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
Summary
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
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.