Abstract

We propose a minimal and self-contained model in non-compact flat five dimensions which localizes the Standard Model (SM) on a domain wall. Localization of gauge fields is achieved by the condensation of Higgs field via a Higgs dependent gauge kinetic term in five-dimensional Lagrangian. The domain wall connecting vacua with unbroken gauge symmetry drives the Higgs condensation which provides both electroweak symmetry breaking and gauge field localization at the same time. Our model predicts higher-dimensional interactions $|H|^{2n}(F_{\mu\nu})^2$ in the low-energy effective theory. This leads to two expectations: The one is a new tree-level contribution to $H \to \gamma\gamma$ ($H \to gg$) decay whose signature is testable in future LHC experiment. The other is a finite electroweak monopole which may be accessible to the MoEDAL experiment. Interactions of translational Nambu-Goldstone boson is shown to satisfy a low-energy theorem.

Highlights

  • The hypothesis that our four-dimensional world is embedded in higher-dimensional spacetime has been a hot topic in high energy physics for decades

  • Let us highlight several results: We investigated the geometric Higgs mechanism which is the conventional Higgs mechanism driven by the positions of multiple domain walls in an extra dimension in Ref. [49]

  • We propose a minimal and self-contained model in non-compact flat five dimensions which localizes the Standard Model (SM) on a domain wall

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Summary

INTRODUCTION

The hypothesis that our four-dimensional world is embedded in higher-dimensional spacetime has been a hot topic in high energy physics for decades. Non-trivial gauge kinetic term (I.1) by extending the Rξ gauge in any spacetime dimensions D [51] Another group recently studied the SM in a similar model with β2 taken as a given background in D = 5 [52, 53]. The Higgs field is an active player in five dimensions with a new role as a localizing agent of gauge fields on the domain wall, in addition to the conventional roles giving masses to gauge bosons and fermions. We point out that the localization via Eq (I.1) yields higher dimensional interactions |H|2n(Fμν) in the low-energy effective theory and it provides a natural reason to have a finite electroweak monopole solution. We explain how a domain wall drives condensation of the Higgs field and at the same time localizes massless/massive gauge bosons and chiral fermions.

A HIGGS MECHANISM
Mass scales
Translational zero mode
Generalized models
THE STANDARD MODEL
FINITE ELECTROWEAK MONOPOLES
CONCLUSIONS AND DISCUSSION
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