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 if zα12/7<const (in case A) and zα2<const (in case B), (z{divides}e{divides}=nuclear charge, α=fine structure constant), but a new feature enters in case B. There one also requires α<const, regardless of the value of z.
Original language | English (US) |
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Pages (from-to) | 271-282 |
Number of pages | 12 |
Journal | Communications In Mathematical Physics |
Volume | 104 |
Issue number | 2 |
DOIs | |
State | Published - Jun 1986 |
All Science Journal Classification (ASJC) codes
- Statistical and Nonlinear Physics
- Mathematical Physics