Abstract

We study the phenomenology of light scalars of masses $m_1$ and $m_2$ coupling to heavy flavour-violating vector bosons of mass $m_V$. For $m_{1,2}\lesssim $ few GeV, this scenario triggers the rare $B$ meson decays $B_s^0\to 3\mu^+ 3\mu^-$, $B^0\to 3\mu^+ 3\mu^-$, $B^+\to K^+ 3\mu^+ 3\mu^-$ and $B_s^0\to K^{0*} 3\mu^+ 3\mu^-$; the last two being the most important ones for $m_1\sim m_2$. None of these signals has been studied experimentally; therefore we propose analyses to test these channels at the LHCb. We demonstrate that the reach of this facility extends to branching ratios as small as $6.0\times 10^{-9}$, $1.6\times 10^{-9}$, $5.9\times 10^{-9}$ and $1.8\times 10^{-8}$ for the aforementioned channels, respectively. For $m_{1,2}\gg \mathcal{O}(1)$ GeV, we show that slightly modified versions of current multilepton and multitau searches at the LHC can probe wide regions of the parameter space of this scenario. Altogether, the potential of the searches we propose outperform other constraints such as those from meson mixing.

Highlights

  • Searches for new physics in final states often considered as “standard candles,” most notably in searches for supersymmetry (SUSY), have not provided any evidence of physics beyond the Standard Model (BSM) so far

  • This scenario is especially motivated, as it arises naturally in nonminimal composite Higgs models (CHM) [4,5,6,7,8,9]. (V and a1;2 can be seen as the counterparts of the ρ and the pions in QCD.) Likewise, such vector boson can explain the apparent anomalies observed in tests of lepton flavor universality [10,11,12,13,14,15,16,17]

  • Under very mild conditions, a2 decays mostly into a1, which subsequently decays into pairs of leptons

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Summary

INTRODUCTION

Searches for new physics in final states often considered as “standard candles,” most notably in searches for supersymmetry (SUSY), have not provided any evidence of physics beyond the Standard Model (BSM) so far This fact does not necessarily disproves low energy SUSY or other popular BSM extensions [1], such as composite Higgs models (CHM) [2,3]. The scalars couple to the mediator as a vector current ∼a1∂a2 When the latter is conserved, namely for m1 ∼ m2 (and in particular in the massless limit), the B meson decay into such scalars vanishes. By studying the regime of large scalar masses V, while we dedicate Appendix to building a complete model that predicts definite values of several of the parameters that we scan over

FRAMEWORK
LOW-MASS REGIME AT THE LHCb
HIGH-MASS REGIME AT THE LHC
Findings
CONCLUSIONS
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