1993
DOI: 10.1016/0550-3213(93)90111-2
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More about discrete gauge anomalies

Abstract: I discuss and extend several results concerning the cancellation of discrete gauge anomalies. I show how heavy fermions do not decouple in the presence of discrete gauge anomalies. As a consequence, in general, cancellation of discrete gauge anomalies cannot be described merely in terms of low energy operators involving only the light fermions. I also discuss cancellation of discrete gauge anomalies through a discrete version of the Green-Schwarz (GS) mechanism as well as the possibility of discrete gauge R-sy… Show more

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Cited by 89 publications
(45 citation statements)
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“…Assuming this condition to hold we show that the discrete Z 2 gauge anomalies are automatically cancelled for any flux which satisfies our modified transversality condition. This is indeed required [16,54] because for the type of genus-one fibrations considered here, the discrete symmetry is non-perturbatively exact [55,56]. This is the final non-trivial check for our construction.…”
Section: Jhep01(2016)098mentioning
confidence: 99%
See 1 more Smart Citation
“…Assuming this condition to hold we show that the discrete Z 2 gauge anomalies are automatically cancelled for any flux which satisfies our modified transversality condition. This is indeed required [16,54] because for the type of genus-one fibrations considered here, the discrete symmetry is non-perturbatively exact [55,56]. This is the final non-trivial check for our construction.…”
Section: Jhep01(2016)098mentioning
confidence: 99%
“…In general, discrete field theoretic anomalies need not vanish by themselves provided they are cancelled by a suitable discrete version of the Green-Schwarz mechanism [54]. This happens when an anomalous U(1) is Higgsed to a discrete subgroup which is also anomalous.…”
Section: Cancellation Of Z 2 Anomaliesmentioning
confidence: 99%
“…In some cases they are gauged in the σ-model sense, and their anomalies are cancelled by a Green-Schwarz mechanism, see e.g. [75][76][77][78][79][80][81][82][83]. They are eventually broken upon SUSY breaking by dimension < 4 operators.…”
Section: Embedding Into the U(1) S R-symmetrymentioning
confidence: 99%
“…Further constraints on the charges α Q and α L could be obtained by considering discrete gauge anomalies [10,13]. Unless the anomalies cancel, it is impossible for the discrete symmetry to be a remnant of a gauged U(1).…”
Section: Anomaliesmentioning
confidence: 99%
“…Unfortunately, discrete anomalies are notoriously ambiguous [12,13]. Theoretically, we should have several anomalies to consider.…”
Section: Anomaliesmentioning
confidence: 99%