Abstract

We explore the interplay between $h(125) \to \tau\mu$ search at the LHC and $\tau \to \mu\gamma$ at the up and coming Belle~II experiment, in context of the general two Higgs doublet model with extra Yukawa couplings such as $\rho_{\tau\mu}$. The search for $h \to \tau\mu$ constrains $\rho_{\tau\mu} \cos\gamma$, where $\cos\gamma$ is the $h$--$H$ mixing angle of $h$ with the exotic $CP$-even scalar $H$. For $\tau \to \mu\gamma$, we define the "BSM-benchmark" by setting the extra top Yukawa coupling $\rho_{tt} = 1\ (\cong \lambda_t)$ in two-loop diagrams, and $\cos\gamma = 0$ to decouple $h$. We show that this leading effect due to $H$ and $CP$-odd scalar $A$ can be readily probed by Belle~II, even for the conservative value of $\rho_{\tau\mu} = 0.7\lambda_\tau$. We define the subleading "$h$-benchmark" by setting $\rho_{tt} = 0$ in two-loop diagrams, and take the conservative maximal value of $\cos\gamma = 0.2$. We show that it falls beyond Belle~II reach, but can interfere with the BSM-benchmark effect, which in principle probes the phase of $\rho_{tt}$. We further show that the one-loop $H$, $A$ effect, proportional to $\rho_{\tau\mu}\rho_{\tau\tau}$ in amplitude, is beyond the sensitivity of Belle~II to probe, even for $\rho_{\tau\tau}$ as large as $3\lambda_\tau$. With the working assumption that $\rho_{32}^f, \rho_{33}^f = {\cal O}(\lambda_3^f)$ for all charged fermions $f$, we find good discovery potential for both $\tau$ lepton flavor violation searches in the coming decade.

Highlights

  • Ever since the discovery of the muon and an empirical “muon number” that is separate from the electron number, the issue of lepton number violation has been pursued

  • The discovery of the 125 GeV scalar boson h [5] completes the last piece of the Standard Model (SM), and it is a triumph of the Large Hadron Collider (LHC)

  • What about the other two types of diagrams in Fig. 1? We propose two benchmarks to elucidate the leading and subleading effects, clarifying that, in contrast to the much larger ρτμ, ρττ values taken in the past, the one-loop diagram cannot really be probed by Belle II under the rule of thumb of Eq (9)

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Summary

INTRODUCTION

Ever since the discovery of the muon and an empirical “muon number” that is separate from the electron number, the issue of lepton number violation has been pursued. With LHC run 1 data at 8 TeV collision energy, the CMS experiment found [6] an intriguing 2σ hint for the τ lepton. Flavor violating (τLFV) h → τμ process, which subsequently disappeared [7] with 13 TeV data at run 2, Bðh → τμÞ < 0.25% ðCMS18Þ: ð2Þ. With a similar amount of data at ∼36 fb−1, the ATLAS experiment reported [8] a consistent bound of 0.28%. As this is still less than 1=3 of the full run 2 data at hand for each experiment, updates are expected. Let us trace some major steps in the phenomenological development

Published by the American Physical Society
To illustrate the interference effect between the leading
DISCUSSION AND SUMMARY
It should be noted that exotic Higgs bosons as light as
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