{"arxiv_id":"2204.05085","incoming":{"papers":63,"sentences":70,"groups":[{"kind":"background","label":"Cites it as background","papers":37,"sentences":38,"quotes":[{"arxiv_id":"2307.12105","title":"$W$-boson Mass Anomaly from High-Dimensional Scalar Multiplets","url":"/paper/2307.12105","section":"Introduction","sentence":"Extensive studies have been carried out in the literature to explain the CDF-2 $W$-boson mass anomaly with low-dimensional scalar multiplets, which include a scalar singlet [ref] , a second Higgs doublet [ref] , and a scalar triplet [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"2205.02217","title":"$W$ boson mass shift, dark matter and $(g-2)_\\ell$ in a scotogenic-Zee model","url":"/paper/2205.02217","section":"Introduction","sentence":"Some possible explanations to the $W$ boson mass shift can arise at tree-level [ref] , or at loop level [ref] , along with the prospect of reconciling one or more discrepancies [ref] such as flavor anomalies and dark matter.","intent_p":0.89,"contests_p":null},{"arxiv_id":"2209.11421","title":"Constraints from New CDF II W-Boson Mass On Top-Bottom Seesaw and the TopFlavor Models","url":"/paper/2209.11421","section":"Introduction","sentence":"There have been many attempts to resolve the W mass anomaly, see e.g. [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"2302.01641","title":"Consistency of New CDF-II W Boson Mass with 123-Model","url":"/paper/2302.01641","section":"Introduction","sentence":"Recently, several novel physics models, including the : Two-Higgs doublet model [ref] , Higgs triplet model [ref] , supersymmetry [ref] , leptoquark model [ref] , seesaw mechanism [ref] , vector-like leptons and/or vector-like quarks [ref] and other SM extensions [ref] are proposed to explain the W boson mass anomaly.","intent_p":0.97,"contests_p":null},{"arxiv_id":"2205.01701","title":"CDF $W$ boson mass and muon $g-2$ in type-X two-Higgs-doublet model with a Higgs-phobic light pseudoscalar","url":"/paper/2205.01701","section":"Introduction","sentence":"Various BSM models have been studied to explain the new oblique parameters [ref] .","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":32},"outgoing":{"papers":74,"sentences":85,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1803.02846","title":"BSMPT - Beyond the Standard Model Phase Transitions -A Tool for the Electroweak Phase Transition in Extended Higgs Sectors","url":"/paper/1803.02846","section":"Phase transition in the 2HDM","sentence":"This method has been numerically implemented in public package $$ [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1808.02037","title":"Type-II 2HDM under the Precision Measurements at the $Z$-pole and a Higgs Factory","url":"/paper/1808.02037","section":"$m_W$ in the 2HDM","sentence":"Here $m_W^SM=80.357 GeV ±4_inputs ±$ $4_theory MeV$ [ref] , $S, T, U$ are oblique parameters in the 2HDM [ref] , and $δρ^2HDM =|λ_hhh^2HDM|^2/16 π^2 m_h^2$ are higher order 2HDM effects from enhanced Higgs boson self-interactions.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1912.01431","title":"Type-I 2HDM under the Higgs and Electroweak Precision Measurements","url":"/paper/1912.01431","section":"Z-pole and Higgs precision measurements","sentence":"We adopt the Higgs measurements results presented in Table 3 in Ref. 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