2021
DOI: 10.1007/jhep03(2021)279
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Lepton-quark fusion at Hadron colliders, precisely

Abstract: When a TeV-scale leptoquark has a sizeable Yukawa coupling, its dominant production mechanism at hadron colliders is the partonic-level lepton-quark fusion. Even though the parton distribution functions for leptons inside the proton are minuscule, they get compensated by the resonant enhancement. We present the first computation of higher order radiative corrections to the resonant leptoquark production cross section at the Large Hadron Collider (LHC). Next-to-leading (NLO) QCD and QED corrections are similar … Show more

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Cited by 33 publications
(35 citation statements)
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“…While the lepton PDFs are now accurately known, official PS codes can at present not correctly handle incoming leptons. In addition, fully differential NLO QCD and QED hadron-collider predictions are not available for processes like bτ → U → bτ -a first step into this direction has been made very recently in [61] by calculating the NLO QCD and QED corrections to the inclusive quark-lepton induced cross sections of singly-produced scalar LQs. Once fully differential NLO QCD and QED corrections are available, they should be consistently combined with the PS to obtain NLO+PS predictions that provide an accurate modelling of the exclusive final states targeted at the LHC by ATLAS and CMS.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…While the lepton PDFs are now accurately known, official PS codes can at present not correctly handle incoming leptons. In addition, fully differential NLO QCD and QED hadron-collider predictions are not available for processes like bτ → U → bτ -a first step into this direction has been made very recently in [61] by calculating the NLO QCD and QED corrections to the inclusive quark-lepton induced cross sections of singly-produced scalar LQs. Once fully differential NLO QCD and QED corrections are available, they should be consistently combined with the PS to obtain NLO+PS predictions that provide an accurate modelling of the exclusive final states targeted at the LHC by ATLAS and CMS.…”
Section: Discussionmentioning
confidence: 99%
“…The main goal of this article is to extend and generalise the basic ideas and results presented in the publication [60] (see subsequently also [61]) to the case of singlet vector LQs, coupled mainly to third-generation fermions. To this purpose, we develop three search strategies for LQ signatures that are induced by quark-lepton annihilation at the LHC.…”
Section: Introductionmentioning
confidence: 88%
“…As it turns out, the t-channel contribution of figure 1 towards the leptoquark pair production at LHC becomes relevant only when the leptoquark interacts very strongly, i.e., with the couplings of order one, to the quarks of the first generation [55]. However, in this particular regime other processes such as a single leptoquark production [55][56][57][58], induced by the diagrams in panels (b) and (c) of figure 1, the Drell-Yan di-lepton production [59][60][61][62][63][64], and/or a resonant leptoquark production [65][66][67][68] might become equally capable of or even more important in constraining the leptoquark parameter space. Moreover, one also needs to take into account the experimental constraints from flavor physics, such as the Atomic Parity Violation ones, for a given l-q-LQ scenario to ensure its viability, especially within a large Yukawa coupling regime [69] space see ref.…”
Section: Introductionmentioning
confidence: 99%
“…To leading order in this scenario the effects on the Higgs phenomenology and on the B anomalies are decoupled, with the first ones being dominated byR 2 andS 1 , and the second ones by S 1 . Whereas current limits do not exclude an explanation of the B anomalies [72], one may wonder to which extent this possibility might be affected by single resonant LQ production searches at the LCH in the future [73][74][75]. Since the constraints arising from these searches would only impact on LQs coupled to leptons, they would not impose restrictions on the lightest LQ which in this scenario drives the increase of the double Higgs production and is mainly identified withS 1 , whose couplings to leptons we put to zero.…”
Section: B Anomaliesmentioning
confidence: 96%