Abstract

LHCb has reported hints of lepton-flavor universality violation in the rare decays B → K(*)ℓ+ℓ−, both in high- and low-q2 bins. Although the high-q2 hint may be explained by new short-ranged interactions, the low-q2 one cannot. We thus explore the possibility that the latter is explained by a new light resonance. We find that LHCb’s central value of {R}_{K^{*}} in the low-q2 bin is achievable in a restricted parameter space of new-physics scenarios in which the new, light resonance decays preferentially to electrons and has a mass within approximately 10 MeV of the di-muon threshold. Interestingly, such an explanation can have a kinematic origin and does not require a source of lepton-flavor universality violation. A model-independent prediction is a narrow peak in the differential B → K*e+e− rate close to the di-muon threshold. If such a peak is observed, other observables, such as the differential B → Ke+e− rate and RK, may be employed to distinguish between models. However, if a low-mass resonance is not observed and the low-q2 anomaly increases in significance, then the case for an experimental origin of the lepton-flavor universality violating anomalies would be strengthened. To further explore this, we also point out that, in analogy to J/ψ decays, e+e− and μ+μ− decays of ϕ mesons can be used as a cross check of lepton-flavor universality by LHCb with 5 fb−1 of integrated luminosity.

Highlights

  • If the discrepancies between measurements and SM predictions are due to New Physics (NP) from four-fermion contact interactions, the ratio RK∗ is expected to have a non-trivial q2 dependence

  • We find that LHCb’s central value of RK∗ in the low-q2 bin is achievable in a restricted parameter space of new-physics scenarios in which the new, light resonance decays preferentially to electrons and has a mass within approximately 10 MeV of the di-muon threshold

  • We explored possible NP explanations of the anomaly in the low-q2 bin of RK∗ observed by LHCb

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Summary

Off-shell effect of a light resonance

The off-shell exchange of a resonance far below the di-muon threshold can in principle contribute to the B → K∗ + − rate in the low-q2 bin. We show here that such a setup is unlikely to satisfy existing experimental constraints To illustrate this point, we consider a very light resonance, X, with a mass far below the low-q2 bin of RK∗, i.e., m2X 0.045 GeV2, that couples to leptons Given that the coupling of light (∼ 10’s of MeV) new degrees of freedom to electrons and muons are constrained to be 10−3 (see figure 7 in section A), the B → XsX decay width typically exceeds the experimentally determined total B width by a factor of a few, which excludes such a scenario.

On-shell production of a light resonance
Dark photon — LFU violation without LFU violation
Generic resonance
Model-independent predictions
Model-dependent implications
Cross-checking lepton-universality violation
Discussion and conclusions
B Form factors
Full Text
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