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On the finite-temperature generalization of the C-theorem and the interplay between classical and quantum fluctuations

机译:C定理的有限温度推广以及经典与量子涨落之间的相互作用

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The behaviour of the finite-temperature C-function, defined by Neto and Fradkin (1993 Nucl. Phys. B 400 525), is analysed within a d-dimensional exactly solvable lattice model, recently considered by Vojta (1996 Phys. Rev. B 53 710), which is of the same universality class as the quantum nonlinear O(n) sigma model in the limit n -> infinity. The scaling functions of C for the cases d = 1 (absence of long-range order), d = 2 (existence of a quantum critical point), d = 4 (existence of a line of finite-temperature critical points that ends up with a quantum critical point) are derived and analysed. The locations of regions where C is monotonically increasing (which) depend significantly of d) are exactly determined. The results are interpreted within the finite-size scaling theory that has to be modified for d = 4.
机译:由Neto和Fradkin(1993 Nucl。Phys。B 400 525)定义的有限温度C函数的行为在最近由Vojta(1996 Phys。Rev. B)考虑的d维精确可解晶格模型中进行了分析。 53 710),它与极限n->无穷大中的量子非线性O(n)sigma模型具有相同的通用性。 d = 1(不存在长距离阶数),d = 2(存在量子临界点),d = 4(存在以结束的有限温度临界点线的情况)下C的缩放函数量子临界点)并进行分析。精确确定C单调增加(显着取决于d)的区域的位置。结果在有限尺寸缩放理论中解释,必须对d = 4进行修改。

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