Origin of Yukawa couplings for Higgs and leptoquarks

We propose a model in which the Yukawa couplings of Higgs doublets are related to the couplings of the chiral fermions to a scalar leptoquark triplet. This is due to their common origin via mixing with a vector-like family distinguished by a discrete $Z_5$ symmetry, under which only the three chiral families are neutral. The model predicts lepton non-universality in $B$ to $K$ decays, depending on the leptoquark mass, $V_{ts}$ and $m_{\mu }\mathrm{/}{m}_{\tau }$. The model can only consistently explain the anomalies in $R_{K^{(\ast )}}$ for a leptoquark mass close to the collider lower bound of about $1\text{ TeV}$. Constraints from $B_s-{\bar{B}}_s$ mixing and eventually $\tau \to \mu \gamma$ become relevant for low leptoquark masses and large couplings, while $\mu \to e \gamma$ remains automatically under control due to the absence of leptoquark couplings to the electron in this model.