Abstract
The asymptotic closure cross section, derived in I of this series, is calculated for the $1s{\ensuremath{\sigma}}_{g}\ensuremath{-}2p{\ensuremath{\sigma}}_{u}$ excitation of $\mathrm{H}_{2}^{}{}_{}{}^{+}$ by fast electrons. These data are compared with earlier treatments of this system which were based on a less rigorous theory. The earlier data are observed to be surprisingly accurate. The Bethe cross section for exciting discrete vibrational modes in the $2p{\ensuremath{\sigma}}_{u}$ orbital of $\mathrm{H}_{2}^{}{}_{}{}^{+}$ is calculated. This cross section is then used, along with the asymptotic closure cross section, to generate the Bethe cross section for all continuum modes of nuclear motion in the $2p{\ensuremath{\sigma}}_{u}$ orbital of $\mathrm{H}_{2}^{}{}_{}{}^{+}$. Two approximations are considered for this partitioning of the asymptotic closure cross section and they are not found to be, in general, very useful.
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