Abstract

A massive $U(1)^{\prime}$ gauge boson known as a "dark photon" or $A^{\prime}$, has long been proposed as a potential explanation for the discrepancy observed between the experimental measurement and theoretical determination of the anomalous magnetic moment of the muon, ($g_{\mu} - 2$) anomaly. Recently, experimental results have excluded this possibility for a dark photon exhibiting exclusively visible or invisible decays. In this work, we revisit this idea and consider a model where $A^{\prime}$ couples inelastically to dark matter and an excited dark sector state, leading to a more exotic decay topology we refer to as a semi-visible decay. We show that for large mass splittings between the dark sector states this decay mode is enhanced, weakening the previous invisibly decaying dark photon bounds. As a consequence, $A^{\prime}$ resolves the $g_{\mu} - 2$ anomaly in a region of parameter space the thermal dark matter component of the Universe is readily explained. Interestingly, it is possible that the semi-visible events we discuss may have been vetoed by experiments searching for invisible dark photon decays. A re-analysis of the data and future searches may be crucial in uncovering this exotic decay mode or closing the window on the dark photon explanation of the $g_{\mu} - 2$ anomaly.

Highlights

  • The anomalous magnetic moment of the muon aμ ≡ ðgμ − 2Þ=2 remains to this day one of the few outstanding problems in particle physics

  • The primary goal of this paper is to illustrate that in an iDM model with large mass splittings (Δ ≳ 40%) we can significantly weaken the existing limits such that the previously excluded 2σ dark photon explanation of the gμ − 2 anomaly is still viable, and in a region of parameter space the thermal relic dark matter abundance is readily explained

  • We have shown that a dark photon coupled to inelastic dark matter can explain both the ∼3.7σ discrepancy observed in the anomalous magnetic moment of the muon, 115001-4

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Summary

Introduction

The anomalous magnetic moment of the muon aμ ≡ ðgμ − 2Þ=2 remains to this day one of the few outstanding problems in particle physics. A difference between theory and experiment of. Δaμ ≡ aeμxp − atμh 1⁄4 ð274 Æ 73Þ × 10−11; ð1Þ has resulted in a ∼3.7σ discrepancy [1,2] which is yet to be understood. While impressive agreement has existed between the Standard Model (SM) prediction and measurements on the electron’s anomalous magnetic moment ae [3], a recent improvement in the determination of the fine structure constant α from atomic Cesium measurements [4] has pushed the discrepancy in Δae from ∼1.7σ to ∼2.4σ with opposite sign to that of the muon [5,6,7].1

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