{"arxiv_id":"1007.1918","incoming":{"papers":7,"sentences":12,"groups":[{"kind":"background","label":"Cites it as background","papers":4,"sentences":6,"quotes":[{"arxiv_id":"2308.06558","title":"Testing $Z$ boson rare decays $Z\\to H_1 \\gamma, A_1 \\gamma$ with $(g-2)_\\mu$, $M_W$, and $BR(h_{\\rm SM}\\to Z\\gamma)$ in the NMSSM","url":"/paper/2308.06558","section":"Introduction","sentence":"The decay $Z →ϕγ$ was studied in the extensions of the SM including Minimal Supersymmetric Standard Model (MSSM) [ref] .","intent_p":0.86,"contests_p":null},{"arxiv_id":"1712.07237","title":"Exposing Dark Sector with Future Z-Factories","url":"/paper/1712.07237","section":"Introduction","sentence":"There have been previous work on constraining dark sector related new physics from Z properties at future $e^+e^-$ colliders, including dark photon [ref] , sterile neutrino model [ref] , Z invisible width e.g. [ref] , rare SM Z decays [ref] , light CP-odd Higgs bosons and supersymmetric models [ref] , .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1904.10661","title":"Long-lived light neutralinos at future $Z-$factories","url":"/paper/1904.10661","section":"Introduction","sentence":"Studies have investigated the discovery potential of future lepton colliders for a variety of new physics and SM scenarios related to $Z-$properties [ref] .","intent_p":0.95,"contests_p":null},{"arxiv_id":"1101.4758","title":"W mass and Leptonic Z-decays in the NMSSM","url":"/paper/1101.4758","section":"Introduction","sentence":"[ref] studied $Z$-decays involving very-light CP-odd Higgs bosons, e.g. in the NMSSM, in view of future searches at GigaZ.","intent_p":0.97,"contests_p":null}]}],"unlabelled_sentences":6},"outgoing":{"papers":9,"sentences":14,"groups":[{"kind":"data_used","label":"Uses data or values from","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1003.0705","title":"Search for neutral Higgs bosons decaying into four taus at LEP2","url":"/paper/1003.0705","section":"Constraints on the new physics models","sentence":"We compute the signals from the Higgs-strahlung production $e^+ e^- →Z h_i$ ($i= 1, 2$) with $h_i →2 b, 2 τ, 4 b, 4 τ, 2 b 2 τ$ [ref] and from the associated production $e^+ e^- →h_i a$ with $h_i a →4 b, 4 τ, 2 b 2 τ, 6 b, 6 τ$ [ref] , and compare them with the corresponding LEP data which have been inputted into our code.","intent_p":0.9,"contests_p":null},{"arxiv_id":"0907.5135","title":"The Two Higgs Doublet of Type II facing flavour physics data","url":"/paper/0907.5135","section":"Constraints on the new physics models","sentence":"In this work, we use the results of Fig.11 in [ref] to exclude the unfavored points.","intent_p":0.98,"contests_p":null},{"arxiv_id":"0803.0586","title":"Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Likelihoods and Parameters from the WMAP data","url":"/paper/0803.0586","section":"Constraints on the new physics models","sentence":"(c) Dark matter constraints from the WMAP relic density 0.0975 $< Ωh^2 <$ 0.1213 [ref] .","intent_p":0.95,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0910.1785","title":"The Next-to-Minimal Supersymmetric Standard Model","url":"/paper/0910.1785","section":"CALCULATIONS","sentence":"Since for a light $a$, its doublet component, parameterized by $sinθ_A$ in Eq.([ref]), is usually small, the couplings of $a$ with the sparticles will never be tremendously large [ref] .","intent_p":0.81,"contests_p":null}]}],"unlabelled_sentences":10},"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/1007.1918"}}