Abstract

We construct models with minimal field content that can simultaneously explain the muon g − 2 anomaly and give the correct dark matter relic abundance. These models fall into two general classes, whether or not the new fields couple to the Higgs. For the general structure of models without new Higgs couplings, we provide analytical expressions that only depend on the SU(2)L representation. These results allow to demonstrate that only few models in this class can simultaneously explain (g − 2)μ and account for the relic abundance. The experimental constraints and perturbativity considerations exclude all such models, apart from a few fine-tuned regions in the parameter space, with new states in the few 100 GeV range. In the models with new Higgs couplings, the new states can be parametrically heavier by a factor sqrt{1/{y}_{mu }} , with yμ the muon Yukawa coupling, resulting in masses for the new states in the TeV regime. At present these models are not well constrained experimentally, which we illustrate on two representative examples.

Highlights

  • The explanation of Dark Matter (DM) requires physics beyond the Standard Model (SM)

  • We assume that the DM particle χ with mass mχ is a thermal relic, so that its relic density is primarily determined by its annihiliation to SM particles

  • In this paper we have performed a systematic study of models with minimal field content that can simultaneously address the muon g − 2 anomaly and account for the observed DM relic density

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Summary

Introduction

The explanation of Dark Matter (DM) requires physics beyond the Standard Model (SM). A plausible possibility is that DM is a new stable neutral particle with electroweak scale mass that is a thermal relic. To test concrete realizations of this scenario it often suffices to use simplified models These keep only the minimal set of phenomenologically relevant fields out of the full set contained in complete new physics models. It is possible to build minimal extensions of the SM addressing the muon g − 2 anomaly with a single new field — as systematically discussed in [11,12,13,14] — including leptoquarks [15, 16], a second Higgs doublet [17, 18], and axion-like particles [19].

General setup
Phenomenology
DM relic density
DM direct detection
Electroweak precision observables
LHC phenomenology
Models without Higgs insertion
General structure of LL models
General structure of RR models
Numerical results
Models with Higgs insertion
General discussion of FLR and SLR models
Numerical results for the FLR1 model
Numerical results for the SLR1 model
Summary and conclusions
A Electroweak representations
B Lagrangians for explicit models
C Correction to the Zμμ vertex
Full Text
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