{"arxiv_id":"1307.5270","incoming":{"papers":17,"sentences":26,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1410.5396","title":"Elliptic and triangular flow of heavy flavor in heavy-ion collisions","url":"/paper/1410.5396","section":"Introduction","sentence":"For the incoherent gluon radiation spectra the calculation in [ref] are extended to finite quark masses [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":5,"sentences":5,"quotes":[{"arxiv_id":"1604.02343","title":"Degrees of Freedom of the Quark Gluon Plasma, tested by Heavy Mesons","url":"/paper/1604.02343","section":"The standard MC@sHQ approach","sentence":"In the standard MC@sHQ approach [ref] the heavy quarks can interact with the plasma constituents purely elastically or in a combination of elastic and inelastic collisions.","intent_p":0.89,"contests_p":null},{"arxiv_id":"1809.07894","title":"Towards the determination of heavy-quark transport coefficients in quark-gluon plasma","url":"/paper/1809.07894","section":"Nantes approach","sentence":"Heavy quarks propagate through the QGP and experience elastic [ref] and radiative collisions [ref] with the plasma constituents (assumed to be massless).","intent_p":0.81,"contests_p":null},{"arxiv_id":"2407.20919","title":"System size dependence of energy loss and correlations of heavy mesons at LHC energies","url":"/paper/2407.20919","section":"heavy quark production and evolution in EPOS4","sentence":"We include both, elastic [ref] and radiative [ref] collisions.","intent_p":0.89,"contests_p":null},{"arxiv_id":"2401.17096","title":"Heavy flavour hadron production in relativistic heavy ion collisions at RHIC and LHC in EPOS4HQ","url":"/paper/2401.17096","section":"EPOS4HQ: Heavy quark energy loss in hot medium","sentence":"We include in this study both, elastic [ref] and radiative [ref] collisions.","intent_p":0.88,"contests_p":null},{"arxiv_id":"1305.6544","title":"Influence of hadronic bound states above $T_c$ on heavy-quark observables in Pb+Pb collisions at at the CERN Large Hadron Collider","url":"/paper/1305.6544","section":"Introduction","sentence":"The incoherent emission of bremsstrahlung gluons are included via matrix elements from scalar QCD [ref] .","intent_p":0.97,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1504.07151","title":"Inclusive, prompt and non-prompt J/$\\psi$ production at mid-rapidity in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV","url":"/paper/1504.07151","section":"Results","sentence":"In fig:raanonprompt the nuclear modification factor for non-prompt for $1.5 < < 4.5$ and $4.5 < < 10$ is shown together with the result by CMS for $6.5 < < 30$ [ref] and with theoretical model predictions [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1803.03824","title":"Extraction of Heavy-Flavor Transport Coefficients in QCD Matter","url":"/paper/1803.03824","section":"Reference Results in an Infinite and Finite QGP","sentence":"The Nantes calculation [ref] is characterized by a running $α_s$, reaching rather large values, and a reduced Debye mass in the elastic HQ scattering that triggers the radiation; it has been constructed to be primarily applicable at intermediate $p_t$ and therefore neglects finite-path length effects due to gluon formation outside the QGP.","intent_p":0.94,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2204.01561","title":"Exploring jet transport coefficients by elastic scattering in the strongly interacting quark-gluon plasma","url":"/paper/2204.01561","section":"Introduction","sentence":"The suppression of the emission of gluons with finite masses has been shown in Ref. [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2308.03105","title":"Inelastic and elastic parton scatterings in the strongly interacting quark-gluon plasma","url":"/paper/2308.03105","section":"Introduction","sentence":"The emission of massless and massive gluons by heavy quark scattering with massless quarks and gluons from the QGP medium has been studied within scalar pQCD in Refs. [ref] .","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":16},"outgoing":{"papers":4,"sentences":4,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1302.5250","title":"Radiative parton processes in perturbative QCD - an improved version of the Gunion and Bertsch cross section from comparisons to the exact result","url":"/paper/1302.5250","section":"Introduction","sentence":"The same viewpoint will be adopted in the present work in order to deduce and study the radiative cross section that will be later implemented in our Monte Carlo simulations in the same spirit as [ref] .","intent_p":0.81,"contests_p":null}]}],"unlabelled_sentences":3},"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/1307.5270"}}