Abstract

The long-standing muon g − 2 anomaly has been confirmed recently at the Fermilab. The combined discrepancy from Fermilab and Brookhaven results shows a difference from the theory at a significance of 4.2 σ. In addition, the LHC has updated the lower mass bound of a pure wino. In this letter, we study to what extent the g − 2 can be explained in anomaly mediation scenarios, where the pure wino is the dominant dark matter component. To this end, we derive some model-independent constraints on the particle spectra and g − 2. We find that the g − 2 explanation at the 1σ level is driven into a corner if the higgsino threshold correction is suppressed. On the contrary, if the threshold correction is sizable, the g − 2 can be explained. In the whole viable parameter region, the gluino mass is at most 2 − 4 TeV, the bino mass is at most 2 TeV, and the wino dark matter mass is at most 1 − 2 TeV. If the muon g − 2 anomaly is explained in the anomaly mediation scenarios, colliders and indirect search for the dark matter may find further pieces of evidence in the near future. Possible UV models for the large threshold corrections are discussed.

Highlights

  • JHEP06(2021)029 representing the Higgsino threshold correction, μ the Higgsino mass parameter, tan β the ratio of the vacuum expectation values (VEVs) of the two higgs fields, and mA the MSSM higgs boson mass

  • We study to what extent the g − 2 can be explained in anomaly mediation scenarios, where the pure wino is the dominant dark matter component

  • We have assumed the wino LSP composes the dominant dark matter component, the thermal relic abundance of the pure wino in the mass range is smaller than the observed one

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Summary

Introduction

JHEP06(2021) representing the Higgsino threshold correction, μ the Higgsino mass parameter, tan β the ratio of the vacuum expectation values (VEVs) of the two higgs fields, and mA the MSSM higgs boson mass. When the higgsino threshold correction is negligible, L vanishes The split SUSY has higgsino as light as gaugino while others are much heavier [17,18,19]. The pure gravity mediation or mini-split SUSY has all other fields much heavier than the gauginos [20,21,22,23]. [24]) By taking account of a Higgs mediation [25], i.e. in the Higgs-anomaly mediation, the sfermions of the first two generations are as light as gauginos while others are heavy [26,27,28,29].3. We show that the g − 2 is difficult to be explained if the higgsino threshold correction is negligible, i.e. L ∼ 0. We do not consider a light higgsino because the enhanced DM-nucleon coupling is strongly disfavored by the direct detection experiments [37,38,39].4 The LHC data, sets a stringent bound on the wino LSP and the lepton mass: msmuons Mwino 660(474) GeV,

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