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arXiv 2610.20006quant-phhep-thmath-phmath.MP

多阱量子力学中的多瞬子与精确WKB Stokes跃变

Multi-Instantons and Exact-WKB Stokes Jumps in Multi-Well Quantum Mechanics

Stacks;Department of Physics, The University of Tokyo(东京大学物理学系)

Alireza Behtash, Syo Kamata

AI总结:

该研究探讨多阱量子力学中精确WKB Stokes跃变与多瞬子展开的关系,将单势垒的Bogomolny--Zinn-Justin抵消扩展到多势垒,通过局部Weber近似等方法推导相关周期与系数,构造了特定事件序列并以三阱数值解验证结果。

摘要:

我们研究了精确WKB Delabaere--Dillinger--Pham Stokes跃变与具有N个等深极小值的一维势的多瞬子展开之间的关系。对于单个势垒,这种关系是瞬子-反瞬子歧义与微扰理论的Borel歧义之间的Bogomolny--Zinn-Justin抵消,我们将其扩展到每个连续势垒区间以及积分轮廓本身。在固定非微扰等级的稀大T regime中,我们从欧几里得路径积分导出了瞬子间距上的准零模积分,并将其简化为Gamma和Hankel周期。通过每个阱的局部Weber能级函数以及每个阱由局部Weber连接矩阵确定的一个归一化,这些周期再现了两个横向连通的精确WKB系数。每个瞬子-反瞬子间距的两个横向轮廓恰好相差一个Hankel周期,这种线性Picard--Lefschetz关系再现了连通系数的Stokes跃变。对称三阱的薛定谔方程数值解证实了所得的双势垒能级分裂。在更高的固定等级下,从有序事件序列到归一化标量系数乘积的映射不是单射。在主导稀阶,闭合事件序列的标量权重仅取决于势垒交叉数、$\boldsymbol{\textit{I}}\bar{\boldsymbol{\textit{I}}}$对以及$\boldsymbol{\textit{I}}\boldsymbol{\textit{I}}$ / $\bar{\boldsymbol{\textit{I}}}\bar{\boldsymbol{\textit{I}}}$对的数量。我们构造了两个不等价的六级三阱事件序列,具有相同的局部Weber振幅乘积,它们嵌入在每个N≥3个阱的势中。我们的结果在规则稀、单圈、局部Weber近似范围内成立。

英文摘要:

We study the relation between the exact-WKB Delabaere--Dillinger--Pham Stokes jumps and the multi-instanton expansion of a one-dimensional potential with $N$ equal-depth minima. For a single barrier this relation is the Bogomolny--Zinn-Justin cancellation between the instanton--anti-instanton ambiguity and the Borel ambiguity of perturbation theory, and we extend it to every consecutive barrier interval and to the integration contours themselves. In the dilute large-$T$ regime at fixed nonperturbative grade, we derive the quasi-zero mode integral over the instanton separations from the Euclidean path integral and reduce it to Gamma and Hankel periods. With the local Weber level function of each well and one normalization per well fixed by the local Weber connection matrix, these periods reproduce the two lateral connected exact-WKB coefficients. The two lateral contours of each instanton--anti-instanton separation differ by exactly one Hankel cycle, and this linear Picard--Lefschetz relation reproduces the Stokes jump of the connected coefficient. A numerical solution of the Schrödinger equation for a symmetric triple well confirms the resulting two-barrier level splitting. At higher fixed grade, the map from ordered event sequences to normalized scalar coefficient products is not one-to-one. At leading dilute order the scalar weight of a closed event sequence depends only on the numbers of barrier crossings, $\mathcal I\bar{\mathcal I}$ pairs, and $\mathcal I\mathcal I$/$\bar{\mathcal I}\bar{\mathcal I}$ pairs. We construct two inequivalent grade-six triple-well event sequences with the same product of local Weber amplitudes, which embed in every potential with $N\ge3$ wells. Our results hold within the regular dilute, one-loop, local Weber approximation.

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