Abstract
We introduce the $CP$ violating scalar leptoquark ${S}_{3}$ to explain the measured values of the lepton universality ratios ${R}_{{K}^{(*)}}$. We derive constraints on the $CP$-even and $CP$-odd components of the leptoquark Yukawa couplings stemming from effects in $b\ensuremath{\rightarrow}s\ensuremath{\mu}\ensuremath{\mu}$ and ${B}_{s}$ mixing. For the $b\ensuremath{\rightarrow}s\ensuremath{\mu}\ensuremath{\mu}$ processes we impose ${R}_{{K}^{(*)}}$, $\mathcal{B}({B}_{s}\ensuremath{\rightarrow}{\ensuremath{\mu}}^{+}{\ensuremath{\mu}}^{\ensuremath{-}})$, as well as $CP$-sensitive angular asymmetries ${A}_{7,8,9}$, whereas in the ${B}_{s}$ mixing sector $\mathrm{\ensuremath{\Delta}}{M}_{s}$ and ${S}_{\ensuremath{\psi}\ensuremath{\phi}}$ are considered. Combining the constraints within the ${S}_{3}$ model reveals that a large $CP$ phase with a definite sign is perfectly viable for a leptoquark of mass below a few TeV. For larger mass of the ${S}_{3}$ leptoquark the $CP$ phase is suppressed due to the observables pertaining to the ${B}_{s}$ system. We provide predictions of direct and mixing-induced $CP$ asymmetries in $B\ensuremath{\rightarrow}K\ensuremath{\mu}\ensuremath{\mu}$ that could reveal the presence of the novel $CP$ phase.
Highlights
The flavor structure of the Yukawa sector is probably the least understood aspect of the Standard Model (SM)
The persistent hints of lepton flavor universal (LFU) violation in b → sll may imply an existence of leptoquarks close to the TeV scale that couple to bμ and sμ
We have shown that large CP-violating phases in S3 couplings are bounded neither by RKðÃÞ nor by BðBs → μμÞ, whereas existing measurements of CP asymmetries A7;8;9 constrain ImðδC9Þ, preferably towards negative values
Summary
The flavor structure of the Yukawa sector is probably the least understood aspect of the Standard Model (SM). Large ImðδC9Þ imprints its CP-violating effects on processes connected to b → sμμ via electroweak mixing Such a connection between the RKðÃÞ anomalies and the Bs mixing observables has been studied in Refs. In this paper we consider the phenomenological consequences of ImðδC9Þ, generated by a concrete model with a scalar LQ S3 1⁄4 ð3 ̄; 3; 1Þ, and paying particular attention to the effects in Bs mixing This LQ naturally realizes the lefthanded scenario δC9 1⁄4 −δC10 since the gauge quantum numbers allow only Yukawa couplings to fermion doublets [2]. This LQ state was considered in attempts to address RKðÃÞ and RDðÃÞ simultaneously [18,19,20,21,22] as well as in broader context including dark sectors [23,24].
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