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Non-invertible symmetry in 4-dimensi...
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Koide, Masataka.
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Non-invertible symmetry in 4-dimensional Z2 lattice gauge theory
Record Type:
Electronic resources : Monograph/item
Title/Author:
Non-invertible symmetry in 4-dimensional Z2 lattice gauge theory/ by Masataka Koide.
Author:
Koide, Masataka.
Published:
Singapore :Springer Nature Singapore : : 2025.,
Description:
xiv, 88 p. :ill., digital ;24 cm.
Notes:
"Doctoral theses accepted by Osaka University, Toyonaka, Osaka, Japan."
[NT 15003449]:
Chapter 1 Introduction -- Chapter 2 Symmetry and Topological defect -- Chapter 3 Ising model and Kramers-Wannier duality -- Chapter 4 KWW defect in 4-dimensional lattice gauge theory -- Chapter 5 Application to g-functions -- Chapter 6 Conclusion and discussion -- Appendix.
Contained By:
Springer Nature eBook
Subject:
Symmetry (Physics) -
Online resource:
https://doi.org/10.1007/978-981-96-2272-6
ISBN:
9789819622726
Non-invertible symmetry in 4-dimensional Z2 lattice gauge theory
Koide, Masataka.
Non-invertible symmetry in 4-dimensional Z2 lattice gauge theory
[electronic resource] /by Masataka Koide. - Singapore :Springer Nature Singapore :2025. - xiv, 88 p. :ill., digital ;24 cm. - Springer theses,2190-5061. - Springer theses..
"Doctoral theses accepted by Osaka University, Toyonaka, Osaka, Japan."
Chapter 1 Introduction -- Chapter 2 Symmetry and Topological defect -- Chapter 3 Ising model and Kramers-Wannier duality -- Chapter 4 KWW defect in 4-dimensional lattice gauge theory -- Chapter 5 Application to g-functions -- Chapter 6 Conclusion and discussion -- Appendix.
This book provides a method for concretely constructing defects that represent non-invertible symmetries in four-dimensional lattice gauge theory. In terms of generalized symmetry, a symmetry is considered to be equivalent to a topological operator whose value does not change even if the shape is topologically transformed. Even for models that lack symmetry in the traditional sense and are difficult to analyze, it is possible to analyze them as long as a generalized symmetry exists. Therefore, generalized symmetry is important for the non-perturbative analysis of quantum field theory. Some topological operators have no group structure, and the corresponding symmetries are called non-invertible symmetries. Concrete examples of non-invertible symmetries in higher-dimensional theories were discovered around 2020, and they have been actively studied as a field of generalized symmetries since then. This book explains the non-invertible symmetry represented by the Kramers-Wannier-Wegner duality, which was found firstly in a four-dimensional theory, represented by three-dimensional defects. This book is intended for those with preliminary knowledge of quantum field theory and statistical mechanics.
ISBN: 9789819622726
Standard No.: 10.1007/978-981-96-2272-6doiSubjects--Topical Terms:
532077
Symmetry (Physics)
LC Class. No.: QC174.17.S9
Dewey Class. No.: 539.725
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This book provides a method for concretely constructing defects that represent non-invertible symmetries in four-dimensional lattice gauge theory. In terms of generalized symmetry, a symmetry is considered to be equivalent to a topological operator whose value does not change even if the shape is topologically transformed. Even for models that lack symmetry in the traditional sense and are difficult to analyze, it is possible to analyze them as long as a generalized symmetry exists. Therefore, generalized symmetry is important for the non-perturbative analysis of quantum field theory. Some topological operators have no group structure, and the corresponding symmetries are called non-invertible symmetries. Concrete examples of non-invertible symmetries in higher-dimensional theories were discovered around 2020, and they have been actively studied as a field of generalized symmetries since then. This book explains the non-invertible symmetry represented by the Kramers-Wannier-Wegner duality, which was found firstly in a four-dimensional theory, represented by three-dimensional defects. This book is intended for those with preliminary knowledge of quantum field theory and statistical mechanics.
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