Abstract

Processes commonly studied at the Large Hadron Collider (LHC) are induced by quarks and gluons inside the protons of the LHC beams. In this Letter, we demonstrate that, since protons also contain leptons, it is possible to target lepton-induced processes at the LHC as well. In particular, by picking a lepton from one beam and a quark from the other beam, we present for the first time a comprehensive analysis of resonant single leptoquark (LQ) production at a hadron collider. In the case of minimal scalar LQs, we derive novel bounds that arise from the LHC Run II considering all possible flavor combinations of an electron or a muon and an up (u), a down (d), a strange, or a charm quark. For the flavor combinations with a u or a d quark, the obtained limits represent the most stringent constraints to date on LQs of this type. The prospects of our method at future LHC runs are also explored. Given the discovery reach of the proposed LQ signature, we argue that dedicated resonance searches in final states featuring a single light lepton and a single light-flavor jet should be added to the exotics search canon of both the ATLAS and the CMS Collaborations.

Highlights

  • Introduction.—At the Large Hadron Collider (LHC) an immense number of collisions between quarks and gluons took place and many more are expected in the upcoming Run III and the high-luminosity (HL LHC) upgrade

  • Given the discovery reach of the proposed LQ signature, we argue that dedicated resonance searches in final states featuring a single light lepton and a single light-flavor jet should be added to the exotics search canon of both the ATLAS and the CMS Collaborations

  • Taking the case of LQs as an example, we demonstrate that lepton-induced processes, which so far have been completely neglected at the LHC, can be complementary to quark- or gluoninduced channels in searches for beyond the standard model (SM) physics

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Summary

Introduction

Introduction.—At the Large Hadron Collider (LHC) an immense number of collisions between quarks and gluons took place and many more are expected in the upcoming Run III and the high-luminosity (HL LHC) upgrade. In the case of minimal scalar LQs, we derive novel bounds that arise from the LHC Run II considering all possible flavor combinations of an electron or a muon and an up (u), a down (d), a strange, or a charm quark.

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