Abstract

The observed muon anomalous magnetic moment deviates from the Standard Model predictions. There are two scalar leptoquarks with simultaneous couplings to the quark-muon pairs of both chiralities that can singly explain this discrepancy. We discuss an alternative mechanism that calls for the mixing of two scalar leptoquarks of the same electric charge through the interaction with the Higgs field, where the two leptoquarks separately couple to the quark-muon pairs of opposite chirality structures. Three scenarios that satisfy this requirement are S1 & S3, {tilde{S}}_1 & S3, and {tilde{R}}_2 & R2, where the first scenario is realised with the up-type quarks running in the loops while the other two scenarios proceed through the down-type quark loops. We introduce only two non-zero Yukawa couplings to the relevant quarks and a muon, at the time, to study ability of these three scenarios to explain (g − 2)μ and be in accord with available experimental constraints. We find that the S1 & S3 scenario with the top-quark loops is consistent with all existing measurements. The {tilde{S}}_1 & S3 and {tilde{R}}_2 & R2 scenarios can accommodate the observed discrepancy through the bottom-quark loops but exhibit significant tension with the existing data on the high-pT dilepton-tails at LHC for the required values of Yukawa couplings and leptoquark masses.

Highlights

  • The influence of scalar LQs on aμ = (g −2)μ/2 is well-documented in the literature [12]

  • In this work we investigate the viability of those scenarios where the one-loop contributions towards the anomalous magnetic moment of muon are induced through the mixing of two scalar LQs of the same electric charge via the SM Higgs field, where the LQs in question need to couple to the muons of opposite chiralities

  • We investigate viability of those scenarios where the one-loop contributions towards the anomalous magnetic moment of muon are induced through the mixing of two scalar LQs of the same electric charge Q via the interactions with the SM Higgs field

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Summary

General classification

We list in table 2 all possible pairs of scalar LQs that can mix through the SM Higgs field [20] at the renormalizable level. We denote the SM Higgs field as H = (1, 2, 1/2) and indicate the number of H fields in the contraction in the second column of table 2 Those LQ pairs that couple to the muons of opposite chiralities can generate the one-loop contribution towards (g − 2)μ that we are interested in whereas the pairs that couple to neutrinos can yield neutrino masses of Majorana nature [21,22,23] at the one-loop level. There are, clearly, three possible LQ pairs that might generate large enough contributions towards (g − 2)μ through the mixing with the SM Higgs field These combinations are S1 & S3, S1 & S3, and R2 & R2, where, in all three instances, at least one of the LQ multiplets is chiral in nature. We find these constraints to be marginally relevant for those LQ masses and associated Yukawa couplings that are not in conflict with the results of the existing LHC analyses

Mixing formalism
Phenomenological constraints
Numerical results
Conclusions
Full Text
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