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强磁场中的双势阱:耦合常数取无穷多个值时隧穿的缺失

Double-wells in a strong magnetic field: absence of tunneling for infinitely many values of the coupling constant

Kevin Buck, Charles L. Fefferman, Javier Gómez-Serrano, Amaury Hayat, Jacob Shapiro, Michael I. Weinstein

arXiv 2609.21078首次发表:更新:

发表机构

Brown University; Princeton University; CERMICS, École des Ponts, Institut Polytechnique de Paris; University of Vienna; Department of Mathematics, Columbia University(布朗大学; 普林斯顿大学; 巴黎高等师范学院 CERMICS,巴黎理工学院; 维也纳大学; 哥伦比亚大学数学系)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本文证明反演对称磁双阱的固定势猜想,构造特定单阱势,使得耦合常数趋于无穷时,双阱哈密顿量最低两特征值出现无穷多次精确简并,且基态宇称反复变化。

AI 中文摘要

我们证明了Fefferman、Shapiro和Weinstein关于反演对称磁双势阱的固定势猜想。我们构造了一个数$L_0>0$和一个光滑、紧支撑、非正、非径向的单阱势$v$,该势与耦合参数$\lambda$和阱位移均无关,使得对于每个固定的$L\ge L_0$,当$\lambda\to\infty$时,相关的磁双阱哈密顿量的两个最低特征值具有无穷多个精确简并。磁跳跃系数也沿一个趋于无穷的无限序列消失。该势由一个径向核心和两个小的、反射相关的微扰组成,这些微扰支撑在单侧二次尖点上。它们的对数平坦轮廓隔离了两个主要的跳跃贡献,我们在插入径向基态渐近后通过最速下降法对其进行评估。由此得到的渐近余弦表达式,连同偶-奇分裂的误差界,产生了无穷多个精确的特征值交叉和基态宇称变化。

英文摘要

We prove the fixed-potential conjecture of Fefferman, Shapiro, and Weinstein for inversion-symmetric magnetic double wells. We construct a number $L_0>0$ and one smooth, compactly supported, nonpositive, nonradial single-well potential $v$, independent of both the coupling parameter $λ$ and the well displacement, such that for every fixed $L\ge L_0$ the associated magnetic double-well Hamiltonian has infinitely many exact degeneracies of its two lowest eigenvalues as $λ\to\infty$. The magnetic hopping coefficient also vanishes along an infinite sequence tending to infinity. The potential consists of a radial core and two small, reflection-related perturbations supported on one-sided quadratic cusps. Their log-flat profiles isolate two dominant hopping contributions, which we evaluate by steepest descent after inserting the radial ground-state asymptotics. The resulting asymptotic cosine expression, together with error bounds for the even--odd splitting, yields infinitely many exact eigenvalue crossings and changes of ground-state parity.

论文原文

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