Gauged Wess-Zumino terms for a general coset space

The low-energy physics of systems with spontaneously broken continuous symmetry is dominated by the ensuing Nambu-Goldstone bosons. It has been known for half a century how to construct invariant Lagrangian densities for the low-energy effective theory of Nambu-Goldstone bosons. Contributions, invar...

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Main Authors: Tomáš Brauner, Helena Kolešová
Format: Article
Language:English
Published: Elsevier 2019-08-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321319301622
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spelling doaj-27f909ce2e644e65b23a8f54da5e16a02020-11-24T21:30:45ZengElsevierNuclear Physics B0550-32132019-08-01945Gauged Wess-Zumino terms for a general coset spaceTomáš Brauner0Helena Kolešová1Corresponding author.; Department of Mathematics and Physics, University of Stavanger, N-4036 Stavanger, NorwayDepartment of Mathematics and Physics, University of Stavanger, N-4036 Stavanger, NorwayThe low-energy physics of systems with spontaneously broken continuous symmetry is dominated by the ensuing Nambu-Goldstone bosons. It has been known for half a century how to construct invariant Lagrangian densities for the low-energy effective theory of Nambu-Goldstone bosons. Contributions, invariant only up to a surface term – also known as the Wess-Zumino (WZ) terms – are more subtle, and as a rule are topological in nature. Although WZ terms have been studied intensively in theoretically oriented literature, explicit expressions do not seem to be available in sufficient generality in a form suitable for practical applications. Here we construct the WZ terms in d=1,2,3,4 spacetime dimensions for an arbitrary compact, semisimple and simply connected symmetry group G and its arbitrary connected unbroken subgroup H, provided that the d-th homotopy group of the coset space G/H is trivial. Coupling to gauge fields for the whole group G is included throughout the construction. We list a number of explicit matrix expressions for the WZ terms in four spacetime dimensions, including those for QCD-like theories, that is vector-like gauge theories with fermions in a complex, real or pseudoreal representation of the gauge group.http://www.sciencedirect.com/science/article/pii/S0550321319301622
collection DOAJ
language English
format Article
sources DOAJ
author Tomáš Brauner
Helena Kolešová
spellingShingle Tomáš Brauner
Helena Kolešová
Gauged Wess-Zumino terms for a general coset space
Nuclear Physics B
author_facet Tomáš Brauner
Helena Kolešová
author_sort Tomáš Brauner
title Gauged Wess-Zumino terms for a general coset space
title_short Gauged Wess-Zumino terms for a general coset space
title_full Gauged Wess-Zumino terms for a general coset space
title_fullStr Gauged Wess-Zumino terms for a general coset space
title_full_unstemmed Gauged Wess-Zumino terms for a general coset space
title_sort gauged wess-zumino terms for a general coset space
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
publishDate 2019-08-01
description The low-energy physics of systems with spontaneously broken continuous symmetry is dominated by the ensuing Nambu-Goldstone bosons. It has been known for half a century how to construct invariant Lagrangian densities for the low-energy effective theory of Nambu-Goldstone bosons. Contributions, invariant only up to a surface term – also known as the Wess-Zumino (WZ) terms – are more subtle, and as a rule are topological in nature. Although WZ terms have been studied intensively in theoretically oriented literature, explicit expressions do not seem to be available in sufficient generality in a form suitable for practical applications. Here we construct the WZ terms in d=1,2,3,4 spacetime dimensions for an arbitrary compact, semisimple and simply connected symmetry group G and its arbitrary connected unbroken subgroup H, provided that the d-th homotopy group of the coset space G/H is trivial. Coupling to gauge fields for the whole group G is included throughout the construction. We list a number of explicit matrix expressions for the WZ terms in four spacetime dimensions, including those for QCD-like theories, that is vector-like gauge theories with fermions in a complex, real or pseudoreal representation of the gauge group.
url http://www.sciencedirect.com/science/article/pii/S0550321319301622
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