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Comparison of results from a (2+1)-D relativistic viscous hydrodynamic model to elliptic and hexadecapole flow of charged hadrons measured in Au-Au collisions at sNN = 200 GeV

机译:(2 + 1)-D相对论粘性流体力学模型与在sNN = 200 GeV的Au-Au碰撞中测量的带电强子的椭圆和十六极流的比较

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Simulated results from a (2+1)-D relativistic viscous hydrodynamic model have been compared to thenexperimental data on the centrality dependence of invariant yield, elliptic flow (v2), and hexadecapole flow (v4)nas a function of transverse momentum (pT ) of charged hadrons in Au-Au collisions atn√nsNN = 200 GeV. Resultsnfrom two types of initial transverse energy density profile, one based on the Glauber model and other based onnthe color glass condensate (CGC) model, are presented. We observe no difference in the simulated results onnthe invariant yield of charged hadrons for the calculations with different initial conditions. The comparison tonthe experimental data on invariant yield of charged hadrons supports a shear-viscosity to entropy-density ration(η/s) between 0 and 0.12 for the 0%–10% to 40%–50% collision centralities. The simulated v2(pT ) is found tonbe higher for a fluid with CGC based initial condition compared to Glauber based initial condition for a givenncollision centrality. Consequently the Glauber based calculations when compared to the experimental data requirena lower value of η/s relative to CGC based calculations. In addition, a centrality dependence of the estimatednη/s is observed from the v2(pT ) study. The v4(pT ) for the collision centralities 0%–10% to 40%–50% supports anη/s value between 0 and 0.08 for a CGC based initial condition. Simulated results using the Glauber based initialncondition for the ideal fluid evolution underestimate the v4(pT ) for collision centralities 0%–10% to 30%–40%.
机译:将(2 + 1)-D相对论粘性流体力学模型的模拟结果与不变屈服,椭圆流(v2)和十六极流(v4)的中心性相关性的实验数据进行了比较,这是横向动量(pT)的函数Au-Au碰撞中带电强子的数量为n√nsNN= 200 GeV。提出了两种类型的初始横向能量密度分布图的结果,一种基于Glauber模型,另一种基于彩色玻璃冷凝物(CGC)模型。我们观察到在不同初始条件下,带电强子的不变产量的模拟结果没有差异。带电强子不变屈服的实验数据的比较结果表明,对于0%–10%至40%–50%的碰撞中心,剪切粘度与熵密度比(η/ s)在0至0.12之间。对于给定的碰撞中心度,与基于GGC的初始条件相比,对于基于CGC的初始条件,发现模拟的v2(pT)更高。因此,与实验数据相比,基于Glauber的计算相对于基于CGC的计算需要较低的η/ s值。此外,从v2(pT)研究中可以观察到估计值n / s的中心依赖性。对于基于CGC的初始条件,碰撞中心0%–10%到40%–50%的v4(pT)支持n / s值在0和0.08之间。使用基于Glauber的理想流体演化初始条件的模拟结果低估了碰撞中心0%–10%到30%–40%的v4(pT)。

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