Directed flow and freeze-out in relativistic heavy-ion collisions at NICA and FAIR energies

L. Bravina, Yu. Kvasiuk, D. Sachenko, S. Sivoklokov, O. Vitiuk, E. Zabrodin
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Abstract

Directed flow of charged particles is studied in nucleus-nucleus collisions simulated within the energy range accessible for NICA and FAIR facilities. Two transport cascade models, UrQMD and QGSM, are employed. These models use different mechanisms of the string excitation and string fragmentation. Despite of the differences, directed flows of charged pions and charged kaons in both models remain antiflow-oriented with reduction of the collision energy from $\sqrt{s} = 11.5$~GeV to 3.5~GeV. In contrast, the directed flow of protons changes its sign from antiflow to normal flow within the investigated energy interval. Both models favor continuous non-uniform emittence of hadrons from the expanding fireball rather than sharp, or sudden, freeze-out picture adopted by majority of hydrodynamic models. We found that the earlier frozen hadrons carry the strongest directed flow at midrapidity, although the flow development even at $|y| \leq 0.5$ takes about 8-12~fm/$c$ for different hadron species.
NICA和FAIR能量下相对论性重离子碰撞中的定向流动和冻结
在NICA和FAIR设备可及的能量范围内,研究了模拟核-核碰撞中带电粒子的定向流动。采用了UrQMD和QGSM两种传输级联模型。这些模型使用了不同的弦激发和弦破碎机制。尽管存在差异,但两种模型中带电介子和带电介子的定向流动仍然是反流动的,碰撞能量从$\sqrt{s} = 11.5$ GeV降低到3.5 GeV。相反,质子定向流在所研究的能量区间内由反流变为正流。这两种模型都倾向于从膨胀的火球中连续而不均匀地发射强子,而不是大多数流体动力学模型所采用的尖锐或突然的冻结图像。我们发现较早的冰冻强子在中速时携带最强的定向流,尽管不同强子种类在$|y| \leq 0.5$处的流动发展大约需要8-12 fm/ $c$。
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