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Main Author: Matsuda, Tomohiro
Format: Preprint
Published: 2025
Subjects:
Online Access:https://arxiv.org/abs/2505.09240
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author Matsuda, Tomohiro
author_facet Matsuda, Tomohiro
contents The Berry phase is a geometric phase that is important in explaining topological quantum phenomena. The Berry phase is also important in non-perturbative phenomena, as the imaginary part of the phase explains the non-perturbative transitions. However, problems arose because the singular perturbation with respect to the Planck constant has not been treated adequately in conventional calculations, where the most serious problem is the arbitrariness of approximate calculations. To solve this problem, we consider the exact WKB, which is a mathematical method that treats perturbative expansion with respect to the Planck constant as a rigorous singular perturbation. This method is also a powerful computational tool that makes analytical computation much easier for mathematical software. Using the exact WKB, we analyze the derivation of the dynamical and the geometric exponents in generalized Landau-Zener models, highlighting the differences from other calculational methods. The discontinuity of complex geometric factor is a universal phenomenon that manifests itself in phase transitions, boundaries, particle generation, and topology changes. These phenomena are ``non-perturbative'' in physics, while mathematically, these discontinuities can be deeply related to the singular structure of complex analysis. The mathematical structure of these phenomena will be revealed by using the exact WKB.
format Preprint
id arxiv_https___arxiv_org_abs_2505_09240
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Exact WKB analysis for dynamical and geometric exponents in generalized and nonlinear Landau-Zener transitions
Matsuda, Tomohiro
High Energy Physics - Theory
The Berry phase is a geometric phase that is important in explaining topological quantum phenomena. The Berry phase is also important in non-perturbative phenomena, as the imaginary part of the phase explains the non-perturbative transitions. However, problems arose because the singular perturbation with respect to the Planck constant has not been treated adequately in conventional calculations, where the most serious problem is the arbitrariness of approximate calculations. To solve this problem, we consider the exact WKB, which is a mathematical method that treats perturbative expansion with respect to the Planck constant as a rigorous singular perturbation. This method is also a powerful computational tool that makes analytical computation much easier for mathematical software. Using the exact WKB, we analyze the derivation of the dynamical and the geometric exponents in generalized Landau-Zener models, highlighting the differences from other calculational methods. The discontinuity of complex geometric factor is a universal phenomenon that manifests itself in phase transitions, boundaries, particle generation, and topology changes. These phenomena are ``non-perturbative'' in physics, while mathematically, these discontinuities can be deeply related to the singular structure of complex analysis. The mathematical structure of these phenomena will be revealed by using the exact WKB.
title Exact WKB analysis for dynamical and geometric exponents in generalized and nonlinear Landau-Zener transitions
topic High Energy Physics - Theory
url https://arxiv.org/abs/2505.09240