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VECTOR MESON RADIATION IN RELATIVISTIC HEAVY-ION COLLISIONS

机译:相对论重离子碰撞中的矢量介子辐射

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摘要

The (sigma,omega) model in the mean-field approximation where the meson fields are treated classically, describes much of observed nuclear structure and has been employed to describe the nuclear equation of state up to the quark-gluon phase transition. The acceleration of the meson sources, for example, in relativistic heavy-ion collisions, should result in bremsstrahlung-like radiation of the meson fields. The many mesons emitted serve to justify the use of classical meson fields. The slowing of the nuclei during the collision is modeled here as a smooth transition from initial to final velocity. Under ultra-relativistic conditions, vector radiation dominates. The angular distribution of energy flux shows a characteristic shape. It appears that if the vector meson field couples to the conserved baryon current, independent of the baryonic degrees of freedom, this mechanism will contribute to the radiation seen in relativistic heavy-ion collisions. The possible influence of the quark-gluon plasma is also considered. (C) 1997 Elsevier Science B.V. [References: 25]
机译:在平均场近似中对介子场进行经典处理的(sigma,omega)模型描述了观察到的大部分核结构,并已被用来描述直到夸克-胶子相变为止的状态核方程。介子源的加速,例如在相对论重离子碰撞中,应导致介子场的致辐射状辐射。发出的许多介子有助于证明经典介子场的使用。在碰撞过程中,原子核的减速在此建模为从初始速度到最终速度的平滑过渡。在超相对论条件下,矢量辐射占主导地位。能量通量的角度分布显示出特征形状。看来,如果矢量介子场耦合至守恒的重子电流,而与重子自由度无关,则该机理将有助于相对论重离子碰撞中的辐射。还考虑了夸克-胶子等离子体的可能影响。 (C)1997 Elsevier Science B.V. [参考:25]

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