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Semiclassical analysis of the magnetic Laplacian on hyperbolic surfaces

Thibault Lefeuvre

TL;DR

This work analyzes the semiclassical limits of eigenfunctions for the magnetic Laplacian on a closed hyperbolic surface with constant magnetic field, focusing on the regime $k\to\infty$ for eigenpairs $k^{-2}\Delta_k u_k=(E+\varepsilon_k)u_k$. It identifies three energy regimes with distinct quantum limits: below the critical energy $E_c=\tfrac{1}{2}B^2$ all invariant measures on the energy shell $\{p=E\}$ occur as defect measures, at $E=E_c$ the Liouville measure is the unique defect measure and a quantitative ergodic statement holds, and above $E_c$ a density-one subsequence equidistributes toward Liouville in the spirit of QUE. The proofs combine Weinstein's periodic-operator construction, magnetic Gaussian beams, and a quantitative version of QUE via horocycle ergodicity and a long-time Egorov argument that remains valid up to polynomial times near the critical energy. The paper also derives improved $L^\infty$ bounds in the critical regime and constructs magnetic zonal states that saturate Hörmander bounds, including a detailed description of their defect measures supported on a two-dimensional invariant torus. Together, these results illuminate how classical magnetic dynamics on hyperbolic surfaces governs quantum limits and provides new quantitative aspects of QUE in a curved, magnetized setting.

Abstract

The magnetic Laplacian on hyperbolic surfaces provides a rich analytic framework in which a variety of quantum phenomena emerge. The present note, written for the \emph{Proceedings of the Journées EDP 2025}, is a concise overview of the main results obtained in [arXiv:2505.08584] and work in preparation by the author with L. Charles and A. Chabert.

Semiclassical analysis of the magnetic Laplacian on hyperbolic surfaces

TL;DR

This work analyzes the semiclassical limits of eigenfunctions for the magnetic Laplacian on a closed hyperbolic surface with constant magnetic field, focusing on the regime for eigenpairs . It identifies three energy regimes with distinct quantum limits: below the critical energy all invariant measures on the energy shell occur as defect measures, at the Liouville measure is the unique defect measure and a quantitative ergodic statement holds, and above a density-one subsequence equidistributes toward Liouville in the spirit of QUE. The proofs combine Weinstein's periodic-operator construction, magnetic Gaussian beams, and a quantitative version of QUE via horocycle ergodicity and a long-time Egorov argument that remains valid up to polynomial times near the critical energy. The paper also derives improved bounds in the critical regime and constructs magnetic zonal states that saturate Hörmander bounds, including a detailed description of their defect measures supported on a two-dimensional invariant torus. Together, these results illuminate how classical magnetic dynamics on hyperbolic surfaces governs quantum limits and provides new quantitative aspects of QUE in a curved, magnetized setting.

Abstract

The magnetic Laplacian on hyperbolic surfaces provides a rich analytic framework in which a variety of quantum phenomena emerge. The present note, written for the \emph{Proceedings of the Journées EDP 2025}, is a concise overview of the main results obtained in [arXiv:2505.08584] and work in preparation by the author with L. Charles and A. Chabert.
Paper Structure (15 sections, 5 theorems, 38 equations)

This paper contains 15 sections, 5 theorems, 38 equations.

Key Result

Theorem 2.1

Under the above assumptions on $(\Sigma,g)$ and $(L,\nabla)$, the following statements hold:

Theorems & Definitions (5)

  • Theorem 2.1: Three semiclassical regimes
  • Theorem 2.2: Polynomial convergence rate at the critical energy
  • Theorem 3.1: $L^\infty$ bounds for magnetic eigenfunctions
  • Proposition 3.2
  • Theorem 3.3: Semiclassical defect measure of magnetic zonal states