LHC signals of the SO(5)×U(1) gauge-Higgs unification

We study the LHC signals of SO(5)×U(1) gauge-Higgs unification as a beyond the standard model (SM). When the extra dimensional space is not simply-connected, dynamics of the Aharonov-Bohm (AB) phase, θH, in the extra dimension can induce dynamical gauge symmetry breaking by the Hosotani mechanism. T...

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Main Author: Shimotani Takuya
Format: Article
Language:English
Published: EDP Sciences 2015-01-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20149504062
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author Shimotani Takuya
author_facet Shimotani Takuya
author_sort Shimotani Takuya
collection DOAJ
description We study the LHC signals of SO(5)×U(1) gauge-Higgs unification as a beyond the standard model (SM). When the extra dimensional space is not simply-connected, dynamics of the Aharonov-Bohm (AB) phase, θH, in the extra dimension can induce dynamical gauge symmetry breaking by the Hosotani mechanism. The Kaluza-Klein (KK) mass spectra of γ, Z, ZR and Higgs self couplings obey universal relations with θH in the fifth dimension. In our model, three neutral gauge bosons, Z′ bosons, appear at TeV scale. Z′ bosons are the first KK modes ZR(1), Z(1), and γ(1). We analyze Z′ bosons through dilepton events at LHC. For θH = 0.114, the mass and decay width of ZR(1), Z(1), and γ(1) are (5.73, 482), (6.07, 342), and (6.08 TeV, 886 GeV), respectively. For θH = 0.073 their masses are 8.00 ∼ 8.61 TeV. An excess of events in the dilepton invariant mass should be observed in the Z′ search at the upgraded LHC at 14 TeV.
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spelling doaj.art-9711ff0462ea4f21bc45155c4d222c362022-12-21T22:33:53ZengEDP SciencesEPJ Web of Conferences2100-014X2015-01-01950406210.1051/epjconf/20149504062epjconf_icnfp2014_04062LHC signals of the SO(5)×U(1) gauge-Higgs unificationShimotani Takuya0Department of Physics, Osaka UniversityWe study the LHC signals of SO(5)×U(1) gauge-Higgs unification as a beyond the standard model (SM). When the extra dimensional space is not simply-connected, dynamics of the Aharonov-Bohm (AB) phase, θH, in the extra dimension can induce dynamical gauge symmetry breaking by the Hosotani mechanism. The Kaluza-Klein (KK) mass spectra of γ, Z, ZR and Higgs self couplings obey universal relations with θH in the fifth dimension. In our model, three neutral gauge bosons, Z′ bosons, appear at TeV scale. Z′ bosons are the first KK modes ZR(1), Z(1), and γ(1). We analyze Z′ bosons through dilepton events at LHC. For θH = 0.114, the mass and decay width of ZR(1), Z(1), and γ(1) are (5.73, 482), (6.07, 342), and (6.08 TeV, 886 GeV), respectively. For θH = 0.073 their masses are 8.00 ∼ 8.61 TeV. An excess of events in the dilepton invariant mass should be observed in the Z′ search at the upgraded LHC at 14 TeV.http://dx.doi.org/10.1051/epjconf/20149504062
spellingShingle Shimotani Takuya
LHC signals of the SO(5)×U(1) gauge-Higgs unification
EPJ Web of Conferences
title LHC signals of the SO(5)×U(1) gauge-Higgs unification
title_full LHC signals of the SO(5)×U(1) gauge-Higgs unification
title_fullStr LHC signals of the SO(5)×U(1) gauge-Higgs unification
title_full_unstemmed LHC signals of the SO(5)×U(1) gauge-Higgs unification
title_short LHC signals of the SO(5)×U(1) gauge-Higgs unification
title_sort lhc signals of the so 5 u 1 gauge higgs unification
url http://dx.doi.org/10.1051/epjconf/20149504062
work_keys_str_mv AT shimotanitakuya lhcsignalsoftheso5u1gaugehiggsunification