{"arxiv_id":"2112.14295","incoming":{"papers":1,"sentences":2,"groups":[{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2512.17002","title":"Intrinsic Properties of Large CP Violation in the Complex Two-Higgs-Doublet Model","url":"/paper/2512.17002","section":"Introduction","sentence":"A substantial body of phenomenological studies has already explored these possibilities, focusing on collider observables across a variety of benchmark channels [ref] .","intent_p":0.94,"contests_p":null}]}],"unlabelled_sentences":1},"outgoing":{"papers":88,"sentences":113,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":8,"sentences":12,"quotes":[{"arxiv_id":"2012.11408","title":"Constraining new physics from Higgs measurements with Lilith-2","url":"/paper/2012.11408","section":"SM Higgs data","sentence":"In order to properly combine the constraints coming from the LHC-Higgs data, we used Lilith [ref] 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cross sections via gluon fusion are calculated at NLO using SusHiv1.6.0 [ref] and interfaced with ScannerS [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1003.1643","title":"THE TOOLS AND MONTE CARLO WORKING GROUP Summary Report from the Les Houches 2009 Workshop on TeV Colliders","url":"/paper/1003.1643","section":"Neutral heavy Higgs Boson decay rates","sentence":"The branching ratios of the various physical scalars in CPV 2HDM were calculated using C2HDM HDECAY [ref] through the HDECAY interface [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":8,"sentences":8,"quotes":[{"arxiv_id":"1209.2716","title":"The Electroweak Fit of the Standard Model after the Discovery of a New Boson at the LHC","url":"/paper/1209.2716","section":"S, T, U parameters","sentence":"This theoretical constraint comes from the oblique parameters, constrained by the global fit [ref] to be [equation]","intent_p":0.93,"contests_p":null},{"arxiv_id":"1511.05066","title":"Flavor constraints on the Two Higgs Doublet Models of $Z_2$ symmetric and aligned types","url":"/paper/1511.05066","section":"S, T, U parameters","sentence":"This theoretical constraint comes from the oblique parameters, constrained by the global fit [ref] to be [equation]","intent_p":0.93,"contests_p":null},{"arxiv_id":"2111.08340","title":"Constraints on Higgs boson production with large transverse momentum using $H\\rightarrow b\\bar{b}$ decays in the ATLAS detector","url":"/paper/2111.08340","section":"Allowed Parameter Space","sentence":"We show contours for the signal strengths of the Higgs channels $gg→h →ZZ$ (red-thick), $Vh →(h→bb̅)$ (green-light) and $gg→h →γγ$ (black-thin), using the bounds set by ATLAS, with 36 fb$^-1$ (dashed/dot-dashed/dotted) and with 139 fb$^-1$ (solid) of integrated luminosity [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"2004.03969","title":"Measurements of the 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(dashed/dot-dashed/dotted) and with 139 fb$^-1$ (solid) of integrated luminosity [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1708.00435","title":"CP-Violation in the Two Higgs Doublet Model: from the LHC to EDMs","url":"/paper/1708.00435","section":"Electric Dipole Moments","sentence":"It has also been shown that, in unlike in the Type-I 2HDM, the electron and mercury EDMs are not able to probe the parameter space when $tanβ$ is close to 1, which will be our case, due to the cancellation in Barr-Zee diagrams [ref] .","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":35,"sentences":38,"quotes":[{"arxiv_id":"1503.01114","title":"Complementarity of LHC and EDMs for Exploring Higgs CP Violation","url":"/paper/1503.01114","section":"Introduction and Motivation","sentence":"the impact of CP violation on the Higgs bosons and their respective decay channels, we consider the CPV 2HDM potential parameters [ref] in the approximate $Z_2$ case [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1908.03952","title":"Constraining new physics from Higgs measurements with Lilith: update to LHC Run 2 results","url":"/paper/1908.03952","section":"Introduction and Motivation","sentence":"the impact of CP violation on the Higgs bosons and their respective decay channels, we consider the CPV 2HDM potential parameters [ref] in the approximate $Z_2$ case [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"1110.3812","title":"What the Oblique Parameters S, T, and U and Their Extensions Reveal About the 2HDM: A Numerical Analysis","url":"/paper/1110.3812","section":"S, T, U parameters","sentence":"The implication of electroweak precision on the mass spectrum of heavier neutral and on the charged Higgs was thoroughly investigated before [ref] , in the context of CPV 2HDM.","intent_p":0.88,"contests_p":null},{"arxiv_id":"1011.6560","title":"CP violation in charged Higgs production and decays in the Complex Two Higgs Doublet Model","url":"/paper/1011.6560","section":"Introduction and Motivation","sentence":"Also, recent studies of charged Higgs bosons phenomenology in the context of the CPV 2HDMs have been presented in [ref] and a CPV 2HDM analysis of viable parameter space regions which pass experimental constraints has been given in [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"1310.1385","title":"Constraints on CP-violating Higgs couplings to the third generation","url":"/paper/1310.1385","section":"Introduction and Motivation","sentence":"Also, recent studies of charged Higgs bosons phenomenology in the context of the CPV 2HDMs have been presented in [ref] and a CPV 2HDM analysis of viable parameter space regions which pass experimental constraints has been given in [ref] 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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/2112.14295"}}