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.
5 pages, 2 figures
References in corpus (8)
- Nonperturbative Heavy-Quark Diffusion in the Quark-Gluon Plasma
- Radiative and Collisional Jet Energy Loss in the Quark-Gluon Plasma at RHIC
- -Meson as Quantitative Probe of Diffusion and Hadronization in Nuclear Collisions
- J/psi Production in Quark-Gluon Plasma
- Upsilon Production as a Probe for Early State Dynamics in High Energy Nuclear Collisions at RHIC
- Thermal Charm Production in Quark-Gluon Plasma at LHC
- production and elliptic flow in relativistic heavy-ion collisions
- Probe the tilted Quark-Gluon Plasma with charmonium directed flow