Answers are grounded in this paper and cite their sources.
The cross section σ₁(ε;E) has been calculated for the direct impact ionization of hydrogen atoms by protons, H⁺+H(1s)→2H⁺+e^-, for low relative collision energies E between 100 and 500 eV, and all electron energies ε for which it is significant. Fundamental theory and most electronic matrix-element calculations were presented in earlier papers of the series. In the present paper we complete the electronic matrix-element calculations (in particular, the "optimization" of Coriolis or angular coupling matrix elements for ionizing transitions, through introduction of an angular velocity electron-translation factor); and we perform the final integrations over classical trajectories and impact parameters to obtain the cross sections. The cross sections σ₁(ε;E) show the expected steep falloff with increasing ε and decreasing E, owing to the increasing inefficiency of momentum and energy transfer from the heavy particles to the electron under such changes; σ₁ decreases by about two orders of magnitude from E=500 eV to $E=100$ eV, and by four orders of magnitude from ε=0 a.u. to ε=1.0 a.u. A strong dependence of cross section on isotopic mass at fixed E is also predicted thereby. Finally, the most significant conclusion is that the cross section for ionization from the 1sσᵤ(2pσᵤ) molecular electronic state is about 500 times greater than that for ionizing a 1sσg molecular electron, the main source of transitions being the Coriolis coupling operator.
No takes yet. Share an insight, caveat, or question.
Sethuraman et al. (1973) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: