Abstract

In the four-dimensional supersymmetric standard model extended with gauge singlets the lightest Higgs boson mass, M H , has an important contribution proportional to the squared of the superpotential coupling λ of singlets to Higgs fields, λ SH 1·H 2 . The requirement of perturbativity up to the unification scale yields an upper bound on M H ∼140 GeV. In extensions to theories with (longitudinal) extra dimensions at the TeV where such coupling exists and massive Kaluza-Klein states fall into N=2 representations, if either of the Higgs or singlet fields live in the bulk of the extra dimensions, the β-function of λ is suppressed due to the absence of anomalous dimension of hypermultiplets to leading order. This implies a slower running of λ and an enhancement of its low energy value. The M H upper bound increases to values M H ≲165 GeV.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.