Abstract

We apply the quantum-defect theory for $\ensuremath{-}1/{R}^{4}$ potential to study the resonant charge exchange process. We show that by taking advantage of the partial-wave-insensitive nature of the formulation, resonant charge exchange of the type of ${}^{1}\phantom{\rule{-0.16em}{0ex}}S+{}^{2}\phantom{\rule{-0.16em}{0ex}}S$ can be accurately described over a wide range of energies using only three parameters, such as the gerade and the ungerade $s$-wave scattering lengths, and the atomic polarizability, even at energies where many partial waves contribute to the cross sections. The parameters can be determined experimentally, without having to rely on accurate potential-energy surfaces, of which few exist for ion-atom systems. The theory further relates ultracold interactions to interactions at much higher temperatures.

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