2020
DOI: 10.48550/arxiv.2001.02766
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Partonic transport model application to heavy flavor

Abstract: Heavy-flavor particles are excellent probes of the properties of the hot and dense nuclear medium created in the relativistic heavy-ion collisions. Heavyflavor transport coefficients in the quark-gluon plasma (QGP) stage of the collisions are particularly interesting, as they contain important information on the strong interaction at finite temperatures. Studying the heavy-flavor evolution in a dynamically evolving medium requires a comprehensive multistage modeling approach of both the medium and the probes, … Show more

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Cited by 2 publications
(2 citation statements)
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References 209 publications
(336 reference statements)
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“…This suggests that induced-radiation processes alone can build up energy storage near the thermal scale p ∼ T , no matter how energetic the initial hard jets are. Such behavior has also been confirmed in recent numerical simulations including the effective kinetic theory with resummed radiation vertex [84] and the LIDO transport model in the large-medium L med τ f limit, which is discussed in section 3.5.3 of [85]. We will see immediately that this feature indeed emerges from our simulation.…”
Section: Energy Transport Via Vacuum and Induced Radiationssupporting
confidence: 85%
“…This suggests that induced-radiation processes alone can build up energy storage near the thermal scale p ∼ T , no matter how energetic the initial hard jets are. Such behavior has also been confirmed in recent numerical simulations including the effective kinetic theory with resummed radiation vertex [84] and the LIDO transport model in the large-medium L med τ f limit, which is discussed in section 3.5.3 of [85]. We will see immediately that this feature indeed emerges from our simulation.…”
Section: Energy Transport Via Vacuum and Induced Radiationssupporting
confidence: 85%
“…Although an explicit parametric form is intuitive and meaningful to humans, it is unnecessarily complicated for machine learning as it often contains strong non-linear correlations. For example, in the parametrization of a previous study [102] q/T 3 = (1 + (aT /T c ) p ) −1 , a linear variation in a or p causes a strong non-linear change in the effective value of q. Even though the physical model maps values of q to observables in a rather well-behaved fashion, the performance of the emulator can still be impaired by the non-linear response to those individual input parameters.…”
Section: A the Prior Distribution Of An Unknown Function As A Random ...mentioning
confidence: 99%