Abstract

The Supersymmetric Custodial Triplet Model (SCTM) adds to the particle content of the MSSM three $SU(2)_L$ triplet chiral superfields with hypercharge $Y=(0,\pm1)$. At the superpotential level the model respects a global $SU(2)_L \otimes SU(2)_R$ symmetry only broken by the Yukawa interactions. The pattern of vacuum expectation values of the neutral doublet and triplet scalar fields depends on the symmetry pattern of the Higgs soft breaking masses. We study the cases where this symmetry is maintained in the Higgs sector, and when it is broken only by the two doublets attaining different vacuum expectation values. In the former case, the symmetry is spontaneously broken down to the vectorial subgroup $SU(2)_V$ and the $\rho$ parameter is protected by the custodial symmetry. However in both situations the $\rho$ parameter is protected at tree level, allowing for light triplet scalars with large vacuum expectation values. We find that over a large range of parameter space, a light neutralino can supply the correct relic abundance of dark matter either through resonant s-channel triplet scalar funnels or well tempering of the Bino with the triplet fermions. Direct detection experiments have trouble probing these model points because the custodial symmetry suppresses the coupling of the neutralino and the $Z$ and a small Higgsino component of the neutralino suppresses the coupling with the Higgs. Likewise the annihilation cross sections for indirect detection lie below the Fermi-LAT upper bounds for the different channels.

Highlights

  • The Standard Model (SM) of strong and electroweak interactions is incredibly successful in explaining all high- and low-energy particle physics data, it is known to be incomplete

  • We focus on dark matter coming from the neutralino sector of the supersymmetric custodial triplet model (SCTM) [37,38] in which the content of the minimal supersymmetric Standard Model (MSSM) is extended by three triplets with hypercharge Y 1⁄4 ð0; Æ1Þ

  • We have studied a supersymmetric model in which the Higgs sector of the superpotential is extended by three SUð2ÞL triplet fields and is manifestly invariant under SUð2ÞL ⊗ SUð2ÞR

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Summary

INTRODUCTION

The Standard Model (SM) of strong and electroweak interactions is incredibly successful in explaining all high- and low-energy particle physics data, it is known to be incomplete. The recent discovery of the Higgs by the ATLAS [3] and CMS [4] experiments seems to point toward a single SUð2ÞL doublet as being responsible for the breaking of the electroweak symmetry This cannot be known for sure without more precise measurements of its properties. We assume a Higgs sector with a potential allowing for a noncustodial vacuum, provided that this only comes from the ratio of the doublet vacuum expectation values (VEVs), parametrized by tan β. This turns out to be a very good approximation to the situation explored in Ref.

NEUTRALINO DARK MATTER
SCALAR MASSES
NEUTRALINO MIXING
DARK MATTER
Thermal relic density
Direct detection
Indirect detection
Findings
DISCUSSION AND CONCLUSIONS
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