{"arxiv_id":"hep-ph/0406319","incoming":{"papers":34,"sentences":45,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1104.4924","title":"Non-commutative Holographic QCD and Jet Quenching Parameter","url":"/paper/1104.4924","section":"Introduction","sentence":"The time-averaged jet quenching parameter determined in comparison with RHIC data was found to be around 5-15 Gev$^2$/fm [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"0907.1219","title":"Lectures on high-energy heavy-ion collisions at the LHC","url":"/paper/0907.1219","section":"Jet quenching","sentence":"* Taking the same geometry, a cylinder of radius $L=6$ fm, but now computing the suppression of the yields before averaging in the length, the resulting value is[The same value is obtained if instead of a cylinder a Woods–Saxon distribution is assumed for the energy density [ref] .] $q̂≃5÷15$ GeV$^2$/fm [ref] .","intent_p":0.92,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":3,"sentences":4,"quotes":[{"arxiv_id":"1003.1692","title":"On heavy-quarkonia suppression by final-state multiple scatterings in most central Au+Au collisions at RHIC","url":"/paper/1003.1692","section":"Discussion of the fits","sentence":"Our results of $q̂_0 ≃0.33 - 0.95 ^2$/fm are in sharp contrast with those obtained by the analysis of high-$p_T$ hadron spectra in Ref. [ref] in which the authors conclude that the values of the time-averaged $q̂$ exceed $5 ^2$/fm.","intent_p":0.9,"contests_p":null},{"arxiv_id":"1407.2233","title":"Investigating jet quenching on the lattice","url":"/paper/1407.2233","section":"Lattice study","sentence":"This value is close to those obtained from holography [ref] and from phenomenological models [ref] (even though the latter exhibit some dependence on the details of the underlying approach [ref] , and more recent studies suggest smaller values [ref] ).","intent_p":1.0,"contests_p":null},{"arxiv_id":"1407.2963","title":"Jet quenching from the lattice","url":"/paper/1407.2963","section":"Discussion and conclusions","sentence":"This value is close to estimates obtained from holographic studies [ref] , and also from certain phenomenological model computations [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":2,"sentences":2,"quotes":[{"arxiv_id":"0705.3060","title":"Mapping out the Jet correlation landscape: Jet quenching and Medium response","url":"/paper/0705.3060","section":"Introduction","sentence":"But single hadron yield can't constrain the shape of $P^'(ΔE)=∫dϕdrP(ΔE,ϕ, r)$, hence the dynamics of energy loss models, very well (the fragility [ref] ).","intent_p":0.97,"contests_p":null},{"arxiv_id":"0908.2306","title":"Jet Quenching in Heavy Ion Collisions","url":"/paper/0908.2306","section":"Trigger biases","sentence":"This may limit the ability of testing the medium with single inclusive hadron spectra [ref] , simply since the sample of hard processes selected by measuring single inclusive hadrons cannot be embedded deeply into the medium, and since the surface bias induces additional uncertainties in analyzing the medium modification.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":5,"sentences":5,"quotes":[{"arxiv_id":"1002.1165","title":"Bulk matter evolution and extraction of jet transport parameter in heavy-ion collisions at RHIC","url":"/paper/1002.1165","section":"Introduction","sentence":"Extensive phenomenological studies on the suppression of single hadron spectra [ref] and dihadron correlations [ref] at large transverse momentum have been carried out since the first observation of the strong jet quenching phenomena.","intent_p":0.92,"contests_p":null},{"arxiv_id":"1809.02525","title":"Interplaying mechanisms behind single inclusive jet suppression in heavy-ion collisions","url":"/paper/1809.02525","section":"Introduction","sentence":"The simplest form of jet quenching is the suppression of single inclusive hadron spectra at large transverse momentum, dihadron and $γ$-hadron correlation in heavy-ion collisions relative to proton-proton collisions [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1712.05603","title":"Constraints on jet quenching in p-Pb collisions at $\\mathbf{\\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of semi-inclusive hadron-jet distributions","url":"/paper/1712.05603","section":"Observable and raw data","sentence":"For collision systems in which jet quenching occurs, selection of high- hadrons is thought to bias towards the fragments of jet that have experienced little quenching, due to the combined effect of jet energy loss and the shapes of the inclusive jet production and the jet fragmentation distributions [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"0705.1047","title":"Chromohydrodynamical instabilities induced by relativistic jets","url":"/paper/0705.1047","section":"Introduction","sentence":"In order to describe these processes and the subsequent modification of the hadronic spectra due to the interaction of the high $p_T$ partons with the medium, various models have been proposed where perturbative QCD is supplemented with medium-induced parton energy loss [ref] or where the AdS/CFT correspondence [ref] is employed.","intent_p":0.9,"contests_p":null},{"arxiv_id":"0707.3893","title":"Jet-induced gauge field instabilities in the quark-gluon plasma: A kinetic theory approach","url":"/paper/0707.3893","section":"Introduction","sentence":"The description of this process is currently undertaken employing various models, where perturbative QCD is supplemented with medium-induced parton energy loss [ref] or where the AdS/CFT correspondence [ref] is employed.","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":32},"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/hep-ph/0406319"}}