Generalized global symmetries
Abstract
A q-form global symmetry is a global symmetry for which the charged operators are of space-time dimension q; e.g. Wilson lines, surface defects, etc., and the charged excitations have q spatial dimensions; e.g. strings, membranes, etc. Many of the properties of ordinary global symmetries (q = 0) apply here. They lead to Ward identities and hence to selection rules on amplitudes. Such global symmetries can be coupled to classical background fields and they can be gauged by summing over these classical fields. These generalized global symmetries can be spontaneously broken (either completely or to a sub-group). They can also have ’t Hooft anomalies, which prevent us from gauging them, but lead to ’t Hooft anomaly matching conditions. Such anomalies can also lead to anomaly inflow on various defects and exotic Symmetry Protected Topological phases. In conclusion, our analysis of these symmetries gives a new unified perspective of many known phenomena and uncovers new results.
- Authors:
-
- Perimeter Inst. for Theoretical Physics, Waterloo, ON (Canada)
- State Univ. of New York (SUNY), Stony Brook, NY (United States). Simons Center for Geometry and Physics
- Inst. for Advanced Study, Princeton, NJ (United States). School of Natural Sciences
- Publication Date:
- Research Org.:
- Institute for Advanced Study, Princeton, NJ (United States)
- Sponsoring Org.:
- USDOE; Simons Foundation; United States-Israel Binational Science Foundation (BSF)
- OSTI Identifier:
- 1440979
- Grant/Contract Number:
- SC0009988; FG02-92ER40701; 2010/629
- Resource Type:
- Accepted Manuscript
- Journal Name:
- Journal of High Energy Physics (Online)
- Additional Journal Information:
- Journal Name: Journal of High Energy Physics (Online); Journal Volume: 2015; Journal Issue: 2; Journal ID: ISSN 1029-8479
- Publisher:
- Springer Berlin
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; Global Symmetries; Wilson; ’t Hooft and Polyakov loops; Topological States of Matter; Anomalies in Field and String Theories
Citation Formats
Gaiotto, Davide, Kapustin, Anton, Seiberg, Nathan, and Willett, Brian. Generalized global symmetries. United States: N. p., 2015.
Web. doi:10.1007/JHEP02(2015)172.
Gaiotto, Davide, Kapustin, Anton, Seiberg, Nathan, & Willett, Brian. Generalized global symmetries. United States. https://doi.org/10.1007/JHEP02(2015)172
Gaiotto, Davide, Kapustin, Anton, Seiberg, Nathan, and Willett, Brian. Thu .
"Generalized global symmetries". United States. https://doi.org/10.1007/JHEP02(2015)172. https://www.osti.gov/servlets/purl/1440979.
@article{osti_1440979,
title = {Generalized global symmetries},
author = {Gaiotto, Davide and Kapustin, Anton and Seiberg, Nathan and Willett, Brian},
abstractNote = {A q-form global symmetry is a global symmetry for which the charged operators are of space-time dimension q; e.g. Wilson lines, surface defects, etc., and the charged excitations have q spatial dimensions; e.g. strings, membranes, etc. Many of the properties of ordinary global symmetries (q = 0) apply here. They lead to Ward identities and hence to selection rules on amplitudes. Such global symmetries can be coupled to classical background fields and they can be gauged by summing over these classical fields. These generalized global symmetries can be spontaneously broken (either completely or to a sub-group). They can also have ’t Hooft anomalies, which prevent us from gauging them, but lead to ’t Hooft anomaly matching conditions. Such anomalies can also lead to anomaly inflow on various defects and exotic Symmetry Protected Topological phases. In conclusion, our analysis of these symmetries gives a new unified perspective of many known phenomena and uncovers new results.},
doi = {10.1007/JHEP02(2015)172},
journal = {Journal of High Energy Physics (Online)},
number = 2,
volume = 2015,
place = {United States},
year = {Thu Feb 26 00:00:00 EST 2015},
month = {Thu Feb 26 00:00:00 EST 2015}
}
Web of Science
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