| He2+ + Li0(2s) → He+ + Li+ | total |
| He2+ + Li0(2s) → He+(n=1) + Li+ | n-resolved |
| He2+ + Li0(2s) → He+(1s) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(n=2) + Li+ | n-resolved |
| He2+ + Li0(2s) → He+(2s) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(2p) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(n=3) + Li+ | n-resolved |
| He2+ + Li0(2s) → He+(3s) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(3p) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(3d) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(n=4) + Li+ | n-resolved |
| He2+ + Li0(2s) → He+(4s) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(4p) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(4d) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(4f) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(n=5) + Li+ | n-resolved |
| He2+ + Li0(2s) → He+(5s) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(5p) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(5d) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(5f) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(5g) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(n=6) + Li+ | n-resolved |
| He2+ + Li0(2s) → He+(6s) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(6p) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(6d) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(6f) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(6g) + Li+ | nl-resolved |
| He2+ + Li0(2s) → He+(6h) + Li+ | nl-resolved |
----------------------------------------------------------------------------------------------------- Source: The data consists of results of CTMC calculations made at the University of Missouri over the period 1995-97. Comments: From the comparison of CTMC calculations for Be+4, B+5 and C+6 with experiments performed at KVI, it seems that in the 1-15 keV/amu energy range, these collisions are well described by the theory. For verification, we compared our data with the recommended scaled cross-sections of Schweinzer et al (1994). Agreement is good. It is to be noted that the scaled formulae of Schweinzer are to be used with the effective principal quantum number of the donor state. Calculations of Fritsch and Lin (1984) for C+4 are in agreement with the CTMC results for Be+4. Also total one-electron capture cross-sections, which were experimentally determined by different groups confirm the results for one-electron capture in He+2 collisions. The data was assembled as ADAS data files of type adf01 at JET Joint Undertaking in the period Authors: J. W. Turkstra, G. Lubinski, R. Hoekstra*, R. E. Olson# * KVI, Groningen, Netherlands # University of Missouri, Rolla, USA. Date: 9 June 1997. Updates: 23/12/97 R. Hoekstra & H.P. Summers - amended comments section following clarifications by Schweinzer. ----------------------------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------