| He2+ + H0(n=2) → He+ + H+ | total |
| He2+ + H0(n=2) → He+(n=2) + H+ | n-resolved |
| He2+ + H0(n=2) → He+(2s) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(2p) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(n=3) + H+ | n-resolved |
| He2+ + H0(n=2) → He+(3s) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(3p) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(3d) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(n=4) + H+ | n-resolved |
| He2+ + H0(n=2) → He+(4s) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(4p) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(4d) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(4f) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(n=5) + H+ | n-resolved |
| He2+ + H0(n=2) → He+(5s) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(5p) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(5d) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(5f) + H+ | nl-resolved |
| He2+ + H0(n=2) → He+(5g) + H+ | nl-resolved |
------------------------------------------------------------------------------------------ Data prepared by R. Hoekstra, F. Bliek and H. P. Summers from analysis of CTMC calculations of Olson. . High n behaviour was fitted with the alpha parameter. Smooth alpha behviour at low energy was imposed where CTMC statistics were poor. l-substate cross-sections, for n=5, were obtained by using the n-1 distribution using code adasxx30.fort(adev312) H. P. Summers 20 Sept. 1995 ------------------------------------------------------------------------------------------ Erratic behaviour and omitted l-substates for n=2 a low energy has been modified in the primary data. The data before adjustment is below. 0.01 0.02 0.05 0.1 0.2 0 2.0 5.0 / energies (keV.amu) 15.0 15.0 14.5 13.3 12.0 2 6.4 4.4 / alpha 1.11E-14 1.18E-14 1.18E-14 1.16E-14 1.16E-14 4 1.34E-14 1.34E-14 / total n l m / partial cross sections 2 0.00E+00 5.50E-19 5.50E-19 3.04E-18 2.75E-18 7 4.81E-17 9.32E-17 2 0 0.00E+00 0.00E+00 0.00E+00 1.01E-18 2.20E-18 8 1.22E-17 3.09E-17 2 1 0.00E+00 0.00E+00 0.00E+00 2.03E-18 5.50E-19 7 3.60E-17 6.23E-17 H. P. Summers 20 Sept. 1995 ------------------------------------------------------------------------------------------ --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------