Abstract

Vectorlike leptons are an intriguing possibility for physics beyond the Standard Model. We study the reach for discovering (at 5$\sigma$ significance) or excluding (at 95 per cent confidence) models of charged vectorlike leptons that mix predominantly with the tau, using multi-lepton signatures at various future proton-proton collider options: a high-luminosity LHC with $\sqrt{s} =$ 14 TeV, a high-energy LHC with $\sqrt{s} =$ 27 TeV, and possible new longer-tunnel colliders with $\sqrt{s} =$ 70 or 100 TeV. For weak isodoublet vectorlike leptons, we estimate that a 27 TeV high-energy LHC with 15 ab$^{-1}$ could exclude masses up to about 2300 GeV, or discover them if the mass is less than about 1700 GeV, while a 100 TeV collider with 30 ab$^{-1}$ could exclude masses up to about 5750 GeV, or make a discovery if the mass is less than about 4000 GeV. However, we find that weak isosinglet vectorlike leptons present a much more difficult challenge, with some reach for exclusion, but not for discovery at any of the collider options considered.

Highlights

  • The Large Hadron Collider (LHC) has conducted speraortcohne-psrfootor nncewentpehr yosficmsabsseyeonnerdgitehseuSptatondparffisffid1⁄4M1o3deTle, Vat

  • Until recently the LHC detector collaborations had not put limits on vectorlike leptons (VLLs) beyond those that could be inferred from the CERN large electron-positron (LEP) e−eþ collider, which excluded [74] masses up to 101.2 GeV

  • We considered Standard Model production of the final states WZ, ZZ, ttZ, ttW, hW, hZ, tth, WWW, WWZ, ZZW, and ZZZ as the main backgrounds contributing to multilepton final states

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Summary

INTRODUCTION

The Large Hadron Collider (LHC) has conducted speraortcohne-psrfootor nncewentpehr yosficmsabsseyeonnerdgitehseuSptatondparffisffid1⁄4M1o3deTle, Vat. Vectorlike leptons (VLLs) [21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71] are pairproduced by s-channel electroweak vector boson diagrams, leading to cross sections that are much smaller and dependent on the choices of weak isospin and weak hypercharge of the new states.2 For this reason, until recently the LHC detector collaborations had not put limits on VLLs beyond those that could be inferred from the CERN large electron-positron (LEP) e−eþ collider, which excluded [74] masses up to 101.2 GeV. We have assumed that b is always at least one event, to be conservative

MINIMAL MODELS FOR PRODUCTION AND DECAY OF VECTORLIKE LEPTONS
RESULTS
Doublet VLL model
Singlet VLL models
OUTLOOK
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