Thermodynamic Bethe ansatz and wall crossing for deformed supersymmetric quantum mechanics

We study the deformed supersymmetric quantum mechanics with a polynomial superpotential with <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mi>ℏ</a:mi> </a:math> correction. In the minimal chamber, where all turning points are real and distinct, it was shown that the exact Wentzel–Kramers–Brillouin periods obey the <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msub> <c:mi mathvariant="double-struck">Z</c:mi> <c:mn>4</c:mn> </c:msub> </c:math> -extended thermodynamic Bethe ansatz (TBA) equations of the undeformed potential. By changing the energy parameter above/below the critical points, the turning points become complex, and the moduli are outside of the minimal chamber. We study the wall crossing of the <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:msub> <f:mi mathvariant="double-struck">Z</f:mi> <f:mn>4</f:mn> </f:msub> </f:math> -extended TBA equations by this change of moduli and show that the <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:msub> <i:mi mathvariant="double-struck">Z</i:mi> <i:mn>4</i:mn> </i:msub> </i:math> structure is preserved after the wall crossing. In particular, the TBA equations for the cubic superpotential are studied in detail, where there are two chambers (minimal and maximal). At the maximally symmetric point in the maximal chamber, the TBA system becomes the two sets of the <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"> <l:msub> <l:mi>D</l:mi> <l:mn>3</l:mn> </l:msub> </l:math> -type TBA equations, which are regarded as the <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"> <n:msub> <n:mi mathvariant="double-struck">Z</n:mi> <n:mn>4</n:mn> </n:msub> </n:math> extension of the <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"> <q:msub> <q:mi>A</q:mi> <q:mn>3</q:mn> </q:msub> <q:mo>/</q:mo> <q:msub> <q:mi mathvariant="double-struck">Z</q:mi> <q:mn>2</q:mn> </q:msub> </q:math> -type TBA equation.

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Publication Details

Journal
Physical review. D/Physical review. D.
Published
2026-01-05
DOI
https://doi.org/10.1103/7r3h-lmwg
Citations
1
Primary Topic
Quantum Chromodynamics and Particle Interactions
Type
article
Field-Weighted Citation Impact
27.96

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article

Thermodynamic Bethe ansatz and wall crossing for deformed supersymmetric quantum mechanics

Hongfei Shu, Yang Jingjing, Katsushi Ito
1 citations
Physical review. D/Physical review. D.
Quantum Chromodynamics and Particle Interactions
27.96
article

Thermodynamic Bethe ansatz and wall crossing for deformed supersymmetric quantum mechanics

Hongfei Shu, Yang Jingjing, Katsushi Ito
article en
1 citations

Abstract

We study the deformed supersymmetric quantum mechanics with a polynomial superpotential with <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:mi>ℏ</a:mi> </a:math> correction. In the minimal chamber, where all turning points are real and distinct, it was shown that the exact Wentzel–Kramers–Brillouin periods obey the <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msub> <c:mi mathvariant="double-struck">Z</c:mi> <c:mn>4</c:mn> </c:msub> </c:math> -extended thermodynamic Bethe ansatz (TBA) equations of the undeformed potential. By changing the energy parameter above/below the critical points, the turning points become complex, and the moduli are outside of the minimal chamber. We study the wall crossing of the <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:msub> <f:mi mathvariant="double-struck">Z</f:mi> <f:mn>4</f:mn> </f:msub> </f:math> -extended TBA equations by this change of moduli and show that the <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"> <i:msub> <i:mi mathvariant="double-struck">Z</i:mi> <i:mn>4</i:mn> </i:msub> </i:math> structure is preserved after the wall crossing. In particular, the TBA equations for the cubic superpotential are studied in detail, where there are two chambers (minimal and maximal). At the maximally symmetric point in the maximal chamber, the TBA system becomes the two sets of the <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"> <l:msub> <l:mi>D</l:mi> <l:mn>3</l:mn> </l:msub> </l:math> -type TBA equations, which are regarded as the <n:math xmlns:n="http://www.w3.org/1998/Math/MathML" display="inline"> <n:msub> <n:mi mathvariant="double-struck">Z</n:mi> <n:mn>4</n:mn> </n:msub> </n:math> extension of the <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"> <q:msub> <q:mi>A</q:mi> <q:mn>3</q:mn> </q:msub> <q:mo>/</q:mo> <q:msub> <q:mi mathvariant="double-struck">Z</q:mi> <q:mn>2</q:mn> </q:msub> </q:math> -type TBA equation.

Physical review. D/Physical review. D.Vol. 113(4)
University of Science and Technology of China (CN), Zhengzhou University (CN), Shanghai Institute for Science of Science (CN), Peng Huanwu Center for Fundamental Theory (CN), Institute of Science Tokyo (JP)
National Natural Science Foundation of China, Zhengzhou University, Japan Society for the Promotion of Science
Openalex Percentile: Top 2%
Quantum Chromodynamics and Particle Interactions
27.96
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