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[ref] reduces to [ref] [equation] We have implemented the relevant interactions in [ref] and, generated a [ref] model file using [ref] and [ref] , and obtained the DY cross-section $σ_prod(m_S^Q+)$ at NLO in QCD [ref] using the [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1207.2666","title":"A search for a doubly-charged Higgs boson in pp collisions at sqrt(s) = 7 TeV","url":"/paper/1207.2666","section":"Introduction","sentence":"The relevant Feynman diagrams and production cross sections, calculated following [ref] , are presented in Figures [ref] and [ref].","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":10,"sentences":11,"quotes":[{"arxiv_id":"2308.10314","title":"Search for a leptophobic doubly charged Higgs in same-sign four-lepton and six-lepton signatures in a left-right symmetric model","url":"/paper/2308.10314","section":"Four-lepton, six-lepton, and eight-lepton signal processes","sentence":"We use a naive NLO to LO $k$-factor of $1.15$ [ref] to obtain the NLO cross-sections.","intent_p":0.96,"contests_p":null},{"arxiv_id":"2109.04490","title":"Leptonic Scalars and Collider Signatures in a UV-complete Model","url":"/paper/2109.04490","section":"Small Yukawa coupling scenario","sentence":"Next-to-leading order corrections are included by a $k$-factor of $1.25$ [ref] for our signal process.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1911.12783","title":"Limits on 331 vector bosons from LHC proton collision data","url":"/paper/1911.12783","section":"Cross-sections and widths","sentence":"The LO cross-sections are multiplied by a $k$-factor of 1.25 to take into account NLO effects [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1805.06910","title":"Investigating the scalar sector of left-right symmetric models with leptonic probes","url":"/paper/1805.06910","section":"Main Feature of our Benchmark Scenario","sentence":"By virtue of the smallness of the Standard Model Yukawa couplings and the heavy mass of the $Z_R$ and extra Higgs bosons, virtual $Z$-boson and photon contributions dominate and lead to a cross section of about 0.197 fb and 0.076 fb for the production of a pair of $SU(2)_L$ and $SU(2)_R$ doubly-charged Higgs bosons respectively, including in both case a next-to-leading order (NLO) $K$-factor of 1.25 [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"0706.0441","title":"Pair Production of Doubly-Charged Scalars: Neutrino Mass Constraints and Signals at the LHC","url":"/paper/0706.0441","section":"Drell-Yan production","sentence":"The QCD corrections to this process have been also computed, yielding a next-to leading order (NLO) K-factor of the order of 1.25 at the LHC energy for the entire mass range between 200 GeV and 1 TeV [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2206.14833","title":"Doubly Charged Higgs Boson Production at Hadron Colliders II: A Zee-Babu Case Study","url":"/paper/2206.14833","section":"$k^++k^–$ and $h^+h^-$ pairs at the LHC","sentence":"For both DY channels, $K^NLO$ spans roughly [equation] These numbers are comparable to exotically charged scalar production in the Type II Seesaw [ref] when adjusted for PDF and scale choices.","intent_p":0.9,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":10,"sentences":10,"quotes":[{"arxiv_id":"2608.18023","title":"Can $\\gamma\\gamma$ collisions rival $e^-e^+$ in probing doubly charged Higgs bosons?","url":"/paper/2608.18023","section":"Introduction","sentence":"In the past few years, considerable attention has been devoted to the study of doubly charged Higgs boson production and decay at both hadron and lepton colliders[Here, lepton colliders include both $e^-e^+$ and $γγ$ collision modes.] [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"2211.07505","title":"Search for doubly charged Higgs boson production in multi-lepton final states using 139 fb$^{-1}$ of proton-proton collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","url":"/paper/2211.07505","section":"Introduction","sentence":"However, various theories beyond the Standard Model (BSM theories), namely type-II seesaw models [ref] , left-right symmetric models (LRSMs) [ref] , the Zee–Babu neutrino mass model [ref] , 3-3-1 models [ref] , and the Georgi–Machacek model [ref] , predict the existence of doubly charged bosons decaying into same-charge lepton pairs.","intent_p":0.97,"contests_p":null},{"arxiv_id":"2205.14983","title":"Type-II see-saw: searching the LHC elusive low-mass triplet-like Higgses at $e^-e^+$ colliders","url":"/paper/2205.14983","section":"Introduction","sentence":"Phenomenology of these states, in particular, the doubly-charged ones, has been studied extensively at the Large Hadron Collider (LHC) [ref] , $e^-e^+$ colliders [ref] and $e^-p$ collider [ref] ; see Refs. 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