Elastic and charge transfer cross sections for low to ultralow $\rm{H}(1s) + \rm{H}^{+}$ collisions. Quantal and semiclassical calculations
Mykhaylo Khoma
TL;DR
This work addresses elastic and resonant charge-transfer cross sections in $\rm{H}(1s)+\rm{H}^+$ collisions over $E_{ m cm}$ from $10^{-10}$ to $10$ eV. It combines fully quantum radial-equation solutions with Born–Oppenheimer potentials $E^{\rm BO}_{g,u}(R)$ and a semiclassical JWKB treatment (including a three-turning-point extension) to obtain phase shifts $\delta_{g}(l)$, $\delta_{u}(l)$ and the corresponding cross sections $\sigma^{(i)}_{\rm EL}$, $\sigma^{(d)}_{ m EL}$, and $\sigma_{ m CT}$. The results show excellent agreement (∼0.1%) with prior data across most energies, reveal new oscillations in the charge-transfer cross section around $E_{ m cm}\approx 0.127$ eV and $0.363$ eV, and demonstrate that the semiclassical approach remains reliable down to $E_{ m cm}\sim 0.01$ eV while highlighting the need for three-turning-point corrections at lower energies. The study thus extends the practical applicability of semiclassical methods to ultra-low-energy ion–atom collisions and provides detailed phase-shift data for $\rm{H}(1s)+\rm{H}^+$.
Abstract
The elastic scattering and resonant charge transfer integral cross sections in $\rm{H}(1s) + \rm{H^+}$ collisions are computed for the center-of-mass energy range of $10^{-10}-10$ eV. Fully quantal and semiclassical approaches are utilized in these calculations. The reliability of the semiclassical approximation for very low collision energies is discussed. The results are compared with available data from the literature.
