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Title: Flavor symmetries and automatic enhancement in the 6D supergravity swampland

Abstract

We argue for the quantum-gravitational inconsistency of certain 6D $$\mathscr{N}$$ = (1,0) supergravity theories, whose anomaly-free gauge algebra g and hypermultiplet spectrum M were observed by Raghuram et al.to be realizable only as part of a larger gauge sector (g' ⊃ g, M' ⊃ M) in F-theory. To detach any reference to a string theoretic method of construction, we utilize flavor symmetries to provide compelling reasons why the vast majority of such (g, M) theories are not compatible with quantum gravity constraints, and how the “automatic enhancement” to (g',M') remedies this. In the first class of models, with g' = g ⊕ h, we show that there exists an unbroken flavor symmetry h acting on the matter M, which, if ungauged, would violate the no-global-symmetries hypothesis. This argument also applies to 1-form center symmetries, which govern the gauge group topology and massive states in representations different from those of massless states. In a second class, we find that g is incompatible with the flavor symmetry of certain supersymmetric strings that must exist by the completeness hypothesis.

Authors:
; ; ORCiD logo
Publication Date:
Research Org.:
Univ. of Pennsylvania, Philadelphia, PA (United States)
Sponsoring Org.:
USDOE Office of Science (SC), High Energy Physics (HEP); Simons Foundation; Slovenian Research Agency
OSTI Identifier:
1844009
Alternate Identifier(s):
OSTI ID: 1980031
Grant/Contract Number:  
SC0013528; 724069; P1-0306
Resource Type:
Published Article
Journal Name:
Physical Review D
Additional Journal Information:
Journal Name: Physical Review D Journal Volume: 105 Journal Issue: 4; Journal ID: ISSN 2470-0010
Publisher:
American Physical Society
Country of Publication:
United States
Language:
English
Subject:
79 ASTRONOMY AND ASTROPHYSICS; 71 CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS; gauge theories; higher-dimensional field theories; strings and branes; supergravity; symmetries

Citation Formats

Cvetič, Mirjam, Lin, Ling, and Turner, Andrew P. Flavor symmetries and automatic enhancement in the 6D supergravity swampland. United States: N. p., 2022. Web. doi:10.1103/PhysRevD.105.046005.
Cvetič, Mirjam, Lin, Ling, & Turner, Andrew P. Flavor symmetries and automatic enhancement in the 6D supergravity swampland. United States. https://doi.org/10.1103/PhysRevD.105.046005
Cvetič, Mirjam, Lin, Ling, and Turner, Andrew P. Tue . "Flavor symmetries and automatic enhancement in the 6D supergravity swampland". United States. https://doi.org/10.1103/PhysRevD.105.046005.
@article{osti_1844009,
title = {Flavor symmetries and automatic enhancement in the 6D supergravity swampland},
author = {Cvetič, Mirjam and Lin, Ling and Turner, Andrew P.},
abstractNote = {We argue for the quantum-gravitational inconsistency of certain 6D $\mathscr{N}$ = (1,0) supergravity theories, whose anomaly-free gauge algebra g and hypermultiplet spectrum M were observed by Raghuram et al.to be realizable only as part of a larger gauge sector (g' ⊃ g, M' ⊃ M) in F-theory. To detach any reference to a string theoretic method of construction, we utilize flavor symmetries to provide compelling reasons why the vast majority of such (g, M) theories are not compatible with quantum gravity constraints, and how the “automatic enhancement” to (g',M') remedies this. In the first class of models, with g' = g ⊕ h, we show that there exists an unbroken flavor symmetry h acting on the matter M, which, if ungauged, would violate the no-global-symmetries hypothesis. This argument also applies to 1-form center symmetries, which govern the gauge group topology and massive states in representations different from those of massless states. In a second class, we find that g is incompatible with the flavor symmetry of certain supersymmetric strings that must exist by the completeness hypothesis.},
doi = {10.1103/PhysRevD.105.046005},
journal = {Physical Review D},
number = 4,
volume = 105,
place = {United States},
year = {Tue Feb 08 00:00:00 EST 2022},
month = {Tue Feb 08 00:00:00 EST 2022}
}

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