{"arxiv_id":"2104.10709","incoming":{"papers":3,"sentences":5,"groups":[{"kind":"background","label":"Cites it as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2211.01543","title":"Custodial Symmetry Violation in Scalar Extensions of the Standard Model","url":"/paper/2211.01543","section":"Case A: General $SU(2)_L$ $N$-plet scalar with $ℤ_2$ symmetry","sentence":"The most general forms of renormalizable scalar potential are discussed in detail in Ref. [ref] , and there are usually 3 free parameters for $ϕ$-$H$ Higgs portal interactions depending on the quantum number of the multiplet in the $ℤ_2$ symmetric case.","intent_p":0.82,"contests_p":null},{"arxiv_id":"2402.11506","title":"Higgs-strahlung at the LHC in the inert doublet model","url":"/paper/2402.11506","section":"Introduction","sentence":"The IDM has a rich phenomenology both at the colliders and in Dark Matter (DM) physics, and as such has been widely studied [ref] mostly in tree-level analyses, but also including higher-order corrections, either electroweak (EW) or QCD.","intent_p":0.92,"contests_p":null}]}],"unlabelled_sentences":3},"outgoing":{"papers":57,"sentences":118,"groups":[{"kind":"extends","label":"Builds on","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1202.1316","title":"Complex Scalar Singlet Dark Matter: Vacuum Stability and Phenomenology","url":"/paper/1202.1316","section":"Numerical Results in $$ Scheme","sentence":"This relation is an extension to the approximate perturbativity constraint on the couplings in the complex singlet model in Ref. [ref] which is based on the work in Ref. [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"hep-ph/9608280","title":"Ruling Out a Strongly-Interacting Standard Higgs Model","url":"/paper/hep-ph/9608280","section":"Numerical Results in $$ Scheme","sentence":"This relation is an extension to the approximate perturbativity constraint on the couplings in the complex singlet model in Ref. [ref] which is based on the work in Ref. [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":2,"sentences":3,"quotes":[{"arxiv_id":"1812.07829","title":"Scalar Electroweak Multiplet Dark Matter","url":"/paper/1812.07829","section":"Degenerate with Higgs Diphoton Decay Sensitivity","sentence":"In what follows, we follow the representation of the $$ EW scalar multiplet and the convention of the formulism adopted in Ref. [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"0709.1075","title":"Techniques for the calculation of electroweak radiative corrections at the one-loop level and results for W-physics at LEP200","url":"/paper/0709.1075","section":"On-shell Renormalization Scheme","sentence":"The renormalized quantities and renormalization constants are in accordance with the scheme of Denner [ref] , and are defined as follows [equation] where quantities with subscript $0$ denote the bare parameters.","intent_p":1.0,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":4,"sentences":7,"quotes":[{"arxiv_id":"1811.10545","title":"CEPC Conceptual Design Report: Volume 2 - Physics & Detector","url":"/paper/1811.10545","section":"Numerical Results in $$ Scheme","sentence":"In what follows, provide numerical results assuming the CEPC projections [ref] for purposes of concrete illustration [The precision for the Higgs production via the gluon and $bb̅$ fusion in $h→γγ$ channel is applied in addition in the complex triplet model to illustrate a straightforward improvement for the constraints in the parameter space. ].","intent_p":0.95,"contests_p":null},{"arxiv_id":"1810.09450","title":"Type-II Seesaw Scalar Triplet Model at a 100 TeV $pp$ Collider: Discovery and Higgs Portal Coupling Determination","url":"/paper/1810.09450","section":"Complementary with Higgs Diphoton Decays","sentence":"In Ref. [ref] the regions of $> 5σ$ significance [The significance is defined as $Sig/√(Sig+Bkg)$ with Sig and Bkg the total signal and background event numbers.] are obtained using the discovery channels $H^++H^–$ and $H^±±H^∓$ with $H^±±$ decaying into same-sign di-leptons and/or di-bosons in the $,v_Δ$ plane with fixed neutrino masses ($m_ν_l=0.01$ eV for $l=e,μ,τ$) and Higgs portal couplings ($λ_4=0,λ_5=-0.1$) (see Fig. 7 therein).","intent_p":0.8,"contests_p":null},{"arxiv_id":"0706.4071","title":"Cosmology and Astrophysics of Minimal Dark Matter","url":"/paper/0706.4071","section":"Degenerate with Higgs Diphoton Decay Sensitivity","sentence":"Due to small mass splitting between the charged and neutral triplet scalars ($ΔM=166$) [ref] in the large scalar mass regime $M_Σ≫M_W$, the direct search for the dark matter involves the process of charged scalar pair production accompanying the decay to neutral scalar and a soft $π^±$, the so-called disappearing charge tracks (DCTs).","intent_p":0.87,"contests_p":null},{"arxiv_id":"hep-ph/0512090","title":"Minimal Dark Matter","url":"/paper/hep-ph/0512090","section":"Degenerate with Higgs Diphoton Decay Sensitivity","sentence":"Due to small mass splitting between the charged and neutral triplet scalars ($ΔM=166$) [ref] in the large scalar mass regime $M_Σ≫M_W$, the direct search for the dark matter involves the process of charged scalar pair production accompanying the decay to neutral scalar and a soft $π^±$, the so-called disappearing charge tracks (DCTs).","intent_p":0.87,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":19,"sentences":21,"quotes":[{"arxiv_id":"hep-ph/9703392","title":"Precision observables in SU(2) x U(1) models with an additional Higgs triplet","url":"/paper/hep-ph/9703392","section":"Potentials in Specific Models","sentence":"Real Triplet model [ref] : Here we consider $Y = 0$.","intent_p":0.94,"contests_p":null},{"arxiv_id":"0809.4185","title":"Higgs Triplets, Decoupling, and Precision Measurements","url":"/paper/0809.4185","section":"Potentials in Specific Models","sentence":"Real Triplet model [ref] : Here we consider $Y = 0$.","intent_p":0.94,"contests_p":null},{"arxiv_id":"0811.3957","title":"Triplet Scalars and Dark Matter at the LHC","url":"/paper/0811.3957","section":"Potentials in Specific Models","sentence":"Real Triplet model [ref] : Here we consider $Y = 0$.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1310.8152","title":"Scalar Representations in the Light of Electroweak Phase Transition and Cold Dark Matter Phenomenology","url":"/paper/1310.8152","section":"Potentials in Specific Models","sentence":"Complex Triplet model [ref] : For the complex triplet, there is another possibility with $n = 3, Y = ±2$, additional terms appear [(H H)_1 Φ]_0, [(H H)_1 Φ]_0.","intent_p":0.86,"contests_p":null},{"arxiv_id":"2009.03250","title":"One-loop radiative corrections to $e^+ e^-\\to Zh^0/H^0A^0$ in the Inert Higgs Doublet Model","url":"/paper/2009.03250","section":"Introduction","sentence":"The full one-loop radiative corrections to $e^+e^-→Zh/H^0A^0$ processes in the inert doublet model has been recently calculated [ref] .","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":85},"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/2104.10709"}}