Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons

Abstract We consider experimental constraints in the MeV region in order to determine the parameter space for the U(1) X extension of the Standard Model, presented in the first part of our work. In particular, we focus on the model UV-completed by cold WIMPs. We conclude that the electron anomalous...

Full description

Bibliographic Details
Main Authors: F. C. Correia, Svjetlana Fajfer
Format: Article
Language:English
Published: SpringerOpen 2019-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP10(2019)279
id doaj-c73644c2ea674b3c93ea40fe03ba3d17
record_format Article
spelling doaj-c73644c2ea674b3c93ea40fe03ba3d172020-11-25T04:06:07ZengSpringerOpenJournal of High Energy Physics1029-84792019-10-0120191013010.1007/JHEP10(2019)279Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosonsF. C. Correia0Svjetlana Fajfer1Institut für Physik, Technische Universität DortmundDepartment of Physics, University of LjubljanaAbstract We consider experimental constraints in the MeV region in order to determine the parameter space for the U(1) X extension of the Standard Model, presented in the first part of our work. In particular, we focus on the model UV-completed by cold WIMPs. We conclude that the electron anomalous magnetic moment and the neutrino trident production provide the most stringent bounds to g X 2 $$ {g}_X^2 $$ ∼ 10 −6 in the mass interval below the di-muon threshold. By allowing the axial-vector coupling of the dark gauge boson Z′, the interference effect with the SM gauge bosons may reduce the bounds coming from the neutrino trident production. At the same time, such coupling allows a region of the parameter space already favored both by the relic abundance and by the discrepancy between experimental result and theoretical prediction for the muon anomalous magnetic moment. We emphasize that light-Z′ interactions, non-universal for the two first lepton families, necessarily create a difference in the proton charge radius measured in the Lamb shift of the e-hydrogen and μ-hydrogen. Finally, we determine the effects of the new gauge boson on the forward-backward asymmetry in e + e − → f ¯ f $$ \overline{f}f $$ = μ, τ, and on the leptonic decays M → jν j l + l − , where M = π, K, D, D s , B and j, l = e, μ.http://link.springer.com/article/10.1007/JHEP10(2019)279Beyond Standard ModelHiggs PhysicsNeutrino Physics
collection DOAJ
language English
format Article
sources DOAJ
author F. C. Correia
Svjetlana Fajfer
spellingShingle F. C. Correia
Svjetlana Fajfer
Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons
Journal of High Energy Physics
Beyond Standard Model
Higgs Physics
Neutrino Physics
author_facet F. C. Correia
Svjetlana Fajfer
author_sort F. C. Correia
title Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons
title_short Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons
title_full Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons
title_fullStr Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons
title_full_unstemmed Light mediators in anomaly free U (1) X models. Part II. Constraints on dark gauge bosons
title_sort light mediators in anomaly free u (1) x models. part ii. constraints on dark gauge bosons
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-10-01
description Abstract We consider experimental constraints in the MeV region in order to determine the parameter space for the U(1) X extension of the Standard Model, presented in the first part of our work. In particular, we focus on the model UV-completed by cold WIMPs. We conclude that the electron anomalous magnetic moment and the neutrino trident production provide the most stringent bounds to g X 2 $$ {g}_X^2 $$ ∼ 10 −6 in the mass interval below the di-muon threshold. By allowing the axial-vector coupling of the dark gauge boson Z′, the interference effect with the SM gauge bosons may reduce the bounds coming from the neutrino trident production. At the same time, such coupling allows a region of the parameter space already favored both by the relic abundance and by the discrepancy between experimental result and theoretical prediction for the muon anomalous magnetic moment. We emphasize that light-Z′ interactions, non-universal for the two first lepton families, necessarily create a difference in the proton charge radius measured in the Lamb shift of the e-hydrogen and μ-hydrogen. Finally, we determine the effects of the new gauge boson on the forward-backward asymmetry in e + e − → f ¯ f $$ \overline{f}f $$ = μ, τ, and on the leptonic decays M → jν j l + l − , where M = π, K, D, D s , B and j, l = e, μ.
topic Beyond Standard Model
Higgs Physics
Neutrino Physics
url http://link.springer.com/article/10.1007/JHEP10(2019)279
work_keys_str_mv AT fccorreia lightmediatorsinanomalyfreeu1xmodelspartiiconstraintsondarkgaugebosons
AT svjetlanafajfer lightmediatorsinanomalyfreeu1xmodelspartiiconstraintsondarkgaugebosons
_version_ 1724432371211567104