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Comparison of results from a 2+1D relativistic viscous hydrodynamic model to elliptic and hexadecapole flow of charged hadrons measured in Au-Au collisions at $\sqrt{s_{ m {NN}}}$ = 200 GeV

机译:比较2 + 1D相对论粘性流体动力学的结果   在au-au中测量的带电强子的椭圆和十六极流模型   碰撞$ \ sqrt {s _ {\ rm {NN}}} $ = 200 GeV

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摘要

Simulated results from a 2+1D relativistic viscous hydrodynamic model havebeen compared to the experimental data on the centrality dependence ofinvariant yield, elliptic flow ($v_{2}$), and hexadecapole flow ($v_{4}$) as afunction of transverse momentum ($p_{T}$) of charged hadrons in Au-Aucollisions at $\sqrt{s_{\rm {NN}}}$ = 200 GeV. Results from two types ofinitial transverse energy density profile, one based on the Glauber model andother based on Color-Glass-Condensate (CGC) are presented. We observe nodifference in the simulated results on the invariant yield of charged hadronsfor the calculations with different initial conditions. The comparison to theexperimental data on invariant yield of charged hadrons supports a shearviscosity to entropy density ratio ($\eta/s$) between 0 to 0.12 for the 0-10%to 40-50% collision centralities. The simulated $v_{2}(p_{T})$ is found to behigher for a fluid with CGC based initial condition compared to Glauber basedinitial condition for a given collision centrality. Consequently the Glauberbased calculations when compared to the experimental data requires a lowervalue of $\eta/s$ relative to CGC based calculations. In addition, a centralitydependence of the estimated $\eta/s$ is observed from the $v_{2}(p_{T})$ study.The $v_{4}(p_{T})$ for the collision centralities 0-10% to 40-50% supports a$\eta/s$ value between 0 - 0.08 for a CGC based initial condition. Whilesimulated results using the Glauber based initial condition for the ideal fluidevolution under estimates the $v_{4}(p_{T})$ for collision centralities 0-10%to 30-40%.
机译:已将2 + 1D相对论粘性流体力学模型的结果与不变屈服,椭圆流量($ v_ {2} $)和十六极流量($ v_ {4} $)作为横向函数的中心性相关的实验数据进行了比较= \ sqrt {s _ {\ rm {NN}}} $ = 200 GeV时Au-Aucollisions中带电强子的动量($ p_ {T} $)。给出了两种类型的初始横向能量密度分布图的结果,一种是基于Glauber模型的,另一种是基于彩色玻璃凝结的(CGC)。我们观察到模拟结果在带电强子不变产量的模拟结果中没有差异,用于不同初始条件下的计算。与带电强子不变产的实验数据的比较表明,对于0-10%至40-50%的碰撞中心,剪切粘度与熵密度比($ \ eta / s $)在0至0.12之间。对于给定的碰撞中心,发现基于CGC的初始条件的流体的模拟$ v_ {2}(p_ {T})$高于基于Glauber的初始条件的流体。因此,与实验数据相比,基于Glauber的计算相对于基于CGC的计算需要$ \ eta / s $的较低值。另外,从$ v_ {2}(p_ {T})$研究中可以观察到估计的$ \ eta / s $的中心性依赖性。碰撞中心性的$ v_ {4}(p_ {T})$ 0对于基于CGC的初始条件,-10%到40-50%支持0 / 0.08之间的$ \ eta / s $值。虽然使用基于Glauber的初始条件进行的理想流体演化的模拟结果在估计碰撞中心0-10%至30-40%的情况下估计为v_ {4}(p_ {T})$。

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