Abstract

Flavor violating processes in the lepton sector have highly suppressed branching ratios in the standard model mainly due to the tiny neutrino mass. This means that observing lepton flavor violation (LFV) in the next round of experiments would constitute a clear indication of physics beyond the standard model (BSM). We revisit a discussion of one possible way to search for LFV, muonium-antimuonium oscillations. This process violates muon lepton number by two units and could be sensitive to the types of BSM physics that are not probed by other types of LFV processes. Using techniques of effective field theory, we calculate the mass and width differences of the mass eigenstates of muonium. We argue that its invisible decays give the parametrically leading contribution to the lifetime difference and put constraints on the scales of new physics probed by effective operators in muonium oscillations.

Highlights

  • Flavor-changing neutral current (FCNC) interactions serve as a powerful probe of physics beyond the standard model (BSM)

  • Since no local operators generate FCNCs in the standard model (SM) at tree level, new physics (NP) degrees of freedom can effectively compete with the SM particles running in the loop graphs, making their discovery possible

  • Eq (16) contains terms that do not follow from the dimension six in the standard model effective field theory (SMEFT) but could be generated by higher order operators

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Summary

INTRODUCTION

Flavor-changing neutral current (FCNC) interactions serve as a powerful probe of physics beyond the standard model (BSM). Since no local operators generate FCNCs in the standard model (SM) at tree level, new physics (NP) degrees of freedom can effectively compete with the SM particles running in the loop graphs, making their discovery possible. This is, only true provided the BSM models include flavor-violating interactions. Even in this case, a subsequent application of two ΔL 1⁄4 1 interactions would generate an effective ΔL 1⁄4 2 interaction.

PHENOMENOLOGY OF MUONIUM OSCILLATIONS
EFFECTIVE THEORY OF OSCILLATIONS
Mass difference
Paramuonium
Orthomuonium
Width difference
EXPERIMENTAL CONSTRAINTS
CONCLUSIONS
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