Abstract

We explore the signatures of the $\tilde{R}_2$ class of leptoquark (LQ) models at the proposed $e^- p$ and $e^+p$ colliders. We carry out an analysis for the proposed colliders LHeC and FCC-eh with center of mass (c.m.) energy 1.3 TeV and 3.46 TeV, respectively. For $\tilde{R}_2$ class of LQ models, there are a number of final states that can arise from LQ production and its subsequent decay. In this report we do a detailed cut-based analysis for the $l^{\pm}j$ final state. We also discuss the effect of polarized electron and positron beams on LQ production and in turn on $l^{\pm}j$ production. At LHeC, the final state $l^+j$ has very good discovery prospect. We find that, only 100 $\text{fb}^{-1}$ of data can probe LQ mass upto 1.2 TeV with $5\sigma$ significance, even with a generic set of cuts. On the contrary, at FCC-eh, one can probe LQ masses upto 2.2 TeV (for $e^-$ beam) and 3 TeV (for $e^+$ beam), at more than $5\sigma$ significance with luminosity $1000\,\text{fb}^{-1}$ and $500\,\text{fb}^{-1}$, respectively.

Highlights

  • LQs are hypothetical particles which can emerge from the unification of quarks and leptons in the Pati-Salam model [1]

  • Z11 has been fixed to its lower limit for given mass of the LQ (MLQ) and Y11, according to the upper bound from LHC search

  • In this work we study the discovery prospect of R 2 class of LQ models at the proposed ep colliders such as LHeC and FCC-eh

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Summary

INTRODUCTION

LQs are hypothetical particles which can emerge from the unification of quarks and leptons in the Pati-Salam model [1]. The advantage with R 2 type of scalar LQ is that in addition to the coupling with the lepton and jet, the model has right handed (RH) neutrinos coupled to the LQ. [14], both single and pair production of scalar LQs (with QEM 1⁄4 1=3; 5=3) have been studied with the decay. [16], pair production LQs (S3) and their decay to a μμjj final state has been explored at future hadron colliders. The paper is organized as follows: First we review the model and the existing constraints on LQs. Following this, we discuss the production of a LQ at an ep collider and compare with that at the LHC. We present a detailed collider analysis and discuss the discovery prospects of the final state lÆj. We review the existing constraints on LQ mass and couplings

CONSTRAINTS ON LQ MASS AND COUPLINGS
Atomic parity violation
Collider bounds
LQ PRODUCTION
ANALYSIS
RESULTS
CONCLUSIONS
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