Abstract

There are two well-known approaches to studying nonperturbative aspects of quantum mechanical systems: saddle point analysis of the partition functions in Euclidean path integral formulation and the exact-WKB analysis based on the wave functions in the Schrödinger equation. In this work, based on the quantization conditions obtained from the exact-WKB method, we determine the relations between the two formalism and in particular show how the two Stokes phenomena are connected to each other: the Stokes phenomenon leading to the ambiguous contribution of different sectors of the path integral formulation corresponds to the change of the “topology” of the Stoke curves in the exact-WKB analysis. We also clarify the equivalence of different quantization conditions including Bohr-Sommerfeld, path integral and Gutzwiller’s ones. In particular, by reorganizing the exact quantization condition, we improve Gutzwiller’s analysis in a crucial way by bion contributions (incorporating complex periodic paths) and turn it into an exact result. Furthermore, we argue the novel meaning of quasi-moduli integral and provide a relation between the Maslov index and the intersection number of Lefschetz thimbles.

Highlights

  • In each one of these constructions, to see the connection between P/NP physics, the most prominent role is played by resurgence theory, and Stokes phenomena

  • In this work, based on the quantization conditions obtained from the exact-WKB method, we determine the relations between the two formalism and in particular show how the two Stokes phenomena are connected to each other: the Stokes phenomenon leading to the ambiguous contribution of different sectors of the path integral formulation corresponds to the change of the “topology” of the Stoke curves in the exactWKB analysis

  • We explored the connections between exact WKB method, saddle point analysis of Euclidean path integration, and the Gutzwiller trace formula

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Summary

Preparation

We introduce the tools other than the exact-WKB analysis as prerequisite knowledge. Our discussion is basic and is streamlined according to what we need later

Lefschetz thimble decomposition and resolvent method
Gutzwiller’s quantization
Maslov index
Exact WKB
Borel summation
Stokes curves and Stokes phenomena
Connection formula and monodromy matrix
Warm-up
A Sodd e
Resolvent and spectral form
Symmetric double-well potential
Partition function
The intersection number of Lefschetz thimble
Unambiguity of the partition function under the Borel resummation
DA1 DA2
Discussion and summary
B Imaginary ambiguity cancellation for the double well potential
Full Text
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