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Supersymmetric interpretation of the muon g – 2 anomaly

Motoi Endo, Koichi Hamaguchi, Sho Iwamoto, Teppei Kitahara

2021Journal of High Energy Physics91 citationsDOIOpen Access PDF

Abstract

A bstract The Fermilab Muon g − 2 collaboration recently announced the first result of measurement of the muon anomalous magnetic moment ( g − 2), which confirmed the previous result at the Brookhaven National Laboratory and thus the discrepancy with its Standard Model prediction. We revisit low-scale supersymmetric models that are naturally capable to solve the muon g − 2 anomaly, focusing on two distinct scenarios: chargino-contribution dominated and pure-bino-contribution dominated scenarios. It is shown that the slepton pair-production searches have excluded broad parameter spaces for both two scenarios, but they are not closed yet. For the chargino-dominated scenario, the models with $$ {m}_{{\tilde{\mu}}_{\mathrm{L}}}\gtrsim {m}_{{\tilde{\chi}}_1^{\pm }} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>m</mml:mi><mml:msub><mml:mover><mml:mi>μ</mml:mi><mml:mo>˜</mml:mo></mml:mover><mml:mi>L</mml:mi></mml:msub></mml:msub><mml:mo>≳</mml:mo><mml:msub><mml:mi>m</mml:mi><mml:msubsup><mml:mover><mml:mi>χ</mml:mi><mml:mo>˜</mml:mo></mml:mover><mml:mn>1</mml:mn><mml:mo>±</mml:mo></mml:msubsup></mml:msub></mml:math> are still widely allowed. For the bino-dominated scenario, we find that, although slightly non-trivial, the region with low tan β with heavy higgsinos is preferred. In the case of universal slepton masses, the low mass regions with $$ {m}_{\tilde{\mu}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>m</mml:mi><mml:mover><mml:mi>μ</mml:mi><mml:mo>˜</mml:mo></mml:mover></mml:msub></mml:math> ≲ 230 GeV can explain the g − 2 anomaly while satisfying the LHC constraints. Furthermore, we checked that the stau-bino coannihilation works properly to realize the bino thermal relic dark matter. We also investigate heavy staus case for the bino-dominated scenario, where the parameter region that can explain the muon g − 2 anomaly is stretched to $$ {m}_{\tilde{\mu}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>m</mml:mi><mml:mover><mml:mi>μ</mml:mi><mml:mo>˜</mml:mo></mml:mover></mml:msub></mml:math> ≲ 1 . 3 TeV.

Topics & Concepts

PhysicsMuonCharginoParticle physicsAnomalous magnetic dipole momentAnomaly (physics)Physics beyond the Standard ModelDark matterSupersymmetryMinimal Supersymmetric Standard ModelFermilabLarge Hadron ColliderNuclear physicsStandard Model (mathematical formulation)Parameter spaceStatisticsQuantum mechanicsHistoryMathematicsGauge (firearms)ArchaeologyParticle physics theoretical and experimental studiesComputational Physics and Python ApplicationsDark Matter and Cosmic Phenomena