Unified framework for B-anomalies, muon g − 2 and neutrino masses

A bstract We present a model of radiative neutrino masses which also resolves anomalies reported in B -meson decays, R D ∗ and R K ∗ , as well as in muon g − 2 measurement, ∆ a μ . Neutrino masses arise in the model through loop diagrams involving TeV-scale leptoquark (LQ) scalars R 2 and S 3 . Fits...

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Veröffentlicht in:The journal of high energy physics 2021-03, Vol.2021 (3), p.1-54, Article 179
Hauptverfasser: Babu, K. S., Dev, P. S. Bhupal, Jana, Sudip, Thapa, Anil
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Sprache:eng
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Zusammenfassung:A bstract We present a model of radiative neutrino masses which also resolves anomalies reported in B -meson decays, R D ∗ and R K ∗ , as well as in muon g − 2 measurement, ∆ a μ . Neutrino masses arise in the model through loop diagrams involving TeV-scale leptoquark (LQ) scalars R 2 and S 3 . Fits to neutrino oscillation parameters are obtained satisfying all flavor constraints which also explain the anomalies in R D ∗ , R K ∗ and ∆ a μ within 1 σ . An isospin-3/2 Higgs quadruplet plays a crucial role in generating neutrino masses; we point out that the doubly-charged scalar contained therein can be produced in the decays of the S 3 LQ, which enhances its reach to 1.1 (6.2) TeV at s = 14 TeV high-luminosity LHC ( s = 100 TeV FCC-hh). We also present flavor-dependent upper limits on the Yukawa couplings of the LQs to the first two family fermions, arising from non-resonant dilepton ( pp → ℓ + ℓ − ) processes mediated by t -channel LQ exchange, which for 1 TeV LQ mass, are found to be in the range (0 . 15 − 0 . 36). These limits preclude any explanation of R D ∗ through LQ-mediated B -meson decays involving ν e or ν μ in the final state. We also find that the same Yukawa couplings responsible for the chirally-enhanced contribution to ∆ a μ give rise to new contributions to the SM Higgs decays to muon and tau pairs, with the modifications to the corresponding branching ratios being at (2–6)% level, which could be tested at future hadron colliders, such as HL-LHC and FCC-hh.
ISSN:1029-8479
1029-8479
DOI:10.1007/JHEP03(2021)179