Heavy Quark Diffusion with Relativistic Langevin Dynamics in the Quark-Gluon Fluid
arXiv:0809.1499 · doi:10.1103/PhysRevC.79.054907
Abstract
The relativistic diffusion process of heavy quarks is formulated on the basis of the relativistic Langevin equation in Itô discretization scheme. The drag force inside the quark-gluon plasma (QGP) is parametrized according to the formula for the strongly coupled plasma obtained by the AdS/CFT correspondence. The diffusion dynamics of charm and bottom quarks in QGP is described by combining the Langevin simulation under the background matter described by the relativistic hydrodynamics. Theoretical calculations of the nuclear modification factor R_{AA} and the elliptic flow v_{2} for the single electrons from the charm and bottom decays are compared with the experimental data from the relativistic heavy ion collisions. The R_{AA} for electrons with large transverse momentum (p_{T} > 3 GeV) indicates that the drag force from the QGP is as strong as the AdS/CFT prediction.
13 pages, 10 figures
References in corpus (9)
- The order of the quantum chromodynamics transition predicted by the standard model of particle physics
- Energy Loss and Flow of Heavy Quarks in Au+Au Collisions at sqrt(s_NN) = 200 GeV
- Heavy quark diffusion in perturbative QCD at next-to-leading order
- Comparing the drag force on heavy quarks in N=4 super-Yang-Mills theory and QCD
- The effect of partonic wind on charm quark correlations in high-energy nuclear collisions
- Centrality-dependent direct photon pt spectra in Au+Au collisions at RHIC
- Theoretical developments in heavy and light flavor energy loss
- Onset of Melting in Quark-Gluon Fluid at RHIC
- Jet-fluid string formation and decay in high-energy heavy-ion collisions