Abstract

The measured branching fractions of B-mesons into leptonic final states derived by the LHCb, Belle and BaBar collaborations hint towards the breakdown of lepton flavour universality. In this work we take at face value the so-called {R}_{D^{left(ast right)}} observables that are defined as the ratios of neutral B-meson charged-current decays into a D(*)-meson, a charged lepton and a neutrino final state in the tau and light lepton channels. A well-studied and simple solution to this charged current anomaly is to introduce a scalar leptoquark S1 that couples to the second and third generation of fermions. We investigate how S1 can also serve as a mediator between the Standard Model and a dark sector. We study this scenario in detail and estimate the constraints arising from collider searches for leptoquarks, collider searches for missing energy signals, direct detection experiments and the dark matter relic abundance. We stress that the production of a pair of leptoquarks that decays into different final states (i.e. the commonly called “mixed” channels) provides critical information for identifying the underlying dynamics, and we exemplify this by studying the tτbν and the resonant S1 plus missing energy channels. We find that direct detection data provides non-negligible constraints on the leptoquark coupling to the dark sector, which in turn affects the relic abundance. We also show that the correct relic abundance can not only arise via standard freeze-out, but also through conversion-driven freeze-out. We illustrate the rich phenomenology of the model with a few selected benchmark points, providing a broad stroke of the interesting connection between lepton flavour universality violation and dark matter.

Highlights

  • Strong evidence for Lepton Flavour Universality Violation (LFUV) has been established by the LHCb, Belle, and BaBar collaborations in their measurements of the RK(∗) [1,2,3,4,5] and RD(∗) [6,7,8] observables

  • We study this scenario in detail and estimate the constraints arising from collider searches for leptoquarks, collider searches for missing energy signals, direct detection experiments and the dark matter relic abundance

  • We have studied the connection between these models and dark matter, which necessarily requires to add new particles and couplings to the theory

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Summary

Introduction

Strong evidence for Lepton Flavour Universality Violation (LFUV) has been established by the LHCb, Belle, and BaBar collaborations in their measurements of the RK(∗) [1,2,3,4,5] and RD(∗) [6,7,8] observables. Coupling a leptoquark to a dark sector requires the introduction of at least two additional particles, χ0, our dark matter candidate, and χ1 As the latter must carry colour charge, it can be looked for at colliders in final states with transverse missing energy (MET) plus SM particles. Direct searches for leptoquarks (LQ) would in principle constrain the parameter space in a way in which mLQ 1 TeV for O(1) couplings [30,31,32] Those constraints are relaxed in our scenario, given that novel LQ decays in the dark sector dilute the “visible” branching fractions (i.e. those associated with SM final states).

Theoretical setup
Particle content and interactions
Leptoquark solutions to RD anomalies
Phenomenological features
LHC constraints
Missing energy searches
Searches for leptoquark pair-production under consideration
Reinterpreting LHC leptoquark search results in the mixed bνtτ channel
LHC sensitivity to our model via searches for leptoquark pair production
LHC sensitivity to our model via leptoquark single production and decay
Resonant leptoquark plus missing energy search
Conclusive statements about all considered LHC searches
Dark matter constraints
Direct detection
Relic density
Benchmark scenarios
Conclusions and outlook
A FeynRules model
C Reinterpretation of MET searches
ATLAS mono-jet
ATLAS multi-jet plus MET
CMS search at the LHC in the muon channel: details of the selection
Resonant leptoquark plus MET: prospects at the future HL-LHC
E Dark matter direct detection at the one-loop level
Findings
F Implementation of conversion-driven freeze-out in MicrOMEGAs
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