Hydrodynamic description of D meson production in high-energy heavy-ion collisions

被引:7
作者
Ding, Chi [1 ,2 ]
Ke, Wei-Yao [3 ,4 ]
Pang, Long-Gang [1 ,2 ]
Wang, Xin-Nian [1 ,2 ,3 ,4 ]
机构
[1] Cent China Normal Univ, Key Lab Quark & Lepton Phys, MOE, Wuhan 430079, Peoples R China
[2] Cent China Normal Univ, Inst Particle Phys, Wuhan 430079, Peoples R China
[3] Univ Calif Berkeley, Phys Dept, Berkeley, CA 94720 USA
[4] Lawrence Berkeley Natl Lab, Nucl Sci Div, Berkeley, CA 94720 USA
基金
美国国家科学基金会; 中国国家自然科学基金;
关键词
D meson; relativistic hydrodynamics; heavy ion collisions; heavy flavor thermalization; HADRON; MODEL;
D O I
10.1088/1674-1137/abf645
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The large values and constituent-quark-number scaling of the elliptic flow of low- D mesons imply that charm quarks, initially produced through hard processes, might be partially thermalized through strong interactions with quark-gluon plasma (QGP) in high-energy heavy-ion collisions. To quantify the degree of thermalization of low-p(T) charm quarks, we compare the D-0 meson spectra and elliptic flow from a hydrodynamic model to experimental data as well as transport model simulations. We use an effective charm chemical potential at the freeze-out temperature to account for the initial charm quark production from hard processes and assume that they are thermalized in the local comoving frame of the medium before freeze-out. D-0 mesons are sampled statistically from the freeze-out hyper-surface of the expanding QGP as described by the event-by-event (3+1)D viscous hydrodynamic model CLVisc. Both the hydrodynamic and transport models can describe the elliptic flow of c as measured in Au+Au collisions at root s(NN) = 200 GeV, they deviate from the hydrodynamic model at high transverse momentum, c. The diffusion and parton energy loss mechanisms in the transport model can describe the measured spectra reasonably well within the theoretical uncertainty. Our comparative study indicates that charm quarks only approach local thermal equilibrium at small p(T), even though they acquire sizable elliptic flow comparable to light-quark hadrons at both small and intermediate p(T).
引用
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页数:9
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