Open quantum system approach for heavy quark thermalization
arXiv:2205.13302 · doi:10.1088/1674-1137/acbc0f
Abstract
We treat heavy quark as an open quantum system in the hot medium and rederive the Stochastic Schrödinger Equation (SSE) from the full Schrödinger equation for both heavy quarks and the medium. We apply the SSE to the dynamical evolutions of heavy quarks (as a system) in the static hot medium (as an environment). Heavy quarks interact with the medium via random scatterings, which exchange the momentum and phase factor randomly between two wave functions of the system and the environment. The exchange of momentum and phase factor results in the transition between different eigenstates of the system. These are included via an external stochastic potential in the Hamiltonian of SSE. Stochastic wave functions of heavy quarks are evolved with the stochastic external potential. The mean wave functions and the corresponding momentum distributions of heavy quarks are obtained after the ensemble average over a large set of stochastic wave functions. We present the thermalization of heavy quarks in the static medium with different coupling strength.
arXiv comment5 pages, 2 figures
References in corpus (38)
- Radiative energy loss of high energy quarks and gluons in a finite volume quark-gluon plasma
- How Much do Heavy Quarks Thermalize in a Heavy Ion Collision?
- Enhanced J/Psi Production in Deconfined Quark Matter
- Heavy Quark Anti-Quark Free Energy and the Renormalized Polyakov Loop
- Quark Coalescence for Charmed Mesons in Ultrarelativistic Heavy-Ion Collisions
- Nonperturbative Heavy-Quark Diffusion in the Quark-Gluon Plasma
- Linearized Boltzmann transport model for jet propagation in the quark-gluon plasma: Heavy quark evolution
- Extraction of Heavy-Flavor Transport Coefficients in QCD Matter
- Heavy quark dynamics and hadronization in ultra-relativistic heavy-ion collisions: collisional versus radiative energy loss
- Radiative and Collisional Jet Energy Loss in the Quark-Gluon Plasma at RHIC
- Heavy-Quark Diffusion and Hadronization in Quark-Gluon Plasma
- -Meson as Quantitative Probe of Diffusion and Hadronization in Nuclear Collisions
- In-Medium Effects on Charmonium Production in Heavy-Ion Collisions
- J/psi Production in Quark-Gluon Plasma
- Explanation of Di-jet asymmetry in Pb+Pb collisions at the Large Hadron Collider
- Quantum linear Boltzmann equation
- Azimuthal correlations of heavy quarks in Pb+Pb collisions at LHC ( TeV)
- Quantum and Classical Dynamics of Heavy Quarks in a Quark-Gluon Plasma
- Quarkonium In-Medium Transport Equation Derived from First Principles
- The Schrödinger-Langevin equation with and without thermal fluctuations
- Bottomonium suppression in an open quantum system using the quantum trajectories method
- Upsilon Production as a Probe for Early State Dynamics in High Energy Nuclear Collisions at RHIC
- Coupled Boltzmann Transport Equations of Heavy Quarks and Quarkonia in Quark-Gluon Plasma
- Quarkonium inside Quark-Gluon Plasma: Diffusion, Dissociation, Recombination and Energy Loss
- Improved Gauss law model and in-medium heavy quarkonium at finite density and velocity
- Open Quantum Systems for Quarkonia
- A stochastic approach to open quantum systems
- Thermal Charm Production in Quark-Gluon Plasma at LHC
- Quarkonium Semiclassical Transport in Quark-Gluon Plasma: Factorization and Quantum Correction
- Bottomonium Continuous Production from Unequilibrium Bottom Quarks in Ultrarelativistic Heavy Ion Collisions
- Quantum dissipation of a heavy quark from a nonlinear stochastic Schrödinger equation
- Gluon radiation by heavy quarks at intermediate energies
- Strong Diffusion Effect of Charm Quarks on Production in Pb-Pb collisions at the LHC
- Thermal Charm and Charmonium Production in Quark Gluon Plasma
- production and elliptic flow in relativistic heavy-ion collisions
- Probe the tilted Quark-Gluon Plasma with charmonium directed flow
- Charmonium production from nonequilibrium charm and anticharm quarks in quark-gluon plasma
- Thermal production of charm quarks in heavy ion collisions at Future Circular Collider