Abstract
The analysis of the ground state energy of Coulomb systems interacting with magnetic fields, begun in Part I, is extended here to two cases. Case A: The many electron atom; Case B: One electron with arbitrarily many nuclei. As in Part I we prove that stability occurs ifzα12/7<const (in case A) andzα2<const (in case B), (z∣e∣=nuclear charge, α=fine structure constant), but a new feature enters in case B. There onealso requires α<const, regardless of the value ofz.
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Communicated by A. Jaffe
Work partially supported by U.S. National Science Foundation grant PHY-8116101-A03
Work partially supported by U.S. and Swiss National Science Foundation Cooperative Science Program INT-8503858.
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Lieb, E.H., Loss, M. Stability of Coulomb systems with magnetic fields. Commun.Math. Phys. 104, 271–282 (1986). https://doi.org/10.1007/BF01211594
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DOI: https://doi.org/10.1007/BF01211594