba51+ 8.7−24keV The + Ba52+ 8.7−24keV The + Ba53+ 8.7−24keV The + Ba54+ 8.7−24keV The + I45+ 8.7−24keV The + I46+ 8.7−24keV The + I47+ 8.7−24keV The + I48+ 8.7−24keV The + I49+ 8.7−24keV The + I50+ 8.7−24keV The + I51+ 8.7−24keV The + Kr28+ 8.7−24keV The + Kr29+ 8.7−24keV The + Kr30+ 8.7−24keV The + Kr31+ 8.7−24keV The + Kr32+ 8.7−24keV The + Kr33+ 8.7−24keV The + Kr34+ 8.7−24keV Th

695. Jun-Bo Liu, Ya-Jun ZhouElastic scattering of electrons from water moleculeChin. Phys. B 19, 093403 (2010)

e + H2O 6−50eV Th

696. Y. Zhang, C. Y. Chen, M. Huang, Y. S. Wang, Y. M. ZouDielectronic recombination rate coefficients for the NiI isoelectronic sequenceEur. Phys. J. D 56, 157 (2010)

e + U64+ 5−69000eV The + At57+ 5−69000eV The + Pb54+ 5−69000eV The + Au51+ 5−69000eV The + W46+ 5−69000eV The + Yb42+ 5−69000eV The + Gd36+ 5−69000eV The + Nd32+ 5−69000eV The + Xe26+ 5−69000eV The + Sn22+ 5−69000eV The + Ag19+ 5−69000eV The + Mo14+ 5−69000eV The + Kr8+ 5−69000eV Th

697. E. Yu Remeta, V. I. KelemenPotential elastic electron scattering by atoms in the spin-polarized approachJ. Phys. B 43, 045202 (2010)

195

e + Eu 10eV, 20eV The + Mn 10eV, 20eV The + Sb 10eV, 20eV The + Ag 10eV, 20eV Th

698. R. K. Gangwar, A. N. Tripathi, L. Sharma, R. SrivastavaElastic scattering of electrons from Rb, Cs and Fr atomsJ. Phys. B 43, 085205 (2010)

e + Fr 2−300eV The + Cs 2−300eV The + Rb 2−300eV Th

699. H. Cho, M. Y. Song, J. S. Yoon, M. Hoshino, H. TanakaElastic electron scattering from CF3H and CF3IJ. Phys. B 43, 135205 (2010)

e + CF3H 1.5−30eV Expe + CF3I 1.5−30eV Exp

700. C. P. Ballance, S. D. Loch, M. S. Pindzola, D. C. GriffinDielectronic recombination of W35+J. Phys. B 43, 205201 (2010)

e + W35+ 5−3000eV Th

701. V. I. Kelemen, E. Yu RemetaElastic electron scattering from the antimony atom in the spin-polarized opticalpotential approachJ. Phys. B 43, 235204 (2010)

e + Sb 6−1000eV The + Sb 6−1000eV Th

702. Ireneusz Linert, Brygida Mielewska, George C. King, Mariusz ZubekElastic electron scattering in krypton in the energy range from 5 to 10 eVPhys. Rev. A 81, 012706 (2010)

e + Kr 5−10eV Exp

703. Jessica R. Francis-Staite, Brett A. Schmerl, Michael J. Brunger, H. Kato, Stephen J. BuckmanElastic electron scattering from CF3IPhys. Rev. A 81, 022704 (2010)

e + CF3I 10−50eV Exp

704. Z. Felfli, A. Z. Msezane, D. SokolovskiComplex angular momentum analysis of low-energy electron elastic scattering fromlanthanide atomsPhys. Rev. A 81, 042707 (2010)

e + Er 0−1eV The + Ho 0−1eV The + Sm 0−1eV The + Dy 0−1eV The + Hf 0−1eV The + Tm 0−1eV The + Pr 0−1eV Th

196

705. Magdalena Kaminska, Vitali Zhaunerchyk, Erik Vigren, Mathias Danielsson, Mathias Hamberg,Wolf D. Geppert, Mats Larsson, Stefan Rosen, Richard D. Thomas, Jacek SemaniakDissociative recombination of CH5+ and CD5+: Measurement of the productbranching fractions and the absolute cross sections, and the breakup dynamics in theCH3 + H + H product channelPhys. Rev. A 81, 062701 (2010)

e + CD5+ 0.0001− 1eV Exp

e + CH5+ 0.0001− 1eV Exp

706. H. Buhr, M. B. Mendes, O. Novotny, D. Schwalm, M. H. Berg, D. Bing, O. Heber, C. Krantz, D.A. Orlov, M. L. Rappaport, T. Sorg, J. Stuetzel, J. Varju, A. Wolf, D. ZajfmanEnergy-sensitive imaging detector applied to the dissociative recombination of D2H+Phys. Rev. A 81, 062702 (2010)

e + D2H+ 0.0001 − 10eV Exp

707. Vladimir A. Yerokhin, Andrey SurzhykovOff-resonant dielectronic recombination in a collision of an electron with a heavyhydrogenlike ionPhys. Rev. A 81, 062703 (2010)

e + U91+ 1−700MeV/nucleon Th

708. M. A. Khakoo, J. Muse, K. Ralphs, R. F. daCosta, M. H. F. Bettega, M. A. P. LimaLow-energy elastic electron scattering from furanPhys. Rev. A 81, 062716 (2010)

e + C4H4O 1−50eV Expe + C4H4O 1−50eV Exp

709. O. May, D. Kubala, M. AllanAbsolute cross sections for dissociative electron attachment to HCN and DCNPhys. Rev. A 82, 010701 (2010)

e + DCN 1.2−3.1eV Expe + HCN 1.2−3.1eV Exp

710. W. Zhang, K. Yao, Y. Yang, C. Chen, R. Hutton, Y. ZouLeaky ion extraction method for dielectronic recombination strength measurements atelectron-beam ion trapsPhys. Rev. A 82, 020702 (2010)

e + N2 400−1600eV Exp

711. Christopher J. Bostock, Dmitry V. Fursa, Igor BrayRelativistic convergent close-coupling method applied to electron scattering frommercuryPhys. Rev. A 82, 022713 (2010)

e + Hg 0−200eV Th

712. Holger Kreckel, Oldrich Novotny, Kyle N. Crabtree, Henrik Buhr, Annemieke Petrignani, Brian A.Tom, Richard D. Thomas, Max H. Berg, Dennis Bing, Manfred Grieser, Claude Krantz, MichaelLestinsky, Mario B. Mendes, Christian Nordhorn, Roland Repnow, Julia Stuetzel, Andreas Wolf,Benjamin J. McCallHigh-resolution storage-ring measurements of the dissociative recombination of H-3(+)using a supersonic expansion ion sourcePhys. Rev. A 82, 042715 (2010)

e + H3+ 0.00001−30eV Exp

197

713. Jorge L. S. LinoElastic scattering of electrons on Ne atoms at intermediate energiesPhys. Scr. 81, 035301 (2010)

e + Ne 0−200eV Th

714. A. K. F. Haque, M. Shahjahan, M. A. Uddin, M. A. R. Patoary, A. K. Basak, B. C. Saha, F. B.MalikGeneralized Kolbenstvedt model for electron impact ionization of the K-, L- and M-shell ionsPhys. Scr. 81, 045301 (2010)

e + Ni5+ 10−1000000eV The + Ar5+ 10−1000000eV The + Ti2+ 10−1000000eV The + S4+ 10−1000000eV The + Cr8+ 10−1000000eV The + Si3+ 10−1000000eV The + U82+ 10−1000000eV The + N3+ 10−1000000eV The + Ne3+ 10−1000000eV The + Ne8+ 10−1000000eV The + U89+ 10−1000000eV The + C5+ 10−1000000eV Th

715. M. M. Fujimoto, S. E. Michelin, F. Arretche, K. T. Mazon, M. -T. Lee, I. IgaSpin-Exchange Effects in Elastic Electron Scattering from Linear Triatomic RadicalsJ. Braz. Chem. Soc. 21, 226 (2010)

e + CNN 0−10eV The + NCN 0−10eV Th

716. M. Radmilovic-Radjenovic, Z. Lj. PetrovicCalculations of Cross Sections Data for Scattering of Electrons on HBrActa Phys. Pol. A 117, 745 (2010)

e + HBr 0−1000eV The + HBr 0−1000eV Th

717. E. A. Y. Castro, G. L. C. Souza, L. M. Brescansin, L. E. Machado, A. S. dosSantos, M-T LeeApplication of the scaled quasi-free scattering model absorption potential to electronscattering by CHx (x=1,2,3,4)J. Electron Spectrosc. Relat. Phenom. 182, 4 (2010)

e + CH4 5−1000eV The + CH3 5−1000eV The + CH2 5−1000eV The + CH 5−1000eV The + CH4 5−1000eV The + CH3 5−1000eV The + CH2 5−1000eV The + CH 5−1000eV The + CH4 5−1000eV The + CH3 5−1000eV The + CH2 5−1000eV The + CH 5−1000eV Th

718. D. G. M. Silva, T. Tejo, J. Muse, D. Romero, M. A. Khakoo, M. C. A. LopesTotal electron scattering cross sections for methanol and ethanol at intermediateenergiesJ. Phys. B 43, 015201 (2010)

198

e + C2H5OH 60−500eV Expe + CH3OH 60−500eV Exp

719. A. Zecca, L. Chiari, G. Garcia, F. Blanco, E. Trainotti, M. J. BrungerTotal cross sections for positron and electron scattering from pyrimidineJ. Phys. B 43, 215204 (2010)

e + C4H4N2 0.1−1000eV Th

720. P. Rawat, M. G. P. Homem, R. T. Sugohara, I. P. Sanches, I. Iga, G. L. C. deSouza, A. S. dosSantos,R. R. Lucchese, L. E. Machado, L. M. Brescansin, M-T LeeCross sections for electron scattering by ethane in the low- and intermediate-energyrangesJ. Phys. B 43, 225202 (2010)

e + C2H6 40−100eVe + C2H6 40−100eV

721. Xiao-Ming Tan, Zi-Jiang Liu, Xiao-Hong TianA revised additivity rule for electron scattering from ethylene, propene, butene,ethane, propane and butaneNucl. Instrum. Methods Phys. Res. B 268, 1535 (2010)

e + C4H10 10−1000eV The + C3H8 10−1000eV The + C2H6 10−1000eV The + C4H8 10−1000eV The + C3H6 10−1000eV The + C2H4 10−1000eV Th

722. W. M. Ariyasinghe, G. VilelaAn empirical expression for total scattering cross sections of normal hydrocarbons,and experimental total cross sections of C2H2 and C3H4Nucl. Instrum. Methods Phys. Res. B 268, 2217 (2010)

e + C3H4 200−4500eV Expe + C2H2 200−4500eV Exp

723. L. M. Brescansin, I. Iga, L. E. Machado, S. E. Michelin, M. -T. LeeCross sections for electron scattering by carbon disulfide in the low- and intermediate-energy rangePhys. Rev. A 81, 012709 (2010)

e + CS2 1−1000eV The + CS2 1−1000eV Th

724. J. Fedor, C. Winstead, V. McKoy, M. Cizek, K. Houfek, P. Kolorenc, J. HoracekElectron scattering in HCl: An improved nonlocal resonance modelPhys. Rev. A 81, 042702 (2010)

e + HCl 0−4eV Th

725. G. L. C. deSouza, M. -T. Lee, I. P. Sanches, P. Rawat, I. Iga, A. S. dosSantos, L. E. Machado, R.T. Sugohara, L. M. Brescansin, M. G. P. Homem, R. R. LuccheseCross sections for electron scattering by propane in the low- and intermediate-energyrangesPhys. Rev. A 82, 012709 (2010)

e + C3H8 40−500eVe + C3H8 40−500eV

199

726. M. Kurokawa, M. Kitajima, K. Toyoshima, T. Odagiri, H. Kato, H. Kawahara, M. Hoshino, H.Tanaka, K. ItoThreshold photoelectron source for the study of low-energy electron scattering: Totalcross section for electron scattering from krypton in the energy range from 14 meV to20 eVPhys. Rev. A 82, 062707 (2010)

e + Kr 0.014− 20eV Exp

727. M. H. F. Bettega, C. Winstead, V. McKoyLow-energy electron scattering from C4H9OH isomersPhys. Rev. A 82, 062709 (2010)

e + C4H9OH 1−50eV The + C4H9OH 1−50eV Th

728. C. Malespin, C. P. Ballance, M. S. Pindzola, M. C. Witthoeft, T. R. Kallman, S. D. LochElectron-impact excitation of H-like Cr, Mn, Fe, Co, and Ni for applications inmodeling X-ray astrophysical sourcesAstron. Astrophys. 526, A115 (2011)

e + H Z= 24-28 7E5−1E9 K Th

729. G. Y. Liang, N. R. BadnellR-matrix electron-impact excitation data for the Li-like iso-electronic sequenceincluding Auger and radiation dampingAstron. Astrophys. 528, A69 (2011)

e + Li Z= 4-36 2E2−2E6 (Z+1)2 K Th

730. G. Y. Liang, N. R. Badnell, G. Zhao, J. Y. Zhong, F. L. WangR-matrix electron-impact excitation data for astrophysically abundant sulphur ionsAstron. Astrophys. 533, A87 (2011)

e + S8+ 2E2−2E6 (Z+1)2 K The + S9+ 2E2−2E6 (Z+1)2 K The + S10+ 2E2−2E6 (Z+1)2 K The + S11+ 2E2−2E6 (Z+1)2 K Th

731. K. M. Aggarwal, F. P. Keenan, K. D. LawsonElectron impact excitation of Kr XXVIIIAt. Data Nucl. Data Tables 97, 225 (2011)

e + Kr27+ 1E7−1E9 K Th

732. K. Wang, C. Y. Chen, M. Huang, Y. S. Wang, Y. M. ZouRadiative rates and electron impact excitation rate coefficients for Ne-like selenium,Se XXVAt. Data Nucl. Data Tables 97, 426 (2011)

e + Se24+ 100−10000 eV Th

733. C. M. Cassidy, C. A. Ramsbottom, M. P. ScottELECTRON-IMPACT EXCITATION OF Ni II: EFFECTIVE COLLISIONSTRENGTHS FOR OPTICALLY ALLOWED FINE-STRUCTURE TRANSITIONSAstrophys. J. 738, 5 (2011)

e + Ni+ 30 − 1E6 K Th

200

734. S. S. Tayal, O. ZatsarinnyEFFECTIVE COLLISION STRENGTHS FOR ELECTRON-IMPACT EXCITATIONOF Fe VIIIAstrophys. J. 743, 206 (2011)

e + Fe7+ 5E3−5E6 K Th

735. Tayal, S. S.ELECTRON EXCITATION COLLISION STRENGTHS FOR SINGLY IONIZEDNITROGENAstrophys. J., Suppl. Ser. 195, 12 (2011)

e + N+ 500 − 1E5 K Th

736. I. R. Wasson, C. A. Ramsbottom, M. P. ScottELECTRON-IMPACT EXCITATION OF Cr II: A THEORETICALCALCULATION OF EFFECTIVE COLLISION STRENGTHS FOR OPTICALLYALLOWED TRANSITIONSAstrophys. J., Suppl. Ser. 196, 24 (2011)

e + Cr+ 2E3−1E5 K Th

737. S. Taj, B. Manaut, L. OufniSemirelativistic 1s-2s Excitation of Atomic Hydrogen by Electron ImpactActa Phys. Pol. A 119, 769 (2011)

e + H 50−300 eV The + H 50−300 eV Th

738. Hsiao-Ling Sun, Ju-Tang Hsiao, Sheng-Fang Lin, Keh-Ning HuangConspicuous QED Effects in the Positron-Impact Ionization of U91+Chin. J. Phys. 49, 175 (2011)

e+ + U91+ 1−10 threshold unit Th

739. S. Taj, B. Manaut, M. ElIdrissi, L. OufniLaser-Assisted Semi-Relativistic Excitation of Atomic Hydrogen by Electronic ImpactChin. J. Phys. 49, 1164 (2011)

e + H 50−300 eV The + H 50−300 eV Th

740. Lin-Mao Ren, You-Yan Wang, Dong-Dong Li, Zhen-Sheng Yuan, Lin-Fan ZhuInner-Shell Excitations of 2p Electrons of Argon Investigated by Fast Electron Impactwith High ResolutionChin. Phys. Lett. 28, 053401 (2011)

e + Ar 2500 eV Exp

741. Yang-Yang Zeng, Hao Feng, Wei-Guo SunIntegral and Momentum Cross Sections for Electron Elastic and Vibrational ExcitationScattering with Nitrogen in the Energy Range 5-30 eVChin. Phys. Lett. 28, 073401 (2011)

e + N2 5−30 eV The + N2 5−30 eV Th

742. M. Stroe, M. FifirigDissociation and vibrational excitation of cold HD+ by electron impactEur. Phys. J. D 61, 63 (2011)

201

e + HD+ 1−12 eV Th

743. M. Vinodkumar, C. G. Limbachiya, K. N. Joshipura, N. J. MasonElectron impact calculations of total elastic cross sections over a wide energy range-0.01 eV to 2 keV for CH4, SiH4 and H2OEur. Phys. J. D 61, 579 (2011)

e + CH4 0.01−2E3 eV The + SiH4 0.01−2E3 eV The + H2O 0.01−2E3 eV Th

744. L. Sharma, R. Srivastava, A. D. StaufferExcitation of the 5p(5)7p levels of xenon by electron impactEur. Phys. J. D 62, 399 (2011)

e + Xe threshold−200 eV Th

745. G. F. Du, J. Jiang, C. Z. DongElectron impact excitation into the 3p(5)4p levels from the 3p(5)4s metastable levelsof argonEur. Phys. J. D 63, 103 (2011)

e + Ar 4−12 eV, 50−400 eV Th

746. J. Lecointre, D. S. Belic, S. Cherkani-Hassani, P. DefranceElectron impact dissociation of ND+: formation of D+Eur. Phys. J. D 63, 441 (2011)

e + Nd+ threshold−2.5 keV E/T

747. P. Defrance, T. Kereselidze, J. Lecointre, Z. S. MachavarianiElectron-impact ionization of atomic hydrogen: dynamical variational treatmentEur. Phys. J. D 64, 303 (2011)

e + H 150, 250 eV The + H 150, 250 eV Th

748. Hee Seo, Maria Grazia Pia, Paolo Saracco, Chan Hyeong KimIonization Cross Sections for Low Energy Electron TransportIEEE Trans. Nucl. Sci. 58, 3219 (2011)

e threshold−1 keV Th

749. Kumar, RajeevElectron impact ionization cross-sections of carbonyl sulfide moleculeInt. J. Mass Spectrom. 303, 69 (2011)

e + e 0−300 eV Exp

750. Kevin M. Douglas, Stephen D. PriceElectron ionization of hydrogen sulfideInt. J. Mass Spectrom. 303, 147 (2011)

e + H2S 20−200 eV Exp

751. Minaxi Vinodkumar, Kirti Korot, P. C. VinodkumarComputation of the electron impact total ionization cross sections of CnH(2n+1)OHmolecules from the threshold to 2 keV energy rangeInt. J. Mass Spectrom. 305, 26 (2011)

202

e threshold−2 keV The + e threshold−2 keV Th

752. Minaxi Vinodkumar, Harshad Bhutadia, Chetan Limbachiya, K. N. JoshipuraElectron impact total ionization cross sections for H2S, PH3, HCHO and HCOOHInt. J. Mass Spectrom. 308, 35 (2011)

e + e threshold−2 keV The + HCOOH threshold−2 keV The + PH3 threshold−2 keV The + H2S threshold−2 keV Th

753. Svetlana V. Malinovskaya, Alexander V. Glushkov, Olga Yu. Khetselius, Yury M. Lopatkin, AndreyV. Loboda, Ludmila V. Nikola, Andrey A. Svinarenko, Tat’Yana B. PerelyginaGeneralized Energy Approach for Calculating Electron Collision Cross-Sections forMulticharged Ions in a Plasma: Debye Shielding ModelInt. J. Quantum Chem. 111, 288 (2011)

e + Ba46+ 5.69, 8.2 keV Th

754. M. A. R. Patoary, M. Alfaz Uddin, A. K. F. Haque, M. Shahjahan, A. K. Basak, B. C. SahaElectron Impact Ionization in K-, L-, and M-Shells of Atomic TargetsInt. J. Quantum Chem. 111, 923 (2011)

e + U threshold−200 MeV, −1GeV The + Bi threshold−200 MeV, −1GeV The + Pb threshold−200 MeV, −1GeV The + Au threshold−200 MeV, −1GeV The + Ta threshold−200 MeV, −1GeV The + Ni4+ threshold−200 MeV, −1GeV The + Ni7+ threshold−200 MeV, −1GeV The + Fe5+ threshold−200 MeV, −1GeV The + Ni8+ threshold−200 MeV, −1GeV The + Fe6+ threshold−200 MeV, −1GeV The + Ti2+ threshold−200 MeV, −1GeV The + e+ threshold−200 MeV, −1GeV The + Ar3+ threshold−200 MeV, −1GeV The + Cr10+ threshold−200 MeV, −1GeV The + Ar4+ threshold−200 MeV, −1GeV The + Ar5+ threshold−200 MeV, −1GeV The + Cl4+ threshold−200 MeV, −1GeV The + Ar6+ threshold−200 MeV, −1GeV The + Cl5+ threshold−200 MeV, −1GeV The + S4+ threshold−200 MeV, −1GeV The + Mg2+ threshold−200 MeV, −1GeV The + Si5+ threshold−200 MeV, −1GeV The + Ne+ threshold−200 MeV, −1GeV The + Si6+ threshold−200 MeV, −1GeV The + Ne2+ threshold−200 MeV, −1GeV The + F2+ threshold−200 MeV, −1GeV The + O+ threshold−200 MeV, −1GeV The + O2+ threshold−200 MeV, −1GeV The + N+ threshold−200 MeV, −1GeV The + O3+ threshold−200 MeV, −1GeV The + N2+ threshold−200 MeV, −1GeV The + C+ threshold−200 MeV, −1GeV The + U88+ threshold−200 MeV, −1GeV The + Ne6+ threshold−200 MeV, −1GeV The + C2+ threshold−200 MeV, −1GeV The + Li+ threshold−200 MeV, −1GeV Th

203

e + B3+ threshold−200 MeV, −1GeV The + C4+ threshold−200 MeV, −1GeV The + N5+ threshold−200 MeV, −1GeV The + O6+ threshold−200 MeV, −1GeV The + U90+ threshold−200 MeV, −1GeV The + Be+ threshold−200 MeV, −1GeV The + B2+ threshold−200 MeV, −1GeV The + N4+ threshold−200 MeV, −1GeV The + O5+ threshold−200 MeV, −1GeV The + Ne7+ threshold−200 MeV, −1GeV The + U89+ threshold−200 MeV, −1GeV Th

755. R. O. Jung, Garrett A. Piech, M. L. Keeler, John B. Boffard, L. W. Anderson, Chun C. LinElectron-impact excitation cross sections into Ne(2p(5)3p) levels for plasmaapplicationsJ. Appl. Phys. 109, 123303 (2011)

e + Ne threshold−200 eV Th

756. Michael D. Ward, Simon J. King, Stephen D. PriceElectron ionization of methane: The dissociation of the methane monocation anddicationJ. Chem. Phys. 134, 024308 (2011)

e + CH4 30−200 eV Exp

757. Simon J. King, Stephen D. PriceElectron ionization of SiCl4J. Chem. Phys. 134, 074311 (2011)

e + SiCl4 30−200 eV Exp

758. Hidetoshi Kato, Masamitsu Hoshino, Hiroshi Tanaka, Paulo Limao-Vieira, Oddur Ingolfsson,Laurence Campbell, Michael J. BrungerA study of electron scattering from benzene: Excitation of the B-1(1u), E-3(2g), andE-1(1u) electronic statesJ. Chem. Phys. 134, 134308 (2011)

e + C6H6 10−200 eV E/Te + C6H6 10−200 eV E/T

759. T. P. T. Do, M. Leung, M. Fuss, G. Garcia, F. Blanco, K. Ratnavelu, M. J. BrungerExcitation of electronic states in tetrahydrofuran by electron impactJ. Chem. Phys. 134, 144302 (2011)

e + C4H8O 15−50 eV Expe + C4H8O 15−50 eV Exp

760. S. J. Brotton, J. W. McConkeyDissociative excitation and fragmentation of S-8 by electron impactJ. Chem. Phys. 134, 204301 (2011)

e + e threshold−360 eV Exp

761. Allan, M.Electron scattering in Pt(PF3)(4): Elastic scattering, vibrational, and electronicexcitationJ. Chem. Phys. 134, 204309 (2011)

e + e 0.4−20 eV Expe + e 0.4−20 eV Expe + e 0.4−20 eV Exp

204

762. Noboru Watanabe, Daisuke Suzuki, Masahiko TakahashiVibronic effects on the 1t(1) -¿ 3s Rydberg excitation in CF4 induced by electronimpactJ. Chem. Phys. 134, 234309 (2011)

e + CF4 Th

763. Mariusz Zubek, Marcin Dampc, Ireneusz Linert, Tomasz NeumannElectronic states of tetrahydrofuran molecules studied by electron collisionsJ. Chem. Phys. 135, 134317 (2011)

e + C4H8O 5.5−10 eV Exp

764. Z Masn, J. D. GorfinkielElastic and inelastic low-energy electron collisions with pyrazineJ. Chem. Phys. 135, 144308 (2011)

e + C4H4N2 0−20 eV Th

765. P. Limao-Vieira, M. Horie, H. Kato, M. Hoshino, F. Blanco, G. Garcia, S. J. Buckman, H. TanakaDifferential elastic electron scattering cross sections for CCl4 by 1.5-100 eV energyelectron impactJ. Chem. Phys. 135, 234309 (2011)

e + CCl4 1.5−100 eV Exp

766. Harshad Bhutadia, Minaxi Vinodkumar, Bobby AntonyTheoretical Investigation of Electron Impact Total Ionization Cross Sections forN(CH3)(3), NH(CH3)(2), NH2CH3, P(CH3)(3), PH(CH3)(2), and PH2CH3MoleculesJ. Korean Phys. Soc. 59, 2873 (2011)

e + e threshold−2 keV The + P(CH3)3 threshold−2 keV Th

767. M. Z. M. Kamali, Kuru RatnaveluPositron Impact Excitation (n=2 states) of Hydrogen at 20 eVJ. Korean Phys. Soc. 59, 2895 (2011)

e+ + H 20 eV The+ + H 20 eV Th

768. Keh-Ning Huang, Hsiao-Ling Sun, Sheng-Fang Lin, Hao-Tse Shiao, Xin-Zeng WuRelativistic Quantum Collision Theory for Many-particle SystemsJ. Korean Phys. Soc. 59, 2941 (2011)

H+ + U91+ 1−15 threshold unit, 1−2000 keVThe + U91+ 1−15 threshold unit, 1−2000 keVTh

769. J. D. Hein, S. Kidwai, P. W. Zetner, C. Bostock, D. V. Fursa, I. Bray, L. Sharma, R. Srivastava,A. StaufferDifferential cross sections for electron-impact excitation of laser-excited Yb-174 (centerdot center dot center dot 6s6p (3)P1)J. Phys. B 44, 015202 (2011)

e + Yb 20 eV E/Te + Yb 20 eV E/T

770. C. DalCappello, A. Haddadou, F. Menas, A. C. RoyThe second Born approximation for the single and double ionization of atoms byelectrons and positronsJ. Phys. B 44, 015204 (2011)

205

e+ + H 250 eV The + H 250 eV The+ + H 250 eV The + H 250 eV Th

771. Rui Zhang, K. L. Baluja, Jan Franz, Jonathan TennysonPositron collisions with molecular hydrogen: cross sections and annihilationparameters calculated using the R-matrix with pseudo-states methodJ. Phys. B 44, 035203 (2011)

e+ + H2 0−10 eV Th

772. Khakoo, A. MurtadhaSymmetry relations in the relative intensities of the energy loss lines of argon excitedby electrons from the ground state to the 3p(5)4s fine-structure statesJ. Phys. B 44, 045208 (2011)

e + Ar threshold−100 eV Expe + Ar threshold−100 eV Exp

773. R. Ward, D. Cubric, N. Bowring, G. C. King, F. H. Read, D. V. Fursa, I. Bray, O. Zatsarinny, K.BartschatDifferential cross sections for electron impact excitation of the n=2 states of heliumat intermediate energies (80, 100 and 120 eV) measured across the complete angularscattering range (0-180 degrees)J. Phys. B 44, 045209 (2011)

e + He 80, 100, 120 eV E/Te + He 80, 100, 120 eV E/T

774. E. M. Staicu Casagrande, C. Li, A. Lahmam-Bennani, C. DalCappello, M. Schulz, M. CiappinaExperimental and theoretical confirmation of the role of higher order mechanisms inthe electron impact double ionization of heliumJ. Phys. B 44, 055201 (2011)

e + He 500 eV E/Te + He 500 eV E/T

775. Marcin Dampc, Ewelina Szymanska, Brygida Mielewska, Mariusz ZubekIonization and ionic fragmentation of tetrahydrofuran molecules by electron collisionsJ. Phys. B 44, 055206 (2011)

e + C4H8O 5−150 eV Exp

776. B. Predojevic, V. Pejcev, D. M. Filipovic, D. Sevic, B. Tomcik, B. P. MarinkovicElectron impact excitation of the 3s3p P-3 state of magnesium from the ground stateJ. Phys. B 44, 055208 (2011)

e + Mg 10, 15, 20, 40, 60 eV Expe + Mg 10, 15, 20, 40, 60 eV Exp

777. Igor Bray, Dmitry V. FursaBenchmark cross sections for electron-impact total single ionization of heliumJ. Phys. B 44, 061001 (2011)

e + He threshold−1 keV Th

778. M. Allan, O. Zatsarinny, K. BartschatElectron impact excitation of the (4p(5) 5s) states in krypton: high-resolution electronscattering experiments and B-spline R-matrix calculationsJ. Phys. B 44, 065201 (2011)

206

e + Kr 10−15 eV E/Te + Kr 10−15 eV E/T

779. Saha, P. HariTarget correlation and polarization effects on the electron impact ionization of HeatomsJ. Phys. B 44, 065202 (2011)

e + He 28.6 eV The + He 28.6 eV Th

780. P. Defrance, J. J. Jureta, J. Lecointre, X. UrbainIsotope effects in electron-impact dissociation of D2H+J. Phys. B 44, 075202 (2011)

e + D2H+ 5 eV−2.5 keV Exp

781. Yaqiu Liang, Zhangjin Chen, D. H. Madison, C. D. LinCalibration of distorted wave Born approximation for electron impact excitation of Neand Ar at incident energies below 100 eVJ. Phys. B 44, 085201 (2011)

e + Ar 20−100 eV The + Ne 20−100 eV The + Ar 20−100 eV The + Ne 20−100 eV Th

782. M. Fifirig, M. StroeDissociation of H-2(+) ions by collisions with electronsJ. Phys. B 44, 085202 (2011)

e + H2+ 1−12 eV Th

783. M. S. Pindzola, J. A. Ludlow, C. P. Ballance, F. Robicheaux, J. ColganElectron-impact double ionization of B+J. Phys. B 44, 105202 (2011)

e + B+ 63−750 eV Th

784. Alex Knight-Percival, Sarah Jhumka, Martyn Hussey, Andrew James MurraySuper-elastic electron scattering from the laser-excited 4(1)P(1) state of calcium atlow incident energyJ. Phys. B 44, 105203 (2011)

e + Ca 10−12 eV Expe + Ca 10−12 eV Exp

785. R. Naghma, B. N. Mahato, M. Vinodkumar, B. K. AntonyElectron impact total ionization cross sections for atoms with Z=49-54J. Phys. B 44, 105204 (2011)

e + Xe threshold−2000 eV The + I threshold−2000 eV The + Te threshold−2000 eV The + Sb threshold−2000 eV The + Sn threshold−2000 eV The + In threshold−2000 eV Th

786. C. Li, A. Lahmam-Bennani, E. M. Staicu Casagrande, C. DalCappelloElectron impact double ionization of neon, argon and molecular nitrogen: role of thetwo-step mechanismJ. Phys. B 44, 115201 (2011)

207

e + N2 600−700 eV Expe + Ar 600−700 eV Expe + Ne 600−700 eV Expe + N2 600−700 eV Expe + Ar 600−700 eV Expe + Ne 600−700 eV Exp

787. L. Vainshtein, I. Beigman, Ph Mertens, S. Brezinsek, A. Pospieszczyk, D. BorodinIonization of W atoms and W+ ions by electronsJ. Phys. B 44, 125201 (2011)

e + W+ threshold−500 eV The + W threshold−500 eV Th

788. Harshit N. Kothari, Siddharth H. Pandya, K. N. JoshipuraElectron impact ionization of plasma important SiClX (X=1-4) molecules: theoreticalcross sectionsJ. Phys. B 44, 125202 (2011)

e threshold−2000 eV Th

789. A. Borovik, A. Kupliauskiene, O. ZatsarinnyExcitation cross sections and spectroscopic classification of autoionizing levels in acaesium atomJ. Phys. B 44, 145203 (2011)

e + Cs 10−600 eV Exp

790. Y. K. Hahn, E. ZerradOptimized scattering functions and amplitudes for electron impact ionization and thepost-prior symmetryJ. Phys. B 44, 165201 (2011)

e + H Ea/E = 0.1, 0.3 (ratio of outgoing electron energy to incident electron energy)Th

791. J. Rausch, A. Becker, K. Spruck, J. Hellhund, A., Jr. Borovik, K. Huber, S. Schippers, A. MuellerElectron-impact single and double ionization of W17+J. Phys. B 44, 165202 (2011)

e + W17+ threshold−1000 eV E/T

792. M. A. Khakoo, O. Zatsarinny, K. BartschatNear-threshold electron impact excitation of the argon 3p(5)4s configuration-new andrevised normalized differential cross sections using recent time-of-flight measurementsfor normalization (vol 44, 015201, 2011)J. Phys. B 44, 169801 (2011)

e + Ar 13 eV Expe + Ar 13 eV Exp

793. J. Ma, Y. Cheng, Y. Cwang, Y. Zhou2s-3s excitation for positron-metastable hydrogen collisionsJ. Phys. B 44, 175203 (2011)

e+ + H 10−200 eV Th

794. B. M. McLaughlin, Teck-Ghee Lee, J. A. Ludlow, E. Landi, S. D. Loch, M. S. Pindzola, C. P.BallanceA large-scale R-matrix calculation for electron-impact excitation of the Ne2+, O-likeionJ. Phys. B 44, 175206 (2011)

208

e + Ne2+ 1E3−1E6 K Th

795. Toshinori Tsuchida, Takeshi Odagiri, Lisa Ishikawa, Kazufumi Yachi, Keisuke Shigemura, NaruhitoOhno, Kouichi Hosaka, Masashi Kitajima, Noriyuki KouchiDoubly excited states of water as studied by electron energy loss spectroscopy incoincidence with detecting Lyman-alpha photonsJ. Phys. B 44, 175207 (2011)

e + H2O 100 eV Exp

796. C. Q. Jiao, S. F. AdamsElectron ionization of selected cyclohexanesJ. Phys. B 44, 175209 (2011)

e + C8H16 10−200 eV Expe + C6H12 10−200 eV Exp

797. Rui Zhang, Pavlos G. Galiatsatos, Jonathan TennysonPositron collisions with acetylene calculated using the R-matrix with pseudo-statesmethodJ. Phys. B 44, 195203 (2011)

e+ + C2H2 0−5 eV Th

798. M. S. Sulc, R. Curik, J. P. Ziesel, N. C. Jones, D. FieldA new type of interference phenomenon in cold collisions of electrons with N-2J. Phys. B 44, 195204 (2011)

e + N2 0−250 meV E/T

799. I. Toth, L. NagyIonization of molecular nitrogen by electron impact in (e, 2e) processesJ. Phys. B 44, 195205 (2011)

e + N2 500−600 eV The + N2 500−600 eV Th

800. H. Kato, M. Ohkawa, H. Tanaka, I. Shimamura, M. J. BrungerVibrational excitation functions for inelastic and superelastic electron scattering fromthe ground electronic state in hot N2OJ. Phys. B 44, 195208 (2011)

e + N2O 0.65−4.55 eV Expe + N2O 0.65−4.55 eV Exp

801. Czeslaw Szmytkowski, Pawel Mozejko, Elzbieta Ptasinska-DengaElectron scattering from hexafluoroacetone molecules: cross section measurements andcalculationsJ. Phys. B 44, 205202 (2011)

e + e 1−400 eV E/Te + e 1−400 eV E/T

802. A., Jr. Borovik, C. Brandau, J. Jacobi, S. Schippers, A. MuellerElectron-impact single ionization of Xe10+ ionsJ. Phys. B 44, 205205 (2011)

e + Xe10+ threshold−1000 eV E/T

803. S. J. Brotton, J. W. McConkeyElectron-impact dissociative excitation of S-2J. Phys. B 44, 215202 (2011)

209

e + S2 threshold−370 eV E/T

804. F. Kossoski, T. C. Freitas, M. H. F. BettegaResonances in electron collisions with C2H2Cl2 isomersJ. Phys. B 44, 245201 (2011)

e + C2H2CL2 0−20 eV Th

805. Ken-ichi Akita, Shinobu Nakazaki, Akinori IgarashiStudy of Angular Momentum Transfer in Electron-Impact 2s -¿ 2p Excitation forLithium Isoelectronic SequenceJ. Phys. Soc. Japan 80, 034302 (2011)

e + Li Z= 3-6 1−1.5 threshold unit The + Li Z= 3-6 1−1.5 threshold unit Th

806. Yuko Tohyama, Tetsuo NagataAbsolute and Relative Measurements of Optical Emission Cross Sections for the N-2(+) 1Nd(v ’,v ”) Bands by Electron ImpactJ. Phys. Soc. Japan 80, 034304 (2011)

e + N2 18.8−300 eV Exp

807. Ken-ichi Akita, Shinobu Nakazaki, Akinori Igarashi, Akihiko OhsakiElastic Scattering and 3p Excitation from Ground State of Sodium IsoelectronicSequence by Electron ImpactJ. Phys. Soc. Japan 80, 114301 (2011)

e + Na Z= 12-14 threshold−20 eV Th

808. Marius Stroe, Magda FifirigDissociation of vibrationally excited D-2(+) by electronsMol. Phys. 109, 1617 (2011)

e + D2 1−12 eV Th

809. Y. Wu, Z. An, Y. M. Duan, M. T. Liu, J. WuK-shell ionization cross sections of Cl and L-alpha, L-beta X-ray production crosssections of Ba by 6-30 keV electron impactNucl. Instrum. Methods Phys. Res. B 269, 117 (2011)

e + Ba 6−30 keV Expe + Cl 6−30 keV Exp

810. R. Dey, A. C. RoyThe role of projectile interactions in triply differential cross sections for excitation-ionization of heliumNucl. Instrum. Methods Phys. Res. B 269, 364 (2011)

e + He 500, 1240−4260 eV The + He 500, 1240−4260 eV Th

811. Z. Felfli, A. Z. Msezane, D. SokolovskiLow-energy electron elastic collision cross sections for ground and excited Tm, Lu andHf atomsNucl. Instrum. Methods Phys. Res. B 269, 1046 (2011)

e + Hf 0−1.0 eV The + Lu 0−1.0 eV The + Tm 0−1.0 eV Th

210

812. Z. Rezkallah, S. Houamer, C. DalCappello, I. Charpentier, A. C. RoyIonization of molecules by electron impact: Differential and total cross sectionsNucl. Instrum. Methods Phys. Res. B 269, 2750 (2011)

e + CH4 threshold−1000 eV The + NH3 threshold−1000 eV The + H2O threshold−1000 eV The + Hf threshold−1000 eV Th

813. Saidou Diallo, I. G. Faye, I. A. Diedhiou, M. S. Tall, L. Gomis, C. S. DiattaTriple differential cross section for the ionization of helium by electronic impactNucl. Instrum. Methods Phys. Res. B 269, 2807 (2011)

e + He 1000 eV The + He 1000 eV Th

814. Tapasi Das, Rajesh Srivastava, A. D. StaufferElectron impact excitation of the resonance transition 5p(2)P(1/2)-6s(2)S(1/2) inindium atoms at small scattering anglesPhys. Lett. A 375, 568 (2011)

e + In 10−100 eV The + In 10−100 eV Th

815. Chuji Wang, Peeyush Sahay, Susan T. ScherrerA new optical method of measuring electron impact excitation cross section of atoms:Cross section of the metastable 6s6p P-3(0) level of HgPhys. Lett. A 375, 2366 (2011)

e + Hg 4−10 eV Exp

816. Zhongjun Li, Xu Shan, Jing Zhang, Damin Meng, Rui WangTriple differential cross section in (e, 2e) collisions for sodium in a coplanar symmetricgeometryPhys. Lett. A 375, 2563 (2011)

e + Na 10−65 eV The + Na 10−65 eV Th

817. S. J. Brotton, J. W. McConkeyVUV fluorescence following electron-impact dissociative excitation of CS2Phys. Rev. A 83, 012702 (2011)

e + Cs2 100 eV E/T

818. D. B. Jones, M. Yamazaki, N. Watanabe, M. TakahashiElectron-impact ionization of the water molecule at large momentum transfer abovethe double-ionization thresholdPhys. Rev. A 83, 012704 (2011)

e + H2O 2055 eV E/Te + H2O 2055 eV E/T

819. D. Oubaziz, H. Aouchiche, C. ChampionDouble ionization of the water molecule: Influence of the target orientation on thesecondary-electron angular distributionsPhys. Rev. A 83, 012708 (2011)

e + H2O 1 keV The + H2O 1 keV Th

211

820. Jose M. Fernandez-Varea, Silvina Segui, Michael DingfelderL alpha, L beta, and L gamma x-ray production cross sections of Hf, Ta, W, Re, Os,Au, Pb, and Bi by electron impact: Comparison of distorted-wave calculations withexperimentPhys. Rev. A 83, 022702 (2011)

e + Bi threshold−50 keV The + Pb threshold−50 keV The + Au threshold−50 keV The + Os threshold−50 keV The + Re threshold−50 keV The + W threshold−50 keV The + Ta threshold−50 keV The + Hf threshold−50 keV Th

821. W. Cao, J. -Cl. Dousse, J. Hoszowska, M. Kavcic, Y. Kayser, J. -L. Schenker, M. ZitnikDouble L3M ionization of Pd induced by impact with medium-energy electronsPhys. Rev. A 83, 022708 (2011)

e + Pd threshold−18 keV Exp

822. O. Zatsarinny, K. Bartschat, M. AllanHigh-resolution experiments and B-spline R-matrix calculations for elastic electronscattering from kryptonPhys. Rev. A 83, 032713 (2011)

e + Kr 0.3−9.8 eV Th

823. Xiangfu Jia, Shiyan SunEffects of dynamical screening on single ionization of sodium by electron impact indoubly symmetric geometryPhys. Rev. A 83, 032715 (2011)

e + Na 6−60 eV The + Na 6−60 eV Th

824. Song Bin Zhang, Jian Guo Wang, R. K. Janev, Xiang Jun ChenElectron-hydrogen atom-impact 1s -¿ 2s and 1s -¿ 2p excitation with screened Coulombinteraction between the n=2 and n=3 excitation thresholdsPhys. Rev. A 83, 032724 (2011)

e + H 11.2−12.1 eV Th

825. L. Pravica, J. F. Williams, D. Cvejanovi, S. Samarin, K. Bartschat, O. Zatsarinny, A. D. Stauffer,R. SrivastavaUnexpected effects in spin-polarized electron-impact excitation of the (3d(10)4s5s)S-3(1) state in zincPhys. Rev. A 83, 040701 (2011)

e + Zn 6.5−8.5 eV Exp

826. O. Zatsarinny, K. Bartschat, G. Garcia, F. Blanco, L. R. Hargreaves, D. B. Jones, R. Murrie, J. R.Brunton, M. J. Brunger, M. Hoshino, S. J. BuckmanElectron-collision cross sections for iodinePhys. Rev. A 83, 042702 (2011)

e + I 1−50 eV E/T

827. Chetan Limbachiya, Minaxi Vinodkumar, Nigel MasonCalculation of electron-impact rotationally elastic total cross sections for NH3, H2S,and PH3 over the energy range from 0.01 eV to 2 keVPhys. Rev. A 83, 042708 (2011)

212

e + PH3 0.01−2000 eV The + H2S 0.01−2000 eV The + NH3 0.01−2000 eV Th

828. Brent R. Yates, Murtadha A. KhakooNear-threshold electron-impact doubly differential cross sections for the ionization ofargon and kryptonPhys. Rev. A 83, 042712 (2011)

e + Kr 15−30 eV Expe + Ar 15−30 eV Expe + Kr 15−30 eV Expe + Ar 15−30 eV Exp

829. M. M. Ristic, G. B. Poparic, D. S. BelicExcitation of the a (3)Pi state of CO by electron impactPhys. Rev. A 83, 042714 (2011)

e + Co threshold−10 eV Expe + Co threshold−10 eV Exp

830. M. Allan, O. May, J. Fedor, B. C. Ibanescu, L. AndricAbsolute angle-differential vibrational excitation cross sections for electron collisionswith diacetylenePhys. Rev. A 83, 052701 (2011)

e + C4H2 1−10 eV Expe + C4H2 1−10 eV Exp

831. S. Xu, X. Ma, X. Ren, A. Senftleben, T. Pflueger, A. Dorn, J. UllrichFormation of protons from dissociative ionization of methane induced by 54 eVelectronsPhys. Rev. A 83, 052702 (2011)

e + CH4 54 eV Exp

832. M. Silenou Mengoue, M. G. Kwato Njock, B. Piraux, Yu. V. Popov, S. A. ZaytsevElectron-impact double ionization of He by applying the Jacobi matrix approach tothe Faddeev-Merkuriev equationsPhys. Rev. A 83, 052708 (2011)

e + He 5500−5600 eV The + He 5500−5600 eV Th

833. Christopher J. Bostock, Dmitry V. Fursa, Igor BrayCalculation of electron scattering from the ground state of ytterbiumPhys. Rev. A 83, 052710 (2011)

e + Yb threshold−200 eV The + Yb threshold−200 eV Th

834. X. Ren, I. Bray, D. V. Fursa, J. Colgan, M. S. Pindzola, T. Pflueger, A. Senftleben, S. Xu, A.Dorn, J. UllrichElectron-impact ionization of helium: A comprehensive experiment benchmarkstheoryPhys. Rev. A 83, 052711 (2011)

e + He 70.6 eV E/Te + He 70.6 eV E/T

213

835. Xueguang Ren, Arne Senftleben, Thomas Pflueger, Alexander Dorn, Klaus Bartschat, JoachimUllrichBenchmark experiment for electron-impact ionization of argon: Absolutetriple-differential cross sections via three-dimensional electron emission imagesPhys. Rev. A 83, 052714 (2011)

e + Ar 195 eV E/Te + Ar 195 eV E/T

836. L. Sharma, A. Surzhykov, R. Srivastava, S. FritzscheElectron-impact excitation of singly charged metal ionsPhys. Rev. A 83, 062701 (2011)

e + Ba+ threshold−300 eV The + Cd+ threshold−300 eV The + Zn+ threshold−300 eV The + Ca+ threshold−300 eV The + Mg+ threshold−300 eV Th

837. M. Allan, C. Winstead, V. McKoyAbsolute angle-differential elastic cross sections for electron collisions with diacetylenePhys. Rev. A 83, 062703 (2011)

e + C4H2 1−15 eV E/T

838. M. S. Pindzola, C. P. Ballance, S. D. LochElectron-impact ionization of moderately charged atomic ions in excited statesPhys. Rev. A 83, 062705 (2011)

e + C3+ threshold−50 eV Th

839. Savinder Kaur, Anand Bharadvaja, K. L. BalujaElectron-impact study of S-3 using the R-matrix methodPhys. Rev. A 83, 062707 (2011)

e + e 500−30000 K The + e 500−30000 K The + e 500−30000 K Th

840. C. DalCappello, C. Champion, I. Kada, A. MansouriDouble ionization of single oriented water molecules by electron impact: Second-orderBorn descriptionPhys. Rev. A 83, 062716 (2011)

e + H2O 310−340 eV The + H2O 310−340 eV Th

841. Chen, G. X.Breit-Pauli R-matrix method for electron-impact excitation to magnetic sublevels andx-ray-line polarization of ionsPhys. Rev. A 84, 012705 (2011)

e + Fe16+ 820−1150 eV Th

842. R. Celiberto, R. K. Janev, J. M. Wadehra, A. LaricchiutaCross sections for 14-eV e-H-2 resonant collisions: Isotope effect in dissociative electronattachmentPhys. Rev. A 84, 012707 (2011)

e + H2 1−1000 eV Th

214

843. J. A. Ludlow, T. G. Lee, C. P. Ballance, S. D. Loch, M. S. PindzolaLevel-resolved R-matrix calculations for the electron-impact excitation of Ne3+ andNe6+Phys. Rev. A 84, 022701 (2011)

e + Ne3+ 1E4−1E6, 1E7 K The + Ne6+ 1E4−1E6, 1E7 K Th

844. Omer Sise, Mevlut Dogan, Ibrahim Okur, Albert CroweElectron-impact excitation of the (2p(2)) D-1 and (2s2p) P-1(o) autoionizing states ofheliumPhys. Rev. A 84, 022705 (2011)

e + He 250 eV E/Te + He 250 eV E/T

845. Yong-Feng Wang, Shan Xi TianLow-energy electron collisions with thioformaldehydePhys. Rev. A 84, 022709 (2011)

e + e 0−10 eV The + e 0−10 eV Th

846. Zhangjin Chen, Yaqiu Liang, D. H. Madison, C. D. LinStrong-field nonsequential double ionization of Ar and NePhys. Rev. A 84, 023414 (2011)

e + Ne threshold−100 eV The + Ar threshold−100 eV The + Ne threshold−100 eV The + Ar threshold−100 eV Th

847. Hao Xu, Robin ShakeshaftNear-threshold behavior of electron-impact excitation of He+(2s) and He+(2p)Phys. Rev. A 84, 024701 (2011)

e + He 40.84−45.60 eV Th

848. L. E. Machado, R. T. Sugohara, A. S. dosSantos, M. -T. Lee, I. Iga, G. L. C. deSouza, M. G. P.Homem, S. E. Michelin, L. M. BrescansinAbsorption effects in electron-sulfur-dioxide collisionsPhys. Rev. A 84, 032709 (2011)

e + SO2 100−1000 eV E/T

849. C. DalCappello, Z. Rezkallah, S. Houamer, I. Charpentier, P. A. Hervieux, M. F. Ruiz-Lopez, R.Dey, A. C. RoySecond-order Born approximation for the ionization of molecules by electron andpositron impactPhys. Rev. A 84, 032711 (2011)

e+ + H2O 250 eV The + H2O 250 eV The+ + H2O 250 eV The + H2O 250 eV Th

850. Zhong-Wen Wu, Jun Jiang, Chen-Zhong DongInfluence of Breit interaction on the polarization of radiation following inner-shellelectron-impact excitation of highly charged berylliumlike ionsPhys. Rev. A 84, 032713 (2011)

215

e + Nd56+ (1−5)?threshold The + Mo38+ (1−5)?threshold The + Bi79+ (1−5)?threshold Th

851. M. Fogle, E. M. Bahati, M. E. Bannister, S. H. M. Deng, C. R. Vane, R. D. Thomas, V. ZhaunerchykElectron-impact dissociative excitation and ionization of N2D+Phys. Rev. A 84, 032714 (2011)

e + N2D+ 5−100 eV Exp

852. O. A. Fojon, C. R. Stia, R. D. RivarolaErasing the traces of classical mechanics in ionization of H-2 by quantum interferencesPhys. Rev. A 84, 032715 (2011)

e + H2 4087 eV Th

853. Pragya Bhatt, Raj Singh, Namita Yadav, R. ShankerDissociative-ionization cross sections for 12-keV-electron impact on CO2Phys. Rev. A 84, 042701 (2011)

e + CO2 12 keV Exp

854. M. H. F. Bettega, C. Winstead, V. McKoy, A. Jo, A. Gauf, J. Tanner, L. R. Hargreaves, M. A.KhakooCollisions of low-energy electrons with isopropanolPhys. Rev. A 84, 042702 (2011)

e + C3H7OH 1.5−30 eV E/T

855. Jasmeet Singh Rajvanshi, K. L. BalujaElectron-impact study of the S-2 molecule using the R-matrix methodPhys. Rev. A 84, 042711 (2011)

e + S2 0−10 eV The + S2 0−10 eV The + S2 0−10 eV Th

856. Minaxi Vinodkumar, Harshad Bhutadia, Bobby Antony, Nigel MasonElectron-impact rotationally elastic total cross sections for H2CO and HCOOH overa wide range of incident energy (0.01-2000 eV)Phys. Rev. A 84, 052701 (2011)

e + H2CO 1−1000 eV The + HCOOH 1−1000 eV Th

857. Michal Tarana, Karel Houfek, Jiri Horacek, Ilya I. FabrikantDissociative electron attachment and vibrational excitation of CF3Cl: Effect of twovibrational modes revisitedPhys. Rev. A 84, 052717 (2011)

e + CF3Cl 0.4−2.4 eV Th

858. A. L. Harris, B. Milum, D. H. MadisonIndistinguishability in electron-impact excitation-ionization of heliumPhys. Rev. A 84, 052718 (2011)

e + He 112−319 eV The + He 112−319 eV The + He 112−319 eV Th

216

859. Bettega, M. H. F.Elastic collisions of low-energy electrons with SiY4 (Y = Cl, Br, I) moleculesPhys. Rev. A 84, 052725 (2011)

e + SiBR4 1−10 eV The + SiI4 1−10 eV The + SiCl4 1−10 eV Th

860. L. R. Hargreaves, R. Albaridy, G. Serna, M. C. A. Lopes, M. A. KhakooElectron-impact vibrational excitation of furanPhys. Rev. A 84, 062705 (2011)

e + C4H4O 5−15 eV Exp

861. C. P. Ballance, S. D. Loch, J. A. Ludlow, Sh. A. Abdel-Naby, M. S. PindzolaElectron-impact ionization of C+ excited statesPhys. Rev. A 84, 062713 (2011)

e + C+ threshold−25 eV The + C+ threshold−25 eV Th

862. T. C. Freitas, S. d’A. Sanchez, M. T. do N. Varella, M. H. F. BettegaElectron collisions with hydrogen-bonded complexesPhys. Rev. A 84, 06714 (2011)

e 1−6 eV The + e 1−6 eV Th

863. Kate L. Nixon, Andrew James MurrayDifferential Cross Sections for Ionization of Laser-Aligned Atoms by Electron ImpactPhys. Rev. Lett. 106, 123201 (2011)

e + Mg 47.65 eV Expe + Mg 47.65 eV Exp

864. Oleg Zatsarinny, Klaus BartschatNonperturbative Treatment of Ionization with Excitation of Helium by ElectronImpactPhys. Rev. Lett. 107, 023203 (2011)

e + He 70 − 150 eV The + He 70 − 150 eV The + He 70 − 150 eV Th

865. K. M. Aggarwal, T. Kato, F. P. Keenan, I. MurakamiEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Li II, Be III, B IV and C VPhys. Scr. 83, 015302 (2011)

e + Li+ 1E4−1E6 K The + Be2+ 1E4−1E6 K The + B3+ 1E4−1E6 K The + C4+ 1E4−1E6 K Th

866. Stancalie, V.Forbidden transitions in excitation by electron impact in Co3+: an R-matrix approachPhys. Scr. 83, 025301 (2011)

e + Co3+ 40−70 eV Th

217

867. Satyendra Pal, Anshu, C. SinghElectron impact ionization cross sections for C-60 fullerenePhys. Scr. T144, 014036 (2011)

e + C60 threshold−1000 eV Th

868. D. -H. Kwon, D. W. SavinEFFECTS OF CONFIGURATION INTERACTION FOR DIELECTRONICRECOMBINATION OF Na-LIKE IONS FORMING Mg-LIKE IONSAstrophys. J. 734, 2 (2011)

e + Ca9+ 1−5000 eV The + Ti11+ 1−5000 eV The + Cr13+ 1−5000 eV The + Fe15+ 1−5000 eV The + Ni17+ 1−5000 eV The + Zn19+ 1−5000 eV Th

869. M. Hahn, M. Grieser, C. Krantz, M. Lestinsky, A. Mueller, O. Novotny, R. Repnow, S. Schippers,A. Wolf, D. W. SavinSTORAGE RING CROSS SECTION MEASUREMENTS FOR ELECTRONIMPACT IONIZATION OF Fe12+ FORMING Fe13+ AND Fe14+Astrophys. J. 735, 105 (2011)

e + Fe12+ 1E5−1E8 K Exp

870. A. Urbanowicz, A. Bielski, D. Lisak, R. Ciurylo, R. S. TrawinskiTemperature Effects on Dissociative Recombination in NeonActa Phys. Pol. A 119, 336 (2011)

e + Ne2+ 100−700 K Expe + Ne2+ 100−700 K Exp

871. Viatcheslav Kokoouline, Nicolas Douguet, Chris H. GreeneBreaking bonds with electrons: Dissociative recombination of molecular ionsChem. Phys. Lett. 507, 1 (2011)

e + H3+ 10−2000 K Th

872. N. Bhargava Ram, E. KrishnakumarDissociative electron attachment to methane probed using velocity slice imagingChem. Phys. Lett. 511, 22 (2011)

e + CH4 8−12 eV Exp

873. P. Lukac, O. Mikus, I. Morva, Z. Zabudla, J. Trnovec, M. MorvovaElectron Temperature Dependence of the Dissociative Recombination Coefficient ofMolecular Argon Ions Ar-2(+) with ElectronsContrib. Plasma Phys. 51, 672 (2011)

e + Ar2+ 3E3−1E4 K Exp

874. S. E. Huber, J. Seebacher, A. Kendl, D. ReiterAssessment of Hydrocarbon Electron-Impact Ionization Cross Section Measurementsfor Magnetic FusionContrib. Plasma Phys. 51, 931 (2011)

e + C2H2 threshold−1000 eV The + C2H4 threshold−1000 eV The + C3H6 threshold−1000 eV Th

218

875. H. Elabidi, S. Sahal-BrechotChecking the dependence on the upper level ionization potential of electron impactwidths using quantum calculationsEur. Phys. J. D 61, 285 (2011)

e + Mg6+ 1E5 K The + Na6+ 1E5 K The + Al7+ 1E5 K The + Na7+ 1E5 K The + Mg8+ 1E5 K The + Al9+ 1E5 K The + Mg9+ 1E5 K The + Al10+ 1E5 K The + Si10+ 1E5 K The + Ti10+ 1E5 K The + Cr12+ 1E5 K The + Cr13+ 1E5 K The + Fe14+ 1E5 K The + Fe15+ 1E5 K The + Ni17+ 1E5 K The + Fe22+ 1E5 K Th

876. M. Hoshino, P. Limao-Vieira, M. Probst, Y. Nunes, H. TanakaDissociative electron attachment to carbonyl fluoride, F2COInt. J. Mass Spectrom. 303, 125 (2011)

e + e 0−30 eV Exp

877. Patrick A. Lawson, David, Jr. Osborne, Nigel G. AdamsEffect of isotopic content on the rate constants for the dissociative electron-ionrecombination of N2H+Int. J. Mass Spectrom. 304, 41 (2011)

e + N2H 300−500 K Exp

878. David, Jr. Osborne, Patrick A. Lawson, Nigel G. AdamsFlowing afterglow studies of dissociative electron-ion recombination for a series ofsingle ring compounds at room temperatureInt. J. Mass Spectrom. 305, 35 (2011)

e + e+ 300 K Exp

879. M. Hoshino, S. Matejcik, Y. Nunes, F. FerreiradaSilva, P. Limao-Vieira, H. TanakaNegative ion formation through dissociative electron attachment to GeH4:Comparative studies with CH4 and SiH4Int. J. Mass Spectrom. 306, 51 (2011)

e + GeH4 6−11 eV Expe + CH4 6−11 eV Expe + SiH4 6−11 eV Exp

880. David S., Jr. Osborne, Patrick A. Lawson, Nigel G. AdamsThe effect of N-heteroatoms and CH3 substituents on dissociative electron-ionrecombination of protonated single six membered ring compounds at roomtemperatureInt. J. Mass Spectrom. 308, 114 (2011)

e + e 300 K Exp

219

881. Nicholas S. Shuman, Thomas M. Miller, Jeffrey F. Friedman, Albert A. Viggiano, Anatol I.Maergoiz, Juergen TroePressure and temperature dependence of dissociative and non-dissociative electronattachment to CF3: Experiments and kinetic modelingJ. Chem. Phys. 135, 054306 (2011)

e + CF3 300−600 K E/T

882. Gordon A. Gallup, Ilya I. FabrikantDissociative electron attachment to CH2Cl2, CHCH3Cl2, and C(CH3)(2)Cl-2J. Chem. Phys. 135, 134316 (2011)

e + CH2Cl2 0−2.0 eV The + C2H4Cl2 0−2.0 eV The + e 0−2.0 eV Th

883. U. I. Safronova, A. S. Safronova, P. Beiersdorfer, W. R. JohnsonExcitation energies, radiative and autoionization rates, dielectronic satellite lines anddielectronic recombination rates for excited states of Ag-like W from Pd-like WJ. Phys. B 44, 035005 (2011)

e + W28+ 0.1−10000 eV Th

884. L. R. Hargreaves, J. R. Brunton, A. Prajapati, M. Hoshino, F. Blanco, G. Garcia, S. J. Buckman,M. J. BrungerElastic cross sections for electron scattering from iodomethaneJ. Phys. B 44, 045207 (2011)

e + CH3I 5−50 eV Exp

885. S. Yan, X. Ma, P. Zhang, S. Xu, S. F. Zhang, X. L. Zhu, W. T. Feng, H. P. LiuSignatures of the projectile electron-target core elastic scattering in Ar (e, 2e) reactionsat low and intermediate impact energiesJ. Phys. B 44, 055202 (2011)

e + Ar 80−220 eV Exp

886. Bostock, James ChristopherThe fully relativistic implementation of the convergent close-coupling methodJ. Phys. B 44, 083001 (2011)

e + Ar17+ (2−28)*threshold, threshold−100 eVThe + Ti21+ (2−28)*threshold, threshold−100 eVThe + Fe25+ (2−28)*threshold, threshold−100 eVThe + Hg (2−28)*threshold, threshold−100 eVTh

887. N. R. Badnell, A. Foster, D. C. Griffin, D. Kilbane, M. O’Mullane, H. P. SummersDielectronic recombination of heavy species: the tin 4p64dq ? 4p64d(q?1)4f +4p54d(q+1) transition arrays for q = 1?10J. Phys. B 44, 135201 (2011)

e + Sn4+ 1−1000 eV The + Sn5+ 1−1000 eV The + Sn6+ 1−1000 eV The + Sn7+ 1−1000 eV The + Sn8+ 1−1000 eV The + Sn9+ 1−1000 eV The + Sn10+ 1−1000 eV The + Sn11+ 1−1000 eV The + Sn12+ 1−1000 eV The + Sn13+ 1−1000 eV Th

220

888. Z. Felfli, A. Z. Msezane, D. SokolovskiElastic scattering of slow electrons from Y, Ru, Pd, Ag and Pt atoms: search forJ. Phys. B 44, 135204 (2011)

e + Y 0−7 eV The + Ru 0−7 eV The + Pd 0−7 eV The + Ag 0−7 eV The + Pt 0−7 eV Th

889. D. S. Slaughter, H. Adaniya, T. N. Rescigno, D. J. Haxton, A. E. Orel, C. W. McCurdy, A. BelkacemDissociative electron attachment to carbon dioxide via the 8.2 eV Feshbach resonanceJ. Phys. B 44, 205203 (2011)

e + CO2 8.2 eV E/T

890. U. I. Safronova, P. G. Wilcox, A. S. SafronovaRelativistic calculations of dielectronic recombination and satellite lines of an Ar-likeNi ionJ. Phys. B 44, 225002 (2011)

e + Ni10+ 0.1−5000 eV Th

891. Fabrikant, I. IlyaDissociative electron attachment to CH3I on surfaces and in bulk media: vibrationalFeshbach resonance suppressionJ. Phys. B 44, 225202 (2011)

e + S2 threshold−100 eV E/T

892. G. Purohit, Vinod Patidar, K. K. SudDifferential cross section calculations of positron and electron impact ionization of Ar(3p)Nucl. Instrum. Methods Phys. Res. B 269, 745 (2011)

e + Ar 100−500 eV The+ + Ar 100−500 eV The + Ar 100−500 eV The+ + Ar 100−500 eV Th

893. Duck-Hee Kwon, Daniel Wolf SavinFe15+ dielectronic recombination and the effects of configuration interaction betweenresonances with different captured electron principal quantum numbersPhys. Rev. A 83, 012701 (2011)

e + Fe15+ 300−900 eV Th

894. Gordon A. Gallup, Ilya I. FabrikantVibrational Feshbach resonances in dissociative electron attachment to uracilPhys. Rev. A 83, 012706 (2011)

e + C4H4N2O2 0.7−2.3 eV The + e 0.7−2.3 eV Th

895. S. Schippers, D. Bernhardt, A. Mueller, C. Krantz, M. Grieser, R. Repnow, A. Wolf, M. Lestinsky,M. Hahn, O. Novotny, D. W. SavinDielectronic recombination of xenonlike tungsten ionsPhys. Rev. A 83, 012711 (2011)

e + W20+ 0−140 eV Exp

221

896. D. Bernhardt, C. Brandau, Z. Harman, C. Kozhuharov, A. Mueller, W. Scheid, S. Schippers, E. W.Schmidt, D. Yu, A. N. Artemyev, I. I. Tupitsyn, S. Boehm, F. Bosch, F. J. Currell, B. Franzke, A.Gumberidze, J. Jacobi, P. H. Mokler, F. Nolden, U. Spillman, Z. Stachura, M. Steck, Th. StoehlkerBreit interaction in dielectronic recombination of hydrogenlike uraniumPhys. Rev. A 83, 020701 (2011)

e + U91+ 63−90 keV E/T

897. S. T. Chourou, A. E. OrelIsotope effect in dissociative electron attachment to HCNPhys. Rev. A 83, 032709 (2011)

e + HCN 0−4 eV The + DCN 0−4 eV Th

898. Annemieke Petrignani, Simon Altevogt, Max H. Berg, Dennis Bing, Manfred Grieser, JensHoffmann, Brandon Jordon-Thaden, Claude Krantz, Mario B. Mendes, Oldrich Novotny, SteffenNovotny, Dmitry A. Orlov, Roland Repnow, Tobias Sorg, Julia Stuetzel, Andreas Wolf, HenrikBuhr, Holger Kreckel, Viatcheslav Kokoouline, Chris H. GreeneResonant structure of low-energy H-3(+) dissociative recombinationPhys. Rev. A 83, 032711 (2011)

e + H3+ 1E−5−1E0 eV E/T

899. M. S. Pindzola, S. D. Loch, F. RobicheauxDielectronic recombination in C3+ above and below the ionization thresholdPhys. Rev. A 83, 042705 (2011)

e + C3+ threshold Th

900. Z. Felfli, A. Z. Msezane, D. SokolovskiLow-energy electron elastic scattering from Mn, Cu, Zn, Ni, Ag, and Cd atomsPhys. Rev. A 83, 052705 (2011)

e + Mn 0−1 eV The + Ni 0−1 eV The + Cu 0−1 eV The + Zn 0−1 eV The + Ag 0−1 eV The + Cd 0−1 eV Th

901. Y. B. Fu, C. Z. Dong, M. G. Su, F. Koike, G. O’Sullivan, J. G. WangTheoretical investigation of dielectronic recombination of Sn12+ ionsPhys. Rev. A 83, 062708 (2011)

e + Sn12+ 1−1000 eV Th

902. Jeremy S. Savage, Dmitry V. Fursa, Igor BrayConvergent close-coupling calculations of positron-magnesium scatteringPhys. Rev. A 83, 062709 (2011)

e+ + Mg 0.01−100 eV Th

903. A. R. Lopes, S. d’A. Sanchez, M. H. F. BettegaElastic scattering of low-energy electrons by nitromethanePhys. Rev. A 83, 062713 (2011)

e + e 0−10 eV Th

222

904. F. O. Waffeu Tamo, H. Buhr, O. Motapon, S. Altevogt, V. M. Andrianarijaona, M. Grieser, L.Lammich, M. Lestinsky, M. Motsch, I. Nevo, S. Novotny, D. A. Orlov, H. B. Pedersen, D. Schwalm,F. Sprenger, X. Urbain, U. Weigel, A. Wolf, I. F. SchneiderAssignment of resonances in dissociative recombination of HD+ ions: High-resolutionmeasurements compared with accurate computationsPhys. Rev. A 84, 022710 (2011)

e + HD+ 1E−4−20 eV E/T

905. D. J. Haxton, H. Adaniya, D. S. Slaughter, B. Rudek, T. Osipov, T. Weber, T. N. Rescigno, C. W.McCurdy, A. BelkacemObservation of the dynamics leading to a conical intersection in dissociative electronattachment to waterPhys. Rev. A 84, 030701 (2011)

e + H2O 11.3 eV E/T

906. Daniel J. Haxton, Chris H. GreeneAb initio frame-transformation calculations of direct and indirect dissociativerecombination rates of HeH+ + e(-) (vol 79, 022701, 2009)Phys. Rev. A 84, 039903 (2011)

e + HeH+ 0.01−1 eV Th

907. C. J. Colyer, S. M. Bellm, F. Blanco, G. Garcia, B. LohmannElastic electron scattering from the DNA bases cytosine and thyminePhys. Rev. A 84, 042707 (2011)

e + C4H5N3O 60−500 eV E/Te + e 60−500 eV E/T

908. Mingwu Zhang, Xiaohong Cai, Asa Larson, Ann E. OrelTheoretical study of dissociative recombination of Cl-2(+)Phys. Rev. A 84, 052707 (2011)

e + Cl2+ 1E1−1E5 K Th

909. Serov, V. VladislavCalculation of intermediate-energy electron-impact ionization of molecular hydrogenand nitrogen using the paraxial approximationPhys. Rev. A 84, 062701 (2011)

e + H2 200−600 eV The + N2 200−600 eV Th

910. R. T. Sugohara, M. -T. Lee, G. L. C. deSouza, M. G. P. Homem, I. IgaCross sections for elastic electron scattering by tetramethylsilane in the intermediate-energy rangePhys. Rev. A 84, 062709 (2011)

e + e 100−1000 eV E/T

911. N. Bhargava Ram, Vaibhav S. Prabhudesai, E. KrishnakumarComment on Imaging the Molecular Dynamics of Dissociative Electron Attachmentto WaterPhys. Rev. Lett. 106, 049301 (2011)

e + H2O 8.5,9.5 eV The + H2O 8.5,9.5 eV Th

223

912. E. Krishnakumar, S. Denifl, I. Cadez, S. Markelj, N. J. MasonDissociative Electron Attachment Cross Sections for H-2 and D-2Phys. Rev. Lett. 106, 243201 (2011)

e + H2 0−20 eV Expe + D2 0−20 eV Exp

913. D. Androic, D. S. Armstrong, J. Arvieux, S. L. Bailey, D. H. Beck, E. J. Beise, J. Benesch, F.Benmokhtar, L. Bimbot, J. Birchall, P. Bosted, H. Breuer, C. L. Capuano, Y. -C. Chao, A. Coppens,C. A. Davis, C. Ellis, G. Flores, G. Franklin, C. Furget, D. Gaskell, M. T. W. Gericke, J. Grames,G. Guillard, J. Hansknecht, T. Horn, M. K. Jones, P. M. King, W. Korsch, S. Kox, L. Lee, J.Liu, A. Lung, J. Mammei, J. W. Martin, R. D. McKeown, A. Micherdzinska, M. Mihovilovic, H.Mkrtchyan, M. Muether, S. A. Page, V. Papavassiliou, S. F. Pate, S. K. Phillips, P. Pillot, M. L.Pitt, M. Poelker, B. Quinn, W. D. Ramsay, J. -S. Real, J. Roche, P. Roos, J. Schaub, T. Seva,N. Simicevic, G. R. Smith, D. T. Spayde, M. Stutzman, R. Suleiman, V. Tadevosyan, W. T. H.vanOers, M. Versteegen, E. Voutier, W. Vulcan, S. P. Wells, S. E. Williamson, S. A. Wood, B.Pasquini, M. VanderhaeghenTransverse Beam Spin Asymmetries at Backward Angles in Elastic Electron-Protonand Quasielastic Electron-Deuteron ScatteringPhys. Rev. Lett. 107, 022501 (2011)

e + H+ 362,687 eV Expe + D+ 362,687 eV Exp

914. Christopher J. Bostock, Michael J. Berrington, Dmitry V. Fursa, Igor BrayRelativistic and Close-Coupling Effects in the Spin Polarization of Low-EnergyElectrons Scattered Elastically from CadmiumPhys. Rev. Lett. 107, 093202 (2011)

e + Cd 0.3−9.0 eV Th

915. Oleg Y. Andreev, Leonti N. Labzowsky, Alexander V. PrigorovskyDielectronic recombination with one-electron highly charged ionsPhys. Scr. T144, 014008 (2011)

e + U91+ 63−73.5, 0−31.3 keV The + Gd63+ 63−73.5, 0−31.3 keV Th

916. Zhi-min Hu, Yue-ming Li, Akira Yamazaki, Nobuyuki NakamuraTwo-photon observations of dielectronic recombination processesPhys. Scr. T144, 014047 (2011)

e + Kr35+ 9.22, 9.24 keV E/T

917. C. E. Hudson, P. H. Norrington, C. A. Ramsbottom, M. P. ScottDirac R-matrix collision strengths and effective collision strengths for transitions ofNi XVIIAstron. Astrophys. 537, A12 (2012)

e + Ni16+ 1E4.5−1E8 K Th

918. S. S. TayalBreit-Pauli oscillator strengths and electron excitation collision strengths for Si VIIIAstron. Astrophys. 541, A61 (2012)

e + Si7+ 1E4−1E6.5 K Th

919. G. Y. Liang, N. R. Badnell, G. ZhaoR-matrix electron-impact excitation data for the B-like iso-electronic sequenceAstron. Astrophys. 547, A87 (2012)

224

e + Kr31+ 0−−400 Ryd The + Fe21+ 0−−400 Ryd The + Ar13+ 0−−400 Ryd The + Ne5+ 0−−400 Ryd Th

920. S. S. TayalOscillator strengths and effective collision strengths for electron excitation of Mg VIAstron. Astrophys. 548, A27 (2012)

e + Mg5+ 10000−200000 K Th

921. L. Di, J. R. Shi, G. ZhaoElectron impact collision strengths in Ne VIIAt. Data Nucl. Data Tables 98, 437 (2012)

e + Ne6+ 1E5.8−1E7 K Th

922. K. Wang, J. Yan, M. Huang, C. Y. Li, J. L. Zeng, C. Y. Chen, Y. S. Wang, Y. M. ZouElectron impact excitation rate coefficients for P-like Ni XIVAt. Data Nucl. Data Tables 98, 779 (2012)

e + Ni13+ 1E5 1E8 K Th

923. C. E. Hudson, C. A. Ramsbottom, M. P. ScottCOLLISION STRENGTHS AND EFFECTIVE COLLISION STRENGTHS FORTRANSITIONS WITHIN THE GROUND-STATE CONFIGURATION OF S IIIAstrophys. J. 750, 65 (2012)

e + S2+ 0−2 RYD Th

924. S. Mahmood, S. Ali, I. Orban, S. Tashenov, E. Lindroth, R. SchuchRECOMBINATION AND ELECTRON IMPACT EXCITATION RATECOEFFICIENTS FOR S XV AND S XVIAstrophys. J. 754, 86 (2012)

e + S15+ 1.4−3.0 keV Expe + S14+ 1.4−3.0 keV Expe + S15+ 1.4−3.0 keV Expe + S14+ 1.4−3.0 keV Exp

925. M. Hahn, A. Becker, M. Grieser, C. Krantz, M. Lestinsky, A. Mueller, O. Novotny, R. Repnow, S.Schippers, K. Spruck, A. Wolf, D. W. SavinSTORAGE RING CROSS-SECTION MEASUREMENTS FOR ELECTRONIMPACT SINGLE AND DOUBLE IONIZATION OF Fe9+ AND SINGLEIONIZATION OF Fe10+Astrophys. J. 760, 80 (2012)

e + Fe10+ 250−1200 eV Expe + Fe9+ 250−1200 eV Exp

926. A. M. Sossah, S. S. TayalTRANSITION PROBABILITIES AND COLLISION STRENGTHS FORELECTRON-IMPACT EXCITATION OF Cl IIIAstrophys. J., Suppl. Ser. 202, 12 (2012)

e + Cl2+ 5E3−1E6 K Th

927. S. Y. Sun, X. Y. Ma, X. Li, X. Y. Miao, X. F. JiaEffect of initial-state target polarization on the single ionization of helium by 1-keVelectron impactChin. Phys. B 21, 73402 (2012)

225

e + He 1keV Th

928. S. S. Zang, Z. M. GePost-collision interactions and the polarization effect in (e, 2e) collisions of heliumChin. Phys. B 21, 73403 (2012)

e + He 50, 102eV Th

929. Y. Wang, Y. J. Zhou, L. G. JiaoSecond-Order Born Effect in Single Ionization of Argon by Electron ImpactChin. Phys. Lett. 29, 13401 (2012)

e + Ar 37,74,205eV Th

930. R. Celiberto, R. K. Janev, J. M. Wadehra, J. TennysonDissociative electron attachment to vibrationally excited H-2 molecules involving the(2)Sigma(+)(g) resonant Rydberg electronic stateChem. Phys. 398, 206 (2012)

e + H2 8−18eV Th

931. M. M. Ristic, M. Vojnovic, G. B. Poparic, D. S. BelicRate coefficients for electron impact excitation of the a(3)Pi state of COChem. Phys. 405, 16 (2012)

e + Co 0−17eV Th

932. Y. Y. Zeng, H. Feng, W. G. SunStudies on the vibrational excitation differential cross sections of non-resonant e-N-2scattering using augmented polarization potentialsEur. Phys. J. D 66, 3 (2012)

e + N2 4−15eV Th

933. I. Linert, M. Dampc, B. Mielewska, M. ZubekCross sections for ionization and ionic fragmentation of pyrimidine molecules byelectron collisionsEur. Phys. J. D 66, 20 (2012)

e + C4H4N2 10−150eV Exp

934. I. Toth, R. I. Campeanu, L. NagyTriple differential cross sections for the ionization of water by electron and positronimpactEur. Phys. J. D 66, 21 (2012)

e + H2O 250eV The + H2O 250eV Th

935. K. Chakrabarti, J. TennysonElectron collisions with the BeH+ molecular ion in the R-matrix approachEur. Phys. J. D 66, 31 (2012)

e + BeH+ 0−24eV Th

936. K. Anzai, H. Kato, M. Hoshino, H. Tanaka, Y. Itikawa, L. Campbell, M. J. Brunger, S. J. Buckman,H. Cho, F. Blanco, G. Garcia, P. Limao-Vieira, O. IngolfssonCross section data sets for electron collisions with H-2, O-2, CO, CO2, N2O and H2OEur. Phys. J. D 66, 36 (2012)

226

e + H2 0.01−1000eV Expe + H2O 0.01−1000eV Expe + N2O 0.01−1000eV Expe + CO2 0.01−1000eV Expe + Co 0.01−1000eV Expe + O2 0.01−1000eV Expe + H2 0.01−1000eV Expe + H2O 0.01−1000eV Expe + N2O 0.01−1000eV Expe + CO2 0.01−1000eV Expe + Co 0.01−1000eV Expe + O2 0.01−1000eV Expe + H2 0.01−1000eV Expe + H2O 0.01−1000eV Expe + N2O 0.01−1000eV Expe + CO2 0.01−1000eV Expe + Co 0.01−1000eV Expe + O2 0.01−1000eV Exp

937. P. Mozejko, E. Ptasinska-Denga, C. SzmytkowskiCross sections for electron collision with five-membered ring heterocyclesEur. Phys. J. D 66, 44 (2012)

e + C3H3NO 8−3000eV Expe + C3H3NO 8−3000eV Exp

938. I. Cadez, S. Markelj, Z. RupnikLow energy H- production by electron collision with small hydrocarbonsEur. Phys. J. D 66, 73 (2012)

e + C3H8 0−20eV Expe + C2H6 0−20eV Expe + C2H4 0−20eV Expe + C2H2 0−20eV Expe + CH4 0−20eV Expe + C3H8 0−20eV Expe + C2H6 0−20eV Expe + C2H4 0−20eV Expe + C2H2 0−20eV Expe + CH4 0−20eV Exp

939. M. Vinodkumar, C. G. Limbachiya, M. Y. Barot, N. J. MasonComputation of the total scattering cross sections for electron impact on HCl and HBrbetween 0.1 eV and 2000 eVEur. Phys. J. D 66, 74 (2012)

e + HBr 0.1−2000 eV The + HCl 0.1−2000 eV Th

940. S. Kumari, L. K. JhaElectron impact double ionization of Mg+ ionsEur. Phys. J. D 66, 87 (2012)

e + Mg+ 100−1000 eV Th

941. L. K. Jha, M. P. Singh, S. KumarDouble ionization of Ne5+ and Ne6+ ions by electron impactEur. Phys. J. D 66, 116 (2012)

e + Ne6+ 450−5000 eV The + Ne5+ 450−5000 eV Th

227

942. M. M. Fujimoto, W. J. Brigg, J. TennysonR-matrix calculations of differential and integral cross sections for low-energy electroncollisions with ethanolEur. Phys. J. D 66, 204 (2012)

e + C2H5OH 0−10 eV The + C2H5OH 0−10 eV Th

943. D. S. Belic, J. J. Jureta, J. Lecointre, H. Cherkani-Hassani, S. Cherkani-Hassani, P. DefranceElectron-impact dissociation and ionization of OH+ and OD+ ionsEur. Phys. J. D 66, 218 (2012)

e + OD+ 20−2500 eV The + OH+ 20−2500 eV The + OD+ 20−2500 eV The + OH+ 20−2500 eV Th

944. M. Guerra, F. Parente, P. Indelicato, J. P. SantosModified binary encounter Bethe model for electron-impact ionizationInt. J. Mass Spectrom. 313, 1 (2012)

e + Zn 0.1−1E6 keV The + Fe 0.1−1E6 keV The + Cr 0.1−1E6 keV The + V 0.1−1E6 keV The + Ti 0.1−1E6 keV The + Sc 0.1−1E6 keV The + Si 0.1−1E6 keV The + Ne 0.1−1E6 keV The + C 0.1−1E6 keV The + Bi 0.1−1E6 keV The + Pb 0.1−1E6 keV The + Ba 0.1−1E6 keV The + Xe 0.1−1E6 keV The + Sb 0.1−1E6 keV The + Ag 0.1−1E6 keV The + Kr 0.1−1E6 keV The + Se 0.1−1E6 keV The + Sr 0.1−1E6 keV The + Co 0.1−1E6 keV Th

945. K. Wnorowski, M. Stano, W. Barszczewska, A. Jowko, S. MatejcikElectron ionization of W(CO)(6): Appearance energiesInt. J. Mass Spectrom. 314, 42 (2012)

e + W(CO)6 0−150eV Exp

946. M. A. Rahman, S. Gangopadhyay, C. Limbachiya, K. N. Joshipura, E. KrishnakumarElectron ionization of NF3Int. J. Mass Spectrom. 319, 48 (2012)

e + NF3 20−500eV E/T

947. S. H. Pandya, F. A. Shelat, K. N. Joshipura, B. G. VaishnavElectron ionization of exotic molecular targets CN, C2N2, HCN, HNC andBF-Theoretical cross sectionsInt. J. Mass Spectrom. 323, 28 (2012)

e + BF 10−2000eV The + HNC 10−2000eV The + HCN 10−2000eV The + C2N2 10−2000eV The + CN 10−2000eV Th

228

948. H. Kato, A. Suga, M. Hoshino, F. Blanco, G. Garcia, P. Limao-Vieira, M. J. Brunger, H. TanakaElastic cross sections for electron scattering from GeF4: Predominance of atomic-F inthe high-energy collision dynamicsJ. Chem. Phys. 136, 134313 (2012)

e + GeF4 3−200eV Exp

949. M. Vinodkumar, A. Barot, B. AntonyElectron impact total cross section for acetylene over an extensive range of impactenergies (1 eV-5000 eV)J. Chem. Phys. 136, 184308 (2012)

e + C2H2 1−5000eV Th

950. T. P. T. Do, K. L. Nixon, M. Fuss, G. Garcia, F. Blanco, M. J. BrungerElectron impact excitation of the (a)over-tilde B-3(1u) electronic state in C2H4: Anexperimentally benchmarked system?J. Chem. Phys. 136, 184313 (2012)

e + C2H4 5−50eV Exp

951. M. Ziolkowski, A. Vikar, M. L. Mayes, A. Bencsura, G. Lendvay, G. C. SchatzModeling the electron-impact dissociation of methaneJ. Chem. Phys. 137, 22 (2012)

e + CH4 10−30eV The + CH4 10−30eV Th

952. M. Vinodkumar, M. BarotScattering of N2O on electron impact over an extensive energy range (0.1 eV-2000 eV)J. Chem. Phys. 137, 74311 (2012)

e + N2O 0.1−2000eV Th

953. A. Senftleben, T. Pflueger, X. Ren, B. Najjari, A. Dorn, J. UllrichTuning the internuclear distance in ionization of H-2J. Phys. B 45, 21001 (2012)

e + H2 0−360 Deg. Th

954. S. Harrison, J. TennysonElectron collisions with the CN radical: bound states and resonancesJ. Phys. B 45, 35204 (2012)

e + CN 0−10eV The + CN 0−10eV Th

955. M. L. deSanctis, M. F. Politis, R. Vuilleumier, C. R. Stia, O. A. FojonLiquid water ionization by fast electron impact: a multiple differential study for the1B(1) orbitalJ. Phys. B 45, 45206 (2012)

e + H2O 0−360 Deg. The + H2O 0−360 Deg. Th

956. S. D. Loch, C. P. Ballance, D. Wu, S. A. Abdel-Naby, M. S. PindzolaElectron-impact ionization of AlJ. Phys. B 45, 65201 (2012)

e + Al 0−30eV Th

229

957. M. Sahlaoui, M. BouamoudElectron impact single ionization of the water molecule in the second BornapproximationJ. Phys. B 45, 85201 (2012)

e + H2O 0−360 Deg. The + H2O 0−360 Deg. Th

958. X. Liu, D. E. ShemanskyNondissociative electron and photon ionization cross sections of molecular hydrogenand deuteriumJ. Phys. B 45, 95203 (2012)

P + H2 16−3000eV The + D2 16−3000eV The + H2 16−3000eV ThP + D2 16−3000eV Th

959. H. Kato, K. Anzai, T. Ishihara, M. Hoshino, F. Blanco, G. Garcia, P. Limao-Vieira, M. J.Brunger, S. J. Buckman, H. TanakaA study of electron interactions with silicon tetrafluoride: elastic scattering andvibrational excitation cross sectionsJ. Phys. B 45, 95204 (2012)

e + SiF4 1.5−200eV The + SiF4 1.5−200eV Th

960. C. C. Montanari, J. E. MiragliaAntiproton, proton and electron impact multiple ionization of rare gasesJ. Phys. B 45, 105201 (2012)

e + Xe 20−1E4 keV The + Kr 20−1E4 keV The + Ar 20−1E4 keV The + Ne 20−1E4 keV Th

961. C. Li, S. Casagrande, A. Lahmam-Bennani, A. NajaIdentification of first order and non-first order contributions in the (e,3-1e) and (e,3e)double ionization of molecular nitrogenJ. Phys. B 45, 135201 (2012)

e + N2 0−360 Deg. The + N2 0−360 Deg. Th

962. S. Harrison, J. Tennyson, A. FaureCalculated electron impact spin-coupled rotational cross-sections for (2S+1)Sigma(+)linear molecules: CN as an exampleJ. Phys. B 45, 175202 (2012)

e + CN 0.1−4eV Th

963. L. Hargreaves, K. Ralphs, G. Serna, M. A. Khakoo, C. Winstead, V. McKoyExcitation of the (a)over-tilde B-3(1) and (A)over-tilde B-1(1) states of H2O by low-energy electron impactJ. Phys. B 45, 201001 (2012)

e + H2O 9−20eV Th

964. M. S. Pindzola, S. A. Abdel-Naby, J. Colgan, A. DornPentuple energy and angle differential cross sections for the electron-impact doubleionization of heliumJ. Phys. B 45, 225201 (2012)

230

e + He 9eV The + He 9eV Th

965. A. A. Illarionov, A. D. StaufferCalculation of non-coplanar electron-impact ionization of xenonJ. Phys. B 45, 225202 (2012)

e + Xe 1−35eV Th

966. J. N. Bull, P. W. Harland, C. ValianceAbsolute Total Electron Impact Ionization Cross-Sections for Many-Atom Organic andHalocarbon SpeciesJ. Phys. Chem. A 116, 767 (2012)

e + C2H4O 0−300eV E/T

967. T. L. Phan, B. H. JeonDetermination of Electron Collision of Cross-Sections for the H-2 Molecule for PlasmaDischarge SimulationJ. Phys. Soc. Japan 81, 104501 (2012)

e + H2 0.01−1000eV Th

968. H. Elabidi, N. BenNessib, S. Sahal-BrechotElectron impact broadening of Si IV spectral lines: Comparison with recentexperimentsJ. Quant. Spectrosc. Radiat. Transfer 113, 1606 (2012)

e + Si3+ 0−20E4 K Th

969. M. F. R. Grieve, C. A. RamsbottomElectron-impact excitation of Sc ii: collision strengths and effective collision strengthsfor fine-structure transitionsMon. Not. R. Astron. Soc. 424, 2461 (2012)

e + Sc+ 1E1−1E5 K Th

970. P. WangELECTRON IMPACT DISSOCIATIVE IONIZATION OF NITROSYL CHLORIDEMod. Phys. Lett. B 26, 1250065 (2012)

e + NOCl 200 eV Th

971. R. Dey, A. C. Roy, C. DalCappelloFivefold differential cross sections for the ionization of aligned hydrogen molecule byelectron and positron impactNucl. Instrum. Methods Phys. Res. B 271, 82 (2012)

e + H2 200 eV The + H2 200 eV Th

972. P. V. GrujicClassical theory of atomic collisions - The first hundred yearsNucl. Instrum. Methods Phys. Res. B 279, 44 (2012)

e + H 0−20eV Th

973. S. D. Tosic, V. Pejcev, D. Sevic, R. P. McEachran, A. D. Stauffer, B. P. MarinkovicAbsolute differential cross sections for electron excitation of silver at small scatteringanglesNucl. Instrum. Methods Phys. Res. B 279, 53 (2012)

231

e + Ag 10−100eV The + Ag 10−100eV Th

974. K. HoufekResonant inelastic collisions of electrons with diatomic moleculesNucl. Instrum. Methods Phys. Res. B 279, 71 (2012)

e + HBr 0.2−1eV The + HCl 0.2−1eV Th

975. S. J. Ward, J. ShertzerHyperspherical hidden crossing method applied to Ps(1s)-formation in low energye(+)-H, e(+)-Li and e(+)-Na collisionsNew J. Phys. 14, 25003 (2012)

e + Li 6−10eV,0−2eV The + H 6−10eV,0−2eV Th

976. R. D. DuBoisDoubly and triply differential ionization measurements using femtoamp beams ofpositrons and electronsNew J. Phys. 14, 25004 (2012)

e + N2 250eV Exp

977. J. Annaloro, V. Morel, A. Bultel, P. OmalyGlobal rate coefficients for ionization and recombination of carbon, nitrogen, oxygen,and argonPhys. Plasmas 19, 73515 (2012)

e + N 3000−20000 K The + C 3000−20000 K The + Ar 3000−20000 K The + O 3000−20000 K The + N 3000−20000 K The + C 3000−20000 K The + Ar 3000−20000 K The + O 3000−20000 K Th

978. Y. Wang, L. Jiao, Y. ZhouSecond-order Born effect in coplanar doubly symmetric (e, 2e) collisions for sodiumPhys. Lett. A 376, 2122 (2012)

e + Na 6−60eV Th

979. R. Celiberto, R. K. Janev, D. ReiterState-to-state electron impact cross sections for BeH+ molecular ions in ITER-likefusion edge plasmas with Be wallsPlasma Phys. and Controlled Fusion 54, 35012 (2012)

e + BeH+ 1−1E4 eV Th

980. M. S. Pindzola, S. A. Abdel-Naby, J. A. Ludlow, F. Robicheaux, J. ColganElectron-impact ionization of Li-2 using a time-dependent close-coupling methodPhys. Rev. A 85, 12704 (2012)

e + Li2 5−25eV Th

981. Y. F. Wang, S. X. TianLow-energy electron collisions with formamide using the R-matrix methodPhys. Rev. A 85, 12706 (2012)

232

e + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVThe + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVThe + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVThe + NH2CHO 5−10eV,0−180eV,0−10eV,0−10eVTh

982. D. Wu, S. D. Loch, M. S. Pindzola, C. P. BallanceElectron-impact ionization of Al2+Phys. Rev. A 85, 12711 (2012)

e + Al2+ 20−200eV Th

983. G. Purohit, P. Singh, V. Patidar, Y. Azuma, K. K. SudEffects of target polarization and postcollision interaction on the electron-impact singleionization of Ne(2p), Ar(3p), and Na(3s) atomsPhys. Rev. A 85, 22714 (2012)

e + Na 5−50eV The + Ar 5−50eV The + Ne 5−50eV The + Na 5−50eV The + Ar 5−50eV The + Ne 5−50eV Th

984. X. Ren, T. Pflueger, J. Ullrich, O. Zatsarinny, K. Bartschat, D. H. Madison, A. DornLow-energy electron-impact ionization of argon: Three-dimensional cross sectionPhys. Rev. A 85, 32702 (2012)

e + Ar 3−15eV The + Ar 3−15eV Th

985. O. Zatsarinny, K. BartschatNonperturbative treatment of electron-impact ionization of Ar(3p)Phys. Rev. A 85, 32708 (2012)

e + Ar 195eV The + Ar 195eV Th

986. P. Bhatt, R. Singh, N. Yadav, R. ShankerRelative partial ionization cross sections of N2O under 10-25-keV electron impactPhys. Rev. A 85, 34702 (2012)

e + N2O 10−25keV Exp

987. K. M. Dunseath, M. Terao-DunseathComment on Near-threshold behavior of electron-impact excitation of He+(2s) andHe+ (2p)Phys. Rev. A 85, 36701 (2012)

e + He+ 40−46eV Th

988. M. J. Berrington, C. J. Bostock, D. V. Fursa, I Bray, R. P. McEachran, A. D. StaufferCalculations of electron scattering from cadmiumPhys. Rev. A 85, 42708 (2012)

e + Cd 3−85eV Th

989. L. R. Hargreaves, C. Campbell, M. A. Khakoo, O. Zatsarinny, K. BartschatUnusual angular momentum transfer in electron-impact excitation of neonPhys. Rev. A 85, 50701 (2012)

e + Ne 25eV E/T

233

990. S. Kaur, K. L. BalujaElectron-impact study of an NCO molecule using the R-matrix methodPhys. Rev. A 85, 52701 (2012)

e + NCO 0−10eV,10−5000eV,0−10eV The + NCO 0−10eV,10−5000eV,0−10eV The + NCO 0−10eV,10−5000eV,0−10eV Th

991. H. R. J. Walters, C. T. WhelanIonization of He by C6+, C-6-, e(-), and e(+)Phys. Rev. A 85, 62701 (2012)

hν + He 1keV,100MeV The + He 1keV,100MeV Thhν + He 1keV,100MeV The + He 1keV,100MeV Th

992. Z. Zhang, X. Shan, E. Wang, X. ChenEjected-electron spectroscopy of autoionizing resonances of helium excited by fast-electron impactPhys. Rev. A 85, 62702 (2012)

e + He 250−2000eV Exp

993. C. P. Malone, P. V. Johnson, X. Liu, B. Ajdari, I. Kanik, M. A. KhakooIntegral cross sections for the electron-impact excitation of the b (1)Pi(u), c(3)(1)Pi(u), o(3) (1)Pi(u), b ’ (1)Sigma(+)(u), c ’(4) (1)Sigma(+)(u), G (3)Pi(u), and F(3)Pi(u) states of N-2Phys. Rev. A 85, 62704 (2012)

e + N2 17.5−100eV Th

994. R. F. daCosta, M. H. F. Bettega, M. A. P. Lima, M. C. A. Lopes, L. R. Hargreaves, G. Serna, M.A. KhakooElectronic excitation of gas-phase furan molecules by electron impactPhys. Rev. A 85, 62706 (2012)

e + C4H4O 0−30eV E/Te + C4H4O 0−30eV E/Te + C4H4O 0−30eV E/T

995. O. Zatsarinny, K. BartschatNonperturbative B-spline R-matrix-with-pseudostates calculations for electron-impactionization of heliumPhys. Rev. A 85, 62709 (2012)

e + He 20−500eV The + He 20−500eV Th

996. O. Zatsarinny, K. BartschatLarge-scale pseudostate calculations for electron scattering from neon atomsPhys. Rev. A 85, 62710 (2012)

e + Ne 0.1−200eV The + Ne 0.1−200eV The + Ne 0.1−200eV The + Ne 0.1−200eV Th

997. A. Laricchiuta, G. Capitta, R. Celiberto, M. CapitelliElectron-impact-induced allowed transitions in Cs-2Phys. Rev. A 85, 62713 (2012)

234

e + Cs2 0−20eV Th

998. D. H. Kwon, D. W. SavinTheoretical electron-impact-ionization cross section for Fe11+ forming Fe12+Phys. Rev. A 86, 22701 (2012)

e + Fe11+ 300−2500eV Th

999. I. Linert, M. ZubekElastic electron scattering and vibrational excitation of isoxazole molecules in theenergy range from 2 to 20 eVPhys. Rev. A 86, 22708 (2012)

e + C3H3NO 2−20eV Expe + C3H3NO 2−20eV Expe + C3H3NO 2−20eV Exp

1000. T. Das, L. Sharma, R. Srivastava, A. D. StaufferElectron-impact excitation of zinc and ytterbium atomsPhys. Rev. A 86, 22710 (2012)

e + Yb 10−100eV The + Zn 10−100eV The + Yb 10−100eV The + Zn 10−100eV Th

1001. Z. W. Wu, C. Z. Dong, J. JiangDegrees of polarization of the two strongest 5 f -¿ 3d lines following electron-impactexcitation and dielectronic recombination processes of Cu-like to Se-like gold ionsPhys. Rev. A 86, 22712 (2012)

e + Au49+ 100−10000eV The + Au48+ 100−10000eV The + Au47+ 100−10000eV The + Au46+ 100−10000eV The + Au45+ 100−10000eV The + Au50+ 100−10000eV Th

1002. O. Zatsarinny, K. BartschatElectron-impact excitation of neon at intermediate energiesPhys. Rev. A 86, 22717 (2012)

e + Ne 10−300eV The + Ne 10−300eV Th

1003. J. S. Rajvanshi, K. L. BalujaElectron-impact study of the B-2 molecule using the R-matrix methodPhys. Rev. A 86, 32704 (2012)

e + B2 300−30000K The + B2 300−30000K The + B2 300−30000K Th

1004. S. P. Limandri, M. A. Z. Vasconcellos, R. Hinrichs, J. C. TrincavelliExperimental determination of cross sections for K-shell ionization by electron impactfor C, O, Al, Si, and TiPhys. Rev. A 86, 42701 (2012)

e + Ti 2.5−25keV Expe + Si 2.5−25keV Expe + Al 2.5−25keV Expe + O 2.5−25keV Expe + C 2.5−25keV Exp

235

1005. D. A. Konovalov, D. V. Fursa, I. BrayJ-matrix calculation of electron-helium S-wave scattering. II. Single ionization andsingle excitationPhys. Rev. A 86, 52704 (2012)

e + He 19−24eV,25−60eV The + He 19−24eV,25−60eV Th

1006. R. Curik, P. Carsky, M. AllanVibrational excitation of cyclopropane by electron impact: An experimental test ofthe discrete-momentum-representation theory with density-functional-theoryapproximation of polarization and correlationPhys. Rev. A 86, 62709 (2012)

e + C3H6 5.5eV Expe + C3H6 5.5eV Exp

1007. X. Ren, T. Pflueger, S. Xu, J. Colgan, M. S. Pindzola, A. Senftleben, J. Ullrich, A. DornStrong Molecular Alignment Dependence of H-2 Electron Impact Ionization DynamicsPhys. Rev. Lett. 109, 123202 (2012)

e + H2 18eV The + H2 18eV Th

1008. I. Bray, D. V. Fursa, A. S. Kadyrov, A. T. Stelbovics, A. S. Kheifets, A. M. MukhamedzhanovElectron- and photon-impact atomic ionisationPhys. Rep. 520, 135 (2012)

e + He 1−1000eV The + H 1−1000eV The + He 1−1000eV The + H 1−1000eV Th

1009. M. R. Talukder, M. Shahjahan, M. A. UddinElectron impact double ionization cross-sections of heavy elementsPhys. Scr. 85, 15301 (2012)

e + U 10−1E6eV The + Ba2+ 10−1E6eV The + Cs+ 10−1E6eV The + Xe4+ 10−1E6eV The + In 10−1E6eV The + Sb+ 10−1E6eV The + Bi+ 10−1E6eV The + Ag 10−1E6eV The + Mo3+ 10−1E6eV The + Rb+ 10−1E6eV The + Kr4+ 10−1E6eV The + Ga 10−1E6eV The + Pb 10−1E6eV The + Ni3+ 10−1E6eV The + Fe6+ 10−1E6eV The + Ti5+ 10−1E6eV The + Sc+ 10−1E6eV The + Hg 10−1E6eV The + W6+ 10−1E6eV The + Sm6+ 10−1E6eV The + Pr3+ 10−1E6eV Th

236

1010. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Mg XI, Al XII, P XIV and S XVPhys. Scr. 85, 25305 (2012)

e + S14+ 130−550 RYD The + P13+ 130−550 RYD The + Al11+ 130−550 RYD The + Mg10+ 130−550 RYD Th

1011. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Cl XVI, K XVIII, Ca XIX and Sc XXPhys. Scr. 85, 25306 (2012)

e + Ca18+ 359−900 RYD The + K17+ 359−900 RYD The + Cl15+ 359−900 RYD The + Sc19+ 359−900 RYD Th

1012. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Ti XXI, V XXII, Cr XXIII and Mn XXIVPhys. Scr. 85, 65301 (2012)

e + Mn23+ 500−1200 RYD The + Cr22+ 500−1200 RYD The + V21+ 500−1200 RYD The + Ti20+ 500−1200 RYD Th

1013. H. Elabidi, S. Sahal-Brechot, N. BenNessibFine structure collision strengths for S VII linesPhys. Scr. 85, 65302 (2012)

e + S6+ 20−120 RYD Th

1014. T. Das, L. Sharma, R. SrivastavaElectron impact excitation of the M-shell electrons from Zn-like through Co-liketungsten ionsPhys. Scr. 85, 35301 (2012)

e + W44+ 0−50keV The + W47+ 0−50keV The + W46+ 0−50keV The + W45+ 0−50keV Th

1015. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Kr XXXVPhys. Scr. 85, 35302 (2012)

e + Kr34+ 1E5.4−1E8.1 K Th

1016. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inBe-like Ti XIXPhys. Scr. 85, 55301 (2012)

e + Ti18+ 100−1100 RYD Th

237

1017. V. Laporta, C. M. Cassidy, J. Tennyson, R. CelibertoElectron-impact resonant vibration excitation cross sections and rate coefficients forcarbon monoxidePlasma Sources Sci. Technol. 21, 45005 (2012)

e + Co 1−10eV Th

1018. V. Laporta, R. Celiberto, J. M. WadehraTheoretical vibrational-excitation cross sections and rate coefficients forelectron-impact resonant collisions involving rovibrationally excited N-2 and NOmoleculesPlasma Sources Sci. Technol. 21, 55018 (2012)

e + NO 0.1−100eV The + N2 0.1−100eV Th

1019. S. Abdel-Naby, D. Nikolic, T. W. Gorczyca, K. T. Korista, N. R. BadnellDielectronic recombination data for dynamic finite-density plasmas XIV. Thealuminum isoelectronic sequenceAstron. Astrophys. 537, A40 (2012)

e + S3+ 0.1−1000eV The + Zn17+ 0.1−1000eV The + Cu16+ 0.1−1000eV The + Ni15+ 0.1−1000eV The + Co14+ 0.1−1000eV The + Mn12+ 0.1−1000eV The + Cr11+ 0.1−1000eV The + V10+ 0.1−1000eV The + Ti9+ 0.1−1000eV The + Sc8+ 0.1−1000eV The + Ca7+ 0.1−1000eV The + K6+ 0.1−1000eV The + Ar5+ 0.1−1000eV The + Cl4+ 0.1−1000eV The + P2+ 0.1−1000eV The + Si+ 0.1−1000eV Th

1020. E. Vigren, V. Zhaunerchyk, M. Hamberg, M. Kaminska, J. Semaniak, M. afUgglas, M. Larsson,R. D. Thomas, W. D. GeppertREASSESSMENT OF THE DISSOCIATIVE RECOMBINATION OF N2H+ ATCRYRINGAstrophys. J. 757, 34 (2012)

e + N2H+ 10−1000 K Exp

1021. R. D. Thomas, I. Kashperka, E. Vigren, W. D. Geppert, M. Hamberg, M. Larsson, M. afUgglas,V. Zhaunerchyk, N. Indriolo, K. Yagi, S. Hirata, B. J. McCallDISSOCIATIVE RECOMBINATION OF VIBRATIONALLY COLD CH3+ ANDINTERSTELLAR IMPLICATIONSAstrophys. J. 758, 55 (2012)

e + CH3+ 1E−1−10eV Exp

1022. M. Hahn, D. Bernhardt, M. Lestinsky, A. Mueller, S. Schippers, A. Wolf, D. W. SavinSTORAGE RING MEASUREMENT OF ELECTRON IMPACT IONIZATION FORMg7+ FORMING Mg8+ (vol 712, pg 1166, 2010)Astrophys. J. 761, 77 (2012)

e + Mg7+ 250−1500eV Exp

238

1023. M. Hahn, D. Bernhardt, M. Grieser, C. Krantz, M. Lestinsky, A. Mueller, O. Novotny, R.Repnow, S. Schippers, A. Wolf, D. W. SavinSTORAGE RING CROSS SECTION MEASUREMENTS FOR ELECTRONIMPACT IONIZATION OF Fe11+ FORMING Fe12+ AND Fe13+ (vol 729, pg 76,2011)Astrophys. J. 761, 78 (2012)

e + Fe11+ 300−2000eV Exp

1024. M. Hahn, M. Grieser, C. Krantz, M. Lestinsky, A. Mueller, O. Novotny, R. Repnow, S. Schippers,A. Wolf, D. W. SavinSTORAGE RING CROSS-SECTION MEASUREMENTS FOR ELECTRONIMPACT IONIZATION OF Fe12+ FORMING Fe13+ AND Fe14+ (vol 735, pg 105,2011)Astrophys. J. 761, 79 (2012)

e + Fe12+ 350−1910eV Exp

1025. D.-H. Zhang, Y.-L. Shi, J. Jiang, C.-Z. Dong, F. KoikeKLL dielectronic recombination process of He-like to O-like xenon ionsChin. Phys. B 21, 13402 (2012)

e + Xe52+ 20−22.4keV The + Xe51+ 20−22.4keV The + Xe50+ 20−22.4keV The + Xe49+ 20−22.4keV The + Xe48+ 20−22.4keV The + Xe47+ 20−22.4keV The + Xe46+ 20−22.4keV Th

1026. Y. Wang, Y.-J. Zhou, L.-G. JiaoStudy of (e, 2e) process on potassium at 6 eV-60 eV above threshold in a second-orderBorn approximationChin. Phys. B 21, 83401 (2012)

e + K 6−60eV Th

1027. L.-X. Zhou, Y.-G. Yan(e, 2e) triple-differential cross sections for Ag+(4p, 4s) in coplanar symmetric geometryChin. Phys. B 21, 93401 (2012)

e + Ag+ 50−1000eV Th

1028. X.-L. Hu, Y.-Z. Qu, S.-B. Zhang, Y. ZhangDielectronic recombination and resonant transfer excitation processes for helium-likekryptonChin. Phys. B 21, 103401 (2012)

e + Kr34+ 8−13keV Th

1029. O. Sasic, S. Dujko, T. Makabe, Z. L. PetrovicA set of cross sections and transport coefficients for electrons in HBrChem. Phys. 398, 154 (2012)

e + HBr 0.001−1E4eV The + HBr 0.001−1E4eV The + HBr 0.001−1E4eV Th

1030. Y. Sugioka, T. TakayanagiA practical approach to temperature effects in dissociative electron attachment crosssections using local complex potential theoryChem. Phys. 405, 189 (2012)

239

e + CF3Cl 300−800K The + H2O 300−800K Th

1031. J. Troe, T. M. Miller, A. A. ViggianoCommunication: Revised electron affinity of SF6 from kinetic dataJ. Chem. Phys. 136, 121102 (2012)

e + SF6 1−2eV Th

1032. N. B. Ram, E. KrishnakumarDissociative electron attachment resonances in ammonia: A velocity slice imagingbased studyJ. Chem. Phys. 136, 164308 (2012)

e + NH3 0−20eV Exp

1033. S. A. Haughey, T. A. Field, J. Langer, N. S. Shuman, T. M. Miller, J. F. Friedman, A. A. ViggianoDissociative electron attachment to C2F5 radicalsJ. Chem. Phys. 137, 54310 (2012)

e + C2F5 300−600K Exp

1034. S. L. GubermanSpectroscopy above the ionization threshold: Dissociative recombination of the groundvibrational level of N-2(+)J. Chem. Phys. 137, 74309 (2012)

e + N2+ 0.001−0.1eV Th

1035. S. T. Pratt, C. JungenThe isotope dependence of dissociative recombination via the indirect mechanismJ. Chem. Phys. 137, 174306 (2012)

e + D3O 0.0001−1eV Expe + H3O 0.0001−1eV Expe + ND4

+ 0.0001−1eV Expe + NH4

+ 0.0001−1eV Expe + N2D

+ 0.0001−1eV Expe + N2H

+ 0.0001−1eV Exp

1036. P. Palihawadana, J. P. Sullivan, S. J. Buckman, M. J. BrungerElectron scattering from pyrazine: Elastic differential and integral cross sectionsJ. Chem. Phys. 137, 204307 (2012)

e + C4H4N2 3−50eV Exp

1037. O. Chuluunbaatar, A. A. Gusev, B. B. JoulakianThe correlated two-centre double continuum and the double ionization of H-2 and N-2by fast electron impactJ. Phys. B 45, 15205 (2012)

e + N2 500−600eV The + H2 500−600eV Th

1038. C. P. Ballance, D. C. Griffin, S. D. Loch, N. R. BadnellDielectronic recombination of Au20+: a theoretical description of the resonances atlow electron energiesJ. Phys. B 45, 45001 (2012)

e + Au20+ 1−1000eV Th

240

1039. Z. Felfli, A. Z. Msezane, D. SokolovskiSlow electron elastic scattering cross sections for In, Tl, Ga and At atomsJ. Phys. B 45, 189501 (2012)

e + At 0.01−10eV The + Ga 0.01−10eV The + Tl 0.01−10eV The + In 0.01−10eV Th

1040. A. L. Harris, M. Foster, C. Ryan-Anderson, J. L. Peacher, D. H. MadisonProjectile interactions in theoretical triple differential cross sections for simultaneousexcitation-ionization of helium (vol 41, 135203, 2008)J. Phys. B 45, 59501 (2012)

e + He 110−270eV The + He 110−270eV The + He 110−270eV Th

1041. U. I. Safronova, A. S. Safronova, P. BeiersdorferExcitation energies, radiative and autoionization rates, dielectronic satellite lines, anddielectronic recombination rates for excited states of Yb-like WJ. Phys. B 45, 85001 (2012)

e + W4+ 0.1−5000eV Th

1042. V. I. Kelemen, Y. RemetaCritical minima and spin polarization in the elastic electron scattering by the mercuryatomsJ. Phys. B 45, 185202 (2012)

e + Hg 0.1−2000eV The + Hg 0.1−2000eV The + Hg 0.1−2000eV Th

1043. D. H. Jakubassa-Amundsen, R. BardayThe Sherman function in highly relativistic elastic electron-atom scatteringJournal Of Physics G Nuclear And Particle Physics 39, 25102 (2012)

e + U 20−200MeV The + Pb 20−200MeV The + Zn 20−200MeV Th

1044. C. Champion, S. Incerti, H. N. Tran, Z. ElBitarElectron and proton elastic scattering in water vapourNucl. Instrum. Methods Phys. Res. B 273, 98 (2012)

e + H2O 0.01−1E4eV Th

1045. V. StancalieContribution of near threshold states to dielectronic recombination in recombiningplasma with Li-like Al ionsNucl. Instrum. Methods Phys. Res. B 279, 147 (2012)

e + Al10+ 0−0.1 RYD Th

1046. B. W. Li, G. O’Sullivan, Y. B. Fu, C. Z. DongDielectronic recombination of Pd-like gadoliniumPhys. Rev. A 85, 012712 (2012)

e + Gd18+ 1−50000eV Th

241

1047. M. Vandevraye, C. Drag, C. BlondelElectron affinity of selenium measured by photodetachment microscopyPhys. Rev. A 85, 015401 (2012)

e + Se 0.4-0.8 cm−1 Exp

1048. U. I. Safronova, A. S. SafronovaDielectronic recombination of Er-like tungstenPhys. Rev. A 85, 032507 (2012)

e + W6+ 0.1−575eV Th

1049. A. Larson, M. Stenrup, A. E. OrelRole of the direct mechanism in dissociative recombination of HCO+ and HOC+Phys. Rev. A 85, 042702 (2012)

e + HOC+ 0−10eV The + HCO+ 0−10eV Th

1050. M. Hahn, D. Bernhardt, M. Grieser, C. Krantz, M. Lestinsky, A. Mueller, O. Novotny, R. Repnow,S. Schippers, A. Wolf, D. W. SavinElectron-impact-ionization measurements using hyperfine-assisted state preparation ofground-state berylliumlike sulfurPhys. Rev. A 85, 042713 (2012)

e + S12+ 500−3000eV Exp

1051. B. W. Li, G. O’Sullivan, Y. B. Fu, C. Z. DongDielectronic recombination of Rh-like Gd and WPhys. Rev. A 85, 052706 (2012)

e + Gd19+ 1−5000eV The + W29+ 1−5000eV Th

1052. N. R. Badnell, C. P. Ballance, D. C. Griffin, M. O’MullaneDielectronic recombination of W20+ (4d(10)4 f(8)): Addressing the half-open f shellPhys. Rev. A 85, 052716 (2012)

e + W20+ 1−1000eV E/T

1053. C. J. Bostock, D. V. Fursa, I. BrayRelativistic convergent close-coupling method calculation of the spin polarization ofelectrons scattered elastically from zinc and mercuryPhys. Rev. A 85, 062707 (2012)

e + Hg 1−14eV The + Zn 1−14eV Th

1054. R. Janeckova, O. May, J. FedorDissociative electron attachment to methylacetylene and dimethylacetylene:Symmetry versus proximityPhys. Rev. A 86, 052702 (2012)

e + C 1−6eV Exp

1055. C. J. Bostock, D. V. Fursa, I. BrayRelativistic convergent close-coupling calculation of spin asymmetries for electron-thallium scatteringPhys. Rev. A 86, 062701 (2012)

e + Ta 4−180eV Th

242

1056. D. J. Haxton, C. H. GreeneEstimates of rates for dissociative recombination of NO2+ + e(-) via variousmechanismsPhys. Rev. A 86, 062712 (2012)

e + NO2+ 0−10eV Th

1057. N. Douguet, A. E. Orel, C. H. Greene, V. KokooulineDissociative Recombination of Highly Symmetric Polyatomic IonsPhys. Rev. Lett. 108, 023202 (2012)

e + CH3+ 0.0001−1eV Th

e + H3O+ 0.0001−1eV Th

1058. Z. Hu, X. Han, Y. Li, D. Kato, X. Tong, N. NakamuraExperimental Demonstration of the Breit Interaction which Dominates the AngularDistribution of X-ray Emission in Dielectronic RecombinationPhys. Rev. Lett. 108, 073002 (2012)

e + Au76+ 45eV Exp

1059. P. Lukac, O. Mikus, I. Morva, Z. Zabudla, J. Trnovec, M. Morvova, K. HenselDependence of the dissociative recombination coefficient of molecular ions Kr-2(+)with electrons on the electron and gas temperaturesPlasma Sources Sci. Technol. 21, 065002 (2012)

e + Kr2+ 300−19000K Exp

1060. M. Honigmann, R. J. Buenker, H. P. LiebermannComplex configuration interaction calculations of the cross section for thedissociative electron attachment process e(-)+F-2 -¿ F-2(-) -¿ F+F- using thecomplex basis function methodJ. Comput. Phys. 33, 355 (2012)

e + F2− 0.01−1.4eV Th

e + F2 0.01−1.4eV The + F2

− 0.01−1.4eV The + F2 0.01−1.4eV Th

1061. H. Kreckel, A. Petrignani, O. Novotny, K. Crabtree, H. Buhr, B. J. McCall, A. WolfStorage ring measurements of the dissociative recombination of H-3(+)Phil. Trans. R. Soc. A 370, 5088 (2012)

e + H3+ 0.00001−1000eV Exp

1062. M. LarssonDissociative recombination of H-3(+): 10 years in retrospectPhil. Trans. R. Soc. A 370, 5118 (2012)

e + H3+ 0.00001−10eV Exp

1063. B. Zhou, M. Y. Zheng, D. Y. WenThe second Born approximation of electron argon elastic scattering in a bichromaticlaser fieldPramana 78, 399 (2012)

e + Ar 9.5−19.5eV Th

1064. B. O’Dwyer, G. DelZanna, N. R. Badnell, H. E. Mason, P. J. StoreyAtomic data for the X-ray lines of Fe VIII and Fe IXAstron. Astrophys. 537, A22 (2012)

243

e + Fe8+ 0−80 RYD The + Fe7+ 0−80 RYD Th

1065. G. DelZanna, P. J. Storey, N. R. Badnell, H. E. MasonAtomic data for astrophysics: Fe x soft X-ray linesAstron. Astrophys. 541, A90 (2012)

e + Fe9+ 10−60 RYD Th

1066. G. DelZanna, P. J. Storey, N. R. Badnell, H. E. MasonAtomic data for astrophysics: Fe XII soft X-ray linesAstron. Astrophys. 543, A139 (2012)

e + Fe11+ 10−60 RYD Th

1067. G. DelZanna, P. J. StoreyAtomic data for astrophysics: Fe XIII soft X-ray linesAstron. Astrophys. 543, A144 (2012)

e + Fe12+ 10−50 RYD Th

1068. X. M. Tan, X. M. LiuTotal Electron Scattering Cross Sections of SiH4 and PH3 Molecules in the EnergyRange from 10 eV to 5000 eVChin. J. Phys. 50, 573 (2012)

e + PH3 10−5000eV The + SiH4 10−5000eV Th

1069. X. M. Tan, G. ZhaoTotal cross sections for electron scattering from fluoromethanes: A revised additivityrule methodChin. Phys. B 21, 063402 (2012)

e + CH3F 1E2−2E3 eV The + CH2F2 1E2−2E3 eV The + CF3H 1E2−2E3 eV The + CF4 1E2−2E3 eV Th

1070. G. L. C. deSouza, A. S. dosSantos, R. R. Lucchese, L. E. Machado, L. M. Brescansin, H. V. Manini,I. Iga, M. -T. LeeTheoretical investigation on electron scattering by benzene in the intermediate-energyrangeChem. Phys. 393, 19 (2012)

e + C6H6 20−500eV Th

1071. S. Pancheshnyi, S. Biagi, M. C. Bordage, G. J. M. Hagelaar, W. L. Morgan, A. V. Phelps, L. C.PitchfordThe LXCat project: Electron scattering cross sections and swarm parameters for lowtemperature plasma modelingChem. Phys. 398, 148 (2012)

e + Ar 40−1000Td Th

1072. M. C. Zammit, D. V. Fursa, I. BrayElectron scattering in a helium Debye plasmaChem. Phys. 398, 214 (2012)

244

e + He 20−1000eV The + He 20−1000eV The + He 20−1000eV The + He 20−1000eV Th

1073. D. B. Jones, S. M. Bellm, P. Limao-Vieira, M. J. BrungerLow-energy electron scattering from pyrimidine: Similarities and differences withbenzeneChem. Phys. 535, 30 (2012)

e + C4H4N2 15−30eV Expe + C4H4N2 15−30eV Expe + C4H4N2 15−30eV Exp

1074. M. Kitajima, M. Kurokawa, T. Kishino, K. Toyoshima, T. Odagiri, H. Kato, K. Anzai, M. Hoshino,H. Tanaka, K. ItoUltra-low-energy electron scattering cross section measurements of Ar, Kr and Xeemploying the threshold photoelectron sourceEur. Phys. J. D 66, 130 (2012)

e + Xe 0.005−20eV Expe + Kr 0.005−20eV Expe + Ar 0.005−20eV Expe + Xe 0.005−20eV Expe + Kr 0.005−20eV Expe + Ar 0.005−20eV Exp

1075. M. -T. Lee, G. L. C. deSouza, L. E. Machado, L. M. Brescansin, A. S. dosSantos, R. R. Lucchese,R. T. Sugohara, M. G. P. Homem, I. P. Sanches, I. IgaElectron scattering by methanol and ethanol: A joint theoretical-experimentalinvestigationJ. Chem. Phys. 136, 114311 (2012)

e + C2H5OH 1−1000eV E/Te + CH3OH 1−1000eV E/T

1076. A. G. Sanz, M. C. Fuss, F. Blanco, F. Sebastianelli, F. A. Gianturco, G. GarciaElectron scattering cross sections from HCN over a broad energy range (0.1-10 000eV): Influence of the permanent dipole moment on the scattering processJ. Chem. Phys. 137, 124103 (2012)

e + HCN 0.1−10000eV The + HCN 0.1−10000eV Th

1077. A. V. Khrabrov, I. D. KaganovichElectron scattering in helium for Monte Carlo simulationsPhys. Plasmas 19, 093511 (2012)

e + He 0.1−1000eV Th

1078. H. Miyagi, T. Morishita, S. WatanabeElectron scattering and photoionization of one-electron diatomic moleculesPhys. Rev. A 85, 022708 (2012)

e + HeH2+ 10−150eV The + H2

+ 10−150eV Th

1079. V. Gedeon, S. Gedeon, V. Lazur, E. Nagy, O. Zatsarinny, K. BartschatElectron scattering from siliconPhys. Rev. A 85, 022711 (2012)

245

e + Si 0−60eV The + Si 0−60eV The + Si 0−60eV Th

1080. R. P. McEachran, M. VosLarge-angle scattering of energetic electrons from Xe: A combined theoretical andexperimental approachPhys. Rev. A 85, 032703 (2012)

e + Xe 500,750eV E/T

1081. A. R. Lopes, M. H. F. Bettega, S. d’A. SanchezResonances in low-energy-electron scattering by nitro compoundsPhys. Rev. A 85, 044701 (2012)

e + C3H7NO2 0−8eV The + C2H5NO2 0−8eV The + C2H3NO2 0−8eV Th

1082. M. Vinodkumar, C. Limbachiya, A. Barot, N. MasonTheoretical total cross sections for e-SO2 scattering over a wide energy range (0.1-2000eV) revealing a 3.4-eV shape resonancePhys. Rev. A 86, 012706 (2012)

e + SO2 0.1−2000eV Th

1083. C. J. Bostock, D. V. Fursa, I. BrayNonperturbative electron-ion-scattering theory incorporating the Moller interactionPhys. Rev. A 86, 042709 (2012)

e + U91+ 100−120eV Th

1084. N. Morrison, C. H. GreeneLaser-assisted electron-argon scattering at small anglesPhys. Rev. A 86, 053422 (2012)

e + Ar Th

1085. K. S. JassimThe electron scattering form factor of B-10, S-32 and Ca-48 nucleiPhys. Scr. 86, 035202 (2012)

e + Kr34+ 1000−3500eV Th

1086. K. L. Nixon, A. J. Murray, H. Chaluvadi, S. Amami, D. H. Madison, C. NingLow energy (e,2e) measurements of CH4 and neon in the perpendicular planeJ. Chem. Phys. 136, 94302 (2012)

e + Ne 0.5−50eV E/Te + CH4 0.5−50eV E/T

1087. I. I. Fabrikant, S. Caprasecca, G. A. Gallup, J. D. GorfinkielElectron attachment to molecules in a cluster environmentJ. Chem. Phys. 136, 184301 (2012)

e + CF3Cl 0−2.5 eV The + CF2Cl2 0−2.5 eV Th

1088. S. Xu, H. Chaluvadi, X. Ren, T. Pflueger, A. Senftleben, C. G. Ning, S. Yan, P. Zhang, J. Yang,X. Ma, J. Ullrich, D. H. Madison, A. DornLow energy (e, 2e) study from the 1t(2) orbital of CH4J. Chem. Phys. 137, 24301 (2012)

246

e + CH4 10−20eV E/Te + CH4 10−20eV E/T

1089. J. Troe, T. M. Miller, N. S. Shuman, A. A. ViggianoAnalysis by kinetic modeling of the temperature dependence of thermal electronattachment to CF3BrJ. Chem. Phys. 137, 24303 (2012)

e + CF3Br 100−20000K Th

1090. N. S. Shuman, T. M. Miller, A. A. ViggianoElectron attachment to fluorocarbon radicalsJ. Chem. Phys. 137, 214318 (2012)

e + C3F5 300−550K Expe + C2F3 300−550K Expe + CF2 300−550K Exp

1091. K. L. Nixon, A. J. MurrayMapping the xenon (e,2e) differential cross section from coplanar to perpendiculargeometriesPhys. Rev. A 85, 22716 (2012)

e + Xe 5−40eV Expe + Xe 5−40eV Exp

1092. J. N. Bull, M. Bart, C. Vallance, P. W. HarlandElectron-impact-ionization dynamics of five C-2 to C-4 perfluorocarbonsPhys. Rev. A 88, 62710 (2013)

e + C4 0−220 eV E/Te + C2 0−220 eV E/T

1093. E. Ghanbari-Adivi, R. Abdollahi-TadiA four-body approach to electron-impact single ionization of helium atomsEur. Phys. J. D 67, 266 (2013)

e + He 100−600eV Th

1094. D. H. Kwon, Y. S. Cho, Y. O. LeeElectron-impact ionization of W+ forming W2+Int. J. Mass Spectrom. 356, 7 (2013)

e + W2+ 10−1000 eV The + W+ 10−1000 eV Th

1095. M. C. Zammit, D. V. Fursa, I. BrayCalculations of electron scattering from H-2(+)Phys. Rev. A 88, 62709 (2013)

e + H2+ 0−1000eV Th

1096. Q. Fan, G. Jiang, L. Cao, W. Wang, S. DuCollision strengths for transitions of Ni XXIEur. Phys. J. D 67, 255 (2013)

e + Ni10+ 0−450eV Th

1097. J. C. Lower, E. Ali, S. Bellm, E. Weigold, A. Harris, C. G. Ning, D. MadisonExperimental and theoretical cross sections for molecular-frame electron-impactexcitation-ionization of D-2Phys. Rev. A 88, 62705 (2013)

247

e + D2 178 eV E/Te + D2 178 eV E/T

1098. R. Celiberto, R. K. Janev, V. Laporta, J. Tennyson, J. M. WadehraElectron-impact vibrational excitation of vibrationally excited H-2 molecules involvingthe resonant (2)Sigma(+)(g) Rydberg-excited electronic statePhys. Rev. A 88, 62701 (2013)

e + H2 0−100eV Th

1099. B. Goswami, U. Saikia, R. Naghma, B. AntonyElectron Impact Total Ionization Cross Sections for Plasma Wall Coating ElementsChin. J. Phys. 51, 1172 (2013)

e + Fe 5−2000eV The + Ti 5−2000eV The + B 5−2000eV The + Be 5−2000eV The + Li 5−2000eV Th

1100. H. Elabidi, S. Sahal-BrechotExcitation cross-sections by electron impact for O v and O vi levelsMon. Not. R. Astron. Soc. 436, 1452 (2013)

e + O5+ 1−140 RYD The + O4+ 1−140 RYD Th

1101. Y. Y. Qi, L. N. Ning, J. G. Wang, Y. Z. QuPlasma effect on fast-electron-impact-ionization from 2p state of hydrogen-like ionsPhys. Plasmas 20, 123301 (2013)

e + H 1E−6−10 A.U. Th

1102. D. P. Kilcrease, S. BrookesCorrection of the near threshold behavior of electron collisional excitationcross-sections in the plane-wave Born approximationHigh En. Dens. Phys. 9, 722 (2013)

e + He+ 40−1000eV The + C5+ 40−1000eV The + C3+ 40−1000eV Th

1103. Y. SmirnovExcitation of Even Configurations of a Nickel Atom Containing Nine 3d ElectronsOpt. Spectrosc. 115, 787 (2013)

e + Ni 50 eV Exp

1104. A. Kupliauskiene, G. KereviciusTheoretical study of the 4p(5)nln ’ l ’ autoionizing states of Rb excited by electronimpactPhys. Scr. 88, 65305 (2013)

e + Rb 0−400eV Th

1105. S. I. Lopatin, S. M. Shugurov, K. A. EmelyanovaHigh-temperature mass spectrometric determinations of relative ionizationcross-sections of gaseous TiO, TiO2, VO, VO2, YO, HfO and GeO moleculesRap. Comm. Mass. Spect. 27, 2338 (2013)

248

e + GeO 45−55eV Expe + HfO 45−55eV Expe + YO 45−55eV Expe + VO2 45−55eV Expe + VO 45−55eV Expe + TiO2 45−55eV Expe + TiO 45−55eV Exp

1106. M. Hoshino, H. Murai, H. Kato, M. J. Brunger, Y. Itikawa, H. TanakaElectron impact excitation of the low-lying 3s[3/2](1) and 3s ’[1/2](1) levels in neonfor incident energies between 20 and 300 eVJ. Chem. Phys. 139, 184301 (2013)

e + Ne 20−300eV Exp

1107. A. Borovik, A. Kupliauskiene, O. ZatsarinnyExcitation-autoionization cross section of alkali atoms by electron impactJ. Phys. B 46, 215201 (2013)

e + Li 10−600eV Expe + Cs 10−600eV Expe + Rb 10−600eV Expe + K 10−600eV Expe + Na 10−600eV Expe + Li 10−600eV Expe + Cs 10−600eV Expe + Rb 10−600eV Expe + K 10−600eV Expe + Na 10−600eV Exp

1108. M. S. Pindzola, S. D. Loch, A. BorovikJr, M. F. Gharaibeh, J. K. Rudolph, S. Schippers, A. MuellerElectron-impact ionization of moderately charged xenon ionsJ. Phys. B 46, 215202 (2013)

e + Xe12+ 100−1000eV The + Xe11+ 100−1000eV The + Xe17+ 100−1000eV The + Xe10+ 100−1000eV The + Xe16+ 100−1000eV The + Xe15+ 100−1000eV The + Xe14+ 100−1000eV The + Xe13+ 100−1000eV Th

1109. S. Harrison, A. Faure, J. TennysonCN excitation and electron densities in diffuse molecular cloudsMon. Not. R. Astron. Soc. 435, 3541 (2013)

e + CN 0−1000 K Th

1110. B. Goswami, R. Naghma, B. AntonyCalculations of electron collision and ionisation of rare gas dimersMol. Phys. 111, 3047 (2013)

e + Kr2 0−2000eV The + He2 0−2000eV The + Ar2 0−2000eV The + Ne2 0−2000eV The + He2 0−2000eV The + Kr2 0−2000eV The + Ar2 0−2000eV The + Ne2 0−2000eV Th

249

1111. M. U. Bug, E. Gargioni, H. Nettelbeck, W. Y. Baek, G. Hilgers, A. B. Rosenfeld, H. RabusIonization cross section data of nitrogen, methane, and propane for light ions andelectrons and their suitability for use in track structure simulationsPhys. Rev. E 88, 43308 (2013)

e + C3H8 10−10000eV The + N2 10−10000eV Th

1112. J. Lecointre, K. A. Kouzakov, D. S. Belic, P. Defrance, Y. V. Popov, V. P. ShevelkoMultiple ionization of C+, N+ and O+ ions by fast electron impactJ. Phys. B 46, 205201 (2013)

e + N+ 10−10000eV E/Te + C+ 10−10000eV E/Te + O+ 10−10000eV E/T

1113. D. Oubaziz, C. Champion, H. AouchicheElectron-induced double ionization of isolated water moleculesPhys. Rev. A 88, 42709 (2013)

e + H2O 50−500eV Th

1114. M. Hoshino, H. Mura, H. Kato, Y. Itikawa, M. J. Brunger, H. TanakaResolution of a significant discrepancy in the electron impact excitation of the3s[3/2](1) and 3s ’[1/2](1) low-lying electronic states in neonChem. Phys. Lett. 585, 33 (2013)


1115. S. y. Sun, X. f. Jia(e, 2e) Investigations of the Simultaneous Ionization and Excitation Helium to He+(n=2)Chin. J. Chem. Phys. 26, 576 (2013)

e + He 5.5−570eV The + He 5.5−570eV Th

1116. L. J. Liu, C. C. Jia, L. M. Zhang, J. J. Chen, Z. J. ChenThe effect of wave function orthogonality on the simultaneous ionization and excitationof heliumChin. Phys. B 22, 103401 (2013)

e + He 645−676eV The + He 645−676eV Th

1117. M. Dance, E. Palay, S. N. Nahar, A. K. PradhanFine-structure collision strengths and line ratios for [Ne v] in infrared and opticalsourcesMon. Not. R. Astron. Soc. 435, 1576 (2013)

e + Ne4+ 0−2.5 RYD Th

1118. A. K. F. Haque, I. Hossain, T. I. Talukder, M. Hasan, A. Uddin, A. K. Basak, B. C. Saha, F. B.MalikElectron impact ionization cross-section of K-shell and H- to Be-isoelectronic series:An empirical modelRadiat. Phys. Chem. 91, 50 (2013)

250

e + Au 0−1E8 keV The + Ne8+ 0−1E8 keV The + Ne7+ 0−1E8 keV The + Be+ 0−1E8 keV The + Li+ 0−1E8 keV The + Ag 0−1E8 keV The + Ne6+ 0−1E8 keV The + O6+ 0−1E8 keV The + Li 0−1E8 keV The + He+ 0−1E8 keV The + Cu 0−1E8 keV The + O4+ 0−1E8 keV The + N6+ 0−1E8 keV The + He 0−1E8 keV The + H 0−1E8 keV The + Ar 0−1E8 keV The + N4+ 0−1E8 keV The + N3+ 0−1E8 keV The + U90+ 0−1E8 keV The + U91+ 0−1E8 keV The + C4+ 0−1E8 keV The + C2+ 0−1E8 keV The + U89+ 0−1E8 keV The + U88+ 0−1E8 keV The + C 0−1E8 keV The + B4+ 0−1E8 keV The + U 0−1E8 keV The + Mo41+ 0−1E8 keV The + B2+ 0−1E8 keV The + B+ 0−1E8 keV Th

1119. R. Choubisa, M. JainOn the spin interplay of the ejected electrons in the relativistic electron impact K-shelldouble ionization of atomsJ. Phys. B 46, 185202 (2013)

e + Xe 540eV The + Mo 540eV The + Ca 540eV Th

1120. B. Goswami, R. Naghma, B. AntonyCross sections for electron collisions with NF3Phys. Rev. A 88, 32707 (2013)

e + NF3 1−5keV The + NF3 1−5keV Th

1121. M. Vojnovic, M. Popovic, M. M. Ristic, M. D. Vicic, G. B. PoparicRate coefficients for electron impact excitation of COChem. Phys. 423, 1 (2013)

e + Co 0−1000 Td Th

1122. A. N. Gomonai, Y. I. Hutych, A. I. GomonaiEmission cross sections for spectral lines transiting from the In2+ lower laser 4d(10)5pP-2(1/2,3/2) states excited by electron impact on the In+ ionNucl. Instrum. Methods Phys. Res. B 311, 37 (2013)

e + In+ 0−120eV Exp

251

1123. A. BorovikJr, M. F. Gharaibeh, P. M. Hillenbrand, S. Schippers, A. MuellerDetailed investigation of electron-impact single-ionization cross sections and plasmarate coefficients of N-shell tin ionsJ. Phys. B 46, 175201 (2013)

e + Sn7+ 0−1000eV E/Te + Sn13+ 0−1000eV E/Te + Sn6+ 0−1000eV E/Te + Sn12+ 0−1000eV E/Te + Sn5+ 0−1000eV E/Te + Sn11+ 0−1000eV E/Te + Sn4+ 0−1000eV E/Te + Sn10+ 0−1000eV E/Te + Sn9+ 0−1000eV E/Te + Sn8+ 0−1000eV E/T

1124. K. BartschatComputational methods for electron-atom collisions in plasma applicationsJ. Phys. D 46, 334004 (2013)

e + I 0−10eV The + Ar 0−10eV The + Ne 0−10eV The + He 0−10eV The + He 0−10eV The + Hg 0−10eV The + Kr 0−10eV The + I 0−10eV The + Ar 0−10eV The + Ne 0−10eV The + He 0−10eV The + Hg 0−10eV The + Kr 0−10eV The + I 0−10eV The + Ar 0−10eV The + Ne 0−10eV The + Hg 0−10eV The + He 0−10eV The + Hg 0−10eV The + Kr 0−10eV The + Kr 0−10eV The + I 0−10eV The + Ar 0−10eV The + Ne 0−10eV Th

1125. M. Guerra, F. Parente, J. P. SantosElectron impact ionization cross sections of several ionization stages of Kr, Ar and FeInt. J. Mass Spectrom. 348, 1 (2013)

e + Ar6+ 0−1000keV The + Ar5+ 0−1000keV The + Ar4+ 0−1000keV The + Ar3+ 0−1000keV The + Ar2+ 0−1000keV The + Ar7+ 0−1000keV Th

1126. R. Naghma, B. AntonyTotal and elastic cross sections for methyl halides by electron impactJ. Electron Spectrosc. Relat. Phenom. 189, 17 (2013)

252

e + CH3I 20−5000 eV The + CH3Br 20−5000 eV The + CH3Cl 20−5000 eV The + CH3F 20−5000 eV Th

1127. M. F. R. Grieve, C. A. Ramsbottom, F. P. KeenanElectron impact excitation of Mg VIII Collision strengths, transition probabilities andtheoretical EUV and soft X-ray line intensities for Mg VIIIAstron. Astrophys. 556, A24 (2013)

e + Mg8+ 1E4−1E7 K Th

1128. F. Li, G. Y. Liang, M. A. Bari, G. ZhaoDirac R-matrix calculation for electron-impact excitation of S XIIIAstron. Astrophys. 556, A32 (2013)

e + S12+ 1E4−1E8 K Th

1129. H. S. Uhm, Y. H. Na, E. H. Choi, G. ChoDissociation and excitation coefficients of nitrogen molecules and nitrogen monoxidegenerationPhys. Plasmas 20, 83502 (2013)

e + N2 0−40 eV The + N2 0−40 eV Th

1130. C. DalCappello, B. Hmouda, A. Naja, G. GasaneoIonization of atomic hydrogen by electrons: the role of the contributions of the pseudo-states in the second Born approximationJ. Phys. B 46, 145203 (2013)

e + H 250eV Th

1131. A. L. Harris, K. MorrisonComprehensive study of 3-body and 4-body models of single ionization of heliumJ. Phys. B 46, 145202 (2013)

e + He 64−600eV Th

1132. C. J. Bostock, C. J. Fontes, D. V. Fursa, H. L. Zhang, I. BrayCalculation of the relativistic rise in electron-impact-excitation cross sections for highlycharged ionsPhys. Rev. A 88, 12711 (2013)

e + U91+ 0−160eV The + Xe53+ 0−160eV The + Ni27+ 0−160eV Th

1133. L. Sigaud, N. Ferreira, E. C. MontenegroAbsolute cross sections for O-2 dication production by electron impactJ. Chem. Phys. 139, 24302 (2013)

e + O2 30−400eV Exp

1134. T. N. Rescigno, A. E. OrelTheoretical study of excitation of the low-lying electronic states of water by electronimpactPhys. Rev. A 88, 12703 (2013)

e + H2O 0−30eV Th

253

1135. Y. Z. Zhang, Y. J. ZhouIonization cross sections for electron scattering from metastable rare-gas atoms (Ne*and Ar*)Chin. Phys. B 22, 73402 (2013)

e + Ar 4−200eV The + Ne 4−200eV Th

1136. V. V. Serov, V. L. Derbov, T. A. Sergeeva, S. I. VinitskiiModern methods for calculating photoionization and electron-impact ionization of two-electron atoms and moleculesPhysics Of Particles And Nuclei 44, 757 (2013)

e + N2 550−600eV The + He 550−600eV The + H2 550−600eV Th

1137. Y. C. Wang, J. Ma, Y. J. ZhouElectronic Excitation of H-2 by Electron Impact Using Multichannel Static-Exchange-Optical MethodChin. Phys. Lett. 30, 73401 (2013)

e + H2 20−30eV The + H2 20−30eV Th

1138. Q. Fan, G. Jiang, L. Cao, B. DengCollision strength calculations of Ni XXIIIPhys. Scr. 88, 15302 (2013)

e + Ni22+ 100−500 RYD Th

1139. H. L. Zhang, C. J. FontesRelativistic distorted-wave collision strengths for the 16 Delta n=0 optically allowedtransitions with n=2 in the 67 Be-like ions with 26 ¡= Z ¡= 92At. Data Nucl. Data Tables 99, 416 (2013)

e + U89+ 0−150 keV The + Xe51+ 0−150 keV Th

1140. K. Ralphs, G. Serna, L. R. Hargreaves, M. A. Khakoo, C. Winstead, V. McKoyExcitation of the six lowest electronic transitions in water by 9-20 eV electronsJ. Phys. B 46, 125201 (2013)

e + H2O 9−20eV E/T

1141. A. Moy, C. Merlet, X. Llovet, O. DugneMeasurements of absolute L- and M-subshell x-ray production cross sections of Pb byelectron impactJ. Phys. B 46, 115202 (2013)

e + Pb 3−38keV E/T

1142. M. Sahlaoui, M. Bouamoud, B. Lasri, M. DoganIonization of a water molecule by electron impact in coplanar symmetric andasymmetric geometriesJ. Phys. B 46, 115206 (2013)

e + H2O 52−107eV Th

254

1143. P. Singh, G. Purohit, V. PatidarSecond-order Born effects in the coplanar to perpendicular plane single ionization ofXe (5p)J. Phys. B 46, 115207 (2013)

e + Xe 20−40eV Th

1144. M. Ulu, Z. N. Ozer, M. Yavuz, O. Zatsarinny, K. Bartschat, M. Dogan, A. CroweExperimental and theoretical investigation of (e, 2e) ionization of Ar(3p) in asymmetrickinematics at 200 eVJ. Phys. B 46, 115204 (2013)

e + Ar 200eV E/T

1145. O. Zatsarinny, K. BartschatThe B-spline R-matrix method for atomic processes: application to atomic structure,electron collisions and photoionizationJ. Phys. B 46, 112001 (2013)

e + Xe 2−500eV The + Kr 2−500eV The + Ar 2−500eV The + Ne 2−500eV The + He 2−500eV The + Xe 2−500eV The + Kr 2−500eV The + Ar 2−500eV The + Ne 2−500eV The + He 2−500eV The + Xe 2−500eV The + Kr 2−500eV The + Ar 2−500eV The + Ne 2−500eV The + He 2−500eV Th

1146. A. Bharadvaja, S. Kaur, K. L. BalujaElectron-impact study of PO2 using the R-matrix methodPhys. Rev. A 87, 62703 (2013)

e + PO2 0−10eV The + PO2 0−10eV The + PO2 0−10eV The + PO2 0−10eV Th

1147. A. Barot, D. Gupta, M. Vinodkumar, B. AntonyComputation of electron-impact total and differential cross sections for allene (C3H4)in the energy range 0.1-2000 eVPhys. Rev. A 87, 62701 (2013)

e + C3H4 0.1−2000eV Th

1148. Y. L. Shi, C. Z. Dong, X. Y. Ma, Z. W. Wu, L. Y. Xie, S. FritzschePolarization of M2 Line Emitted Following Electron-Impact Excitation of Beryllium-Like IonsChin. Phys. Lett. 30, 63401 (2013)

e + Ho63+ 0−5 TH The + Mo38+ 0−5 TH The + U88+ 0−5 TH Th

255

1149. J. D. Fletcher, M. A. Parkes, S. D. PriceElectron ionisation of sulfur dioxideJ. Chem. Phys. 138, 184309 (2013)

e + SO2 0−200eV Exp

1150. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Fe XXV, Co XXVI, Ni XXVII, Cu XXVIII and Zn XXIXPhys. Scr. 87, 55302 (2013)

e + Zn18+ 700−1300 RYD The + Cu17+ 700−1300 RYD The + Ni16+ 700−1300 RYD The + Co15+ 700−1300 RYD The + Fe14+ 700−1300 RYD Th

1151. G. Gasaneo, D. M. Mitnik, J. M. Randazzo, L. U. Ancarani, F. D. ColavecchiaS-model calculations for high-energy-electron-impact double ionization of heliumPhys. Rev. A 87, 42707 (2013)

e + He 500−5600eV Th

1152. M. Hahn, A. Becker, D. Bernhardt, M. Grieser, C. Krantz, M. Lestinsky, A. Mueller, O. Novotny,R. Repnow, S. Schippers, K. Spruck, A. Wolf, D. W. SavinSTORAGE RING CROSS SECTION MEASUREMENTS FOR ELECTRONIMPACT SINGLE AND DOUBLE IONIZATION OF Fe13+ AND SINGLEIONIZATION OF Fe16+ AND Fe17+Astrophys. J. 767, 47 (2013)

e + Fe17+ 0−3000eV The + Fe16+ 0−3000eV The + Fe13+ 0−3000eV Th

1153. T. Pflueger, O. Zatsarinny, K. Bartschat, A. Senftleben, X. Ren, J. Ullrich, A. DornElectron-Impact Ionization of Neon at Low Projectile Energy: An InternormalizedExperiment and Theory for a Complex TargetPhys. Rev. Lett. 110, 153202 (2013)

e + Ne 100eV E/T

1154. Y. M. SmirnovExcitation of undecuplet levels of the gadolinium atom belonging to the 4f (7)5d (2)6pconfigurationOpt. Spectrosc. 114, 492 (2013)

e + Gd 0−200eV E/T

1155. V. Laporta, R. Celiberto, J. TennysonResonant vibrational-excitation cross sections and rate constants for low-energyelectron scattering by molecular oxygenPlasma Sources Sci. Technol. 22, 25001 (2013)

e + O2 0−18eV Th

1156. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Ga XXX, Ge XXXI, As XXXII, Se XXXIII and Br XXXIVPhys. Scr. 87, 45304 (2013)

256

e + As31+ 1E5.2−1E7.7 K The + Ge30+ 1E5.2−1E7.7 K The + Ga29+ 1E5.2−1E7.7 K The + Br33+ 1E5.2−1E7.7 K The + Se32+ 1E5.2−1E7.7 K Th

1157. C. P. Ballance, S. D. Loch, M. S. Pindzola, D. C. GriffinElectron-impact excitation and ionization of W3+ for the determination of tungsteninflux in a fusion plasmaJ. Phys. B 46, 55202 (2013)

e + W3+ 0−100eV The + W3+ 0−100eV Th

1158. B. Najjari, A. B. VoitkivExcitation of highly charged hydrogenlike ions by the impact of equivelocity electronsand protons: A comparative studyPhys. Rev. A 87, 34701 (2013)

e + U91+ 0−500keV The + Bi80+ 0−500keV The + Xe53+ 0−500keV The + Er67+ 0−500keV The + Ni27+ 0−500keV Th

1159. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates, and electron impact excitation rates for transitions inLi-like ions with 12 ¡= Z ¡= 20At. Data Nucl. Data Tables 99, 156 (2013)

e + Ca17+ 1E4.5−1E7.5 K The + K16+ 1E4.5−1E7.5 K The + Ar15+ 1E4.5−1E7.5 K The + Cl14+ 1E4.5−1E7.5 K The + S13+ 1E4.5−1E7.5 K The + P12+ 1E4.5−1E7.5 K The + Al10+ 1E4.5−1E7.5 K The + Mg9+ 1E4.5−1E7.5 K Th

1160. P. X. Hien, B. H. Jeon, A. T. DoElectron Collision Cross Sections for the BF3 Molecule and Electron TransportCoefficients in BF3-Ar and BF3-SiH4 MixturesJ. Phys. Soc. Japan 82, 34301 (2013)

e + BF3 0.1−200eV The + BF3 0.1−200eV Th

1161. S. Niyonzima, F. Lique, K. Chakrabarti, A. Larson, A. E. Orel, I. F. SchneiderMultichannel-quantum-defect-theory treatment of reactive collisions between electronsand BeH+Phys. Rev. A 87, 22713 (2013)

e + BeH+ 0.001−3eV Th

1162. K. L. Nixon, A. J. Murray(e,2e) ionization studies of the stable noble gases in a coplanar symmetric geometryPhys. Rev. A 87, 22712 (2013)

e + He 1.2−200eV The + Xe 1.2−200eV The + Kr 1.2−200eV The + Ne 1.2−200eV Th

257

1163. S. Abdel-Naby, C. P. Ballance, T. G. Lee, S. D. Loch, M. S. PindzolaElectron-impact ionization of the C atomPhys. Rev. A 87, 22708 (2013)

e + C 0−60eV Th

1164. K. D. Lawson, I. H. Coffey, K. M. Aggarwal, F. P. KeenanThe effect of ionization on the populations of excited levels of C IV and C V in tokamakedge plasmasJ. Phys. B 46, 35701 (2013)

e + C4+ 20−130eV The + C3+ 20−130eV The + C4+ 20−130eV The + C3+ 20−130eV Th

1165. O. Zatsarinny, Y. Wang, K. BartschatRelativistic B-spline R-matrix calculations for electron collisions with lead atoms:differential cross sections and spin asymmetriesJ. Phys. B 46, 35202 (2013)

e + Pb 9−10eV Th

1166. Y. Wang, O. Zatsarinny, K. Bartschat, J. P. BoothFine-structure-resolved electron collisions from chlorine atoms in the (3p(5))(2) P-3/2(0) and (3p(5))(2) P-1/2(0) statesPhys. Rev. A 87, 22703 (2013)

e + Cl 0.01−100eV The + Cl 0.01−100eV Th

1167. Y. C. Wang, J. Ma, Y. J. ZhouMomentum-space calculation of electron-CO elastic collisionChin. Phys. B 22, 23402 (2013)

e + Co 2−10eV Th

1168. R. Singh, P. Bhatt, N. Yadav, R. ShankerPartial ionization cross-sections of H2O molecule by 10-25 keV electron ionizationJ. Electron Spectrosc. Relat. Phenom. 186, 58 (2013)

e + H2O 10−25keV Exp

1169. Z. N. Ozer, F. Olgac, M. Ulu, M. DoganDouble Differential Cross-Section Measurements for Electron Impact Ionization ofHeliumAstron. Astrophys. 123, 361 (2013)

e + He 100−300eV Exp

1170. D. H. Ki, Y. D. JungELECTRON IMPACT DISSOCIATION X (1)Sigma(+)(g) -¿ b (3)Sigma(+)(u)AND EXCITATIONS X (1)Sigma(+)(g) -¿ a (3)Sigma(+)(g) AND X(1)Sigma(+)(g) -¿ B (1)Sigma(+)(u) OF MOLECULAR HYDROGEN INNONTHERMAL ASTROPHYSICAL PLASMASAstrophys. J., Suppl. Ser. 204, 18 (2013)

e + H2 9.2−3000eV The + H2 9.2−3000eV Th

258

1171. R. Celiberto, K. L. Baluja, R. K. JanevElectron-impact state-to-state resolved cross sections and rate coefficients for the X(v)-¿ A(v ’) excitation in BeH moleculesPlasma Sources Sci. Technol. 22, 15008 (2013)

e + BeH 1−1000eV Th

1172. R. Kumar, S. PalEvaluation of electron ionization cross-sections of methyl halidesRap. Comm. Mass. Spect. 27, 223 (2013)

e + CH3Br 13−1000eV The + CH3Cl 13−1000eV The + CH3F 13−1000eV Th

1173. A. Borovik, V. Roman, O. Zatsarinny, K. BartschatElectron impact excitation of the lowest doublet and quartet core-excited autoionizingstates in Rb atomsJ. Phys. B 46, 15203 (2013)

e + Rb 15−50eV E/T

1174. Y. Wang, O. Zatsarinny, K. BartschatB-spline R-matrix-with-pseudostates calculations for electron-impact excitation andionization of carbonPhys. Rev. A 87, 12704 (2013)

e + C 0−100eV The + C 0−100eV The + C 0−100eV Th

1175. M. Vinodkumar, C. Limbachiya, A. Barot, N. MasonComputation of electron-impact rotationally elastic total cross sections for methanolover an extensive range of impact energy (0.1-2000 eV)Phys. Rev. A 87, 12702 (2013)

e + CH3OH 0.1−2000eV The + CH3OH 0.1−2000eV The + CH3OH 0.1−2000eV The + CH3OH 0.1−2000eV Th

1176. M. Dogan, M. Ulu, Z. N. Ozer, M. Yavuz, G. BozkurtDouble Differential Cross-Sections for Electron Impact Ionization of Atoms andMoleculesJ. Spectroc. 2013, 192917 (2013)

e + CH4 200−250 eV Expe + H2 200−250 eV Expe + Ar 200−250 eV Expe + He 200−250 eV Exp

1177. V. StancalieELECTRON COLLISIONS WITH Fe-PEAK ELEMENT Co IV: ACOMPUTATIONAL GRAND CHALLENGERomanian Reports In Physics 65, 745 (2013)

e + Co3+ 3−5 RYD Th

1178. B. M. SmirnovExcitation of helium atoms in collisions with plasma electrons in an electric fieldJournal Of Experimental And Theoretical Physics 116, 48 (2013)

259

e + He 1−8eV Th

1179. T. Maihom, I. Sukuba, R. Janev, K. Becker, T. Maerk, A. Kaiser, J. Limtrakul, J. Urban, P. Mach,M. ProbstElectron impact ionization cross sections of beryllium and beryllium hydridesEur. Phys. J. D 67, 2 (2013)

e + Be2H4 0−1000eV The + Be2H2 0−1000eV The + BeH2 0−1000eV The + BeH 0−1000eV The + Be 0−1000eV Th

1180. R. Naghma, B. AntonyElectron impact ionization cross-section of C2, C3, Si2, Si3, SiC, SiC2 and Si2CMol. Phys. 111, 269 (2013)

e + Si2C 10−2000eV The + SiC2 10−2000eV The + SiC 10−2000eV The + Si3 10−2000eV The + Si2 10−2000eV The + C3 10−2000eV The + C2 10−2000eV Th

1181. N. A. Borovoy, R. N. IshchenkoIonization of M subshells of Pb atoms by electron impact in an energy range of 5-30keVOpt. Spectrosc. 114, 1 (2013)

e + Pb 5−30keV Exp

1182. HM Boechat-Roberty, EO Uhl, FN Rodrigues, MCA Lopes, MLM Rocco, CA Lucas, AB Rocha,CE Bielschowsky, GGB deSouzaElectron scattering from trans 1,3-butadiene molecule: cross-sections, oscillatorstrength and VUV photoabsorption cross-sectionsEur. Phys. J. D 67, 26 (2013)

e + C4H6 1000 eV E/T

1183. H Murai, Y Ishijima, T Mitsumura, Y Sakamoto, H Kato, M Hoshino, F Blanco, G Garcia, PLimao-Vieira, MJ Brunger, SJ Buckman, H TanakaA comprehensive and comparative study of elastic electron scattering from OCS andCS2 in the energy region from 1.2 to 200 eVJ. Chem. Phys. 138, 54302 (2013)

e + OCS 1.2−200eV E/Te + Cs2 1.2−200eV E/T

1184. L Chiari, A Zecca, G Garcia, F Blanco, MJ BrungerLow-energy positron and electron scattering from nitrogen dioxideJ. Phys. B 46, 235202 (2013)

e + NO2 1−1000eV Exp

1185. A Gauf, C Navarro, G Balch, LR Hargreaves, MA Khakoo, C Winstead, V McKoyLow-energy elastic electron scattering by acetylenePhys. Rev. A 87, 12710 (2013)

e + C2H2 1−1000eV E/Te + C2H2 1−1000eV E/T

260

1186. JR Brunton, LR Hargreaves, TM Maddern, SJ Buckman, G Garcia, F Blanco, O Zatsarinny, KBartschat, DB Jones, GB daSilva, MJ BrungerDifferential cross sections for low-energy elastic electron scattering from the CF3radicalJ. Phys. B 46, 245203 (2013)

e + CF3 7−50eV E/T

1187. RP McEachran, M Vos, LF ZhuFast-electron scattering from Ne: A comparison of distorted-wave theory withexperimentPhys. Rev. A 87, 52703 (2013)

e + Ne 300−2500eV E/T

1188. R Ward, D Cubric, N Bowring, GC King, FH Read, DV Fursa, I BrayNegative ion resonance measurements in the autoionizing region of helium measuredacross the complete angular scattering range (0 degrees-180 degrees)J. Phys. B 46, 35001 (2013)

e + He 56−60eV E/Te + He 56−60eV E/T

1189. G DelZanna, PJ StoreyAtomic data for astrophysics: Fe xi soft X-ray linesAstron. Astrophys. 549, A42 (2013)

e + Fe10+ 1E5−1E7 K Th

1190. VK Dolmatov, MY Amusia, LV ChernyshevaElectron elastic scattering off a semifilled-shell atom: The Mn atomPhys. Rev. A 88, 42706 (2013)

e + Mn 0−25eV The + Mn 0−25eV Th

1191. NS Shuman, TM Miller, AA Viggiano, J TroeElectron attachment to CF3 and CF3Br at temperatures up to 890 K: Experimentaltest of the kinetic modeling approachJ. Chem. Phys. 138, 204316 (2013)

e + CF3Br 300−890K Expe + CF3 300−890K Exp

1192. R Janeckova, D Kubala, O May, J Fedor, M AllanExperimental Evidence on the Mechanism of Dissociative Electron Attachment toFormic AcidPhys. Rev. Lett. 111, 213201 (2013)

e + HCOOH 1−3.5eV Exp

1193. KL Nixon, AJ Murray, H Chaluvadi, CG Ning, J Colgan, DH MadisonLow energy (e,2e) coincidence studies of NH3: Results from experiment and theoryJ. Chem. Phys. 138, 174304 (2013)

e + CH4 11−28eV E/Te + NH3 11−28eV E/Te + CH4 11−28eV E/Te + NH3 11−28eV E/T

261

1194. O Novotny, A Becker, H Buhr, C Domesle, W Geppert, M Grieser, C Krantz, H Kreckel, R Repnow,D Schwalm, K Spruck, J Stuuetzel, B Yang, A Wolf, DW SavinDISSOCIATIVE RECOMBINATION MEASUREMENTS OF HCl+ USING AN IONSTORAGE RINGAstrophys. J. 777, 54 (2013)

e + HCl+ 1E−5−5eV Exp

1195. T Sochi, PJ StoreyDielectronic recombination lines of C+At. Data Nucl. Data Tables 99, 633 (2013)

e + C+ 1E3−1E4.8 K Th

1196. GSJ Armstrong, J Colgan, MS PindzolaAngular distributions for the electron-impact single ionization of sodium andmagnesiumPhys. Rev. A 88, 42713 (2013)

e + Mg 10−60eV The + Na 10−60eV Th

1197. M Braun, II Fabrikant, MW Ruf, H HotopHigh-resolution studies of (SF6)(q)(-) (q=1-3) cluster anion formation in low-energyelectron collisions with (SF6)N clusters (N ¿= 2)J. Phys. B 46, 195202 (2013)

e + SF6 0.−3000eV Exp

1198. C CornaggiaElectron elastic back-scattering from aligned CO2+ molecular ions in the 15-30 eVenergy rangeJ. Phys. B 46, 191001 (2013)

e + CO2 10−30eV Th

1199. SL GubermanThe vibrational dependence of dissociative recombination: Cross sections for N-2(+)J. Chem. Phys. 139, 124318 (2013)

e + N2+ 0.001−1eV Th

1200. A Sasaki, I MurakamiAlgorithm-based modelling of fractional ion abundance and rates of ionization andrecombination for tungsten plasmasJ. Phys. B 46, 175701 (2013)

e + W42+ 100−10000eV The + W41+ 100−10000eV The + W46+ 100−10000eV The + W45+ 100−10000eV The + W44+ 100−10000eV The + W436+ 100−10000eV The + W42+ 100−10000eV The + W41+ 100−10000eV The + W46+ 100−10000eV The + W45+ 100−10000eV The + W44+ 100−10000eV The + W436+ 100−10000eV Th

262

1201. ZM Hu, YM Li, N NakamuraResonance strength for KLL dielectronic recombination of hydrogenlike kryptonPhys. Rev. A 87, 52706 (2013)

e + K35+ E/T

1202. D Nikolic, TW Gorczyca, KT Korista, GJ Ferland, NR BadnellSUPPRESSION OF DIELECTRONIC RECOMBINATION DUE TO FINITEDENSITY EFFECTSAstrophys. J. 768, 82 (2013)

e + C3+ 0.01−30eV Th

1203. MA Khakoo, H Silva, J Muse, MCA Lopes, C Winstead, V McKoyElectron scattering from H2O: Elastic scattering (vol 78, 052710, 2008)Phys. Rev. A 87, 49902 (2013)

e + H2O 1−100eV Exp

1204. K Chakrabarti, DR Backodissa-Kiminou, N Pop, JZ Mezei, O Motapon, F Lique, O Dulieu, AWolf, IF SchneiderDissociative recombination of electrons with diatomic molecular cations abovedissociation threshold: Application to H-2(+) and HD+Phys. Rev. A 87, 22702 (2013)

e + HD+ 0−14eV The + H2

+ 0−14eV Th

1205. R Curik, FA GianturcoIndirect dissociative recombination of LiHe+ ions driven by vibrational FeshbachresonancesPhys. Rev. A 87, 12705 (2013)

e + LiHe+ 0.02−500eV Th

1206. O. NovotnDISSOCIATIVE RECOMBINATION MEASUREMENTS OF HCl+ USING AN IONSTORAGE RINGAstrophys. J. 777, 54 (2014)

e + HCl+ 1E−5−4.06eV Exp

1207. D.H. Ki, Y.D. JungELECTRON IMPACT DISSOCIATION X (1)Sigma(+)(g) -¿ b (3)Sigma(+)(u)AND EXCITATIONS X (1)Sigma(+)(g) -¿ a (3)Sigma(+)(g) AND X(1)Sigma(+)(g) -¿ B (1)Sigma(+)(u) OF MOLECULAR HYDROGEN INNONTHERMAL ASTROPHYSICAL PLASMASAstrophys. J., Suppl. Ser. 204, 18 (2014)

e + H2 9.2−3000eV Th

1208. Z.N. Ozera, F. Olgaca, M. Ulua, B. Aktasb, M. DoganaMeasurements of Double Differential Cross-Sections for He at Intermediate EnergyActa Phys. Pol. A 125, 341 (2014)

e + He 200eV Exp

1209. M. Yavuz, N. Isik, Z. N. OzerDouble Differential Cross-Section Measurements for Methane Molecule at 350 eVActa Phys. Pol. A 125, 442 (2014)

263

e + CH4 25−300eV Exp

1210. G. DelZanna, P. J. Storey, N. R. Badnell, H. E. MasonAtomic data for astrophysics: Fe IXAstron. Astrophys. 565, A77 (2014)

e + Fe8+ 1E5−1E6.4 K Th

1211. G. DelZanna, N. R. BadnellAtomic data for astrophysics: improved collision strengths for Fe VIIIAstron. Astrophys. 570, A56 (2014)

e + Fe7+ 1E5−1E6.4 K Th

1212. G. DelZanna, P. J. Storey, H. E. MasonAtomic data for astrophysics: Ni xvAstron. Astrophys. 567, A18 (2014)

e + Ni14+ 1E5.6−1E6.7 K Th

1213. G. DelZanna, P. J. Storey, N. R. BadnellAtomic data for astrophysics: Ni XIAstron. Astrophys. 566, A123 (2014)

e + Ni10+ 1E5−1E7 K Th

1214. M. F. R. Grieve, C. A. Ramsbottom, F. P. KeenanElectron impact excitation of Mg VIII Collision strengths, transition probabilities andtheoretical EUV and soft X-ray line intensities for Mg VIIIAstron. Astrophys. 556, A24 (2014)

e + Mg7+ 1E4−1E7 K Th

1215. L. Fernandez-Menchero, G. DelZanna, N. R. BadnellR-matrix electron-impact excitation data for the Be-like iso-electronic sequenceAstron. Astrophys. 566, A104 (2014)

e + Ne6+ 1−1E9 K The + C2+ 1−1E9 K The + Fe22+ 1−1E9 K The + Mg8+ 1−1E9 K Th

1216. F. Li, G. Y. Liang, M. A BariDirac R-matrix calculation for electron-impact excitation of S XIIIAstron. Astrophys. 556, A32 (2014)

e + S12+ 0−150 RYD Th

1217. A. N. Zavilopulo, P. P. Markush, O. B. Shpenik, M. I. MykytaElectron-impact ionization of sulfur in the gas phaseAtomic And Molecular Physics 59, 951 (2014)

e + Sn− 0−10eV Exp

1218. H. L. Zhang, C. J. FontesRelativistic distorted-wave collision strengths for the 16 Delta n=0 optically allowedtransitions with n=2 in the 67 Be-like ions with 26 ¡= Z ¡= 92At. Data Nucl. Data Tables 99, 416 (2014)

e + U88+ 0−1E5 eV The + Xe50+ 0−1E5 eV Th

264

1219. E. Landi, A. K BhatiaAtomic data and spectral line intensities for Ca IXAt. Data Nucl. Data Tables 100, 1519 (2014)

e + Ca8+ 0−60 RYD Th

1220. M. YavuzComprehensive experimental and theoretical study of double-differential cross sectionsfor CH4 at 300 and 350 eV incident electron energiesCan. J. Phys. 92, 1676 (2014)

e + CH4 300−350eV E/T

1221. M. Vojnovi, M. PopoviRate coefficients for electron impact excitation of COChem. Phys. 423, 1 (2014)

e + Co 0−1000 Td Th

1222. R. KumarElectron ionization cross sections for the PH3 moleculeChem. Phys. Lett. 609, 108 (2014)

e + PH3 14−1000eV Th

1223. M. Hoshino, H. Mura, H. KatoResolution of a significant discrepancy in the electron impact excitation of the3s[3/2](1) and 3s ’[1/2](1) low-lying electronic states in neonChem. Phys. Lett. 585, 33 (2014)

e + Ne 20−300eV Th

1224. J. R. Brunton, L. R. Hargreaves, S. J. BuckmanAnomalously large low-energy elastic cross sections for electron scattering from theCF3 radicalChem. Phys. Lett. 568, 55 (2014)

e + CF3 7−50eV E/T

1225. N. X. Yang, J. J. Zhang, C. Z. DongAbsolute Cross Sections for Near-Threshold Electron-Impact Excitation of the 2s S-2-¿ 2p P-2 Transition of Li-Like C3+, N4+, and O5+ IonsChin. Phys. Lett. 31, 083401 (2014)

e + O5+ 8−17eV The + N4+ 8−17eV The + C3+ 8−17eV Th

1226. Z. B. Chen, C. Z. Dong, L. Y. Xie, J. JiangElectron Impact Excitation of Xenon from the Ground State and the Metastable Stateto the 5p(5)7p LevelsChin. Phys. Lett. 31, 033401 (2014)

e + Xe 0−200eV Th

1227. J. Jiang, C. Z. Dong, L. Y. XieElectron Impact Excitations and Linear Polarization for 1s(2) S-1(0)-1s2P P-3,1(1)Lines of Fe24+ Ions under Screened Coulomb InteractionsChin. Phys. Lett. 31, 023401 (2014)

e + Fe24+ 0−100 eV Th

265

1228. Y. Z. Zhang, Y. J. ZhouIonization cross sections for electron scattering from metastable rare-gas atoms (Ne*and Ar*)Chin. Phys. B 22, 073402 (2014)

e + Ar 50−200eV The + Ne 50−200eV Th

1229. X. M. Tan, Y. W. WangTotal cross sections for electron scattering from sulfur compoundsChin. Phys. B 22, 023403 (2014)

e + SO2 0−3000eV The + SO 0−3000eV Th

1230. Y. Wu, G. Y. Wang, Q. Mu, Q. ZhaoM-alpha beta X-ray production cross sections of Pb and Bi by 9-40 keV electron impactChin. Phys. B 23, 013401 (2014)

e + Bi 9−40 keV Expe + Pb 9−40 keV Exp

1231. Y. B. Tang, C. B. Li, H. X. QiaoCalculations on polarization properties of alkali metal atoms using Dirac-Fock pluscore polarization methodChin. Phys. B 23, 063101 (2014)

e + Fr The + Cs The + Rb The + K The + Na The + Li Th

1232. L. X. ZhouPolarization effect in (e, 2e) reaction process for Ar (3s) in coplanar asymmetricgeometryChin. Phys. B 23, 113402 (2014)

e + Ar 2−10eV Th

1233. Y. Z. Zhang, W. Yangb, Y. J. ZhouSecond-order Born calculation of coplanar symmetric (e, 2e) process on MgChin. Phys. B 23, 063402 (2014)

e + Mg 3−10eV Th

1234. Y. C. WangElectronic Excitation of H-2 by Electron Impact Using Multichannel Static-Exchange-Optical MethodChin. Phys. Lett. 30, 073401 (2014)

e + H2 20−30eV The + H2 20−30eV Th

1235. Y. L. Shi, C. Z. Dong, X. Y. MaPolarization of M2 Line Emitted Following Electron-Impact Excitation of Beryllium-Like IonsChin. Phys. Lett. 30, 063401 (2014)

266

e + U88+ 0−5eV The + Ho63+ 0−5eV The + Mo38+ 0−5eV Th

1236. E. S. ChenHyperfine electron affinities of molecular oxygenComput. Theo. Chem 1050, 89 (2014)

e + O2 E/T

1237. Q. Fan, G. Jiang, L. CaoCollision strengths for transitions of Ni XXIEur. Phys. J. D 67, 255 (2014)

e + Ni20+ 1E6.4−1E7.4 Th

1238. J. Li, Z. Zhao, X. ZhangMCDHF calculation of electron affinities of Group I and Group IB atomic anionsEurophys. Lett. 107, 33001 (2014)

e + Au− The + Ag− The + Cu− The + Fr− The + Cs− The + Rb− The + K− The + Na− The + Li− The + H− Th

1239. H. Cho, J. S. Yoon, M. Y. SongEVALUATION OF TOTAL ELECTRON SCATTERING CROSS SECTIONS OFPLASMA-RELEVANT MOLECULESFusion Sci. Technol. 63, 349 (2014)

e + C2H6 0.01−100eV The + C2H4 0.01−100eV The + CH4 0.01−100eV The + C-C4F8 0.01−100eV The + C3F8 0.01−100eV The + CF3I 0.01−100eV The + CF3Cl 0.01−100eV The + C2F6 0.01−100eV Th

1240. G. Karwasz, K. FedusSOME SYSTEMATICS IN ELECTRON SCATTERING CROSS SECTIONSFusion Sci. Technol. 63, 338 (2014)

e + Si2H6 0.1−100eV E/Te + CF4 0.1−100eV E/Te + CCl4 0.1−100eV E/Te + H2O 0.1−100eV E/Te + HCl 0.1−100eV E/Te + BCl3 0.1−100eV E/Te + BF3 0.1−100eV E/Te + CO2 0.1−100eV E/Te + NO 0.1−100eV E/Te + CF3Br 0.1−100eV E/Te + CH4 0.1−100eV E/T

267

e + WF6 0.1−100eV E/Te + H2O 0.1−100eV E/Te + CH3Br 0.1−100eV E/Te + CCl2F2 0.1−100eV E/Te + SF6 0.1−100eV E/Te + C2F6 0.1−100eV E/Te + HCl 0.1−100eV E/Te + BCl3 0.1−100eV E/Te + BF3 0.1−100eV E/Te + Si2H6 0.1−100eV E/Te + CF4 0.1−100eV E/Te + CCl4 0.1−100eV E/Te + CH4 0.1−100eV E/Te + CO2 0.1−100eV E/Te + NO 0.1−100eV E/Te + CF3Br 0.1−100eV E/Te + WF6 0.1−100eV E/Te + H2O 0.1−100eV E/Te + HCl 0.1−100eV E/Te + BCl3 0.1−100eV E/Te + CH3Br 0.1−100eV E/Te + CCl2F2 0.1−100eV E/Te + SF6 0.1−100eV E/Te + BF3 0.1−100eV E/Te + CO2 0.1−100eV E/Te + NO 0.1−100eV E/Te + CF3Br 0.1−100eV E/Te + C2F6 0.1−100eV E/Te + Si2H6 0.1−100eV E/Te + CF4 0.1−100eV E/Te + CH3Br 0.1−100eV E/Te + CCl2F2 0.1−100eV E/Te + SF6 0.1−100eV E/Te + C2F6 0.1−100eV E/Te + CCl4 0.1−100eV E/Te + CH4 0.1−100eV E/Te + WF6 0.1−100eV E/T

1241. G. Y. Liang, N. R. Badnell, G. ZhaoEVALUATION OF ELECTRON IMPACT EXCITATION DATA ALONGISOELECTRONIC SEQUENCESFusion Sci. Technol. 63, 372 (2014)

e + Ar15+ 800−1200eV The + Fe16+ 800−1200eV Th

1242. M. Guerra, F. Parente, J.P. SantosElectron impact ionization cross sections of several ionization stages of Kr, Ar and FeInt. J. Mass Spectrom. 348, 1 (2014)

e + Ar4+ 10eV−5E3keV The + Kr5+ 10eV−5E3keV The + Kr+ 10eV−5E3keV The + Fe 10eV−5E3keV The + Ar 10eV−5E3keV The + Ar3+ 10eV−5E3keV The + Kr 10eV−5E3keV The + Ar2+ 10eV−5E3keV The + Kr17+ 10eV−5E3keV The + Kr15+ 10eV−5E3keV Th

268

e + Fe13+ 10eV−5E3keV The + Fe11+ 10eV−5E3keV The + Fe9+ 10eV−5E3keV The + Fe6+ 10eV−5E3keV The + Kr10+ 10eV−5E3keV The + Fe5+ 10eV−5E3keV The + Fe2+ 10eV−5E3keV The + Ar7+ 10eV−5E3keV The + Ar6+ 10eV−5E3keV The + Ar5+ 10eV−5E3keV The + Kr6+ 10eV−5E3keV Th

1243. G. P. Karwasz, P. Mozejko, M. Y. SongElectron-impact ionization of fluoromethanes - Review of experiments and binary-encounter modelsInt. J. Mass Spectrom. 365, 232 (2014)

e + CF4 10−1000 eV Expe + CHF3 10−1000 eV Expe + CH2F2 10−1000 eV Expe + CH3F 10−1000 eV Exp

1244. J. KopyraElectron attachment to molecules studied by electron beam and electron swarmexperimentsInt. J. Mass Spectrom. 365, 98 (2014)

e + CF2Cl2 0−4E19 mole/cm3 Exp

1245. T. M. Miller, N. S. Shuman, A. A. ViggianoArrhenius behavior of electron attachment to CH3Br from 303 to 1100KInt. J. Mass Spectrom. 365, 75 (2014)

e + CH3Br 330−1100 K Exp

1246. J. Wang, C. Z. Gao, F. Calvayrac, F. S. ZhangCollision dynamics of proton with formaldehyde: Fragmentation and ionizationJ. Chem. Phys. 140, 124306 (2014)

e + CH2O 85eV Th

1247. D. L. Huang, P. D. Dau, H. T. Liu, L. S. WangHigh-resolution photoelectron imaging of cold C-60(-) anions and accuratedetermination of the electron affinity of C-60J. Chem. Phys. 140, 224315 (2014)

e + C60 Exp

1248. S. L. GubermanThe vibrational dependence of dissociative recombination: Rate constants for N-2(+)J. Chem. Phys. 141, 204307 (2014)

e + N2+ 100−3000 K Th

1249. X. Llovet, C. J. Powell, F. Salvat, A. JablonskiCross Sections for Inner-Shell Ionization by Electron ImpactJ. Phys. Chem. Ref. Data 43, 013102 (2014)

269

e + Pt 5−1E6 keV The + Os 5−1E6 keV The + Re 5−1E6 keV The + Hf 5−1E6 keV The + Dy 5−1E6 keV The + I 5−1E6 keV The + U 5−1E6 keV The + Pb 5−1E6 keV The + Au 5−1E6 keV The + W 5−1E6 keV The + Ta 5−1E6 keV The + Y 5−1E6 keV The + Tm 5−1E6 keV The + Er 5−1E6 keV The + Ho 5−1E6 keV The + Gd 5−1E6 keV The + Eu 5−1E6 keV The + Sm 5−1E6 keV The + Nd 5−1E6 keV The + Pr 5−1E6 keV The + Ce 5−1E6 keV The + La 5−1E6 keV The + Te 5−1E6 keV The + Xe 5−1E6 keV The + Sb 5−1E6 keV The + Sn 5−1E6 keV The + In 5−1E6 keV The + Cd 5−1E6 keV The + Pd 5−1E6 keV The + Mo 5−1E6 keV The + Nb 5−1E6 keV The + Zr 5−1E6 keV The + Sr 5−1E6 keV The + Rb 5−1E6 keV The + Kr 5−1E6 keV The + Br 5−1E6 keV The + Se 5−1E6 keV The + As 5−1E6 keV The + Ge 5−1E6 keV The + Ga 5−1E6 keV The + Zn 5−1E6 keV The + Cu 5−1E6 keV The + Ni 5−1E6 keV The + Co 5−1E6 keV The + Mn 5−1E6 keV The + Cr 5−1E6 keV The + V 5−1E6 keV The + Ti 5−1E6 keV The + Sc 5−1E6 keV The + Ca 5−1E6 keV The + K 5−1E6 keV The + Ar 5−1E6 keV The + Cl 5−1E6 keV The + S 5−1E6 keV The + Al 5−1E6 keV The + Mg 5−1E6 keV The + Na 5−1E6 keV The + O 5−1E6 keV The + H 5−1E6 keV Th

270

e + C 5−1E6 keV The + Bi 5−1E6 keV The + Ag 5−1E6 keV The + Fe 5−1E6 keV The + Si 5−1E6 keV The + N 5−1E6 keV Th

1250. M. Hoshino, H. Murai, H. Kato, M. J. Brunger, Y. Itikawa, H. TanakaElectron impact excitation of the low-lying 3s[3/2](1) and 3s ’[1/2](1) levels in neonfor incident energies between 20 and 300 eVJ. Chem. Phys. 139, 184301 (2014)


1251. L. Sigaud, N. Ferreira, E. C. MontenegroAbsolute cross sections for O-2 dication production by electron impactJ. Chem. Phys. 139, 024302 (2014)

e + O2 30−400eV Exp

1252. M. Hoshino, M. Horie, H KatoCross sections for elastic scattering of electrons by CF3Cl, CF2Cl2, and CFCl3J. Chem. Phys. 138, 214305 (2014)

e + CFCl3 1.5−100eV E/Te + CF2Cl2 1.5−100eV E/Te + CF3Cl 1.5−100eV E/T

1253. R. Naghma, B. AntonyTotal and elastic cross sections for methyl halides by electron impactJ. Electron Spectrosc. Relat. Phenom. 189, 17 (2014)

e + CH3I 20−5000eV The + CH3Br 20−5000eV The + CH3Cl 20−5000eV The + CH3F 20−5000eV Th

1254. J. R. Ferraz, A. S. dosSantos, G. L. C. deSouzaCross sections for electron scattering by methylfluoride (CH3F) in the low- andintermediate-energy rangesJ. Electron Spectrosc. Relat. Phenom. 193, 16 (2014)

e + CH3F 15−500eV Th

1255. R. Naghma, D. Gupta, B. AntonyTotal cross sections for electron scattering with halocarbon moleculesJ. Electron Spectrosc. Relat. Phenom. 193, 48 (2014)

e + CHCl3 20−5000eV The + CH2Cl2 20−5000eV Th

1256. B. Goswami, D. Gupta, B. Antony0.1-2000 eV electron impact cross sections for dichlorine monoxideJ. Electron Spectrosc. Relat. Phenom. 193, 86 (2014)

e + Cl2O 0.1−2000eV Th

1257. M. O. A. ElGhazaly, J. B. A. Mitchell, J. J JuretaElectron Impact Induced Fragmentation of N2H+ and N2D+J. Phys. Chem. A 118, 10020 (2014)

271

e + N2D+ 5−3000eV Exp

e + N2H+ 5−3000eV Exp

1258. A Moy, C MerletMeasurements of absolute L- and M-subshell x-ray production cross sections of Pb byelectron impactJ. Phys. B 46, 115202 (2014)

e + Pb 3−38keV E/T

1259. A BorovikElectron impact excitation of the lowest doublet and quartet core-excited autoionizingstates in Rb atomsJ. Phys. B 46, 015203 (2014)

e + Rb 15−50eV E/T

1260. C. P. Ballance, S. D. Loch, M. S. Pindzola, D. C. GriffinElectron-impact excitation and ionization of W3+ for the determination of tungsteninflux in a fusion plasmaJ. Phys. B 46, 055202 (2014)

e + W3+ 0.2−100eV The + W3+ 0.2−100eV Th

1261. J. R. Brunton, L. R. Hargreaves, T. M MaddernDifferential cross sections for low-energy elastic electron scattering from the CF3radicalJ. Phys. B 46, 245203 (2014)

e + CF3 7−50eV Exp

1262. A Borovik, A Kupliauskiene, O ZatsarinnyExcitation-autoionization cross section of alkali atoms by electron impactJ. Phys. B 46, 215201 (2014)

e + Na 30−400eV Exp

1263. B. Jr, M. F. Gharaibeh, P. M. HillenbrandDetailed investigation of electron-impact single-ionization cross sections and plasmarate coefficients of N-shell tin ionsJ. Phys. B 46, 175201 (2014)

e + Sn13+ 40−1000eV Expe + Sn12+ 40−1000eV Expe + Sn11+ 40−1000eV Expe + Sn10+ 40−1000eV Expe + Sn9+ 40−1000eV Expe + Sn8+ 40−1000eV Expe + Sn7+ 40−1000eV Expe + Sn6+ 40−1000eV Expe + Sn5+ 40−1000eV Expe + Sn4+ 40−1000eV Exp

1264. J Lecointre, J. J. Jureta, X Urbain, P DefranceElectron-impact dissociation of HeH+: absolute cross sections for the production ofHeq+ (q=1-2) fragmentsJ. Phys. B 47, 015203 (2014)

e + HeH+ 10−3000eV Exp

272

1265. Y. M. SmirnovExcitation of GeII in collisions of slow electrons with germanium atomsJ. Phys. B 47, 225204 (2014)

e + Ge+ 0−200eV Exp

1266. A Moy, C Merlet, X Llovet, O DugneM-subshell ionization cross sections of U by electron impactJ. Phys. B 47, 055202 (2014)

e + U 4−40keV Exp

1267. J. M. Fernandez-Varea, V Jahnke, N. L. Maidana, A. A. Malafronte, V. R. VaninCross sections of K-shell ionization by electron impact, measured from threshold to100 keV, for Au and BiJ. Phys. B 47, 155201 (2014)

e + Bi 80−100keV Expe + Au 80−100keV Exp

1268. G. A. Alna’washi, K. K. Baral, N. B. Aryal, C. M. Thomas, R. A. PhaneufElectron-impact ionization of Se3+J. Phys. B 47, 105201 (2014)

e + Se3+ 30−1000eV Exp

1269. G. A. Alna’washi, N. B. Aryal, K. K. Baral, C. M. Thomas, R. A. PhaneufElectron-impact ionization of Se2+J. Phys. B 47, 135203 (2014)

e + Se2+ 30−500eV Exp

1270. C. C. Montanari, J. E. MiragliaElectron-impact multiple ionization of Ne, Ar, Kr and XeJ. Phys. B 47, 105203 (2014)

e + Ar 0.1−10keV The + Ne 0.1−10keV The + Xe 0.1−10keV The + Kr 0.1−10keV Th

1271. M. S. CasagrandeComparison of the electron impact experimental and theoretical fourfold differentialcross sections for Ne and CH4J. Phys. B 47, 115203 (2014)

e + CH4 500eV E/Te + Ne 500eV E/T

1272. M. C. BordageComparisons of sets of electron-neutral scattering cross sections and swarm parametersin noble gases: III. Krypton and xenonJ. Phys. D 46, 334003 (2014)

e + Xe 0.01−400eV E/Te + Kr 0.01−400eV E/Te + Xe 0.01−400eV E/Te + Kr 0.01−400eV E/Te + Xe 0.01−400eV E/Te + Kr 0.01−400eV E/Te + Xe 0.01−400eV E/Te + Kr 0.01−400eV E/T

273

1273. L. L. Alves, K Bartschat, S. F. Biagi, M. C. BordageComparisons of sets of electron-neutral scattering cross sections and swarm parametersin noble gases: II. Helium and neonJ. Phys. D 46, 334002 (2014)

e + He 20−1000eV E/Te + Ne 20−1000eV E/Te + He 20−1000eV E/Te + Ne 20−1000eV E/Te + He 20−1000eV E/Te + Ne 20−1000eV E/Te + He 20−1000eV E/Te + Ne 20−1000eV E/T

1274. L. C. Pitchford, L. L. Alves, K BartschatComparisons of sets of electron-neutral scattering cross sections and swarm parametersin noble gases: I. ArgonJ. Phys. D 46, 334001 (2014)

e + Ar 0.01−200eV E/Te + Ar 0.01−200eV E/Te + Ar 0.01−200eV E/T

1275. L.Y. Xie, X.Y. Maa, C.Z. Donga, Z.W. Wua, Y.L. Shia, J. JiangPolarization of the nf -¿ 3d (n=4, 5, 6) x-rays from tungsten ions following electron-impact excitation and dielectronic recombination processesJ. Quant. Spectrosc. Radiat. Transfer 141, 31 (2014)

e + W46+ 0−12 keV The + W45+ 0−12 keV The + W44+ 0−12 keV The + W43+ 0−12 keV The + W42+ 0−12 keV Th

1276. K. Shigemura, M. Kitajima, M. Kurokawa, K. Toyoshima, T. Odagiri, A. Suga, H. Kato, M.Hoshino, H. Tanaka, K. ItoTotal cross sections for electron scattering from He and Ne at very low energiesPhys. Rev. A 89, 022709 (2014)

e + Ne 0.06−20eV Expe + He 0.06−20eV Exp

1277. C. J. Bostock, D. V. Fursa, I. Bray, K. BartschatCalculation of the polarization fraction and electron-impact excitation cross sectionfor the Cd+ 5(p) P-2(3/2) statePhys. Rev. A 90, 012707 (2014)

e + Cd+ 20−200eV Th

1278. A. Muller, A. Borovik, K. Huber, S. Schippers, D. V. Fursa, I. BrayDouble- K- vacancy states in electron-impact single ionization of metastabletwo-electron N5+(1s2s S-3(1)) ionsPhys. Rev. A 90, 010701 (2014)

e + N5+ 100−1000eV Exp

1279. D. Bernhardt, A. Becker, M. Grieser, M. Hahn, C. Krantz, M. Lestinsky, O. Novotny, R. Repnow,D. W. SavinAbsolute rate coefficients for photorecombination and electron-impact ionization ofmagnesiumlike iron ions from measurements at a heavy-ion storage ringPhys. Rev. A 90, 012702 (2014)

274

e + Fe14+ 0.5−1000eV Expe + Fe14+ 0.5−1000eV Exp

1280. R. D. Thomas, A. Ehlerding, W. D. GeppertDissociative recombination of LiH2+Phys. Rev. A 89, 050701 (2014)

e + LiH2+ 0.001−20eV E/T

1281. V. Jonauskas, A. Prancikevicius, S. Masys, A. KynieneElectron-impact direct double ionization as a sequence of processesPhys. Rev. A 89, 052714 (2014)

e + W5+ 50−10000eV The + Ar2+ 50−10000eV The + C+ 50−10000eV The + O3+ 50−10000eV The + O2+ 50−10000eV The + O+ 50−10000eV Th

1282. S. Amami, M. UluTheoretical and experimental investigation of (e,2e) ionization of argon 3p inasymmetric kinematics at intermediate energyPhys. Rev. A 90, 012704 (2014)

e + Ar 200 eV E/T

1283. C. Y. Lin, C. W. McCurdy, T. N. RescignoComplex Kohn approach to molecular ionization by high-energy electrons: Applicationto H2OPhys. Rev. A 89, 012703 (2014)

e + H2O 0−50eV Th

1284. C. Y. Lin, C. W. McCurdy, T. N. RescignoTheoretical study of (e, 2e) from outer- and inner-valence orbitals of CH4: A complexKohn treatmentPhys. Rev. A 89, 052718 (2014)

e + CH4 500 eV Th

1285. S. Amami, A. MurrayTheoretical and experimental (e,2e) study of electron-impact ionization of laser-alignedMg atomsPhys. Rev. A 90, 062707 (2014)

e + Mg 10−25eV Th

1286. A. Makhoute, I. Ajana, D. KhalilLow- energy electron- impact laser- assisted ionization of atomic hydrogenPhys. Rev. A 90, 053415 (2014)

e + H 25−250eV Th

1287. C. J. BostockRelativistic convergent close-coupling calculation of inelastic scattering of electronsfrom cesiumPhys. Rev. A 89, 032712 (2014)

e + Cs 7−12eV Th

275

1288. X. RenBenchmark experiment for electron-impact ionization of argon: Absolutetriple-differential cross sections via three-dimensional electron emission images (vol83, 052714, 2011)Phys. Rev. A 89, 029904 (2014)

e + Ar 195eV E/T

1289. A. GaufLow-energy elastic electron scattering by acetaldehydePhys. Rev. A 89, 022708 (2014)

e + CH3CHO 1−50eV E/T

1290. I. Bray, C. J. Guilfoile, A. S. Kadyrov, D. V. Fursa, A. T. StelbovicsIonization amplitudes in electron-hydrogen collisionsPhys. Rev. A 90, 022710 (2014)

e + Kr+ 0−5eV Th

1291. P. Singh, G. Purohit, C. Champion, V. PatidarElectron- and positron-induced ionization of water molecules: Theory versusexperiment at the triply differential scalePhys. Rev. A 89, 032714 (2014)

e + H2O 4−40eV Th

1292. G. JalbertElectron-detachment cross section for CN(-)and O-2(-) incident on N-2 at intermediatevelocitiesPhys. Rev. A 89, 012712 (2014)

e + N2 0.088−10 A.U. The + O− 0.088−10 A.U. The + CN− 0.088−10 A.U. Th

1293. M. C. Zammit, D. V. Fursa, I. BrayElectron scattering from the molecular hydrogen ion and its isotopologuesPhys. Rev. A 90, 022711 (2014)

e + HD+ 0−1000eV The + T2

+ 0−1000eV The + D2

+ 0−1000eV The + H2

+ 0−1000eV The + T2

+ 0−1000eV The + D2

+ 0−1000eV The + H2

+ 0−1000eV The + He+ 0−1000eV The + D2

+ 0−1000eV The + H2

+ 0−1000eV The + He+ 0−1000eV The + H2

+ 0−1000eV The + He+ 0−1000eV The + HT+ 0−1000eV The + He+ 0−1000eV The + HT+ 0−1000eV The + HD+ 0−1000eV The + HT+ 0−1000eV The + HD+ 0−1000eV The + T2

+ 0−1000eV Th

276

e + HT+ 0−1000eV The + HD+ 0−1000eV The + T2

+ 0−1000eV The + D2

+ 0−1000eV Th

1294. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Ga XXX, Ge XXXI, As XXXII, Se XXXIII and Br XXXIVPhys. Scr. 87, 045304 (2014)

e + Br33+ 900−2100 RYD The + Se32+ 900−2100 RYD The + As31+ 900−2100 RYD The + Ge30+ 900−2100 RYD The + Ga29+ 900−2100 RYD Th

1295. A. Barot, D. GuptaComputation of electron-impact total and differential cross sections for allene (C3H4)in the energy range 0.1-2000 eVPhys. Rev. A 87, 062701 (2014)

e + C3H4 0.1−2000eV Th

1296. Y. Wang, O. Zatsarinny, K. BartschatB-spline R-matrix-with-pseudostates calculations for electron-impact excitation andionization of carbonPhys. Rev. A 87, 012704 (2014)

e + C 0−100eV The + C 0−100eV The + C 0−100eV The + C 0−100eV Th

1297. M. Vinodkumar, C. Limbachiya, A. BarotComputation of electron-impact rotationally elastic total cross sections for methanolover an extensive range of impact energy (0.1-2000 eV)Phys. Rev. A 87, 012702 (2014)

e + CH3OH 0.1−2000eV The + CH3OH 0.1−2000eV The + CH3OH 0.1−2000eV Th

1298. A. I. Mikhailov, A. V. Nefiodov, G PlunienElectron correlations in cross sections for ionization of heliumlike ions by high-energyparticle impactPhys. Rev. A 87, 032705 (2014)

e + Ar16+ 1−1000eV The + Ne8+ 1−1000eV The + O6+ 1−1000eV The + N5+ 1−1000eV The + C4+ 1−1000eV The + B3+ 1−1000eV The + Li+ 1−1000eV The + He 1−1000eV Th

1299. M. C. Zammit, D. V. Fursa, I. BrayCalculations of electron scattering from H-2(+)Phys. Rev. A 88, 062709 (2014)

e + H2+ 0−1000eV Th

277

1300. J. C. Lower, E. Ali, S. BellmExperimental and theoretical cross sections for molecular-frame electron-impactexcitation-ionization of D-2Phys. Rev. A 88, 062705 (2014)

e + D2 178eV E/Te + D2 178eV E/T

1301. R. Celiberto, R. K. Janev, V. Laporta, J. Tennyson, J. M. WadehraElectron-impact vibrational excitation of vibrationally excited H-2 molecules involvingthe resonant (2)Sigma(+)(g) Rydberg-excited electronic statePhys. Rev. A 88, 062701 (2014)

e + H2 0−100eV Th

1302. C. J. Bostock, C. J. Fontes, D. V. Fursa, H. L. Zhang, I. BrayCalculation of the relativistic rise in electron-impact-excitation cross sections for highlycharged ionsPhys. Rev. A 88, 012711 (2014)

e + U 0−160 keV The + Xe 0−160 keV The + Ni 0−160 keV Th

1303. T. N. Rescigno, A. E. OrelTheoretical study of excitation of the low-lying electronic states of water by electronimpactPhys. Rev. A 88, 012703 (2014)

e + H2O 9−20eV Th

1304. M. Belkhiri, M. PoirierAnalysis of density effects in plasmas and their influence on electron-impact crosssectionsPhys. Rev. A 90, 062712 (2014)

e + Al12+ 100 eV Th

1305. O. Zatsarinny, Y. Wang, K. BartschatElectron-impact excitation of argon at intermediate energiesPhys. Rev. A 89, 022706 (2014)

e + Ar 0.01−300eV The + Ar 0.01−300eV The + Ar 0.01−300eV Th

1306. M. S. PindzolaElectron-impact ionization of the inner subshells of uraniumPhys. Rev. A 90, 022708 (2014)

e + U 0−1000eV Th

1307. Y. Wang, O. Zatsarinny, K. BartschatB-spline R-matrix-with-pseudostates calculations for electron-impact excitation andionization of nitrogenPhys. Rev. A 89, 062714 (2014)

e + N 0.01−140eV The + N 0.01−140eV The + N 0.01−140eV Th

278

1308. V. Gedeon, S. Gedeon, V. Lazur, E. Nagy, O. Zatsarinny, K. BartschatB-spline R-matrix-with-pseudostates calculations for electron-impact excitation andionization of fluorinePhys. Rev. A 89, 052713 (2014)

e + F 0.01−120eV The + F 0.01−120eV The + F 0.01−120eV Th

1309. P. F. Liu, Y. P. Liu, J. L. Zeng, J. M. YuanElectron-impact excitation and single- and multiple-ionization cross sections of heavyions: Sn13+ as an examplePhys. Rev. A 89, 042704 (2014)

e + Sn13+ 0−4000eV The + Sn13+ 0−4000eV Th

1310. D. A. Little, K. Chakrabarti, Z. Mezei, I. F. Schneider, J. TennysonDissociative recombination of N-2(+) : An ab initio studyPhys. Rev. A 90, 052705 (2014)

e + N2+ 0.1−1eV Th

1311. T. M. Baumann, Z. Harman, J. Stark, C. Beilmann, G. Liang, P. H. Mokler, J. Ullrich, C. L. JoseContributions of dielectronic, trielectronic, and metastable channels to the resonantintershell recombination of highly charged silicon ionsPhys. Rev. A 90, 052704 (2014)

e + Si9+ 1330−1550eV E/Te + Si8+ 1330−1550eV E/Te + Si7+ 1330−1550eV E/Te + Si6+ 1330−1550eV E/Te + Si12+ 1330−1550eV E/Te + Si11+ 1330−1550eV E/Te + Si10+ 1330−1550eV E/T

1312. P. Defrance, J. Jureta, J. Lecointre, E. Giglio, B. Gervais, D. Cappello, I. Charpentier, P. A.HervieuxElectron-impact dissociative ionization of the molecular ion HDO+: A global viewPhys. Rev. A 90, 042704 (2014)

e + HDO+ 10−2500eV Exp

1313. Z. B. Chen, C. Z. Dong, J. JiangDominance of the Breit interaction in the cross section and circular polarization ofx-ray radiation following longitudinally-polarized-electron-impact excitation of highlycharged ionsPhys. Rev. A 90, 022715 (2014)

e + Bi79+ The + Ho53+ The + Ag43+ Th

1314. LI Maijuan, FU Yanbiao, SU Maogen, C. DONG, FUMIHIRO KoikeDielectronic Recombination of Br-Like Tungsten IonsPlasma Sci. Technol. 16, 182 (2014)

e + W39+ 1−50000eV Th

1315. X. Yu, D. HongbinAb initio Calculations of Electron-Impact Excitation Cross Sections for N-2 MoleculePlasma Sci. Technol. 16, 104 (2014)

279

e + N2 0−22eV Th

1316. V. Laporta, R. Celiberto, J. TennysonResonant vibrational-excitation cross sections and rate constants for low-energyelectron scattering by molecular oxygenPlasma Sources Sci. Technol. 22, 025001 (2014)

e + O2 0−100eV Th

1317. R Celiberto, K. L. Baluja, R. K. JanevElectron-impact state-to-state resolved cross sections and rate coefficients for the X(v)-¿ A(v ’) excitation in BeH moleculesPlasma Sources Sci. Technol. 22, 015008 (2014)

e + BeH 0−1000eV Th

1318. V Laporta, D. A. Little, R Celiberto, J TennysonElectron-impact resonant vibrational excitation and dissociation processes involvingvibrationally excited N-2 moleculesPlasma Sources Sci. Technol. 23, 065002 (2014)

e + N2 0−100eV The + N2 0−100eV Th

1319. B. GoswamiElectron impact scattering by SF6 molecule over an extensive energy rangeRsc Advances 4, 30953 (2014)

e + SF6 0.1−5000eV The + SF6 0.1−5000eV Th

1320. A. N. Zavilopulo, P. P. Markush, O. B. Shpenik, M. I. MykytaElectron-impact ionization and dissociative ionization of sulfur in the gas phaseTechnical Physics 59, 951 (2014)

e + S 0−10eV Exp

1321. O. NovotnDISSOCIATIVE RECOMBINATION MEASUREMENTS OF NH+ USING AN IONSTORAGE RINGAstrophys. J. 792, 132 (2014)

e + NH+ 1.71E−5−2EeV Exp

1322. S. S. Tayal, O. ZatsarinnyELECTRON IMPACT EXCITATION COLLISION STRENGTHS FOR EXTREMEULTRAVIOLET LINES OF Fe VIIAstrophys. J. 788, 24 (2014)

e + Fe6+ 0.01−40eV Th

1323. N. R. Badnell, C. P. BallanceELECTRON-IMPACT EXCITATION OF Fe2+: A COMPARISON OFINTERMEDIATE COUPLING FRAME TRANSFORMATION, BREIT-PAULIAND DIRAC R-MATRIX CALCULATIONSAstrophys. J. 785, 99 (2014)

e + Fe2+ 1E3−1E5 K Th

1324. D. H. Kwon, D. W. SavinELECTRON-IMPACT IONIZATION OF P-LIKE IONS FORMING Si-LIKE IONSAstrophys. J. 784, 13 (2014)

280

e + Zn15+ 1E4−1E7 K The + Cu14+ 1E4−1E7 K The + Ni13+ 1E4−1E7 K The + Co12+ 1E4−1E7 K The + Fe11+ 1E4−1E7 K The + Mn10+ 1E4−1E7 K The + Cr9+ 1E4−1E7 K The + V8+ 1E4−1E7 K The + Ti7+ 1E4−1E7 K The + Sc6+ 1E4−1E7 K The + Ca5+ 1E4−1E7 K The + K4+ 1E4−1E7 K The + Ar3+ 1E4−1E7 K The + Cl2+ 1E4−1E7 K The + P+ 1E4−1E7 K The + S+ 1E4−1E7 K Th

1325. R.P. McEachran, A.D. StaufferMomentum transfer cross sections for the heavy noble gasesEur. Phys. J. D 68, 153 (2014)

e + Ar 0.01−1000eV The + Xe 0.01−1000eV The + Xe 0.01−1000eV The + Kr 0.01−1000eV The + Kr 0.01−1000eV The + Ar 0.01−1000eV The + Ar 0.01−1000eV The + Xe 0.01−1000eV The + Xe 0.01−1000eV The + Kr 0.01−1000eV The + Kr 0.01−1000eV The + Ar 0.01−1000eV Th

1326. D. F. Pastega, R. F. Costa, M. A. Lima, M. H. BettegaElastic scattering of low-energy electrons by BF3Eur. Phys. J. D 68, 20 (2014)

e + BF3 0−10eV Th

1327. TTriple differential cross sections for the ionization of water by electron impactEur. Phys. J. D 68, 369 (2014)

e + H2O 2−20eV Th

1328. T. Das, A. D. Stauffer, R. SrivastavaA method to obtain static potentials for electron-molecule scatteringEur. Phys. J. D 68, 102 (2014)

e + H2O 30−100eV Th

1329. K. M. AggarwalEnergy levels, radiative rates and electron impact excitation rates for transitions inHe-like Fe XXV, Co XXVI, Ni XXVII, Cu XXVIII and Zn XXIXPhys. Scr. 87, 1 (2014)

e + Zn28+ 450−1300 RYD The + Cu27+ 450−1300 RYD The + Ni26+ 450−1300 RYD The + Co25+ 450−1300 RYD The + Fe24+ 450−1300 RYD Th

281

1330. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions in AlXMon. Not. R. Astron. Soc. 438, 1223 (2014)

e + Al9+ 0−350 RYD Th

1331. K. M. Aggarwal, F. P. KeenanEnergy levels, radiative rates and electron impact excitation rates for transitions in SiIIMon. Not. R. Astron. Soc. 442, 388 (2014)

e + Si+ 1E3.7−1E5.5 K Th

1332. D. D. Reid, J. M. WadehraScattering of low-energy electrons and positrons by atomic beryllium: Ramsauer-Townsend effectJ. Phys. B 47, 225211 (2014)

e + Be 1E−7−1E1 eV Th

1333. K. Scherer, H. Fichtner, H. J. Fahr, M. Bzowski, S. E. S. FerreiraIonization rates in the heliosheath and in astrosheaths Spatial dependence anddynamical relevanceAstron. Astrophys. 563, A69 (2014)

e + He 10−10000eV The + H 10−10000eV Th

1334. D. C. Nicholls, M. A. Dopita, R. S. Sutherland, L. J. Kewley, E. PalayMEASURING NEBULAR TEMPERATURES: THE EFFECT OF NEWCOLLISION STRENGTHS WITH EQUILIBRIUM AND kappa-DISTRIBUTEDELECTRON ENERGIESAstrophys. J., Suppl. Ser. 207, 21 (2014)

e + O2+ 0−40eV Th

1335. C. Mendoza, M. A. BautistaTESTING THE EXISTENCE OF NON-MAXWELLIAN ELECTRONDISTRIBUTIONS IN HII REGIONS AFTER ASSESSING ATOMIC DATAACCURACYAstrophys. J. 785, 91 (2014)

e + S+ 0−20000K The + N+ 0−20000K Th

1336. E. Yarevsky, S. L. Yakovlev, N ElanderOn the Scattering of the Electron off the Hydrogen Atom and the Helium Ion Belowand Above the Ionization Threshold: Temkin-Poet ModelFEW-BODY SYSTEMS 55, 1057 (2014)

e + He+ 40−70eV Th

1337. D.P. Kilcreasea, S. BrookesaCorrection of the near threshold behavior of electron collisional excitationcross-sections in the plane-wave Born approximationHigh En. Dens. Phys. 9, 722 (2014)

e + He+ 0−1000eV Th

282

1338. S. J. Ward, J. H. MacekEffect of a vortex in the triply differential cross section for electron-impact K-shellionization of carbonPhys. Rev. A 90, 062709 (2014)

e + C 1801eV Th

1339. X. Gao, J. M. LiPrecision spectroscopy and electron-ion scatteringPhys. Rev. A 89, 022710 (2014)

e + Kr+ 3.3eV Th

1340. Z. Hu, Y. Li, X. Han, D. Kato, X. Tong, H. Watanabe, N. NakamuraAtomic-number dependence of the magnetic-sublevel population in the autoionizationstate formed in dielectronic recombinationPhys. Rev. A 90, 062702 (2014)

e + Ho64+ 20−40keV The + Ho65+ 20−40keV The + Pr56+ 20−40keV The + Pr57+ 20−40keV Th

1341. J. L. Zeng, L. P. Liu, P. F. Liu, J. M. YuanRole of ionization-excitation processes in the cross section for direct ionization of heavyatomic ions by electron impactPhys. Rev. A 90, 044701 (2014)

e + W28+ 0−4000eV The + Yb24+ 0−4000eV The + Tb19+ 0−4000eV The + Nd14+ 0−4000eV The + Ba10+ 0−4000eV The + Sn4+ 0−4000eV The + Gd18+ 0−4000eV Th

1342. C. MerletMeasurements of absolute Ma x-ray production cross sections of heavy elements Au,Pb, Bi, and U by electron impactSurface And Interface Analysis 46, 12 (2014)

e + U 0−40keV Expe + Bi 0−40keV Expe + Pb 0−40keV Expe + Au 0−40keV Exp

1343. P. Lukac, O. Mikus, I. Morva, Z. Zabudla, J. Trnovec, M. MorvovaElectron and gas temperature dependences of the dissociative recombination coefficientof molecular ions Ar-2(+) with electronsPlasma Sources Sci. Technol. 20, 055012 (2011)

e + Ar2+ 300−10400 K E/T

1344. Sterling, N. C.Atomic data for neutron-capture elements II. Photoionization and recombinationproperties of low-charge krypton ionsAstron. Astrophys. 533, A62 (2011)

283

e + Kr2+ 1E1−1E8 K The + Kr+ 1E1−1E8 K The + Kr 1E1−1E8 K The + Kr4+ 1E1−1E8 K The + Kr3+ 1E1−1E8 K The + Kr5+ 1E1−1E8 K The + Kr6+ 1E1−1E8 K ThP + Kr 1E1−1E8 K ThP + Kr+ 1E1−1E8 K ThP + Kr2+ 1E1−1E8 K ThP + Kr3+ 1E1−1E8 K ThP + Kr4+ 1E1−1E8 K ThP + Kr5+ 1E1−1E8 K ThP + Kr6+ 1E1−1E8 K Th

1345. A. K. Bhatia, E. LandiAtomic data and spectral line intensities for Ni XIAt. Data Nucl. Data Tables 97, 50 (2011)

e + Ni10+ threshold−1000 eV Th

1346. A. K. Bhatia, E. LandiAtomic data and spectral line intensities for Ni XVIIAt. Data Nucl. Data Tables 97, 189 (2011)

e + Ni16+ threshold−1700 eV Th

1347. Landi, E.Atomic data and spectral line intensities for Fe XVAt. Data Nucl. Data Tables 97, 587 (2011)

e + Fe14+ threshold−1670 eV Th

1348. K. Ratnavelu, W. E. OngElectron and positron scattering from atomic potassiumEur. Phys. J. D 64, 269 (2011)

e + K 4−100 eV The+ + K 4−100 eV The + K 4−100 eV The+ + K 4−100 eV Th

1349. Cho, H.Low-energy Electron Scattering with CH3Cl: Comparison with the High-energyCounterpartJ. Korean Phys. Soc. 59, 30 (2011)

e + CH3Cl 5, 10, 20 eV Expe + CH3Cl 5, 10, 20 eV Exp

1350. J. H. Chin, Kuru Ratnavelu, Y. ZhouOptical Potential Study of Electron Scattering by RubidiumJ. Korean Phys. Soc. 59, 2877 (2011)

e + Rb 10−100 eV Th

1351. J. P. Sullivan, C. Makochekanwa, A. Jones, P. Caradonna, D. S. Slaughter, J. Machacek, R. P.McEachran, D. W. Mueller, S. J. BuckmanForward angle scattering effects in the measurement of total cross sections for positronscatteringJ. Phys. B 44, 035201 (2011)

284

e + Ar 0−9 eV E/Te + Xe 0−9 eV E/Te+ + Ar 0−9 eV E/Te+ + Xe 0−9 eV E/Te + Ar 0−9 eV E/Te + Xe 0−9 eV E/Te+ + Ar 0−9 eV E/Te+ + Xe 0−9 eV E/T

1352. A. Zecca, E. Trainotti, L. Chiari, G. Garcia, F. Blanco, M. H. F. Bettega, M. T. do N. Varella, M.A. P. Lima, M. J. BrungerAn experimental and theoretical investigation into positron and electron scatteringfrom formaldehydeJ. Phys. B 44, 195202 (2011)

e + CH2O 0.26−50.3 eV E/Te+ + CH2O 0.26−50.3 eV E/T

1353. Tan Xiao-Ming, Wang De-HuaTotal cross sections for electron scattering from CH3OH and CH3CH2OH moleculesin the energy range from 10 to 1000 eVNucl. Instrum. Methods Phys. Res. B 269, 1094 (2011)

e + CH3OH 10−1000 eV The + e 10−1000 eV Th

1354. A. Zecca, L. Chiari, G. Garcia, F. Blanco, E. Trainotti, M. J. BrungerTotal cross-sections for positron and electron scattering from alpha-tetrahydrofurfurylalcoholNew J. Phys. 13, 063019 (2011)

e + e 0.15−50.15 eV E/Te+ + e 0.15−50.15 eV E/T

1355. A. Zecca, L. Chiari, A. Sarkar, M. J. BrungerPositron scattering from the isoelectronic molecules N-2, CO and C2H2New J. Phys. 13, 115001 (2011)

e+ + N2 0.2−40 eV Expe+ + Co 0.2−40 eV Expe+ + C2H2 0.2−40 eV Exp

1356. A. C. L. Jones, C. Makochekanwa, P. Caradonna, D. S. Slaughter, J. R. Machacek, R. P. McEachran,J. P. Sullivan, S. J. Buckman, A. D. Stauffer, I. Bray, D. V. FursaPositron scattering from neon and argonPhys. Rev. A 83, 032701 (2011)

e+ + Ne 0.3−60 eV E/Te+ + Ar 0.3−60 eV E/T

1357. R. T. Sugohara, M. G. P. Homem, I. P. Sanches, A. F. deMoura, M. -T. Lee, I. IgaCross sections for electron scattering by methanol in the intermediate-energy rangePhys. Rev. A 83, 032708 (2011)

e + CH3OH 100−1000 eV E/Te + CH3OH 100−1000 eV E/T

1358. Denise Assafrao, H. R. J. Walters, Felipe Arretche, Adriano Dutra, J. R. MohallemSemiempirical potentials for positron scattering by atomsPhys. Rev. A 84, 022713 (2011)

285

e+ + Ne 0−200 eV The+ + Ar 0−200 eV The+ + Be 0−200 eV The+ + Mg 0−200 eV The+ + Ne 0−200 eV The+ + Ar 0−200 eV The+ + Be 0−200 eV The+ + Mg 0−200 eV Th

1359. D. A. Konovalov, D. V. Fursa, I. BrayJ-matrix calculation of electron-helium S-wave scatteringPhys. Rev. A 84, 032707 (2011)

e + He 0.1−1000 eV The + He 0.1−1000 eV The + He 0.1−1000 eV Th

1360. Mark C. Zammit, Dmitry V. Fursa, Igor Bray, R. K. JanevElectron-helium scattering in Debye plasmasPhys. Rev. A 84, 052705 (2011)

e + He threshold−1000 eV The + He threshold−1000 eV Th

1361. M. Kurokawa, M. Kitajima, K. Toyoshima, T. Kishino, T. Odagiri, H. Kato, M. Hoshino, H. Tanaka,K. ItoHigh-resolution total-cross-section measurements for electron scattering from Ar, Kr,and Xe employing a threshold-photoelectron sourcePhys. Rev. A 84, 062717 (2011)

e + Ar 7 meV− 20 eV Expe + Kr 7 meV− 20 eV Expe + Xe 7 meV− 20 eV Exp

1362. Thomas Pflueger, Arne Senftleben, Xueguang Ren, Alexander Dorn, Joachim UllrichObservation of Multiple Scattering in (e, 2e) Experiments on Small Argon ClustersPhys. Rev. Lett. 107, 223201 (2011)

e + Ar 100 eV Expe + Ar 100 eV Exp

1363. Arijit Ghoshal, Y. K. HoElastic scattering of positrons from hydrogen atoms with exponential cosine-screenedCoulomb potentialsPhys. Scr. 83, 065301 (2011)

e+ + H 20−300 eV The+ + H 20−300 eV Th

1364. Klaus Bartschat, Oleg ZatsarinnyBenchmark calculations of atomic data for plasma and lighting applicationsPlasma Sources Sci. Technol. 20, 024012 (2011)

e + Ne threshold−20 eV The + Ar threshold−20 eV The + Kr threshold−20 eV The + Xe threshold−20 eV The + Ne threshold−20 eV The + Ar threshold−20 eV The + Kr threshold−20 eV The + Xe threshold−20 eV Th

286

1365. Ghanbari-Adivi, E.Inner-shell electron capture by impact of positron on the multi-electron atomic targetsEur. Phys. J. D 62, 389 (2011)

e+ + He 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + C 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + Ne 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + Na 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + Ar 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + He 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + C 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + Ne 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + Na 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVThe+ + Ar 100−500, 600−1500, 1500−4000, 3000−5500, 8000−12500 eVTh

1366. C. Mitterdorfer, A. Edtbauer, S. Karolczak, J. Postler, D. Gschliesser, S. Denifl, E. Illenberger, P.ScheierStrong fragmentation processes driven by low energy electron attachment to varioussmall perfluoroether moleculesInt. J. Mass Spectrom. 306, 63 (2011)

e + e 0−15 eV Exp

3.2.2 Heavy Particles Collisions

1367. Hui-Ping Liu, Xiao-Ping Ouyang, Hua-Si Hu, al. etSingle electron loss in the collisions of C3+ and atomic hydrogenChin. Phys. B 19, 093401 (2010)

C3+ + H 0−700keV/u Th

1368. Xue-Rong Wang, Ling Liu, Jian-Guo WangElectron Capture Process in Collisions of Proton with Excited State of HeliumChin. Phys. Lett. 27, 123401 (2010)

H+ + He 1−100keV/u Th

1369. L. F. Errea, Clara Illescas, A. Macias, al. etInfluence of nuclear exchange on nonadiabatic electron processes in H++H-2 collisionsJ. Chem. Phys. 133, 244307 (2010)

H+ + H2 5−600eV Th

1370. F. Guzman, L. F. Errea, Clara Illescas, al. etCalculation of total cross sections and effective emission coefficients for B5+ collisionswith ground-state and excited hydrogenJ. Phys. B 43, 144007 (2010)

B5+ + H 0.1− 200keV/amu Th

1371. C. C. Montanari, E. C. Montenegro, J. E. MiragliaCDW-EIS calculations for multiple ionization of Ne, Ar, Kr and Xe by the impact ofH+ and He+, including post-collisional electron emissionJ. Phys. B 43, 165201 (2010)

He+ + Kr 10 − 1000keV/amu ThHe+ + Xe 10 − 1000keV/amu ThHe+ + Ar 10 − 1000keV/amu ThHe+ + Ne 10 − 1000keV/amu ThH+ + Kr 10 − 1000keV/amu ThH+ + Xe 10 − 1000keV/amu ThH+ + Ar 10 − 1000keV/amu ThH+ + Ne 10 − 1000keV/amu Th

287

1372. Keh-Ning Huang, Hsiao-Ling Sun, Sheng-Fang Lin, Hao-Tse Shiao, Xin-Zeng WuRelativistic Quantum Collision Theory for Many-particle SystemsJ. Korean Phys. Soc. 59, 2941 (2011)

H+ + U91+ 1−15 threshold unit, 1−2000 keVThe + U91+ 1−15 threshold unit, 1−2000 keVTh

1373. J. Colgan, M. S. Pindzola, F. Robicheaux, M. F. CiappinaFully differential cross sections for the single ionization of He by C6+ ionsJ. Phys. B 44, 175205 (2011)

C6+ + He 100 MeV ThC6+ + He 100 MeV Th

1374. M. S. Pindzola, T. G. Lee, J. ColganAntiproton-impact ionization of H, He and LiJ. Phys. B 44, 205204 (2011)

H− + Li 0−100 keV ThH− + He 0−100 keV ThH− + H 0−100 keV Th

1375. S. Otranto, R. E. OlsonX-ray emission cross sections following Ar18+ charge-exchange collisions on neutralargon: The role of the multiple electron capturePhys. Rev. A 83, 032710 (2011)

Ar18+ + Ar 5−4000 eV Th

1376. U. Chowdhury, M. Schulz, D. H. MadisonDifferential cross sections for single ionization of H-2 by 75-keV proton impactPhys. Rev. A 83, 032712 (2011)

H+ + H2 75 keV ThH+ + H2 75 keV Th

1377. S. D. Lopez, M. Fiori, C. R. GaribottiAnalysis of the approximations applied in thecontinuum-distorted-wave-eikonal-initial-state theory for the evaluation of ionizationcross sections: Post-prior discrepancy, axial symmetry, and ion-ion interactionPhys. Rev. A 83, 032716 (2011)

H+ + He 100−1000 eV Th

1378. S. D. Lopez, C. R. Garibotti, S. OtrantoDouble ionization of helium by bare ions: Theoretical study of the fully differentialcross sectionsPhys. Rev. A 83, 062702 (2011)

Li3+ + He 700−1000 keV ThHe2+ + He 700−1000 keV ThC6+ + He 700−1000 keV ThH− + He 700−1000 keV ThH+ + He 700−1000 keV ThLi3+ + He 700−1000 keV ThHe2+ + He 700−1000 keV ThC6+ + He 700−1000 keV ThH− + He 700−1000 keV ThH+ + He 700−1000 keV Th

288

1379. P. Botheron, B. PonsClassical interpretation of probability oscillations in low-energy atomic collisionsPhys. Rev. A 83, 062704 (2011)

H+ + H 1−100 keV ThH2+ + H 1−100 keV Th

1380. A. Dubois, S. Carniato, P. D. Fainstein, J. P. HansenIonization of water molecules by fast charged projectilesPhys. Rev. A 84, 012708 (2011)

H+ + H2O 100−1000 keV Th

1381. Y. Iriki, Y. Kikuchi, M. Imai, A. ItohAbsolute doubly differential cross sections for ionization of adenine by 1.0-MeV protonsPhys. Rev. A 84, 032704 (2011)

H+ + H 1.0 MeV ExpH+ + H 1.0 MeV Exp

1382. A. N. Artemyev, S. R. McConnell, A. Surzhykov, B. Najjari, A. B. VoitkivCoulomb excitation of highly charged projectile ions in relativistic collisions withdiatomic moleculesPhys. Rev. A 84, 042709 (2011)

N2 + U91+ 300−1000 MeV ThN2 + Fe25+ 300−1000 MeV ThN2 + Xe53+ 300−1000 MeV Th

1383. R. J. Mawhorter, J. B. Greenwood, A. Chutjian, T. Haley, C. D. Mitescu, J. SimcicMeasurement of absolute charge-exchange cross sections for He2+ collisions with Heand H-2Phys. Rev. A 84, 052714 (2011)

He2+ + H2 0.3−4.6 keV E/THe2+ + He 0.3−4.6 keV E/T

1384. Y. Iriki, Y. Kikuchi, M. Imai, A. ItohProton-impact ionization cross sections of adenine measured at 0.5 and 2.0 MeV byelectron spectroscopyPhys. Rev. A 84, 052719 (2011)

P + P 0.5−2 MeV E/T

1385. Nicolas Sisourat, Ingjald Pilskog, Alain DuboisNonperturbative treatment of multielectron processes in ion-molecule scattering:Application to He2+-H-2 collisionsPhys. Rev. A 84, 052722 (2011)

He2+ + H2 0.01−25 keV Th

1386. I. B. Abdurakhmanov, A. S. Kadyrov, D. V. Fursa, I. Bray, A. T. StelbovicsConvergent close-coupling calculations of helium single ionization by antiproton impactPhys. Rev. A 84, 062708 (2011)

H− + He 1−1000 keV Th

1387. O. Abu-Haija, A. Hasan, A. Kayani, E. Y. KamberState-selective single- and double-electron capture in slow collisions of Ne4+ ions withCO2Phys. Scr. T144, 014017 (2011)

289

Ne4+ + CO2 60−1200 eV E/T

1388. O. Abu-Haija, A. Hasan, A. Kayani, E. Y. KamberElectron capture processes in slow collisions of Ne6+ ions with CO2 and H2OEurophys. Lett. 93, 13003 (2011)

Ne6+ + CO2 450−2400 eV E/TNe6+ + H2O 450−2400 eV E/T

1389. M. N. Guimaraes, F. V. PrudenteA variational adiabatic hyperspherical finite element R matrix methodology: generalformalism and application to H+H-2 reactionEur. Phys. J. D 64, 287 (2011)

H + H2 0.5−1.4 eV Th

1390. J. Perez-Rios, G. Tejeda, J. M. Fernandez, M. I. Hernandez, S. MonteroInelastic collisions in molecular oxygen at low temperature (4 ¡= T ¡= 34 K). Close-coupling calculations versus experimentJ. Chem. Phys. 134, 174307 (2011)

O2 + O2 4−34 K E/T

1391. I. B. Abdurakhmanov, A. S. Kadyrov, I. Bray, A. T. StelbovicsDifferential ionization in antiproton-hydrogen collisions within the convergent-close-coupling approachJ. Phys. B 44, 165203 (2011)

H− + H 30−500, 30−200 keV ThH− + H 30−500, 30−200 keV Th

1392. Teck-Ghee Lee, M. S. PindzolaProton-impact excitation of lithium using a time-dependent close-coupling methodPhys. Rev. A 84, 052712 (2011)

H+ + Li 0−50 keV Th

3.3 Surface Interactions

1393. P. Wang, W. Jacob, M. Balden, A. Manhard, T. Schwarz-SelingerErosion of tungsten-doped amorphous carbon films in oxygen plasmaJ. Nucl. Mater. 420, 101 (2012)

D+ + W 30−100 eV, T: 350K ExpD2

+ + W 30−100 eV, T: 350K ExpD3

+ + W 30−100 eV, T: 350K ExpD+ + C 30−100 eV, T: 350K ExpD2

+ + C 30−100 eV, T: 350K ExpD3

+ + C 30−100 eV, T: 350K Exp

1394. K. Tokunaga, M. J. Baldwin, R. P. Doerner, D. Nishijima, H. Kurishita, T. Fujiwara, K. Araki, Y.Miyamoto, N. Ohno, Y. UedaNanoscale surface morphology of tungsten materials induced by Be-seeded D-Heplasma exposureJ. Nucl. Mater. 417, 528 (2011)

He + W 60eV, T: 1123K ExpD + W 60eV, T: 1123K ExpBe + W 60eV, T: 1123K Exp

290

1395. A. Lasa, C. Bjorkas, K. Vortler, K. NordlundMD simulations of low energy deuterium irradiation on W, WC and W2C surfacesJ. Nucl. Mater. 429, 284 (2012)

D + WC 10−1000eV, T: 300−600K ThD + W 10−1000eV, T: 300−600K ThD + W2C 10−1000eV, T: 300−600K ThD + W2C 10−1000eV, T: 300−600K ThD + WC 10−1000eV, T: 300−600K ThD + W 10−1000eV, T: 300−600K ThD + W2C 10−1000eV, T: 300−600K ThD + WC 10−1000eV, T: 300−600K ThD + W 10−1000eV, T: 300−600K ThD + W2C 10−1000eV, T: 300−600K ThD + WC 10−1000eV, T: 300−600K ThD + W 10−1000eV, T: 300−600K ThD + W2C 10−1000eV, T: 300−600K ThD + WC 10−1000eV, T: 300−600K ThD + W 10−1000eV, T: 300−600K Th

1396. Martin Nieto-Perez, G. Ramos, Jean Paul AllainModeling of Surface Composition Dynamics in the ITER Divertor RegionIEEE Trans. Plasma Sci. 38, 414 (2010)

D + C 10−250eV, T: undef ThBe + C 10−250eV, T: undef ThD + C 10−250eV, T: undef ThC + Be 10−250eV, T: undef ThBe + Be 10−250eV, T: undef ThD + Be 10−250eV, T: undef ThC + C 10−250eV, T: undef ThBe + C 10−250eV, T: undef ThBe + Be 10−250eV, T: undef ThD + Be 10−250eV, T: undef ThC + C 10−250eV, T: undef ThC + Be 10−250eV, T: undef ThBe + Be 10−250eV, T: undef ThD + Be 10−250eV, T: undef ThC + C 10−250eV, T: undef ThBe + C 10−250eV, T: undef ThD + C 10−250eV, T: undef ThC + Be 10−250eV, T: undef ThD + C 10−250eV, T: undef ThBe + C 10−250eV, T: undef ThD + C 10−250eV, T: undef ThC + Be 10−250eV, T: undef ThBe + Be 10−250eV, T: undef ThD + Be 10−250eV, T: undef ThC + C 10−250eV, T: undef ThBe + C 10−250eV, T: undef ThC + Be 10−250eV, T: undef ThBe + Be 10−250eV, T: undef ThD + Be 10−250eV, T: undef ThC + C 10−250eV, T: undef ThBe + C 10−250eV, T: undef ThD + C 10−250eV, T: undef ThC + Be 10−250eV, T: undef ThBe + Be 10−250eV, T: undef ThD + Be 10−250eV, T: undef ThC + C 10−250eV, T: undef Th

291

1397. Ch. Linsmeier, M. Reinelt, K. SchmidSurface chemistry of first wall materials - From fundamental data to modelingJ. Nucl. Mater. 415, S212 (2011)

Be + W undef, T: 670−1470K E/TC + W undef, T: 670−1470K E/TBe + W undef, T: 670−1470K E/TC + W undef, T: 670−1470K E/T

1398. J. N. Brooks, J. P. Allain’Mixed-material evolution analysis of the ITER divertor’J. Nucl. Mater. 390-91, 123 (2009)

D + W 10−1000eV, T: undef ThD + Be 10−1000eV, T: undef Th

1399. Shin Kajita, Daisuke Nishijima, Russ Doerner, Karl Umstadter, Jonathan Yu, Noriyasu Ohno,Yoshio UedaBeryllium erosion induced by transient heat loads and subsequent reactions in adeuterium plasmaJ. Nucl. Mater. 420, 252 (2012)

D + Be ¡80eV, T: 800−2000K Exp

1400. M. F. Stamp, K. Krieger, S. BrezinsekMeasurements of beryllium sputtering yields at JETJ. Nucl. Mater. 415, S173 (2011)

Be + Be 10−1000eV, T: undef E/TD + Be 10−1000eV, T: undef E/T

1401. M. Mehine, C. Bjorkas, K. Vortler, K. Nordlund, M. I. AirilaModelling the erosion of beryllium carbide surfacesJ. Nucl. Mater. 414, 1 (2011)

Be + Be 10−100eV, T: 300K ThD + Be 10−100eV, T: 300K ThD + Be2C 10−100eV, T: 300K Th

1402. Liudvikas Pranevicius, Liudas Pranevicius, Andrius Martinavicius, Arvydas Kanapickas, ClaudeTemplierStudies of carbon behavior in tungsten under carbon and hydrogen mixed irradiationVacuum 83, S45 (2009)

H2 + C 300eV, T: 400K ExpH2 + W 300eV, T: 400K ExpAr + C 300eV, T: 400K ExpAr + W 300eV, T: 400K ExpAr + W 300eV, T: 400K ExpH2 + C 300eV, T: 400K ExpH2 + W 300eV, T: 400K ExpAr + C 300eV, T: 400K Exp

1403. E. Vassallo, M. Canetti, A. Cremona, F. Ghezzi, G. Grosso, L. LaguardiaEvaluation of a method to reduce the redeposition of hydrogenated coatings containingcarbon and tungsten in fusion reactorsVacuum 86, 1528 (2012)

292

Ar + W undef, T: undef ExpAr + W undef, T: undef ExpCH4 + W undef, T: undef ExpH2 + W undef, T: undef ExpAr + C undef, T: undef ExpCH4 + C undef, T: undef ExpH2 + C undef, T: undef ExpAr + H undef, T: undef ExpCH4 + H undef, T: undef ExpH2 + H undef, T: undef ExpH2 + H undef, T: undef ExpCH4 + H undef, T: undef ExpAr + H undef, T: undef ExpH2 + C undef, T: undef ExpCH4 + C undef, T: undef ExpAr + C undef, T: undef ExpH2 + W undef, T: undef ExpCH4 + W undef, T: undef Exp

1404. P. Wang, W. Jacob, M. Balden, T. Hoeschen, A. ManhardErosion of tungsten-doped amorphous carbon films exposed to deuterium plasmasJ. Nucl. Mater. 426, 277 (2012)

D+ + W 30−300eV, T: 300K ExpD2

+ + W 30−300eV, T: 300K ExpD3

+ + W 30−300eV, T: 300K ExpD+ + C 30−300eV, T: 300K ExpD2

+ + C 30−300eV, T: 300K ExpD3

+ + C 30−300eV, T: 300K Exp

1405. A. Kallenbach, M. Balden, R. Dux, T. Eich, C. Giroud, A. Huber, G. P. Maddison, M. Mayer, K.McCormick, R. Neu, T. W. Petrie, T. Puetterich, J. Rapp, M. L. Reinke, K. Schmid, J. Schweinzer,S. WolfePlasma surface interactions in impurity seeded plasmasJ. Nucl. Mater. 415, S19 (2011)

D + W 2−2000eV, T: undef ThHe + W 2−2000eV, T: undef ThC + W 2−2000eV, T: undef ThN + W 2−2000eV, T: undef ThNe + W 2−2000eV, T: undef ThAr + W 2−2000eV, T: undef ThKr + W 2−2000eV, T: undef Th

1406. T. Dittmar, M. J. Baldwin, R. P. Doerner, D. Nishijima, M. Oberkofler, T. Schwarz-Selinger, F.TabaresInteraction of high flux deuterium/nitrogen plasmas with berylliumPhys. Scr. T145, 14009 (2011)

N2 + Be 30−95eV, T: 310−420K ExpD2 + Be 30−95eV, T: 310−420K ExpN2 + Be 30−95eV, T: 310−420K ExpD2 + Be 30−95eV, T: 310−420K ExpN2 + Be 30−95eV, T: 310−420K ExpD2 + Be 30−95eV, T: 310−420K ExpN2 + Be 30−95eV, T: 310−420K ExpD2 + Be 30−95eV, T: 310−420K ExpN2 + Be 30−95eV, T: 310−420K ExpD2 + Be 30−95eV, T: 310−420K Exp

293

1407. Y. Ueda, K. Miyata, Y. Ohtsuka, H. T. Lee, M. Fukumoto, S. Brezinsek, J. W. Coenen, A. Kreter,A. Litnovsky, V. Philipps, B. Schweer, G. Sergienko, T. Hirai, A. Taguchi, Y. Torikai, K. Sugiyama,T. Tanabe, S. Kajita, N. OhnoExposure of tungsten nano-structure to TEXTOR edge plasmaJ. Nucl. Mater. 415, S92 (2011)

D + W 160−320eV, T: 570−1070K ExpHe + W 160−320eV, T: 570−1070K ExpD + W 160−320eV, T: 570−1070K ExpHe + W 160−320eV, T: 570−1070K ExpD + W 160−320eV, T: 570−1070K ExpHe + W 160−320eV, T: 570−1070K ExpD + W 160−320eV, T: 570−1070K ExpHe + W 160−320eV, T: 570−1070K ExpD + W 160−320eV, T: 570−1070K ExpHe + W 160−320eV, T: 570−1070K Exp

1408. S. Brezinsek, D. Borodin, J. W. Coenen, D. Kondratjew, M. Laengner, A. Pospieszczyk, U. SammQuantification of tungsten sputtering at W/C twin limiters in TEXTOR with the aidof local WF6 injectionPhys. Scr. T145, 14016 (2011)

H + W 30−85eV(Te), T: 420K ExpD + W 30−85eV(Te), T: 420K ExpH + C 30−85eV(Te), T: 420K ExpD + C 30−85eV(Te), T: 420K Exp

1409. A. Widdowson, M. J. Baldwin, J. P. Coad, R. P. Doerner, J. Hanna, D. E. Hole, G. F. Matthews,M. Rubel, R. Seraydarian, H. XuTesting of beryllium marker coatings in PISCES-B for the JET ITER-like wallJ. Nucl. Mater. 390-91, 988 (2009)

D + Be 30eV, T: 700−900K Exp

1410. K. Vortler, C. Bjorkas, K. NordlundThe effect of plasma impurities on the sputtering of tungsten carbideJ. Phys. Condens. Matter 23, 85002 (2011)

D + WC 100−300eV, T: 600K ThC + WC 100−300eV, T: 600K ThW + WC 100−300eV, T: 600K ThHe + WC 100−300eV, T: 600K ThNe + WC 100−300eV, T: 600K ThAr + WC 100−300eV, T: 600K Th

1411. P. Sundelin, C. Schulz, V. Philipps, M. Rubel, G. Sergienko, L. MarotNitrogen-assisted removal of deuterated carbon layersJ. Nucl. Mater. 390-91, 647 (2009)

H2 + C undef, T: 300−600K ExpH2 + D undef, T: 300−600K ExpN2 + C undef, T: 300−600K ExpN2 + D undef, T: 300−600K ExpH2 + B undef, T: 300−600K ExpN2 + B undef, T: 300−600K Exp

1412. K. Nordlund, C. Bjorkas, K. Vortler, A. Meinander, A. Lasa, M. Mehine, A. V. KrasheninnikovMechanism of swift chemical sputtering: Comparison of Be/C/W dimer bond breakingNucl. Instrum. Methods Phys. Res. B 269, 1257 (2011)

294

D + Be 2−200eV, T: 300K ThD + Be2C 2−200eV, T: 300K ThD + WC 2−200eV, T: 300K ThD + C 2−200eV, T: 300K Th

1413. M. Tokitani, N. Yoshida, S. Masuzaki, N. Noda, A. Sagara, H. Yamada, A. Komori, S. Nagata, B.TsuchiyaPlasma surface interaction on the surface of tungsten divertor tiles in LHDJ. Nucl. Mater. 415, S87 (2011)

H + W ¡100eV, T: undef ExpH + W ¡100eV, T: undef ExpH + W ¡100eV, T: undef ExpH + W ¡100eV, T: undef ExpH + W ¡100eV, T: undef Exp

1414. K. OhyaModeling of Erosion and Deposition on Plasma Facing WallsAIP Conf. Proc. 1237, 47 (2010)

CH4 + C 3−100eV, T: undef ThCH4 + W 3−100eV, T: undef ThCH4 + H 3−100eV, T: undef ThC2H6 + C 3−100eV, T: undef ThC2H6 + H 3−100eV, T: undef ThCH4 + C 3−100eV, T: undef ThCH4 + W 3−100eV, T: undef ThCH4 + H 3−100eV, T: undef ThC2H6 + C 3−100eV, T: undef ThC2H6 + H 3−100eV, T: undef Th

1415. C. Bjorkas, K. Vortler, K. Nordlund, D. Nishijima, R. DoernerChemical sputtering of Be due to D bombardmentNew J. Phys. 11, 123017 (2009)

D + Be 7−3000eV, T: 373K E/T

1416. A. Kreter, D. Nishijima, M. J. Baldwin, R. P. Doerner, A. PospieszczykMitigation of carbon erosion in beryllium seeded deuterium plasma underbombardment by argon and helium ions in PISCES-BJ. Nucl. Mater. 417, 651 (2011)

D + C 30−126eV, T: 700K ExpBe + C 30−126eV, T: 700K ExpHe + C 30−126eV, T: 700K ExpAr + C 30−126eV, T: 700K Exp

1417. Predrag S. Krstic, Carlos O. ReinholdBurning Plasma - Wall InteractionsAIP Conf. Proc. 1161, 75 (2009)

D2 + C 2−60eV, T: undef E/TD2 + C 2−60eV, T: undef E/TD2 + C 2−60eV, T: undef E/TD2 + C 2−60eV, T: undef E/TD2 + C 2−60eV, T: undef E/T

1418. S. Khakshouri, D. M. DuffyInfluence of electronic effects on the surface erosion of tungstenPhys. Rev. B 80, 35415 (2009)

295

W + W 5000eV, T: 300K Th

1419. Shengguang Liu, Jizhong Sun, Shuyu Dai, Thomas Stirner, Dezhen WangA general model for chemical erosion of carbon materials due to low-energy H+ impactJ. Appl. Phys. 108, 73302 (2010)

H+ + C 25−200eV, T: 300−1000K Th

1420. Q Xu, K Ohya, ZS Yang, K Inai, GN LuoMonte Carlo simulation of erosion and deposition behavior on SiC-coated graphitetiles in EASTJ. Nucl. Mater. 415, S153 (2011)

H + SiC 20eV(Te), T: undef ThH + C 20eV(Te), T: undef ThH + SiC 20eV(Te), T: undef ThH + C 20eV(Te), T: undef Th

1421. K. R. Umstadter, R. Doerner, G. TynanEnhanced erosion of tungsten plasma-facing components subject to simultaneous heatpulses and deuterium plasmaJ. Nucl. Mater. 386-88, 751 (2009)

H+ + W 50−250eV, T: 320−370K ExpD+ + W 50−250eV, T: 320−370K Exp

1422. GR. Tynan, M. Baldwin, R. Doerner, E. Hollmann, D. Nishijima, K. Umstadter, J YuMixed Material Plasma-Surface Interactions in ITER: Recent Results from thePISCES GroupAIP Conf. Proc. 1237, 78 (2010)

D + W 15−70eV, T: 293−1100K ExpD + Be 15−70eV, T: 293−1100K ExpHe + W 15−70eV, T: 293−1100K ExpD + W 15−70eV, T: 293−1100K ExpHe + W 15−70eV, T: 293−1100K ExpD + Be 15−70eV, T: 293−1100K ExpD + W 15−70eV, T: 293−1100K ExpHe + W 15−70eV, T: 293−1100K ExpD + Be 15−70eV, T: 293−1100K ExpD + W 15−70eV, T: 293−1100K ExpD + Be 15−70eV, T: 293−1100K ExpBe + W 15−70eV, T: 293−1100K ExpD + Be 15−70eV, T: 293−1100K ExpHe + W 15−70eV, T: 293−1100K Exp

1423. A. Kirschner, D. Borodin, V. Philipps, U. Samm, R. Ding, K. Schmid, J. Roth, A. Kukushkin, G.Federici, A LoarteEstimations of erosion fluxes, material deposition and tritium retention in the divertorof ITERJ. Nucl. Mater. 390-91, 152 (2009)

T + C undef, T: undef ThT + Be undef, T: undef ThT + C undef, T: undef ThT + Be undef, T: undef ThT + C undef, T: undef ThT + Be undef, T: undef ThT + C undef, T: undef ThT + Be undef, T: undef Th

296

1424. K OhyaProgress in modeling erosion and redeposition on plasma facing materialsJ. Nucl. Mater. 415, S10 (2011)

C + W 1−100eV, T: undef ThD + W 1−100eV, T: undef ThCH4 + C 1−100eV, T: undef ThC + C 1−100eV, T: undef ThD + C 1−100eV, T: undef ThCH4 + C 1−100eV, T: undef ThC + C 1−100eV, T: undef ThD + C 1−100eV, T: undef ThC + W 1−100eV, T: undef ThD + W 1−100eV, T: undef ThH + H 1−100eV, T: undef ThH + C 1−100eV, T: undef ThBe + H 1−100eV, T: undef ThBe + C 1−100eV, T: undef ThCH4 + W 1−100eV, T: undef ThCH4 + H 1−100eV, T: undef ThD + W 1−100eV, T: undef ThH + H 1−100eV, T: undef ThH + C 1−100eV, T: undef ThBe + H 1−100eV, T: undef ThBe + C 1−100eV, T: undef ThCH4 + W 1−100eV, T: undef ThCH4 + H 1−100eV, T: undef ThC + C 1−100eV, T: undef ThD + C 1−100eV, T: undef ThC + W 1−100eV, T: undef ThCH4 + W 1−100eV, T: undef ThCH4 + H 1−100eV, T: undef ThCH4 + C 1−100eV, T: undef ThD + C 1−100eV, T: undef ThC + W 1−100eV, T: undef ThD + W 1−100eV, T: undef ThH + H 1−100eV, T: undef ThH + C 1−100eV, T: undef ThBe + H 1−100eV, T: undef ThBe + C 1−100eV, T: undef ThCH4 + H 1−100eV, T: undef ThCH4 + C 1−100eV, T: undef ThC + C 1−100eV, T: undef ThBe + H 1−100eV, T: undef ThBe + C 1−100eV, T: undef ThCH4 + W 1−100eV, T: undef ThC + W 1−100eV, T: undef ThD + W 1−100eV, T: undef ThH + H 1−100eV, T: undef ThH + C 1−100eV, T: undef ThCH4 + C 1−100eV, T: undef ThC + C 1−100eV, T: undef ThD + C 1−100eV, T: undef ThH + H 1−100eV, T: undef ThH + C 1−100eV, T: undef ThBe + H 1−100eV, T: undef ThBe + C 1−100eV, T: undef ThCH4 + W 1−100eV, T: undef ThCH4 + H 1−100eV, T: undef Th

297

1425. D. Borodin, R. Doerner, D. Nishijima, A. Kirschner, A. Kreter, D. Matveev, A. Galonska, V PhilippsSimulation of Be-C interaction dynamics in mixed Be/C layers formed in experimentsat PISCES-BJ. Nucl. Mater. 415, S219 (2011)

D + C 7eV(Te), T: undef ThBe + C 7eV(Te), T: undef ThD + C 7eV(Te), T: undef ThBe + C 7eV(Te), T: undef Th

1426. AY. Pigarov, P. Krstic, SI. Krasheninnikov, R. Doerner, TD RognlienDynamic Models for Plasma-Wall InteractionsContrib. Plasma Phys. 52, 465 (2012)

D + C 1−100eV, T: 300−900K ThD + Be 1−100eV, T: 300−900K ThD + C 1−100eV, T: 300−900K ThD + Be 1−100eV, T: 300−900K ThD + C 1−100eV, T: 300−900K ThD + Be 1−100eV, T: 300−900K ThD + C 1−100eV, T: 300−900K ThD + Be 1−100eV, T: 300−900K ThD + C 1−100eV, T: 300−900K ThD + Be 1−100eV, T: 300−900K ThD + C 1−100eV, T: 300−900K ThD + Be 1−100eV, T: 300−900K Th

1427. D. Nishijima, MJ. Baldwin, RP. Doerner, JH YuSputtering properties of tungsten ’fuzzy’ surfacesJ. Nucl. Mater. 415, S96 (2011)

Ar + W 30−120eV, T: undef Exp

1428. A. Vesel, M. Mozetic, P. Panjan, N. Hauptman, M. Klanjsek-Gunde, M Balat-PichelinEtching of carbon-tungsten composite with oxygen plasmaSurf. Coat. Tech. 204, 1503 (2010)

O + WC undef, T: 800K ExpO + C undef, T: 800K Exp

1429. J. Roth, E. Tsitrone, A. Loarte, T. Loarer, G. Counsell, R. Neu, V. Philipps, S. Brezinsek, M.Lehnen, P. Coad, C. Grisolia, K. Schmid, K. Krieger, A. Kallenbach, B. Lipschultz, R. Doerner, R.Causey, V. Alimov, W. Shu, O. Ogorodnikova, A. Kirschner, G. Federici, A KukushkinRecent analysis of key plasma wall interactions issues for ITERJ. Nucl. Mater. 390-91, 1 (2009)

D + Be 1−1000eV, T: 300−900K E/TD + W 1−1000eV, T: 300−900K E/TAr + W 1−1000eV, T: 300−900K E/TD + C 1−1000eV, T: 300−900K E/TD + W 1−1000eV, T: 300−900K E/TD + Be 1−1000eV, T: 300−900K E/TD + C 1−1000eV, T: 300−900K E/TD + BeC 1−1000eV, T: 300−900K E/TD + W 1−1000eV, T: 300−900K E/TD + Be 1−1000eV, T: 300−900K E/TD + C 1−1000eV, T: 300−900K E/TD + WC 1−1000eV, T: 300−900K E/TD + BeO 1−1000eV, T: 300−900K E/TD + BeC 1−1000eV, T: 300−900K E/T

298

D + BeO 1−1000eV, T: 300−900K E/TD + BeC 1−1000eV, T: 300−900K E/TD + W 1−1000eV, T: 300−900K E/TD + Be 1−1000eV, T: 300−900K E/TD + C 1−1000eV, T: 300−900K E/TD + WC 1−1000eV, T: 300−900K E/TD + BeO 1−1000eV, T: 300−900K E/TD + Be 1−1000eV, T: 300−900K E/TD + C 1−1000eV, T: 300−900K E/TD + WC 1−1000eV, T: 300−900K E/TD + BeO 1−1000eV, T: 300−900K E/TD + BeC 1−1000eV, T: 300−900K E/TD + W 1−1000eV, T: 300−900K E/TD + WC 1−1000eV, T: 300−900K E/T

1430. Y. Igitkhanov, B BazylevEvaluation of energy and particle impact on the plasma facing components in DEMOFusion Eng. Des. 87, 520 (2012)

D + W 10−1000eV, T: undef ThHe + W 10−1000eV, T: undef ThT + W 10−1000eV, T: undef Th

1431. K. Dobes, P. Naderer, C. Hopf, T. Schwarz-Selinger, F AumayrTransient effects during sputtering of a-C:H surfaces by nitrogen ionsNucl. Instrum. Methods Phys. Res. B 286, 20 (2012)

N2 + H 500−1000eV, T: 460K ExpN2 + C 500−1000eV, T: 460K Exp

1432. BI. Khripunov, A. Brukhanov, OK. Chugunov, VM. Gureev, VS. Koidan, SN. Kornienko, BV.Kuteev, ST. Latushkin, AM. Muksunov, VB. Petrov, AI. Ryazanov, EV. Semenov, VP. Smirnov,VG. Stolyarova, VN UnezhevEvidence of radiation damage impact on material erosion in plasma environmentJ. Nucl. Mater. 390-91, 921 (2009)

D + W 100−250eV, T: 300K ExpD + C 100−250eV, T: 300K Exp

1433. C. Bjorkas, N. Juslin, H. Timko, K. Vortler, K. Nordlund, K. Henriksson, P ErhartInteratomic potentials for the Be-C-H systemJ. Phys. Condens. Matter 21, 445002 (2009)

Be + Be 20−500eV, T: 320−670K E/TBe + Be 20−500eV, T: 320−670K E/T

1434. MA El FqihAngular distribution of sputtered alloy. Experimental and simulated studyEur. Phys. J. D 56, 167 (2010)

Kr + CuBe 2000−10000eV, T: undef E/T

1435. K. Bystrov, J. Westerhout, M. Matveeva, A. Litnovsky, L. Marot, E. Zoethout, G De TemmermanErosion yields of carbon under various plasma conditions in Pilot-PSIJ. Nucl. Mater. 415, S149 (2011)

H + B 1−75eV, T: 900−2000K ExpH + C 1−75eV, T: 900−2000K Exp

299

1436. AG. McLean, PC. Stangeby, BD. Bray, S. Brezinsek, NH. Brooks, JW. Davis, RC. Isler, A.Kirschner, R. Laengner, CJ. Lasnier, Y. Mu, J. Munoz, DL. Rudakov, O. Schmitz, EA. Unterberg,JG. Watkins, DG. Whyte, CPC WongQuantification of chemical erosion in the DIII-D divertor and implications for ITERJ. Nucl. Mater. 415, S141 (2011)

D + C 15−200eV, T: 300−1000K Exp

1437. V. Liechtenstein, V. Jaggi, E. Olshanski, JA. Scheer, P. Wurz, SK ZeislerInvestigation of sputtering of thin diamond-like carbon (DLC) target foils by lowenergy light ionsNucl. Instrum. Methods Phys. Res. A 613, 429 (2010)

T + C 1000−4000eV, T: undef ExpHe + C 1000−4000eV, T: undef ExpH + C 1000−4000eV, T: undef ExpD + C 1000−4000eV, T: undef Exp

1438. BI. Khripunov, AN. Brukhanov, VM. Gureev, VS. Koidan, SN. Kornienko, ST. Latushkin, VB.Petrov, AI. Ryazanov, EV. Semenov, VG. Stolyarova, VN. Unezhev, LS. Danelyan, VS.Kulikauskas, VV. Zatekin, VG. Vostrikov, EA RomanovskyPlasma effect on tungsten damaged by high-energy alpha particles: Erosion anddeuterium trappingJ. Nucl. Mater. 415, S649 (2011)

D + W 250eV, T: 400K ExpD + W 250eV, T: 400K ExpD + W 250eV, T: 400K ExpD + W 250eV, T: 400K ExpD + W 250eV, T: 400K Exp

1439. T. Sizyuk, A HassaneinDynamic analysis and evolution of mixed materials bombarded with multiple ionsbeamsJ. Nucl. Mater. 404, 60 (2010)

H + W 333−1000eV, T: 1000−1050K E/TC + W 333−1000eV, T: 1000−1050K E/TH + W 333−1000eV, T: 1000−1050K E/TC + W 333−1000eV, T: 1000−1050K E/T

1440. J. Westerhout, D. Borodin, RS. Al, S. Brezinsek, MHJ. ’t Hoen, A. Kirschner, S. Lisgo, HJ. vander Meiden, V. Philipps, MJ. van de Pol, AE. Shumack, G. De Temmerman, WAJ. Vijvers, GM.Wright, NJL. Cardozo, J. Rapp, GJ van RooijChemical erosion of different carbon composites under ITER-relevant plasmaconditionsPhys. Scr. T138, 014017 (2009)

H2 + C 0.1−2.4eV(Te), T: ¡1000K Exp

1441. JZ. Sun, SY. Li, T. Stirner, JL. Chen, DZ WangMolecular dynamics simulation of energy exchanges during hydrogen collision withgraphite sheetsJ. Appl. Phys. 107, 113533 (2010)

H + C 0.35−200eV, T: undef ThH + C 0.35−200eV, T: undef ThH + C 0.35−200eV, T: undef Th

300

1442. C. Pardanaud, E. Areou, C. Martin, R. Ruffe, T. Angot, P. Roubin, C. Hopf, T. Schwarz-Selinger,W JacobRaman micro-spectroscopy as a tool to measure the absorption coefficient and theerosion rate of hydrogenated amorphous carbon films heat-treated under hydrogenbombardmentDIAMOND AND RELATED MATERIALS 22, 92 (2012)

H + H undef, T: 300−830K ExpH + C undef, T: 300−830K Exp

1443. M. Balden, P. Starke, C. Garcia-Rosales, C. Adelhelm, PA. Sauter, I. Lopez-Galilea, N. Ordas,JMR. Fernandez, MM EscandellCompilation of erosion yields of metal-doped carbon materials by deuterium impactfrom ion beam and low temperature plasmaJ. Nucl. Mater. 417, 612 (2011)

D + Zr 30−200eV ExpD + Ti 30−200eV ExpD + C 30−200eV Exp

1444. GJ. van Rooij, J. Westerhout, S. Brezinsek, J RappChemical erosion of carbon at ITER relevant plasma fluxes: Results from the linearplasma generator Pilot-PSIJ. Nucl. Mater. 415, S137 (2011)

H + C 0.2−2eV(Te), T: 400−1200K Exp

1445. I. Tanarro, JA. Ferreira, VJ. Herrero, FL. Tabares, C Gomez-AleixandreRemoval of carbon films by oxidation in narrow gaps: Thermo-oxidation and plasma-assisted studiesJ. Nucl. Mater. 390-91, 696 (2009)

He + H 3eV(Te), T: undef ExpHe + C 3eV(Te), T: undef ExpO2 + H 3eV(Te), T: undef ExpO2 + C 3eV(Te), T: undef Exp

1446. K. Yada, N. Matsui, N. Ohno, S. Kajita, S. Takamura, M TakagiInvestigation of detached recombining deuterium plasma and carbon chemical erosionin the toroidal divertor simulator NAGDIS-TJ. Nucl. Mater. 390-91, 290 (2009)

D + C 0.1−0.4eV(Te), T: 600−1000K Exp

1447. A. Kreter, S. Brezinsek, JP. Coad, HG. Esser, W. Fundamenski, V. Philipps, RA. Pitts, V. Rohde,T. Tanabe, A WiddowsonDynamics of erosion and deposition in tokamaksJ. Nucl. Mater. 390-91, 38 (2009)

D + C undef, T: undef ExpD + C undef, T: undef Exp

1448. T. Tanabe, K. Masaki, K. Sugiyama, M YoshidaAn overview of recent erosion/deposition and hydrogen retention studies in JT-60UPhys. Scr. T138, 014006 (2009)

H + C undef, T: 300−1200K ExpD + C undef, T: 300−1200K ExpH + C undef, T: 300−1200K ExpD + C undef, T: 300−1200K Exp

301

H + C undef, T: 300−1200K ExpD + C undef, T: 300−1200K ExpH + C undef, T: 300−1200K ExpD + C undef, T: 300−1200K ExpH + C undef, T: 300−1200K ExpD + C undef, T: 300−1200K ExpH + C undef, T: 300−1200K ExpD + C undef, T: 300−1200K Exp

1449. VS. Koidan, AN. Brukhanov, OK. Chugunov, VM. Gureev, BI. Khripunov, SN. Kornienko, BV.Kuteev, ST. Latushkin, AM. Muksunov, VB. Petrov, AI. Ryazanov, VP. Smirnov, VG. Stolyarova,VN UnezhevInfluence of radiation damage on plasma facing material erosionJ. Nucl. Mater. 386-88, 261 (2009)

D + C 100eV, T: ¡340K ExpD + C 100eV, T: ¡340K Exp

1450. S. Porro, G. De Temmerman, S. Lisgo, DL. Rudakov, A. Litnovsky, P. Petersson, P. John, JIBWilsonDiamond coatings exposure to fusion-relevant plasma conditionsJ. Nucl. Mater. 415, S161 (2011)

D + B 44eV(Te), T: 1050−1250K ExpD + C 44eV(Te), T: 1050−1250K ExpD + B 44eV(Te), T: 1050−1250K ExpD + C 44eV(Te), T: 1050−1250K ExpD + B 44eV(Te), T: 1050−1250K ExpD + C 44eV(Te), T: 1050−1250K ExpD + B 44eV(Te), T: 1050−1250K ExpD + C 44eV(Te), T: 1050−1250K Exp

1451. P. Petersson, A. Kreter, G. Possnert, M RubelNuclear micro-beam analysis of deuterium distribution in carbon fibre composites forcontrolled fusion devicesNucl. Instrum. Methods Phys. Res. B 268, 1833 (2010)

D + C undef, T: 470K ExpD + C undef, T: 470K ExpD + C undef, T: 470K ExpD + C undef, T: 470K ExpD + C undef, T: 470K Exp

1452. JP. Allain, DL. Rokusek, SS. Harilal, M. Nieto-Perez, CH. Skinner, HW. Kugel, B. Heim, R.Kaita, R MajeskiExperimental studies of lithium-based surface chemistry for fusion plasma-facingmaterials applicationsJ. Nucl. Mater. 390-91,942 (2009)

He + Li 10−5000eV, T: undef ExpHe + C 10−5000eV, T: undef Exp

1453. R MajeskiLiquid Metal Walls, Lithium, And Low Recycling Boundary Conditions In TokamaksAIP Conf. Proc. 1237, 122 (2010)

D + Li undef, T: 523−673K ExpD + Li undef, T: 523−673K ExpD + Li undef, T: 523−673K ExpD + Li undef, T: 523−673K Exp

302

1454. V. Tiron, S. Dobrea, C. Costin, G PopaOn the carbon and tungsten sputtering rate in a magnetron dischargeNucl. Instrum. Methods Phys. Res. B 267, 434 (2009)

Ar + C undef, T: undef ExpAr + W undef, T: undef Exp

1455. C. Porosnicu, A. Anghel, K. Sugiyama, K. Krieger, J. Roth, CP LunguInfluence of beryllium carbide formation on deuterium retention and releaseJ. Nucl. Mater. 415, S713 (2011)

D + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + O 200eV, T: 300K ExpD + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + O 200eV, T: 300K ExpD + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + O 200eV, T: 300K ExpD + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + O 200eV, T: 300K Exp

1456. S. Ishikawa, K. Katayama, Y. Ohnishi, S. Fukada, M NishikawaSorption and desorption behavior of hydrogen isotopes from tungsten deposits causedby deuterium gas or deuterium plasma exposureFusion Eng. Des. 87, 1390 (2012)

H + W 2.8−10eV(Te), T: 350−600K ExpD + W 2.8−10eV(Te), T: 350−600K ExpH + W 2.8−10eV(Te), T: 350−600K ExpD + W 2.8−10eV(Te), T: 350−600K Exp

1457. BI. Khripunov, LS. Danelyan, VG. Vostrikov, VV. Zatekin, VS. Koidan, VS. Kulikauskas, ST.Latushkin, VB. Petrov, EA. Romanovsky, AI. Ryazanov, VN UnezhevAccumulation of deuterium in radiation-damaged tungstenJOURNAL OF SURFACE INVESTIGATION-X-RAY SYNCHROTRON AND NEUTRONTECHNIQUES 5, 272 (2011)

D + W 250eV, T: undef ExpD + W 250eV, T: undef ExpD + W 250eV, T: undef ExpD + W 250eV, T: undef Exp

1458. B. Khripunov, V. Gureev, VS. Koidan, S. Latushkin, V. Petrov, A. Ryazanov, E. Semenov, V.Stolyarova, V. Unezhev, L. Danelyan, V. Kulikauskas, V ZatekinPlasma impact on materials damaged by high-energy ionsPhys. Scr. T145, 14052 (2011)

D + C 100−250eV, T: ¡400K ExpD + W 100−250eV, T: ¡400K ExpD + C 100−250eV, T: ¡400K ExpD + W 100−250eV, T: ¡400K ExpD + C 100−250eV, T: ¡400K ExpD + W 100−250eV, T: ¡400K ExpD + C 100−250eV, T: ¡400K ExpD + W 100−250eV, T: ¡400K ExpD + C 100−250eV, T: ¡400K ExpD + W 100−250eV, T: ¡400K Exp

303

1459. K. Katayama, S. Kasahara, S. Ishikawa, S. Fukada, M NishikawaHydrogen incorporation in tungsten deposits growing by deuterium plasma sputteringFusion Eng. Des. 86, 1702 (2011)

D + W undef, T: 330−470K ExpH + W undef, T: 330−470K ExpO + W undef, T: 330−470K ExpD + W undef, T: 330−470K ExpH + W undef, T: 330−470K ExpO + W undef, T: 330−470K ExpD + W undef, T: 330−470K ExpH + W undef, T: 330−470K ExpO + W undef, T: 330−470K ExpD + W undef, T: 330−470K ExpH + W undef, T: 330−470K ExpO + W undef, T: 330−470K Exp

1460. GM. Wright, J. Westerhout, RS. Al, E. Alves, LC. Alves, NP. Barradas, MA. van den Berg, D.Borodin, S. Brezinsek, S. Brons, HJN. van Eck, B. de Groot, AW. Kleyn, WR. Koppers, OG. Kruijt,J. Linke, NJL. Cardozo, M. Mayer, HJ. van der Meiden, PR. Prins, GJ. van Rooij, J. Scholten,AE. Shumack, PHM. Smeets, G. De Temmerman, WAJ. Vijvers, J RappMaterials research under ITER-like divertor conditions at FOM RijnhuizenJ. Nucl. Mater. 417, 457 (2011)

D+ + Mo 0.1−3eV(Te), T: 500−1700K ExpD+ + W 0.1−3eV(Te), T: 500−1700K ExpD+ + Mo 0.1−3eV(Te), T: 500−1700K ExpD+ + W 0.1−3eV(Te), T: 500−1700K ExpD+ + Mo 0.1−3eV(Te), T: 500−1700K ExpD+ + W 0.1−3eV(Te), T: 500−1700K ExpD+ + Mo 0.1−3eV(Te), T: 500−1700K ExpD+ + W 0.1−3eV(Te), T: 500−1700K ExpH + Si 0.1−3eV(Te), T: 500−1700K ExpH + C 0.1−3eV(Te), T: 500−1700K Exp

1461. DV. Kovalenko, NS. Klimov, VL. Podkovyrov, AD. Muzichenko, AM. Zhitlukhin, LN. Khimchenko,IB. Kupriyanov, RN GiniyatulinFirst experiments at the QSPA-Be plasma gun facilityPhys. Scr. T145, 14065 (2011)

H + Be undef, T: 300K Exp

1462. YR. Niu, S. Suzuki, XB. Zheng, CX. Ding, JL. Chen, WJ. Wang, Y. Oya, K OkunoChemical states and deuterium retention behavior of vacuum plasma sprayed tungstencoatingsJ. Nucl. Mater. 417, 551 (2011)

D + W 1000eV, T: 300K ExpD + W 1000eV, T: 300K ExpD + W 1000eV, T: 300K ExpD + W 1000eV, T: 300K Exp

1463. Z. Somogyvari, GA. Langer, G. Erdelyi, L BalazsSputtering yields for low-energy Ar+- and Ne+-ion bombardmentVacuum 86, 1979 (2012)

Ne + Fe 30−300eV, T: ¡373K ExpAr + Fe 30−300eV, T: ¡373K ExpAr + W 30−300eV, T: ¡373K ExpAr + Mo 30−300eV, T: ¡373K Exp

304

1464. JP. Roszell, AJ. Labelle, P. Brodersen, JW. Davis, AA HaaszD retention in C- and O-contaminated tungsten during D+ irradiationJ. Nucl. Mater. 427, 193 (2012)

He + W 10−500eV, T: 300−500K ExpD + O 10−500eV, T: 300−500K ExpD + C 10−500eV, T: 300−500K ExpD + W 10−500eV, T: 300−500K ExpD + O 10−500eV, T: 300−500K ExpD + C 10−500eV, T: 300−500K ExpD + W 10−500eV, T: 300−500K ExpHe + O 10−500eV, T: 300−500K ExpHe + C 10−500eV, T: 300−500K ExpHe + W 10−500eV, T: 300−500K ExpD + O 10−500eV, T: 300−500K ExpD + C 10−500eV, T: 300−500K ExpD + W 10−500eV, T: 300−500K ExpHe + O 10−500eV, T: 300−500K ExpHe + C 10−500eV, T: 300−500K ExpHe + O 10−500eV, T: 300−500K ExpHe + C 10−500eV, T: 300−500K ExpHe + W 10−500eV, T: 300−500K ExpD + W 10−500eV, T: 300−500K ExpD + C 10−500eV, T: 300−500K ExpD + O 10−500eV, T: 300−500K ExpHe + W 10−500eV, T: 300−500K ExpHe + C 10−500eV, T: 300−500K ExpHe + O 10−500eV, T: 300−500K Exp

1465. C. Garcia-Rosales, I. Lopez-Galilea, N. Ordas, C. Adelhelm, M. Balden, G. Pintsuk, M.Grattarola, C GualcoTi-doped isotropic graphite: A promising armour material for plasma-facingcomponentsJ. Nucl. Mater. 386-88, 801 (2009)

D + Ti 30−200eV, T: 630−820K ExpD + C 30−200eV, T: 630−820K Exp

1466. A. Ito, K. Ohya, K. Inai, H NakamuraDependency of Tritium Retention in Graphite on Temperature Control of MolecularDynamicsContrib. Plasma Phys. 50, 464 (2010)

H + C 30eV, T: 300−1500K Th

1467. J MarianGeneration of an amorphous graphite substrate by cumulative deuteriumbombardment using molecular dynamics with full nonbonded interactionsJ. Appl. Phys. 109, 63501 (2011)

D + D 25eV, T: 1000K ThD + C 25eV, T: 1000K ThD + D 25eV, T: 1000K ThD + C 25eV, T: 1000K ThD + D 25eV, T: 1000K ThD + C 25eV, T: 1000K ThD + D 25eV, T: 1000K ThD + C 25eV, T: 1000K Th

305

1468. R NeuBenefits and Challenges of the Use of High-Z Plasma Facing Materials in FusionDevicesAIP Conf. Proc. 1237, 62 (2010)

D + W 1−200eV, T: 300K E/TD + Mo 1−200eV, T: 300K E/TD + W 1−200eV, T: 300K E/TNe + W 1−200eV, T: 300K E/TC + W 1−200eV, T: 300K E/TD + Mo 1−200eV, T: 300K E/TD + W 1−200eV, T: 300K E/TD + Mo 1−200eV, T: 300K E/TD + W 1−200eV, T: 300K E/TD + Mo 1−200eV, T: 300K E/TD + W 1−200eV, T: 300K E/TKr + W 1−200eV, T: 300K E/TAr + W 1−200eV, T: 300K E/T

1469. N. Klimov, V. Podkovyrov, A. Zhitlukhin, D. Kovalenko, B. Bazylev, G. Janeschitz, I. Landman,S. Pestchanyi, G. Federici, A. Loarte, M. Merola, J. Linke, T. Hirai, J CompanExperimental study of PFCs erosion under ITER-like transient loads at plasma gunfacility QSPAJ. Nucl. Mater. 390-91, 721 (2009)

H + W undef, T: undef Exp

1470. T. Sizyuk, A HassaneinDynamic analysis of mixed ion beams/materials effects on the performance of ITER-like devicesJ. Nucl. Mater. 415, S293 (2011)

H + W 333−1000eV, T: 453−1050K ThC + W 333−1000eV, T: 453−1050K ThH + W 333−1000eV, T: 453−1050K ThC + W 333−1000eV, T: 453−1050K ThC + W 333−1000eV, T: 453−1050K ThH + W 333−1000eV, T: 453−1050K ThC + W 333−1000eV, T: 453−1050K ThH + W 333−1000eV, T: 453−1050K ThC + W 333−1000eV, T: 453−1050K ThH + W 333−1000eV, T: 453−1050K Th

1471. A.. Allouche, A.. Wiltner, Ch LinsmeierQuantum modeling (DFT) and experimental investigation of beryllium-tungsten alloyformationJ. Phys. Condens. Matter 21, 355011 (2009)

Be + W undef, T: undef Th

1472. A. AlloucheElectronic aspects of beryllium-tungsten surface alloying, a density functional approachChem. Phys. Lett. 470, 119 (2009)

W + Be undef, T: undef ThBe + W undef, T: undef Th

1473. P. E.. Lhuillier, T.. Belhabib, P.. Desgardin, B.. Courtois, T.. Sauvage, M. F.. Barthe, A. L..Thomann, P.. Brault, Y. TessierTrapping and release of helium in tungstenJ. Nucl. Mater. 416, 13 (2011)

306

He + W 320−6000eV, T: 1873K Exp

1474. Xiang-Shan. Kong, Yu-Wei. You, C. S.. Liu, Q. F.. Fang, Jun-Ling. Chen, G. -N. LuoFirst principles study of hydrogen behaviors in hexagonal tungsten carbideJ. Nucl. Mater. 418, 233 (2011)

H + WC undef, T: undef Th

1475. Y. G.. Li, W. H.. Zhou, L. F.. Huang, Z.. Zeng, X. JuCluster dynamics modeling of accumulation and diffusion of helium in neutronirradiated tungstenJ. Nucl. Mater. 431, 26 (2012)

He + W 30−1500eV, T: 300−873K Th

1476. Bojan. Zajec, Vincenc. Nemanic, Cristian RusetHydrogen diffusive transport parameters in W coating for fusion applicationsJ. Nucl. Mater. 412, 116 (2011)

H + EUROFER97 undef, T: 673K E/TH + W undef, T: 673K E/T

1477. Xiang-Shan. Kong, Yu-Wei. You, J. H.. Xia, C. S.. Liu, Q. F.. Fang, G. -N.. Luo, Qun-YingHuangFirst principles study of intrinsic defects in hexagonal tungsten carbideJ. Nucl. Mater. 406, 323 (2010)

W + WC undef, T: undef ThC + WC undef, T: undef Th

1478. Pengbo. Zhang, Jijun. Zhao, Bin WenRetention and diffusion of H, He, O, C impurities in BeJ. Nucl. Mater. 423, 164 (2012)

C + Be undef, T: undef ThO + Be undef, T: undef ThHe + Be undef, T: undef ThH + Be undef, T: undef Th

1479. Shuo. Jin, Yue-Lin. Liu, Hong-Bo. Zhou, Ying. Zhang, Guang-Hong LuFirst-principles investigation on the effect of carbon on hydrogen trapping in tungstenJ. Nucl. Mater. 415, S709 (2011)

H + W undef, T: undef ThH + C undef, T: undef Th

1480. Yue-Lin. Liu, Hong-Bo. Zhou, Ying. Zhang, Chen DuanPoint defect concentrations of impurity carbon in tungstenComp. Mater. Sci. 62, 282 (2012)

C + W undef, T: 300−1000K Th

1481. M.. Reinelt, A.. Allouche, M.. Oberkofler, Ch LinsmeierRetention mechanisms and binding states of deuterium implanted into berylliumNew J. Phys. 11, 43023 (2009)

D + O 1000eV, T: 300−1000K ExpD + Be 1000eV, T: 300−1000K ExpD + O 1000eV, T: 300−1000K ExpD + Be 1000eV, T: 300−1000K ExpD + O 1000eV, T: 300−1000K Exp

307

D + Be 1000eV, T: 300−1000K ExpD + O 1000eV, T: 300−1000K ExpD + Be 1000eV, T: 300−1000K ExpD + O 1000eV, T: 300−1000K ExpD + Be 1000eV, T: 300−1000K Exp

1482. T. Ikeda, T. Otsuka, T TanabeDetermination of hydrogen diffusivity and permeability in W near room temperatureapplying a tritium tracer techniqueJ. Nucl. Mater. 415, S684 (2011)

T + Ni undef, T: 285−1000K ExpT + W undef, T: 285−1000K ExpH + Ni undef, T: 285−1000K ExpH + W undef, T: 285−1000K Exp

1483. I. Takagi, R. Imade, Y. Ikegami, M. Akiyoshi, K. Moritani, T. Sasaki, H MoriyamaDeuterium recombination coefficients on tungsten exposed to RF plasmaJ. Nucl. Mater. 417, 564 (2011)

D + W undef, T: 426−654K Exp

1484. YF. Hua, ZX. Li, X. Zhang, JH. Du, CL. Huang, MH DuInter-diffusion analysis of joint interface of tungsten-rhenium coupleJ. Nucl. Mater. 416, 270 (2011)

W + Re undef, T: 1373−1673K ExpW + W undef, T: 1373−1673K ExpRe + Re undef, T: 1373−1673K ExpRe + W undef, T: 1373−1673K Exp

1485. XS. Kong, YW. You, C. Song, QF. Fang, JL. Chen, GN. Luo, CS LiuFirst principles study of foreign interstitial atom (carbon, nitrogen) interactions withintrinsic defects in tungstenJ. Nucl. Mater. 430, 270 (2012)

N + W undef, T: undef ThC + W undef, T: undef Th

1486. Y. Zayachuk, MHJ. ’t Hoen, I. Uytdenhouwen, G Van OostThermal desorption spectroscopy of W-Ta alloys, exposed to high-flux deuteriumplasmaPhys. Scr. T145, 14041 (2011)

D + Ta 50eV, T: undef ExpD + W 50eV, T: undef Exp

1487. K. Ohsawa, K. Eguchi, H. Watanabe, M. Yamaguchi, M YagiConfiguration and binding energy of multiple hydrogen atoms trapped in monovacancyin bcc transition metalsPhys. Rev. B 85, 94102 (2012)

H + Fe undef, T: undef ThH + W undef, T: undef ThH + Mo undef, T: undef ThH + Cr undef, T: undef ThH + Ta undef, T: undef ThH + Nb undef, T: undef ThH + V undef, T: undef Th

308

1488. Q. Xu, K. Sato, T YoshiieInteraction of tritium plasma and defects in tungsten irradiated with neutronsJ. Nucl. Mater. 390-91, 663 (2009)

T + W 1000eV, T: 473−873K Th

1489. U. von Toussaint, S. Gori, A. Manhard, T. Hoschen, C HoschenMolecular dynamics study of grain boundary diffusion of hydrogen in tungstenPhys. Scr. T145, 14036 (2011)

H + W undef, T: 300−1000K Th

1490. T. Hoshihira, T. Otsuka, R. Wakabayashi, T TanabeHydrogen behavior near surface regions in Mo and W studied by tritium tracertechniqueJ. Nucl. Mater. 417, 559 (2011)

T + Mo undef, T: 273−323K ExpH + Mo undef, T: 273−323K ExpT + W undef, T: 273−323K ExpH + W undef, T: 273−323K Exp

1491. YL. Liu, HB. Zhou, S. Jin, Y. Zhang, GH LuDissolution and diffusion properties of carbon in tungstenJ. Phys. Condens. Matter 22, 445504 (2010)

C + W undef, T: 100−1200K Th

1492. W. Xiao, WT GengRole of grain boundary and dislocation loop in H blistering in W: A density functionaltheory assessmentJ. Nucl. Mater. 430, 132 (2012)

H + W undef, T: undef Th

1493. CJ. Ortiz, MJ. Caturla, CC. Fu, F WillaimeInfluence of carbon on the kinetics of He migration and clustering in alpha-Fe fromfirst principlesPhys. Rev. B 80, 134109 (2009)

C + He undef, T: 300−573K ThC + Fe undef, T: 300−573K Th

1494. CS. Becquart, C DomainAn object Kinetic Monte Carlo Simulation of the dynamics of helium and point defectsin tungstenJ. Nucl. Mater. 385, 223 (2009)

He + W undef, T: 1−1000K Th

1495. WW. Basuki, J AktaaInvestigation on the diffusion bonding of tungsten and EUROFER97J. Nucl. Mater. 417, 524 (2011)

H + EUROFER97 undef, T: 1323K ExpC + EUROFER97 undef, T: 1323K ExpS + EUROFER97 undef, T: 1323K ExpCa + EUROFER97 undef, T: 1323K ExpP + EUROFER97 undef, T: 1323K ExpFe + EUROFER97 undef, T: 1323K ExpCr + EUROFER97 undef, T: 1323K ExpW + EUROFER97 undef, T: 1323K Exp

309

1496. SI. Kim, CW LeeImpurity behaviors of nitrogen in W-C-N thin diffusion barriers for Cu metallizationschemesJ. Electroceram. 23, 488 (2009)

N + W undef, T: 300−1000K ExpN + C undef, T: 300−1000K ExpN + N undef, T: 300−1000K ExpCu + W undef, T: 300−1000K ExpCu + C undef, T: 300−1000K ExpCu + N undef, T: 300−1000K Exp

1497. VB. Vykhodets, TE. Kurennykh, AG. Kesarev, MV. Kuznetsov, VV. Kondrat’ev, C. Hulsen, UKoesterDiffusion of insoluble carbon in zirconium oxidesJETP Letters 93, 5 (2011)

C + ZrO2 undef, T: 1173−1273K Exp

1498. W. Xiao, GN. Luo, WT GengThreshold concentration for H blistering in defect free WJ. Nucl. Mater. 421, 176 (2012)


1499. A. Alkhamees, YL. Liu, HB. Zhou, S. Jin, Y. Zhang, GH LuFirst-principles investigation on dissolution and diffusion of oxygen in tungstenJ. Nucl. Mater. 393, 508 (2009)

O + W undef, T: 300−1000K Th

1500. A. Moitra, K SolankiAdsorption and penetration of hydrogen in W: A first principles studyComp. Mater. Sci. 50, 2291 (2011)

H + W undef, T: ¿300K Th

1501. MJ. Baldwin, RP. Doerner, D. Nishijima, K. Tokunaga, Y UedaThe effects of high fluence mixed-species (deuterium, helium, beryllium) plasmainteractions with tungstenJ. Nucl. Mater. 390-91, 886 (2009)

D2 + W ¡75eV, T: 1070−1320K ExpBe + W ¡75eV, T: 1070−1320K ExpHe + W ¡75eV, T: 1070−1320K Exp

1502. M. Nieto-Perez, G. Ramos, JP AllainModeling of Beryllium-Carbon Dynamics in the ITER Divertor Region2009 23RD IEEE/NPSS SYMPOSIUM ON FUSION ENGINEERING ,424 (2009)

D3+ + C 13.3−48.5eV, T: undef Th

D2+ + C 13.3−48.5eV, T: undef Th

D+ + C 13.3−48.5eV, T: undef ThBe + C 13.3−48.5eV, T: undef ThC + C 13.3−48.5eV, T: undef ThT + C 13.3−48.5eV, T: undef Th

1503. V. Nemanic, B. Zajec, M. Zumer, C. Porosnicu, CP LunguHydrogen permeability of beryllium films prepared by the thermionic vacuum arcmethodFusion Eng. Des. 86, 2421 (2011)

310

H + Be undef, T: 673K Exp

1504. M. Oberkofler, M. Reinelt, C LinsmeierRetention and release mechanisms of deuterium implanted into berylliumNucl. Instrum. Methods Phys. Res. B 269, 1266 (2011)

D3+ + Be 400−3000eV, T: 300K Exp

D2+ + Be 400−3000eV, T: 300K Exp

D3+ + Be 400−3000eV, T: 300K Exp

D2+ + Be 400−3000eV, T: 300K Exp

D3+ + Be 400−3000eV, T: 300K Exp

D2+ + Be 400−3000eV, T: 300K Exp

D3+ + Be 400−3000eV, T: 300K Exp

D2+ + Be 400−3000eV, T: 300K Exp

1505. HY. Peng, HT. Lee, Y. Ohtsuka, Y UedaIon-driven permeation of deuterium in tungsten by deuterium and carbon-mixed ionirradiationPhys. Scr. T145, 14046 (2011)

D+ + W 1000eV, T: 550−1050K ExpD2

+ + W 1000eV, T: 550−1050K ExpD3

+ + W 1000eV, T: 550−1050K ExpC + W 1000eV, T: 550−1050K Exp

1506. A. Anghel, C. Porosnicu, CP. Lungu, K. Sugiyama, C. Krieger, J RothInfluence of thermal treatment on beryllium/carbon formation and fuel retentionJ. Nucl. Mater. 416, 9 (2011)

Be + Be 200eV, T: 300−1023K ExpBe + O 200eV, T: 300−1023K ExpBe + C 200eV, T: 300−1023K ExpO + Be 200eV, T: 300−1023K ExpO + O 200eV, T: 300−1023K ExpO + C 200eV, T: 300−1023K ExpC + Be 200eV, T: 300−1023K ExpC + O 200eV, T: 300−1023K ExpC + C 200eV, T: 300−1023K ExpD + Be 200eV, T: 300−1023K ExpD + O 200eV, T: 300−1023K ExpD + C 200eV, T: 300−1023K ExpD + Be 200eV, T: 300−1023K ExpD + O 200eV, T: 300−1023K ExpD + C 200eV, T: 300−1023K ExpD + Be 200eV, T: 300−1023K ExpD + O 200eV, T: 300−1023K ExpD + C 200eV, T: 300−1023K ExpD + Be 200eV, T: 300−1023K ExpD + O 200eV, T: 300−1023K ExpD + C 200eV, T: 300−1023K Exp

1507. K. Vortler, K NordlundMolecular Dynamics Simulations of Deuterium Trapping and Re-emission in TungstenCarbideJ. Phys. Chem. C 114, 5382 (2010)

D + WC 100−300eV, T: 600K ThAr + WC 100−300eV, T: 600K ThW + WC 100−300eV, T: 600K ThC + WC 100−300eV, T: 600K Th

311

He + WC 100−300eV, T: 600K ThHe + WC 100−300eV, T: 600K ThAr + WC 100−300eV, T: 600K ThNe + WC 100−300eV, T: 600K ThD + WC 100−300eV, T: 600K Th

1508. OV. Ogorodnikova, K. Sugiyama, A. Markin, Y. Gasparyan, V. Efimov, A. Manhard, M BaldenEffect of nitrogen seeding into deuterium plasma on deuterium retention in tungstenPhys. Scr. T145, 14034 (2011)

D+ + W 20−60eV, T: 320−593K ExpD2

+ + W 20−60eV, T: 320−593K ExpD3

+ + W 20−60eV, T: 320−593K ExpHe + W 20−60eV, T: 320−593K ExpD+ + W 20−60eV, T: 320−593K ExpD2

+ + W 20−60eV, T: 320−593K ExpD3


+ + W 20−60eV, T: 320−593K ExpD3


+ + W 20−60eV, T: 320−593K ExpD3

+ + W 20−60eV, T: 320−593K ExpHe + W 20−60eV, T: 320−593K Exp

1509. M. Shimada, G. Cao, Y. Hatano, T. Oda, Y. Oya, M. Hara, P CalderoniThe deuterium depth profile in neutron-irradiated tungsten exposed to plasmaPhys. Scr. T145, 14051 (2011)

D + W 100eV, T: 300−1000K E/TD + W 100eV, T: 300−1000K E/TD + W 100eV, T: 300−1000K E/TD + W 100eV, T: 300−1000K E/T

1510. K. Bystrov, J. Westerhout, M. Matveeva, A. Litnovsky, L. Marot, E. Zoethout, G De TemmermanErosion yields of carbon under various plasma conditions in Pilot-PSIJ. Nucl. Mater. 415, S149 (2011)

H + C 1−75eV, T: undef Exp

1511. K. Schmid, J RothErosion processes due to energetic particle-surface interactionAIP Conf. Proc. 1237, 18 (2010)

Ar + W 10−10000eV, T: 300−1300K ThD + Be 10−10000eV, T: 300−1300K ThD + W 10−10000eV, T: 300−1300K ThAr + Be 10−10000eV, T: 300−1300K ThH + H 10−10000eV, T: 300−1300K ThH + C 10−10000eV, T: 300−1300K ThHe + Be 10−10000eV, T: 300−1300K ThT + C 10−10000eV, T: 300−1300K ThD+ + C 10−10000eV, T: 300−1300K ThH+ + C 10−10000eV, T: 300−1300K Th

1512. K. Sugiyama, K. Krieger, M. Mayer, S. Lindig, M. Balden, T DurbeckDeuterium retention in bulk tungsten exposed to the outer divertor plasma of ASDEXUpgradePhys. Scr. T145, 14033 (2011)

312

D + W 38−500eV, T: 473−673K ExpD + W 38−500eV, T: 473−673K ExpD + W 38−500eV, T: 473−673K ExpD + W 38−500eV, T: 473−673K Exp

1513. I. Bizyukov, K. Krieger, H. Lee, K. Schmid, AA. Haasz, JW DavisAn overview of sputtering-related processes occurring at mixed surfaces formed bysimultaneous C+ and D+ irradiation of WJ. Nucl. Mater. 427, 401 (2012)

He+ + W 100−6000eV, T: 300−2000K E/TC+ + W 100−6000eV, T: 300−2000K E/TC + WC 100−6000eV, T: 300−2000K E/TC + C 100−6000eV, T: 300−2000K E/TC + W 100−6000eV, T: 300−2000K E/T

1514. RD. Kolasinski, KR. Umstadter, JP. Sharpe, RA. Causey, RJ. Pawelko, JA. Whaley, DA.Buchenauer, M ShimadaThe impact of specific surface area on the retention of deuterium in carbon fibercomposite materialsFusion Eng. Des. 84, 1068 (2009)

D+ + C 130−150eV, T: 473K ExpD+ + C 130−150eV, T: 473K ExpD+ + C 130−150eV, T: 473K ExpD+ + C 130−150eV, T: 473K Exp

1515. CS. Becquart, MF. Barthe, A De BackerModelling radiation damage and He production in tungstenPhys. Scr. T145, 14048 (2011)

He + W undef, T: undef Th

1516. A. Rai, A. Mutzke, R SchneiderModeling of chemical erosion of graphite due to hydrogen by inclusion of chemicalreactions in SDTrimSPNucl. Instrum. Methods Phys. Res. B 268, 2639 (2010)

H+ + C 10−1000eV, T: 200−1000K ThAr+ + H 10−1000eV, T: 200−1000K ThAr+ + C 10−1000eV, T: 200−1000K ThH+ + C 10−1000eV, T: 200−1000K ThAr+ + H 10−1000eV, T: 200−1000K ThAr+ + C 10−1000eV, T: 200−1000K Th

1517. RD. Kolasinski, M. Shimada, DA. Buchenauer, RA. Causey, T. Otsuka, WM. Clift, JM. Shea, TR.Allen, P. Calderoni, JP SharpeCharacterization of surface morphology and retention in tungsten materials exposedto high fluxes of deuterium ions in the tritium plasma experimentPhys. Scr. T138, 14042 (2009)

D + W 70eV, T: 420−927K ExpD + W 70eV, T: 420−927K ExpD + W 70eV, T: 420−927K ExpD + W 70eV, T: 420−927K Exp

1518. T. Ogawa, A. Hasegawa, H. Kurishita, S NogamiImprovement of Surface Exfoliation Behavior by Helium-ion Bombardment of aTungsten Alloy Fabricated by Mechanical AlloyingJ. Nucl. Sci. Technol. 46, 717 (2009)

313

He+ + W undef, T: 298−823K Exp

1519. RP. Doerner, MJ. Baldwin, D. Nishijima, J. Roth, K SchmidImpact of beryllium surface layers on deuterium retention in tungstenJ. Nucl. Mater. 415, S717 (2011)

Be + Be 50−60eV, T: 573K ExpBe + W 50−60eV, T: 573K ExpD + Be 50−60eV, T: 573K ExpD + W 50−60eV, T: 573K ExpD + W 50−60eV, T: 573K ExpBe + Be 50−60eV, T: 573K ExpBe + W 50−60eV, T: 573K ExpD + Be 50−60eV, T: 573K ExpD + W 50−60eV, T: 573K ExpBe + Be 50−60eV, T: 573K ExpBe + W 50−60eV, T: 573K ExpD + Be 50−60eV, T: 573K ExpD + W 50−60eV, T: 573K ExpBe + Be 50−60eV, T: 573K ExpBe + W 50−60eV, T: 573K ExpD + Be 50−60eV, T: 573K Exp

1520. CH SkinnerTritium Retention and Removal in Tokamaks2ND ITER INTERNATIONAL SUMMER SCHOOL: CONFINEMENT 1095, 127 (2009)

T + C undef, T: undef ThT + C undef, T: undef ThT + C undef, T: undef ThT + C undef, T: undef Th

1521. K. Sugiyama, J. Roth, A. Anghel, C. Porosnicu, M. Baldwin, R. Doerner, K. Krieger, CP LunguConsequences of deuterium retention and release from Be-containing mixed materialsfor ITER Tritium Inventory ControlJ. Nucl. Mater. 415, S731 (2011)

D3+ + Be 600eV, T: 623K Exp

D3+ + C 600eV, T: 623K Exp

D3+ + W 600eV, T: 623K Exp

D3+ + Be 600eV, T: 623K Exp

D3+ + C 600eV, T: 623K Exp

D3+ + W 600eV, T: 623K Exp

D3+ + Be 600eV, T: 623K Exp

D3+ + C 600eV, T: 623K Exp

D3+ + W 600eV, T: 623K Exp

D3+ + Be 600eV, T: 623K Exp

D3+ + W 600eV, T: 623K Exp

D3+ + C 600eV, T: 623K Exp

1522. VK. Alimov, J. Roth, WM. Shu, DA. Komarov, K. Isobe, T YamanishiDeuterium trapping in tungsten deposition layers formed by deuterium plasmasputteringJ. Nucl. Mater. 399, 225 (2010)

He + W 170−340eV, T: 300−700K ExpD + W 170−340eV, T: 300−700K ExpAr + W 170−340eV, T: 300−700K ExpD + W 170−340eV, T: 300−700K ExpAr + W 170−340eV, T: 300−700K Exp

314

He + W 170−340eV, T: 300−700K ExpD + W 170−340eV, T: 300−700K ExpAr + W 170−340eV, T: 300−700K ExpHe + W 170−340eV, T: 300−700K ExpD + W 170−340eV, T: 300−700K ExpAr + W 170−340eV, T: 300−700K ExpHe + W 170−340eV, T: 300−700K Exp

1523. M. Fukumoto, T. Nakano, K. Itami, T. Wada, Y. Ueda, T TanabeEffects of carbon impurity on deuterium retention in VPS-tungsten coatings exposedto JT-60U divertor plasmasJ. Nucl. Mater. 415, S705 (2011)

C + C undef, T: 1073K ExpC + W undef, T: 1073K Exp

1524. V. Rohde, M. Mayer, V. Mertens, R. Neu, K SugiyamaDynamic and static deuterium inventory in ASDEX Upgrade with tungsten first wallNucl. Fusion 49, 85031 (2009)

C + C undef, T: undef ExpD + W undef, T: undef ExpD + C undef, T: undef ExpC + W undef, T: undef ExpC + C undef, T: undef ExpD + W undef, T: undef ExpD + C undef, T: undef ExpC + W undef, T: undef ExpC + C undef, T: undef ExpD + W undef, T: undef ExpD + C undef, T: undef ExpC + W undef, T: undef ExpC + C undef, T: undef ExpC + W undef, T: undef ExpD + C undef, T: undef ExpD + W undef, T: undef Exp

1525. OV. Ogorodnikova, T. Schwarz-Selinger, K. Sugiyama, VK AlimovDeuterium retention in tungsten exposed to low-energy pure and helium-seededdeuterium plasmasJ. Appl. Phys. 109, 13309 (2011)

D3+ + W 30−60eV, T: 300−700K Exp

D2+ + W 30−60eV, T: 300−700K Exp

D+ + W 30−60eV, T: 300−700K ExpHe+ + W 30−60eV, T: 300−700K ExpD3

+ + W 30−60eV, T: 300−700K ExpD2

+ + W 30−60eV, T: 300−700K ExpD+ + W 30−60eV, T: 300−700K ExpHe+ + W 30−60eV, T: 300−700K ExpD3

+ + W 30−60eV, T: 300−700K ExpD2

+ + W 30−60eV, T: 300−700K ExpD+ + W 30−60eV, T: 300−700K ExpHe+ + W 30−60eV, T: 300−700K ExpD3

+ + W 30−60eV, T: 300−700K ExpD2

+ + W 30−60eV, T: 300−700K ExpD+ + W 30−60eV, T: 300−700K ExpHe+ + W 30−60eV, T: 300−700K Exp

1526. J. Roth, K SchmidHydrogen in tungsten as plasma-facing materialPhys. Scr. T145, 14031 (2011)

315

D + W 38eV, T: 285−1000K E/THe + W 38eV, T: 285−1000K E/TD + W 38eV, T: 285−1000K E/THe + W 38eV, T: 285−1000K E/TD + W 38eV, T: 285−1000K E/THe + W 38eV, T: 285−1000K E/TD + W 38eV, T: 285−1000K E/THe + W 38eV, T: 285−1000K E/TH + W 38eV, T: 285−1000K E/T

1527. S. Ishikawa, K. Katayama, Y. Ohnishi, S. Fukada, M NishikawaSorption and desorption behavior of hydrogen isotopes from tungsten deposits causedby deuterium gas or deuterium plasma exposureFusion Eng. Des. 87, 1390 (2012)

D + W 2.8−10eV(Te), T: 573K ExpH + W 2.8−10eV(Te), T: 573K ExpD + W 2.8−10eV(Te), T: 573K ExpH + W 2.8−10eV(Te), T: 573K ExpD + W 2.8−10eV(Te), T: 573K ExpH + W 2.8−10eV(Te), T: 573K ExpD + W 2.8−10eV(Te), T: 573K ExpH + W 2.8−10eV(Te), T: 573K Exp

1528. T. Fujiki, K. Katayama, S. Kasahara, S. Fukada, M NishikawaEffect of oxygen on hydrogen retention in W deposition layers formed by hydrogenRF plasmaFusion Eng. Des. 85, 1094 (2010)

H + W undef, T: 373−1073K ExpH + O undef, T: 373−1073K ExpD + W undef, T: 373−1073K ExpD + O undef, T: 373−1073K ExpH + W undef, T: 373−1073K ExpH + O undef, T: 373−1073K ExpD + W undef, T: 373−1073K ExpD + W undef, T: 373−1073K ExpH + O undef, T: 373−1073K ExpH + W undef, T: 373−1073K ExpD + O undef, T: 373−1073K ExpD + W undef, T: 373−1073K ExpH + O undef, T: 373−1073K ExpH + W undef, T: 373−1073K ExpD + O undef, T: 373−1073K ExpD + O undef, T: 373−1073K Exp

1529. A. Debelle, PE. Lhuillier, MF. Barthe, T. Sauvage, P DesgardinHelium desorption in He-3 implanted tungsten at low fluence and low energyNucl. Instrum. Methods Phys. Res. B 268, 223 (2010)

He + W undef, T: 200−2000K ExpHe + He undef, T: 200−2000K ExpHe + W undef, T: 200−2000K ExpHe + He undef, T: 200−2000K Exp

1530. K. Ohya, A KirschnerSimulation of hydrogen retention and re-emission from tungsten exposed to divertorplasmasPhys. Scr. T145, 14047 (2011)

316

D3+ + W 100eV, T: ¿298K Th

D3+ + W 100eV, T: ¿298K Th

D3+ + W 100eV, T: ¿298K Th

D3+ + W 100eV, T: ¿298K Th

1531. M. Mayer, V. Rohde, K. Sugiyama, JL. Chen, X. Gong, C. Hopf, J. Likonen, S. Lindig, R. Neu, G.Ramos, E. Vainonen-Ahlgren, A WiltnerCarbon balance and deuterium inventory from a carbon dominated to a full tungstenASDEX UpgradeJ. Nucl. Mater. 390-91, 538 (2009)

B + W undef, T: undef ExpC + W undef, T: undef ExpD + W undef, T: undef ExpB + W undef, T: undef ExpC + W undef, T: undef ExpD + W undef, T: undef ExpB + W undef, T: undef ExpC + W undef, T: undef ExpD + W undef, T: undef ExpB + W undef, T: undef ExpC + W undef, T: undef ExpD + W undef, T: undef Exp

1532. GM. Wright, M. Mayer, K. Ertl, G. de Saint-Aubinc, J RappTMAP7 simulations of deuterium trapping in pre-irradiated tungsten exposed to high-flux plasmaJ. Nucl. Mater. 415, S636 (2011)

D + W undef, T: 360−950K ThD + W undef, T: 360−950K Th

1533. GN. Luo, K. Umstadter, WM. Shu, W. Wampler, GH LuBehavior of tungsten with exposure to deuterium plasmasNucl. Instrum. Methods Phys. Res. B 267, 3041 (2009)

D + W ¡100eV, T: 300−900K ExpD + W ¡100eV, T: 300−900K ExpD + W ¡100eV, T: 300−900K ExpD + W ¡100eV, T: 300−900K Exp

1534. E. Alves, LC. Alves, NP. Barradas, R. Mateus, PA. Carvalho, GM WrightInfluence of temperature and plasma composition on deuterium retention in refractorymetalsNucl. Instrum. Methods Phys. Res. B 268, 2124 (2010)

D+ + Mo 3eV(Te), T: undef ExpD+ + W 3eV(Te), T: undef ExpD+ + Mo 3eV(Te), T: undef ExpD+ + W 3eV(Te), T: undef ExpD+ + Mo 3eV(Te), T: undef ExpD+ + W 3eV(Te), T: undef ExpD+ + Mo 3eV(Te), T: undef ExpD+ + W 3eV(Te), T: undef Exp

1535. K. Okamoto, H. Zushi, Y. Hirooka, R. Bhattacharyay, M. Sakamoto, M SatoSurface temperature effects on the retention and pressure variation in continuous andcyclic plasma exposures on the tungstenJ. Nucl. Mater. 390-91, 671 (2009)

317

He + WC ¡25eV, T: 400−1000K ExpH + WC ¡25eV, T: 400−1000K ExpHe + WC ¡25eV, T: 400−1000K ExpH + WC ¡25eV, T: 400−1000K ExpHe + WC ¡25eV, T: 400−1000K ExpH + WC ¡25eV, T: 400−1000K ExpHe + WC ¡25eV, T: 400−1000K ExpH + WC ¡25eV, T: 400−1000K Exp

1536. OV. Ogorodnikova, B. Tyburska, VK. Alimov, K ErtlThe influence of radiation damage on the plasma-induced deuterium retention in self-implanted tungstenJ. Nucl. Mater. 415, S661 (2011)

D+ + W 38−60eV, T: 300−800K E/TD+ + W 38−60eV, T: 300−800K E/TD+ + W 38−60eV, T: 300−800K E/TD+ + W 38−60eV, T: 300−800K E/TD+ + W 38−60eV, T: 300−800K E/T

1537. C. Porosnicu, A. Anghel, K. Sugiyama, K. Krieger, J. Roth, CP LunguInfluence of beryllium carbide formation on deuterium retention and releaseJ. Nucl. Mater. 415, S713 (2011)

D + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + C 200eV, T: 300K ExpD + Be 200eV, T: 300K ExpD + C 200eV, T: 300K ExpD + Be 200eV, T: 300K Exp

1538. VK. Alimov, B. Tyburska-Puschel, Y. Hatano, J. Roth, K. Isobe, M. Matsuyama, T YamanishiThe effect of displacement damage on deuterium retention in ITER-grade tungstenexposed to low-energy, high-flux pure and helium-seeded deuterium plasmasJ. Nucl. Mater. 420, 370 (2012)

He+ + W 76eV, T: 400−750K ExpD2

+ + W 76eV, T: 400−750K ExpHe+ + W 76eV, T: 400−750K ExpD2



+ + W 76eV, T: 400−750K Exp

1539. PE. Lhuillier, A. Debelle, T. Belhabib, AL. Thomann, P. Desgardin, T. Sauvage, MF. Barthe, P.Brault, Y TessierHelium desorption in He-3 implanted tungsten at low energyJ. Nucl. Mater. 417, 504 (2011)

He + W undef, T: 300−1873K ExpHe + W undef, T: 300−1873K ExpHe + W undef, T: 300−1873K ExpHe + W undef, T: 300−1873K Exp

1540. JP. Sharpe, RD. Kolasinski, M. Shimada, P. Calderoni, RA CauseyRetention behavior in tungsten and molybdenum exposed to high fluences of deuteriumions in TPEJ. Nucl. Mater. 390-91, 709 (2009)

318

D+ + Mo 70eV, T: 300−900K ExpD+ + W 70eV, T: 300−900K ExpD+ + Mo 70eV, T: 300−900K ExpD+ + W 70eV, T: 300−900K ExpD+ + Mo 70eV, T: 300−900K ExpD+ + W 70eV, T: 300−900K ExpD+ + Mo 70eV, T: 300−900K ExpD+ + W 70eV, T: 300−900K Exp

1541. B. Schweer, F. Irrek, M. Zlobinski, A. Huber, G. Sergienko, S. Brezinsek, V. Philipps, U SammIn situ detection of hydrogen retention in TEXTOR by laser induced desorptionJ. Nucl. Mater. 390-91, 576 (2009)

H+ + H undef, T: undef ExpH+ + C undef, T: undef ExpH+ + H undef, T: undef ExpH+ + C undef, T: undef ExpH+ + H undef, T: undef ExpH+ + C undef, T: undef ExpH+ + H undef, T: undef ExpH+ + C undef, T: undef Exp

1542. Y. Oya, S. Suzuki, WJ. Wang, R. Kurata, M. Kobayashi, N. Ashikawa, A. Sagara, N. Yoshida, KOkunoCorrelation between deuterium retention and microstructure change for tungstenunder triple ion implantationPhys. Scr. T138, 14051 (2009)

CH4 + W 1−100eV, T: 1−50eV ThCH4 + H 1−100eV, T: 1−50eV ThCH4 + C 1−100eV, T: 1−50eV Th

1543. GM. Wright, AW. Kleyn, E. Alves, LC. Alves, NP. Barradas, GJ. van Rooij, AJ. van Lange, AE.Shumack, J. Westerhout, RS. Al, WAJ. Vijvers, B. de Groot, MJV. de Pol, HJ. van der Meiden,J. Rapp, NJL CardozoHydrogenic retention in tungsten exposed to ITER divertor relevant plasma fluxdensitiesJ. Nucl. Mater. 390-91, 610 (2009)

D + W 2eV(Te), T: ¡1600K ExpD + W 2eV(Te), T: ¡1600K ExpD + W 2eV(Te), T: ¡1600K ExpD + W 2eV(Te), T: ¡1600K Exp

1544. VK. Alimov, H. Nakamura, B. Tyburska-Puschel, OV. Ogorodnikova, J. Roth, K. Isobe, TYamanishiDeuterium retention in plasma spray tungsten coatings exposed to low-energy, highflux D plasmaJ. Nucl. Mater. 414, 479 (2011)

D2+ + W 38eV, T: 340−1300K Exp

D2+ + W 38eV, T: 340−1300K Exp

D2+ + W 38eV, T: 340−1300K Exp

D2+ + W 38eV, T: 340−1300K Exp

1545. VK. Alimov, B. Tyburska, V. Ogorodnikova, J. Roth, K. Isobe, T YamanishiDeuterium retention in porous vacuum plasma-sprayed tungsten coating exposed tolow-energy, high-flux pure and helium-seeded D plasmasJ. Nucl. Mater. 415, S628 (2011)

319

D2+ + W 76eV, T: 300−800K Exp

He+ + W 76eV, T: 300−800K ExpD2



+ + W 76eV, T: 300−800K ExpHe+ + W 76eV, T: 300−800K Exp

1546. N. Matsunami, N. Ohno, M TokitaniDeuterium retention in tungsten oxide under low energy D-2(+) plasma exposureJ. Nucl. Mater. 390-91, 693 (2009)

D + WO3 20−250eV, T: 300K ExpD + W 20−250eV, T: 300K ExpD + WO3 20−250eV, T: 300K ExpD + W 20−250eV, T: 300K ExpD + WO3 20−250eV, T: 300K ExpD + W 20−250eV, T: 300K ExpD + W 20−250eV, T: 300K ExpD + WO3 20−250eV, T: 300K Exp

1547. OV. Ogorodnikova, K. Sugiyama, T. Schwarz-Selinger, T. Durbeck, M BaldenIon-induced deuterium retention in tungsten coatings on carbon substrateJ. Nucl. Mater. 419, 194 (2011)

D3+ + W 20−200eV, T: 320−593K Exp

D3+ + W 20−200eV, T: 320−593K Exp

D3+ + W 20−200eV, T: 320−593K Exp

D3+ + W 20−200eV, T: 320−593K Exp

1548. T. Ahlgren, K. Heinola, K. Vortler, J KeinonenSimulation of irradiation induced deuterium trapping in tungstenJ. Nucl. Mater. 427, 152 (2012)

D + W 30000eV,T: 298K ThD + W 30000eV,T: 298K ThD + W 30000eV,T: 298K ThD + W 30000eV,T: 298K Th

1549. A. Kirschner, K. Ohya, D. Borodin, R. Ding, D. Matveev, V. Philipps, U SammPrediction of long-term tritium retention in the divertor of ITER: influence ofmodelling assumptions on retention ratesPhys. Scr. T138, 14011 (2009)

D + Be undef, T: undef ExpT + Be undef, T: undef ExpD + Be undef, T: undef ExpT + Be undef, T: undef ExpT + W undef, T: undef ExpD + C undef, T: undef ExpT + C undef, T: undef ExpD + C undef, T: undef ExpT + W undef, T: undef ExpT + Be undef, T: undef ExpD + Be undef, T: undef ExpT + C undef, T: undef ExpD + C undef, T: undef ExpT + C undef, T: undef ExpD + Be undef, T: undef Exp

320

T + Be undef, T: undef ExpT + W undef, T: undef ExpD + C undef, T: undef ExpT + C undef, T: undef ExpT + W undef, T: undef Exp

1550. M. Yamagiwa, Y. Nakamura, N. Matsunami, N. Ohno, S. Kajita, M. Takagi, M. Tokitani, S.Masuzaki, A. Sagara, K NishimuraIn situ measurement of hydrogen isotope retention using a high heat flux plasmagenerator with ion beam analysisPhys. Scr. T145, 14032 (2011)

D + W 17−28eV, T: 497−1000K ExpD + C 17−28eV, T: 497−1000K ExpD + W 17−28eV, T: 497−1000K ExpD + C 17−28eV, T: 497−1000K ExpD + W 17−28eV, T: 497−1000K ExpD + C 17−28eV, T: 497−1000K ExpD + W 17−28eV, T: 497−1000K ExpD + C 17−28eV, T: 497−1000K Exp

1551. KR. Umstadter, R. Doerner, G TynanEffect of bulk temperature on erosion of tungsten plasma-facing components subjectto simultaneous deuterium plasma and heat pulsesPhys. Scr. T138, 14047 (2009)

D + W 40−140eV, T: 323−903K ExpD + W 40−140eV, T: 323−903K ExpD + W 40−140eV, T: 323−903K ExpD + W 40−140eV, T: 323−903K Exp

1552. DG WhyteOn the consequences of neutron induced damage for volumetric fuel retention in plasmafacing materialsJ. Nucl. Mater. 390-91, 911 (2009)

T + W undef, T: 300−750K ThT + W undef, T: 300−750K ThT + W undef, T: 300−750K ThT + W undef, T: 300−750K ThT + W undef, T: 300−750K Th

1553. WR. Wampler, RP DoernerDeuterium retention in tungsten from exposure to plasmaPhys. Scr. T138, 14037 (2009)

D + W undef, T: 473−773K ExpD + W undef, T: 473−773K ExpD + W undef, T: 473−773K ExpD + W undef, T: 473−773K Exp

1554. B. Tyburska, VK. Alimov, OV. Ogorodnikova, K. Schmid, K ErtlDeuterium retention in self-damaged tungstenJ. Nucl. Mater. 395, 150 (2009)

D3+ + W 38−800eV, T: 320−470K Exp

D3+ + W 38−800eV, T: 320−470K Exp

D3+ + W 38−800eV, T: 320−470K Exp

D3+ + W 38−800eV, T: 320−470K Exp

321

1555. LB. Begrambekov, AS. Kuznetsov, PA ShiginHydrogen trapping in depositing carbon filmsJ. Nucl. Mater. 391-91, 685 (2009)

D + C 50−1000eV, T: 300K ExpH + C 50−1000eV, T: 300K ExpD + C 50−1000eV, T: 300K ExpH + C 50−1000eV, T: 300K ExpD + C 50−1000eV, T: 300K ExpH + C 50−1000eV, T: 300K ExpD + C 50−1000eV, T: 300K ExpH + C 50−1000eV, T: 300K Exp

1556. RH. Ning, YG. Li, WH. Zhou, Z. Zeng, X JuModeling D retention in W under D ions and neutrons irradiationJ. Nucl. Mater. 430, 20 (2012)

D+ + W 200−3000eV, T: 300−600K ThD+ + W 200−3000eV, T: 300−600K ThD+ + W 200−3000eV, T: 300−600K ThD+ + W 200−3000eV, T: 300−600K Th

1557. Z. Tian, JW. Davis, AA HaaszDeuterium retention in tungsten at fluences of up to 10(26) D+/m(2) using D+ ionbeamsJ. Nucl. Mater. 399, 101 (2010)

D+ + W 38−500eV, T: 300−643K ExpD+ + W 38−500eV, T: 300−643K ExpD+ + W 38−500eV, T: 300−643K ExpD+ + W 38−500eV, T: 300−643K Exp

1558. B. Tyburska, VK. Alimov, OV. Ogorodnikova, K. Ertl, K. Schmid, J RothTrapping of permeating deuterium in defect induced at the rear side of tungstensamplesJ. Nucl. Mater. 415, S680 (2011)

D2+ + W 38−68eV, T: 300−800K Exp

D+ + W 38−68eV, T: 300−800K ExpD2

+ + W 38−68eV, T: 300−800K ExpD2

+ + W 38−68eV, T: 300−800K ExpD+ + W 38−68eV, T: 300−800K ExpD+ + W 38−68eV, T: 300−800K ExpD2

+ + W 38−68eV, T: 300−800K ExpD+ + W 38−68eV, T: 300−800K Exp

1559. OV. Ogorodnikova, T. Schwarz-Selinger, K. Sugiyama, T. Durbeck, W JacobDeuterium retention in different tungsten gradesPhys. Scr. T138, 14053 (2009)

D3+ + W 3−200eV, T: 320−500K Exp

D2+ + W 3−200eV, T: 320−500K Exp

D+ + W 3−200eV, T: 320−500K ExpD3

+ + W 3−200eV, T: 320−500K ExpD2

+ + W 3−200eV, T: 320−500K ExpD+ + W 3−200eV, T: 320−500K ExpD+ + W 3−200eV, T: 320−500K ExpD2

+ + W 3−200eV, T: 320−500K ExpD3

+ + W 3−200eV, T: 320−500K ExpD+ + W 3−200eV, T: 320−500K ExpD2

+ + W 3−200eV, T: 320−500K ExpD3

+ + W 3−200eV, T: 320−500K Exp

322

1560. A. Manhard, K. Schmid, M. Balden, W JacobInfluence of the microstructure on the deuterium retention in tungstenJ. Nucl. Mater. 415, S632 (2011)

D3+ + W 38eV, T: 300K Exp

D3+ + W 38eV, T: 300K Exp

D3+ + W 38eV, T: 300K Exp

D3+ + W 38eV, T: 300K Exp

1561. T LoarerFuel retention in tokamaksJ. Nucl. Mater. 391-91, 20 (2009)

T + Be undef, T: undef E/TT + W undef, T: undef E/TT + C undef, T: undef E/TD + W undef, T: undef E/TD + Mo undef, T: undef E/TT + Be undef, T: undef E/TT + W undef, T: undef E/TT + C undef, T: undef E/TD + W undef, T: undef E/TD + Mo undef, T: undef E/TT + Be undef, T: undef E/TT + W undef, T: undef E/TT + C undef, T: undef E/TD + W undef, T: undef E/TD + Mo undef, T: undef E/TT + Be undef, T: undef E/TT + W undef, T: undef E/TT + C undef, T: undef E/TD + W undef, T: undef E/TD + Mo undef, T: undef E/T

1562. K.. Ohya, N.. Mohara, K.. Inai, A.. Ito, H.. Nakamura, A.. Kirschner, D. BorodinMolecular dynamics and dynamic Monte Carlo studies of mixed materials and theirimpact on plasma wall interactionsFusion Eng. Des. 85, 1167 (2010)

C + C 1−200eV, T: undef ThCH3 + Be 1−200eV, T: undef ThCH3 + H 1−200eV, T: undef ThCH3 + C 1−200eV, T: undef ThCH2 + Be 1−200eV, T: undef ThCH2 + H 1−200eV, T: undef ThCH2 + C 1−200eV, T: undef ThCH + Be 1−200eV, T: undef ThCH + H 1−200eV, T: undef ThCH + C 1−200eV, T: undef ThC + Be 1−200eV, T: undef ThC + H 1−200eV, T: undef Th

1563. Chen. Duan, Yue-Lin. Liu, Hong-Bo. Zhou, Ying. Zhang, Shuo. Jin, Guang-Hong. Lu, G. -N.LuoFirst-principles study on dissolution and diffusion properties of hydrogen inmolybdenumJ. Nucl. Mater. 404, 109 (2010)

T + Mo undef, T: 600−2000K ThD + Mo undef, T: 600−2000K ThH + Mo undef, T: 600−2000K Th

323

1564. Rudolf Ludwig NeuExperience With High-Z Plasma-Facing Materials and Extrapolation to Future DevicesIEEE Trans. Plasma Sci. 38, 453 (2010)

D + W 100−200eV, T: 298K ExpD + Mo 100−200eV, T: 298K ExpD + W 100−200eV, T: 298K ExpD + W 100−200eV, T: 298K ExpD + Mo 100−200eV, T: 298K ExpD + Mo 100−200eV, T: 298K ExpD + W 100−200eV, T: 298K ExpD + Mo 100−200eV, T: 298K Exp

1565. V.. Chakin, R.. Rolli, A.. Moeslang, P.. Kurinskiy, P.. Vladimirov, C.. Ferrero, R.. Pieritz, W.Van RenterghemStudy of helium bubble evolution in highly neutron-irradiated beryllium by using x-ray micro-tomography and metallography methodsPhys. Scr. T145, 14012 (2011)

Be + Be undef, T: 1123−1273K ExpHe + Be undef, T: 1123−1273K Exp

1566. A.. Allouche, M.. Oberkofler, M.. Reinelt, Ch. LinsmeierQuantum Modeling of Hydrogen Retention in Beryllium Bulk and VacanciesJ. Phys. Chem. C 114, 3588 (2010)

Be + H undef, T: undef ThH + H undef, T: undef ThBe + Be undef, T: undef ThH + Be undef, T: undef Th

1567. V. Kh. Alimov, B.. Tyburska-Pueschel, M. H. J.. ’t Hoen, J.. Roth, Y.. Hatano, K.. Isobe, M..Matsuyama, T. YamanishiHydrogen isotope exchange in tungsten irradiated sequentially with low-energydeuterium and protium ionsPhys. Scr. T145, 14037 (2011)

H + W 38−200eV, T: 300−750K ExpD + W 38−200eV, T: 300−750K ExpH + W 38−200eV, T: 300−750K ExpD + W 38−200eV, T: 300−750K ExpH + W 38−200eV, T: 300−750K ExpD + W 38−200eV, T: 300−750K ExpH + W 38−200eV, T: 300−750K ExpD + W 38−200eV, T: 300−750K Exp

1568. V.. Nemanic, B.. Zajec, D.. Dellasega, M. PassoniHydrogen permeation through disordered nanostructured tungsten filmsJ. Nucl. Mater. 429, 92 (2012)

Re + W undef, T: 673−873K ExpH + W undef, T: 673−873K Exp

1569. S. J.. Zenobia, G. L. KulcinskiFormation and retention of surface pores in helium-implanted nano-grain tungsten forfusion reactor first-wall materials and divertor platesPhys. Scr. T138, 14049 (2009)

He+ + W 30000eV, T: 1273−1423K ExpHe+ + W 30000eV, T: 1273−1423K ExpHe+ + W 30000eV, T: 1273−1423K ExpHe+ + W 30000eV, T: 1273−1423K Exp

324

1570. M.. Wada, T.. Kenmotsu, Y.. Matsumoto, M.. Nishiura, M.. Sasao, K.. Tsumori, H. YamaokaLow-energy particle interaction with plasma-irradiated metal surfacesPlasma Devices Oper. 17, 132 (2009)

O + W 700−2000eV, T: undef ThH2

+ + W 700−2000eV, T: undef ThH+ + W 700−2000eV, T: undef ThH+ + H 700−2000eV, T: undef ThH+ + C 700−2000eV, T: undef Th

1571. Zhongshi. Yang, Qian. Xu, Rongjie. Hong, Qiang. Li, Guang-Nan LuoMolecular dynamics simulation of low-energy atomic hydrogen on tungsten surfaceFusion Eng. Des. 85, 1517 (2010)

D + W 0.5−50eV, T: 298K ThH + W 0.5−50eV, T: 298K ThD + W 0.5−50eV, T: 298K ThH + W 0.5−50eV, T: 298K Th

1572. Yue-Lin. Liu, Hong-Bo. Zhou, Ying. Zhang, Guang-Hong. Lu, Guang-Nan LuoInteraction of C with vacancy in W: A first-principles studyComp. Mater. Sci. 50, 3213 (2011)

C + W undef, T: undef Th

1573. Pengbo. Zhang, Jijun. Zhao, Bin WenVacancy trapping mechanism for multiple hydrogen and helium in beryllium: a first-principles studyJ. Phys. Condens. Matter 24, 95004 (2012)

H + H undef, T: undef ThHe + He undef, T: undef ThHe + Be undef, T: undef ThH + Be undef, T: undef Th

1574. Y. G.. Li, W. H.. Zhou, L. F.. Huang, Z.. Zeng, X. JuCluster dynamics modeling of accumulation and diffusion of helium in neutronirradiated tungstenJ. Nucl. Mater. 431, 26 (2012)

He + W 30−1000eV, T: 837−873K Th

1575. Jingcheng. Xu, Jijun ZhaoFirst-principles study of hydrogen in perfect tungsten crystalNucl. Instrum. Methods Phys. Res. B 267, 3170 (2009)


1576. B.. Jiang, F. R.. Wan, W. T. GengStrong hydrogen trapping at helium in tungsten: Density functional theorycalculationsPhys. Rev. B 81, 134112 (2010)

He + W undef, T: undef ThH + W undef, T: undef Th

1577. Samuel J.. Zenobia, Lauren M.. Garrison, Gerald L. KulcinskiThe response of polycrystalline tungsten to 30 keV helium ion implantation at normalincidence and high temperaturesJ. Nucl. Mater. 425, 83 (2012)

325

He+ + W undef, T: 773−1173K ExpHe+ + W undef, T: 773−1173K ExpHe+ + W undef, T: 773−1173K Exp

1578. Yue-Lin. Liu, Ying. Zhang, Hong-Bo. Zhou, Guang-Hong. Lu, Feng. Liu, G. -N. LuoVacancy trapping mechanism for hydrogen bubble formation in metalPhys. Rev. B 79, 172103 (2009)


1579. R. H.. Ning, Y. G.. Li, W. H.. Zhou, Z.. Zeng, X. JuAN IMPROVED CLUSTER DYNAMICS MODEL FOR HYDROGEN RETENTIONIN TUNGSTENInt. J. Mod. Phys. C 23, 1250042 (2012)

D+ + W 200eV, T: 300−573K E/TD+ + W 200eV, T: 300−573K E/TD+ + W 200eV, T: 300−573K E/TD+ + W 200eV, T: 300−573K E/T

1580. Yue-Lin. Liu, Hong-Bo. Zhou, Shuo. Jin, Ying. Zhang, Guang-Hong LuDissolution and diffusion properties of carbon in tungstenJ. Phys. Condens. Matter 22, 445504 (2010)

C + W undef, T: 300−1000K Th

1581. Kazuhito. Ohsawa, Junya. Goto, Masahiro. Yamakami, Masatake. Yamaguchi, Masatoshi YagiTrapping of multiple hydrogen atoms in a tungsten monovacancy from first principlesPhys. Rev. B 82, 184117 (2010)

H + Fe undef, T: undef ThH + W undef, T: undef Th

1582. W.. Xiao, W. T. GengRole of grain boundary and dislocation loop in H blistering in W: A density functionaltheory assessmentJ. Nucl. Mater. 430, 132 (2012)

H + W undef, T: undef Exp

1583. JP. Allain, JN BrooksLithium surface-response modelling for the NSTX liquid lithium divertorNucl. Fusion 51, 23002 (2011)

D+ + Li 20−10000eV, T: 473−693K Th

1584. R. Ding, A. Kirschner, D. Borodin, S. Brezinsek, A. Kreter, MZ. Tokar, J. Chen, O. Schmitz, V.Philipps, U. Samm, J LiModelling of local carbon deposition from methane and ethene injection throughgraphite and tungsten test limiters in TEXTORPlasma Phys. and Controlled Fusion 52, 45005 (2010)

C2H4 + W undef, T: undef E/TCH4 + W undef, T: undef E/TC2H4 + C undef, T: undef E/TCH4 + C undef, T: undef E/T

1585. RP. Doerner, MJ. Baldwin, PC StangebyAn equilibrium model for tungsten fuzz in an eroding plasma environmentNucl. Fusion 51, 43001 (2011)

326

He+ + W 60−250eV, T: 1120−1320K Exp

1586. RP. Doerner, D. Nishijima, T Schwarz-SelingerMeasuring the difference between gross and net erosionNucl. Fusion 52, 103003 (2012)

He+ + Be 20−160eV, T: undef E/TBe + Be 20−160eV, T: undef E/TD3

+ + Be 20−160eV, T: undef E/TD2

+ + Be 20−160eV, T: undef E/TD+ + Be 20−160eV, T: undef E/T

1587. A KirschnerEROSION AND DEPOSITION MECHANISMS IN FUSION PLASMASFusion Sci. Technol. 57, 277 (2010)

CH4 + C 0.1−1000eV, T: 400−1400K E/TC + C 0.1−1000eV, T: 400−1400K E/TC + W 0.1−1000eV, T: 400−1400K E/TD+ + Be 0.1−1000eV, T: 400−1400K E/TCH4 + C 0.1−1000eV, T: 400−1400K E/TC + C 0.1−1000eV, T: 400−1400K E/TC + W 0.1−1000eV, T: 400−1400K E/TD+ + Be 0.1−1000eV, T: 400−1400K E/T

1588. R NeuPreparing the scientific basis for an all metal ITERPlasma Phys. and Controlled Fusion 53, 124040 (2011)

D + WC undef, T: 273−873K ExpD + BeO undef, T: 273−873K ExpD + BeC undef, T: 273−873K ExpD + W undef, T: 273−873K ExpD + Be undef, T: 273−873K ExpD + C undef, T: 273−873K Exp

1589. M. Oberkofler, C LinsmeierProperties of nitrogen-implanted beryllium and its interaction with energeticdeuteriumNucl. Fusion 50, 125001 (2010)

D + N 2000eV, T: undef ExpD + Be 2000eV, T: undef Exp

1590. AI. Ryazanov, VS. Koidan, BI. Khripunov, ST. Latushkin, VB. Petrov, LS. Danelyan, EV.Semenov, VN UnezhevINVESTIGATIONS OF RADIATION DAMAGE EFFECTS ON ITERSTRUCTURAL AND PLASMA-FACING MATERIALSFusion Sci. Technol. 61, 107 (2012)

D + C 100eV, T: ¡313K Exp

1591. K. Schmid, A. Manhard, C. Linsmeier, A. Wiltner, T. Schwarz-Selinger, W. Jacob, S MandlInteraction of nitrogen plasmas with tungstenNucl. Fusion 50, 25006 (2010)

N + W 20−500V, T: 350K E/TN + W 20−500V, T: 350K E/TN + W 20−500V, T: 350K E/TN + W 20−500V, T: 350K E/T

327

1592. BD. Wirth, K. Nordlund, DG. Whyte, D XuFusion materials modeling: Challenges and opportunitiesMRS BULLETIN 36, 216 (2011)

D + Be 10−100eV, T: undef E/T

1593. RP. Doerner, MJ. Baldwin, G. De Temmerman, J. Hanna, D. Nishijima, J. Roth, K. Schmid, GR.Tynan, K UmstadterCodeposition of deuterium with ITER materialsNucl. Fusion 49, 35002 (2009)

D + Be 10−100eV, T: 273−1073K E/TD + W 10−100eV, T: 273−1073K E/TD + C 10−100eV, T: 273−1073K E/TD + Be 10−100eV, T: 273−1073K E/TD + W 10−100eV, T: 273−1073K E/TD + C 10−100eV, T: 273−1073K E/TD + Be 10−100eV, T: 273−1073K E/TD + W 10−100eV, T: 273−1073K E/TD + C 10−100eV, T: 273−1073K E/TD + Be 10−100eV, T: 273−1073K E/TD + W 10−100eV, T: 273−1073K E/TD + C 10−100eV, T: 273−1073K E/T

1594. CF. Sang, X. Bonnin, M. Warrier, A. Rai, R. Schneider, JZ. Sun, DZ WangModelling of hydrogen isotope inventory in mixed materials including porous depositedlayers in fusion devicesNucl. Fusion 52, 43003 (2012)

D + C 200−1500eV, T: 300−1000K E/TH + C 200−1500eV, T: 300−1000K E/TT + W 200−1500eV, T: 300−1000K E/TD + W 200−1500eV, T: 300−1000K E/TH + W 200−1500eV, T: 300−1000K E/TT + C 200−1500eV, T: 300−1000K E/TD + C 200−1500eV, T: 300−1000K E/TH + C 200−1500eV, T: 300−1000K E/TT + W 200−1500eV, T: 300−1000K E/TD + W 200−1500eV, T: 300−1000K E/TH + W 200−1500eV, T: 300−1000K E/TT + C 200−1500eV, T: 300−1000K E/TH + W 200−1500eV, T: 300−1000K E/TD + W 200−1500eV, T: 300−1000K E/TT + W 200−1500eV, T: 300−1000K E/TH + C 200−1500eV, T: 300−1000K E/TD + C 200−1500eV, T: 300−1000K E/TT + C 200−1500eV, T: 300−1000K E/TH + W 200−1500eV, T: 300−1000K E/TD + W 200−1500eV, T: 300−1000K E/TT + W 200−1500eV, T: 300−1000K E/TH + C 200−1500eV, T: 300−1000K E/TD + C 200−1500eV, T: 300−1000K E/TT + C 200−1500eV, T: 300−1000K E/T

1595. S. Takamura, T. Miyamoto, N OhnoEffects of fibre-form nanostructures on particle emissions from a tungsten surface inplasmasNucl. Fusion 52, 123001 (2012)

Ar + W 20−180eV, T: undef Exp

328

1596. A. Yamawaki, M. Fukumoto, Y. Soga, Y. Ohtsuka, Y. Ueda, K OhyaTemperature dependence of carbon deposition on TungstenFusion Sci. Technol. 56, 1038 (2009)

D + C 50eV, T: 473−973K Th

1597. T. Ikeda, T. Otsuka, T TanabeAPPLICATION OF TRITIUM TRACER TECHNIQUE TO DETERMINATIONOF HYDROGEN DIFFUSION COEFFICIENTS AND PERMEATION RATENEAR ROOM TEMPERATURE FOR TUNGSTENFusion Sci. Technol. 60, 1463 (2011)

H + W undef, T: 273−2000K Exp

1598. DF. Johnson, EA CarterHydrogen in tungsten: Absorption, diffusion, vacancy trapping, and decohesionJ. Mater. Res. 25, 315 (2010)

H + W undef, T: 500−1450K ThD + W undef, T: 500−1450K ThT + W undef, T: 500−1450K Th

1599. YG. Li, WH. Zhou, RH. Ning, LF. Huang, Z. Zeng, X JuA Cluster Dynamics Model for Accumulation of Helium in Tungsten under HeliumIons and Neutron IrradiationCommun. Comput. Phys. 11, 1547 (2012)

He + W 1000−5000eV, T: 300−873K E/THe + W 1000−5000eV, T: 300−873K E/THe + W 1000−5000eV, T: 300−873K E/THe + W 1000−5000eV, T: 300−873K E/T

1600. HB. Zhou, YL. Liu, S. Jin, Y. Zhang, GN. Luo, GH LuTowards suppressing H blistering by investigating the physical origin of the H-Heinteraction in WNucl. Fusion 50, 115010 (2010)

H + W undef, T: undef ThHe + W undef, T: undef Th

1601. MJ. Baldwin, RP. Doerner, WR. Wampler, D. Nishijima, T. Lynch, M MiyamotoEffect of He on D retention in W exposed to low-energy, high-fluence (D, He, Ar)mixture plasmas (vol 51, 103021, 2011)Nucl. Fusion 51, 119501 (2011)

D2 + W 30−200eV, T: 420−1100K ExpHe + W 30−200eV, T: 420−1100K ExpAr + W 30−200eV, T: 420−1100K ExpD2 + W 30−200eV, T: 420−1100K ExpHe + W 30−200eV, T: 420−1100K ExpAr + W 30−200eV, T: 420−1100K ExpD2 + W 30−200eV, T: 420−1100K ExpHe + W 30−200eV, T: 420−1100K ExpAr + W 30−200eV, T: 420−1100K ExpD2 + W 30−200eV, T: 420−1100K ExpHe + W 30−200eV, T: 420−1100K ExpAr + W 30−200eV, T: 420−1100K Exp

1602. B. Lipschultz, DG. Whyte, J. Irby, B. LaBombard, GM WrightHydrogenic retention with high-Z plasma facing surfaces in Alcator C-ModNucl. Fusion 49, 45009 (2009)

329

D+ + Mo undef, T: undef ExpD+ + W undef, T: undef ExpHe+ + Mo undef, T: undef ExpHe+ + W undef, T: undef ExpD+ + Mo undef, T: undef ExpD+ + W undef, T: undef ExpHe+ + Mo undef, T: undef ExpHe+ + W undef, T: undef ExpD+ + Mo undef, T: undef ExpD+ + W undef, T: undef ExpHe+ + Mo undef, T: undef ExpHe+ + W undef, T: undef ExpD+ + Mo undef, T: undef ExpD+ + W undef, T: undef ExpHe+ + Mo undef, T: undef ExpHe+ + W undef, T: undef Exp

1603. M. Miyamoto, D. Nishijima, Y. Ueda, RP. Doerner, H. Kurishita, MJ. Baldwin, S. Morito, K. Ono,J HannaObservations of suppressed retention and blistering for tungsten exposed to deuterium-helium mixture plasmasNucl. Fusion 49, 65035 (2009)

D + W 40−70eV, T: ¡573K ExpHe + W 40−70eV, T: ¡573K ExpD + W 40−70eV, T: ¡573K ExpHe + W 40−70eV, T: ¡573K ExpD + W 40−70eV, T: ¡573K ExpHe + W 40−70eV, T: ¡573K ExpD + W 40−70eV, T: ¡573K ExpHe + W 40−70eV, T: ¡573K Exp

1604. Y. Song, QY. Huang, MY NiAnalysis of Plasma-Driven Tritium Permeation Through the First Wall of DFLL-TBMin ITERPlasma Sci. Technol. 11, 730 (2009)

T + F82H undef, T: undef ThT + Be undef, T: undef Th

1605. Y. Zayachuk, MHJ. ’t Hoen, PAZ. van Emmichoven, I. Uytdenhouwen, G van OostDeuterium retention in tungsten and tungsten-tantalum alloys exposed to high-fluxdeuterium plasmasNucl. Fusion 52, 103021 (2012)

D + W ¡50eV, T: ¡480K ExpD + Ta ¡50eV, T: ¡480K ExpD + W ¡50eV, T: ¡480K ExpD + Ta ¡50eV, T: ¡480K ExpD + W ¡50eV, T: ¡480K ExpD + Ta ¡50eV, T: ¡480K ExpD + W ¡50eV, T: ¡480K ExpD + Ta ¡50eV, T: ¡480K Exp

1606. MHJ. ’t Hoen, B. Tyburska-Puschel, K. Ertl, M. Mayer, J. Rapp, AW. Kleyn, PAZ vanEmmichovenSaturation of deuterium retention in self-damaged tungsten exposed to high-fluxplasmasNucl. Fusion 52, 23008 (2012)

330

D + W 0.5−5eV(Te), T: ¡525K ExpD + W 0.5−5eV(Te), T: ¡525K ExpD + W 0.5−5eV(Te), T: ¡525K ExpD + W 0.5−5eV(Te), T: ¡525K Exp

1607. WR. Wampler, RP DoernerThe influence of displacement damage on deuterium retention in tungsten exposed toplasmaNucl. Fusion 49, 115023 (2009)

D + W undef, T: 314−773K ExpHe + W undef, T: 314−773K ExpD + W undef, T: 314−773K ExpHe + W undef, T: 314−773K ExpD + W undef, T: 314−773K ExpHe + W undef, T: 314−773K ExpD + W undef, T: 314−773K ExpHe + W undef, T: 314−773K Exp

1608. GM. Wright, E. Alves, LC. Alves, NP. Barradas, PA. Carvalho, R. Mateus, J RappHydrogenic retention of high-Z refractory metals exposed to ITER divertor-relevantplasma conditionsNucl. Fusion 50, 75006 (2010)

D + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K ExpD + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K ExpD + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K ExpD + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K Exp

1609. GM. Wright, E. Alves, LC. Alves, NP. Barradas, PA. Carvalho, R. Mateus, J RappHydrogenic retention of high-Z refractory metals exposed to ITER divertor-relevantplasma conditionsNucl. Fusion 50, 55004 (2010)

D + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K ExpD + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K ExpD + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K ExpD + Mo ¡5eV(Te), T: 600−1600K ExpD + W ¡5eV(Te), T: 600−1600K Exp

1610. I. Takagi, K. Yamamichi, R. Imade, T. Sasaki, H. Tsuchida, K. Moritani, H MoriyamaTHERMAL GROWTH OF HYDROGEN TRAP IN ION-IRRADIATED WFusion Sci. Technol. 60, 1451 (2011)

D + W undef, T: undef ExpD + W undef, T: undef ExpD + W undef, T: undef ExpD + W undef, T: undef Exp

1611. SJ. Zenobia, GL KulcinskiRETENTION AND SURFACE PORE FORMATION IN HELIUM IMPLANTEDTUNGSTEN AS A FUSION FIRST WALL MATERIALFusion Sci. Technol. 56, 352 (2009)

331

He+ + W undef, T: 1123−1273K ExpHe+ + W undef, T: 1123−1273K ExpHe+ + W undef, T: 1123−1273K ExpHe+ + W undef, T: 1123−1273K Exp

1612. H. Zush, Y. Hirooka, K. Okamoto, R. Bhattacharyay, M. Sakamoto, M. SatoDYNAMIC RESPONSE OF HYDROGEN REEMISSION AND RETENTION FROMAND IN INERT GAS SPRAYED TUNGSTEN EXPOSED TO ECR PLASMASFusion Sci. Technol. 55, 9 (2009)

H+ + W 15−25eV, T: 450−900K ExpHe+ + W 15−25eV, T: 450−900K ExpH+ + W 15−25eV, T: 450−900K ExpHe+ + W 15−25eV, T: 450−900K ExpH+ + W 15−25eV, T: 450−900K ExpHe+ + W 15−25eV, T: 450−900K ExpH+ + W 15−25eV, T: 450−900K ExpHe+ + W 15−25eV, T: 450−900K Exp

1613. ZZ Chen, N GhoniemBiaxial strain effects on adatom surface diffusion on tungsten from first principlesPhys. Rev. B 88, 35415 (2013)

W + W undefined

1614. XG Yu, FJ GouMolecular Dynamics Study on the Diffusion Properties of Hydrogen Atoms in BulkTungstenPlasma Sci. Technol. 15, 710 (2013)

H + W undefined

1615. Y Ferro, A Allouche, C LinsmeierAbsorption and diffusion of beryllium in graphite, beryllium carbide formationinvestigated by density functional theoryJ. Appl. Phys. 113, 213514 (2013)

Be + C undefinedBe + BeC undefinedBe + C undefinedBe + BeC undefinedBe + C undefinedBe + BeC undefinedBe + C undefinedBe + BeC undefinedBe + C undefinedBe + BeC undefined

1616. XL Shu, P Tao, XC Li, Y YuHelium diffusion in tungsten: A molecular dynamics studyNucl. Instrum. Methods Phys. Res. B 303, 84 (2013)

He + W T: 50−3000K

1617. A Drenik, L Salamon, R Zaplotnik, A Vesel, M MozeticErosion of amorphous carbon layers in the afterglow of oxygen microwave plasmaVACUUM 98, 45 (2013)

O + CH undef, T: 473−623K

332

1618. V Yakushin, V Polsky, B Kalin, P Dzhumaev, A Polyansky, O Sevryukov, A Suchkov, V FedotovErosion of tungsten and its brazed joints with bronze irradiated by pulsed deuteriumplasma flowsJ. Nucl. Mater. 442, S237 (2013)

D + W ¡2000eV, T: 1173−1223K

1619. X Yang, A HassaneinMolecular dynamics simulation of erosion and surface evolution of tungsten due tobombardment with deuterium and carbon in Tokamak fusion environmentsNucl. Instrum. Methods Phys. Res. B 308, 80 (2013)

D + W 1−250eV, T: 300−1500KC + W 1−250eV, T: 300−1500KD + WC 1−250eV, T: 300−1500KC + WC 1−250eV, T: 300−1500K

1620. RP Doerner, C Bjorkas, D Nishijima, T Schwarz-SelingerErosion of beryllium under high-flux plasma impactJ. Nucl. Mater. 438, S272 (2013)

D+ + Be 10−140eV, T: ¡330KD2

+ + Be 10−140eV, T: ¡330KD3

+ + Be 10−140eV, T: ¡330KD+ + BeD 10−140eV, T: ¡330KD2

+ + BeD 10−140eV, T: ¡330KD3

+ + BeD 10−140eV, T: ¡330K

1621. K Katayama, Y Ohnishi, T Honda, K Uehara, S Fukada, M Nishikawa, N Ashikawa, T UdaHydrogen incorporation into metal deposits forming from tungsten or stainless steelby sputtering under mixed hydrogen and argon plasma at elevated temperatureJ. Nucl. Mater. 438, S1010 (2013)

H + W 200−300eV, T: 373−773KAr + W 200−300eV, T: 373−773KH + SS 200−300eV, T: 373−773KAr + SS 200−300eV, T: 373−773KH + W 200−300eV, T: 373−773KAr + W 200−300eV, T: 373−773KH + SS 200−300eV, T: 373−773KAr + SS 200−300eV, T: 373−773KH + W 200−300eV, T: 373−773KAr + W 200−300eV, T: 373−773KH + SS 200−300eV, T: 373−773KAr + SS 200−300eV, T: 373−773KH + W 200−300eV, T: 373−773KAr + W 200−300eV, T: 373−773KH + SS 200−300eV, T: 373−773KAr + SS 200−300eV, T: 373−773KH + W 200−300eV, T: 373−773KAr + W 200−300eV, T: 373−773KH + SS 200−300eV, T: 373−773KAr + SS 200−300eV, T: 373−773K

1622. M Laengner, S Brezinsek, JW Coenen, A Pospieszczyk, D Kondratyev, D Borodin, H Stoschus, OSchmitz, V Philipps, U SammPenetration depths of injected/sputtered tungsten in the plasma edge layer ofTEXTORJ. Nucl. Mater. 438, S865 (2013)

D + W 1−100eV(Te), T: undef

333

1623. F Sefta, N Juslin, KD Hammond, BD WirthMolecular dynamics simulations on the effect of sub-surface helium bubbles on thesputtering yield of tungstenJ. Nucl. Mater. 438, S493 (2013)

He + W 300−1000eV, T: 298K

1624. GJ van Rooij, JW Coenen, L Aho-Mantila, S Brezinsek, M Clever, R Dux, M Groth, K Krieger, SMarsen, GF Matthews, A Meigs, R Neu, S Potzel, T Putterich, J Rapp, MF StampTungsten divertor erosion in all metal devices: Lessons from the ITER like wall of JETJ. Nucl. Mater. 438, S42 (2013)

D + W 1−50eV(Te), T: undef

1625. Y Yuan, H Greuner, B Boswirth, GN Luo, BQ Fu, HY Xu, W LiuMelt layer erosion of pure and lanthanum doped tungsten under VDE-like high heatflux loadsJ. Nucl. Mater. 438, S229 (2013)

H + W 20000eV, T: undef

1626. C Bjorkas, D Borodin, A Kirschner, RK Janev, D Nishijima, R Doerner, K NordlundMolecules can be sputtered also from pure metals: sputtering of beryllium hydride byfusion plasma-wall interactionsPlasma Phys. and Controlled Fusion 55, 74004 (2013)

D+ + BeD 5−100eV, T: 300−725KD+ + BeW 5−100eV, T: 300−725KD2

+ + BeD 5−100eV, T: 300−725KD2

+ + BeW 5−100eV, T: 300−725KD3

+ + BeD 5−100eV, T: 300−725KD3

+ + BeW 5−100eV, T: 300−725K

1627. XH Tang, LQ Shi, Q Qi, B Zhang, WY Zhang, JS Hu, DJ O’Connor, B KingDeuterium retention in the carbon co-deposition layers deposited by magnetronsputtering in D-2/He atmosphereJ. Nucl. Mater. 436, 93 (2013)

D2 + Cd 210eV, T: 300−773KHe + Cd 210eV, T: 300−773KD2 + Cd 210eV, T: 300−773KHe + Cd 210eV, T: 300−773KD2 + Cd 210eV, T: 300−773KHe + Cd 210eV, T: 300−773KD2 + Cd 210eV, T: 300−773KHe + Cd 210eV, T: 300−773K

1628. Y Furuta, I Takagi, S Kawamura, K Yamamichi, M Akiyoshi, T Sasaki, T KobayashiIn situ deuterium observation in deuterium-implanted tungstenNucl. Instrum. Methods Phys. Res. B 315, 121 (2013)

D + W 3000eV, T: 384−673KD + W 3000eV, T: 384−673KD + W 3000eV, T: 384−673KD + W 3000eV, T: 384−673K

1629. H Atsumi, Y Takemura, T Miyabe, T Konishi, T Tanabe, T ShikamaDesorption of hydrogen trapped in carbon and graphiteJ. Nucl. Mater. 442, S746 (2013)

334

H + C undef, T: undefH + C undef, T: undefH + C undef, T: undefH + C undef, T: undef

1630. I Takagi, K Yamamichi, Y Furuta, M Akiyoshi, T Sasaki, H Tsuchida, Y HatanoIn situ observation of deuterium trapping in self-ion irradiated tungstenJ. Nucl. Mater. 442, S246 (2013)


1631. HB Zhou, X Ou, Y Zhang, XL Shu, YL Liu, GH LuEffect of carbon on helium trapping in tungsten: A first-principles investigationJ. Nucl. Mater. 440, 338 (2013)

He + WC undef, T: undefHe + WC undef, T: undefHe + WC undef, T: undefHe + WC undef, T: undefHe + WC undef, T: undef

1632. L Begrambekov, V Barsuk, M Dubrov, A Kaplevsky, N Klimov, D Kovalenko, A Kuzmin, AMischenko, V Podkovyrov, P Shigin, A Zhitlukhin, A ZakharovDeuterium trapping in carbon films formed in different deposition conditionsJ. Nucl. Mater. 438, S971 (2013)

H2 + C 5−8eVHD + C 5−8eVD2 + C 5−8eVH2 + C 5−8eVHD + C 5−8eVD2 + C 5−8eVH2 + C 5−8eVHD + C 5−8eVD2 + C 5−8eVH2 + C 5−8eVHD + C 5−8eVD2 + C 5−8eV

1633. Y Hatano, M Shimada, VK Alimov, J Shi, M Hara, T Nozaki, Y Oya, M Kobayashi, K Okuno,T Oda, G Cao, N Yoshida, N Futagami, K Sugiyama, J Roth, B Tyburska-Puschel, J Dorner, ITakagi, M Hatakeyama, H Kurishita, MA SokolovTrapping of hydrogen isotopes in radiation defects formed in tungsten by neutron andion irradiationsJ. Nucl. Mater. 438, S114 (2013)

D + W undef, T: 673−973KD + W undef, T: 673−973KD + W undef, T: 673−973KD + W undef, T: 673−973K

1634. Y Hatano, M Shimada, T Otsuka, Y Oya, VK Alimov, M Hara, J Shi, M Kobayashi, T Oda, G Cao,K Okuno, T Tanaka, K Sugiyama, J Roth, B Tyburska-Puschel, J Dorner, N Yoshida, N Futagami,H Watanabe, M Hatakeyama, H Kurishita, M Sokolov, Y KatohDeuterium trapping at defects created with neutron and ion irradiations in tungstenNucl. Fusion 53, 73006 (2013)

335

D + W 1−400eV, T: 473−773KD + W 1−400eV, T: 473−773KD + W 1−400eV, T: 473−773KD + W 1−400eV, T: 473−773K

1635. A Alkhamees, HB Zhou, YL Liu, S Jin, Y Zhang, GH LuVacancy trapping behaviors of oxygen in tungsten: A first-principles studyJ. Nucl. Mater. 437, 6 (2013)

O + W undef, T: undefO + W undef, T: undefO + W undef, T: undefO + W undef, T: undefO + W undef, T: undef

1636. X Yang, A HassaneinMolecular dynamics simulation of deuterium trapping and bubble formation intungstenJ. Nucl. Mater. 434, 1 (2013)

D + W 5−100eV, T: 600−2000K

1637. L Sun, S Jin, XC Li, Y Zhang, GH LuHydrogen behaviors in molybdenum and tungsten and a generic vacancy trappingmechanism for H bubble formationJ. Nucl. Mater. 434, 395 (2013)

H + Mo undef, T: 50−1500KH + W undef, T: 50−1500KH + Mo undef, T: 50−1500KH + W undef, T: 50−1500KH + Mo undef, T: 50−1500KH + W undef, T: 50−1500KH + Mo undef, T: 50−1500KH + W undef, T: 50−1500KH + Mo undef, T: 50−1500KH + W undef, T: 50−1500K

1638. PE Lhuillier, T Belhabib, P Desgardin, B Courtois, T Sauvage, MF Barthe, AL Thomann, PBrault, Y TessierHelium retention and early stages of helium-vacancy complexes formation in lowenergy helium-implanted tungstenJ. Nucl. Mater. 433, 305 (2013)

He + W 320eV, T: undefHe + W 320eV, T: undefHe + W 320eV, T: undefHe + W 320eV, T: undef

1639. A Ying, HB Liu, M AbdouANALYSIS OF TRITIUM/DEUTERIUM RETENTION AND PERMEATION INFW/DIVERTOR INCLUDING GEOMETRIC AND TEMPERATUREOPERATING FEATURESFusion Sci. Technol. 64, 303 (2013)

T + W 200eV, T: 300−623KD + W 200eV, T: 300−623KT + W 200eV, T: 300−623KD + W 200eV, T: 300−623KT + W 200eV, T: 300−623K

336

D + W 200eV, T: 300−623KT + W 200eV, T: 300−623KD + W 200eV, T: 300−623KT + W 200eV, T: 300−623KD + W 200eV, T: 300−623K

1640. L Begrambekov, A Ayrapetov, V Ermakov, A Kaplevsky, Y Sadovsky, P ShiginHydrogen and oxygen trapping and retention in stainless steel and graphite materialsirradiated in plasmaNucl. Instrum. Methods Phys. Res. B 315, 110 (2013)

H + SS 10−1000eV, T: undefO + SS 10−1000eV, T: undefH + C 10−1000eV, T: undefO + C 10−1000eV, T: undefH + SS 10−1000eV, T: undefO + SS 10−1000eV, T: undefH + C 10−1000eV, T: undefO + C 10−1000eV, T: undefH + SS 10−1000eV, T: undefO + SS 10−1000eV, T: undefH + C 10−1000eV, T: undefO + C 10−1000eV, T: undefH + SS 10−1000eV, T: undefO + SS 10−1000eV, T: undefH + C 10−1000eV, T: undefO + C 10−1000eV, T: undef

1641. MHJ t Hoen, M Mayer, AW Kleyn, H Schut, PAZ van EmmichovenReduced deuterium retention in self-damaged tungsten exposed to high-flux plasmasat high surface temperaturesNucl. Fusion 53, 43003 (2013)

D + W ¡1.6eV, T: ¡1250KD + W ¡1.6eV, T: ¡1250KD + W ¡1.6eV, T: ¡1250KD + W ¡1.6eV, T: ¡1250K

1642. B Zajec, V Nemanic, M Zumer, C Porosnicu, CP LunguHydrogen permeability through beryllium films and the impact of surface oxidesJ. Nucl. Mater. 443, 185 (2013)

H + Be undef, T: 673KH + BeO undef, T: 673KH + Be undef, T: 673KH + BeO undef, T: 673KH + Be undef, T: 673KH + BeO undef, T: 673KH + Be undef, T: 673KH + BeO undef, T: 673KH + Be undef, T: 673KH + BeO undef, T: 673K

1643. A Rivera, G Valles, MJ Caturla, I Martin-BragadoEffect of ion flux on helium retention in helium-irradiated tungstenNucl. Instrum. Methods Phys. Res. B 303, 81 (2013)

He + W undef, T: 700−1600KHe + He undef, T: 700−1600KHe + W undef, T: 700−1600K

337

He + He undef, T: 700−1600KHe + W undef, T: 700−1600KHe + He undef, T: 700−1600KHe + W undef, T: 700−1600KHe + He undef, T: 700−1600K

1644. PV Vladimirov, A MoeslangAb initio static and molecular dynamics studies of helium behavior in berylliumJ. Nucl. Mater. 442, S694 (2013)

He + Be undef, T: undef

1645. Y Torikai, A Taguchi, M Saito, RD Penzhorn, Y Ueda, H Kurishita, K Sugiyama, V Philipps, AKreter, M ZlobinskiTritium loading study of tungsten pre-exposed to TEXTOR plasmasJ. Nucl. Mater. 438, S1121 (2013)

T + W 140eV, T: 573KT + W 140eV, T: 573KT + W 140eV, T: 573KT + W 140eV, T: 573K

1646. Y Oya, S Masuzaki, T Fujishima, M Tokitani, N Yoshida, H Watanabe, Y Yamauchi, T Hino, MMiyamoto, Y Hatano, K OkunoEnhancement of hydrogen isotope retention in tungsten exposed to LHD plasmasJ. Nucl. Mater. 438, S1055 (2013)

D2+ + W 1000eV, T: ¡373K

H + W 1000eV, T: ¡373KD2

+ + W 1000eV, T: ¡373KH + W 1000eV, T: ¡373KD2

+ + W 1000eV, T: ¡373KH + W 1000eV, T: ¡373KD2

+ + W 1000eV, T: ¡373KH + W 1000eV, T: ¡373K

1647. J Roth, T Schwarz-Selinger, VK Alimov, E MarkinaHydrogen isotope exchange in tungsten: Discussion as removal method for tritiumJ. Nucl. Mater. 432, 341 (2013)

H + W 200eV, T: 320−450KH + W 200eV, T: 320−450KH + W 200eV, T: 320−450KH + W 200eV, T: 320−450KH + W 200eV, T: 320−450KD + W 200eV, T: 320−450KD + W 200eV, T: 320−450KD + W 200eV, T: 320−450KD + W 200eV, T: 320−450KD + W 200eV, T: 320−450K

1648. CF Sang, JZ Sun, X Bonnin, SG Liu, DZ WangNumerical simulation of the bubble growth due to hydrogen isotopes inventoryprocesses in plasma-irradiated tungstenJ. Nucl. Mater. 443, 403 (2013)

D + W 20eV, T: 300−1200K

1649. TV Kulsartov, YN Gordienko, IL Tazhibayeva, EA Kenzhin, NI Barsukov, AO Sadvakasova, AVKulsartova, ZA ZaurbekovaTritium migration in the materials proposed for fusion reactors: Li2TiO3 and berylliumJ. Nucl. Mater. 442, S740 (2013)

338

D + Be undef, T: 570−1333KT + Be undef, T: 570−1333KHe + Be undef, T: 570−1333K

1650. Q Xu, K Sato, XZ Cao, P Zhang, BY Wang, T Yoshiie, H Watanabe, N YoshidaInteraction of deuterium with vacancies induced by ion irradiation in WNucl. Instrum. Methods Phys. Res. B 315, 146 (2013)

D2+ + W 500eV, T: 298K

D2+ + W 500eV, T: 298K

D2+ + W 500eV, T: 298K

D2+ + W 500eV, T: 298K

D2+ + W 500eV, T: 298K

1651. V Chakin, R Rolli, A Moeslang, M Klimenkov, M Kolb, P Vladimirov, P Kurinskiy, HC Schneider,S van Til, AJ Magielsen, M ZmitkoTritium release and retention properties of highly neutron-irradiated beryllium pebblesfrom HIDOBE-01 experimentJ. Nucl. Mater. 442, S483 (2013)

T + Be undef, T: 298−1373KT + He undef, T: 298−1373KT + Be undef, T: 298−1373KT + He undef, T: 298−1373KT + Be undef, T: 298−1373KT + He undef, T: 298−1373KT + Be undef, T: 298−1373KT + He undef, T: 298−1373K

1652. P Wang, W Jacob, L Gao, T Durbeck, T Schwarz-SelingerComparing deuterium retention in tungsten films measured by temperatureprogrammed desorption and nuclear reaction analysisNucl. Instrum. Methods Phys. Res. B 300, 54 (2013)

D3+ + W 38eV, T: 370−600K

D3+ + W 38eV, T: 370−600K

D3+ + W 38eV, T: 370−600K

D3+ + W 38eV, T: 370−600K

1653. VK Alimov, Y Hatano, B Tyburska-Puschel, K Sugiyama, I Takagi, Y Furuta, J Dorner, M Fusseder,K Isobe, T Yamanishi, M MatsuyamaDeuterium retention in tungsten damaged with W ions to various damage levelsJ. Nucl. Mater. 441, 280 (2013)


1654. AV Arzhannikov, VA Bataev, IA Bataev, AV Burdakov, IA Ivanov, MV Ivantsivsky, KN Kuklin,KI Mekler, AF Rovenskikh, SV Polosatkin, VV Postupaev, SL Sinitsky, AA ShoshinSurface modification and droplet formation of tungsten under hot plasma irradiationat the GOL-3J. Nucl. Mater. 438, S677 (2013)

undef + W undef, T: undef

1655. A Rusinov, M Sakamoto, K Honda, R Ohyama, N Yoshida, H Zushi, T Tanabe, I TakagiDEUTERIUM RETENTION IN TUNGSTEN WITH DIFFERENT GRAINELONGATION DIRECTION IRRADIATED BY PLASMA IN APSEDASFusion Sci. Technol. 63, 229 (2013)

339

D + W 30eV, T: 500KD + W 30eV, T: 500KD + W 30eV, T: 500KD + W 30eV, T: 500K

1656. J Roth, R Doerner, M Baldwin, T Dittmar, H Xu, K Sugiyama, M Reinelt, C Linsmeier, MOberkoflerOxidation of beryllium and exposure of beryllium oxide to deuterium plasmas inPISCES BJ. Nucl. Mater. 438, S1044 (2013)

D+ + Be 1−300eV, T: 273−523KD2

+ + Be 1−300eV, T: 273−523KD3

+ + Be 1−300eV, T: 273−523KD+ + Be 1−300eV, T: 273−523KD2

+ + Be 1−300eV, T: 273−523KD3

+ + Be 1−300eV, T: 273−523KD+ + Be 1−300eV, T: 273−523KD2

+ + Be 1−300eV, T: 273−523KD3

+ + Be 1−300eV, T: 273−523KD+ + Be 1−300eV, T: 273−523KD2

+ + Be 1−300eV, T: 273−523KD3

+ + Be 1−300eV, T: 273−523K

1657. JL Barton, YQ Wang, T Schwarz-Selinger, RP Doerner, GR TynanIsotope exchange experiments in tungsten with sequential deuterium and protiumplasmas in PISCESJ. Nucl. Mater. 438, S1183 (2013)

D2+ + W 110eV, T: ¡373K

H2+ + W 110eV, T: ¡373K

D2+ + W 110eV, T: ¡373K

H2+ + W 110eV, T: ¡373K

D2+ + W 110eV, T: ¡373K

H2+ + W 110eV, T: ¡373K

D2+ + W 110eV, T: ¡373K

H2+ + W 110eV, T: ¡373K

1658. F Sefta, KD Hammond, N Juslin, BD WirthTungsten surface evolution by helium bubble nucleation, growth and ruptureNucl. Fusion 53, 73015 (2013)

He + W 60eV, T: 500−2000K

1659. T Otsuka, T Tanabe, K TokunagaRetention and release mechanisms of tritium loaded in plasma-sprayed tungstencoatings by plasma exposureJ. Nucl. Mater. 438, S1048 (2013)

T + W 400eV, T: 453−573KT + W 400eV, T: 453−573KT + W 400eV, T: 453−573KT + W 400eV, T: 453−573K

1660. M Zlobinski, V Philipps, B Schweer, A Huber, M Reinhart, S Moller, G Sergienko, U Samm, MHJt Hoen, A Manhard, K SchmidHydrogen retention in tungsten materials studied by Laser Induced DesorptionJ. Nucl. Mater. 438, S1155 (2013)

340


1661. VK Alimov, Y Hatano, K Sugiyama, J Roth, B Tyburska-Puschel, J Dorner, J Shi, M Matsuyama,K Isobe, T YamanishiThe effect of displacement damage on deuterium retention in tungsten exposed to Dneutrals and D-2 gasJ. Nucl. Mater. 438, S959 (2013)

D + W 1−150eV, T: 423−1073KD2 + W 1−150eV, T: 423−1073KD + W 1−150eV, T: 423−1073KD2 + W 1−150eV, T: 423−1073KD + W 1−150eV, T: 423−1073KD2 + W 1−150eV, T: 423−1073KD + W 1−150eV, T: 423−1073KD2 + W 1−150eV, T: 423−1073K

1662. K SchmidImplementation of a diffusion convection surface evolution model in WallDYNJ. Nucl. Mater. 438, S484 (2013)

Be + Be 300−500eV, T: undefD + Be 300−500eV, T: undefAr + Be 300−500eV, T: undefBe + Be 300−500eV, T: undefD + Be 300−500eV, T: undefAr + Be 300−500eV, T: undefBe + Be 300−500eV, T: undefD + Be 300−500eV, T: undefAr + Be 300−500eV, T: undefBe + Be 300−500eV, T: undefD + Be 300−500eV, T: undefAr + Be 300−500eV, T: undefBe + Be 300−500eV, T: undefD + Be 300−500eV, T: undefAr + Be 300−500eV, T: undef

1663. B Tyburska-Puschel, VK AlimovOn the reduction of deuterium retention in damaged Re-doped WNucl. Fusion 53, 123021 (2013)

D2+ + ReW 76eV, T: 350−750K

D+ + ReW 76eV, T: 350−750KD2

+ + ReW 76eV, T: 350−750KD+ + ReW 76eV, T: 350−750KD2

+ + ReW 76eV, T: 350−750KD+ + ReW 76eV, T: 350−750KD2

+ + ReW 76eV, T: 350−750KD+ + ReW 76eV, T: 350−750K

1664. M Oya, K Uekita, HT Lee, Y Ohtsuka, Y Ueda, H Kurishita, A Kreter, JW Coenen, V Philipps, SBrezinsek, A Litnovsky, K Sugiyama, Y TorikaiDeuterium retention in Toughened, Fine-Grained Recrystallized TungstenJ. Nucl. Mater. 438, S1052 (2013)


341

1665. A Sagara, R Nygren, M Miyamoto, D Nishijima, R Doerner, S Fukada, Y Oya, T Oda, Y Watanabe,K Morishita, F Gao, T NorimatsuIntegrated Material System Modeling of Fusion BlanketMat. Trans. 54, 477 (2013)

He+ + W 10−10000eV, T: 298−1600KD+ + W 10−10000eV, T: 298−1600KHe+ + W 10−10000eV, T: 298−1600KD+ + W 10−10000eV, T: 298−1600KHe+ + W 10−10000eV, T: 298−1600KD+ + W 10−10000eV, T: 298−1600KHe+ + W 10−10000eV, T: 298−1600KD+ + W 10−10000eV, T: 298−1600K

1666. MHJ t Hoen, M Mayer, AW Kleyn, PAZ van EmmichovenStrongly Reduced Penetration of Atomic Deuterium in Radiation-Damaged TungstenPhys. Rev. Lett. 111, 22 (2013)

D + W 5eV, T: 470−560K

1667. Y Oya, M Shimada, T Tokunaga, H Watanabe, N Yoshida, Y Hatano, R Kasada, T Nagasaka, AKimura, K OkunoBehavior of deuterium retention and surface morphology for VPS-W/F82HJ. Nucl. Mater. 442, S242 (2013)

D + W 100−1500eV, T: 300−473KD2

+ + W 100−1500eV, T: 300−473KD + W 100−1500eV, T: 300−473KD2

+ + W 100−1500eV, T: 300−473KD + W 100−1500eV, T: 300−473KD2

+ + W 100−1500eV, T: 300−473KD + W 100−1500eV, T: 300−473KD2

+ + W 100−1500eV, T: 300−473K

1668. O El-Atwani, M Efe, B Heim, JP AllainSurface damage in ultrafine and multimodal grained tungsten materials induced bylow energy helium irradiationJ. Nucl. Mater. 434, 170 (2013)

He + W 200eV, T: 1223K

1669. V Borovikov, XZ Tang, D Perez, XM Bai, BP Uberuaga, AF VoterCoupled motion of grain boundaries in bcc tungsten as a possible radiation-damagehealing mechanism under fusion reactor conditionsNucl. Fusion 53, 63001 (2013)

W + W undef, T: undef

1670. A Keim, M Harnisch, P Scheier, Z HermanCollisions of low-energy ions Ar + and N-2( + ) with room-temperature and heatedsurfaces of tungsten, beryllium, and a mixed beryllium-tungsten thin filmInt. J. Mass Spectrom. 354, 78 (2013)

Ar+ + Be 15−70eV, T: 298−573KAr+ + W 15−70eV, T: 298−573KAr+ + BeW 15−70eV, T: 298−573KN2

+ + Be 15−70eV, T: 298−573KN2

+ + W 15−70eV, T: 298−573KN2

+ + BeW 15−70eV, T: 298−573K

342

1671. C Bjorkas, K NordlundVariables affecting simulated Be sputtering yieldsJ. Nucl. Mater. 439, 174 (2013)

D + Be 5−100eV, T: 300KBe + Be 5−100eV, T: 300K

1672. M Miyamoto, D Nishijima, MJ Baldwin, RP Doerner, Y Ueda, A Sagara, H KurishitaMicrostructures and Deuterium-Retention Behavior of Tungsten Exposed to D + (Heand/or Be) Mixture PlasmasMat. Trans. 54, 420 (2013)

D+ + W 60eV, T: 573KHe + W 60eV, T: 573KBe + W 60eV, T: 573KD+ + W 60eV, T: 573KHe + W 60eV, T: 573KBe + W 60eV, T: 573KD+ + W 60eV, T: 573KHe + W 60eV, T: 573KBe + W 60eV, T: 573KD+ + W 60eV, T: 573KHe + W 60eV, T: 573KBe + W 60eV, T: 573K

1673. A Lasa, KOE Henriksson, K NordlundMD simulations of onset of tungsten fuzz formation under helium irradiationNucl. Instrum. Methods Phys. Res. B 303, 156 (2013)

He + W 60eV, T: 573−1603KC + W 60eV, T: 573−1603K

1674. BI Khripunov, VM Gureev, VS Koidan, SN Kornienko, ST Latushkin, VB Petrov, AI Ryazanov,EV Semenov, VG Stolyarova, LS Danelyan, VS Kulikauskas, VV Zatekin, VN UnezhevStudy of ion-irradiated tungsten in deuterium plasmaJ. Nucl. Mater. 438, S1014 (2013)

D + W 250eV, T: ¡373K

1675. P Wang, W Jacob, L Gao, T DurbeckDeuterium retention in tungsten-doped amorphous carbon films exposed to deuteriumplasmaJ. Nucl. Mater. 438, S1134 (2013)

D + WC 30−100eV, T: undefD + WC 30−100eV, T: undefD + WC 30−100eV, T: undefD + WC 30−100eV, T: undef

1676. Y Hatano, M Shimada, Y Oya, GP Cao, M Kobayashi, M Hara, BJ Merrill, K Okuno, MA Sokolov,Y KatohRetention of Hydrogen Isotopes in Neutron Irradiated TungstenMat. Trans. 54, 437 (2013)

D + W 100eV, T: 373−773KD + W 100eV, T: 373−773KD + W 100eV, T: 373−773KD + W 100eV, T: 373−773KD + W 100eV, T: 373−773K

343

1677. JT Zhao, Q Wang, TS Wang, XX Xu, S Zhang, YS Zhou, XC Guan, KH Fang, J KasagiDynamical saturated concentration of deuterium in a beryllium foil studied by lowenergy D(d,p)T reactionNucl. Instrum. Methods Phys. Res. B 316, 13 (2013)

D3+ + Be 20000−75000eV, T: ¡340K

D3+ + Be 20000−75000eV, T: ¡340K

D3+ + Be 20000−75000eV, T: ¡340K

D3+ + Be 20000−75000eV, T: ¡340K

1678. K Sugiyama, C Porosnicu, W Jacob, J Roth, T Durbeck, I Jepu, CP LunguStudy of deuterium retention in/release from ITER-relevant Be-containing mixedmaterial layers implanted at elevated temperaturesJ. Nucl. Mater. 438, S1113 (2013)

D + Be 200eV, T: 398−623KD + BeW 200eV, T: 398−623KD + BeC 200eV, T: 398−623KD + Be 200eV, T: 398−623KD + BeW 200eV, T: 398−623KD + BeC 200eV, T: 398−623KD + Be 200eV, T: 398−623KD + BeW 200eV, T: 398−623KD + BeC 200eV, T: 398−623KD + Be 200eV, T: 398−623KD + BeW 200eV, T: 398−623KD + BeC 200eV, T: 398−623K

1679. XB Wu, XS Kong, YW You, CS Liu, QF Fang, JL Chen, GN Luo, ZG WangEffects of alloying and transmutation impurities on stability and mobility of helium intungsten under a fusion environmentNucl. Fusion 53, 73049 (2013)

He + W undef, T: undefHe + Be undef, T: undefHe + C undef, T: undefHe + N undef, T: undefHe + O undef, T: undefHe + Re undef, T: undefHe + Ta undef, T: undefHe + Nb undef, T: undefHe + V undef, T: undefHe + Ti undef, T: undefHe + Si undef, T: undefHe + Zr undef, T: undefHe + Y undef, T: undefHe + Sc undef, T: undefHe + W undef, T: undefHe + Be undef, T: undefHe + C undef, T: undefHe + N undef, T: undefHe + O undef, T: undefHe + Re undef, T: undefHe + Ta undef, T: undefHe + Nb undef, T: undefHe + V undef, T: undefHe + Os undef, T: undefHe + Ti undef, T: undefHe + Si undef, T: undefHe + Zr undef, T: undef

344

He + Y undef, T: undefHe + Sc undef, T: undefHe + W undef, T: undefHe + Be undef, T: undefHe + C undef, T: undefHe + N undef, T: undefHe + O undef, T: undefHe + Re undef, T: undefHe + Ta undef, T: undefHe + Nb undef, T: undefHe + V undef, T: undefHe + Os undef, T: undefHe + Ti undef, T: undefHe + Si undef, T: undefHe + Zr undef, T: undefHe + Y undef, T: undefHe + Sc undef, T: undefHe + W undef, T: undefHe + Be undef, T: undefHe + C undef, T: undefHe + N undef, T: undefHe + O undef, T: undefHe + Re undef, T: undefHe + Ta undef, T: undefHe + Nb undef, T: undefHe + V undef, T: undefHe + Os undef, T: undefHe + Ti undef, T: undefHe + Si undef, T: undefHe + Zr undef, T: undefHe + Y undef, T: undefHe + Sc undef, T: undefHe + W undef, T: undefHe + Be undef, T: undefHe + C undef, T: undefHe + N undef, T: undefHe + O undef, T: undefHe + Re undef, T: undefHe + Ta undef, T: undefHe + Nb undef, T: undefHe + V undef, T: undefHe + Ti undef, T: undefHe + Si undef, T: undefHe + Zr undef, T: undefHe + Y undef, T: undefHe + Sc undef, T: undef

1680. Y Zayachuk, MHJ t Hoen, PAZ van Emmichoven, D Terentyev, I Uytdenhouwen, G van OostSurface modification of tungsten and tungsten-tantalum alloys exposed to high-fluxdeuterium plasma and its impact on deuterium retentionNucl. Fusion 53, 13013 (2013)

D + W 50eV, T: 460−510KD + Ta 50eV, T: 460−510KD + W 50eV, T: 460−510KD + Ta 50eV, T: 460−510KD + W 50eV, T: 460−510KD + Ta 50eV, T: 460−510KD + W 50eV, T: 460−510KD + Ta 50eV, T: 460−510K

345

1681. A Adachi, M Yoshida, T Takeishi, T Tanabe, T Hayashi, T Nakano, M Fukumoto, J Yagyuu, YMiyo, K Masaki, K ItamiTritium retention to the first wall of JT-60UFusion Eng. Des. 88, 295 (2013)

T + C undef, T: 1273KT + C undef, T: 1273KT + C undef, T: 1273KT + C undef, T: 1273K

3.4 Data Collection, Bibliographic and Progress Report

1682. Ch Jungen, S. T. PrattLow-energy dissociative recombination in small polyatomic moleculesJ. Chem. Phys. 133, 214303 (2010)

e + ND4+ 0.001−1eV

e + NH4+ 0.001−1eV

e + CH5+ 0.001−1eV

e + NO+ 0.001−1eVe + H3O

+ 0.001−1eV

1683. Do Anh Tuan, Byung-Hoon JeonDetermination of the Momentum Transfer Cross-section for the Cl-2 Molecule in aPlasma Discharge SimulationJ. Korean Phys. Soc. 57, 1224 (2010)

e + Cl2 0.01 − 100 eV Exp

1684. J. Gregorio, L. C. PitchfordUpdated compilation of electron-Cl-2 scattering cross sectionsPlasma Sources Sci. Technol. 21, 032002 (2012)

e + Cl2 0.01−100eV E/T

1685. X. Llovet, C. J. Powell, F. Salvat, A. JablonskiCross Sections for Inner-Shell Ionization by Electron ImpactJ. Phys. Chem. Ref. Data 43, 013102 (2014)

e + Cl 5−1E6 keV The + S 5−1E6 keV The + Al 5−1E6 keV The + Mg 5−1E6 keV The + Na 5−1E6 keV The + O 5−1E6 keV The + H 5−1E6 keV The + C 5−1E6 keV The + Bi 5−1E6 keV The + Ta 5−1E6 keV The + Xe 5−1E6 keV The + Au 5−1E6 keV The + Ag 5−1E6 keV The + Y 5−1E6 keV The + Fe 5−1E6 keV The + Si 5−1E6 keV The + N 5−1E6 keV The + Pt 5−1E6 keV The + Os 5−1E6 keV The + Re 5−1E6 keV Th

346

e + Hf 5−1E6 keV The + Dy 5−1E6 keV The + I 5−1E6 keV The + U 5−1E6 keV The + Pb 5−1E6 keV The + W 5−1E6 keV The + Tm 5−1E6 keV The + Er 5−1E6 keV The + Ho 5−1E6 keV The + Gd 5−1E6 keV The + Eu 5−1E6 keV The + Sm 5−1E6 keV The + Nd 5−1E6 keV The + Pr 5−1E6 keV The + Ce 5−1E6 keV The + La 5−1E6 keV The + Te 5−1E6 keV The + Sb 5−1E6 keV The + Sn 5−1E6 keV The + In 5−1E6 keV The + Cd 5−1E6 keV The + Pd 5−1E6 keV The + Mo 5−1E6 keV The + Nb 5−1E6 keV The + Zr 5−1E6 keV The + Sr 5−1E6 keV The + Rb 5−1E6 keV The + Kr 5−1E6 keV The + Br 5−1E6 keV The + Se 5−1E6 keV The + As 5−1E6 keV The + Ge 5−1E6 keV The + Ga 5−1E6 keV The + Zn 5−1E6 keV The + Cu 5−1E6 keV The + Ni 5−1E6 keV The + Co 5−1E6 keV The + Mn 5−1E6 keV The + Cr 5−1E6 keV The + V 5−1E6 keV The + Ti 5−1E6 keV The + Sc 5−1E6 keV The + Ca 5−1E6 keV The + K 5−1E6 keV The + Ar 5−1E6 keV Th

1686. M. C. BordageComparisons of sets of electron-neutral scattering cross sections and swarm parametersin noble gases: III. Krypton and xenonJ. Phys. D 46, 334003 (2014)

e + Xe 0.01−400eV E/Te + Kr 0.01−400eV E/T

1687. L. L. Alves, K Bartschat, S. F. Biagi, M. C. BordageComparisons of sets of electron-neutral scattering cross sections and swarm parametersin noble gases: II. Helium and neonJ. Phys. D 46, 334002 (2014)

e + Ne 20−1000eV E/Te + He 20−1000eV E/T

347

1688. L. C. Pitchford, L. L. Alves, K BartschatComparisons of sets of electron-neutral scattering cross sections and swarm parametersin noble gases: I. ArgonJ. Phys. D 46, 334001 (2014)

e + Ar 0.01−200eV E/T

3.5 Interactions of Atomic Particles with Fields

1689. Ph V. Demekhin, I. D. Petrov, V. L. Sukhorukov, al. etStrong interference effects in the angularly resolved Auger decay and fluorescenceemission spectra of the core-excited NO moleculeJ. Phys. B 43, 165103 (2010)

B5+ + NO 399 −401eV

1690. Hao Xu, Robin ShakeshaftR-matrix approach with proper boundary conditions for dissipative and nondissipativecollision processesPhys. Rev. A 83, 012714 (2011)

P + He 80−240 eV Th

1691. Hao Xu, Robin ShakeshaftR-matrix approach to collision processes: Study of the threshold behavior of gammaplus He -¿ He+(2s) plus e(-) or He+(2p) plus e(-)Phys. Rev. A 83, 012716 (2011)

P + He 65−71 eV Th

1692. Sterling, N. C.Atomic data for neutron-capture elements II. Photoionization and recombinationproperties of low-charge krypton ionsAstron. Astrophys. 533, A62 (2011)

e + Kr 1E1−1E8 K The + Kr+ 1E1−1E8 K The + Kr2+ 1E1−1E8 K The + Kr3+ 1E1−1E8 K The + Kr4+ 1E1−1E8 K The + Kr5+ 1E1−1E8 K The + Kr6+ 1E1−1E8 K ThP + Kr 1E1−1E8 K ThP + Kr+ 1E1−1E8 K ThP + Kr2+ 1E1−1E8 K ThP + Kr3+ 1E1−1E8 K ThP + Kr4+ 1E1−1E8 K ThP + Kr5+ 1E1−1E8 K ThP + Kr6+ 1E1−1E8 K Th

348

Chapter 3

Author Index

’t Hoen M. H. J. 1440, 1486, 1567, 1605, 1606A Bari M. 1216Abdalmoneam M. H. 341Abdel-Naby S. 1019, 1163Abdel-Naby S. A. 956, 964, 980Abdel-Naby Sh. A. 861Abdelaziz W. S. 203Abdellahi ElGhazaly M. O. 521Abdollahi-Tadi R. 1093Abdou M. 1639Abdurakhmanov I. B. 1386, 1391Abou El-Maaref A. 52, 172, 232, 280, 398, 436Abu-Haija O. 1387, 1388Adachi A. 1681Adamowicz L. 24, 89, 222, 264, 382Adams N. G. 601, 877, 878, 880Adams S. F. 796Adaniya H. 889, 905Adelhelm C. 1443, 1465Adelman S. J. 425AfUgglas M. 1020, 1021Aggarwal K. M. 50, 72, 73, 84, 171, 178, 179, 187,218, 270, 272, 284, 298, 300, 426, 428, 438, 444,446, 620, 731, 865, 1010, 1011, 1012, 1015, 1016,1150, 1156, 1159, 1164, 1294, 1329, 1330, 1331Aggarwal S. 42, 55, 69, 119, 164, 174, 176, 207,283, 286, 348, 437, 439, 475Agnihotri A. N. 33Aguiar J. C. 101, 258Aguilar A. 331, 337Aguilera J. A. 196Ahlgren T. 1548Ahmad M. 280, 436Aho-Mantila L. 1624Airila M. I. 1401Ajana I. 1286Ajdari B. 538, 544, 545, 993Akita K. 620Akita K. i. 805, 807Akiyoshi M. 1483, 1628, 1630Aktaa J. 1495Aktasb B. 1208Al R. S. 1440, 1460, 1543Al Shorman M. M. 108, 344Al-Hagan O. 531, 554, 564Albaridy R. 860Alfaz Uddin M. 511, 512, 754Ali E. 1097, 1300Ali R. 488Ali S. 924Alimov V. 1429Alimov V. K. 1522, 1525, 1536, 1538, 1544, 1545,

1554, 1558, 1633, 1634, 1647, 1653, 1661, 1663Alimov V. Kh. 1567Alkauskas A. 47, 170, 266, 423Alkhamees A. 1499, 1635Allain J. P. 1396, 1398, 1452, 1502, 1583, 1668Allam S. H. 52, 172, 280, 436Allan M. 594, 608, 669, 709, 761, 778, 822, 830,837, 1006, 1192Allen T. R. 1517Allende Prieto C. 150Aller L. H. 144, 145Allouche A. 1471, 1472, 1481, 1566, 1615Alna’washi G. A. 1268, 1269Alonizan N. 464Alonso-Medina A. 139, 154, 448Alshaiub R. 124, 213Altevogt S. 898, 904Alves E. 1460, 1534, 1543, 1608, 1609Alves L. C. 1460, 1534, 1543, 1608, 1609Alves L. L. 1273, 1274, 1687, 1688Amami S. 1086, 1282, 1285Amaro P. 8, 114, 201, 281, 360Amorim E. 259Amorim P. 103Ampleford D. J. 121Amusia M. Y. 1190An Z. 555, 648, 660, 661, 809Ancarani L. U. 1151Anderson L. W. 565, 755Andersson M. 184, 198, 450Andreev O. V. 364Andreev O. Y. 915Andrianarijaona V. M. 904Andric L. 40, 830Androic D. 913Angeli C. 37Anghel A. 1455, 1506, 1521, 1537Angom D. 318Angot T. 1442Annaloro J. 977Anshu 867Antony B. 766, 856, 949, 1099, 1110, 1120, 1126,1147, 1180, 1253, 1255, 1256Antony B. K. 785Anzai K. 936, 959, 1074Aouchiche H. 819, 1113Aparicio J. A. 409Aragon C. 196Araki K. 1394Arcimowicz B. 16Areou E. 1442Argaman U. 66

349

Ariyasinghe W. M. 609, 722Armstrong D. S. 913Armstrong G. 1196Arora B. 192Arretche F. 515, 715, 1358Artamonova T. O. 536Artemyev A. N. 70, 896, 1382Arvieux J. 913Aryal N. B. 1268, 1269Arzhannikov A. V. 1654Asahina T. 591, 636Asghar H. 488Ashbourn J. M. A. 342Ashikawa N. 1542, 1621Assafrao D. 1358Atsumi H. 1629Aumayr F. 1431Ayrapetov A. 1640Azuma Y. 293, 332, 469, 983Babich I. L. 462Bacar Go. 230, 231, 249Bacar Gu. 231, 249Baccarelli I. 557, 605Bacher A. 510Backer A. D. 1515Backodissa-Kiminou D. R. 1204Badnell N. R. 242, 243, 401, 404, 405, 692, 729,730, 887, 919, 1019, 1038, 1052, 1064, 1065, 1066,1202, 1210, 1211, 1213, 1215, 1241, 1323Baek W. Y. 1111Bahati E. M. 553, 681, 851Bai X. M. 1669Baig M. A. 413, 488Bailey S. L. 913Balat-Pichelin M. 1428Balazs L. 1463Balch G. 1185Balden M. 1393, 1404, 1405, 1443, 1465, 1508,1512, 1547, 1560Baldwin M. 1422, 1521, 1656Baldwin M. J. 1394, 1406, 1409, 1416, 1427, 1501,1519, 1585, 1593, 1601, 1603, 1672Ballance C. P. 9, 202, 331, 533, 542, 548, 639, 641,646, 682, 700, 728, 783, 794, 838, 843, 861, 956,982, 1038, 1052, 1157, 1163, 1260, 1323Baluja K. L. 523, 547, 562, 678, 685, 693, 771, 839,855, 990, 1003, 1146, 1171, 1317Bannister M. E. 553, 681, 687, 851Baral K. K. 1268, 1269Barday R. 1043Bari M. A. 1128Barot A. 949, 1082, 1147, 1175, 1295, 1297Barot M. 952Barot M. Y. 939Barradas N. P. 1460, 1534, 1543, 1608, 1609Barrow J. D. 36Barstow M. A. 36Barsuk V. 1632Barsukov N. I. 1649

Barszczewska W. 945Bart M. 1092Barthe M. F. 1473, 1515, 1529, 1539, 1638Bartlett P. L. 659, 664, 665Barton J. L. 1657Bartschat K. 111, 199, 307, 309, 452, 454, 518,549, 551, 552, 586, 644, 650, 673, 773, 778, 792,822, 825, 826, 835, 864, 984, 985, 989, 995, 996,1002, 1079, 1124, 1144, 1145, 1153, 1165, 1166,1173, 1174, 1186, 1273, 1274, 1277, 1296, 1305,1307, 1308, 1364, 1687, 1688Basak A. K. 511, 512, 714, 754, 1118Bashkin S. 142Basuki W. W. 1495Bata S. S. 545Bataev I. A. 1654Bataev V. A. 1654Batha S. H. 351Baumann T. 386Baumann T. M. 1311Bautista M. A. 1335Bazylev B. 1430, 1469Becher M. 520Beck A. R. 317Beck D. H. 913Beck D. R. 341Becker A. 295, 791, 925, 1152, 1194, 1279Becker K. 1179Becker W. 589Becquart C. S. 1494, 1515Begrambekov L. 1632, 1640Begrambekov L. B. 1555Behar E. 388Beiersdorfer P. 1, 10, 20, 71, 82, 94, 131, 136, 146,156, 177, 190, 211, 227, 235, 248, 253, 296, 363,369, 370, 383, 387, 395, 443, 489, 883, 1041Beigman I. 787Beilmann C. 35, 211, 487, 1311Beise E. J. 913Belhabib T. 1473, 1539, 1638Beliaeva A. A. 536Belic D. S. 508, 509, 521, 628, 629, 630, 653, 746,829, 931, 943, 1112Belie D. S. 674Belkacem A. 889, 905Belkhiri M. 1304Bell M. J. 317Bellm S. 1097, 1300Bellm S. M. 907, 1073Belmonte M. T. 409Ben Nessib N. 464BenLakhdar Z. 626BenNessib N. 968, 1013Bencsura A. 951Benesch J. 913Bengtsson P. 5, 149Benmokhtar F. 913Bennadji K. 99, 193Berengut J. C. 36, 60, 247

350

Berg M. H. 706, 712, 898Bernhardt B. 317Bernhardt D. 182, 295, 621, 895, 896, 1022, 1023,1050, 1152, 1279Bernitt S. 35, 211, 487Bernshtam V. A. 575Berrington M. J. 914, 988Berset M. 546Betancourt-Martinez G. L. 370Bettega 859Bettega M. H. 1326Bettega M. H. F. 498, 566, 610, 708, 727, 804, 854,862, 903, 994, 1081, 1352Bharadvaja A. 839, 1146Bhargava Ram N. 872, 911Bhatia A. K. 87, 493, 494, 603, 1345, 1346Bhatt P. 683, 853, 986, 1168Bhattacharyay R. 1535, 1612Bhattacharyya S. 33Bhushan K. G. 585Bhutadia H. 634, 635, 638, 752, 766, 856Biagi S. 1071Biagi S. F. 1273, 1687Bian G. J. 229, 273, 397, 429Biaye M. 225, 380Bielschowsky C. E. 1182Bielski A. 870Bieron J. 391, 479Biewer T. M. 320Bimbot L. 913Bing D. 706, 712, 898Birchall J. 913Birkl G. 98Bitter M. 363Bizau J. M. 108, 344Bizyukov I. 1513Bjorkas C. 1395, 1401, 1410, 1412, 1415, 1433,1620, 1626, 1671Blaess C. 299, 445Blancard C. 108, 344Blanco F. 591, 662, 719, 759, 765, 826, 884, 907,936, 948, 950, 959, 1076, 1183, 1184, 1186, 1352,1354Blaum K. 41, 377Blin-Simiand N. 504Blondel C. 1047Blundell S. A. 83Boblest S. 7, 78Boechat-Roberty H. M. 1182Boehm S. 896Boffard J. B. 565, 755Bogdanovich P. 45, 167, 181, 271, 427, 466Bohme D. K. 510Bolorizadeh M. A. 590Bonnin X. 1594, 1648Booth J. P. 1166Bordage M. C. 1071, 1272, 1273, 1686, 1687Boretskij V. F. 462Borodin D. 787, 1408, 1423, 1425, 1440, 1460,

1549, 1562, 1584, 1622, 1626Borovik A. 518, 530, 789, 1107, 1173, 1259, 1262,1278Borovik Jr A. 297, 517, 791, 802, 1108, 1123Borovikov V. 1669Borovoy N. A. 1181Bosch F. 896Bosted P. 913Bostock 886Bostock C. 769Bostock C. J. 561, 563, 711, 833, 914, 988, 1053,1055, 1083, 1132, 1277, 1287, 1302Boswirth B. 1625Bote D. 497Botheron P. 1379Bouamoud M. 957, 1142Bouarissa N. 583Bouazza S. 86, 90, 91Boucard S. 76Bouchiha D. 524Bougas L. 457Bowen I. S. 145Bowen K. P. 9Bowring N. 773, 1188Bozkurt G. 1176Bradley P. A. 351Brage T. 1, 146, 182, 184, 198, 289, 291, 308, 333,441, 450, 453, 479Brandau C. 287, 802, 896Brault P. 1473, 1539, 1638Braun J. 125Braun M. 1197Bray B. D. 1436Bray I. 297, 517, 527, 528, 534, 549, 561, 563, 586,672, 676, 684, 711, 769, 773, 777, 833, 834, 902,914, 988, 1005, 1008, 1053, 1055, 1072, 1083, 1095,1132, 1188, 1277, 1278, 1290, 1293, 1299, 1302,1356, 1359, 1360, 1386, 1391Brenner G. 372, 386Brescansin L. M. 559, 717, 720, 723, 725, 848,1070, 1075Breuer H. 913Brewer N. R. 410Brewer S. M. 95, 459Brezinsek S. 787, 1400, 1407, 1408, 1429, 1436,1440, 1444, 1447, 1460, 1541, 1584, 1622, 1624,1664Brickhouse N. S. 235, 248, 253Brigg W. J. 942Bristow P. 135Brodersen P. 1464Brons S. 1460Brookes S. 1102Brookesa S. 1337Brooks J. N. 1398, 1583Brooks N. H. 1436Brotton S. J. 550, 760, 803, 817Brown G. V. 35, 136, 211, 370, 387, 487Brown R. C. 95

351

Bruch R. 142Bruhns H. 125Brukhanov A. 1432Brukhanov A. N. 1438, 1449Brunger M. J. 514, 528, 560, 590, 703, 719, 758,759, 800, 826, 884, 936, 948, 950, 959, 1036, 1073,1106, 1114, 1183, 1184, 1186, 1250, 1352, 1354,1355Brunton J. R. 826, 884, 1186, 1224, 1261Bryans P. 570Bubin S. 24, 89, 222, 264, 382Buchenauer D. A. 1514, 1517Buckman S. J. 528, 590, 703, 765, 826, 884, 936,959, 1036, 1183, 1186, 1224, 1351, 1356Budker D. 457Buenker R. J. 1060Bug M. U. 1111Buhr H. 706, 712, 898, 904, 1061, 1194Bull J. N. 966, 1092Bultel A. 977Burdakov A. V. 1654Burrow P. D. 615Bystrov K. 1435, 1510Bzowski M. 1333C. N. 1344, 1692Cadez I. 912, 938Caffarel M. 53Cai J. 346Cai X. 908Calderoni P. 1509, 1517, 1540Calvayrac F. 1246Campbell C. 989Campbell L. 514, 758, 936Campeanu R. I. 934Canetti M. 1403Canuto S. 566Cao G. 1509, 1633, 1634Cao G. P. 1676Cao L. 1096, 1138, 1237Cao L. F. 77, 100Cao W. 546, 821Cao X. N. 130Cao X. Z. 1650Capitelli M. 997Capitta G. 997Cappello D. 1312Caprasecca S. 524, 557, 1087Capuano C. L. 913Caradonna P. 1351, 1356Cardozo N. 1543Cardozo N. J. L. 1440, 1460Carette T. 112, 310Carette Th. 67Carniato S. 1380Caron L. G. 524Carsky P. 1006Carter E. A. 1598Carvalho P. A. 1534, 1608, 1609Casagrande M. S. 1271

Casagrande S. 961Cassidy C. M. 618, 733, 1017Castro E. A. Y. 717Caturla M. J. 1493, 1643Causey R. 1429Causey R. A. 1514, 1517, 1540Celiberto R. 541, 558, 842, 930, 979, 997, 1017,1018, 1098, 1155, 1171, 1301, 1316, 1317, 1318Celik G. 434, 435Cerkic A. 589Chakin V. 1565, 1651Chakrabarti K. 526, 935, 1161, 1204, 1310Chaluvadi H. 1086, 1088, 1193Champion C. 583, 679, 819, 840, 1044, 1113, 1291Champion N. 299, 445Chang J. C. 670Chantler C. T. 38, 110, 288, 334, 353, 411Chao Y. C. 913Charpentier I. 529, 812, 849, 1312Chatterjee S. 519Chattopadhyay S. 318Chen 841Chen C. 4, 26, 62, 93, 102, 122, 148, 189, 194, 261,422, 710Chen C. Y. 336, 471, 506, 571, 580, 651, 696, 732,922Chen E. S. 1236Chen F. 4, 102, 148, 194Chen H. J. 499Chen J. 1584Chen J. J. 1116Chen J. L. 1441, 1462, 1485, 1531, 1679Chen Jun-Ling. 1474Chen M. H. 393Chen S. 223Chen W. C. 282Chen X. 992Chen X. J. 824Chen Y. 105, 116, 117Chen Z. 581, 781, 846Chen Z. B. 282, 442, 1226, 1313Chen Z. J. 1116Chen Z. Z. 1613Cheng X. L. 499, 694Cheng Y. 640, 793Cheng Y. J. 183, 501Cherkani-Hassani H. 628, 629, 630, 633, 943Cherkani-Hassani S. 628, 633, 746, 943Chernov V. E. 12, 123, 128, 152, 210, 347, 474Chernysheva L. V. 1190Chiari L. 719, 1184, 1352, 1354, 1355Chilenski M. A. 342Chin J. H. 1350Cho G. 1129Cho H. 590, 699, 936, 1239, 1349Cho Y. S. 1094Choi E. H. 1129Choubisa R. 1119Chourou S. T. 595, 596, 897

352

Chowdhury U. 1376Christopher J. 886Chugunov O. K. 1432, 1449Chuluunbaatar O. 1037Chung K. T. 389Chutjian A. 1383Ciappina M. 774Ciappina M. F. 1373Cihelka J. 128Cisneros C. 337Ciurylo R. 870Civiv s S. 12, 123, 128, 133, 152, 210, 347, 474Cizek M. 724Clark R. W. 121Clementson J. 1, 10, 82, 146, 211Clever M. 1624Clift W. M. 1517Coad J. P. 1409, 1447Coad P. 1429Coenen J. W. 1407, 1408, 1622, 1624, 1664Coffey I. H. 320, 1164Cohen M. 326Colavecchia F. D. 1151Colgan J. 527, 531, 537, 554, 783, 834, 964, 980,1007, 1193, 1196, 1373, 1374Colon C. 139, 154, 448Colyer C. 564Colyer C. J. 907Compan J. 1469Contributors J. E. 320Coppens A. 913Cornaggia C. 1198Costa A. M. 33, 486Costa R. F. 1326Costin C. 1454Counsell G. 1429Courtois B. 1473, 1638Covita D. S. 76Cowan J. J. 158, 217, 417, 483Crabtree K. 1061Crabtree K. N. 712Crasemann B. 393Cremona A. 1403Crespo Lopez Urrutia J. R. 386Crespo Lopez-Urrutia J. R. 35, 125, 211, 292, 371,372, 487Crosby D. N. 110Crowe A. 844, 1144Cubaynes D. 108, 344Cubric D. 773, 1188Curik R. 798, 1006, 1205Currell F. J. 896Curry J. J. 361Cvejanovi D. 825Cvejanovic D. 549Cwang Y. 793D’Arcy R. 385DONG C. 1314DaCosta R. F. 498, 708, 994

DaSilva G. B. 1186DaSilva L. S. S. 515Dai S. 1419Dai Z. W. 204, 415, 468DalCappello C. 529, 770, 774, 786, 812, 840, 849,971, 1130Dampc M. 763, 775, 933Dance M. 1117Danelyan L. 1458Danelyan L. S. 1438, 1457, 1590, 1674Danielsson M. 705Das M. 335, 470Das T. 304, 451, 814, 1000, 1014, 1328Dasgupta A. 121Dau P. D. 1247Dave R. 634Davis C. A. 913Davis J. W. 1436, 1464, 1513, 1557De Groot B. 1460, 1543De Pol M. J. V. 1543De Saint-Aubinc G. 1532De Temmerman G. 1440, 1450, 1460, 1593DeMoura A. F. 1357DeSanctis M. L. 955DeSouza G. 1182DeSouza G. L. C. 720, 725, 848, 910, 1070, 1075,1254DeWitt D. 142DeYonker N. J. 373Deb B. M. 390Deb N. C. 58, 408Debelle A. 1529, 1539Defrance P. 508, 509, 521, 645, 653, 746, 747, 780,943, 1112, 1264, 1312Del Zanna G. 13, 153, 240, 242, 243, 401, 402, 404,405, 492, 1065, 1066, 1067, 1189, 1210, 1211, 1212,1213DelZanna G. 1064, 1215Delabie E. 320Delanis D. 413Delgado-Aparicio L. 342Dellasega D. 1568Dembczynski J. 16, 230, 256, 419Demekhin P. V. 1689Demir G. 249Den Hartog E. A. 217, 410Deng B. 219, 1138Deng B. L. 77, 273, 274, 429, 430Deng S. H. M. 687, 851Denifl S. 912, 1366Derbov V. L. 1136Deschaud B. 99, 193Desgardin P. 1473, 1529, 1539, 1638Deshmukh P. C. 584Dey R. 810, 849, 971Di L. 921Di Rocco H. O. 101, 258Diakhate B. 225Diallo S. 813

353

Diatta C. S. 813Diaz F. 20, 156, 369Diedhiou I. A. 813Dieng M. 68, 225, 380Dimitrijevic M. S. 328, 464, 465Ding C. X. 1462Ding D. J. 65Ding R. 1423, 1549, 1584Ding X. B. 220, 357, 362, 368Ding Y. N. 572Dingfelder M. 820Diop B. 68Dipti 304, 451Dittmar T. 1406, 1656Dixit G. 186Dixit S. K. 329Djurovic S. 409Do A. T. 1160Do T. P. T. 759, 950Dobes K. 1431Dobrea S. 1454Docenko D. 249Doerner R. 1399, 1415, 1421, 1422, 1425, 1426,1429, 1521, 1551, 1626, 1656, 1665Doerner R. P. 1394, 1406, 1409, 1416, 1427, 1501,1519, 1553, 1585, 1586, 1593, 1601, 1603, 1607,1620, 1657, 1672Dogan M. 844, 1142, 1144, 1169, 1176Dogana M. 1208Dolmatov V. K. 1190Domain C. 1494Domesle C. 1194Dong C. F. 356Dong C. Z. 109, 130, 197, 215, 220, 262, 282, 357,368, 442, 502, 623, 624, 631, 745, 850, 901, 1001,1025, 1046, 1051, 1148, 1225, 1226, 1227, 1235,1313Dong H. J. 349Donga C.Z. 1275Dopita M. A. 1334Dorn A. 831, 834, 835, 953, 964, 984, 1007, 1088,1153, 1362Dorner J. 1633, 1634, 1653, 1661Dos Santos J. M. F. 76DosSantos A. S. 717, 720, 725, 848, 1070, 1075,1254Douglas K. M. 750Douguet N. 598, 871, 1057Dousse J. -Cl. 546, 821Drag C. 1047Draganic I. N. 455Drenik A. 1617Du G. F. 745Du J. H. 1484Du M. H. 1484Du Rietz R. 358, 481Du S. 100, 1096Du S. Y. 336, 471Du W. J. 198

DuBois R. D. 976Duan B. 572Duan C. 1480Duan Chen. 1563Duan Y. M. 648, 660, 661, 809Dubau J. 113Dubois A. 1380, 1385Dubrov M. 1632Duffy D. M. 1418Dugne O. 1141, 1266Dujko S. 1029Dulieu O. 1204Duncan-Chamberlin K. V. 413Dunne P. 343Dunseath K. M. 987Durbeck T. 1512, 1547, 1559, 1652, 1675, 1678Dutra A. 1358Dutta N. N. 56, 186, 313, 458Dux R. 1405, 1624Dzhumaev P. 1618Dzuba V. A. 290, 314, 457Eberle S. 35, 211, 487Edtbauer A. 1366Efe M. 1668Efimov V. 1508Eguchi K. 1487Ehlerding A. 1280Ehresmann A. 345Eich T. 1405Ekman J. 5, 149, 244, 358, 406, 481El Hassan N. 108, 344El-Atwani O. 1668El-Sayed F. 46, 168, 276, 432El-Sherbini Th. M. 52, 172ElBitar Z. 1044ElGhazaly M. O. A. 1257ElIdrissi M. 739Elabidi H. 212, 327, 328, 463, 465, 482, 875, 968,1013, 1100Elander N. 1336Elantkowska M. 16, 230, 256, 419Ellis C. 913Emelyanova K. A. 1105Emigh A. 545Emmanouilidou A. 306Emmichoven P. v. 1606, 1641, 1666, 1680Endo T. 75Endstrasser N. 510Epp S. W. 35, 39, 211, 386, 487Er A. 230, 231, 249Erdelyi G. 1463Erhart P. 1433Ermakov V. 1640Errea L. F. 1369, 1370Ertl K. 1532, 1536, 1554, 1558, 1606Escandell M. M. 1443Esser H. G. 1447Esteves-Macaluso D. 331Et al. 618, 620, 621, 623, 625, 626, 627, 628, 630,

354

631, 633, 634, 636, 639, 640, 641, 642, 646, 647,648, 649, 650, 651, 652, 654, 656, 657, 658, 660,661, 662, 663, 670, 672, 673, 677, 680, 681, 682,683, 687, 690, 691, 1367, 1369, 1370, 1689F. M. H. 859Fabrikant 891Fabrikant I. I. 614, 615, 857, 882, 894, 1087, 1197Fahr H. J. 1333Fainstein P. D. 1380Falck A. S. 515Fan Q. 1096, 1138, 1237Fan Q. P. 77, 100, 229, 397Fan S. 468Fang K. H. 1677Fang Q. F. 1474, 1477, 1485, 1679Farias E. E. 259Faure A. 523, 657, 658, 962, 1109Faye I. G. 813Faye M. 68Federici G. 1423, 1429, 1469Fedor J. 594, 724, 830, 1054, 1192Fedotov V. 1618Fedus K. 1240Fei Z. 289, 441Feil S. 510Feldman U. 338Feldt A. N. 532Felfli Z. 58, 592, 704, 811, 888, 900, 1039Feng H. 500, 503, 532, 741, 932Feng W. T. 885Fennane K. 546Ferber R. 249Ferland G. J. 1202Fernandez J. M. 1390Fernandez J. M. R. 1443Fernandez-Menchero L. 1215Fernandez-Varea J. M. 820, 1267Ferraz J. R. 1254Ferreira J. A. 1445Ferreira N. 1133, 1251Ferreira S. E. S. 1333FerreiradaSilva F. 879Ferrero C. 1565Ferro Y. 1615Ferus M. 12, 123, 152, 210, 347, 474Fichtner H. 1333Field D. 798Field T. A. 1033Fifirig M. 742, 782, 808Filipovic D. M. 776Fiori M. 1377Fischer C. F. 459Flambaum V. V. 36, 60, 290, 314, 457Fletcher J. D. 1149Flores G. 913Florko T. A. 159Fogle M. 455, 553, 681, 851Fojon O. A. 519, 852, 955Foltin V. 582

Fontes C. J. 48, 226, 275, 279, 351, 394, 611, 1132,1139, 1218, 1302Foord M. E. 134, 138Foster A. 887Foster M. 527, 1040Fournier K. B. 134, 136, 137, 138Fqih M. E. 1434Francis-Staite J. R. 590, 703Frankel M. 387Franklin G. 913Franz J. 557, 771Franz K. 608Franzke B. 896Freitas T. C. 566, 610, 804, 862Fricke B. 209Friedman J. F. 614, 616, 881, 1033Fritzsche S. 70, 294, 836, 1148Froese Fischer C. 2, 5, 11, 57, 147, 149, 151, 200,244, 354, 358, 391, 392, 406, 478, 481Frolov A. M. 79, 238, 239Froula D. H. 134Fu B. Q. 1625Fu C. C. 1493Fu Y. B. 130, 901, 1046, 1051Fuhrmann H. 76Fujiki T. 1528Fujimori R. 133Fujimoto M. M. 515, 715, 942Fujishima T. 1646Fujiwara T. 1394Fukada S. 1456, 1459, 1527, 1528, 1621, 1665Fukumoto M. 1407, 1523, 1596, 1681Fulling S. 142Fundamenski W. 1447Furget C. 913Fursa D. 549Fursa D. V. 297, 517, 527, 528, 534, 561, 563, 586,650, 672, 684, 711, 769, 773, 777, 833, 834, 902,914, 988, 1005, 1008, 1053, 1055, 1072, 1083, 1095,1132, 1188, 1277, 1278, 1290, 1293, 1299, 1302,1356, 1359, 1360, 1386Furuta Y. 1628, 1630, 1653Fushitani M. 75Fuss M. 759, 950Fuss M. C. 1076Fusseder M. 1653Futagami N. 1633, 1634Gadkari S. C. 585Gaft M. 378Gaigalas G. 2, 5, 11, 23, 47, 57, 147, 149, 151, 170,200, 244, 266, 277, 278, 358, 406, 423, 479, 481,496Galiatsatos P. G. 797Gallardo M. 259Gallup G. A. 615, 882, 894, 1087Galonska A. 1425Gangopadhyay S. 946Gangopadhyay S. S. 540Gangwar R. K. 698

355

Gao C. 120, 252, 342, 416Gao C. Z. 1246Gao F. 1665Gao L. 1652, 1675Gao L. C. 109, 197Gao W. J. 31, 54, 173Gao X. 312, 412, 456, 663, 1339Garcia G. 591, 719, 759, 765, 826, 884, 907, 936,948, 950, 959, 1076, 1183, 1184, 1186, 1352, 1354Garcia M. C. 591Garcia-Rosales C. 1443, 1465Gardenghi D. J. 9Gargioni E. 1111Garibotti C. R. 1377, 1378Garrison L. M. 1577Gasaneo G. 1130, 1151Gaskell D. 913Gasparyan Y. 1508Gauf A. 854, 1185, 1289Ge Z. M. 928Gedeon S. 309, 454, 1079, 1308Gedeon V. 309, 454, 1079, 1308Geng W. T. 1492, 1498, 1576, 1582Geppert W. 1194Geppert W. D. 705, 1020, 1021, 1280Gericke M. T. W. 913Gervais B. 1312Ghanbari-Adivi E. 1093, 1365Gharaibeh M. F. 108, 337, 344, 1108, 1123, 1263Ghezzi F. 1403Ghoniem N. 1613Ghoshal A. 1363Gianturco F. A. 557, 605, 1076, 1205Giglio E. 1312Gillaspy J. D. 38, 83, 95, 127, 303, 334, 339, 353,361, 367, 472Giner E. 53Giniyatulin R. N. 1461Ginzel R. 386Giroud C. 320, 1405Giuliani A. 121Glazov D. A. 41, 98, 268, 364, 366Glenzer S. H. 137, 138Glover J. L. 338Glowacki L. 315Glowacki P. 15, 16Glukhov I. L. 163, 359, 484Glushkov A. V. 753Gning Y. 225, 380Gochitashvili M. R. 675Godefroid M. 57, 67, 200, 277, 278, 365, 479Godefroid M. R. 112, 244, 310, 358, 406, 481Gokce Y. 434, 435, 440Golub L. 235, 248, 253Gomez-Aleixandre C. 1445Gomis L. 813Gomonai A. I. 1122Gomonai A. N. 652, 1122Gong X. 1531

Gorczyca T. W. 58, 692, 1019, 1202Gordienko Y. N. 1649Gorfinkiel J. D. 524, 764, 1087Gori S. 1489Gornushkin I. 378Goswami B. 1099, 1110, 1120, 1256, 1319Goto Junya. 1581Goto M. 302, 321, 356, 362Gotta D. 76Gottwald T. 61, 106Gou B. C. 4, 30, 93, 102, 148, 162, 189, 194, 261,422Gou F. J. 1614Graf A. 35, 211, 487Grames J. 913Grant I. P. 288, 411Grattarola M. 1465Graupner K. 657Greene C. H. 588, 598, 871, 898, 906, 1056, 1057,1084Greenwood J. B. 1383Gregorio J. 1684Greuner H. 1625Grieser M. 216, 295, 712, 869, 895, 898, 904, 925,1023, 1024, 1050, 1152, 1194, 1279Grieve M. F. R. 969, 1127, 1214Griffin D. C. 202, 537, 548, 700, 887, 1038, 1052,1157, 1260Grisolia C. 1429Grosso G. 1403Groth M. 1624Gruber A. 76Grujic P. V. 972Grumer J. 182, 184, 289, 308, 333, 441, 450, 453Gschliesser D. 1366Gu M. F. 1, 146, 387Gualco C. 1465Guan X. C. 1677Guberman S. L. 1034, 1199, 1248Guerassimova N. 386Guerra M. 8, 14, 114, 201, 281, 360, 944, 1125,1242Gueye M. 68Guilbaud S. 108, 344Guilfoile C. J. 1290Guillard G. 913Guillemin R. 58Guimaraes M. N. 1389Guise N. D. 459Gumberidze A. 8, 114, 201, 281, 360, 896Guo X. L. 336, 471Gupta D. 1147, 1255, 1256, 1295Gupta G. P. 74, 180, 319, 384, 460, 490Gupta M. 523Gupta S. K. 585Gureev V. 1458Gureev V. M. 1432, 1438, 1449, 1674Gusev A. A. 1037Gustafsson S. 5, 149, 244, 358, 406, 481

356

Guthohrlein G. H. 16Guzelcimen F. 230, 231, 249Guzman A. 158Guzman F. 1370Haasz A. A. 1464, 1513, 1557Habibi M. 331Haddadou A. 770Hagelaar G. J. M. 1071Hagstrom S. A. 263Hahn M. 295, 621, 869, 895, 925, 1022, 1023, 1024,1050, 1152, 1279Hahn Y. K. 790Hakel P. 351Haley T. 1383Hamada K. 620Hamasha S. 44, 124, 166, 213Hamberg M. 705, 1020, 1021Hammond K. D. 1623, 1658Han B. P. 257, 420Han C. 257, 420Han X. 1058, 1340Han X. Y. 63, 312, 381, 412, 456, 663Hanna J. 1409, 1593, 1603Hanne G. F. 551Hansen J. P. 1380Hansen S. B. 121, 131, 134Hansknecht J. 913Hao L. 223, 224Hao L. H. 219, 325, 461Haque A. K. F. 505, 511, 512, 647, 714, 754, 1118Hara H. 5, 149, 357Hara M. 1509, 1633, 1634, 1676Hara S. 587Hargreaves L. 963Hargreaves L. R. 564, 586, 655, 826, 854, 860, 884,989, 994, 1140, 1185, 1186, 1224, 1261Hari P. 779Harilal S. S. 1452Haris K. 301, 447Harland P. W. 966, 1092Harman Z. 35, 211, 487, 896, 1311Harnisch M. 1670Harris A. 1097Harris A. L. 858, 1040, 1131Harris C. L. 136Harrison S. 954, 962, 1109Harte C. S. 302, 385Hartman H. 244, 358, 406, 481Haruyama Y. 485Harvey A. G. 579Hasan A. 1387, 1388Hasan M. 1118Hasegawa A. 1518Hasegawa S. 293Hasovic E. 589Hassanein A. 1439, 1470, 1619, 1636Hasuo M. 356Hatakeyama M. 1633, 1634Hatano Y. 1509, 1538, 1567, 1630, 1633, 1634,

1646, 1653, 1661, 1667, 1676Haughey S. A. 1033Hauptman N. 1428Havener C. C. 106, 455Hawkes N. C. 320Haxton D. J. 317, 588, 889, 905, 906, 1056Hayashi T. 1681He F. 229, 397He Z. W. 116, 117Heber O. 706Heeter R. F. 134Heim B. 1452, 1668Hein J. D. 654, 769Heinola K. 1548Hell N. 35, 211, 487Hellhund J. 791Henins A. 38, 281, 334, 353Hennebach M. 76Henriksson K. 1433, 1673Hensel K. 1059Herman Z. 1670Hernandez M. I. 1390Herrero V. J. 1445Hervieux P. A. 849, 1312Hibbert A. 58, 169, 330, 408, 467Hien P. X. 1160Higashiguchi T. 302, 343, 385Hikosaka Y. 40, 75Hilgers G. 1111Hillenbrand P. M. 1123, 1263Hino T. 1646Hinrichs R. 1004Hirahara Y. 133Hirai T. 1407, 1469Hirata S. 1021Hirooka Y. 1535, 1612Hirtl A. 76Hishikawa A. 75Hmouda B. 1130Ho Y. K. 1363Hoen M. t. 1641, 1660, 1666, 1680Hoeschen T. 1404Hoffmann J. 898Hoffmann T. H. 608Holberg J. B. 36Holczer T. 388Hole D. E. 1409Hollmann E. 1422Homem M. G. P. 720, 725, 848, 910, 1075, 1357Honda K. 1655Honda T. 1621Hong Rongjie. 1571Hongbin D. 1315Honigmann M. 1060Hopf C. 1431, 1442, 1531Horacek J. 543, 724, 857Horie M. 765, 1252Horn T. 913Hosaka K. 795

357

Hoschen C. 1489Hoschen T. 1489Hoshihira T. 1490Hoshino M. 514, 528, 591, 642, 690, 699, 726, 758,765, 826, 876, 879, 884, 936, 948, 959, 1074, 1106,1114, 1183, 1223, 1250, 1252, 1276, 1361Hossain I. 1118Hoszowska J. 546, 821Hotop H. 608, 1197Hou Y. J. 499Houamer S. 529, 812, 849Houfek K. 724, 857, 974Howard N. T. 342Hsiao J. T. 670, 738Hu F. 118, 206, 223, 224, 229, 257, 267, 397, 420,424Hu H. S. 1367Hu H. W. 282Hu J. S. 1627Hu Q. B. 574Hu X. L. 1028Hu Z. 1058, 1340Hu Z. M. 63, 85, 305, 572, 1201Hu Z. m. 916Hua Y. F. 1484Huang C. L. 1484Huang D. L. 1247Huang K. N. 738, 768, 1372Huang K. S. 349Huang L. F. 1475, 1574, 1599Huang M. 571, 580, 651, 696, 732, 922Huang Q. Y. 1477, 1604Huang X. L. 321Hubbard A. E. 342Huber A. 1405, 1541, 1660Huber K. 297, 791, 1278Huber S. E. 874Hudson C. E. 917, 923Hudson L. 338Hudson L. T. 38, 334, 353, 379Hughes J. W. 342Huldt S. 289, 308, 333, 441, 453Hulsen C. 1497Hussey M. 784Hutton R. 182, 184, 198, 289, 308, 333, 336, 441,450, 453, 471, 710Huttula M. 40Huttula S. M. 40Hutych Y. I. 1122Ibanescu B. C. 830Idziaszek Z. 607Iga I. 515, 559, 715, 720, 723, 725, 848, 910, 1070,1075, 1357Igarashi A. 805, 807Igitkhanov Y. 1430Ikeda T. 1482, 1597Ikegami Y. 1483Illana A. 662Illarionov A. A. 965

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358

Jha A. K. S. 55, 174Jha L. K. 507, 940, 941Jhumka S. 784Jia C. C. 1116Jia S. T. 349Jia X. 823Jia X. F. 613, 927Jia X. f. 1115Jian B. 17Jiang B. 1576Jiang C. 267, 424Jiang G. 77, 100, 118, 206, 219, 223, 224, 229, 257,267, 273, 274, 397, 420, 424, 429, 430, 1096, 1138,1237Jiang J. 183, 215, 262, 442, 502, 623, 624, 631,745, 850, 1001, 1025, 1226, 1227, 1275, 1313Jiang L. Y. 204, 415Jiang Z. K. 204Jiang Z. S. 352Jiao C. Q. 796Jiao L. 671, 978Jiao L. G. 604, 929, 1026Jin F. T. 120Jin R. 312, 412, 456Jin S. 1491, 1499, 1600, 1635, 1637Jin Shuo. 1479, 1563, 1580Jing L. 223Jo A. 854Johansson S. 22John P. 1450Johnson D. F. 1598Johnson P. V. 535, 538, 544, 545, 993Johnson W. R. 883Jonauskas V. 266, 423, 569, 1281Jones A. 1351Jones A. C. L. 1356Jones B. 121Jones D. B. 818, 826, 1073, 1186Jones M. K. 913Jones N. C. 798Jonsson P. 2, 5, 11, 47, 57, 147, 149, 151, 170, 182,184, 200, 244, 277, 278, 291, 358, 391, 406, 450,459, 479, 481, 496Jorand F. 504Jordon-Thaden B. 898Jose C. L. 1311Joshipura K. N. 540, 649, 743, 752, 788, 946, 947Joulakian B. 520Joulakian B. B. 567, 1037Jowko A. 945Jr B. 1263Ju X. 1475, 1556, 1574, 1579, 1599Juettemann F. 551Juha L. 347, 474Jung R. O. 565, 755Jung Y. D. 1170Jung Y.D. 1207Jungen C. 1035, 1682Jungen Ch. 599

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Mayer M. 1405, 1460, 1512, 1524, 1531, 1532,1606, 1641, 1666Mayes M. L. 951Mayo-Garcia R. 196Mazon K. T. 515, 715McCall B. J. 712, 1021, 1061McCammon D. 455McConkey J. W. 550, 760, 803, 817McConnell S. R. 1382McCormick K. 1405McCurdy C. M. 317McCurdy C. W. 889, 905, 1283, 1284McEachran R. P. 578, 973, 988, 1080, 1187, 1351,1356McEachran R.P. 1325McKeown R. D. 913McKoy V. 556, 590, 724, 727, 837, 854, 963, 1140,1185, 1203McLain J. L. 601McLaughlin B. M. 9, 108, 331, 337, 344, 794McLean A. G. 1436Mehine M. 1401, 1412Mei M. F. 257, 420Meigs A. 1624Meinander A. 1412Mekler K. I. 1654Mel’nikov A. S. 536Menas F. 770Mendes M. B. 706, 712, 898Mendoza C. 1335Meng D. 816Meng F. C. 571, 580Menmuir S. 320Merkelis G. 266, 423Merlet C. 1141, 1258, 1266, 1342Merola M. 1469Merrill B. J. 1676Mertens P. 787Mertens V. 1524Meyer D. 78Meyer W. 608Mezei J. Z. 1204Mezei Z. 1310Miao X. Y. 613, 927Michael D. 536Michelin S. E. 515, 715, 723, 848Micherdzinska A. 913Mielewska B. 702, 775, 933Migdalek J. 315, 473Mihovilovic M. 913Mikhailov A. I. 1298Mikus O. 602, 873, 1059, 1343Miller T. M. 614, 616, 881, 1031, 1033, 1089, 1090,1191, 1245Milosevic D. B. 589Milum B. 858Minamisono K. 64Minkowski R. 145Minoshima M. 368

Miraglia J. E. 960, 1270, 1371Miron C. 108Mischenko A. 1632Misra D. 33Mitchell J. B. A. 1257Mitescu C. D. 1383Mitnik D. M. 1151Mitroy J. 183Mitsumura T. 1183Mitterdorfer C. 1366Miyabe T. 1629Miyagi H. 1078Miyamoto M. 1601, 1603, 1646, 1665, 1672Miyamoto T. 1595Miyamoto Y. 1394Miyata K. 1407Miyo Y. 1681Mkrtchyan H. 913Moeslang A. 1565, 1644, 1651Mohallem J. R. 1358Mohan M. 42, 55, 69, 119, 164, 174, 176, 207, 283,286, 437, 439Mohara N. 1562Moitra A. 1500Mokler P. H. 125, 292, 371, 386, 896, 1311Moller S. 1660Mondal P. K. 186Montanari C. C. 960, 1270, 1371Montenegro E. C. 1133, 1251, 1371Montero S. 1390Morel V. 977Moreno-Diaz C. 154, 448Morgan K. 455Morgan W. L. 1071Morishita K. 1665Morishita T. 581, 1078Morita S. 302, 321, 356, 362Moritani K. 1483, 1610Morito S. 1603Moriyama H. 1483, 1610Morrison K. 1131Morrison M. A. 532Morrison N. 1084Morva I. 582, 602, 873, 1059, 1343Morvova M. 582, 602, 873, 1059, 1343Motapon O. 904, 1204Motsch M. 904Moy A. 1141, 1258, 1266Mozejko P. 677, 801, 937, 1243Mozetic M. 1428, 1617Msezane A. Z. 58, 73, 74, 179, 180, 319, 384, 460,490, 592, 704, 811, 888, 900, 1039Mu Q. 1230Mu Y. 1436Mu Z. D. 104, 195Mueller A. 517, 534, 791, 802, 869, 895, 896, 925,1022, 1023, 1024, 1050, 1108, 1123, 1152Mueller D. W. 1351Muether M. 913

364

Mukhamedzhanov A. M. 1008Mukherjee P. K. 33, 209Mukherjee T. K. 33, 209Muksunov A. M. 1432, 1449Muller A. 35, 211, 232, 295, 297, 331, 337, 398,487, 1278Munjal H. 547Munoz J. 1436Mura H. 1114, 1223Murai H. 1106, 1183, 1250Murakami I. 5, 149, 218, 220, 302, 356, 357, 362,368, 865, 1200Murashov S. V. 536Murphy M. T. 247Murphy T. J. 351Murray A. 1285Murray A. J. 531, 554, 784, 863, 1086, 1091, 1162,1193Murrie R. 826Murtadha A. 772Muse J. 708, 718, 1203Musielok J. 418Mutzke A. 1516Muzichenko A. D. 1461Mykyta M. I. 1217, 1320Na Y. H. 1129Naderer P. 1431Nagai Y. 642Nagasaka T. 1667Nagasono M. 75Nagata S. 1413Nagata T. 293, 332, 469, 806Nagendra K. N. 234Naghma R. 785, 1099, 1110, 1120, 1126, 1180,1253, 1255Nagli L. 378Nagy E. 309, 454, 1079, 1308Nagy L. 799, 934Nahar S. N. 208, 431, 1117Naja A. 529, 961, 1130Najjari B. 953, 1158, 1382Nakamura H. 1466, 1544, 1562Nakamura N. 5, 63, 85, 149, 220, 302, 356, 357,362, 368, 597, 916, 1058, 1201, 1340Nakamura Y. 1550Nakano T. 302, 357, 1523, 1681Nakazaki S. 805, 807Nakhe S. V. 329Nandi T. 332, 469Nandy D. K. 245, 407Napier S. A. 549Natarajan L. 59, 80, 175, 185Navarro C. 1185Nave G. 22, 135, 150, 250, 254, 410Naze C. 277, 278, 365Nefiodov A. V. 1298Neill P. A. 136Nemanic V. 1503, 1568, 1642Nemanic Vincenc. 1476

Nemouchi M. 67Nestmann B. M. 543Nettelbeck H. 1111Neu R. 1405, 1429, 1468, 1524, 1531, 1588, 1624Neu R. L. 1564Neumann T. 763Neumark D. M. 317Nevo I. 904Nguyen T. V. B. 288, 411Ni M. Y. 1604Nicholls D. C. 1334Nicolas C. 108Nieto-Perez M. 1396, 1452, 1502Nikitina E. A. 163, 359, 484Nikola L. V. 753Nikolic D. 692, 1019, 1202Nikulin V. K. 49Ning C. 1086Ning C. G. 564, 1088, 1097, 1193Ning L. N. 1101Ning R. H. 1556, 1579, 1599Nishijima D. 1394, 1399, 1406, 1415, 1416, 1422,1425, 1427, 1501, 1519, 1586, 1593, 1601, 1603,1620, 1626, 1665, 1672Nishikawa M. 1456, 1459, 1527, 1528, 1621Nishimura K. 1550Nishimura Y. 133Nishiura M. 1570Niu Y. R. 1462Nixon K. L. 863, 950, 1086, 1091, 1162, 1193Niyonzima S. 1161Noda N. 1413Nogami S. 1518Nolden F. 896Nordhorn C. 712Nordlund K. 1395, 1401, 1410, 1412, 1415, 1433,1507, 1592, 1626, 1671, 1673Norimatsu T. 1665Norrington P. H. 619, 917Novotn O. 1206, 1321Novotny O. 295, 706, 712, 869, 895, 898, 925,1023, 1024, 1050, 1061, 1152, 1194, 1279Novotny S. 898, 904Nozaki T. 1633Nunes Y. 876, 879Nygren R. 1665O’Connor D. J. 1627O’Dwyer B. 1064O’Mullane M. 887, 1052O’Sullivan G. 302, 343, 367, 385, 901, 1046, 1051Obara S. 293Oberkofler M. 1406, 1481, 1504, 1566, 1589, 1656Oda T. 1509, 1633, 1634, 1665Odagiri T. 726, 795, 1074, 1276, 1361Ogawa T. 1518Ogorodnikova O. 1429Ogorodnikova O. V. 1508, 1525, 1536, 1544, 1547,1554, 1558, 1559Ogorodnikova V. 1545

365

Ohashi H. 357Ohkawa M. 800Ohnishi Y. 1456, 1527, 1621Ohno N. 795, 1394, 1399, 1407, 1446, 1546, 1550,1595Ohrwall G. 58Ohsaki A. 807Ohsawa K. 1487Ohsawa Kazuhito. 1581Ohtani S. 597Ohtsuka Y. 1407, 1505, 1596, 1664Ohya K. 1414, 1420, 1424, 1466, 1530, 1549, 1562,1596Ohyama R. 1655Oishi T. 321, 356Oka T. N. 133Okamoto K. 1535, 1612Okumus N. 529Okunishi M. 581Okuno K. 1462, 1542, 1633, 1634, 1646, 1667, 1676Okur I. 844Olgac F. 1169Olgaca F. 1208Oliveira H. L. 515Oliver P. 169Olshanski E. 1437Olson R. E. 1375Omaly P. 977Ong A. 36, 60Ong W. E. 1348Ono K. 1603Oost G. V. 1486Oost G. v. 1605, 1680Orban I. 924Ordas N. 1443, 1465Orel A. E. 593, 595, 596, 889, 897, 908, 1049,1057, 1134, 1161, 1303Orlov D. A. 706, 898, 904Ortiz C. J. 1493Ortiz M. 196Osborne Jr D. S. 877, 878, 880Osin D. 83, 127, 361Osipov T. 905Otranto S. 1375, 1378Otsuka T. 343, 385, 1482, 1490, 1517, 1597, 1634,1659Ou X. 1631Ouart N. D. 121Oubaziz D. 819, 1113Oufni L. 737, 739Ouyang X. P. 1367Ovcharenko E. V. 652Ovsiannikov V. D. 163, 340, 359, 484Oya M. 1664Oya Y. 1462, 1509, 1542, 1633, 1634, 1646, 1665,1667, 1676Ozdemir L. 27, 160, 260, 421Ozer Z. N. 1144, 1169, 1176, 1209Ozera Z.N. 1208

Ozturk I. K. 230, 231, 249Pachucki K. 6, 34, 96, 316Page S. A. 913Pal S. 335, 470, 867, 1172Palaudoux J. 40Palay E. 1117, 1334Palihawadana P. 609, 1036Palmeri P. 415Pancheshnyi S. 1071Pandya C. V. 693Pandya S. H. 788, 947Panjan P. 1428Papavassiliou V. 913Pardanaud C. 1442Parente F. 14, 103, 126, 214, 365, 486, 944, 1125,1242Parkes M. A. 1149Pascal 221Pasquiers S. 504Pasquini B. 913Passoni M. 1568Pastega D. F. 1326Pate S. F. 913Patel P. M. 693Patidar V. 516, 600, 892, 983, 1143, 1291Patoary M. A. R. 511, 512, 714, 754Pawelko R. J. 1514Payne A. T. 38, 334, 353Peacher J. L. 1040Pedersen H. B. 904Pei S. H. 204Pejcev V. 776, 973Pelaez R. J. 409Penent F. 40Peng H. Y. 1505Penzhorn R. D. 1645Pereira N. 338Perelygina Tat’Yana B. 753Perez D. 1669Perez-Rios J. 1390Persson J. R. 51Pestchanyi S. 1469Peterson K. A. 373Petersson P. 1450, 1451Petrie T. W. 1405Petrignani A. 712, 898, 1061Petrov I. D. 345, 1689Petrov V. 1458Petrov V. B. 1432, 1438, 1449, 1457, 1590, 1674Petrovic Z. L. 1029Petrovic Z. Lj. 716Pflueger T. 831, 834, 835, 953, 984, 1007, 1088,1153, 1362Phan T. L. 967Phaneuf R. A. 331, 337, 1268, 1269Phelps A. V. 1071Philipps V. 1407, 1411, 1423, 1425, 1429, 1440,1447, 1541, 1549, 1584, 1622, 1645, 1660, 1664Phillips S. K. 913

366

Pia M. G. 748Pickering J. C. 18, 19, 150, 155, 410Piech G. A. 755Pieritz R. 1565Pigarov A. Y. 1426Pillot P. 913Pilskog I. 1385Pindzola M. S. 202, 527, 531, 533, 537, 542, 548,554, 639, 641, 646, 700, 728, 783, 794, 834, 838,843, 861, 899, 956, 964, 980, 982, 1007, 1108, 1157,1163, 1196, 1260, 1306, 1373, 1374, 1392Pintsuk G. 1465Piracha N. K. 413Piraux B. 832Pitchford L. C. 1071, 1274, 1684, 1688Pitt M. L. 913Pitts R. A. 1447Plunien G. 41, 70, 98, 268, 287, 364, 366, 1298Podkovyrov V. 1469, 1632Podkovyrov V. L. 1461Podpaly Y. A. 339, 361, 472Poelker M. 913Poirier M. 1304Polidan R. S. 144Politis M. F. 955Polosatkin S. V. 1654Polsky V. 1618Polyansky A. 1618Pomeroy J. M. 38Pons B. 1379Pop N. 1204Popa G. 1454Poparic G. B. 829, 931, 1121Poparie G. B. 674Popov Y. V. 1112Popov Yu. V. 832Popovi M. 1221Popovic M. 1121Porosnicu C. 1455, 1503, 1506, 1521, 1537, 1642,1678Porro S. 1450Porsev S. G. 188Porter F. S. 211, 370, 387Porto J. V. 95Pospieszczyk A. 787, 1408, 1416, 1622Possnert G. 1451Postler J. 1366Postupaev V. V. 1654Potzel S. 1624Powell C. J. 497, 513, 1249, 1685Prabhudesai V. S. 911Pradhan A. K. 1117Prajapati A. 884Prancikevicius A. 1281Pranevicius L. 1402, 1402Pratt S. T. 599, 1035, 1682Pravica L. 549, 825Predojevic B. 776Preval S. P. 36

Price S. D. 750, 756, 757, 1149Prigorovsky A. V. 915Prins P. R. 1460Probst M. 510, 876, 1179Prudente F. V. 1389Pruemper G. 581Ptasinska-Denga E. 677, 801, 937Puchalski M. 6, 23, 34, 96, 316Puetterich T. 1405Purohit G. 516, 600, 892, 983, 1143, 1291Purohit S. P. 576Putterich T. 1624Qi Q. 1627Qi Y. Y. 1101Qiao H. X. 88, 350, 1231Qindeel R. 464Qiu M. L. 336, 471Qu Y. Z. 381, 1028, 1101Quinet 221Quinet P. 228, 396, 415Quinn B. 913Quint W. 41, 98, 377Raassen A. J. J. 140, 141Rabus H. 1111Radmilovic-Radjenovic M. 716Raeder S. 61Rahman M. A. 946Rahman S. S. 545Rai A. 1516, 1594Raineri M. 101, 259Rajeev 749Raju G. G. 612Rajvanshi J. S. 678, 685, 855, 1003Rakcheeva L. P. 536Rakitzis T. P. 457Ralchenko Yu. 83, 127, 338, 339, 361, 367, 472,575Ralphs K. 708, 963, 1140Ram N. B. 1032Ramos G. 1396, 1502, 1531Ramsay W. D. 913Ramsbottom C. A. 330, 467, 618, 619, 733, 736,917, 923, 969, 1127, 1214Randazzo J. M. 1151Ranjit G. 376Rao K. C. 585Rapp J. 1405, 1440, 1444, 1460, 1532, 1543, 1606,1608, 1609, 1624Rappaport M. L. 706Ratnavelu K. 233, 352, 560, 759, 767, 1348, 1350Rausch J. 791Rawat P. 720, 725Read F. H. 773, 1188Reader J. 83, 127, 339, 361, 367, 472Real J. S. 913Redman S. L. 254Regan S. P. 351Reid D. D. 1332Reinelt M. 1397, 1481, 1504, 1566, 1656

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Reinhart M. 1660Reinhold C. O. 1417Reinke M. L. 342, 1405Reiter D. 541, 874, 979Remeta Y. 1042Ren L. M. 740Ren X. 831, 834, 835, 953, 984, 1007, 1088, 1153,1288, 1362Renwick A. C. 534Repnow R. 216, 295, 712, 869, 895, 898, 925, 1023,1024, 1050, 1152, 1194, 1279Rescigno T. N. 889, 905, 1134, 1283, 1284, 1303Reyna Almandos J. 259Rezkallah Z. 812, 849Rhodes Jr. E. J. 144Riahi R. 626, 627Rice J. E. 342Ristic M. M. 829, 931, 1121Rivarola R. D. 519, 679, 852Rivera A. 1643Robert E. 108Robicheaux F. 537, 646, 783, 899, 980, 1373Rocco M. 1182Rocha A. B. 1182Roche J. 913Rodrigues F. N. 1182Rodriguez-Garcia J. 196Rognlien T. D. 1426Rohde V. 1447, 1524, 1531Rokusek D. L. 1452Rolli R. 1565, 1651Roman V. 1173Romanovsky E. A. 1438, 1457Romero D. 718Rooij G. v. 1440, 1624Roos J. B. 593Roos P. 913Roquemore A. L. 363Rosa A. 135Rosa M. R. 135Rosado J. 662Rosen S. 705Rosenfeld A. B. 1111Rosmej F. B. 99, 193Roszell J. P. 1464Roth J. 1423, 1429, 1455, 1506, 1511, 1519, 1521,1522, 1526, 1537, 1538, 1544, 1545, 1558, 1567,1593, 1633, 1634, 1647, 1656, 1661, 1678Rothe S. 61Rouabah Z. 583Roubin P. 1442Roueff E. 570Rovenskikh A. F. 1654Roy A. C. 770, 810, 812, 849, 971Roy A. K. 390Roy B. N. 507Roy S. 313, 458Rubel M. 1409, 1411, 1451Ruczkowski J. 16, 230, 256, 419

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Santana J. A. 227, 395, 643Santos J. P. 8, 14, 33, 114, 201, 281, 360, 486, 944,1125Santos J.P. 1242Sanz A. G. 1076Sapirstein J. 457Saracco P. 748Sarkar A. 1355Sarker M. S. I. 512Sasaki A. 356, 1200Sasaki D. K. 654Sasaki T. 1483, 1610, 1628, 1630Sasao M. 1570Sasic O. 1029Sato H. 587Sato K. 1488, 1650Sato M. 1535, 1612Sauter G. 608Sauter P. A. 1443Sauvage T. 1473, 1529, 1539, 1638Savage J. S. 902Savin D. W. 295, 570, 868, 869, 893, 895, 925, 998,1022, 1023, 1024, 1050, 1152, 1194, 1279, 1324Scemama A. 53Schaffer L. C. 614, 616Schatz G. C. 951Schaub J. 913Scheer J. A. 1437Scheid W. 896Scheier P. 510, 1366, 1670Schenker J. L. 821Schepetnov A. A. 366Scherer K. 1333Scherrer S. T. 815Schimeczek C. 7, 78Schine N. A. 376Schippers S. 182, 211, 232, 295, 297, 331, 337, 398,480, 517, 534, 791, 802, 869, 895, 896, 925, 1022,1023, 1024, 1050, 1108, 1123, 1152, 1278Schlachter A. S. 337Schlage K. 35, 487Schlesser S. 8, 76, 281, 360Schlotter W. 211Schmerl B. A. 703Schmid K. 1397, 1405, 1423, 1429, 1511, 1513,1519, 1526, 1554, 1558, 1560, 1591, 1593, 1660,1662Schmidt E. W. 896Schmitt B. L. 386Schmitt M. J. 351Schmitz O. 1436, 1584, 1622Schmoranzer H. 345Schneider A. E. 376Schneider H. C. 1651Schneider I. F. 904, 1161, 1204, 1310Schneider M. B. 134Schneider R. 1516, 1594Scholten J. 1460Schuch R. 924

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Yang J. M. 63, 118, 206, 257, 305, 420, 572Yang N. X. 502, 623, 624, 1225Yang X. 1619, 1636Yang Y. 184, 291, 450, 710Yang Z. S. 1420Yang Zhongshi. 1571Yangb W. 1233Yao K. 198, 289, 336, 441, 471, 710Yapici B. 249Yarevsky E. 1336Yates B. R. 525, 828Yavac H. 35, 487Yavuz M. 1144, 1176, 1209, 1220Yerokhin V. A. 294, 707Yi T. 305Yildiz M. 28, 434, 435, 440Yin J. R. 204Ying A. 1639Yoon J. S. 656, 691, 699, 1239Yoshida F. 293Yoshida M. 1448, 1681Yoshida N. 1413, 1542, 1633, 1634, 1646, 1650,1655, 1667Yoshiie T. 1488, 1650You Y. W. 1485, 1679You Yu-Wei. 1474, 1477Young B. K. F. 134Young J. A. 58, 535, 538Yu D. 896Yu J. 1399, 1422Yu J. H. 1427Yu R. M. 604Yu Remeta E. 697, 701Yu S. W. 58Yu W. W. 346Yu X. 1315Yu X. G. 1614Yu Y. 1616Yuan J. 324Yuan J. M. 81, 92, 107, 120, 252, 311, 416, 1309,1341Yuan Y. 1625Yuan Z. S. 740Yugami N. 343Zabaydullin O. 113Zabudla Z. 602, 873, 1059, 1343Zajec B. 1503, 1568, 1642Zajec Bojan. 1476Zajfman D. 706Zakharov A. 1632Zammit M. C. 684, 1072, 1095, 1293, 1299, 1360Zang S. S. 928Zang Y. 267, 424Zanozina E. M. 12, 123, 152, 210, 347, 474Zaplotnik R. 1617Zappa F. 510Zatekin V. 1458Zatekin V. V. 1438, 1457, 1674Zatsarinny O. 111, 199, 236, 307, 309, 399, 452,

454, 518, 549, 551, 552, 617, 622, 644, 673, 734,773, 778, 789, 792, 822, 825, 826, 864, 984, 985,989, 995, 996, 1002, 1079, 1107, 1144, 1145, 1153,1165, 1166, 1173, 1174, 1186, 1262, 1296, 1305,1307, 1308, 1322, 1364Zaurbekova Z. A. 1649Zavilopulo A. N. 1217, 1320Zayachuk Y. 1486, 1605, 1680Zaytsev S. A. 832Zecca A. 719, 1184, 1352, 1354, 1355Zeisler S. K. 1437Zeng D. L. 312, 412, 456Zeng J. 92, 324Zeng J. L. 107, 120, 252, 311, 416, 922, 1309, 1341Zeng Y. Y. 500, 503, 741, 932Zeng Z. 1475, 1556, 1574, 1579, 1599Zenobia S. J. 1569, 1577, 1611Zerrad E. 790Zetner P. W. 769Zhang B. 1627Zhang B. H. 63, 572Zhang C. 274, 430Zhang D. H. 109, 197, 1025Zhang F. S. 1246Zhang H. 694Zhang H. L. 48, 226, 275, 279, 394, 611, 1132,1139, 1218, 1302Zhang H. M. 321Zhang J. 816Zhang J. F. 613Zhang J. J. 1225Zhang J. S. 117Zhang J. Y. 63, 305, 572Zhang L. 31, 219Zhang L. J. 349Zhang L. M. 1116Zhang M. 908Zhang N. 346Zhang P. 885, 1088, 1650Zhang Pengbo. 1478, 1573Zhang R. 771, 797Zhang S. 1677Zhang S. B. 668, 686, 688, 824, 1028Zhang S. F. 885Zhang W. 415, 710Zhang W. Y. 1627Zhang X. 1238, 1484Zhang X. M. 269Zhang Y. 696, 1028, 1491, 1499, 1600, 1631, 1635,1637Zhang Y. Z. 1135, 1228, 1233Zhang Ying. 1479, 1480, 1563, 1572, 1578, 1580Zhang Z. 992Zhao G. 241, 403, 730, 919, 921, 1069, 1128, 1241Zhao J. 1575Zhao J. M. 349, 450Zhao J. T. 1677Zhao Jijun. 1478, 1573Zhao Q. 1230

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Zhao R. 289, 333, 441Zhao R. F. 308, 336, 453, 471Zhao Y. 305Zhao Z. 269, 1238Zhao Z. Z. 336, 471Zhaunerchyk V. 553, 705, 851, 1020, 1021Zhen J. F. 105, 116, 117Zheng M. Y. 1063Zheng X. B. 1462Zheng Z. J. 572Zhitlukhin A. 1469, 1632Zhitlukhin A. M. 1461Zhong J. Y. 241, 403, 730Zhou B. 573, 1063Zhou C. 31, 54, 173, 265, 285, 323, 433Zhou H. B. 1491, 1499, 1600, 1631, 1635Zhou Hong-Bo. 1479, 1480, 1563, 1572, 1578, 1580Zhou L. 571, 580Zhou L. X. 1027, 1232Zhou W. H. 1475, 1556, 1574, 1579, 1599Zhou Y. 560, 640, 671, 793, 978, 1350Zhou Y. J. 501, 604, 695, 929, 1026, 1135, 1137,1167, 1228, 1233Zhou Y. S. 1677Zhu J. 555Zhu L. F. 637, 740, 1187Zhu T. 572Zhu X. L. 885Zhu Z. L. 606Ziesel J. P. 798Ziolkowski M. 951Zissis G. 536Zitnik M. 821Zlobinski M. 1541, 1645, 1660Zmeskal J. 76Zmitko M. 1651Zoethout E. 1435, 1510Zou Y. 289, 333, 336, 441, 471, 710Zou Y. M. 182, 184, 198, 308, 453, 506, 580, 696,732, 922Zubek M. 522, 702, 763, 775, 933, 999Zubova N. A. 287Zumer M. 1503, 1642Zush H. 1612Zushi H. 1535, 1655

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