Elastic Differential Scattering of Low-Energy H+ by Rare-Gas Atoms
Roy L. Champion, L. D. Doverspike, W. G. Rich, Stephen M. Bobbio
Abstract
Roy L. Champion, L. D. Doverspike, W. G. Rich, Stephen M. Bobbio
Abstract
Elastic scattering experiments have been performed on the systems ${\mathrm{H}}^{+}$ + Kr, ${\mathrm{H}}^{+}$ + Ar, ${\mathrm{H}}^{+}$ + Ne, and ${\mathrm{H}}^{+}$ + He with collision energies between 3 and 60 eV. For each of the above systems the experimental differential cross section $\ensuremath{\sigma}(\ensuremath{\theta})$ at one of the lower energies (typically 4 or 6 eV) has been compared with the results of a partial-wave calculation where the JWKB method was used to find the phase shifts and consequently the differential cross section. For the systems Kr${\mathrm{H}}^{+}$, Ne${\mathrm{H}}^{+}$, and Ar${\mathrm{H}}^{+}$an analyticalform was chosen for $V(r)$, and parameters (e.g., the well depth $U$ and the value ${r}_{m}$ of the internuclear separation for which the potential is a minimum) in this model were varied until the calculated $\ensuremath{\sigma}(\ensuremath{\theta})$ agreed quite well with the experimental results. In the case of ${\mathrm{H}}^{+}$ + He two ab initio calculations of the interatomic potential $V(r)$ are available, and each has been used in the JWKB expression to determine the differential cross section. For one of the potentials the predicted $\ensuremath{\sigma}(\ensuremath{\theta})$ is in striking agreement with the experiment. This method is seen, therefore, to provide a sensitive test of such calculations when they exist.
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Elastic scattering experiments have been performed on the systems ${\mathrm{H}}^{+}$ + Kr, ${\mathrm{H}}^{+}$ + Ar, ${\mathrm{H}}^{+}$ + Ne, and ${\mathrm{H}}^{+}$ + He with collision energies between 3 and 60 eV. For each of the above systems the experimental differential cross section $\ensuremath{\sigma}(\ensuremath{\theta})$ at one of the lower energies (typically 4 or 6 eV) has been compared with the results of a partial-wave calculation where the JWKB method was used to find the phase shifts and consequently the differential cross section. For the systems Kr${\mathrm{H}}^{+}$, Ne${\mathrm{H}}^{+}$, and Ar${\mathrm{H}}^{+}$an analyticalform was chosen for $V(r)$, and parameters (e.g., the well depth $U$ and the value ${r}_{m}$ of the internuclear separation for which the potential is a minimum) in this model were varied until the calculated $\ensuremath{\sigma}(\ensuremath{\theta})$ agreed quite well with the experimental results. In the case of ${\mathrm{H}}^{+}$ + He two ab initio calculations of the interatomic potential $V(r)$ are available, and each has been used in the JWKB expression to determine the differential cross section. For one of the potentials the predicted $\ensuremath{\sigma}(\ensuremath{\theta})$ is in striking agreement with the experiment. This method is seen, therefore, to provide a sensitive test of such calculations when they exist.
Key concepts: Physics, Scattering, Atomic physics, Section (typography), Energy (signal processing), Elastic scattering, Ab initio, Quantum mechanics