Abstract

Heavy neutrinos (N) remain one of most promising explanations for the ori-gin of neutrinos’ tiny masses and large mixing angles. In light of broad advances in un-derstanding and modeling of hadron collisions at large momentum transfers, we revisit the long-standard search strategy for heavy N decaying to multiple charged leptons (ℓ), pp → NℓX → 3ℓνX. For electroweak and TeV-scale N, we propose a qualitatively new collider analysis premised on a dynamic jet veto and discriminating, on an event-by-event basis, according to the relative amount of hadronic and leptonic activity. We report that the sensitivity to heavy neutrinos at the CERN Large Hadron Collider (LHC) can be improved by roughly an order of magnitude at both ℒ = 300 fb−1 and 3 ab−1. At sqrt{s}=14 TeV with ℒ = 3 ab−1, we find active-sterile mixing as small as |VℓN|2 = 10− 2(10− 3) [5 × 10− 4] can be probed at 95% CL for heavy Dirac neutrinos masses mN ≲ 1200 (300) [200] GeV, well beyond the present |VℓN|2 ≲ 10− 3 − 10− 1 constraints for such heavy states set by indirect searches and precision measurements. The improvement holds also for Majorana N, and is largely independent of whether charged lepton flavor is conserved or violated. The analysis, built almost entirely from inclusive, transverse observables, is designed to be robust across increasing collider energies, and hence serves as a basis for searches at future colliders: with ℒ = 15ab− 1 at sqrt{s} = 27 TeV,onecanprobemixingbelow |VℓN|2 = 10− 2(10− 3)[2 × 10− 4] for mN ≲ 3500 (700) [200] GeV. At a hypothetical 100 TeV pp collider with ℒ = 30 ab− 1, one can probe mixing down to 9 × 10−5 for mN ≲ 200 GeV, below 10−3 for mN ≲ 4 TeV, and below 10−2 for mN ≲ 15 TeV. We anticipate these results can be further improved with detector-specific tuning and application of multi-variant / machines learning techniques. To facilitate such investigations, we make publicly available Monte Carlo libraries needed for the precision computations/simulations used in our study.

Highlights

  • The origin of tiny neutrino masses and clarity on neutrinos’ Majorana nature remain some of the most pressing mysteries in particle physics today

  • We report that the sbeynrsoituivgihtlyytaonhoeardveyrnoefumtraingonsitautdtehaetCbEoRthNLL=arg3e00Hfabd−r1onanCdo3lliadbe−r1(.LAHtC√) csa=n be 14 improved TeV with

  • We remain inclusive with respect to soft and forward hadronic activity: events may contain an arbitrary number of jets with parton-level transverse momentum (pT) < max(25 GeV, pT1) and/or |y| > 4.5

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Summary

Introduction

The origin of tiny neutrino masses and clarity on neutrinos’ Majorana nature remain some of the most pressing mysteries in particle physics today. (This is the case searches of other colorless Seesaw particles [34, 39, 79].) Aside from vetoing central jets that have been b-tagged, essentially no information about jet activity in exploited in searches for high-mass Nm This is despite the CC DY and W γ fusion mechanisms having qualitatively different QCD radiation patterns than their leading backgrounds. While never intended for such circumstance√s, with the incredible increase of top quark and multi-jet cross sections at higher s, it is doubtful that current search strategies will remain sufficient for future pp colliders [27, 29,30,31, 33] In light of these observations, we have revisited the long-standard, hadron collider search strategy for heavy neutrinos that decay to fully leptonic final states, as given in eq (1.3).

Neutrino mass models
Inverse seesaw
Phenomenological type I seesaw
Constraints on heavy sterile neutrinos
Computational setup
Monte Carlo event generation and public accessibility
Heavy neutrino signal event generation
Standard Model background event generation
Standard Model inputs
Benchmark heavy neutrino inputs
Heavy neutrinos at hadron colliders
Heavy neutrino production formalism
Heavy neutrino production at the LHC and beyond
14 TeV LHC
Summary
Heavy neutrinos and dynamic jet vetoes
Dynamic vetoes beyond pT ratios
Dynamical jet vetoes at leading logarithmic accuracy
Observability of heavy neutrinos at hadron colliders
Hadron collider detector modeling
Results: sensitivity at the LHC and beyond
Summary and outlook
Findings
Conclusions
Full Text
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