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Magnetization dynamics: path-integral formalism for the stochastic Landau-Lifshitz-Gilbert equation

机译:磁化动力学:随机的路径积分形式   Landau-Lifshitz-Gilbert方程

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摘要

We construct a path-integral representation of the generating functional forthe dissipative dynamics of a classical magnetic moment as described by thestochastic generalization of the Landau-Lifshitz-Gilbert equation proposed byBrown, with the possible addition of spin-torque terms. In the process ofconstructing this functional in the Cartesian coordinate system, we criticallyrevisit this stochastic equation. We present it in a form that accommodates forany discretization scheme thanks to the inclusion of a drift term. Thegeneralized equation ensures the conservation of the magnetization modulus andthe approach to the Gibbs-Boltzmann equilibrium in the absence of non-potentialand time-dependent forces. The drift term vanishes only if the mid-pointStratonovich prescription is used. We next reset the problem in the morenatural spherical coordinate system. We show that the noise transformsnon-trivially to spherical coordinates acquiring a non-vanishing mean value inthis coordinate system, a fact that has been often overlooked in theliterature. We next construct the generating functional formalism in thissystem of coordinates for any discretization prescription. The functionalformalism in Cartesian or spherical coordinates should serve as a startingpoint to study different aspects of the out-of-equilibrium dynamics of magnets.Extensions to colored noise, micro-magnetism and disordered problems arestraightforward.
机译:如布朗提出的Landau-Lifshitz-Gilbert方程的随机概括,并可能加上自旋转矩项,我们构造了经典磁矩的耗散动力学的生成函数的路径积分表示。在笛卡尔坐标系中构造该函数的过程中,我们严格地重新研究了该随机方程。由于包含了漂移项,我们以适合任何离散化方案的形式展示了它。广义方程确保了在没有非势和时变力的情况下磁化模量的守恒和吉布斯-玻尔兹曼平衡的逼近。仅当使用中点Stratonovich处方时,漂移项才消失。接下来,我们在更自然的球坐标系中重设该问题。我们表明,在该坐标系中,噪声非平凡地转换为球面坐标,获得了不消失的平均值,这一事实在文献中经常被忽略。接下来,我们在任何离散化处方的坐标系统中构造生成函数的形式主义。笛卡尔坐标系或球面坐标系中的功能形式主义应该作为研究磁体失衡动力学的各个方面的起点。对彩色噪声,微磁性和无序问题的扩展是直接的。

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