Abstract

At present, there are outstanding discrepancies between standard model predictions and measurements of the muon's $g-2$ and several $B$-meson properties. We resolve these anomalies by considering a two-Higgs-doublet model extended to include leptoquarks and a dark Higgs boson $S$. The leptoquarks modify $B$-meson decays and also induce an $S \gamma \gamma$ coupling, which contributes to the muon's $g-2$ through a Barr-Zee diagram. We show that, for TeV-scale leptoquarks and dark Higgs boson masses $m_{S} \sim 10-200~\text{MeV}$, a consistent resolution to all of the anomalies exists. The model predicts interesting new decays, such as $B \to K^{(*)} e^+ e^-$, $B \to K^{(*)} \gamma \gamma$, $K \to \pi \gamma \gamma$, and $h \to \gamma \gamma \gamma \gamma$, with branching fractions not far below current bounds.

Highlights

  • At present, there are a number of anomalies in lowenergy measurements

  • We find solutions that depend on only a small number of parameters and show that these explanations motivate interesting new searches, for rare meson decays to diphoton final states and Higgs boson decays to four photons

  • The couplings to fermions are inherited from the mixing of the dark Higgs boson with the 2HDM Higgs bosons: they are suppressed by Yukawa couplings, and the down-type couplings are enhanced by tan β, while the up-type couplings are suppressed by cot β

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Summary

INTRODUCTION

There are a number of anomalies in lowenergy measurements Among these are the anomalous magnetic moment of the muon, ðg − 2Þμ, and several in the decays of B mesons. Motivated by the leptoquark solution to the B anomalies, we note that leptoquarks (as well as other TeV-scale particles) will generically induce an Sγγ coupling, and this can resolve the ðg − 2Þμ anomaly through a two-loop Barr-Zee diagram In this way, the solutions to the ðg − 2Þμ and B anomalies proposed here are connected. Given the light state S and its couplings to electrons and photons, the model predicts new meson decays, such as B → KS and K → πS, followed by S → eþe−; γγ, leading to dilepton and diphoton signals that could be discovered in current and near-future experiments. Appendixes A and B contain details of the 2HDM model and the effective Sγγ coupling, respectively

THE MODEL
Dark Higgs boson contribution from effective Sγγ coupling
Dark Higgs boson contribution from Sγγ coupling induced by V leptoquarks
U Leptoquark contribution
The U leptoquark and B anomalies
Hadronic constraints
CONCLUSIONS
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