2017
DOI: 10.1007/jhep08(2017)110
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Spontaneous breaking of gauge groups to discrete symmetries

Abstract: Many models of beyond Standard Model physics connect flavor symmetry with a discrete group. Having this symmetry arise spontaneously from a gauge theory maintains compatibility with quantum gravity and can be used to systematically prevent anomalies. We minimize a number of Higgs potentials that break gauge groups to discrete symmetries of interest, and examine their scalar mass spectra.

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Cited by 17 publications
(17 citation statements)
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“…Despite the measurement of a non-zero reactor angle, it remains an intriguing possibility that the large mixing angles in the lepton sector can be explained using some discrete non-Abelian family symmetry [1,2]. The origin of such a symmetry could either be a continuous non-Abelian gauge symmetry, broken to a discrete subgroup [3][4][5][6][7][8][9], or it could emerge from extra dimensions [10][11][12][13][14][15][16][17][18][19][20][21], either as an accidental symmetry of the orbifold fixed points, or as a subgroup of the symmetry of the extra dimensional lattice vectors, commonly referred to as modular symmetry [22][23][24].…”
Section: Introductionmentioning
confidence: 99%
“…Despite the measurement of a non-zero reactor angle, it remains an intriguing possibility that the large mixing angles in the lepton sector can be explained using some discrete non-Abelian family symmetry [1,2]. The origin of such a symmetry could either be a continuous non-Abelian gauge symmetry, broken to a discrete subgroup [3][4][5][6][7][8][9], or it could emerge from extra dimensions [10][11][12][13][14][15][16][17][18][19][20][21], either as an accidental symmetry of the orbifold fixed points, or as a subgroup of the symmetry of the extra dimensional lattice vectors, commonly referred to as modular symmetry [22][23][24].…”
Section: Introductionmentioning
confidence: 99%
“…In this case, the discrete symmetry cannot be imposed directly, as it is in conflict with gauge invariance. However, it might be available as the remaining symmetry of a larger, spontaneously broken gauge group, see, e.g., [105]. In summary, in constructing QFTs, one a priori has a large amount of freedom in choosing the fundamental symmetries.…”
Section: Discussionmentioning
confidence: 99%
“…It is a suggestive pattern: matching the representations of the gauge group to those of the discrete group. The mother symmetry could be E 6 × G f , where G f is a continuous group that contains T 13 [43].…”
Section: Theoretical Musingsmentioning
confidence: 99%