## Abstract The exchange polarization energy for the H~2~^+^ ion is expressed as an infinite sum of its angular components. At large internuclear distances __R__, a particular __l__‐component, referred to as __induced__ __2__^__l__^‐__pole exchange energy__, behaves asymptotically like For larger
Exact calculation of exchange polarization energy for H ion
✍ Scribed by G. Chałasiński; B. Jeziorski
- Book ID
- 104578275
- Publisher
- John Wiley and Sons
- Year
- 1973
- Tongue
- English
- Weight
- 502 KB
- Volume
- 7
- Category
- Article
- ISSN
- 0020-7608
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✦ Synopsis
Abstract
The exchange polarization energy and higher‐order exchange corrections arising in the second order of the Murrell‐Shaw and Musher‐Amos (MS‐MA) theory are evaluated analytically for the hydrogen molecule ion. At large internuclear distances the second‐order exchange energy predicted by MS‐MA theory behaves like \documentclass{article}\pagestyle{empty}\begin{document}$- \frac{1}{{18}}Re^{ - R}$\end{document}. It represents only 80% of the difference between the exact result of Holstein and the asymptotic value of the first‐order exchange energy. The same result holds for the case of Hirschfelder‐van der Avoird (HAV) and Hirschfelder‐Silbey (HS) theories.
📜 SIMILAR VOLUMES
The exact analytic first-order wavefunction of an H atom in the field of a proton obtained from the unsymmetrized perturbation theory as calculated in 1957 by Dalgamo and Lynn is used to calculate the exchange energy of Hz with the Holstein-Herring method. The asymptotic exchange energy obtained fro
The exchange energy between two atoms has been expressed in terms of a flux integral over a localized wavefunction by Holstein and Herring. By approximating this wavefunction to first order in polarization perturbation theory (Rayleigh-Schrijdinger theory) it is possible to calculate the exchange en