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THE DECONFINEMENT PHASE TRANSITION IN ASYMMETRIC MATTER

机译:不对称物质中的超限定相变

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摘要

We study the phase transition of asymmetric hadronic matter to a quark-gluon plasma within the framework of a simple two-phase model. The analysis is performed in a system with two conserved charges (baryon number and isospin) using the stability conditions on the free energy, the conservation laws and Gibbs' criteria for phase equilibrium. The EOS is obtained in a separate description for the hadronic phase and for the quark-gluon plasma. For the hadrons, a relativistic mean-field model calibrated to the properties of nuclear matter is used, and a bag-model type EOS is used for the quarks and gluons. The model is applied to the deconfinement phase transition that may occur in matter created in ultra-relativistic collisions of heavy ions. Based on the two-dimensional coexistence surface (binodal), various phase separation scenarios and the Maxwell construction through the mixed phase are discussed. In the framework of the two-phase model the phase transition in asymmetric matter is continuous (second-order by Ehrenfest's definition) in contrast to the discontinuous (first-order) transition of symmetric systems. (C) 1997 Elsevier Science B.V. [References: 41]
机译:我们在一个简单的两相模型的框架内研究了不对称强子物质向夸克-胶子等离子体的相变。该分析是在具有两个守恒电荷(重子数和同位旋)的系统中使用自由能的稳定性条件,守恒律和吉布斯的相平衡标准进行的。 EOS在强子相和夸克-胶子等离子体的单独描述中获得。对于强子,使用针对核物质特性校准的相对论平均场模型,而夸克和胶子则使用袋模型EOS。该模型适用于在重离子的超相对论碰撞中产生的物质中可能发生的脱限相变。基于二维共存表面(二面体),讨论了各种相分离方案和混合相中的麦克斯韦构造。在两相模型的框架中,与对称系统的不连续(一阶)跃迁相反,非对称物质中的相变是连续的(根据埃伦菲斯特的定义为二阶)。 (C)1997 Elsevier Science B.V. [参考:41]

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