Use the Coulomb-Born approximation to get scattering cross sections for e⁻ + target. Also determines Einstein A coefficients and excited state average lifetimes within !! the radiative dipole/multipole approximation. The target charge Z is supplied and used by the routine that are called here, so various target charges can be used, including Z = 0 (neutral targets). This routine loops over the different pairs Nτ —→ N'τ'
| Type | Intent | Optional | Attributes | Name | ||
|---|---|---|---|---|---|---|
| type(config_type), | intent(in) | :: | cfg | |||
| type(N_states_type), | intent(inout), | allocatable | :: | n_states(:) | ||
| type(rvector_type), | intent(out), | allocatable | :: | egrid_elec_cb(:) |
Array of arrays of electron/collision energies for each transition |
|
| type(asymtop_rot_transition_type), | intent(out), | allocatable | :: | transitions_cb(:) |
Array containing transitions between rotational states for the long-range CB excitations |
|
| type(rvector_type), | intent(out), | allocatable | :: | xs_xcite_pcb(:) |
Array of arrays of the Partial and Total Coulomb-Born cross sections for each transition |
|
| type(rvector_type), | intent(out), | allocatable | :: | xs_xcite_tcb(:) |
Array of arrays of the Partial and Total Coulomb-Born cross sections for each transition |
|
| character(len=*), | intent(in) | :: | pcb_output_directory | |||
| character(len=*), | intent(in) | :: | tcb_output_directory |