szd02#li_li1.dat
Electron Impact Ionisation Coefficients
- Ion
- Li1+
- Temperature Range
- 0.600 eV → 4000 eV
ADF07
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- szd02#li_li1.dat
- Full Path
- adf07/szd02#li/szd02#li_li1.dat
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- Li+(1s2 1S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 2s1 3S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 2s1 1S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 2p1 3P) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 2p1 1P) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 3s1 3S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 3s1 1S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 3p1 3P) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 3d1 3D) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 3d1 1D) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 3p1 1P) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4s1 3S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4s1 1S) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4p1 3P) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4d1 3D) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4f1 3F) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4f1 1F) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4d1 1D) + e → Li2+(1s1 2S) + e + e
- Li+(1s1 4p1 1P) + e → Li2+(1s1 2S) + e + e
---------------------------------------------------------------------------- ISEL INITIAL MET. DESIG. FINAL MET. DESIG. ION CODE ION CODE ---- ------- ---- ------------------- ------- ---- --------------- 1 Li+ 1 1 1s2(1S) Li+ 2 1 1s1(2S) 2 Li+ 1 2 1s1 2s1(3S) Li+ 2 1 1s1(2S) 3 Li+ 1 3 1s1 2s1(1S) Li+ 2 1 1s1(2S) 4 Li+ 1 4 1s1 2p1(3P) Li+ 2 1 1s1(2S) 5 Li+ 1 5 1s1 2p1(1P) Li+ 2 1 1s1(2S) 6 Li+ 1 6 1s1 3s1(3S) Li+ 2 1 1s1(2S) 7 Li+ 1 7 1s1 3s1(1S) Li+ 2 1 1s1(2S) 8 Li+ 1 8 1s1 3p1(3P) Li+ 2 1 1s1(2S) 9 Li+ 1 9 1s1 3d1(3D) Li+ 2 1 1s1(2S) 10 Li+ 1 10 1s1 3d1(1D) Li+ 2 1 1s1(2S) 11 Li+ 1 11 1s1 3p1(1P) Li+ 2 1 1s1(2S) 12 Li+ 1 12 1s1 4s1(3S) Li+ 2 1 1s1(2S) 13 Li+ 1 13 1s1 4s1(1S) Li+ 2 1 1s1(2S) 14 Li+ 1 14 1s1 4p1(3P) Li+ 2 1 1s1(2S) 15 Li+ 1 15 1s1 4d1(3D) Li+ 2 1 1s1(2S) 16 Li+ 1 16 1s1 4f1(3F) Li+ 2 1 1s1(2S) 17 Li+ 1 17 1s1 4f1(1F) Li+ 2 1 1s1(2S) 18 Li+ 1 18 1s1 4d1(1D) Li+ 2 1 1s1(2S) 19 Li+ 1 19 1s1 4p1(1P) Li+ 2 1 1s1(2S) The rates were calculated using configuration-average ionization cross sections, with semi-relativistic wavefunctions, using the relaxed-core approximation, the prior form for the scattering potentials, and the natural-phase approximation. They were then multiplied by the appropriate angular coefficients. Data generated by Stuart Loch on 14-Jul-2002 ---------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------