Abstract
The conditions on the behavior of a wavefunction for a system of charged particles near the coalescence of any two of them are derived. The new features of the derivation are: (a) the fixed-nucleus approximation is not required; (b) the wavefunction is not spherically averaged; (c) the wavefunction can have a node at the singularity; and (d) the consequences of the two particles being identical are examined. In addition to the general treatment, the electron—nucleus cusp conditions for diatomic molecules are discussed in detail.
References
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Dates
Type | When |
---|---|
Created | 20 years, 7 months ago (Jan. 9, 2005, 4:42 a.m.) |
Deposited | 1 year, 6 months ago (Feb. 8, 2024, 8:01 p.m.) |
Indexed | 3 weeks, 2 days ago (Aug. 6, 2025, 8 a.m.) |
Issued | 59 years, 1 month ago (July 15, 1966) |
Published | 59 years, 1 month ago (July 15, 1966) |
Published Print | 59 years, 1 month ago (July 15, 1966) |
@article{Pack_1966, title={Cusp Conditions for Molecular Wavefunctions}, volume={45}, ISSN={1089-7690}, url={http://dx.doi.org/10.1063/1.1727605}, DOI={10.1063/1.1727605}, number={2}, journal={The Journal of Chemical Physics}, publisher={AIP Publishing}, author={Pack, Russell T and Brown, W. Byers}, year={1966}, month=jul, pages={556–559} }