{"arxiv_id":"1204.1998","incoming":{"papers":21,"sentences":31,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1207.6836","title":"Suppression of high $p_T$ hadron spectra in $p+A$ collisions","url":"/paper/1207.6836","section":"Introduction","sentence":"We also extropolate our calculation to LHC energy and give the prediction of $dN_ch/dη$ for $p+Pb$ at $√(s)=4.4$ TeV [ref] .","intent_p":0.91,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":4,"sentences":6,"quotes":[{"arxiv_id":"1309.6735","title":"Relics of Minijets amid Anisotropic Flows in High-energy Heavy-ion Collisions","url":"/paper/1309.6735","section":"Introduction","sentence":"We will first use HIJING Monte Carlo model [ref] to study the intrinsic dihadron correlations in p+p and A+A collisions from minijets without final state interaction.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1702.01479","title":"Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV","url":"/paper/1702.01479","section":"Analysis strategy","sentence":"The HIJING 2.1 generator [ref] is employed to estimate the systematic uncertainty (Section [ref]).","intent_p":1.0,"contests_p":null},{"arxiv_id":"1605.09479","title":"Predictions for $p+$Pb Collisions at $\\sqrt{s_{NN}} = 5$ TeV: Comparison with Data","url":"/paper/1605.09479","section":"Charged particles","sentence":"Examples employed here include $𝙷𝙸𝙹𝙸𝙽𝙶$ [ref] , $𝙷𝙸𝙹𝙸𝙽𝙶𝙱𝙱$ [ref] and $𝙰𝙼𝙿𝚃$ [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1712.07198","title":"Study of Bose-Einstein correlations in pp, pPb, and PbPb collisions at $\\sqrt{s_\\mathrm{NN}} =$ 0.9-7 TeV","url":"/paper/1712.07198","section":"Particle identification and cluster subtraction method","sentence":"The employed event generators are 6.426 (with the tunes D6T and Z2) for $$ collisions, and 2.1 [ref] for $$Pb collisions.","intent_p":0.99,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":4,"sentences":6,"quotes":[{"arxiv_id":"1210.3615","title":"Pseudorapidity density of charged particles in p-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV","url":"/paper/1210.3615","section":"Introduction","sentence":"A comparison of the model calculations with the data shows that most of the models that include shadowing [ref] or saturation [ref] predict the measured multiplicity values to within 20% (see also Tab. [ref]).","intent_p":1.0,"contests_p":null},{"arxiv_id":"1807.09061","title":"ALICE results on system-size dependence of charged-particle multiplicity density in p-Pb, Pb-Pb and Xe-Xe collisions","url":"/paper/1807.09061","section":"Results and discussion","sentence":"Phenomenological models like HIJING [ref] , EPOS LHC [ref] and EPOS 3 [ref] reproduce the data better for the Pb-going side than for the proton-going side.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1210.4520","title":"Transverse momentum distribution and nuclear modification factor of charged particles in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV","url":"/paper/1210.4520","section":"Introduction","sentence":"The prediction from the HIJING 2.1 model [ref] describes, with shadowing, the trend seen in the data, although it seems that, with the present shadowing parameter $s_g$, the model underpredicts the data.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1710.09355","title":"Pseudorapidity distributions 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TeV","url":"/paper/2303.00590","section":"Introduction","sentence":"Among these effects, an important role is played by transverse momentum ($k_T$) broadening of initial- and final-state partons [ref] , and by the modification of the parton distributions functions in bound nucleons compared to those of free nucleons, leading in particular to a reduction of parton densities (shadowing) at small parton fractional momentum $x$ [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"1209.6030","title":"Nuclear modification of high transverse momentum particle production in p+A collisions at RHIC and LHC","url":"/paper/1209.6030","section":"Introduction","sentence":"There are also calculations and predictions for the nuclear modification factor in Monte Carlo models such as HIJING [ref] .","intent_p":0.94,"contests_p":null}]}],"unlabelled_sentences":15},"outgoing":{"papers":7,"sentences":7,"groups":[{"kind":"comparison","label":"Compares 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panel) collisions (solid) at $√(s)_NN=200$ GeV and 5.0 TeV, respectively, as compared to $d+Au$ data from the STAR experiment [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":4,"sentences":4,"quotes":[{"arxiv_id":"1006.0366","title":"Decoherence and energy loss in QCD cascades in nuclear collisions","url":"/paper/1006.0366","section":"Introduction","sentence":"Recent studies show that multiple parton scatterings inside a quark-gluon plasma can in fact change the the color flow of the jet parton shower from that in vacuum [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1009.2965","title":"Antiangular Ordering of Gluon Radiation in QCD Media","url":"/paper/1009.2965","section":"Introduction","sentence":"Recent studies show that multiple parton scatterings inside a quark-gluon plasma can in fact change the the color flow of the jet parton shower from that in vacuum [ref] 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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/1204.1998"}}