bibliographic survey of medium energy inclusive reaction data · 208pb,h8sn 27 al,cu experimental...

LA-10699-MS

LA— 10699-MS U C . 3 4 C

DE86 012837 Issued: April 1986

Bibliographic Survey ofMedium Energy Inclusive Reaction Data

E. D. ArthurD. G. MadlandD. M. McClellan

DISCLAIMER

This report was prepared as an account of work sponsored by an agency of the United StatesGovernment. Neither the United States Government nor any agency thereof, nor any of theiremployees, makes any warranty, express or implied, or assumes any legal liability or responsi-bility for the accuracy, completeness, or usefulness of any information, apparatus, product, orprocess disclosed, or represents that its use would not infringe privately owned rights. Refer-ence herein to any specific commercial product, process, or service by trade name, trademark,manufacturer, or otherwise does not necessarily consti"ite or imply its endorsement, recom-mendation, or favoring by the United States Government or any agency thereof. The viewsand opinions of authors expressed herein do not necessarily state or reflect those of theUnited States Government or any agency thereof.

Los Alamos National LaboratoryLos Alamos.New Mexico 87545

BISTRIBUTION OF THIS DOCUMENT IS UNU

TABLE OF CONTENTS

OVERVIEW AND APPROACH 1

TABLE I - PROTON-INDUCED REACTIONS - 5

TABLE II - DEUTERON-INDUCED REACTIONS 95

TABLE III - TRITON- AND 3He-INDUCED REACTIONS 113

TABLE IV - ALPHA-PARTICLE INDUCED REACTIONS 121

TABLE V - 6>7Li INDUCED REACTIONS 145

TABLE VI - EXPERIMENTAL DATA REFERENCE TABLE FOR PROTON ELASTICSCATTERING AT MEDIUM ENERGIES 151

TABLE VII - EXPERIMENTAL DATA REFERENCE TABLE FOR PROTON TOTALREACTION CROSS SECTIONS AT MEDIUM ENERGIES 155

iv

BIBLIOGRAPHIC SURVEY OF MEDIUM ENERGY INCLUSIVE REACTION DATA

by

E. D. Arthur, D. G. Madland, and D. M, McClellan

ABSTRACT

A bibliographic survey of inclusive reaction data (ex-perimentcl and theoretical) for several projectile typeshaving energies between 50 and 1000 MeV h«s been completed.Approximately one thousand references selected from thissurvey describe the current state of knowledge for particle-induced inclusive reaction data.

I. OVERVIEW AND APPROACH

This report provides results of a recently completed search of bibliograph-

ic information pertaining to currently available inclusive reaction data. Par-

ticularly emphasized were medium energy data describing experimental and theore-

tical results for particle and gamma-ray emission. Other types of information

that were included pertain to the use of appropriate medium-energy theoretical

models and to experimental results for materials damage, nuclear recoils, and

radiation effects produced by medium-energy projectiles.3 4

The search covered data for the following projectiles: p, d, t, He, He,

and lithium ions, over an incident energy range extending from approximately 50

MeV to 1000 MeV. The search utilized the US Department of Energy RECON" (Remote

Console) bibliographic data system and spanned the time period from 1947-1985.

Initially, more than 17 000 possible entries were identified using key word

techniques. Subsequently, approximately 1000 references were selected by scan-

ning abstracts, and in some cases, text. TLese have been judged appropriate for

describing the current state of knowledge concerning inclusive reaction data,

both from an experimental and theoretical viewpoint. We have also included

bibliographic information needed for assessment, validation, and refinement of

nuclear model capabilities.

1

For the selected bibliographic entries, the following is provided: refer-

ence, author(s), title, target materials, and descriptor(s) characterizing the

content of the bibliographic entry. Tables I-V list such information for in-

o 6 7

cident protons, deuterons, tritons, He, alpha-particles, and ' Li ions.

The bibliographic entries in Tables I-V follow a rough sequence where more

recent data precedes older publications. Additionally, an attempt was made to

place entries for higher energy data (100 i E g 1000 MeV) before those appro-

priate for lower energies. This ordering was followed for publications appear-

ing between 1975-1985; but for entries occurring before 1975, such a grouping

became more difficult. Particularly for data occurring between 1947-1960, no

energy ranges could be specified, so that a mixture of higher and lower energy

data results.

Finally, Tables VI and VII summarize selected references for proton elastic

scattering and total reaction cross-section data. Such infoj.-nation is provided

because of the important constraints it imposes upon the several theoretical mod-

els that are currently used to calculate proton-induced inclusive reaction data.

II. OTHER SOURCES OF CHARGED-PARTICLE REACTION DATA

The following is a partial list of other sources of bibliographic data for

charged-particle reaction data.

1. N. E. Holden, S. Ramavataram, C. L. Dunford, "Integral Charged-ParticleNuclear Data Bibliography," Brookhaven National Laboratory report BNL-NCS-51771, First Edition (1984) and Supplement One (1985).

2. N. E. Holden and T. W. Burrows, "The Bibliography of Integral ChargedParticle Nuclear Data," Brookhaven National Laboratory report BNL-NCS-50640(1982), Fourth Edition, Supplement 2.

3. T. W. Burrows and G. Wyant, "The Bibliography of Integral Charged ParticleNuclear Data," Brookhaven National Laboratory report BNL-NCS-60640 (1931),Fourth Edition, Supplement 1.

4. T. W. Burrows and P. Dempsey, "The Bibliography of Integral Charged Par-ticle Nuclear Data," Brookhaven National Laboratory BNL-NCS-50640 (1980),Fourth Edition (Archival Edition).

5. F. K. McGown and W. T. Milner, Reaction List for Charged-Particle-InducedReactions. Atomic Data Nuclear Data Reprints 2 (Academic Press, New York,1974).

6. K. A. Keller, et al., Q-Values and Excitation Functions of Nuclear Reac-tions . Landholt-Boernstein, Group I, Vol. 5 Parts A-C (Springer-Verlag,Berlin, 1973).

TABLE I

PROTON INDUCED REACTIONS

TARGET TITLE REFERENCE DESCRIPTORS

Relativistic vs Nonrelati-vistic Description of ProtonElastic Scattering in theEnergy Range 200-500 MeV

9Be, 12c Contribution of Quasi-ElectricMechanism to Inclusive Spectraof Light Fragments Emitted tothe Back Hemisphere

C,Pb, Ag Production Mechanism of Back-ward Energetic Protons Studiedfrom Two-Particle Correlationsin 800 MeV Proton-NucleusCollisions

27A1,197AU Energetic Protons at Large6Li,58Ni Angles in Coincidence with28si Gamma Rays

51V 51v(p,n)51Cr Reaction at Ep=160 MeV

27 AI, 12c Energy Dependence of Nuclear63Qj,4He Reaction Cross Sections208pb,H8sn

27 Al,Cu Experimental Study of DirectKnockout of Proton Pairs fromNuclei by 640-MeV Protons

56Fe,51V Systematics of Spallation75 As,59Co Yields with a Four-Parameter63Cu Formula

207,208pb Microscopic Analyses of Pro-ton Scattering from Lead

Phys Lett B152.319(1985)R.Dymarz

Bull Acad SciencesUSSR, Phys Series47,2130 ( 1983)L.I.Galanina,N.S.Zelenskaya

Phys Rev C3L2168(1985)Y.Miake et al

Workshop onCoincident ParticleEmission from Conti-nuum States, Bad Honnef,W.Germany, INIS-MF-9280(1984) M.Avanetal

NuclPhysA427,332,(1984)J.Rapaport et al

Phys Lett B146,370(1984)N.H.Wong,J.Huefner

Sov J Nucl Phys40,17(1984)V.S.Nadezhdin cu al

RadActa 35,121(1984) M.Foshinaetal

Nucl Phys A426.496(1984)L.Rikus,H.V.Von Geramb

optical model,Dirac equation

knock-outreactions

quasi elasticscattering

inclusiveinteractions

neutron spectra

total crosssections

proton spectra

spallation

optical models

2 7 A 1 , 5 9 C O

55Mn,58Ni48 T i ,5Iv

7Li

208Bi

238u

27 Al,197 Au,6Li,58Ni

58Ni,16028Si,90Zr

40,48ca

12Q64CUPb

27A1.6U197Au,58Ni28S i

182W

Table I

Proton Induced Reactions onTi.V.MnJe.CoandNi.Measurement and Hybrid ModelAnalysis of Integral ExcitationFunctions and Their Appli-cation in Model CalculationFor the Production ofCosmogenic Nuclides

Activation Measurements ofthe 7U(p,n)7Be Reactionsfrom 60-480 MeV

Inclusive Measurement ofQuasi-free (p,xn) ChargeExchange Reactions on Bismuthfrom 62 to 800 MeV

Comparison of High-EnergyFission Models

200 MeV Proton Scattering onNuclei, Energetic ProtonAnalysis at Large Angle

Neutron Deep-Hole States fromthe (p,pn) Reaction

Neutron-Knockout Reactionsfrom 2H,40Ca and 48Ca

Role of the Delta-Resonancein Intranuclear Cascades

Energetic Proton Analysis atLarge Angle by 200 MeV ProtonScattering on Nuclei: Inclu-sive Spectra; Proton-GammaCoincidence Spectra

Inelastic Scattering of Inter-mediate Energy Protons fromTungsten

(Cont.)

KoelnUniv.W.Germany reportINIS-MF-9214p. 165(1983)R.Stueck

Phys Rev £30,1999(1984)J.D'Auriaetal

Phys Rev £30,236(1984)LMD'Auriaetal

NuclInstMeth222,540(1984)T.W.Armstrong

Thesis, Clermont-Ferrand UnivFrance(1983)G.Chaigne

J de Physique 45,91(1984) J.W.Watson

NuclPhysA424,92(1984) M.Ahmadetal

Dubna report JINR-R-2-83-768 p. 10(1983) N.S.Amelin

Thesis, Clermont-Ferrand Univ.France(1984)M.A1-Zoubidi

Tenth NuclearPhysics Conf, Can-berra, AustINIS-MF-9064,p.34(1984) BJLay

knock-outreactions

proton reactions

quasi-freereactions,nuclear cascades

cascade theory,fission neutrons

knock-outreactions.quasi-elastic scattering

knock-outreactions

knock-outreactions,neutron spectra

nuclear cascades

gamma radiation,nuclear cascades

inelasticscattering

Table I (Cont.)

Al.Ca.FeMg

40ca,56Fe

28Si,6Li

27 Al,

58Ni,9QZr

Bi,Pb

27 Al,197 A u

27 Al

9Be

Mo

Measurement of Cross Sectionsfoe 22Na,20Ne,22Ne and 36AT-42 AT in the Spallation of Mg,Si,Ca and Fe. ProductionRatios of Some CosmogenicNuclides in Meteorites

Nucleon Optical Potential

Backward Emission of EnergeticProtons

New Developments in the Studyof Continuum Spectra

Statistical Simulation ofHadron-Nucleus and LightNucleus-Nucleus InteractionIntranuclear Cascade Model

Evaluation of Computational!Models for Fission and Spal-lation Reactions used inAccelerator Breeding andTransmutation Analysis Code

Quasi-Free Scattering andExciton Model Analysis at 200MeV

Backward Emission ofEnergetic Protons

Survey of Neutron Energy Spec-tra and Angular Distributionsof the 9Be(p,n)9B Reaction forFast Neutron Radiotherapy

Medium-Energy SpallationCross Sections. 2. Mo Irradia-tion with 800-MeV Protons

J de Physique 45,855(1984)F.Baros,SJlegnier

Nuovo Cimento81,250(1984) P.E.Hodgson

J de Physique 45,25(1984) M.Avanetal

J de Fhysique 45j3(1984)HMachner

GosudarstvennyjInst. Moscow,ITEF-91(1983)S.Y.YaderetalNTIS #PC A03/MF A01

J .Nucl Sci & Tech20,511(1983)Y.Nakahara

Phvs Lett B 138.39(1984)H.Machneretal

PhysRevC30,521(1984)M.Avan

IAEA report INDC(NDS)--153/Lp.31(1984)M.Allab

IntJ Appi.Rad&Iso.34,l63l(1983)P.M.Grant et al

spallanon

optical models

proton inter-actions.nuclearcascades

proton reactions,precompound-nucleus,exclusive.inclu-sive interactions

hadron reactions,nuclear cascades

spallation,evaporation,nuclear cascades

quasi-freereactions,inclusiveinteractions


neutron spectra,charge-exchangereactions

spallation,fragments

107Ag

Pb,U

27A1.C.I,Fe,Pb,NbTa,U

12C

209B i238U

T a b l e I

Fragmentation Reactions onNuclei: Condensation ofVapour or Shattering of Glass

Model Predictions of Neutronand Isotope Production fromProton Induced Fission atHigh Energies

Inclusive Quasi-ElasticKnockout of CompositeParticles at Large MomentumTransfers

Model Predictions ofDifferential Neutron Produc-tion Cross Sections for Leadand Uranium Bombarded by590-MeV Protons

Differential Neutron Produc-tion for 590 MeV Protons

Analysis of Results on ElasticScattering of Intermediate-Energy Protons by Light andIntermediate Nuclei

Case Study and Progress Reporton Microscopic Analyse?, ofNucleon-Nucleus Scattering upto 400 MeV

Rapidity Dependence ofEntropy Production inProton- and Nucleus-InducedReactions on Heavy Nuclei

Medium Energy Proton InducedFission in Uranium-238 andBismuth-209

( C o n t . )

Phys Lett 136,15(1984) J.Aichelin

ProcIntConfonNuclear Data forSci & Tech, Antwerpp.391(Sept6-10,1982)T.Armstrong et al

Sov J Nucl Phys38,805(1983)S.G.Kadmenskii,Y.L.Ratis

Nucl Data Sci &Tech Int ConfAntwerp(Sept6-10,1982) p.387T.W.Armstrong,DJilges

Nucl Data Sci &Tech Int ConfAntwerp(Sept6-10,1982) p.383S.Cierjacks et al

Sov J Nucl Phys38,706(1983)N.I.Zaika,V.A.Shityuk

Verhandlunger derDeutPhysGesel-lschaft(E.Ger.)19,1047(1984)H.V.Geramb,LJlikus

Phvs Rev C29.1744(1984)B.V.Jacaketal

UofDl,Thesis (1983)M.Ali

proton reactions,inclusiveinteractions

fission,spallation,evaporation modelnuclear cascades


proton knockoutreactions,spallation

spallation

elasticscattering

nucleon reactioninelasticscattering

heavy ion reac-tion.heavy nuclei,proton reactions,spallation,statistical models

spallation

Table I (Cent . )

kg

'LU2C

197 A u

137Cs90Sr

12C

9Be

27 Al40Ca208pb90zr

40Ca

Table I

Comparison of Methods forDetermining Neutron DetectorEfficiencies at MediumEnergies

Estimation of Secondary Neu-tron Yield from Heavy IonBeams

Light Particle Correlationsin the Framework of theExciton Coalescence Model

High Energy ProtonInteractions with Sr and Cs:Contribution to the WasteTransmutation Study

Inclusive (p.p1) Reactionsat Medium Energies

Large-Angle Proton Emissionin the 9Be(pv2p) Reactionat300MeV

Imaginary Part of theNucleon-NucleusOptical Potential

Global Features of theProton-Nucleus Inter-actions

Energy Dependence of theRelativistic Impulse Approxi-mation for Proton-NucleusElastic Scattering

Simulation Study of ProtonInelastic Interaction withNuclei in the 50 to 350 MeVRange by Monte Carlo Method

( C o n t . )

Nucl Instr & Meth215.413(1983^J.W.Watson etal

Meeting on Heavy-Ion & Light IonIrradiations,Tokoyo, INS-NUMA-29,p.56(1981)H.Nakamura

Phys Rev £29,109(1984)H.Machner

Nucl Inst & Meth212,359(1983)P.Feliceetal

Phvs Lett B129.379(1983)Y.Tzeng.T.Tamura

Nucl Phvs A405.463(1983)R.EJL.Green et al

ZeitfurPhysikA3J199(1983)S.Bhattacharya,S.Kailas

Proclnt SympNuc Phys.CalcuttaSept 14-16,1977p.222,PP.Singh

Phys Rev £28,1421(1983)B.C.Clarketal

FRNC-TH--1128,p.107(1982) ToulouseUniv ThesisJ.CPeres

neutron detectors,proton reactions

proton reactionssecondary emissionneutron spectra,nuclear cascades

proton reactions,precompound-nucleus emission

computerizedsimulation.knock-out and protonreactions

proton reactions,inelasticscattering,inclusiveinteractions

inclusiveinteractions,proton spectra

optical models,proton reactions

proton reactions,energy and gammaspectra

impulseapproximation

proton reactions,inelasticscattering,nuclear cascades

10

T a b l e I (Con t . )

232Th235u238U

208pb

Ce,Eu165Ho159Tb

Comparison of the (p.xn)CrossSections from 238u,235u,and232jh Targets Irradiated with200 MeV Protons

Measurement of the AverageNeutron Yield from 250 MeVProtons Absorbed in a LeadTarget

190 MeV Proton-Induced Symme-tric and Asymmetric Fission

IEEE Trans.NucSci 30,1153(1983)Y.Y.Chu,M.L.Zhou

ZeitPhysikA311,363(1983)Yu. Ryabov et al

Phys Rev C28.276(1983) F.D.Becchetti et al

proton reactions

Ispallation,evaporationmodel

precompoundnucleus emission

197Au

Bi,197AuIr, 165Ho169Tm

27 Al,209Bi

28Si

40Ca

90Zr

40Ca209pb

27Al

Yield of Deep SpallationProducts of Medium to HeavyMass Targets Bombarded with480-MeV Protons

Energy and Angular Distri-butionof Neutrons from90 MeV Proton and 140MeV-Alpha Particle Bombard-ment of Nuclei

Estimation of the SecondaryParticle Production Time inInelastic Light NucleiInteractions

Nonlocal and Local EquivalentMicroscopic Optical Potentials

Giant Spin-Isospin Vibrationsand the Continuum Spectra fromthe (p,n) Reaction at ForwardAngles

Dirac-Equation ImpulseApproximation for Intermedi-ate Energy Nucleon-NucleusScattering

Energy Deposition in Inter-mediate Energy Nccleon-Nucleus Collisions

Inclusive Proton Spectra andTotal Reaction Cross Sectionsfor Proton-Nucleus Scatteringat 800 MeV

CTOM~44886,p.ni(1979) Simon FraserUniv, British Columbia,Thesis, H.P.E.Dautet

Phys Rev C28,105(1983) A.M.Kalendeta!

YadFiz 36,8,390(1982)V.M.Dmitrievetal

Phys Rev C27.2466(1983) W.Bauhoff

NucPhys A395.189(1983) T.Izumoto

Phys Rev Lett 50,1644(1983)B.C.Clark et al

Phys Rev Lett 50,1648(1983)K.Kwiatkowskl

Thesis (1981)U.of Texas,AustinJ.A.McGill

proton reactionsneutron sptvtra

particleproduction

proton reactions,optical models

neutron spectra


nuclear cascades,precompoundnucleus emission

impulse approxi-mation.inelasticscattering.protonspectra

11

Table I (Con t . )

58Ni

g60Ni,28si

2?A1,CCu,Sn,Ta

40Ca,12c24Mg

Al.As.Br,Rb,Y

27Al,40Ca12c,208pb

Continuum Spectrum in theQuasifree (p,2p) Scattering

Proton-Gamma CoineidsnceExperiment on Medi iiMassNuclei at 400 MeV and Studyof Reaction Mechanisms

Neutron Production fromProtons and Deuterons

Simulation of InelasticCollisions of Light Nuclei

Proton-Nucleus Total InelasticCross Sections: An EmpiricalFormula for E>10 MeV

Inclusive Charged ParticleSpectrum from the Interactionof Nuclei with IntermediateEnergy Protons

Studies of (p,n) Reactions atIntermediate Energies

Shell Effect Role in NucleusFission by Fast Protons

Cross Sections for Reactionswith 593 and 540 MeV Protonsin Aluminiun^ArsenicBromine,Rubidium and Yttrium

Real Part of the Nucleon-Nucleus Optical Potential

Phys Rev C2L1360(1983)G.Ciangaru et al

PCCF-T-81-02(1981) Clermont-Ferrand Univ.France.ThesisA.Baldit

DL/NUC/TM-60A(1982) DaresburyLab(UK) report(1982)R.Ryder

Sov Phys Usp. 31,119(1982)VJM.Dmitriev

Astrophy J. 51.271(1983)J Jl ietaw et al

Thesis(1981)Northwestern UEvanston.il.T.Chen

Thesis(1980)Kent State UnivOhio, J.N.Knudson

Sov J Nud Phys35,5,1131(1982)M.M.Nesterov et al

Int J Applied Radand Isotopes(Eng-land)33,9,725(1982) A.Gruetter

Zeit fur PhysikA309,325(1983)S.Bhattacharya,S.Kailas

quasi-freereactions.pre-compound-nucleusemission

quasi-ulasticscattering,nuclear cascades

spallation,neutron spectra

inelasticscattering

inelasticscattering

heavy nuclei,intermediate,light nuclei,inclusiveinteractions

charge-exchangereactions

fission, energydependence

optical models

12

Table I ( C o n t . )

27Al,208pb58,62Ni

235.238U232Th

Au

235,238u

233.238U

Pb

40,48Ca

27Al,24Mg60Ni,28Si

C

Inclusive Proton Reactionsat 164 MeV

Comparison of the (p.xn)Cross Sections from 238u,235u,and 232 rh Targets Irradiatedwith 200-MeV Protons

Study of the Pre-EquilibriumEmission Following the Bom-bardment of Nuclei with200 MeV Protons

Comparison of High-EnergyFission Models for Uie HETCTransport Code

Neutron Production Yields andSpectra from 590 MeV ProtonBombardment of Thick Uranium

High Energy Particle Spectrafrom Spallation Targets

Single Particle Intranuclear"Cascade" and Pion Production

40Ca(p,pn),39Ca and 48Ca(p,pn)Neutron Knockout Reactions at149.5 MeV

Study o? the Reactions of 400MeV Protons on IntermediateMass Nuclei by a Proton-GammaCoincidence Experiment

Quasifree Knockout of ProtonPairs from Carbon

Phys Rev C26.2424(1982) R.E. Segeletal

Brookhaven reportBNL-32166(i982)Y.Y.Chu,M.L.Zhou

Julich reportJUEL-SPEZ-146 p.33(1982)J.P.Didelez

Julich report JUEL-CONF-45Ptl,p.281,Pt2,p.299(1981)Proc 5th Mtg of theInt. Collab on Advan-ced Neutron Sources,T.W.Armstrong et al

Julich reportJUEL-CONF-45,p.333(1981) F.Raupp etal

Julich reportJUEL-CONF-45,p215(1981) G.S.Bauer,D.Filges

Phys Rev £26,1558(1982)D.G.Long,M.M.Sternheim

Phys Rev £26,961(1982)J.W. Watsonetal

Nuc Phvs A384.323(1982)G.Landaudetal

IntConfHighEnergy Physics& Nucl StructureVersaittes,France(7-6-81)p.560V.I.Ko-marov, G.E.Kosarev

inclusiveinteractions,evaporationmodel

knock-outreactions

energy spectra

fission


spallation

particleproduction,nuclear cascades

knock-outreactions


quasi-freereactions

13

6Li

154SmP6 Y b

In.SmAg.Sn

Rb,Br

58Ni

Al.BeCCu

238u

?.08pb90Zr.116sn

62Ni

Table I

Development of IntranuclearCorrelations in the Diffrac-tive Scattering Cross Sectionsof Fast Hadrons by Nuclei

Microscopic Analysis of ProtonScattering on Deformed Nucleiat Intermediate Energies

Anisotropy and Cross Sectionof Fission of Light Nuclei(100

Table I (Cont . )

27A1,CU

In,Pb,U

12C.64CU

12C.64CU

fiu

Pb

27A1.12C64Cu207P b

C,Cu,Fe

Ge

107 A u

40Ca

238u

Determination of the Differ-ential Cross Section forthe Reaction X{p,n)Y Using800 MeV Proton Bombardment ofAl,Cu,In,Pb,andU

Energetic Particles Emittedfrom Energetic NuclearReactions

Model of Intranuclear Cascadewith Account for Resonances

Scattering of 136 MeV Protonsfrom6Li

Neutron and Charged ParticleProduction Yields and Spectrafrom Thick Metal Targets by590 MeV Protons

Isobaric Model in IntranuclearCascade Method

Study on the Neutron Yieldfrom Thick Targets underthe Action of 645 MeV Protons

Proton Loss by NuclearInelastic Interactions inGermanium

Self-Consistent Method forCalculating the Evaporationof Heavy Fragments FollowingEnergetic Initial Reactions _

Model Independent OpticalPotential for Protons at 155MeV

Analysis of the Yield ofNeutrons Produced by High-Energy Protons

Kansas State UThesis(1980)SD.Howe

Zeit fur Physik£306,177(1982)A.H.Elin et al

Dubna reportJINR-2-80-661(1980)N.S.Amelin

NuclPhvsA372.117(1981)R.S.Henderson et al

Karlsruhe reportKFK-3097-B(l980)S.Cierjacks et al

Bull Acad Sci(USSR)45,,U65(1981) V.E.Bunakovetal

Dubna reportJINR-18-80-540(1980) A.Y.Serov etal

Nucl Instr & Meth188,465(1981)R.F.Carlson et al

Nucl Instr & Meth185.195(1981)E.L.Green.R.G.Korteliiig

Zeit fur Physik£300,247(1981)I.Brissaud

Sov At Energy 50,150(1981)V.S.Bara3henkov,S.Y.Shmakov

neutron spectra

inclusiveinteractions,energy spectra

proton reactions,nuclear cascades

inelasticscattering

neutron spectra


neutron emission

inelasticscattering

evaporation model,compound-nucleusreactions

optical models

nuclear reactionyield,gamma radiation

15

Table I (Cont.)

5b

5U

Al,Be,CCu

12C

58,6ONi

27AI,58Ni208pb

232Th235,238u

18lTa

209Bi197 Au

12Q35C163Cu,19F208pb

Angular and Depth DependentNeutron Yields and Spectrafrom 590 MeV (p,n) Reactionsin Thick Lead Targets

Quasifree A(p,p,d)B Large-Angle Scattering at Inter-mediate Energies

Probability of Nuclear Fissionby Intermediate EnergyParticles

Two-Particle DifferentialCross Sections of ProtonEmission in Proton-NucleusInteractions at 640 MeV

Proton-Proton Correlationsin High Energy NuclearCollisions

Elastic and InelasticScattering of 178 MeVProtons from 58Ni and 60Ni

Quasi-Free Proton-Scatteringat 164 MeV

Main Aspects of Proton LinearAccelerators for Nuclear FuelProduction

Neutron Production by Protons(190 to 268 MeV) in a Water-Cooled Tantalum Target

Studies of IntermediateEnergy Fission

One- and Two-Proton InclusiveSpectra in 800 MeV Proton-Nucleus Collisions and theMean Free Path of Protons inNuclei

Proc 5 th All-Union Conf NeutronPhysics, p.269(1980)S.Cierjacks

J of Physics G7.1045(1981)L.Vegh

YadFiz 32,322(1980)A.S.n'Inovetal

YadFiz 32,313(1980)V.I.Komarov

Phvs Lett B 103.264(1981)J.Knoll,LRandrup

NuclPhvsA365.426(1981)A.Ingemarsson et al

Phys Lett B103.192(1981) T.Chenetal

Proc 6th All-UnionConf Charged Par-ticles AcceleratorsV.l,p.24l(1979)B.P.Murin, AP.Fedotov

Oak Ridge reportORNL/TM-7949(1981)R.G.Alsmiller et al

Thesis(19S0)S.FraserUniv. (BC)D.M.G. Dautet

Phvs Lett B100,121(1981)I.Tanihataetal


quasi-freereactions,knock-outreactions

fission.cascadetheory

cascade theory

inclusiveinteractions,cascade theory

elastic andinelasticscattering

quasi-freereactions

linearaccelerators

neutron spectra


16

Table I (Cont.)

CPb

27 Al181Ta

Au,Ho,ReTa,Tl

Ce,Yb

CN.O

12r

238u

Hadron Cascades in ThickMaterials PU Monte-CarloMethod for Simulation ofCascades

Proton-Inclusive CrossSections from 600 MeV Proton-Nucleus Reactions

Study on the SecondaryRadiation Field behind theLead Absorber Exposedto the 640 MeV Proton Beam

Yield of Deep SpallationProducts of Medium to HeavyMass Targets Bombardedwith 480 MeV Protons

Mass Distributions in theFission of Medium-Heavy andLight Nuclei

Specific Features of Quasi-Elastic Knock-Out of Slow(E<or approximately 10 MeV)Protons from C, N, O Nucleiby High Energy Protons

12C(p,n)12N Reaction at 120,160, and 200 MeV

Delayed-Neutron Fraction ina Pulsed Spallation NeutronSource

Two-Particle DifferentialCross Sections for ProtonEmission in Proton-NucleusInteractions at 640 MeV

Test of Models for InclusiveProduction of Energetic LightFragments a: IntermediateEnergies

Mechanisms for (p,p')Reactions in the Continuum

Nucl Inst & Meth179.77(1981)M.Nieminen, JJ.Torsti

Nucl Phys A352,485(1981)K.R.Cordell

Dubna report JINR-R-16-12765(1979)A.Y.Serov et al

Can J Phys 58,891(1980)HJ3autetetal

Phys Rev £24,769(1981)H.Gustafsson et al

YadFiz31,569(1980)A.A.Levkovskii,E.F. Dreiman

Phys Rev C24.335(1981)J.Rapaport et al

Nucl Instr & Meth175.2.87(1980)LM.Carpenter

Sov J Nucl Phys32,161(1980)V.LKomarov et al

Phys Rev C23.2788(1981)D.H.Boaletal

PhvsLettB91.169(1980)J.R.Wu

knock-outreactions,neutron spectra


nuclear cascadesproton spectra

spallation

Fission

proton spectra,quasi-elasticscattering


spallation

inelasticscattering,quasi-freereactions,cascade theory

evaporationmodel.inclusiveinteractions

inelasticscattering,proton spectra

17

Table I (Cont.)

La

40Ca

209Bi207Pfc

27 AJ18lTa

Ni.Ta

U,Pb232Th

238U

Pb

235.238U

238U

Calculation of SpaltationYields: Application to theSpallation of LanthanumInduced by 600 MeV Protons

Dirac Optical Model Analysisof 40Ca Elastic Scattering at180 MeV and the Wine-Bottle-Bottom Shape

Nuclear Fission Induced byHigh Energy Protons

High Energy Proton Productionin Medium Energy NuclearReactions

Inclusive Scattering ofProtons on Helium,Nickel,and Tantalum at 500 MeV

Neutron Production in ThickTargets of Lead,Thorium andUranium Bombarded by480 MeV Protons

Fission Reaction in HighEnergy Proton Cascade

Neutron Yields and Spectrafrom 590 MeV (p,n) Reactionson Lead Targets

Phenomenological Model forParticle Production from theCollisions of Nucleons andPions with Fissile Elementsat Medium Energies

Spallation and Fission inHeavy Metal Nuclei under Med-ium Energy Proton Bombardment

Phys Rev £23,2129(1981) GHuds tarn,EUagebo

Phys Rev £23,1949(1981)L.G.Amoldetai

Dubna reportJINR-E-1-12902(1979)V.S.Barashenkovetal

U of VirginiaThesis(1979)K.R.Cordell

Phys Rev £23,1670(1981) G.Royetal

Brookhaven reportBNL-NCS-51245(Vol.l)p.l55(1980)J.S.Fraser et al

Brookhaven reportBNL-NCS-51245p.l33(1980)H.Takahashi

Brookhaven reportBNL-NCS-51245p.201(1980)S.Cieijacks et al

Oak Ridge reportORNL/TM-7528(1981)F.S.Alsmiller

Mich Mtg. onTargets for NeutronBeam Spallation SourcesJUEL-CONF-34,p.l7(1580)F.Atchison

evaporation modelnuclear cascades

elasticscattering,Dirac equation

neutron spectra,nuclear cascades


spallation

nuclear cascades

neutron spectra,nuclear cascades

spallation


18

40Ca208pb

Pb

Ag

58,62Ni

27 Al

208pb

175Lu

159Tb

12C

Table I

Elastic Scattering of 80-180MeV Protons and the Proton-Nucleus Optical Potential

Neutron Production bySpallation in Heavy MetalTargets: Experiments andCalculation

Differential Production Cross-Sections of Multiply ChargedFragments in 800 MeV Proton-Induced Spallation of Carbon,Aluminum, and Nickel

Fragment Production from p+AgInteractions at IntermediateEnergies

Recoil Ranges of Nudei. Pro-duced in the Interaction of80-164 MeV Protons with Ni

Microscopic Description ofNucleon-Nucleus TotalReaction Cross Sections

Pre-Equilibrium Process for175Lu(p,xn gamma), 176Yb(3He,xn.yp gamma)and 174,176 Yb(alpha,xn gamma) Reactions

Medium Energy Proton InducedFission in Tb,La and Ag

Do Quasifree ReactionMechanisms ExplainReaction Cross Sectionsin Intermediate-EnergyProton-Nucleus Scattering

( C o n t . )

Phys Rev £23,1023(1981)A.Nadasen

Julich Mtg. onTargets for NeutronBeam Spallation SourcesJUEL-CONF-34,p.(1980)P.Garvey

Wash. State UThesis (1978)S.C.Luckstead

Phys Rev £22,1594(1980)R.E.Green,R.G.Korteling

Phys Rev £22,1443(1980)J Jastrzebski et al

Phys Rev Lett 45,527(1980)N.J.Digiacomoetal

Phys Rev C22,1002(1980)H.Sakaietal

Zeit fur PhysikA293.24U1979)G.Andersson et al

Phys Rev Lett 24,1579(1980)Y.Alexander etal

optical models

neutron spectra,spallation

spallation

energy spectra,evaporationmodel

compound-nucleus reaction,gamma spectra,nuclear cascades

compound-nucleusreactions1'

precompound-nucleus emission

evaporationmodel

quasi-freereactions

19

Table I (Cont.)

!8Si

197 Au

40Ca12C

27Al,9BeC,Pb

209Bi238u

58,60Ni62Ni

58,60Ni

Gennanium Charged ParticleTelescopes with Ultra-ThinDetector Contacts

Use of A Ge(Li) GammaDetector Near A 400 MeVIntense Proton Beam ina p-Gamma CoincidenceExperiment

Cross-Section Measure-ments of NuclidesFormed by the Reactionof0.20-6.0GeVProtons with 197 Au

Scattering and ReactionCross Sections MeasuredatSPESI

Proton-Nucleus Inter-actions at 640 MeVAccompanied by Back-ward Emission of EnergeticProtons

Solid State Detectorsof Fission Fragments forthe Rem-Dose Measurementof Mixed and Proton andNeutron Radiation

Interaction of 80 -164 MeV Protons withNickel Isotopes

Mechanism of NucleonRemoval from MediumMass Nuclei Induced by80 to 164 MeV Protons

Particles and Gamma RaysFollowing Preequilibriumand EquilibriumReaction Processes

NuclInstMeth164.121(1979)G.S.Hubbard,E.E.Haller

Nucl Instr Meth165.409(1979)C.Lebrun et al

Phys Rev £22,167(1980)S.B.Kaufman,E.P.Steinberg

J de Physique40,635(1979)CBruge

Nucl Phvs A326.297(1979)V.I.Komarovetal

Health Physics 37,677(1979)M.F.Lomanov et al

Phys Rev C21.2303(1980)R.E.Segel

Thesis(1977)Indiana UM.E.Sadler

Osaka Univ (Japanreport) RCNP-P-21p.83 (1978)H.Ejiri et al

high-pur ty GEdetectors

Li-drifted Gedetectors,prompt gammaradiation

spallation

data compilationdeuteron, alphareactions

quasi-elasticscattering

compound-nucleusreactions,gamma spectra

precompound-nucleus emission,nuclear cascades


20

Table I (Cont.)

12r

27A1.40C

12C

14N

238u

Br,C,NO,Ag

9Be,12c

i81Ta

Inclusive DifferentialCross Sections forProton Production I».Proton-Nuckus inter-actions in the Model ofCoherent Fluctons

Neutron Formation from7Li,10B,nB,12c,16o,19F,24,25,26Mg,27Ai,40>44Ca,Cu,116,1245^18^3, PbNuclei with 1 GeV Protons

Proton Spectra from800 MeV Protons onSelected Nuclides

Elastic and InelasticScattering of 185 MeVProtons from 12c

Determination of theOptical Potential forElastic Proton Scat-tering on 6Li, 12c, and14N at 144 MeV

Neutron Multiplicationin Uranium Bombardedby 300-600 MeV Protons

Scaling in MultiplicityDistributions of Heavy,Black and Grey Prongs inNuclear Emulsions

Proton Total CrossSections on lH,2H,4He,9Be,C and O in the EnergyRange 180 to 560 MeV

Neutron Spectrum at 900from 800 MeV (p,n)Reactions on a Ta Target

Calculated Particle Pro-duction Spectra andMultiplicities fromNucleon-Fissile ElementCollisions at MediumEnergies

Dubna reportJINR-R-4-12207(1979)(Russian)A.N.Antonovetal

JETP Lett 30,86(1979)V.N.Baturinetal

Phys Rev £21,1014(1980) R.E.Chrienetal

Nucl Phys A319.377(1979)A.Ingemarssonetal

Phys Rev £21,25(1980) G.L.Moake,P.T.Debevec

Sov At Energy 44,329(1978) :iR.G.Vasil'kov et al

Physica Scripta19,307(1979)M.Nieminen et al

Nucl Phys A316,317(1979) P.Schwalleretal

Los Alamos reportLA-UR-79-3201(1979)S.D. Howe et al

Int Conf NuclearCross Sections forTechnology, Knox-ville,CONF-791058(1979)F.S.Alsmilleretal

particleproduction,inclusiveinteractions

light nuclei,knock-outreactions,quasi-elasticscattering,neutron spectra


inelastic.elasticscattering,optical models

ift

optical models!*

fission

multiplicity

total crosssections

neutron spectra

nuclear cascades,statisticalmodels

21

Table I (Cont.)

12C

lSlja

238u

209Bi197 Au206,207pb208pb,Sm232xh235U

27A1.12C63Cu,Ge56Fe208pb16o

40Ca56Fe16o

Ag

27 Al

Inclusive Double Dif-ferential Cross Sectionsfor Backward EmittedProtons in Proton-NucleiInteractions at 640 MeV

Cluster Recoil Mechanismfor Inclusive NuclearReactions

Analysis of NeutronYield Produced byHigh Energy Protons

Determination of FissionCross Sections of 238u235u,232Th,209Bi,208,206pb,197Au)18lTa,Yb and 3m Nuclei by1 GeV Protons

Proton-Nucleus TotalCross Sections in theIntermediate EnergyRange

Phenomenology of ProtonElastic Scattering andEvidence for Angular-Momentum-DependentOptical-Model Potentials

Study of Highly ExcitedNuclei from 300 MeV pon Ag by Use of HeavyFragment Evaporation Yields

Analysis of the NucleonsEjected in a Quasi-ElasticScattering (p.p.gamma)at 400 MeV

Phenomenology of NuclearInclusive Reactions

Dubna reportJINR-E-1-11513(1978)V.I.Komarov et al

Nucl Phys A306.333(1978)R.M.Woloshyn

Brookhaven reportBNL-26805(1979)H.Takahashi,Y.Nakanara

YadFiz 28,572(1978)B.A.Bochagovetal

Phys Rev £20,1857(1979) L.Ray

energy spectra

inelasticscattering

evaporationmodel,spallation

total crosssections

JofPhysG5,97(1979)A.M.Kobos,R.S.MacKintosh

AlPConfProc.£7,672(1978)R.E.L.Green,R.G.Korteling

J de Physique 3̂138(1978)C. Lebrun et al

AlPConfProc 47,457(1978)R.M.Woloshyn

optical models

spallation,evaporationmodel

quasi-elasticscattering,gamma radiation

knock-outreactions,inelasticscattering

22

27A1.58Ni90zr

238U

Alje238uLucite

232Th238u

Yb

Table I

Medium Energy NuclearReactions: "Quasi-Two-Body Scaling" and"Hot Spots"

Spallation Neutron Sourcesfor Neutron Beam Research

Measurements and Calcula-tions of Reaction Lossesof Medium-Energy Protonsin NAI Detectors

Thick-Target Neutron andGamma Ray Yields Inducedby Medium-Energy Protonand Deuteron Bombardments

Breeding Nuclear Fuel WithAccelerators: The Electro-nuclear Method. NuclearPhysics Aspects

Analysis of Nuclear Fissil-ity for Intermediate-Energy Proton InducedReactions

Observation of the Effectof Central CollisionsLeading to Formation of

(Cont . )

Phys Rev C2., 1079(1979)N.S.Walletal

Contemporary Phys19,505(1978)

G.Mann ing

Nucl Instr Meth153.511(1978)C.A.Goulding,J.G.Rogers

Lawrence LivermoreNat Lab reportUCID-18086(1979)J.A.Becker et al

Sov J Particles &Nuclei(U.S.) 9,452V.S.Barashenkov (1978)

Zeit fur PhysikA287.37(1978)A.S.Iiinov et al

Sov J Nucl Phys27,751(1978)O.E.Shigaev et al

compound-nucleusreactions,energy spectra

spallation

NAI detectors,energy losses

gamma radiation

Fission,evaporation,precompound-nucleus emission

heavy nuclei,compound nuclei

208pb58Ni

90zr

40,42Ca12c,20Sp58Ni

a Compound Nucleus inInteraction of 200-MeVProtons with Nuclei

Elastic Scattering of 100MeV Protons and SystematicOptical Model Analysis

Microscopic Approaches tothe Intermediate EnergyNucleon-Nucleus OpticalPotential

Nucl Phys A301,349(1978)K.Kwiatkowski,N.S.Wall

U of TexasThesis(1977)R.L.Ray

optical models

optical models

Sm,Yb L-Shell X-Ray ProductionCross Sections Due to lH,^He, and 7Li Ion Bombard-ment of Selected Thin RareEarth and Pb Targets

North Texas StateU, Thesis(1978)G.M.Light

x-radiation

23

Table I (Cont . )

LJ

27A1.12CNi

27Al/»0Ca12C,6Li7Li,24Mg

2O9Bi238u

27A!.CUPb.Ti.WU

Ca,208pbSi,90zr

27Al,9Be10,11B12C

C,6Li18lTa

Analysis of Neutron YieldProduced by High-EnergyProtons

Differential ProductionCross Sections of MultiplyCharged Fragments in800 MeV Proton-InducedSpallation of Carbon,Aluminum, and Nickel

Low-Energy Particles inNuclear Reactions Producedby Nuclei with Energiesof 0.1-1 GeV/Nucleon

Quasielastic Knockout ofAlpha Clusters fromLight and Medium Nucleiby 600 MeV Protons

Nucleon Losses by Uraniumand Bismuth Nuclei at High-Energy Fission

Systemacics of 00 NeutronProduction by 800 MeVProtons on Targets with27

12c,Pb

27 Al

197Au,Ag181Ta

9Be

160

59Co,56Fe58Ni

T a b l e I

Determination of the Pene-tration Range with the Aidof Total Cross Sections ofProtons, Pions, and AlphaParticles Between 200 MeVand2GeV

Inclusive Spectra and theAngular Distribution ofProtons Emitted Backwardsin the Interaction of 640MeV Protons with Nuclei

High Energy (E less than orequal to 1000 GeV) Intra-nuclear Cascade Model for

( C o n t . )

J Plasma Phys 3,1497(1977)I.Brissaad

Phvs Lett B69.37(1977)V.I.Komarovetal

Oak Ridge reportORNL/TM-5710(1977)H.W.Bertini et al

total crosssections


nuclearcascades

Nucleons and Pions Incidenton Nuclei and Comparisonswith Experimental Data

Cross Section Measurementsof High Energy Proton Indu-ced Reactions in Gold,Tantalum and Silver Targets

Correlated Clusters" andInclusive Spectra of Ener-getic Protons at 180° inProton-Nucleus Collisions

Neutron Spectra at 00Degrees from 83.7-MeVDeuterons and 100.2-MeVProtons on Beryllium

Maxwell Distribution andMass Motion in p-NucleusReactions

Gamma Specttometry withHigh Energy Protons

Systematics in the Inter-action of Intermediate-Energy Protons withMedium-Mass Nuclei

Calculation of the NuclearReaction Cross Sectionswith an Intranuclear-Cascade Model

Inorg & Nucl ChemLett 13,205(1977)S.Kraemer et al

Phys Rev Lett 39,174(1977) TJujita

Medical Physics 4,322(1977) RMadeyetal

Phvs Rev D15.2533(1977) T.FHoang

Saclay reportCEA-N-186l(nd)J.P.Alard et al

Phys Rev Lett 17,950(1977) M.Sadleretal

Japan Atomic Re-search Institutereport JAERI-M-6306(1975)S.Baba

inclusiveinteractions,backscattering

neutron spectra

inelasticscattering,Boltzmannstatistics:

prompt gammaradiation

precompound-nucleus,gamma spectra

heavy nuclei,Monte Carlomethod, nuclearcascades

25

T a b l e I ( C o n t . )

CPb

27 Al

9Be,C,Li

27 Al

27A1,45SC

Ti,51V,Fe

Picton and Deuteron DoubleDifferential Cross Sectionsat Angles from 10 Deg to 60Deg from Qe, C, Al. Fe, Cu,Ge, W. and Pb Under 558-MeV-Proton Irradiation

Neutron Spectra at ZeroDegrees from Proton Bombard-ment of Light Nuclei atMedium Energies

Production of Fast Fragmentsby Bombarding Light Nucleiwith Intermediate-EnergyProtons

Neutron Spectra at 00 from(p,n) Reactions on 9Be, 12c,and 27Al at 647 and 800 MeV

A Two-Parameter Scintill-ation Spectrometer Systemfor Measurement of Secondaryp, d, t Distributionsfrom Materials under 558MeV Proton Irradiation

NASA report NASA-TN-D-8119(1976)S^.Beck,C.A.Powell

Univ of New MexicoThesis(1975)C.G.Cassapakis

Nucl Phys A256.362(1976)V.I.Komarovetal

Phvs Lett B63.35(1976)C.G.Cassapakis et al

NASA report NASA-TN-D-7925(1975)S.M.Beck

proton reactions,quasi-elasticscattering



charge-exchangereactions,neutron spectra

time of flightspectrometer

90Zr

Recoil Propteries ofSpallation Products fromBombardment of Z= 13-29Targets with 150, 300,and 600 MeV Protons

Elastic and InelasticScattering of 185 MeVProtons from 6Li

Monte-Carlo EvaporationCalculation!! for the Inter-pretation of Isotope YieldDistribution in High EnergyNuclear Reactions

Systematic Study of Proton-and Alpha-Induced SimpleReactions

Nucl Phys A260,369(1976) M.Lagarde-Simonoff et al

Zeit furPhysikA275.169(1975)M.Y-MJHassan et al

Marburg U.GermanyThesis(1974)G.Stark

Carnegie-Mellon UThesis(1976)M.A.Yates

spallation


heavy nuclei,intermediatemass nuclei,evaporationmodel, Monte-Carlo method,Weisskopf Model

knock-outreactions

26

27A1,CCu,Fe

Ugypsum

27A1.MOLa,V

20Ne,S8Ni154S m

120Sn

56Fe,60Ni

6,7Li

56,57pe

Table I

Interlaboratory Comparisonof Spallation-ReactionCross Sections for Iron andCopper with 590-MeV Protons

Spectrum and ShieldingMeasurements and Calcu-lations of NeutronsProduced by 800 MeVProtons

Spallation Cross Sectionsand the LAMPF MedicalRadioisotope Program

Effective Nucleon-NucleonForces and Description ofContinuous and DiscreteSpectra in SemimicroscopicApproach

Analysis of a MultistageMechanism of the (p,p')Reaction in the QuasiParticle-Phonon Model ofa Preequilibrium Decay

Energy Spectra of Particleswith Z < 2 From The 60Ni,62Cu and 64zn IntermediateSystem Decay

Effect of the First Stageof Multistep Direct Pro-cesses at the Energyof the Order of 100 MeV

Energy Spectra and AngularCorrelation Functions ofCharged Particles from the6Li(p,pd) and 7Li(p,pt) atthe Incident Proton Energyof 70MeV

Proton Pre-EquilibriumSpectra from Decay of theComposite System 60Ni

( C o n t . )

Jlnorg&NuclChem 38,13(1976)C.J. Orth et al

Proc on Nucl CrossSections & Tech,Washington.DC.NBS-Spec Pub 425,476(1975) L.R.Veeser et al

NBS Spec Pub 425,492(1975) BJR^rdaletal

34th Conf on NuclSpect & NuclStruct.,Alma-Ata,USSR.INIS-SU-282p.424(1984)CM.Knyaz'kov et al

34th Conf on NuclSpect & NuclStruct.Alma-Ata,USSR.INIS-SU-282,p.302(1984)A.K.Deb et al

Bull Acad ofSciences,Phys.Series 48,1006(l984)N.T.Burtebaev et al

Bull Acad ofSciences,Phys.Series 47,2224(l983)F.A.Zhivo-pistsev et al

34th Conf oh NuclSpect & NuclStruct,Alma-Ata,USSR.INIS-SU-282p.290(!984)M.V.Pasechnik et al

3rd Int Symp onNeutron InducedReactions,p.335(l982)Smolenice,Czech. A.D.Duisebaevetal

spallation

neutronemission

spallation

pru... it.iction


precompound-nucleus emission,energy spectra

direct reactions,precoinpound-nucleus emission

quasi-elasticscattering,proton spectra


27

Table I (Cont . )

59Co

9Be

12c,24Mg28Si

152Sm

6Li

9Be

Th,233u

209Bi54Fe,12uSn

I18Sn,90zr

Pairing and ShellEffects in (p,xn) Pre-equilibrium Emission

One- and Two- NeutronPick-Up Reactions Inducedby Protons Interactingwith 9Be

Inelastic Scattering of 65MeV Protons from 12c, 24Mg,and28si,and32s

Levels in 149EU from the(p,4n gamma) Reaction

Evidence for MultistepProcesses in ProtonCapture Reactions

Reaction of (p,pn) onLithium Isotopes at theProton Energy of 70 MeV

One-Neutron and Two-NeutronPickup in Interaction ofProtons with 9Be

Linear Momentum Transferin Intermediate-EnergyProjectile-NucleusCollisions

Contribution of One- andTv i- Step Processes toInclusive (p,d) Reactions

Mechanism of the (p.alpha)Reaction: Pick-Up or Knock-Out

Workshop on Coinci-dent ParticleEmission fromContinuum States,BadHonnef(W.Ger-many)INIS-MF-9280(1984)M.Blannetal

YadFiz 39,1081(1984)N.l.Zaikaetal

Phys Rev C31,1616(1985)S.Katoicetal

Nuovo CimentoA82,253(1984)G. Lo Bianco et al

Phys Rev C31,660(1985) H.J.Hausman

34thConfonNuclSpect & NuclStruct,Alma-Ata,USSR.INIS-SU-282,p.282(1984)O.K.Gorpinich et al

YadFiz 39,682(1984)N.I.Zaikaetal

3rd Winter Workshopon Nuclear Dynamics,Copper Mtn.,Co.CONF-8403101 pp.126-130(1984)K.Kwiatkowskietal

Nucl Phys A424.1(1984)A.O.Gattoneetal

Zeit fur PhysikA318,145(1984)E.Gadioli et al

intermediatemass nuclei,precompound-nucleus emission,inclusiveinteractions,neutron spectra

pickupreactions

elastic andinelasticscattering

electron spectra,gamma spectra,k conversion

capture

energy spectra

one-nucleontransfer reac-tions, pickupreactions

nuclear cascades

deuteron spectrainclusiveinteractions

knock-outreactions

28

Table I (Cont . )

7Al,58Ni

3Nb

209Bi197 A u

90zr

U6.118Sn122Sn

12C160

9Be

48,50Ti

CCuJ'b

"One, Two, Infinity" Modelfor Precompound Reactionand Nuclear Size Effect

Analysing Power of NeutronContinuum Spectra for the93Nb(p,nx) Reaction at 65MeV

Extension of the Gener-alized Exciton Modeland Calculations of(p,p') and (p.alpha)Angular Distributions

DWB A Description of the90zr(p,d)89zr Reaction atEnergies from 20 MeV to185 MeV

Analysis of (p,p),(p,n),and (n,n) Scattering onthe Even Tin Isotopes Usingthe Lane Coupled Equations

Intranuclear Cascade andFermi Breakup Calculationsof lH- and ̂ He-InducedReactions On Light TargetNuclei

Comparison of the NeutronFields Produced by 50 MeVDeuterons and 65 MeV Protonson 9Be at the Louvain-La-Neuve Cyclotron

48Ti and 50ri (p,xpyn)Excitation FunctionsInduced by Protons from5-85 MeV. Comparison withPre-Equilibrium Calculations

Neutron and Photon Produc-tion from Thick TargetsBombarded by 30-MeVp,33-MeVd,65-MeV3He,and 65-MeV Alpha Ions:Phenoinenological Analysisof Experimental NeutronEnergy Spectra

Chinese Physics 4,636(1984)Ji-Zhi Pan, Huan-Cheng Chiang

J De Physique(Paris)45,31(l983)H.Sakai et al

Nucl Phys A419.472(1984) A.Iwamoto,K.Harada

Phys Lett B137.334(1984)P.W.F.Alonsetal

Phys Rev £29,1710(1984) C.Wong etal

Phys Rev £29,1606(1984)A.Goekmenetal

Int Conf NuclearData for Sci & TechAntwerp.BelgiumSept 6-10(1982)LPivIeulders et al

McGill Univ,Montreal, CanadaThesis(l979)KJ.W.Burns

Phys Rev £29,1317(1984)T.Nakamura,Y.Uwamino

precompound-nucleus,neutron spectra

inelasticscattering,neutron spectra

inelasticscattering,pickup reactions,precompound-nucleus emission

proton-neutroninteractions.one-nucleontransferreactions;


breakup reactions,nuclear cascades

neutron sources


stripping,breakup reaction,evaporation modelnuclear cascades,precompound-nucleus emission,Serber Theory

29

Table I (Cont.)

CCufePb

46.48T1SOTi

14N

Ge

58Ni

6JLi

9Be

208pb,7Li

209Bi,12C

Neutron and Photon Produc-tion from Thick TargetsBombarded by 30-MeV p,33-MeV d, 65-MeV 3He, and 65-MeV Alpha Ions: Experimentand Comparison with CascadeMonte Carlo Calculations

Elastic and Inelastic Scat-tering of 100 MeV Protonsfrom the Even-Even TitaniumIsotopes

(p,n) Reactions on l^Cand 14N and the EffectiveNucleon-Nucleon Interaction

Excitation Functions ofGe(p,xnyp) Reactions andProduction of 68Ge

Two-Step Description of a(p,3He x)-Reaction to theContinuum

(p,px) Reaction on 6Li and7li Nuclei at IncidentProton Energy of 70 MeV

Neutrons Produced by thep + Be and the d +Be Reactions, and theCross Section Measurementwith these Neutrons

Total Neutron Yields from100 MeV Protons on Pband 7Li Targets

Edge and Cluster Effectsin Precompound NuclearReactions

Phys Rev C29,1307(l984)K.Shinetal

Phvs Rev C29.794(1984) L. W. Woo etal

Phys Rev £29,764(1984)T.N.Taddeuccietal

IntJof ApplRad& Isotopes 34,1531(1983)T.Horiguchietal

HelPhys Acta56,975(1983)H Jasicek et al

Bull Acad SciencesPhys Series 47,185(1983)O.K.Gorpinich

Meet on Heavy andLight Ion Irrad. &Rad. MeasurementTokyo,Japan p.33(1981)K.Sugiyama

Nucl Instr & Meth214,333(1983)M.A.Lone et al

Zhonghua HeyixueZazhi(China) 4,216(1982) W.Ye etal

nuclear cascades,neutron spectra

elasticscattering,optical models

charge-exchangenucleon-nucleoninteraction,optical models

knock-outreactions,quasi-elasticscattering,nuclear reactionyield

two-nucleontransfer

quasi-freereactions

neutron spectra

knock-outreactions

precompoundnucleus emissionnaclear cascades

30

27 Al

233.235U

27Al,209Bi79Br,197Au

65Cu,89Y64Zn

197 Au202Hg

40Ca,208pb

9Be

27Al,59Co

27Al,S9Co197Au,232Th

Tab le T

Emission of Alpha Particlesin Statistical MultistepCompound Reactions

Pre-Equilibrium Emission ofLight Composite Particlesin the Framework of theExciton Model

Isotopic and Neutron Yieldsof Products from the Asym-metric and Near-SymmetricProton-Induced Fission of233u and 235u

Cascade-Exciton Model ofNuclear Reactions

Double Differential CrossSections for (p,xn) Reac-tions of 64Zn, 65cu and89y with 26 MeV Protons

Pre-Equilibrium Decay ofNuclei with A ApproximatelyEqual 200 at ExcitationEnergies to 90 MeV

"Wine-Bottle" OpticalPotentials and theInelastic Scattering ofProtons Near 200 MeV

Fragmentation SpectraInduced by Light IonsColliding With LightNuclei

Interpretation of Some(p,n), (n,p), and (3He,p)Reactions by Means ofthe Statistic^ MultistepCompoi .jd Emission Theory

Proton-Induced Alpha -andTau-Emission at 72 MeV

( C o n t . )

Phys Rev £28,1892(1983) R.Bonettietal

Phys Rev C28.1527(1983) K.Sato etal

Phys Rev £28,1188(l983)P.A.Beeleyetal

Nucl Phys A401.329(1983)K.K.Gudimaetal

Zeit fur PhysikA311.323(1983)W.Scobel et al

Nuovo Cimento A40,383(1977) E.Gadiolietal

Nucl Phys A394.349(1983)G.R.Satchler

Phys Rev £27,1876(1983)T.Delbaretal

Phys Rev £27,1003(1983) R.Bonettietal

Nuovo Cimento Lett28,15(1980)Z.Lewandoski et al

statisticalmodels


fission yield

inclusiveinteractions,charge-exchangereactions

neutron spectra


inelasticscattering,optical models

fragmentation,inclusiveinteractions,quasi-freereactions

charge-exchangereactions,statistical models

emission spectra

I•r

31

Table I (Cont . )

"Al .^Co

3e

Pb,Li

209Bi208pb

27Al,209Bi

24Mg

120Sn

3He,238u

Semiernpirical Calculationof Excitation Functions

Energy Dependence ofOptical-Model Parametersfor the p + 32s Systembetween 15 and 135 MeV

Comparison of NeutronTherapy Beams Produced by50 MeV Deuterons and 65MeV Protons on Beryllium

Measured and CalculatedNeutron Yields for100 MeV Protons on ThickTargets of Pb and Li

Analysis of (p,p') Reac-tions into the Continuumin the Microscopic Me*1"1

Continuum Spectra inLight-Ion Reactions

Elastic and InelasticScattering of Protonsfrom 24Mg

Statistical MultistepDirect Emission TheoryRevisited

Pion Production andCharged-ParticleMultiplicity Selectionin Relativistic NuclearCollision

IntConfonNuclCross Sections forTech.Knoxville, NBSSpec Pub 594,778(1979)E.L.Petersen

Nuovo CimentoA59.10U1980)R.De Leo et al

Acta Radiol Oncology,Rad. Therapy, Physics& Biology 21,281(1982)S.Vynckier et al

Proc 6th Meeting IntCollaboration ofAdv .Neutron SourcesJune 28,1982Argonne report ANL-82-80 p.583, R.TJonesetal

INIS-MF-7523(1981)Annual ReportTexas U, AustinT.Tamura, H.Lenske

Int Symp on HighlyExcited States inNuclear ReactionsOsakajapan, May 1980H.Ikegami,M.Muraoka

PhvsRevC27.482(1983)D.KHaselletal

Phvs Utt B 112.189(1982) M.S.Hussein,R.Bonneti

Phys Rev £26,2572(1982)K.L.Wolfetal

excitationfunctions

optical models

neutron beams

spoliation,neutron emission

inelasticscattering,particle-holemodel

directreactions

optical models

direct reactions,cascade theory,statistical models


32

208pb

58Ni

6JLi

9Be,?Li

27AI.63Cu

12C,64Cu208pb

Table I

Mechanism of ClusterEmission in Nucleon-InducedPreequilibrium Reactions

Study of the Hard Partof the Neutron Spectrain (p,n) Reactions

Quasiparticle-Phonon Modelof the PreequilibriumDecay

Study on the High EnergyRange of the Spectrain the (p,n) Reaction

De-Excitation of ContinuumStates Induced by MediumEnergy Protons

(p,px) Reaction onthe 6lj and 7Li Nucleiat the 70 MeV IncidentProtons

Characteristics of Neutronsfrom Be Targets Bombardedwith Protons, Deuterons,and Alpha Particles

Excitation Functions forRadioactive Isotopes Pro-

(Con t . )

Phys Rev £26,1821(1982) A.Iwamoto,KHarada

SovJofNuclPhys35,474(1982)N.S.Biryukov et al

ENIS-SU-125p.44O32. Conf Nucl Spec-troscopy & NuclStructure, Kiev(1982)F.A.Zhivo-pistsev et al

INlS-SU-125p.3O032. Conf Nucl Spec-troscopy & NuclStructure,Kiev(1982)N.S.Biryukov et al

Int Sym on HighlyExcited States inNuclear Reactions,Osaka,] apan(May 12,1980) D.L.Hendrie

INIS-SU-125 p.29732. Conf Nucl Spec-troscopy & NuclStructure,Kiev (1982)O.K.Gorpinich et al

Nucl Instr & Meth189,515(1981)M.A.Loneet al

Nucl Phys A383.98(1982) A.Gruetter

compound-nucleusemission


precompound-nucleus emission,inelasticscattering

light nuclei,charge-exchangereactions,neutron spectra

inelasticscattering

knock-outreactions



duced by Proton Bombardmentof Cu and Al in the EnergyRange of 16 to 70 MeV

How Important Is The FirstInelastic Collision inNuclear PrecompoundReactions

Nucl Phys A384.24(1982)W.Q.Chaoetal

quasi-elasticscattering,inclusiveinteractions

33

7Li

120Sn

208pb

Co,FeCu,Ni

48,50-r/i

54Fe

208pb

Table I

Nucleon Scattering fromLight Nuclei. Pt. 1.The Target 6Li and "?Li

Calculation of Neutron,Proton and Alpha-Particles Absorption CrossSections by Nuclei in theFramework of Optical Modeland Analytical Formulae

Theory of StatisticalMulti-Step Direct andCompound Reactions

Semi-Microscopic OpticalPotential Calculation byNuclear Matter Approach

Integral Excitation Func-tions for Proton andAlpha Induced Reactionson Target Elements 22

Table I (Con t . )

11B, 12C

238u

208pb

Fe.Ni.Ti

50Ti

Ge.Ga

27 Al208Bi,12c208pb

12c,63Cu6,7Li

235,236TJ

238U

Single-Particle Model ofCapture to ContinuumStates

238u Fission at EnergiesUptolOOMeV

To The Problem on theRatio of Contributionsof Multistep Direct andPre-Equilibrium Processesin Inelastic NucleonScattering

Isospin Dependence ofthe 65 MeV Proton OpticalPotential in f-p Shell Nuclei

Emission of Alpha Particlesin the Interaction of 10-85MeV Protons with 48,50ri

Proton Scattering byNuclei of Atoms of Semi-conductors and EnergySpectra of PrimarilyKnocked Out Atoms

Spectral Measurementsof Neutrons Producedby 52 MeV Protons withActivation Detectors

Backward InclusiveSpectra in Proton-NucleusCollisions at 640 MeV

Postfission Neutrons fromProton Induced FissionOf235,236,238u

Neutron Yields fromProton.Deuteron andAlpha Bombardment ofBeryllium

NuclPhvsA375.169(1982) RJ.Philpott,D.Halderson

PhysRevC25,899(1982) C.Chung,J.J.Hogan

INIS-MF-6819p.49O31.ConfNuclSpec-troscopy & NuclStructure,Samark-land, USSR April14,1981,F.A.Zhivo-pistsev, N.P.Yudin

NuclPhysA366,l89(1981)T.Moroetal

ZeitfurPhvsikA301,289(1981) E.Gadiolietal

INIS-MF-6819 p.55731.ConfNuclSpec-troscopy & NuclStructure,Samarkand,USSR April 14,1981I.D.Fedorets et al

Nucl Instr&Meth 187,587(1981) K.Shinetal

Nucl Phys A367.419(1981) J.Eroe etal

Nuclear EnergyAgency reportNEANDC(E)-212U V5,p.37(1980)P.Plischkeetal

Consultants Mtg onNeutron SourceProperties.Debrec-hen.Hungary.INDC(NDS)-114/GT,p308(1980) M.A.Lone,B.CRobertson

capture,inelasticscattering

spallation,fission

inelasticscattering,direct reactions,precompound-nucleus emission

elasticscattering

knock-outreactions

recoils,energy spectra

spectraunfolding


neutron spectra


35

Table I (Cont .)

Co.Ni

27A1.12C56Fe18lTa

12C.14N16o

92Mo

27 Al

232Th

27Al,59Co58Ni

120Sn

K-Shell Ionisation of232xh by Protons andAlpha Particles

Pre-Equilibrium Emissionin Proton-Induced Reactionson Cobalt and Nickel inthe Energy Range 18-84 MeV

One, Two, Infinity: APragmatic Approach toNuclear PrecompoundReactions

Properties of QuasielasticKnockout of Slow Protons(E < or Approx. =10 MeV)From C, N, and O Nucleiby High-Energy Protons

Energy Dependence in ProtonInelastic Scattering

What Happens When A FastNucleon Goes Through ANucleus

Fission Probability ofthe Reaction 232Th(p,p'f)at E p = 52.5 MeV

Symmetric and AsymmetricComponents of EnergySpectra in a PreequilibriumDecay

Statistical MultistepDirect Emission in the120sn(p,n) Reaction

J of Physics B14,2391(1981)P.Hornshoj et al

FRNC-CONF-201, IntConf on Nucl Behav-ior at High AngularMomentum.Strass-bourg.Fr. April 22,1980SJ.Mills,FJ.Haasbroek

Nucl Phys A349.466(1980) H.C.Chiang,J.Huefner

Sov J Nucl Physics31,295(1980)A.A.Levkovskii,E.F.Dreiman

• Nucl Phys A352.221(1981)R.A.Moyeretal

Phys Lett B100,101(1981)E.F.Redish,D.M.Schneider

Acta Physica Aus-triaca 52,125(1980)G.Elder et al

INIS-MF-616Op.5OO30. Conf on NuclearSpectroscopy &Nucl. StructureLeningrad, March 18,1980, F.A.Zhivopistsevetal

Phys Lett B94.463(1980)L.Avaldietal

k-shell,ionization


inclusiveinteractions,precompound-nucleus emission

knock-outreactions,quasi-elasticscattering

elastic andinelasticscattering,optical models

mean free path

inelasticscattering



36

»8Ni

\1

54Fe208pb

232Th

93Nb

208pb

197 Au

Table I

Pickup in the Surface -The Origin of Deuteronsin Nuclear PrecompoundReactions

Excitation Functions of

(tau.t...) and (alpha.t...)-Reactions and Comparisonwith Results of ExcitonModel Calculations

Preequilibrium Emissionof Nucleons and AlphaParticles from 63Cu

Semimicroscopic Analysisof Direct Process Contri-bution to Proton InelasticScattering Spectra

Calculation of Proton-Induced Radioisotope Pro-duction Yields with aStatistical-Model BasedCode

Fission of 232xh atEnergies Up to 90 MeV

Multistep Direct ReactionAnalysis of AnalyzingPowers of Continuum Spectrain (p.alpha) Reactions

Analysis of PrecompoundProcesses in (p,n)Reactions with the Statis-tical Multistep DirectEmission Theory

Proton-Induced Pre-Equili-brium Alpha/Tau-EmissionforE(p) = 72MeV

( C o n t . )

Phvs Lett B97.183(1980)F.Hachenbergetal

Verhandlungen DerDeutschen Physik-alischen Gesell-schaft (E.Ger.)16,790(1981)M.Merkel,H.Muenzel

Verhandlungen DerDeutschen Physik-alischen Gesell-schaft(E.Ger.)16,791(1981)A.Alevra et al

YadFiz 30,1258(1979)A.I.Blokhin,V.G.Pronyaev

Int J of AppliedRadiation & Iso-topes 32,73(1981)R.Nowotny

Phvs Rev C24,180(1981) C.Chung,J.J.Hogan

Phys Rev £23,2769(1981)T.Tamuraetal

Phvs Rev C24.71(1981)R.Bonettietal

Helv Phys Acta 52,421,(1980) Z.Lewan-dowski et al

precompound-nucleus emission,pickup reactions

pickup reactions,exciton model


inelasticscattering

statistical models

evaporation modelspallation

three-nucleontransfer

charge-exchangereactions,precompound-nucleus emission

pickup reaction..

37

3e

^i

58Ni

27 Al209Bi58Ni

U9Sn208pb209Bi

232Th

238U

106Cd

6lNi

Table I

Improved Measurement ofNeutron Spectrum from35 MeV Protons on ThickBeryllium

Damage Analysis andFundamental StudiesQuarterly Report

Energy Dissipation Processfor lOQ-MeV Protons andthe Nucleon-Nucleon Inter-actions in Nuclei

Proton and Neutron Inclu-sive Spectra and theImportance of the SingleNucleon-Nucleon ScatteringProcess

Angular Distributions ofPre-equilibrium ReactionsWithin a GeneralizedExciton Model

Fissionability and ChargeDispersion Studies ofThorium by Protons ofEnergy to 90 MeV

Estimation of NeutronYield from IndividualFragments in Medium-Excitation Fission

Measurement of Compound-Nucleus Lifetime by X-RaySpectroscopy in the106Cd Reaction

Preequilibrium AngularDistributions in theQuasi-Free ScatteringModel

Systematics of Particle-Nucleus Reactions1. Parameters

(Con t . )

Medical Physics 8,396(1981)J.LUUmann et al

Battelle PacificNorthwest Labreport BNL-SA-9039(1980) R.H Jones

Phys Rev Lett 45,1930(1980)A.A.Cowley et al

Phys Rev Lett 46,226(1981)BJD.Anderson et al

NuclPhvsA337.445(1980)PMaedler,R.Reif

McGiUUniv.Montreal,QuebecThesis(1980)C.Chung

JNuclSci&Tech16,466(1979)H.Yamamoto et al

Nucl Phys A331.407(1979)J.F.Cheminetal

INIS-MF-5692 p.40, Annual Report1977-1978J.Bisplinghoff et al

Phys Rev £22,2116(1980) LWinsberg


physicalradiation effects

quasi-elasticscattering,impulseapproximation



precompound-nucleus emission,exciton model

fission fragments,neutron emission

inelasticscattering,x radiation

precompound-nucleus emission,inclusiveinteractions

fission,fragmentation,spallation,energy spectra

38

Table I (Cont.)

12C

12C

197 Au2"*Pb,L181Ta

165n0107 Ag

54,56Fe

12C, 14N160

181Ta

197 Au181Ta

209Bi54,56Fe

27 Al

12C(p,n)12N Reaction at99 MeV

Atomic-Excitation Effectson Nuclear Reactions

Study of K X-Ray NuclearSatellites from (p,xn)Reactions on Heavy Elements

Alpha Emission in ProtonInduced Reactions

Solution of Nuclear KineticEquations for Quasiequili-brium System and\ Descrip-tion of Energy Spectraof Secondary Nucleons

Cross Sections of the50 MeV Proton Reactionson the 12c, 14N, 1 6 O

Statistical Theory ofMulti-Step Compound andDirect Reactions

Measurement of the ProtonTotal Reaction Cross Sec-tion for 159Tb, 18iTa, and197Au Between 20 and 48 MeV

Quasiclassical Method ofNuclear Kinetic EquationSolution and Descriptionof Nucleon AngularDistributions

Proton-Induced Pre-Equili-brium Alpha-Emission atEp = 72 MeV

PhvsRevC22,1826(1980)J.N.Knudsonetal

Phys Rev Lett 45,703 (1980)E.J.Ludwig,E.Merzbacher

J of Physics G6,117(1980)V.Zoran et al

Zeit fur PhysikA293, (1979)A.Ferrero et al

Bull Acad SciPhys Series42,1893 (1978)V.E.Bunakov et a!

Bull Acad SciPhys Series43,148(1979)AJ.Vdovin et al

Annals of Physics125,429(1980)H.Feshbach et al

Nucl Phys A324,109 (1979) R.Abeggetal

Bull Acad SciPhys Series42,2351 (1978)V.E.Bunakov

Helv Phys Acta 52,88(1979)Z.Lewandowski et al


recoils

gamma cascades,k-shell, x-rayspectra

particle-holemodel, knock-outreactions

evaporationmodel,neutron spectra,time dependence

direct reactions

statisticalmodels,preequilibriumtheory

optical models



39

Table I (Cont.)

:,Cu,Fe

27 Al

27Al,9Be59Co,55Mn

24Mg

24c

5$>Co,Fe

40Ca

209Bi

165 H o

Production of Neutrons andPhotons from Thick TargetsBombarded by 52 MeV Protons

Momentum-Dependent StateDensities in the ExcitonModel

Proton Elastic Scatteringon Light Nuclei II.Nuclear Structure Effects

Proton Elastic Scatteringon Light Nuclei I. EnergyDependence

Calculation of Z GreaterThan or Equal to 3 Mass,Energy and AngularDistributions in thep + 12C Reaction

Measurement and Hybrid-ModelAnalysis of Proton-InducedReactions with V, Fe and Co

Penetration of SecondaryNeutrons and Photons froma Graphite Assembly Exposedto 52-MeV Protons

Nucleon Optical Potentialfrom a Realistic Inter-nucleon Potential

(p,n) Reaction on 209Biand Pre Compound Processes

Preequilibrium and Equilib-rium Deexcitation Processesfor Dy(alpha,xn gamma)ErReactions at E aipha = 90MeV and 165Ho(p,xnyp gamma)Reactions at En = 60 MeV

2. Symp AcceleratorSci & Tech.,Tokyo,Japan,p.l97(1978)K.Shin et al

Dresden Univ (E.Germany) reportZFK-376,p.,l 1(1978)P.Maedler, R.Reif

Phvs Rev C21,844(1980)E.Fabricietal

Phvs Rev C21.830(1980)E.Fabricietal

Univ. Marylandreport ORO-5172-14,p.46(1979)A.Goekmen et al

Nucl Phys A322.40(1979) R.Micheletal

Nucl Sci & Eng 71.294 (1979) K.Shinetal

J Phys Soc Japan44.539(1978)F.Brieva, JR.Rook

J Phys Soc Japan45,1071(1978)K.Miyano et al

J Phys Soc Japan44,655(1978)H.Ejiri et al

secondaryemission


optical models

optical models

evaporationmodel,nuclear cascades


fast neutrons,gamma radiation

nucleon-nucleonpotential


neutron spectraprecompound-nucleus emission

40

Table I (Coat.)

JSUUSi

197 A u

9Be

Sn.TiW,Y

27 Al165Ho

Gd,Th

Cu,EuAg

79,8 l B r

56F e

Asymmetry in the Elasticand Inelastic Scatteringof 65 MeV Protons from 28si,29si,30si,3ip,89Yand90Zr

Fissionability of Nuclidesin the Thorium Region atExcitation Energiesto 100 MeV

Preequilibrium Alpha-Emission in the 197 Au(p.alpha x)-Reaction atEp = 72 MeV

Neutron Spectra from 35 and46 MeV Protons, 16 and 28MeV Deuterons, and 44 MeV3He Ions on Thick Beryllium

Contribution to the Studyof Ionization of Elementsby Protons and AlphaParticles of 4 to 30 MeV

Measurement and Analysisof Continuous AlphaSpectra in Proton InducedReactions

Relativistic Effects in K-Shell Ionisation by 7-15MeV Proton Bombardmenton Heavy Elements

Atomic K-Shell IonizationInduced by 20-50 MeVProtons

79Br and 8lBr(p,xn) and(p.pxn) Excitation Func-tions in the EnergyRange 10-85 MeV

Gamma-Ray Production CrossSections

J Phys Soc Japan44,557(1978)M.Nakamura et al

Phys Rev C20.1831(1979)JJ.Hoganetal

Phys Lett B80.350 (1979)Z.Lewandowslti et al

Medical Physics 6,432 (1979)F.M.Waterman et al

Nucl Instr & Meth159.455(1979)M-Poncet,Ch-Engelmann

C:>nf on Clustering\sp xts of Nuclear?


1* B,' lC Radiative-Emission Spec-^^Si trum of 50-MeV Nuclear

Excitations Populatedby Proton Capture

165Ho Gamma Rays and NeutronsFollowing Preequilibriuml65Ho(p,xnp gamma) Reac-tions at Ep = 60 MeV

208pb Simple Unitary Estimatefor Multistep Processes

27 Al Charged-Particle Spectra:58Ni 90 MeV Protons on 27Al,90zr 58Ni,90zr,and209Bi

12c Cross Section of 50 MeV14N Proton Reactions on 12C,

14N, 16O Nuclei withEscape of Four ChargedParticles

208pb Integral Contribution ofDirect Processes InelasticScattering Spectra and thePreequilibrium Decay Model

Ni Proton-Induced Reactionson Nickel with EnergiesBetween 12 and 45 MeV

12C, 14N Cross Sections of 50 MeV160 Proton Induced Reactions

on 12C, 14N,and 160Nuclei with Three ChargedParticles in the Final State

54Fe Study of Two-Particle65Cu Nuclear Reactions in

Framework of theExciton Model

C,Cu, Spectral Measurements ofPb.Fe Neutrons and Photons from

Thick Targets of C, Fe, Cuand Pb by 52 MeV Protons

Phys Rev Lett 42,1253 (1979)L.G.Arnold

Nucl Phys A305,167 (1978) H.Ehirietal

Phys Rev C19.693(1979) S.R.Cotanch

Phys Rev C19.698(1979)J.R.Wuetal

INIS-MF-4388p.l39(1978) 28. Conf NuclSpec & Structure AtomicNucleus Alma-Ata,USSRA.I.Vdovin et al

INIS-MF-4468 pp.130-134 (1977) 4thAll-Union ConfNeutron PhysicsA.I.Blokhin et al

Zeit fur PhysikA286,393(1978)R.Michel et al

Sov J Nucl Phys27,3 (1978)I.G.Golikov et al

UkrPhysJ22,2021(1977) S.N.Ezhov, V.A.Plyuyko

Nucl Instr & Meth151,493(1978)T.Nakamura et al

gamma spectra

precompound-nucleus emission,gamma spectra

pk-,ip reactions


precompoundnucleus emission


breakup reactions

compound-nucleusreactions,inelasticscattering

neutron spectra

42

Table I (Cont . )

«Fe

I81ia

Li

40Ca

56Fe209Bi

Ni,Nb

7Li

27 Al209Bi197 Au

54Fe

Cascade-Exciton Model forNuclear Reactions

Neutron Spectra and Angu-lar Distributions from theReactions l8lTa(p,n)181W.and 18lTa(n,n')18lTa

Neutron Spectra from Deu-4eron and Proton Bombard-ment of Thick LithiumTargets

Two-Step Processes in In-elastic Proton Scattering

Use of the IntranuclearCascade Model for IncidentNucleons of Intermediateand Low Energy

Calculation of EnergySpectra of PrimaryKnock-On Atoms in theProton Elastic Scat-tering by the Nuclei ofDifferent Elements

Neutron Spectra from Deu-teron and Proton Bom-bardment of Thick LithiumTargets: Potential forNeutron Therapy

Complex-Particle Emissionin the Pre-EquilibriumExciton Model

Multi-Jtep-Direct-ReactionAnalysis of ContinuumSpectra of (p,alpha)Reaction

Pre-Equilibrium Emission

Dresden Univ (E.Germany) reportZFK-324,p.79(1976)K.K.Gudima,V.D.Toneev

Sov J Nucl Phys26,606(1977)N.S.Biryukovetal

Brookhaven reportBNL-NCS-125(1977)C.E. Nelson et al

Zeit fur PhysikA284.413(1978)E.F.Hefter

Phys Lett 73,267(1978) VJE.Bunakovetal

Kharkov Physics-Tech. Instit.(Ukraine) reportFTI-76-45,p.29 (1976)B.A.Shilyaev et al

Phys in Medicine &Biology 23,39(1978)C.E .Nelson et al

Phys Rev £17,1540(1978)J.R.Wu,C.C.Chang

Phvs Lett B71,273(1977)T.Tamura,T.Udagawa

Nucl Instr & Meth146.265O977)E.Gadioli, E.E.Gadioli

direct reactions,precompound-nucleus emission,nuclear cascades

neutron spectra,precompound-nucleus emission

energy spectra

multiplescattering

nuclear cascades

optical models

fast neutrons


pickup reactions

precompound-nucleus emission,excitons

43

140Ce24Mg64Zn66,682n

88S r89Y90Zr

209Bi54Fe

27 Al56FeSi,S

14N.16O

Cs

89y

15N40Ca

6.7Li9Be

197 Au

Table I

Measurements of the ProtonTotal Reaction CrossSection for 24fvtg, 64,66,68zn and 140Ce Between17.5 and 48 MeV

Pree^uilibrium Decay ofNuclei with A Approx. =90 at ExcitationEnergies to 100 MeV

A-Priori Pre-EquilbriumDecay Models

Empirical ObservationsAbout the Nucleon OpticalModel Potential

Optical Model and ProtonElastic Scattering from14N and 16o

Proton Loss by NuclearInelastic InteractionsinCsI(Nel02,Ne213and Stilbene

Influence, of Nucleon Mean-Free Paths on IntranuclearCascade Results

Influence of RecoilEffects in the Micro-scopic Description inInelastic Scattering

Study of the (p,pn)Reaction in LightNuclei

Compact Modified ExcitonModel for the Pre-Equili-brium Decay of HighlyExcited Nuclei

( C o n t . )

Nucl Phys A290.45(1977)N£.Davisonetal

Phys Rev C16.1404(1977) E.Gadiolietal

Nukleonika 19,183(1974)M.Blann

Phys Lett B20.U1(1977)J.Rapaport

AustJ Physics 30,287(1977) A.Gabric,K.Amos

Nucl Instr & Meth143.589(1977)A-M.Sourkes et al

Phys Lett 868,405(1977)J.Ginocchio,M.Blann

Phys Lett §69,261(1977)HJ>.Blok,P.D.Kunz

Nucl Phys A28L418(1977)C.N.Waddelletal

Kernenergie 20,180(1977)P.Maedler

total crosssections


precompound-nucleus emission,nucleon-nucleoninteractions



plasticscintillatorsinelasticscattering

inelasticscattering,nuclear cascades,nuclear matter

inelasticscattering,recoils

impulseapproximations,knock-outreactions.breakupreactions


44

?Be,7Li

64,66zn68,70zn

27 Al209Bi

Al,BeCd,C,CuAu,Fe

12C.MN

7Li,9Be

Table I

Thick Target Neutron Yieldsand Spectral Distributionsfrom the 7Li(d(p),n) and9Be(d(p),n) Reactions

Compound and PrecompoundProcesses in (p.p1)and (alpha,p) Reactionsof Even Zn Isotopes

Deep Inelastic ReactionsTreated as Multi-StepDirect Reaction Processes.Application to (p.p1)Reaction

Study of the Pure Continuumin Inelastic ProtonScattering

Energy Spectra of RecoilAtoms While IrradiatingDifferent Elements byFast Protons and Neutrons

Deuteron Break-Up Effectsin (p,d) Reactionsat 65 MeV

Description of SecondaryNuclear Energy SpectraProduced in Low and Inter-mediate Energy ProtonInteraction with Nuclei

Physical Characterizationof Neutron Beams Producedby Protons and Deuteronsof Various Energies Bombard-ing Beryllium and LithiumTargets of Various Thickness

( C o n t . )

Nucl Instr & Meth143.331(1977)M. A.Lone et al

NuclPhysA277.413(1977)C.R.Lux,N.T.Porile

Phys Lett 866,109(1977)T.Tamuraetal

Verhandlungen derDeutschen Physik-alischen Gesell-schaft 6,1016(1977)C. Alderliesten et al

INIS-MF-3329 p.393(1976) 26. Conf NuclSpect & NuclStructure, Baku,USSR, Feb 3 1976B.A.Shilyaev et al

Nucl Phys A274,168(1976) CL.Wales,R.CJohnson

28th Conf on NuclSpect & Struct ofthe Atomic Nucleus,Alma-Ata,USSR,1978,INIS-MF-4388,p.277V.E.Bunakov et al

Medical Physics 4,486(1977) H.I.AmoIsetal

direct reactions.neutron spectra


inelasticscattering,direct reactions

inelasticscattering,quasi-freereactions

elasticscattering,recoils

pickup reactions

nuclear cascades

energy spectra

45

9Be

Cd

208pb

U

18lTa

75As

90zrl20sn208pb48 C a

Table I

Neutron Beams Generated byProtons on Beryllium

Excitation Functions of the(pn) and (p,2n) Reactions onCd Isotopes

Measurement of Lithium,Beryllium and Boron StableIsotope Production Cross Sec-

(Con t . )

BritJ of Radiol-ogy (Eng) 49,587(1976) S.WJohnsenetal

Bull Acad SciPhys Series(USSR) 19,24(1975)E.A.Skakun et al

Paris Univ. Orsay,Thesis, CSNSM-T-75-02(1975)P.Fontes

neutron beams

charge-exchangereactions,knock-outreactions

spallation

tions in Carbon-Spallation byProtons and Alpha Particles.Application to the Study ofthe Propagation of the LightElements in Cosmic Rays

Cross Sections and ReactionMechanisms of (p,pxn) Reacti-ons on 208pb in the 24-52 MeVRange

Relative Mass Yields in ProtonInduced Fission on NaturalUranium from Delayed GammaRays Analysis

Nature of a K X-Ray SatellitePeak as Determined from theAnalysis of FluorescenceSpectra Induced by 20-50 MeVProtons

Pre-Equilibrium StatisticalModel: Comparison of Calcu-lations with Two (p,xn)Reactions

Preequilibrium Analysis of(p,n) Spectra on Various Tar-gets at Proton Energies of 25to 45 MeV

Nucl Phys £262,52(1976) H.Kawakamietal

Revue Roumaine dePhysique 21,69(1976) A.Calboreanuetal

JofPhysC&Leg(1976)CP.Randelletal

J Inorg Nucl Chem38,1581(1976)J.C.Brodovitchetal

Nucl Phys A257,15(1976) M.Blannetal

knock-outreactions

delayed gammaradiation

knock-outreactions,x-radiation


precompound-nucleus emissiongamma spectra

46

56Fe103Rh

12C.6L19Be

48Ca,90Zr120sn208pb

6JLi9Be,12C27 Al

103Rh159-n,169rm

27A1.CCu

48Ca208pb

Be,B12C

90zr

75A s115in

T a b l e I

Generalized Exciton Model forthe Description of Preequili-brium Angular Distributions

Study of the (p.pn) Reactionon lp Shell Nuclei at 46 MeV

Analysis of the PreequilibriumAngular Distributions in the45-MeV (p,n) Reaction

Production of Medium-EnergyNeutrons from Proton Bombard-ment of Light Elements usingRevised Neutron-ProtonDifferential Cross Sections

Comparison of Proton and Neu-tron Spectra. The ExtendedGriffin Model, Pairing andIsospin

Distributions of SecondaryParticles Around Various Tar-gets Exposed to 50 MeV Protons

Pre-Equilibrium Model Evalua-tion of Neutron Spectra fromProton-Induced Reactions

Comparison of Measured NeutronSpectra with Predictions of anIntranuclear-Cascade Model

Li, Be, and B Production inReactions of 45-100 MeV Pro-tons with 12C: AstrophysicalImplications

Charged-Particle Emission inReactions of 90zr with 10-86MeV Protons

Excitation Functions and Iso-meric Yield Ratios of (p,xn)Reactions Induced in 75 As andand 115ln bv 20-85 MeV Protons

( C o n t . )

Zeit fur PhysikA276.145(1976)CMantzouranis et al

Manitoba Univ,Thesis, CTOM-20405(1974)C.AMUer

Phys Rev C 14,2018(1976)G-Mantzouranis

Nucl Instr Meth134.537(1976)J.L.Romeroetal

Zeit fur PhysikA275.175(1975)C.Kalbach et al

Nucl Instr Meth133.213(1976)A.Fasso, M.Hoefert

Phys Rev £14,573(1976) E.Gadiolietal

Phys Rev C14,748(1976) A.Galonskyetal

Phys Rev CJ4,4101976) C.T.Rocheetal

Phys Rev C 14,64(1976)M.V.Kantelo,JJ.Hogan

McGiil Univ(Canada) ThesisCTOM-18162(1973)J.C.Brodovitch

precompound-nucleus emission,neutron spectra

knock-outreactions


neutron sources


spallation

charge-exchangereactions,precompound-nucleus emission,neutron spectra

Monte Carlomethod,neutron spectra,nuclear cascades

spallation


Monte Carlo method

47

2C

;8Ni

208pb

40Ca208pb16o

WlTaH5Sn181W

238U

Table I

Optical Model Analysis of Pro-ton-Carbon Elastic Scatteringin the Range 20 to 50 MeV

Charged Particle Spectra from100 MeV Protons on 58Ni

Alpha-Emission by PrecompoundMechanism in Heavy Nuclei

Quasi-Free Scattering Modelfor Nuclear Reactions in theContinuum

Cross Sections of (p,pxn)Reactions on 2u8pb

Proton Total Reaction CrossSections for the Doubly MagicNuclei 16o, 40Ca, and 208pb inthe Energy Range 20-50 MeV

Angular Distribution ofNucleons in Nucleon-InducedPreequilibrium Reactions

Proton and Deuteron Fission of238tj

Radiation Heating of MaterialsDuring Irradiation withCharged Particles

(Gont . )

Zeit fur PhysA274.339(1975)R.Sprickmann et al

Univ of Marylandreport ORO-4856-26 p.360(1975)J.R.Wuetal

Julich reportJUL-CONF-16,Vl,p.85(1975) Conf onHighly ExcitedStates of NucleiL.Milazzo-Collietal

U of Rochester,N.Y.Thesis(1975)A-L.CMignerey

Tokoyo Univ reportNP-20526p.54(1974)J.CRasmussen et al

Phys Rev CJ2.1167(1975) R J.Carlsonetal

Phys Lett B57,220(1975)CMantzouranisetal

Egypt J Chem, SpecIssue pp. 1-7(1974)A.T.Kandil,CR.Choppin

Izv Akad Nauk KazSSR 6,84(1974)S.S.Ibragimov et al

elasticscattering

energy spectra,precompound-nucleus emission

heavy nuclei,precompound-nucleus emission

heavy nuclei,intermediatemass, quasi-free reactions

compound-nucleusreactions

optical models

angulardistribution,heavy nuclei,intermediate massnuclei.precom-pound nucleusemission

fission

radiation heating

48

«Si

27A1.12C

209Bi12c,54Fe

27Al,9BeC

Al

56Fe>58Ni

Tab le I

Energy Dependence of ProtonDamage in Silicon

COMPD: A Computer Program forthe Calculation of theExcitation Functions byMeans of Monte Carlo Method

A Technique for MeasuringProton Total Reaction CrossSections at Medium Energies

Energy Distributions ofCharged and Neutral HydrogenAtoms Backscattered fromMetal Surfaces Bombardedwith 5 to 18 MeV Protons

Optical Model Analysis of Pro-ton and Deuteron Scattering andDWBA Calculations on (p,d)-Reactions at 185 MeV

Comparisons of Predictions fromTwo Intranuclear-Cascade Modelswith Measured Secondary ProtonSpectra at Several Angles from62- and 39-MeV Protons onVarious Elements

Measurements of the ProtonTotal Reaction Cross Sectionfor Light Nuclei Between20 and 48 MeV

Effect of High-Energy Protonson Mechanical Properties ofAluminum

Gamma Rays Observed from 100-MeV Protons Interacting with56Fe and 58Ni

(Con t . )

Izv Akad Nauk KazSSR 6,50(1974)Ai\Akkerman et al

Tokoyo Univ reportINS-TCH-10(1974)K.Komura, S.Tanaka

Nucl Instr Meth123.509(1975)R.F.Carlson et al

Max Planck Institreport IPP-9/18(1975)P.Meischner,H.Verbeek

PhysScripta 10,159(1974)A.Ingemarsson,G.TibeU

Phys Rev £10,2472(1974)H.W.Bertinietal

Phys Rev 00,2237(1974)W.F.McGill

Fiz Khim ObrabMater 5,151(1974)G.G.Bondarenko,L.Uvanov

Phys Rev Lett 33,1493(1974)C.C.Chang et al

elastic scattering,physical radiationeffects

compound-reactions,evaporationmodel,Monte Carlomethod

elastic scattering

radiation effects

optical models,pickup reactions

energy spectra,inelasticscattering,nuclear cascades,precompound-nucleus emission

total crosssections

dislocations,physical radiation


49


209Bi Reactions on 209BJ Induced byIntermediate Energy Protonsand the Effect of DirectReactions

NuelPhvsA230.98(1974) K.Miyanoetal

direct reactions,precompound-nucleus emission

181Ta

Monte Carlo Programs forCalculating Three-DimensionalHigh-Energy (SOMeV-SOOGeV)Hadron Cascades in Matter

Analysis of (particle,xn) Reac-tions on Tantalum and Gold. I.18lTa(alpha,xn) ExcitationFunctions Up to 104 MeV andEquilibrium Statistical ModelAnalysis

Comput Phys Commun7,327(1974)J .Ranft, J.T.Routti

Nucl Phys A228,165(1974) F.Hermesetal

charged-particletransport, MonteCarlo method,neutron transport

gamma spectra,Monte Carlomethod

2O8pb

209Bi12C

56Fe'18lTa

209Bi

6L1.12C9Be

Periodic Dependence of GaussianElectronic Stopping CrossSection with Energetic Ions inSolid Targets

Effects of Irradiation-InducedDefects on the MechanicalProperties of Tungsten

Optical-Model Analysis of p +208pb Elastic Scattering from15-1000 MeV

Comparisons of Predictions fromTwo Intranuclear-Cascade Modelswith Measured Secondary ProtonSpectra at Several Angles from62- and 39-MeV Protons onVarious Elements

De-Excitation by StatisticalPre-Equilibrium AlphaEmission

A-Priori Pre-Equilibrium DecayModels

(p.pn) Reactions on LightNuclei at 46 MeV

Jap J Appl Phys13,393(1974)K.Kanaya, K.Hojou

U of PittsburghThesis(1973)C.S.Reft

Phys Rev £10,307(1974)W.TH.Van Oers et al

Oak Ridge reportORNL-TM-4638(1974)H.W.Bertini et al

Univ Lyon reportLYCEN-7347(1973)Thesis, N.Chevarier

Nukleonika 19,183(1974)M.Blann

Phys Rev Lett 32,684(1974)C.A. Miller etal

charged-particletransport,electron-ioncollisions,stopping power

dislocations,radiation effects

optical models

nuclear cascades,quasi-elasticscattering

nuclear cascades,precompound-nucleus emission

nucleon-nucleoninteractions,precompound-nucleus emission

knock-outreactions,quasi-elasticscattering

50

Table I (Cont.)

:u

15Sc

7y

209Bi54Fe

Cu

H

Bi197 Au

HOHf181Ta168Yb

Shielding from Neutrons Gener-ated in Targets by a Beam ofI GeV Protons

Charged Particles Produced inthe Bombardment of 45Sc by 45MeV Protons

Fast Forward Neutron Produc-tion in the 7lj(p,n)7BeReaction for 41- and 64 MeVProtons

A Priori Pre-Equilibrium DecayModels

Complete Hydrogen and HeliumParticle Spectra from 30- to60-MeV Proton Bombardment ofNuclei with A = 12 to 209 andComparison with 'he Intra-nuclear Cascade Model

Spallation of Copper by 65-MeYPi+ and Pi- and by 205-MeVProtons

Gold L X-Ray Production by 0.5to 30-MeV Protons

X-Ray Emission FollowingNuclear Reactions

De-Excitation of Even-EvenIsotopes of Yb.Hf, and WProduced in (p,xn gamma)Reactions

Tr Radiotekh Inst9,117(1972)B.V.Man'ko, B.S.Sychev

U of S CalifThesis(1973)H.Spitzer

Nucl Instr Meth113,185(1973)J.W.Wachteretal

Nucl Phvs A213.570(1973) M.Blann

Phys Rev C8,1045(1973)F.E.Bertrand,R.W.Peele

Phys Rev £8,594(1973) CXGarrett,A.L.Turkevich

Phys Rev A7.566(1973)S.M.Shafroth et al

Phys Rev Lett 30,863(1973)CDeconninck,N.Longequeue

J Phys (Paris) 34,345(1973)C.Birattari et al

shielding

reactionmechanisms,DWBA,compound-nucleusreactions.pickupreactions


nucleon-nucleonpotential,optical models

heavy nuclei,light nuclei,nuclear cascades

Nuclear cascades

emission spectrahydrogen ions,x-ray spectra

x-ray spectra

compoundnucleusreactions,gamma radiation

51

u

rLi

160Gd169Tm

12CS8,60Ni

C.27A159Co

Cu

197 Au54Fe

24Mg28Si

Table I

High-Energy Neutrons Producedby 740-MeV Protons on Uranium

Characteristic L X-Ray Spectrafrom Proton, Alpha-Particle,and Oxygen Bombardment of Sn

Fast Forward Neutron Productionin the 7Li(p,n)7Be Reactionfor 41- and 64-MeV Protons

Reaction Mecha

bibliographic survey of medium energy inclusive reaction data · 208pb,h8sn 27 al,cu experimental...

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