Perturbative and non-perturbative interactions between heavy quarks and quark-gluon plasma within a unified approach

TL;DR

This paper develops a unified model combining perturbative and non-perturbative interactions to describe heavy quark behavior in quark-gluon plasma, successfully explaining experimental data across a wide momentum range.

Contribution

It introduces a generalized Cornell potential into the Boltzmann transport model, enabling a comprehensive description of heavy flavor suppression and flow in heavy-ion collisions.

Findings

Extracted in-medium heavy quark potential consistent with lattice QCD

Achieved simultaneous description of R_AA and v_2 at various p_T

Highlighted importance of non-perturbative interactions at low and intermediate p_T

Abstract

While perturbative QCD is sufficient for understanding the color, mass and energy dependences of parton energy loss and jet quenching at large transverse momentum in heavy-ion collisions, a simultaneous description of heavy flavor nuclear modification factor $R_\mathrm{AA}$ and elliptic flow coefficient $v_2$ at low and intermediate $p_\mathrm{T}$ still remains a challenge due to the effects from non-perturbative interactions. In this work, we extend the linear Boltzmann transport model by implementing a generalized Cornell-type potential that incorporates both short-range Yukawa interaction and long-range color confining interaction between heavy quarks and the QGP medium. Combining our new approach for heavy-quark-QGP interaction with a (3+1)-dimensional hydrodynamic model CLVisc for the QGP evolution and a hybrid fragmentation-coalescence model for heavy quark hadronization, we obtain a satisfactory description of heavy meson $R_\mathrm{AA}$ and $v_2$ from low to intermediate to high $p_\mathrm{T}$ observed at both RHIC and the LHC. By model-data-comparison, we extract for the first time the in-medium heavy quark potential from open heavy flavor measurements; the result is in agreement with the lattice QCD calculation. Our study indicates that while jet quenching at high $p_\mathrm{T}$ is dominated by perturbative QCD interactions, non-perturbative interactions are indispensible for understanding heavy flavor quenching and flow at low and intermediate $p_\mathrm{T}$.