{"arxiv_id":"1309.3561","incoming":{"papers":27,"sentences":35,"groups":[{"kind":"background","label":"Cites it as background","papers":11,"sentences":12,"quotes":[{"arxiv_id":"1702.02924","title":"Two-Higgs-Doublet-Portal Dark-Matter Models in Light of Direct Search and LHC Data","url":"/paper/1702.02924","section":"Introduction","sentence":"It is worth mentioning here that there have been a number of studies in the past on various Higgs-portal scenarios in which a THDM was supplemented with a SM-gauge-singlet DM candidate having spin 0 [ref] , 1/2 [ref] , or 1 [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"2003.01788","title":"Higgs portal to dark matter and $B\\to K^{(*)}$ decays","url":"/paper/2003.01788","section":"Introduction","sentence":"A viable scenario involves a gauge singlet Higgs field which mixes with the SM Higgs field through appropriate terms in the Higgs potential, resulting in a dominantly SU(2)-doublet Higgs boson $h_1$ with mass 125 GeV and an additional Higgs boson $h_2$ with a priori arbitrary mass [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"2004.10041","title":"The effect of the early kinetic decoupling in a fermionic dark matter model","url":"/paper/2004.10041","section":"Model","sentence":"The CP-conserving interaction has been studied in Ref. [ref] , and the CP-violating operator has been studied in Refs. [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"1901.02278","title":"Current status and future prospects of the singlet-doublet dark matter model with $CP$ violation","url":"/paper/1901.02278","section":"Effective theory for fermionic DM models","sentence":"The $CP$-conserving interaction has been studied in Ref. [ref] , and the $CP$-violating operator has been studied in Refs. [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"1410.6497","title":"Scalar Simplified Models for Dark Matter","url":"/paper/1410.6497","section":"Higgs Mediators","sentence":"This is the well-known “Higgs Portal” scenario for dark matter [ref] (similarly, one could consider the “dilaton” portal [ref] ).","intent_p":1.0,"contests_p":null}]}],"unlabelled_sentences":23},"outgoing":{"papers":34,"sentences":44,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1304.4219","title":"Light Higgs and Vector-like Quarks without Prejudice","url":"/paper/1304.4219","section":"Analysis of Higgs data","sentence":"In our fitting procedures we follow the method adopted in references [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1210.8120","title":"Higgs couplings beyond the Standard Model","url":"/paper/1210.8120","section":"Analysis of Higgs data","sentence":"In our fitting procedures we follow the method adopted in references [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1212.5244","title":"Higgs Couplings at the End of 2012","url":"/paper/1212.5244","section":"Analysis of Higgs data","sentence":"In our fitting procedures we follow the method adopted in references [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1304.3369","title":"A Bayesian view of the Higgs sector with higher dimensional operators","url":"/paper/1304.3369","section":"Analysis of Higgs data","sentence":"In our fitting procedures we follow the method adopted in references [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":8,"sentences":11,"quotes":[{"arxiv_id":"1301.6620","title":"Limits on spin-dependent WIMP-nucleon cross sections from 225 live days of XENON100 data","url":"/paper/1301.6620","section":"Relic density and direct detection","sentence":"We use XENON100 bounds from Ref. [ref] for spin-independent (SI) case and Ref. [ref] for spin-dependent (SD) case to constrain the parameter space given by the relic density.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1207.5988","title":"Dark Matter Results from 225 Live Days of XENON100 Data","url":"/paper/1207.5988","section":"Relic density and direct detection","sentence":"We use XENON100 bounds from Ref. [ref] for spin-independent (SI) case and Ref. [ref] for spin-dependent (SD) case to constrain the parameter space given by the relic density.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1306.2941","title":"Global fit to Higgs signal strengths and couplings and implications for extended Higgs sectors","url":"/paper/1306.2941","section":"Introduction","sentence":"The resulting invisible decay width of the Higgs is bounded at 95% CL to $ℬ(h→invisible)<0.19 (0.38)$ from global fits with the Higgs couplings to the SM fermions fixed to their SM values (varied freely while also allowing new particles in loops) [ref] (see also [ref] ).","intent_p":0.96,"contests_p":null},{"arxiv_id":"1205.6790","title":"Probing for Invisible Higgs Decays with Global Fits","url":"/paper/1205.6790","section":"Introduction","sentence":"The resulting invisible decay width of the Higgs is bounded at 95% CL to $ℬ(h→invisible)<0.19 (0.38)$ from global fits with the Higgs couplings to the SM fermions fixed to their SM values (varied freely while also allowing new particles in loops) [ref] (see also [ref] ).","intent_p":0.96,"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":"SM + DM with an extra triplet and a singlet","sentence":"The lower limit on $Δ^++$ mass is then $m_Δ> 204$ GeV [ref] , so that correct relic density can still be obtained.","intent_p":0.97,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1108.3546","title":"Constraining Dark Matter Models from a Combined Analysis of Milky Way Satellites with the Fermi Large Area Telescope","url":"/paper/1108.3546","section":"Suppressed Higgs decays to dark sector","sentence":"In Fig. [ref] we compare the bounds on annihilation cross sections $<σv >$ for $bb̅$ (blue lines) and $τ^+τ^-$ (red lines) channels [ref] with the predictions from the last two operators in Eq. [ref], when correct relic density is assumed in the predictions.","intent_p":0.91,"contests_p":null},{"arxiv_id":"1108.2914","title":"Exclusion of canonical WIMPs by the joint analysis of Milky Way dwarfs with Fermi","url":"/paper/1108.2914","section":"Suppressed Higgs decays to dark sector","sentence":"In Fig. [ref] we compare the bounds on annihilation cross sections $<σv >$ for $bb̅$ (blue lines) and $τ^+τ^-$ (red lines) channels [ref] with the predictions from the last two operators in Eq. [ref], when correct relic density is assumed in the predictions.","intent_p":0.91,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"0904.3640","title":"Lepton Flavour Violating Decays tau to lll and mu to e gamma in the Higgs Triplet Model","url":"/paper/0904.3640","section":"SM + DM with an extra triplet and a singlet","sentence":"(For previous study of LFV in the triplet model, see Refs. [ref] .) For $m_Δ=220-350$ GeV as required by the relic abundance, the off-diagonal $f_ab$ are severely constrained.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1101.0365","title":"A Two-Singlet Model for Light Cold Dark Matter","url":"/paper/1101.0365","section":"SM + DM with extra scalar singlet","sentence":"In our final example of a viable Higgs portal model of DM we add to the SM two real scalars, $ϕ$ and $S$ (for existing studies of similar models see [ref] ).","intent_p":0.87,"contests_p":null},{"arxiv_id":"0808.3384","title":"Deducing the nature of dark matter from direct and indirect detection experiments in the absence of collider signatures of new physics","url":"/paper/0808.3384","section":"Suppressed Higgs decays to dark sector","sentence":"[ref] ) and we do not pursue it any further.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1106.0034","title":"Theory and phenomenology of two-Higgs-doublet models","url":"/paper/1106.0034","section":"2HDM-II + DM","sentence":"After electroweak symmetry breaking three out of eight real degrees of freedom in $H_1$ and $H_2$ are absorbed as longitudinal components of $W^±$ and $Z$ bosons (for reviews see e.g. [ref] ).","intent_p":1.0,"contests_p":null}]}],"unlabelled_sentences":23},"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/1309.3561"}}