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The Gross-Neveu model at finite temperature at next-to-leading order in the 1/N expansion

机译:在有限温度下,以1 / N扩展的次于领先顺序的Gross-Neveu模型

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We present new results on the Gross-Neveu model at finite temperature and at next-to-leading order in the 1/N expansion. In particular, a new expression is obtained for the effective potential which is explicitly invariant under renormalization group transformations. The model is used as a playground to investigate various features of field theory at finite temperature. For example we verify that, as expected from general arguments, the cancellation of ultraviolet divergences takes place at finite temperature without the need for introducing counterterms beyond those of zero temperature. As well known, the discrete chiral symmetry of the (1+1)-dimensional model is spontaneously broken at zero temperature and restored, in leading order, at some temperature T-c; we find that the 1/N approximation breaks down for temperatures below T-c: as the temperature increases, the fluctuations become eventually too large to be treated as corrections, and a Landau pole invalidates the calculation of the effective potential in the vicinity of its minimum. Beyond T-c, the 1/N expansion becomes again regular: it predicts that in leading order the system behaves as a free gas of massless fermions and that, at the next-to-leading order, it remains weakly interacting. In the limit of large temperature, the pressure coincides with that given by perturbation theory with a coupling constant defined at a scale of the order of the temperature, as expected from asymptotic freedom. (C) 2003 Elsevier Science (USA). All rights reserved. [References: 46]
机译:我们在有限温度下以1 / N扩展的次要顺序在Gross-Neveu模型上给出新结果。特别地,获得针对有效电位的新表达式,该有效表达式在重归一化组变换下明显不变。该模型用作研究有限温度场论各种特征的场所。例如,我们验证了,正如从一般论证中所期望的那样,消除了紫外线发散是在有限的温度下发生的,而不需要引入超过零温度的对立项。众所周知,(1 + 1)维模型的离散手性对称性在零温度下自发破坏,并在一定温度T-c下按先导顺序恢复;我们发现,对于低于T-c的温度,1 / N近似值会分解:随着温度的升高,波动最终变得太大而无法作为校正,并且Landau极点使有效电势在其最小值附近的计算无效。在T-c之外,1 / N的膨胀又变得规则:它预测系统处于主导地位,表现为无质量费米子的自由气体,并且在接近主导地位的地位,其相互作用仍然微弱。在大温度范围内,压力与微扰理论所给出的压力一致,偶合常数定义为温度量级,如渐近自由所预期的那样。 (C)2003 Elsevier Science(美国)。版权所有。 [参考:46]

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