Abstract

The Mu2e and COMET collaborations will search for nucleus-catalyzed muon conversion to positrons (${\ensuremath{\mu}}^{\ensuremath{-}}\ensuremath{\rightarrow}{e}^{+}$) as a signal of lepton number violation. A key background for this search is radiative muon capture where either (1) a real photon converts to an ${e}^{+}{e}^{\ensuremath{-}}$ pair ``externally'' in surrounding material, or (2) a virtual photon mediates the production of an ${e}^{+}{e}^{\ensuremath{-}}$ pair ``internally.'' If the ${e}^{+}$ has an energy approaching the signal region then it can serve as an irreducible background. In this work we describe how the near end point internal positron spectrum can be related to the real photon spectrum from the same nucleus, which encodes all nontrivial nuclear physics.

Highlights

  • Charged lepton flavor violation (CLFV) is a smoking gun signature of physics beyond the Standard Model (SM) and is one of the most sought-after signals at the intensity frontier [1,2,3,4]

  • We have shown that given the photon spectrum from radiative muon capture (RMC) on a nucleus, the spectrum of high energy positrons or electrons can be computed accurately with errors controlled by δ 1⁄4 ðE− − meÞ=q0

  • External positrons, stemming from real photons pair producing in surrounding detector material, can be calculated from the realphoton spectrum by dedicated Monte Carlo simulations that include the full detector geometry

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Summary

INTRODUCTION

Charged lepton flavor violation (CLFV) is a smoking gun signature of physics beyond the Standard Model (SM) and is one of the most sought-after signals at the intensity frontier [1,2,3,4]. In the case of external conversion, nuclear model uncertainties can be circumvented at either Mu2e or COMET by directly measuring the real photon spectrum from RMC on aluminium. With this information in hand, dedicated Monte Carlo simulations (including the full detector geometry) can be used to predict the resultant electron and positron spectra. Analysis presented in the main text to the case of inclusive final states

RADIATIVE MUON CAPTURE ON A NUCLEUS
REAL PHOTON SPECTRUM
POSITRON SPECTRUM
NEAR END POINT SPECTRUM
CONCLUSIONS AND OUTLOOK
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