2020
DOI: 10.1155/2020/9234130
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Doubly Charged Lepton Search Potential of the FCC-Based Energy-Frontier Electron-Proton Colliders

Abstract: We search for the doubly charged leptons (L−−) predicted in composite models including extended weak isospin multiplets, namely, IW=1 and IW=3/2, at the Future Circular Collider- (FCC-) based energy-frontier electron-proton colliders with the center-of-mass energies of s=3.46 TeV, s=10 TeV, and s=31.6 TeV, respectively. We deal with the e−p⟶L−−X⟶e−W−X process, calculate the production cross sections, and give the normalized transverse momentum and pseudorapidity distributions of final-state electron to obtain … Show more

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Cited by 4 publications
(6 citation statements)
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“…Here, L T = (ν L , L ) is the ordinary lepton doublet, g and g are the SU(2) L and U(1) Y gauge couplings and W W W µν , B µν are the field strength tensor of the corresponding gauge fields respectively; τ τ τ are the Pauli matrices and Y is the hypercharge, f and f are dimensionless couplings and are expected (and assumed) to be of order unity. Excited states interacting with the SM sector through the model Lagrangians (1.1)-(1.2) and (1.3) have been extensively searched for at high-energy collider facilities and their phenomenology has also been discussed in a series of recent papers [24,25,26,27,28,29,30,31,32,33]. The current strongest bounds are due to the recent LHC experiments.…”
Section: Pos(corfu2019)057mentioning
confidence: 99%
“…Here, L T = (ν L , L ) is the ordinary lepton doublet, g and g are the SU(2) L and U(1) Y gauge couplings and W W W µν , B µν are the field strength tensor of the corresponding gauge fields respectively; τ τ τ are the Pauli matrices and Y is the hypercharge, f and f are dimensionless couplings and are expected (and assumed) to be of order unity. Excited states interacting with the SM sector through the model Lagrangians (1.1)-(1.2) and (1.3) have been extensively searched for at high-energy collider facilities and their phenomenology has also been discussed in a series of recent papers [24,25,26,27,28,29,30,31,32,33]. The current strongest bounds are due to the recent LHC experiments.…”
Section: Pos(corfu2019)057mentioning
confidence: 99%
“…Signatures of quintuplet fermions at LHC have been studied in detail in Ref: [33,34]. They are also a good candidate in Future collider experiments [35,36]. In these studies, the quintuplet decay directly into the Standard Model particles.…”
Section: Introductionmentioning
confidence: 99%
“…Cases studied so far include multilepton and multijet signatures both at the LHC [16,33] and the linear colliders [35,36,40]. In standard scenarios, the quintuplet decays directly into the SM particles.…”
Section: Introductionmentioning
confidence: 99%
“…), too [34][35][36][37][38][39][40][41][42][43][44]. In the literature there are phenomenological studies for the doubly charged leptons at the LHC [45][46][47][48][49][50][51][52][53][54], at the future   e e and e colliders [55][56][57][58], and at the future lepton-proton colliders [59][60][61]. The first limits for the mass of doubly charged leptons in ep collisions obtained as like that, for Lint >10 4 fb -1 , ML > 860 (1280) GeV at s =1.3 (1.98) TeV in [59].…”
Section: Introductionmentioning
confidence: 99%