{"arxiv_id":"hep-ph/0406201","incoming":{"papers":42,"sentences":51,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":5,"sentences":5,"quotes":[{"arxiv_id":"0812.0691","title":"Mass Hierarchy of Collisional Energy Loss","url":"/paper/0812.0691","section":"Model of collisional energy loss","sentence":"To evaluate radiative contribution we use ADSW quenching weights [ref] with $q̂ = 1$ GeV$^2$/fm and fix the pathlength at the same value of $L=5$ fm, the set of parameters being close to the one which produces the relevant factor 5 suppression in inclusive cross sections [ref] .","intent_p":0.94,"contests_p":null},{"arxiv_id":"1708.07571","title":"Energy density and path-length dependence of the fractional momentum loss in heavy-ion collisions at $\\sqrt{s_{\\rm NN}}$ from 62.4 to 5020 GeV","url":"/paper/1708.07571","section":"Introduction","sentence":"To this end, the ideas presented in [ref] were implemented.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1805.05145","title":"Measurement of the groomed jet mass in PbPb and pp collisions at $\\sqrt{s_{_\\mathrm{NN}}} =$ 5.02 TeV","url":"/paper/1805.05145","section":"The CMS apparatus and event selection","sentence":"Predictions for medium-modified jets are generated with 2.2.0 [ref] (both with and without recoil, , the scattered recoiling particles from the medium) and 1.0.3 [ref] where the PQM model [ref] is used to model the medium.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1012.0728","title":"Comparison of radiative energy loss models in a hot QCD medium","url":"/paper/1012.0728","section":"Multiple soft scattering approximation","sentence":"For the multiple soft scattering approximation $J_0^3$ and $J_1^3$ are used in which $T^3$ is replaced by the local $q̂(T)$ as is also done in PQM [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1511.06108","title":"Jet Fragmentation and Jet Shapes in JEWEL and Q-PYTHIA","url":"/paper/1511.06108","section":"Introduction","sentence":"to calculate an equivalent density for a uniform medium for each parton passing through the medium, as used in the PQM model [ref]","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":6,"sentences":6,"quotes":[{"arxiv_id":"1705.08856","title":"Absence of jet quenching in peripheral nucleus-nucleus collisions","url":"/paper/1705.08856","section":"Introduction","sentence":"For example, in the model calculation [ref] , the extracted transport coefficient changes by an order of magnitude from $0.1$ GeV$^2/$fm, ie. similar to cold nuclear matter, for $∼1$ in $80$–$92$% to $1$ GeV$^2$/fm, ie. hot nuclear matter, for $∼0.8$ in $60$–$70$% collisions at $=0.2$ TeV.","intent_p":0.84,"contests_p":null},{"arxiv_id":"0712.3443","title":"Introductory lectures on jet quenching in heavy ion collisions","url":"/paper/0712.3443","section":"Last comments","sentence":"We have quoted the values from [ref] of $q̂≃5...15$ GeV$^2$/fm.","intent_p":1.0,"contests_p":null},{"arxiv_id":"0903.5174","title":"Comparing energy loss phenomenology","url":"/paper/0903.5174","section":"Note on geometry","sentence":"For the case of $ρ_coll$ scaling, the parameter has been set to the same value as in the PQM model ($k_coll = 5 ·10^6 fm/A^2$ [ref] ).","intent_p":0.99,"contests_p":null},{"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":5,"sentences":5,"quotes":[{"arxiv_id":"1107.1862","title":"Centrality and pT dependence of charged particle RAA in PbPb collisions at sqrt(sNN) = 2.76 TeV","url":"/paper/1107.1862","section":"Results","sentence":"Measured $$ in the most central PbPb events (0–5 %) is compared to a number of model predictions, both for the LHC design energy of $√(s__NN)$ = 5.5 TeV (PQM [ref] and GLV [ref] ) and for the actual 2010 collision energy of $√(s__NN)$ = 2.76 TeV (ASW, YaJEM, and an elastic scattering energy-loss model with parameterized escape probability [ref] ).","intent_p":1.0,"contests_p":null},{"arxiv_id":"1202.2554","title":"Study of high-pT charged particle suppression in PbPb compared to pp collisions at sqrt(sNN)=2.76 TeV","url":"/paper/1202.2554","section":"Results","sentence":"The high-measurement of from this analysis, up to $= 100$, is also compared to a number of theoretical predictions, for the LHC design energy of $=5.5$(PQM [ref] with medium transport-coefficient $⟨q̂⟩=$ 30–80 $^2$/fm and GLV [ref] for various values of the medium gluon pseudorapidity density $N_g/y$) and for the actual collision energy of $=2.76$(ASW [ref] and YaJEM [ref] including a model for elastic energy loss parameterized with the $P_esc$ variable).","intent_p":1.0,"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},{"arxiv_id":"2010.02874","title":"Jet evolution in a dense QCD medium","url":"/paper/2010.02874","section":"JetMed in the landscape of in-medium event generators","sentence":"In the way the dominant medium effects are implemented, MATTER is close to the Q-PYTHIA and Q-HERWIG implementations of the in-medium parton shower [ref] (or [ref] which uses a similar idea) since medium-modified splitting functions are used.","intent_p":0.91,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":6,"sentences":6,"quotes":[{"arxiv_id":"2411.09647","title":"A unified description of small, peripheral, and large system suppression data from pQCD","url":"/paper/2411.09647","section":"Introduction","sentence":"A variety of partonic energy loss models [ref] based on perturbative Quantum Chromodynamics (pQCD) can, at least qualitatively, describe the $R_AB$ in heavy-ion collisions [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"2408.14426","title":"Collisional and radiative energy loss in small systems","url":"/paper/2408.14426","section":"Introduction","sentence":"Various semi-classical perturbative Quantum Chromodynamics (pQCD) models, which make different sets of approximations, have been successful in making qualitative predictions for the energy loss of hard probes in AA collisions [ref] .","intent_p":0.97,"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":"2410.05081","title":"Unraveling the Energy-Energy Correlators for Heavy Flavor Tagged Jets in pp, p+Pb and Pb+Pb Collisions","url":"/paper/2410.05081","section":"the jet quenching effect of the EEC observable in","sentence":"Since heavy quarks are viewed as effective hard probes to constrain the transport properties of QGP, A lot of theoretical models [ref] have been established to confront the experimental measurements, as seen in Refs. [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"2011.14909","title":"Progress in the Glauber model at collider energies","url":"/paper/2011.14909","section":"INTRODUCTION","sentence":"Another phenomenologically relevant quantity often derived from models is the average QGP path length $L(b)$ traversed by a given perturbative probe, such as an energetic parton, produced in the collision [ref] .","intent_p":0.87,"contests_p":null}]}],"unlabelled_sentences":29},"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/0406201"}}