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Data generated by Stuart Loch on 31/01/06
NOTES.
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ISEL INITIAL MET. DESIG. FINAL MET. DESIG.
ION CODE ION CODE
____ _______ ____ ___________________ _______ ____ _______________
1 be+ 2 1 1s2(1S) be+ 3 1 1s1(2S)
2 be+ 2 1 1s1 2s1(3S) be+ 3 1 1s1(2S)
3 be+ 2 2 1s1 2s1(3S) be+ 3 2 1s0 2s1(2S)
The rates were calculated using the Rost function
for the ionization section, with the peak cross section
values given from TDCC calculations
For the 1s1 2s1(3S)->1s0 2s1(2S) transition, the
rates were 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.
They were then multiplied by the appropriate angular coefficients.
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---------------------------------------------------------------------------- Data generated by Stuart Loch on 31/01/06 NOTES. ______ ISEL INITIAL MET. DESIG. FINAL MET. DESIG. ION CODE ION CODE ____ _______ ____ ___________________ _______ ____ _______________ 1 be+ 2 1 1s2(1S) be+ 3 1 1s1(2S) 2 be+ 2 1 1s1 2s1(3S) be+ 3 1 1s1(2S) 3 be+ 2 2 1s1 2s1(3S) be+ 3 2 1s0 2s1(2S) The rates were calculated using the Rost function for the ionization section, with the peak cross section values given from TDCC calculations For the 1s1 2s1(3S)->1s0 2s1(2S) transition, the rates were 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. They were then multiplied by the appropriate angular coefficients. ----------------------------------------------------------------------------