to join as much as possible of the brazilian scientific and technological production in atomic,...
DESCRIPTION
International goals To offer to the nuclear fusion community, in a global scale, a channel for a direct, easy and rapid access to the brazilian scientific production in AMPP To strenght the worldwide insertion of brazilian AMPP data into the literature.TRANSCRIPT
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• To join as much as possible of the brazilian scientific and technological production in atomic, molecular and plasma physics that may be of interest to nuclear fusion research
BRAMPDAC´s main objectives:
• To provide a direct, easy and rapid access to these data via the web
• To promote, as much as possible, data exchange between the brazilian atomic, molecular and plasma physics communities
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International goals• To offer to the nuclear fusion
community, in a global scale, a channel for a direct, easy and rapid access to the brazilian scientific production in AMPP
• To strenght the worldwide insertion of brazilian AMPP data into the literature.
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A broad-interest data center • Spectroscopic data for atoms (energy
levels, transition rates) and molecules (energy levels, rotational, vibrational, ionization and dissociation parameters, transition rates)
• Collisional data for electron (ion) – atom (molecule) collisions (elastic, rotational, vibrational and electronic excitation, ionization and dissociation cross sections)
• Plasma characterization: data on particle densities and local temperatures
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Selected examples of
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TCS for Li ionization by H+ and He2+
Fiori et al., PRA 64, 012705 (2001)
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TCS for Li ionization by H+ and He2+
Fiori et al., PRA 64, 012705 (2001)
TCS for ionization out of the Li 1s orbital by H^+ impact
Authors: M R Fiori, G Jalbert, C E Bielschowsky and W Cravero,Phys. Rev. A 64, 012705 (2001)
E(keV) TCS(10^-16 cm^2)11.080 1.4392(-4)14.565 6.9272(-4)26.947 6.7036(-3)59.151 5.7743(-2)164.94 1.4652(-1)475.91 1.0953(-1)1744.4 4.3164(-2)
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TCS for multi-ionization of Ne by He+
E(Mev) Ne+ Ne2+ Ne3+
1.00 116±17 15±2 2.4±0.6
1.50 76±11 8.3±1.3 0.86±0.22
2.00 82±12 7.5±1.2 0.80±0.20
2.50 64±10 5.3±0.8 0.50±0.13
3.00 69±10 4.9±0.8
3.50 66±10 4.4±0.7
Santos et al., PRA 63, 062717 (2001)
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TCS for multi-ionization of Ar by He+
E(Mev) Ar+ Ar2+ Ar3+
1.00 229±34 30±5 6.1±1.2
1.50 206±31 21±4 2.3±0.5
2.00 162±24 17±3 2.4±0.5
2.50 132±20 11±2 1.7±0.3
3.00 134±20 8.5±1.4 1.5±0.3
3.50 108±16 9.1±1.5 1.3±0.3
Santos et al., PRA 63, 062717 (2001)
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TCS for multi-ionization of Kr by He+
E(Mev) Kr+ Kr2+ Kr3+
1.00 262±39 47±8 14±2
1.50 179±27 23±4 9.1±1.6
2.00 159±24 23±4 9.2±1.7
2.50 137±21 18±3 9.4±1.7
3.00 133±20 14±2 5.8±1.0
3.50 123±18 12±2 4.7±0.8
Santos et al., PRA 63, 062717 (2001)
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TCS for multi-ionization of Xe by He+
E(Mev) Xe+ Xe2+ Xe3+ Xe4+
1.00 290±44 41±7 15±3 10±2 1.50 219±33 32±5 14±3 6.1±1.3 2.00 175±26 27±5 11±2 5.0±1.0 2.50 168±25
27±5 10±2 4.9±1.0
3.00 146±22 24±4 10±2 4.3±0.9 3.50 132±20 20±3 8.2±1.6 4.7±1.0
Santos et al., PRA 63, 062717 (2001)
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Single-ionization cross sections of He by He+
Santos et al., PRA 63, 062717 (2001)
Single-ionization cross sections of He by He^(+)
Authors: A. C. F. Santos, W. S. Melo, M. M. Sant´Anna, G. M. Sigaud, and E. C. Montenegro, Phys. Rev. A, 63, 062717 (2001)
Energy (MeV) SICS (Mb) 1.00 881.25 701.50 662.00 562.50 453.00 383.50 33
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Double-ionization cross sections of Ar by He+
Double-ionization cross sections of Ar by He^(+)
Authors: A. C. F. Santos, W. S. Melo, M. M. Sant´Anna, G. M. Sigaud, and E. C. Montenegro, Phys. Rev. A, 63, 062717 (2001)
Energy (MeV) DICS (Mb) 1.00 30 1.50 212.00 172.50 113.00 8.53.50 9.1
Santos et al., PRA 63, 062717 (2001)
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TCS for single electron capture
from H and H2 by He2+ impact
Sant´Anna et al., PRA 61, 052717 (2000)
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TCS for single electron capture from H by He2+
Sant´Anna et al., PRA 61, 052717 (2000)
TCS for single electron capture from H by He^(2+)
Authors: M. M. Sant´Anna, W. S. Melo, A. C. F. Santos, V. L. B. de Jesus, M. B. Shah, G. M. Sigaud, E. C. Montenegro, H. S. Busnengo, S. E. Corchs, R. D. Rivarola, and L. Gulyás, Phys. Rev. A, 61, 052717 (2000)
Energy (keV) TCS (10^(-16) cm2) 500 2.83 (-1) 750 5.61 (-2)1000 1.96 (-2)1250 1.00 (-2)1500 4.93 (-3)1750 2.57 (-3)2000 1.37 (-3)2250 8.90 (-4)2500 5.05 (-4)
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TCS for single electron capture from H2 by He2+
Sant´Anna et al., PRA 61, 052717 (2000)
TCS for single electron capture from H2 by He^(2+)
Authors: M. M. Sant´Anna, W. S. Melo, A. C. F. Santos, V. L. B. de Jesus, M. B. Shah, G. M. Sigaud, E. C. Montenegro, H. S. Busnengo, S. E. Corchs, R. D. Rivarola, and L. Gulyás, Phys. Rev. A, 61, 052717 (2000)
Energy (keV) TCS (10^(-16) cm2) 500 7.37 (-1) 750 2.02 (-1)1000 5.96 (-2)1250 2.68 (-2)1500 1.09 (-2)1750 5.24 (-3)2000 3.21 (-3)2250 1.95 (-3)2500 1.03 (-3)2750 7.50 (-4)
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Selected examples of
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DCS for vibrational excitation of H2 by electron impact
Mazon et al., PRA 64, 042705 (2001)
v=0 → v´=1
v=0 → v´=0
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DCS for vibrational excitation of H2 by electron impact
Mazon et al., PRA 64, 042705 (2001)
Differential cross sections for (v=0 --> v´=1) vibrational excitation of H2 by 2.5 eV electron impact
Authors: K T Mazon, R Fujiwara and M.-T. Lee, Phys. Rev A 64,42705 (2001)
Ang(deg) DCS(10^(-16) cm^2/sr)0.2423 6.8263(+0)2.9871 5.0799(+0)5.9481 2.7946(+0)8.9126 1.5272(+0)1.1884 2.2359(+0)1.4922 4.0821(+0)1.7956 5.0301(+0)
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Mazon et al., PRA 64, 042705 (2001)
v=0 → v´=3
v=0 → v´=2
DCS for vibrational excitation of H2 by electron impact
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Mazon et al., PRA 64, 042705 (2001)
DCS for vibrational excitation of H2 by electron impact
Differential cross sections for (v=0 --> v´=3) vibrational excitation of H2 by 3.5 eV electron impact
Authors: K T Mazon, R Fujiwara and M.-T. Lee, Phys. Rev A 64,42705 (2001)
Ang(deg) DCS(10^(-16) cm^2/sr)0.30009 4.5628(+0)30.252 3.8383(+0)59.505 2.3953(+0)89.453 1.5989(+0)89.453 1.5989(+0)117.54 2.3119(+0)147.64 3.7789(+0)179.65 4.5989(+0)
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ICS for electronic excitation of H2 by electron impact
X1Σg+ → b3Σu
+ X1Σg+ → a3Σg
+ X1Σg+ → c3Πu
Machado et al., PRA 63, 032707 (2001)
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ICS for electronic excitation of H2 by electron impact
Machado et al., PRA 63, 032707 (2001)
ICS for the X^1\Sigma_g^+ --> b^3\Sigma_u^+ excitation of H2 by electron impact
Authors: A. M. Machado, M. M. Fujimoto, A. M. A. Taveira, L. M. Brescansin and M. -T. Lee, Phys. Rev. A 63. 032707 (2001)
E(eV) ICS(10^-16 cm^2)15.0 1.41(+0) 17.5 1.22(+0)20.0 1.07(+0) 25.1 8.05(-1) 30.2 5.70(-1) 35.3 4.06(-1) 40.0 3.09(-1)
X1Σg+ → b3Σu
+
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DCS for electronic excitation of H2 by electron impact
X1Σg+ → b3Σu
+ X1Σg+ → a3Σg
+ X1Σg+ → c3Πu
Machado et al., PRA 63, 032707 (2001)
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ICS for vibronic excitation of H2 by electron impact
Lee et al., J. Mol. Struct. (THEOCHEM) 394, 127 (1997)
X1Σg+ (v=0)→ C1Πu (v´=0,1,2,3)
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GOS for vibronic bands in the CO molecule
Rocha et al., PRA 57, 4394 (1998)
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Fragmentation of water by heavy ions
H Luna and E C Montenegro, PRL 94, 043201 (2005)
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Fragmentation of water by heavy ions
H Luna and E C Montenegro, PRL 94, 043201 (2005)
TCS for production of H2O^+ from fragmentation of H2O
by C^(3+) impact
Authors: H Luna and E C Montenegro, Phys Rev Lett 94,043201 (2005)
E(keV/amu) TCS(10^(-18) cm^2)
81.250 4.4789(+2)126.56 3.8451(+2)168.75 1.9859(+2)209.38 1.0141(+2)251.50 1.0986(+2)293.75 1.3944(+2)
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Fragmentation of water by heavy ions
H Luna and E C Montenegro, PRL 94, 043201 (2005)
TCS for production of H^+ from water fragmentation induced by the ionization channel, by O^(5+) impact
Authors: H Luna and E C Montenegro, Phys Rev Lett 94, 043201 (2005)
E(keV/amu) TCS(10^(-18) cm^2)
62.680 1.0791(+2)125.37 2.5036(+2)155.22 2.8921(+2)
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TCS for e--C2H4 scattering
Brescansin et al., JPB 37, 471 (2004)
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TCS for e--C2H4 scattering
Brescansin et al., JPB 37, 471 (2004)
Total cross sections for e^- - C2H4 scattering
Authors: L M Brescansin, P Rawat, I Iga, M G P Homem, M.-T. Lee and L E Machado, J. Phys. B: At Mol Opt Phys 37, 471 (2004)
E(eV) TCS(10^(-16) cm^2)10.137 3.0337(+1)16.569 2.7708(+1)32.340 2.0629(+1)54.321 1.6382(+1)93.768 1.2135(+1)195.94 7.6854(+0)495.65 4.0449(+0)
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TACS for e--C2H4 scattering
Brescansin et al., JPB 37, 471 (2004)
Total absorption cross sections for e^- - C2H4 scattering
Authors: L M Brescansin, P Rawat, I Iga, M G P Homem, M.-T. Lee L E Machado, J. Phys. B: At Mol Opt Phys 37, 471 (2004)
E(eV) TACS(10^(-16) cm^2)10.000 1,3333(-1)17.262 1,3333(+0)31.901 3,8667(+0)55.068 5,1556(+0)92.497 5,0667(+0)185.53 3,2889(+0)495.65 1,2889(+0)
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Selected examples of
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Particle confinement in plasmas
Daltrini and Machida, Rev. Sci. Instrum. 76, 053508 (2005)
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ICS for superelastic e--H2 scattering
Sartori et al., PRA 55, 3243 (1997)
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Transition rates for molecular excitation Ki→f(T):
•μ : electron-molecule reduced mass•σ : cross section for the i→f transition•f(E) : electron energy distribution function
Sartori et al., PRA 58, 2857 (1998)
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Transition rates for electronic excitation of H2
Sartori et al., PRA 58, 2857 (1998)
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Electron energy distribution function in an H2 column
Amorim et al., Chem. Phys. 246, 275 (1999)
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Fast neutral Li beam as a probe of the edge region in
ETE
Oliveira et al., Rev. Sci. Instrum. 75, 3471 (2004)
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BRAMPDAC: present status• More than 1000 electronic data files
prepared, catalogued and stored• Extensive and diversified data in the
area of electron-molecule collisions• Also diversified (not so extensive) data
on electron (ion)-atom collisions and on atomic and molecular spectroscopy
• Still a very small amount of plasma physics data.
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BRAMPDAC: near-future developments
• More agressive “in loco” search for spectroscopy and plasma physics data.
• Talks in national meetings on theoretical chemistry and plasma physics to strengthen BRAMPDAC in these areas
• BRAMPDAC on the web: not yet available. A site for BRAMPDAC, to be set as a mirror site of IAEA data basis site, is expected for soon.
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Acknowledgments• Evandro M S Ribeiro, Andréa M M
Ribeiro and Maíra Machado, BRAMPDAC´s team
• Centro Universitário Central Paulista, UNICEP, São Carlos, SP, Brazil
• Brazilian agencies CNPq and FAPESP