Abstract

The recent confirmation of the muon g-2 anomaly by the Fermilab g-2 experiment may harbinger a new era in mu and tau physics. In the context of general two Higgs doublet model, the discrepancy can be explained via one-loop exchange of sub-TeV exotic scalar and pseudoscalars, namely H and A, that have flavor changing neutral couplings rho _{tau mu } and rho _{mu tau } at sim 20 times the usual tau Yukawa coupling, lambda _tau . Taking rho _{ell ell ^prime }sim lambda _{ mathrm min(ell , ell ^prime )}, we show that the above solution to muon g-2 then predicts enhanced rates of various charged lepton flavor violating processes, which should be accessible at upcoming experiments. We cover muon related processes such as mu rightarrow e gamma , mu rightarrow eee and mu N rightarrow e N, and tau decays tau rightarrow mu gamma and tau rightarrow mu mu mu . A similar one-loop diagram with rho _{etau }= rho _{tau e} = mathcal{O}(lambda _e) induces mu rightarrow egamma , bringing the rate right into the sensitivity of the MEG II experiment. The mu egamma dipole can be probed further by mu rightarrow 3e and mu N rightarrow eN. With its promised sensitivity range and ability to use different nuclei, the mu N rightarrow eN conversion experiments can not only make discovery, but access the extra diagonal quark Yukawa couplings rho _{qq}. For the tau lepton, we find that tau rightarrow mu gamma would probe rho _{tau tau } down to lambda _tau or lower, while tau rightarrow 3mu would probe rho _{mu mu } to mathcal{O}(lambda _{mu }).

Highlights

  • In 1948, Schwinger presented his result [1] for the “anomalous” magnetic moment of the electron, ae ≡/2 α/2π

  • We find that μ → eγ can be enhanced in g2HDM to experimentally accessible values, even for exceptionally small extra Yukawa coupling ρτe = O(λe)

  • This is in context of using large ρτμ coupling to explain the muon g − 2 anomaly

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Summary

Introduction

In 1948, Schwinger presented his result [1] for the “anomalous” magnetic moment of the electron, ae ≡ (ge − 2)/2 α/2π. Many works have discussed charged LFV processes in g2HDM previously, in the context of the muon g − 2 anomaly [26–31]. We shall highlight μN → eN as the ultimate probe of LFV in g2HDM Both μeγ dipole and μeqq contact terms, as well as their interference, play important roles, and can be used to infer the sign of mass splitting, m = m A − m H , which is important for the explanation of muon g − 2 in g2HDM. Before turning to numerical results for μ → eγ , let us quickly recall the muon g − 2 solution in g2HDM [9] This will provide a constraint on ρτμ and help define benchmark masses for heavy scalars.

Two-loop contributions
Dipole dominance
Contact interactions
Two-loop mechanism
Findings
Discussion and summary
Full Text
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