Abstract

The new round of experiments, MEG II, COMET/Mu2e, and Mu3e, would soon start to push the $\mu \to e\gamma$, $\mu N \to eN$ conversion, and $\mu \to 3e$ frontier, while Belle II would probe $\tau \to \mu\gamma$ and $\tau \to 3\mu$. In the general two Higgs doublet model with extra Yukawa couplings, we show that all these processes probe the lepton flavor violating (LFV) dipole transition that arises from the two loop mechanism, with scalar-induced contact terms subdominant. This is because existing data suggest the extra Yukawa couplings $\rho_{\mu e},\, \rho_{ee} \lesssim \lambda_e$, while $\rho_{\tau\mu},\, \rho_{\tau\tau} \lesssim \lambda_\tau$ and $\rho_{tt} \lesssim \lambda_t$, with $\lambda_i$ the usual Yukawa coupling of the Standard Model (SM), where $\rho_{\mu e}\rho_{tt}$ and $\rho_{\tau\mu}\rho_{tt}$ enter the $\mu e\gamma$ and $\tau\mu\gamma$ two loop amplitudes, respectively. With the $B_s \to \mu\mu$ decay rate basically consistent with SM expectation, together with the $B_s$ mixing constraint, we show that $B_s \to \tau\tau$ would also be consistent with SM, while $B_s \to \tau\mu$ and $B \to K\tau\mu$ decays would be out of reach of projected sensitivities, in strong contrast with some models motivated by the B anomalies.

Highlights

  • The study of muon properties is practically the oldest subject of particle physics, but remains at the forefront of current research

  • We show that the MEG II search for μ → eγ would continue to probe ρμe ≲ λe ≪ λμ; ð5Þ

  • We show that the μ → eγ process probes the ρμeρtt product in general 2HDM (g2HDM), as well as cγρμe where cγ is the h-H mixing angle

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Summary

INTRODUCTION

The study of muon properties is practically the oldest subject of particle physics, but remains at the forefront of current research. For nondegenerate mH 1⁄4 300 GeV, mA 1⁄4 500 GeV, we find ρτμρτe=λeλτ ≲ 17 by MEG can be improved to 6.6 with MEG II, with the results similar for flipping H ↔ A It is the two loop mechanism [20] that is of interest for g2HDM, where the ρμe coupling induces μ → eγ decay by inserting the φ → γVÃ vertex [φ 1⁄4 h, H, A; see Fig. 1 (center) and 1(right)] related to the h → γγ process, with V 1⁄4 Z subdominant. Taking the extra top Yukawa coupling ρtt ≃ 1 while setting cγ 1⁄4 0, one maximizes the H, A effect but decouples the h boson This “BSM benchmark” is illustrated, where ρμe 1⁄4 ρeμ ≃ 0.3λe is taken to satisfy the current MEG bound of Eq (1) at mH or mA 1⁄4 200 GeV. We expect τ → eγ to be much suppressed compared with τ → μγ in g2HDM, as ρτe is expected to be much smaller than ρτμ

OTHER μFV PROCESSES
CONTRAST
BSM-enhanced
Purely BSM
SM-like
Contrasting g2HDM with “boldness”
From μFV to PS3
The bqll0 processes in g2HDM
Comparing g2HDM with PS3
DISCUSSION AND CONCLUSION

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