Probing new U(1) gauge symmetries via exotic Z → Z′γ decays

Abstract New U(1) gauge theories involving Standard Model (SM) fermions typically require additional electroweak fermions for anomaly cancellation. We study the non-decoupling properties of these new fermions, called anomalons, in the Z − Z′ − γ vertex function, reviewing the connection between the...

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Main Authors: Lisa Michaels, Felix Yu
Format: Article
Language:English
Published: SpringerOpen 2021-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP03(2021)120
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spelling doaj-2abe983ee4624c989654900b95f742da2021-03-14T12:03:48ZengSpringerOpenJournal of High Energy Physics1029-84792021-03-012021312910.1007/JHEP03(2021)120Probing new U(1) gauge symmetries via exotic Z → Z′γ decaysLisa Michaels0Felix Yu1PRISMA+ Cluster of Excellence & Mainz Institute for Theoretical Physics, Johannes Gutenberg UniversityPRISMA+ Cluster of Excellence & Mainz Institute for Theoretical Physics, Johannes Gutenberg UniversityAbstract New U(1) gauge theories involving Standard Model (SM) fermions typically require additional electroweak fermions for anomaly cancellation. We study the non-decoupling properties of these new fermions, called anomalons, in the Z − Z′ − γ vertex function, reviewing the connection between the full model and the effective Wess-Zumino operator. We calculate the exotic Z → Z′γ decay width in U(1) B−L and U(1) B models, where B and L denote the SM baryon and lepton number symmetries. For U(1) B−L gauge symmetry, each generation of SM fermions is anomaly free and the exotic Z → Z BL ′ γ $$ {Z}_{BL}^{\prime}\gamma $$ decay width is entirely induced by intragenerational mass splittings. In contrast, for U(1) B gauge symmetry, the existence of two distinct sources of chiral symmetry breaking enables a heavy, anomaly-free set of fermions to have an irreducible contribution to the Z → Z B ′ γ $$ {Z}_B^{\prime}\gamma $$ decay width. We show that the current LEP limits on the exotic Z → Z B ′ γ $$ {Z}_B^{\prime}\gamma $$ decay are weaker than previously estimated, and low-mass Z B ′ $$ {Z}_B^{\prime } $$ dijet resonance searches are currently more constraining. We present a summary of the current collider bounds on U(1) B and a projection for a TeraZ factory on the Z → Z B ′ γ $$ {Z}_B^{\prime}\gamma $$ exotic decay, and emphasize how the Z → Z′γ decay is emblematic of new anomalous U(1) gauge symmetries.https://doi.org/10.1007/JHEP03(2021)120Anomalies in Field and String TheoriesBeyond Standard ModelEffective Field TheoriesSpontaneous Symmetry Breaking
collection DOAJ
language English
format Article
sources DOAJ
author Lisa Michaels
Felix Yu
spellingShingle Lisa Michaels
Felix Yu
Probing new U(1) gauge symmetries via exotic Z → Z′γ decays
Journal of High Energy Physics
Anomalies in Field and String Theories
Beyond Standard Model
Effective Field Theories
Spontaneous Symmetry Breaking
author_facet Lisa Michaels
Felix Yu
author_sort Lisa Michaels
title Probing new U(1) gauge symmetries via exotic Z → Z′γ decays
title_short Probing new U(1) gauge symmetries via exotic Z → Z′γ decays
title_full Probing new U(1) gauge symmetries via exotic Z → Z′γ decays
title_fullStr Probing new U(1) gauge symmetries via exotic Z → Z′γ decays
title_full_unstemmed Probing new U(1) gauge symmetries via exotic Z → Z′γ decays
title_sort probing new u(1) gauge symmetries via exotic z → z′γ decays
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-03-01
description Abstract New U(1) gauge theories involving Standard Model (SM) fermions typically require additional electroweak fermions for anomaly cancellation. We study the non-decoupling properties of these new fermions, called anomalons, in the Z − Z′ − γ vertex function, reviewing the connection between the full model and the effective Wess-Zumino operator. We calculate the exotic Z → Z′γ decay width in U(1) B−L and U(1) B models, where B and L denote the SM baryon and lepton number symmetries. For U(1) B−L gauge symmetry, each generation of SM fermions is anomaly free and the exotic Z → Z BL ′ γ $$ {Z}_{BL}^{\prime}\gamma $$ decay width is entirely induced by intragenerational mass splittings. In contrast, for U(1) B gauge symmetry, the existence of two distinct sources of chiral symmetry breaking enables a heavy, anomaly-free set of fermions to have an irreducible contribution to the Z → Z B ′ γ $$ {Z}_B^{\prime}\gamma $$ decay width. We show that the current LEP limits on the exotic Z → Z B ′ γ $$ {Z}_B^{\prime}\gamma $$ decay are weaker than previously estimated, and low-mass Z B ′ $$ {Z}_B^{\prime } $$ dijet resonance searches are currently more constraining. We present a summary of the current collider bounds on U(1) B and a projection for a TeraZ factory on the Z → Z B ′ γ $$ {Z}_B^{\prime}\gamma $$ exotic decay, and emphasize how the Z → Z′γ decay is emblematic of new anomalous U(1) gauge symmetries.
topic Anomalies in Field and String Theories
Beyond Standard Model
Effective Field Theories
Spontaneous Symmetry Breaking
url https://doi.org/10.1007/JHEP03(2021)120
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AT felixyu probingnewu1gaugesymmetriesviaexoticzzgdecays
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