Abstract
The magnetic Schrödinger operator, with Neumann boundary condition, on a smooth, bounded, and simply connected domain \(\Omega \) of the Euclidean plane is considered in the semiclassical limit. When \(\Omega \) has a symmetry axis, the semiclassical splitting of the first two eigenvalues is analyzed. The first explicit tunneling formula in a pure magnetic field is established. The analysis is based on a pseudo-differential reduction to the boundary and the proof of the first known optimal purely magnetic Agmon estimates.
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Notes
and actually of the conjugated operator \({\mathscr {N}}^{\varphi }_{\hbar , r}= e^{\varphi /\hbar ^{\frac{1}{2}}}{\mathscr {N}}_{\hbar , r}e^{-\varphi /\hbar ^{\frac{1}{2}}}\), where \(\varphi \) is an appropriate subsolution of the effective eikonal equation.
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N. R. and F. H. are deeply grateful to the Mittag-Leffler Institute where part of the ideas of this article were discussed. N. R. also thanks Bernard Helffer, Pierig Keraval and Johannes Sjöstrand for many stimulating discussions.
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Bonnaillie-Noël, V., Hérau, F. & Raymond, N. Purely magnetic tunneling effect in two dimensions. Invent. math. 227, 745–793 (2022). https://doi.org/10.1007/s00222-021-01073-x
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DOI: https://doi.org/10.1007/s00222-021-01073-x