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Data generated by Stuart Loch on 04/22/03
NOTES.
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ISEL INITIAL MET. DESIG. FINAL MET. DESIG.
ION CODE ION CODE
____ _______ ____ ___________________ _______ ____ _______________
1 be+ 1 1 1s2 2s1(2S) be+ 2 1 1s2 (1S)
2 be+ 1 1 1s2 2s1(2S) be+ 2 2 1s1 2s1(3S)
3 be+ 1 1 1s2 2p1(2P) be+ 2 1 1s2 (1S)
The rates were calculated using a Rost fit to RMPS ionization
cross sections for the 1s2 2s1 configuration, and to the
TDCC ionization cross for the 1s2 2p1 configuration.
See PRA 68,032712 (2003) for more details.
The inner shell 1s2 2s1(2S) -> 1s1 2s1(3S) process was calculated
using configuration-average ionization cross
sections, with semi-relativistic wavefunctions, using the
relaxed-core approximation, the post form for the scattering
potentials, and the natural-phase approximation.
This was then multiplied by the appropriate angular coefficients.
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---------------------------------------------------------------------------- Data generated by Stuart Loch on 04/22/03 NOTES. ______ ISEL INITIAL MET. DESIG. FINAL MET. DESIG. ION CODE ION CODE ____ _______ ____ ___________________ _______ ____ _______________ 1 be+ 1 1 1s2 2s1(2S) be+ 2 1 1s2 (1S) 2 be+ 1 1 1s2 2s1(2S) be+ 2 2 1s1 2s1(3S) 3 be+ 1 1 1s2 2p1(2P) be+ 2 1 1s2 (1S) The rates were calculated using a Rost fit to RMPS ionization cross sections for the 1s2 2s1 configuration, and to the TDCC ionization cross for the 1s2 2p1 configuration. See PRA 68,032712 (2003) for more details. The inner shell 1s2 2s1(2S) -> 1s1 2s1(3S) process was calculated using configuration-average ionization cross sections, with semi-relativistic wavefunctions, using the relaxed-core approximation, the post form for the scattering potentials, and the natural-phase approximation. This was then multiplied by the appropriate angular coefficients. ----------------------------------------------------------------------------