2018
DOI: 10.5506/aphyspolb.49.1325
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Discrimination of Effective Radiative and Collisional In-medium Energy-loss Models by Their Effects on Angular Jet Structure

Abstract: Energy-loss studies of hard particle probes produced in heavy ion collisions have often been used to get information on the interactions within the medium of a quark-gluon plasma (QGP). However, with the study of inmedium energy-loss of individual particles alone, it remains still ambiguous, whether the occured decrease in particle energy is caused by predominantly radiative or collisional energy-loss mechanisms. Focusing on the in-medium energy-loss of hard jet-partons, we propose additional studies of the an… Show more

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Cited by 5 publications
(7 citation statements)
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“…Each initial hard parton leads to a development of a time-like parton cascade, due to collinear parton splitting caused by bremsstrahlung. The evolution of the parton cascade is performed with a Monte Carlo algorithm [4] representing the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation with leading order q → qg, g → gg and g → q q splitting functions. The evolution of each parton cascade proceeds from an initial virtuality scale Q ↑ given by the EPOS initial state down to a minimal virtuality scale of Q ↓ = 0.6 GeV.…”
Section: Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…Each initial hard parton leads to a development of a time-like parton cascade, due to collinear parton splitting caused by bremsstrahlung. The evolution of the parton cascade is performed with a Monte Carlo algorithm [4] representing the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation with leading order q → qg, g → gg and g → q q splitting functions. The evolution of each parton cascade proceeds from an initial virtuality scale Q ↑ given by the EPOS initial state down to a minimal virtuality scale of Q ↓ = 0.6 GeV.…”
Section: Modelmentioning
confidence: 99%
“…However, it is becoming more understood now [3] that a precise modeling of the background medium evolution is an important component for quantitative description of jet structure in heavy ion collisions. In this report take a first look on the jet structure from a time-like parton cascade [4] coupled with the EPOS3-HQ framework [5]. In particular we show how the transverse expansion of the medium affects the jet structure, and explore the back reaction of the jet to the medium.…”
Section: Introductionmentioning
confidence: 99%
“…[59,63]. In the present investigation, we focus our attention to the collisional energy loss of HQ in the background of a constant magnetic field which may be relevant for the HICs as discussed in literature [63][64][65][66][67].…”
Section: Jhep05(2020)068mentioning
confidence: 99%
“…Each initial hard parton leads to the development of a time-like parton cascade, due to collinear parton splitting caused by bremsstrahlung. The evolution of the parton cascade is performed with a Monte Carlo algorithm [3] representing the Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) equation with leading order q → qg, g → gg and g → q q splitting functions. The evolution of each parton cascade proceeds from an initial virtuality scale Q ↑ , which we set to be equal to parton's p ⊥ , down to a minimal virtuality scale of Q ↓ = 0.6 GeV.…”
Section: Modelmentioning
confidence: 99%