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Gluon radiation by heavy quarks at intermediate energies
High Energy Physics - Phenomenology · Submitted 19 Jul 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In the regime of accessible phenomenology we observe that the emission at small transverse momentum (dead cone effect) is less suppressed than originally suggested.
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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
Employing scalar QCD we study the gluon emission of heavy quarks created by the interaction with light quarks considered as dynamical scattering centers. We develop approximation formulas for the high energy limit and study when the full calculation reaches this high energy limit. For zero quark masses and in the high energy limit our model reproduces the Gunion-Bertsch results. We justify why scalar QCD represents a good approximation to the full QCD approach for the energy loss of heavy quarks. In the regime of accessible phenomenology we observe that the emission at small transverse momentum (dead cone effect) is less suppressed than originally suggested. We also investigate the influence of a finite gluon mass on the discussed results.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Employing scalar QCD we study the gluon emission of heavy quarks created by the interaction with light quarks considered as dynamical scattering centers. | contribution 0.68 | 0.93 | 0.05 | asserted 0.90 |
| s1 | We develop approximation formulas for the high energy limit and study when the full calculation reaches this high energy limit. | contribution 0.72 | 0.96 | 0.07 | asserted 0.96 |
| s2 | For zero quark masses and in the high energy limit our model reproduces the Gunion-Bertsch results. | result 0.98 | 0.79 | 0.12 | asserted 1.00 |
| s3 | We justify why scalar QCD represents a good approximation to the full QCD approach for the energy loss of heavy quarks. | contribution 0.54 | 0.91 | 0.15 | asserted 1.00 |
| s4 | In the regime of accessible phenomenology we observe that the emission at small transverse momentum (dead cone effect) is less suppressed than originally suggested. | result 1.00 | 0.94 | 0.42 | asserted 1.00 |
| s5 | We also investigate the influence of a finite gluon mass on the discussed results. | contribution 0.98 | 0.87 | 0.05 | unclear 0.69 |
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The paper
Original abstract
Employing scalar QCD we study the gluon emission of heavy quarks created by the interaction with light quarks considered as dynamical scattering centers. We develop approximation formulas for the high energy limit and study when the full calculation reaches this high energy limit. For zero quark masses and in the high energy limit our model reproduces the Gunion-Bertsch results. We justify why scalar QCD represents a good approximation to the full QCD approach for the energy loss of heavy quarks. In the regime of accessible phenomenology we observe that the emission at small transverse momentum (dead cone effect) is less suppressed than originally suggested. We also investigate the influence of a finite gluon mass on the discussed results.
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References
How the literature uses it
17 arXiv papers cite this in 26 sentences
Papers citing it · 16 sentences without a confident label
Builds on it 1 paper
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For the incoherent gluon radiation spectra the calculation in [ref] are extended to finite quark masses [ref] .
Elliptic and triangular flow of heavy flavor in heavy-ion collisions · Introduction · 0.97
Uses its method or tool 5 papers
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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.
Degrees of Freedom of the Quark Gluon Plasma, tested by Heavy Mesons · The standard MC@sHQ approach · 0.89
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Heavy quarks propagate through the QGP and experience elastic [ref] and radiative collisions [ref] with the plasma constituents (assumed to be massless).
Towards the determination of heavy-quark transport coefficients in quark-gluon plasma · Nantes approach · 0.81
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We include both, elastic [ref] and radiative [ref] collisions.
System size dependence of energy loss and correlations of heavy mesons at LHC energies · heavy quark production and evolution in EPOS4 · 0.89
Compares with it 2 papers
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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] .
Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV · Results · 0.97
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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.
Extraction of Heavy-Flavor Transport Coefficients in QCD Matter · Reference Results in an Infinite and Finite QGP · 0.94
Cites it as support 1 paper
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The suppression of the emission of gluons with finite masses has been shown in Ref. [ref] .
Exploring jet transport coefficients by elastic scattering in the strongly interacting quark-gluon plasma · Introduction · 1.00
Cites it as background 1 paper
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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] .
Inelastic and elastic parton scatterings in the strongly interacting quark-gluon plasma · Introduction · 0.98
What it cites · 3 sentences without a confident label
Uses the method or tool of 1 paper
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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] .
Radiative parton processes in perturbative QCD - an improved version of the Gunion and Bertsch cross section from comparisons to the exact result · Introduction · 0.81
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