{"arxiv_id":"1806.03760","incoming":{"papers":9,"sentences":11,"groups":[{"kind":"background","label":"Cites it as background","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1811.07227","title":"Deconfinement of non-strange hadronic matter with nucleons and $\\Delta$ baryons to quark matter in neutron stars","url":"/paper/1811.07227","section":"Introduction","sentence":"According to literature, the main mechanisms to solve such puzzles are (i) considering the effect of repulsive hyperon-hyperon interaction via exchange of vector mesons [ref] or scalar meson exchange [ref] , (ii) inclusion of repulsive hyperonic three-body forces [ref] , (iii) effect of phase transition from hadronic to deconfined quark matter [ref] , (iv) calculating NS properties with modified/extended theories of gravity [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"2008.06753","title":"Role of $\\Delta$s in determining the properties of Neutron Stars in parameterized hydrostatic equilibrium","url":"/paper/2008.06753","section":"Introduction","sentence":"Apart from the hadron-quark phase transition [ref] or the hyperon-hyperon interaction via exchange of vector mesons [ref] or scalar mesons [ref] , there are many recent paradigm associated with modifications/extensions to the normal General Relativity (GR) theory to resolve the hyperon and the $Δ$ puzzles.","intent_p":0.96,"contests_p":null},{"arxiv_id":"2007.08493","title":"GW190814 as a massive rapidly-rotating neutron star with exotic degrees of freedom","url":"/paper/2007.08493","section":"Introduction","sentence":"Quark vector-isoscalar and vector-isovector couplings have been used in the NJL model [ref] , 2-flavor confining QM (CQM) model [ref] , FRG within a quark-meson model [ref] , quark-meson-nucleon (QMN) model [ref] , and bag model [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"2112.05546","title":"Hybrid stars from a constrained equation of state","url":"/paper/2112.05546","section":"Introduction","sentence":"The use of the NJL model in such two-model approaches has been widely explored both considering a first-order phase transition [ref] and with a smooth (crossover) transition between both phases [ref] .","intent_p":0.94,"contests_p":null}]}],"unlabelled_sentences":7},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"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/1806.03760"}}