{"arxiv_id":"2307.16250","incoming":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"outgoing":{"papers":23,"sentences":37,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0811.1603","title":"O(g) plasma effects in jet quenching","url":"/paper/0811.1603","section":"Relation to Classical Corrections","sentence":"In more detail, one can use causality properties of $𝒞(k_⊥)$, also revealed in [ref] , to carry out the $k^+$ integral by analytically continuing into the $k^+$ complex plane. $k^+_IR$ then appears as the radius of the arc of the deformed contour, with the arc lying between the zeroth and first Matsubara modes.","intent_p":0.97,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0811.1603","title":"O(g) plasma effects in jet quenching","url":"/paper/0811.1603","section":"Conclusion and Outlook","sentence":"In more detail, we showed how the scale, $ω_T$ cuts off this region of phase space and furthermore, how the region, which gives rise to the classical corrections, computed in [ref] fits in comparison.","intent_p":0.98,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":5,"sentences":5,"quotes":[{"arxiv_id":"2009.06614","title":"The nonperturbative contribution to asymptotic masses","url":"/paper/2009.06614","section":"Introduction","sentence":"A similar program is well underway for the non-perturbative determination of classical corrections to the asymptotic mass [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"2307.09297","title":"Hard parton dispersion in the quark-gluon plasma, non-perturbatively","url":"/paper/2307.09297","section":"Introduction","sentence":"A similar program is well underway for the non-perturbative determination of classical corrections to the asymptotic mass [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"2112.01407","title":"The force-force-correlator in hot QCD perturbatively and from the lattice","url":"/paper/2112.01407","section":"Introduction","sentence":"A similar program is well underway for the non-perturbative determination of classical corrections to the asymptotic mass [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"2203.16352","title":"Heavy quarks and jets as probes of the QGP","url":"/paper/2203.16352","section":"Introduction","sentence":"See the recent reviews on jets in heavy-ion collisions [ref] or extractions of $q̂$ from data [ref] for more information.","intent_p":1.0,"contests_p":null},{"arxiv_id":"2201.02796","title":"Extracting the jet transport coefficient from hadron suppressions by confronting current NLO parton fragmentation functions","url":"/paper/2201.02796","section":"Introduction","sentence":"See the recent reviews on jets in heavy-ion collisions [ref] or extractions of $q̂$ from data [ref] for more information.","intent_p":1.0,"contests_p":null}]}],"unlabelled_sentences":30},"claims":[{"relation":"same_result","label":"States the same result","papers":[{"arxiv_id":"2207.08842","url":"/paper/2207.08842","title":"Classical vs quantum corrections to jet broadening in a weakly-coupled Quark-Gluon Plasma","main_claim":"We find that a thermal population of dynamical gluons changes the boundaries and reduces the size of the double-logarithmic phase space.","p":0.92}]}],"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/2307.16250"}}