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arXiv 1408.0958hep-phhep-lathep-th
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用$T$矩阵方法计算SUSY Yang-Mills等离子体

The SUSY Yang-Mills plasma in a $T$-matrix approach

G. Lacroix, C. Semay, F. Buisseret

摘要:

研究了具有任意规范群的${\cal N}=1$超对称Yang-Mills理论的热力学性质。在有限的范围内,我们表明,识别的束缚态谱与Hagedorn一个来自非临界封闭超弦理论导致预测的值的退澄清温度$T_c$,同意最近的晶格数据。退罚款阶段的研究诉诸$T$ -矩阵制定的统计力学,其中所研究的介质被看作是一个气体的quasigluons和quasigluinos相互作用非微扰。重点讨论了(1-5)~ $T_c$的温度范围,在这个温度范围内相互作用足够强,可以产生束缚态。对于任何规范群,胶子和胶子的二元束缚态确实被发现束缚到1.4 $T_c$。然后数值计算SU($N$)和$G_2$的状态方程,并在任意规范群的情况下进行了讨论。当归一化到Stefan-Boltzmann压力并表示为$T/T_c$的函数时,发现它几乎与规范群无关,并且非常接近于非超对称杨-米尔斯的结果.

英文摘要:

The thermodynamic properties of ${\cal N}=1$ supersymmetric Yang-Mills theory with an arbitrary gauge group are investigated. In the confined range, we show that identifying the bound state spectrum with a Hagedorn one coming from non-critical closed superstring theory leads to a prediction for the value of the deconfining temperature $T_c$ that agrees with recent lattice data. The deconfined phase is studied by resorting to a $T$-matrix formulation of statistical mechanics in which the medium under study is seen as a gas of quasigluons and quasigluinos interacting nonperturbatively. Emphasis is put on the temperature range (1-5)~$T_c$, where the interaction are expected to be strong enough to generate bound states. Binary bound states of gluons and gluinos are indeed found to be bound up to 1.4 $T_c$ for any gauge group. The equation of state is then computed numerically for SU($N$) and $G_2$, and discussed in the case of an arbitrary gauge group. It is found to be nearly independent of the gauge group and very close to that of non-supersymmetric Yang-Mills when normalized to the Stefan-Boltzmann pressure and expressed as a function of $T/T_c$.

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