{"arxiv_id":"hep-ph/0304069","incoming":{"papers":41,"sentences":64,"groups":[{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1909.10495","title":"Probing Doubly and Singly Charged Higgs at $pp$ Collider HE-LHC","url":"/paper/1909.10495","section":"Branching ratios of $H^±±$ and $H^±$","sentence":"In this region of $v_Δ$ it will be possible to find out the correct neutrino mass ordering by measuring the leptonic branching ratios of the charged Higgs states [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":21,"sentences":27,"quotes":[{"arxiv_id":"2006.04610","title":"Discriminating the HTM and MLRSM models in collider studies via doubly charged Higgs boson pair production and the subsequent leptonic decays","url":"/paper/2006.04610","section":"Searching for new scalar bosons at future colliders and a choice of tested models","sentence":"We will explore the simplest one which involves doubly charged Higgs fields in the triplet representation with hypercharge $Y =2$, the Higgs Triplet Model () [ref] .","intent_p":0.8,"contests_p":null},{"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":"0907.4193","title":"Neutrino Masses and Heavy Triplet Leptons at the LHC: Testability of Type III Seesaw","url":"/paper/0907.4193","section":"Introduction","sentence":"Test of seesaw mechanism at LHC has received a lot of attentions recently [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"2308.16897","title":"Distinguishing models with $\\mu \\to e $ observables","url":"/paper/2308.16897","section":"Introduction","sentence":"The first two are neutrino mass models : the TeV-scale version of the type II seesaw mechanism [ref] and the inverse type I seesaw [ref] , whose predictions for LFV processes have been studied, mainly in the top-down approach, by many authors (see e.g. Refs. [ref] for the type II and Refs. [ref] for the inverse seesaw, where [ref] follow an EFT approach).","intent_p":0.89,"contests_p":null},{"arxiv_id":"2109.04490","title":"Leptonic Scalars and Collider Signatures in a UV-complete Model","url":"/paper/2109.04490","section":"Key parameters and decay channels of $H^±±$ and $H^±$","sentence":"The gauge interactions of $H^±$ and $H^±±$ with the SM photon, $W$ and $Z$ bosons in Table [ref] are relevant for the pair production $H^++H^–$ and the associated production $H^±±H^∓$ of the doubly-charged scalar at hadron colliders, as in the Type-II seesaw case [ref] .","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":36},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/0304069"}}