Abstract

Using properties of Goldstino, we show that in generic grand unified theories with gravity-mediated supersymmetry breaking the $\ensuremath{\mu}$-problem is nonexistent. What happens is that supersymmetry breaking universally induces the shifts of the heavy fields that generate $\ensuremath{\mu}$ and ${B}_{\ensuremath{\mu}}$ terms. In the leading order, these are given by the mass of gravitino and are insensitive to the scale of grand unification. The mechanism works regardless whether doublet-triplet splitting is achieved via fine-tuning or not. Moreover, we illustrate this general phenomenon on explicit examples of theories that achieve doublet-triplet splitting dynamically. These include the theories with Higgs doublet as a pseudo-Goldstone boson, as well as the approach based on spontaneous decoupling of the light color triplet from quarks and leptons.

Highlights

  • The hierarchy problem in supersymmetry (SUSY) comes in form of two puzzles

  • What happens is that supersymmetry breaking universally induces the shifts of the heavy fields that generate μ and Bμ terms

  • The mechanism works regardless whether doublet-triplet splitting is achieved via fine-tuning or not. We illustrate this general phenomenon on explicit examples of theories that achieve doublet-triplet splitting dynamically. These include the theories with Higgs doublet as a pseudo-Goldstone boson, as well as the approach based on spontaneous decoupling of the light color triplet from quarks and leptons

Read more

Summary

INTRODUCTION

The hierarchy problem in supersymmetry (SUSY) comes in form of two puzzles. The first one is the origin of supersymmetry breaking. As long as the theory delivers a pair of massless Higgs doublets in supersymmetric limit, the generation of μ and Bμ of the form (3) is generic This way of generating μ has been incorporated in the past within particular scenarios, most notably, within the pseudo-Goldstone approach to the doublet-triplet splitting problem [6,7] (see [8,9,10,11,12,13,14,15]). In these scenarios, in SUSY limit, the Higgs doublets are massless by Goldstone theorem. In the present paper we shall only be concerned with the question of leading order correlation between μ and m3=2

GOLDSTINO ARGUMENT
SIMPLE EXAMPLE
DECOUPLING
Example with fine-tuning
Example
Example: decoupled triplet
COMPARISON WITH LOW-ENERGY SOLUTIONS OF THE μ-PROBLEM
CONCLUSIONS

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.