Abstract

The extra-dimensional model in which the bulk geometry is a slice of anti-de Sitter space is a particularly attractive extension of the Standard Model as it allows to address the gauge hierarchy problem, as well as the mass hierarchy prevailing among fermions. However, to allow for the masses of the Kaluza–Klein excitations of the known particles to be near the Terascale without conflicting with the high-precision electroweak data, one needs to promote the gauge symmetry to a left–right structure SU(2)L×SU(2)R×U(1) which incorporates a new quark b′, the SU(2)R doublet partner of the heavy top quark. We show that this new quark will contribute to the main production process of Higgs bosons at the LHC: the gluon–gluon fusion mechanism which proceeds through heavy quark triangular loops. In most of the parameter space in which the measured values of the heavy t, b quark masses are reproduced, the gg→Higgs production cross section is significantly altered, even if the b′ quark is too heavy to be directly accessible, mb′≳1 TeV. Finally, we briefly discuss the new Higgs production and decay channels involving the b′ quark.

Highlights

  • The extra–dimensional model in which the bulk geometry is a slice of anti–de Sitter space is a attractive extension of the Standard Model as it allows to address the gauge hierarchy problem, as well as the mass hierarchy prevailing among fermions

  • The warped extra–dimensional scenario proposed by Randall and Sundrum (RS) [1] is a attractive extension of the Standard Model (SM)

  • If this extra–dimensional model is to solve the gauge hierarchy problem, the masses of the first Kaluza–Klein (KK) excitations of the SM gauge bosons must be in the vicinity of the TeV scale but such low masses lead to unacceptably large contributions [5] to the precisely measured electroweak observables [6]

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Summary

Introduction

The mass of the first KK excitation of the b′R should be relatively low as it is controlled by the same ct parameter as the top quark tR which must be sufficiently small in order to generate a large mt value.

Results
Conclusion
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