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Dynamical freeze-out criterion in a hydrodynamical description of Au plus Au collisions at root s(NN)=200 GeV and Pb plus Pb collisions at root s(NN)=2760 GeV

机译:Root S(nn)= 200 gev和pb plus pb碰撞的Au Plus Au碰撞中的动态冻结标准在根S(nn)= 2760 gev

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摘要

In hydrodynamical modeling of ultrarelativistic heavy-ion collisions, the freeze-out is typically assumed to take place at a surface of constant temperature or energy density. A more physical approach is to assume that freeze-out takes place at a surface of constant Knudsen number. We evaluate the Knudsen number as a ratio of the expansion rate of the system to the pion-scattering rate and apply the constant Knudsen number freeze-out criterion to the ideal hydrodynamical description of heavy-ion collisions at the Relativistic Heavy Ion Collider at BNL (root s(NN) = 200 GeV) and the Large Hadron Collider (root s(NN) = 2760 GeV) energies. We see that once the numerical values of freeze-out temperature and freeze-out Knudsen number are chosen to produce similar pT distributions, the elliptic and triangular anisotropies are similar too, in both event-by-event and averaged initial state calculations.
机译:在超弧度重离子碰撞的流体动力学建模中,通常假设冻结在恒温或能量密度的表面处发生。 更具物理方法是假设冻结在恒定的knudsen号的表面处发生。 我们将knudsen数评价为系统的膨胀率与沟散射速率的比率,并将恒定的knudsen数冻结标准应用于BNL的相对论重离子撞机的重离子碰撞的理想流体动力学描述( 根S(NN)= 200 GEV)和大型强子撞机(根S(NN)= 2760 GEV)能量。 我们看到,一旦选择冻结温度和冻结knudsen数的数值被选择以产生类似的PT分布,就在逐个事件和平均初始态计算中也是相似的椭圆形和三角形各向异性。

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