Chern-Weil global symmetries and how quantum gravity avoids them

Abstract We draw attention to a class of generalized global symmetries, which we call “Chern-Weil global symmetries,” that arise ubiquitously in gauge theories. The Noether currents of these Chern-Weil global symmetries are given by wedge products of gauge field strengths, such as F 2 ∧ H 3 and tr(...

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Autores principales: Ben Heidenreich, Jacob McNamara, Miguel Montero, Matthew Reece, Tom Rudelius, Irene Valenzuela
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Lenguaje:EN
Publicado: SpringerOpen 2021
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Acceso en línea:https://doaj.org/article/175c60efb2b74b4c9d9844b33ab413a8
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spelling oai:doaj.org-article:175c60efb2b74b4c9d9844b33ab413a82021-11-14T12:40:27ZChern-Weil global symmetries and how quantum gravity avoids them10.1007/JHEP11(2021)0531029-8479https://doaj.org/article/175c60efb2b74b4c9d9844b33ab413a82021-11-01T00:00:00Zhttps://doi.org/10.1007/JHEP11(2021)053https://doaj.org/toc/1029-8479Abstract We draw attention to a class of generalized global symmetries, which we call “Chern-Weil global symmetries,” that arise ubiquitously in gauge theories. The Noether currents of these Chern-Weil global symmetries are given by wedge products of gauge field strengths, such as F 2 ∧ H 3 and tr( F 2 2 $$ {F}_2^2 $$ ), and their conservation follows from Bianchi identities. As a result, they are not easy to break. However, it is widely believed that exact global symmetries are not allowed in a consistent theory of quantum gravity. As a result, any Chern-Weil global symmetry in a low-energy effective field theory must be either broken or gauged when the theory is coupled to gravity. In this paper, we explore the processes by which Chern-Weil symmetries may be broken or gauged in effective field theory and string theory. We will see that many familiar phenomena in string theory, such as axions, Chern-Simons terms, worldvolume degrees of freedom, and branes ending on or dissolving in other branes, can be interpreted as consequences of the absence of Chern-Weil symmetries in quantum gravity, suggesting that they might be general features of quantum gravity. We further discuss implications of breaking and gauging Chern-Weil symmetries for particle phenomenology and for boundary CFTs of AdS bulk theories. Chern-Weil global symmetries thus offer a unified framework for understanding many familiar aspects of quantum field theory and quantum gravity.Ben HeidenreichJacob McNamaraMiguel MonteroMatthew ReeceTom RudeliusIrene ValenzuelaSpringerOpenarticleGauge SymmetryGlobal SymmetriesSuperstrings and Heterotic StringsBrane Dynamics in Gauge TheoriesNuclear and particle physics. Atomic energy. RadioactivityQC770-798ENJournal of High Energy Physics, Vol 2021, Iss 11, Pp 1-76 (2021)
institution DOAJ
collection DOAJ
language EN
topic Gauge Symmetry
Global Symmetries
Superstrings and Heterotic Strings
Brane Dynamics in Gauge Theories
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
spellingShingle Gauge Symmetry
Global Symmetries
Superstrings and Heterotic Strings
Brane Dynamics in Gauge Theories
Nuclear and particle physics. Atomic energy. Radioactivity
QC770-798
Ben Heidenreich
Jacob McNamara
Miguel Montero
Matthew Reece
Tom Rudelius
Irene Valenzuela
Chern-Weil global symmetries and how quantum gravity avoids them
description Abstract We draw attention to a class of generalized global symmetries, which we call “Chern-Weil global symmetries,” that arise ubiquitously in gauge theories. The Noether currents of these Chern-Weil global symmetries are given by wedge products of gauge field strengths, such as F 2 ∧ H 3 and tr( F 2 2 $$ {F}_2^2 $$ ), and their conservation follows from Bianchi identities. As a result, they are not easy to break. However, it is widely believed that exact global symmetries are not allowed in a consistent theory of quantum gravity. As a result, any Chern-Weil global symmetry in a low-energy effective field theory must be either broken or gauged when the theory is coupled to gravity. In this paper, we explore the processes by which Chern-Weil symmetries may be broken or gauged in effective field theory and string theory. We will see that many familiar phenomena in string theory, such as axions, Chern-Simons terms, worldvolume degrees of freedom, and branes ending on or dissolving in other branes, can be interpreted as consequences of the absence of Chern-Weil symmetries in quantum gravity, suggesting that they might be general features of quantum gravity. We further discuss implications of breaking and gauging Chern-Weil symmetries for particle phenomenology and for boundary CFTs of AdS bulk theories. Chern-Weil global symmetries thus offer a unified framework for understanding many familiar aspects of quantum field theory and quantum gravity.
format article
author Ben Heidenreich
Jacob McNamara
Miguel Montero
Matthew Reece
Tom Rudelius
Irene Valenzuela
author_facet Ben Heidenreich
Jacob McNamara
Miguel Montero
Matthew Reece
Tom Rudelius
Irene Valenzuela
author_sort Ben Heidenreich
title Chern-Weil global symmetries and how quantum gravity avoids them
title_short Chern-Weil global symmetries and how quantum gravity avoids them
title_full Chern-Weil global symmetries and how quantum gravity avoids them
title_fullStr Chern-Weil global symmetries and how quantum gravity avoids them
title_full_unstemmed Chern-Weil global symmetries and how quantum gravity avoids them
title_sort chern-weil global symmetries and how quantum gravity avoids them
publisher SpringerOpen
publishDate 2021
url https://doaj.org/article/175c60efb2b74b4c9d9844b33ab413a8
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AT miguelmontero chernweilglobalsymmetriesandhowquantumgravityavoidsthem
AT matthewreece chernweilglobalsymmetriesandhowquantumgravityavoidsthem
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