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Jet Quenching
High Energy Physics - Phenomenology · Submitted 4 Sep 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A short summary of the physics underlying jet quenching is given
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
A short summary of the physics underlying jet quenching is given
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A short summary of the physics underlying jet quenching is given | contribution 0.86 | 0.49 | 0.08 | asserted 0.82 |
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The paper
Original abstract
A short summary of the physics underlying jet quenching is given
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References
How the literature uses it
54 arXiv papers cite this in 64 sentences
Papers citing it · 38 sentences without a confident label
Uses its method or tool 3 papers
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Accounting for the expansion of the produced medium, it reads [ref] [equation] assuming a purely longitudinal expansion.
Quenching of photon and pion spectra at intermediate RHIC energy · Nuclear effects in Au–Au collisions · 0.87
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From the energy dissipation we have evaluated the shear viscosity ($η$) to entropy ($s$) density ratio using the relation [ref] : $η/s∼1.25T^3/q̂$, where $q̂= ⟨p^2_T⟩/L$ and $dE/dx∼α_s⟨p^2_T⟩$ [ref] , $L$ is the length traversed by the heavy quark.
In search of quark gluon plasma in nuclear collisions · Elliptic flow of heavy flavours · 0.92
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From the energy dissipation we have evaluated the shear viscosity ($η$) to entropy ($s$) density ratio using the relation [ref] : $η/s∼1.25T^3/q̂$, where $q̂= ⟨p^2_T⟩/L$ and $dE/dx∼α_s⟨p^2_T⟩$ [ref] , $L$ is the length traversed by the heavy quark and $p_T$ is its transverse momentum.
Elliptic flow of heavy flavors · Introduction · 0.95
Compares with it 4 papers
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At early times, we find $q̂∼1$ GeV$^3$ independent of initial quark energy, about an order of magnitude larger than estimates from pQCD [ref] , and, necessarily, similar to the original $v≈1$ AdS/CFT estimate [ref] .
A semi-classical recipe for wobbly limp noodles in partonic soup · Discussion and Outlook · 0.99
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This number is large compared to expectations for a perturbative QCD plasma, $q̂≃(1-2)GeV^2/fm$ [ref] .
Strongly Correlated Quantum Fluids: Ultracold Quantum Gases, Quantum Chromodynamic Plasmas, and Holographic Duality · Jet Quenching · 0.87
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This is reminiscent of the mechanism of energy loss of a heavy, or light, quark at weak coupling [ref] , with the main difference being in the cause of the medium–induced radiation.
Stochastic trailing string and Langevin dynamics from AdS/CFT · Introduction · 0.85
Cites it as support 2 papers
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However, observed high- hadrons are expected to arise predominantly from jets which experience relatively little medium-induced energy loss, due to the interplay of the steeply falling inclusive jet energy spectrum shape, the hadron fragmentation function, and energy loss [ref] .
Measurements of jet quenching using semi-inclusive hadron+jet distributions in pp and central Pb$-$Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV · Introduction · 0.96
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However, selection of high- hadrons is expected from model studies to bias towards leading fragments of jets that have experienced little quenching, due to the interplay of jet energy loss, the shape of the jet production spectrum, and jet fragmentation [ref] , and thereby limiting the effects of quenching on the trigger bias.
Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV · Discussion of observables · 0.97
Cites it as background 15 papers
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Jet evolution can be characterized by the jet quenching parameter $q̂$ [ref] that measures its transverse momentum broadening square per unit time due to elastic scatterings.
Partonic Critical Opalescence and Its Impact on the Jet Quenching Parameter $\hat{q}$ · Introduction · 0.98
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The transport coefficient $q̂$ [ref] is the mean squared transverse momentum acquired by the parton per unit length and $τ$ is the formation time (equal to the formation length for light-like particles) given by [equation] In the second stage, the multiple scattering and rare emissions on average maintain the virtuality at the medium scale, namely the acquired transverse momentum: $μ^2 ≈μ_med^2 = q̂ τ$.
Modified Coherence and the Transverse Extent of Jets · Introduction · 0.96
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A transition in the dynamics occurs once the virtuality approaches the medium induced scale $μ_S^2 ∼q̂ τ$ [ref] , where $q̂$ is transverse momentum transport coefficient, defined as, [equation] the mean transverse momentum square accrued per unit length by a single parton by scattering in the medium [ref] , and $τ$ is the lifetime of a given parton in the medium.
Final State Gluon Emission in Deep-Inelastic Scattering at Next-to-Leading Twist · Introduction · 0.80
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