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Thermodynamics of the Classical Planar Ferromagnet Close to the Zero-Temperature Critical Point: A Many-Body Approach

机译:接近零温度临界点的经典平面铁磁体的热力学:多体方法

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We explore the low-temperature thermodynamic properties and crossovers of ad-dimensional classical planar Heisenberg ferromagnet in a longitudinal magnetic field close to its field-induced zero-temperature critical point by employing the two-time Green’s function formalism in classical statistical mechanics. By means of a classical Callen-like method for the magnetization and the Tyablikov-like decoupling procedure, we obtain, for anyd, a low-temperature critical scenario which is quite similar to the one found for the quantum counterpart. Remarkably, ford>2the discrimination between the two cases is found to be related to the different values of the shift exponent which governs the behavior of the critical line in the vicinity of the zero-temperature critical point. The observation of different values of the shift-exponent and of the related critical exponents along thermodynamic paths within the typical V-shaped region in the phase diagram may be interpreted as a signature of emerging quantum critical fluctuations.
机译:通过在经典统计力学中采用两次格林函数形式,我们探索了在接近其场感应零温临界点的纵向磁场中,一维经典平面海森堡铁磁体的低温热力学性质和交叉现象。借助于经典的类似于Callen的磁化方法和类似Tyablikov的解耦程序,我们可以得到一种低温临界情况,该情况与量子对应物非常相似。值得注意的是,福特> 2,发现两种情况之间的区别与控制零温度临界点附近的临界线行为的位移指数的不同值有关。在相图中典型的V形区域内沿着热力学路径观察到的位移指数和相关的临界指数的不同值可以解释为新出现的量子临界涨落的标志。

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