Abstract
It is well-known that, due to the interaction between the spin and the magnetic field, the two-dimensional Pauli operator has an eigenvalue 0 at the threshold of its essential spectrum. We show that when perturbed by an effectively positive perturbation, V, coupled with a small parameter ε, these eigenvalues become resonances. Moreover, we derive explicit expressions for the leading terms of their imaginary parts in the limit ε↘0. These show, in particular, that the dependence of the imaginary part of the resonances on ε is determined by the flux of the magnetic field. The cases of non-degenerate and degenerate zero eigenvalue are treated separately. We also discuss applications of our main results to particles with anomalous magnetic moments.
| Original language | English |
|---|---|
| Pages (from-to) | 2839-2875 |
| Number of pages | 37 |
| Journal | Annales Henri Poincare |
| Volume | 25 |
| Issue number | 6 |
| DOIs | |
| State | Published - Jun 2024 |
Bibliographical note
Publisher Copyright:© Springer Nature Switzerland AG 2023.
Keywords
- 35P05
- 35Q40
- 81Q10
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