Abstract

The LHCb Collaboration recently gave an update on testing lepton flavour universality with B+→ K+ℓ+ℓ−, in which a 3.1 standard deviations from the standard model prediction was observed. The g-2 experiment also reports a 3.3 standard deviations from the standard model on muon anomalous magnetic moment measurement. These deviations could be explained by introducing new particles including leptoquarks. In this paper, we show the possibility to search for heavy spin-1 leptoquarks at a future TeV scale muon collider by performing studies from three channels: 1) same flavour final states with either two bottom or two light quarks, 2) different flavour quark final states, and 3) a so-called “VXS” process representing the scattering between a vector boson and a leptoquark to probe the coupling between leptoquark and tau lepton. We conclude that a 3 TeV muon collider with 3 ab−1 of integrated luminosity is already sufficient to cover the leptoquark parameter space in order to explain the LHCb lepton flavour universality anomaly.

Highlights

  • Samples and cutsThe samples we used are generated using MadGraph5_aMC@NLO(MG5aMC) [60]

  • We show the possibility to search for heavy spin-1 leptoquarks at a future TeV scale muon collider by performing studies from three channels: 1) same flavour final states with either two bottom or two light quarks, 2) different flavour quark final states, and 3) a socalled “VXS” process representing the scattering between a vector boson and a leptoquark to probe the coupling between leptoquark and tau lepton

  • We show the possibility to search for heavy leptoquarks at a muon collider through three channels: 1) same flavour di-jet, 2) different flavour di-jet and 3) di-jet+dilepton final states

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Summary

Samples and cuts

The samples we used are generated using MadGraph5_aMC@NLO(MG5aMC) [60]. The BSM leptoquark model is implemented by ref. [37] with FeynRules [61] in the Universal FeynRules Output convention. In MG5aMC, basic cuts on phase space are applied as table 1 documented. Cuts on light jet and charged leptons follows the default setting of MG5aMC. The transverse momentum requirement of b jet is aligned with the light jet case, while the pseudo-rapidity cut on b jet is aligned with the charged lepton as they both need track information provided by the tracker detector. Λbμ b (a) Different Flavour tchannel Di-jet Final State. Λqμb/s/d λqμ b/s/d (b) Same Flavour tchannel Di-jet Final State.

Di-jet final state
Same flavour final state
Different flavour final state
Conclusion
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