| He2+ + Li0(3s) → He+ + Li+ | total |
| He2+ + Li0(3s) → He+(n=3) + Li+ | n-resolved |
| He2+ + Li0(3s) → He+(3s) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(3p) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(3d) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(n=4) + Li+ | n-resolved |
| He2+ + Li0(3s) → He+(4s) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(4p) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(4d) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(4f) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(n=5) + Li+ | n-resolved |
| He2+ + Li0(3s) → He+(5s) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(5p) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(5d) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(5f) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(5g) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(n=6) + Li+ | n-resolved |
| He2+ + Li0(3s) → He+(6s) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(6p) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(6d) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(6f) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(6g) + Li+ | nl-resolved |
| He2+ + Li0(3s) → He+(6h) + Li+ | nl-resolved |
---------------------------------------------------------------------------------------------------------------------- Source: J.Schweinzer, Max Planck Institut fuer Plasmaphysik, Garching, Germany Comments: Atomic Orbital close coupling calculations for He2+ colliding with Lithium atoms in various initial states (2s,3s,2p,3p,3d) have been performed using a single set of basis states. The expansion includes travelling atomic orbitals on the He2+ centre (n-shells 1 - 6) and LiI states up to Li(5g). The latter states have been obtained by diagonalisation of the atomic Hamiltonian with a model potential. In addition to these bound states pseudo-states are included which improve the convergence behaviour and represent ionisation. Altogether, the expansion consists of 87 states on the He centre and 80 on Li. From these calculations partial cross sections for charge exchange into HeII(nl) (n=1-6) have been deduced in an energy range of 1.5 - 20 keV/amu. The accuracy is believed to be 5-10% for cross sections > 10**-15 cm**2 and 30-40% for those < 10**-16 cm**2. Authors: E.Wolfrum, J.Schweinzer IPP Garching Date: September 2004 -----------------------------------------------------------------------------------------------------------------------