2020
DOI: 10.1088/1361-6471/ab4574
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Searching for long-lived particles beyond the Standard Model at the Large Hadron Collider

Abstract: Particles beyond the Standard Model (SM) can generically have lifetimes that are long compared to SM particles at the weak scale. When produced at experiments such as the Large Hadron Collider (LHC) at CERN, these long-lived particles (LLPs) can decay far from the interaction vertex of the primary proton–proton collision. Such LLP signatures are distinct from those of promptly decaying particles that are targeted by the majority of searches for new physics at the LHC, often requiring customized techniques to i… Show more

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Cited by 292 publications
(302 citation statements)
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“…Therefore we do not take seriously the prospect of a long-lived scalar sgluon. Nevertheless, any model that predicts reasonably small mass splitting of left-and right-chiral states also predicts a pseudoscalar long-lived enough to decay with displaced vertices [35]. This is an exciting signature that degrades the efficacy of most searches that constrain the pseudoscalar and calls for searches for long-lived particles (LLPs).…”
Section: Decay Rates and Characteristic Distancesmentioning
confidence: 99%
“…Therefore we do not take seriously the prospect of a long-lived scalar sgluon. Nevertheless, any model that predicts reasonably small mass splitting of left-and right-chiral states also predicts a pseudoscalar long-lived enough to decay with displaced vertices [35]. This is an exciting signature that degrades the efficacy of most searches that constrain the pseudoscalar and calls for searches for long-lived particles (LLPs).…”
Section: Decay Rates and Characteristic Distancesmentioning
confidence: 99%
“…The lightest charged Higgs boson in the ALRM is H AE 2 , which is longlived, so that limits on its mass are probed by searches for heavy stable charged particles. The H AE 2 bosons are pairproduced via the Drell-Yan mechanism, in proton-proton collisions at center-of-mass energies of 7 TeV [33,34], 8 TeV [35] and 13 TeV [36][37][38][39][40][41] and in electron-positron collisions at a center-of-mass energy of 183 GeV [42].…”
Section: Fieldsmentioning
confidence: 99%
“…We display the main constraints from EWPD [57][58][59][60][61] (brown dashed line), L3 [62][63][64] (pink dashed line), DELPHI [65] (blue dashed line), LEP2 [62][63][64] (red solid line), CMS-13 TeV trilepton [66] (black solid line), CMS-13 TeV same-sign dilepton [67] (purple solid line), ATLAS-13 TeV trilepton [68] M N ≳ 50 GeV and U 2 αN ≳ 10 −8 , the decay length of HNL is quite small such that we can simply take the decay of HNL as prompt in most of the parameter space for each lepton flavor. In contrast, the low mass HNL with tiny U 2 αN can easily generate the displaced vertex signature after it has been produced at colliders [32,[49][50][51][52][53][54][55][56], which is of immense interest in the upcoming LHC run.…”
Section: Figmentioning
confidence: 99%