6533b82afe1ef96bd128c2a2

RESEARCH PRODUCT

Quantum and classical dynamics of heavy quarks in a quark-gluon plasma

Jean-paul BlaizotMiguel A. Escobedo

subject

heavy quarksheavy ion: scatteringNuclear Theoryapproximation: semiclassicalHigh Energy Physics::LatticeMonte Carlo methoddensity matrix: reducedhiukkasfysiikkaquantum chromodynamics: plasma01 natural sciencesBoltzmann equationLangevin equationHigh Energy Physics - Phenomenology (hep-ph)quarkonium: heavyquantum electrodynamicsQuarkonium suppression[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]quark gluon: plasmaMathematical physics[PHYS]Physics [physics]Quantum chromodynamicsPhysicsquarkonium: suppressionBoltzmann equationquark gluon plasmaLangevin equationHigh Energy Physics - Phenomenologyheavy quark: couplingQuarkNuclear and High Energy Physicsquark-gluon plasma[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesNuclear Theory (nucl-th)quantum chromodynamics0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivityheavy quarkstochastic010306 general physicsplasma: weak couplingta114010308 nuclear & particles physicsHigh Energy Physics::Phenomenologykvarkki-gluoniplasmaTime evolutionPlasmaHeavy Ion Phenomenologyfree energyrecombinationabelian[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Quark–gluon plasmalcsh:QC770-798[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment

description

We derive equations for the time evolution of the reduced density matrix of a collection of heavy quarks and antiquarks immersed in a quark gluon plasma. These equations, in their original form, rely on two approximations: the weak coupling between the heavy quarks and the plasma, the fast response of the plasma to the perturbation caused by the heavy quarks. An additional semi-classical approximation is performed. This allows us to recover results previously obtained for the abelian plasma using the influence functional formalism. In the case of QCD, specific features of the color dynamics make the implementation of the semi-classical approximation more involved. We explore two approximate strategies to solve numerically the resulting equations in the case of a quark-antiquark pair. One involves Langevin equations with additional random color forces, the other treats the transition between the singlet and octet color configurations as collisions in a Boltzmann equation which can be solved with Monte Carlo techniques.

https://doi.org/10.1007/jhep06(2018)034