Dynamic magnetic properties of two-dimensional (2d) classical square heisenberg lattices

J. Curély, J. Kliava
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Abstract

We start this article by recalling the main exact results previously obtained for describing the static magnetic properties of 2d square lattices composed of classical spins isotropically coupled between first-nearest neighbors (i.e., showing Heisenberg couplings) [4c]. Near the critical temperature TC = 0 K we give criterions allowing to directly determine the magnetic phases characterizing 2d magnetic compounds described by our microscopic model. We show that there are three distinct regimes: The Renormalized Classical Regime (RCR), the Quantum Disordered Regime (QDR) and the Quantum Critical Regime (QCR). The static properties give a good image of the spin arrangement and thus remain a good starting point for the study of dynamic properties. As a result, inside each of the three regimes, we may derive the corresponding dynamic behaviors. For practical reasons that we shall detail, we restrict our study to the RCR and QCR cases. An experimental test is given for illustrating this theoretical work. We notably show that it allows one to derive the static correlation length which is an important tool for understanding both static and dynamic properties.
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二维经典方形海森堡晶格的动态磁性能
本文的开头,我们回顾了先前获得的描述由第一近邻之间各向同性耦合的经典自旋组成的二维方形晶格的静态磁性能的主要精确结果(即显示海森堡耦合)[4c]。在临界温度TC = 0 K附近,我们给出了可以直接确定微观模型所描述的二维磁性化合物的磁性相特征的准则。我们证明了有三种不同的状态:重正态经典状态(RCR),量子无序状态(QDR)和量子临界状态(QCR)。静态性质提供了自旋排列的良好图像,因此仍然是研究动态性质的良好起点。因此,在这三种状态中,我们可以推导出相应的动态行为。由于我们将详细说明的实际原因,我们将研究局限于RCR和QCR案例。最后给出了一个实验来说明这一理论工作。我们值得注意的是,它允许人们推导静态相关长度,这是理解静态和动态特性的重要工具。
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