2020
DOI: 10.1103/physrevc.102.024906
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Sensitivity study with a D and B mesons modular simulation code of heavy flavor RAA and azimuthal anisotropies based on beam energy, initial conditions, hadronization, and su

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Cited by 37 publications
(33 citation statements)
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“…The theoretical uncertainties, when available, are displayed with a coloured band or a double line. Among the transport models, the mc@shq+epos2 [190], phsd [178], lbt [198], lido [114], bamps el+rad [173], and dab-mod(m&t) [199] calculations include charm-quark interactions with the medium constituents via both collisional (elastic) and radiative (gluon radiation) processes. In the tamu [170,200] powlang [201], and bamps el [173] models only the collisional processes are implemented.…”
Section: Comparison Of D-meson V 2 and R Aa To Theoretical Modelsmentioning
confidence: 99%
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“…The theoretical uncertainties, when available, are displayed with a coloured band or a double line. Among the transport models, the mc@shq+epos2 [190], phsd [178], lbt [198], lido [114], bamps el+rad [173], and dab-mod(m&t) [199] calculations include charm-quark interactions with the medium constituents via both collisional (elastic) and radiative (gluon radiation) processes. In the tamu [170,200] powlang [201], and bamps el [173] models only the collisional processes are implemented.…”
Section: Comparison Of D-meson V 2 and R Aa To Theoretical Modelsmentioning
confidence: 99%
“…All the considered pQCD-based energy-loss models (i.e. djordjevic [180], cu-jet3.0 [202], scet MG [203], and dab-mod(E loss ) [199] models) include radiative energyloss processes, while only djordjevic, cujet3.0, and dab-mod(E loss ) [199] calculations include also collisional processes. A positive v 2 in these calculations arises from the pathlength dependent energy loss.…”
Section: Comparison Of D-meson V 2 and R Aa To Theoretical Modelsmentioning
confidence: 99%
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“…Various formalisms, such as AMY [10], ASW [11], BDMPS-Z [12,13], DGLV [14,15], higher-twist [16,17], and SCET [18,19], have been developed for the phenomenology of light-flavor jet quenching in URHICs. Among them, some have been extended to massive quarks [11,[20][21][22][23][24] and implemented into numerical simulations for their transport in URHICs [8,[25][26][27][28][29][30], see also refs. [31] and [32,33] for recent comparisons between different energy loss formalisms for light-flavor jets and heavy quarks, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…Another observable extensively studied is the elliptic flow [33,34], v 2 ( p T ) = cos(2φ) , a measure of the anisotropy in the angular distribution of heavy mesons in momentum space, as a response to the initial anisotropy in coordinate space in non-central collisions. In literature several studies have been performed in these years, to study theoretically both these observables with the aim to understand heavy quark dynamics in QGP employing the Langevin or the on-shell Boltzmann transport equation [9,12,13,22,25,29,[35][36][37][38][39][40][41][42][43][44]. However, being the QGP strongly interacting, a full quantum description of the charm quark interaction should include in principle also the off-shell dynamics, an approach that has been developed only in [45] for the study of the transport coefficients and it is included in the PHSD approach to heavy-ion collisions [27,38,46].…”
Section: Introductionmentioning
confidence: 99%