2022
DOI: 10.1007/jhep01(2022)111
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New leptons with exotic decays: collider limits and dark matter complementarity

Abstract: We describe current and future hadron collider limits on new vector-like leptons with exotic decays. We consider the possibility that, besides standard decays, the new leptons can also decay into a Standard Model charged lepton and a stable particle like a dark photon. To increase their applicability, our results are given in terms of arbitrary branching ratios in the different decay channels. In the case that the dark photon is stable at cosmological scales we discuss the interplay between the dark photon and… Show more

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Cited by 25 publications
(14 citation statements)
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“…Vector-like leptons will be dominantly pair-produced at the LHC through the s− channel Z/γ exchange (see figure 1), and then decay to leptons and vector boson dark matter, yielding a promising pp → l + l − + / E T signature. This will resemble the signals of supersymmetric slepton searches [37][38][39] leading to dilepton and missing energy signatures. It is worth noting that the pair-production rate of vector-like leptons (fermion) in our scenario is substantially larger than the pair-production rate of slepton (scalar).…”
Section: Collider Implicationsmentioning
confidence: 81%
“…Vector-like leptons will be dominantly pair-produced at the LHC through the s− channel Z/γ exchange (see figure 1), and then decay to leptons and vector boson dark matter, yielding a promising pp → l + l − + / E T signature. This will resemble the signals of supersymmetric slepton searches [37][38][39] leading to dilepton and missing energy signatures. It is worth noting that the pair-production rate of vector-like leptons (fermion) in our scenario is substantially larger than the pair-production rate of slepton (scalar).…”
Section: Collider Implicationsmentioning
confidence: 81%
“…Perhaps the most obvious channel, portal matter pair production from either QCD (in the case of color-triplet portal matter) or electroweak interactions (for leptonic portal matter), has been well-explored in the perfectly analogous scenarios of [19-21, 57, 58], and summarized well in [59], so we see no need to perform the analysis again here-we shall simply quote some results and comment on their relevance in our context. In both the leptonic and quark-like portal matter cases, the pair production cross sections scale quite strongly with the portal matter mass [19,57], so for pair production searches we are especially concerned with the very lightest portal matter states that are present, even in the event of a large ensemble of portal matter states in the model, as long as there are O(1) differences in brane-localized kinetic terms (and hence masses O(1) proportional differences in masses) between portal matter states. In the event that the dark Higgs and dark photon decay invisibly (or are long-lived enough to decay outside of the detector), direct contact can be made with squark and slepton searches for jets or leptons and missing energy to find these lightest portal matter particles.…”
Section: Portal Matter and Su (2) D Bosons: Productionmentioning
confidence: 99%
“…We have discussed in section 5.4 how CLFV processes constrain typical values of the Yukawa couplings Ỹ E i of the NB-VLL with the SM and have seen that the no observation of µ → e flavor change leads 10 A recent reanalysis can be seen in ref. [63]. 11 We roughly projected on the 95% CL region with 2 dgf.…”
Section: Parameter Spacementioning
confidence: 99%