Abstract

Lepton flavor universality violating $B\to K\ell\ell$ and $K^*\ell\ell$ decays tentatively observed by LHCb can be explained by leptoquark exchange. We explore a simple model for the $B$ anomalies with a composite leptoquark from new strong dynamics at the TeV scale, a confining SU($N_{\rm HC}$) hypercolor interaction. The new matter fields, fundamentals under SU($N_{\rm HC}$), are heavy vectorlike fermions $\Psi,\, S,$ and an inert scalar doublet $\phi$. $\Psi$ is colored under QCD while $S$ is neutral, and the hyperbaryon $S^N$ is a dark matter candidate. The model is tightly constrained by meson-antimeson oscillations, lepton flavor violation, and LHC searches for resonant production of the exotic bound states. The dark matter may be detectable through its magnetic dipole moment. If $m_S$ is sufficiently small, composite leptoquarks and heavy lepton partners can be pair-produced at an observable level at LHC.

Highlights

  • While the Standard Model (SM) continues to accurately describe particle interactions at the shortest probed distance scales, there is an encouraging hint of new physics from decays of neutral B mesons to K or KÃ and charged leptons

  • Uncertainties from the hadronic matrix elements cancel in the ratios, greatly reducing the theoretical errors and making these ratios interesting probes of new physics that could violate lepton flavor universality

  • Reference [89] calculates the decay widths assuming that the bound state constituents do not form a resonance of definite spin, but these are straightforward to rescale for the physical eigenstates of spin

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Summary

INTRODUCTION

While the Standard Model (SM) continues to accurately describe particle interactions at the shortest probed distance scales, there is an encouraging hint of new physics from decays of neutral B mesons to K or KÃ and charged leptons. One of the hyperquarks (denoted by S) is a singlet under the SM gauge group It is a constituent of the composite leptoquark, and the baryonlike SNHC bound state is the dark matter. It is motivated by the need to couple the new physics to left-handed quarks and leptons [Eq (2)] Previous models achieved this by taking the fermionic hyperquarks to be doublets, but it is more straightforward to have a dark matter candidate if this is avoided, and the massless limit of S can be safely taken without introducing new relatively light scalars that would be produced in colliders. The fields Ψ and S can consistently be assigned normal baryon and lepton numbers, respectively

LOW-ENERGY EFFECTIVE THEORY
FLAVOR CONSTRAINTS
Meson-antimeson mixing
Lepton flavor violating decays
Radiative transitions
FCNC quark transitions
FCNC leptonic decays
Muon anomalous magnetic moment
Precision electroweak constraints
Higgs coupling strengths
COMPOSITE DARK MATTER
COLLIDER CONSTRAINTS
Production cross section
Predicted widths
ΨΨresonances
Composite fermion
Vertex correction
Resonant search constraints
Pair production of bound states
SUMMARY AND CONCLUSIONS
Nonrelativistic constituents
Findings
Heavy-light or relativistic systems
Full Text
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