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arXiv 2407.02469cond-mat.mes-hall
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具有Gilbert阻尼的磁性系统中热激活的稳健理论

A robust theory of thermal activation in magnetic systems with Gilbert damping

Hugo Bocquet, Peter M. Derlet

AI总结:

受Langer谐振理论启发,推导了多维自旋系统作为Gilbert阻尼参数$α$函数的一般激活速率,发现其在$α\ll1$范围内有效,并揭示了有限反铁磁自旋链中Meyer-Neldel规则的失效。

摘要:

磁性系统可以表现出热激活跃迁,其时间尺度通常由Arrhenius定律描述。然而,对此类时间尺度的稳健预测仅适用于某些情况。受Langer的谐振理论启发,我们推导了多维自旋系统的一般激活速率。假设在初始极小值处存在局部热平衡,并推导出在鞍点处沿真实不稳定动力学模式的概率密度流表达式,我们获得了作为Gilbert阻尼参数$α$函数的激活速率表达式。我们发现该表达式在$α\ll1$的物理相关范围内仍然有效。当激活以所有自旋的相干重定向为特征时,我们通过用自旋波频率表示Arrhenius定律的前因子获得了深入理解,并且对于有限反铁磁自旋链的情况,获得了一个依赖于系统尺寸平方的指数表达式,表明Meyer-Neldel规则的失效。

英文摘要:

Magnetic systems can exhibit thermally activated transitions whose timescales are often described by an Arrhenius law. However, robust predictions of such timescales are only available for certain cases. Inspired by the harmonic theory of Langer, we derive a general activation rate for multi-dimensional spin systems. Assuming local thermal equilibrium in the initial minimum and deriving an expression for the flow of probability density along the real unstable dynamical mode at the saddle point, we obtain the expression for the activation rate that is a function of the Gilbert damping parameter, $α$. We find that this expression remains valid for the physically relevant regime of $α\ll1$. When the activation is characterized by a coherent reorientation of all spins, we gain insight into the prefactor of the Arrhenius law by writing it in terms of spin wave frequencies and, for the case of a finite antiferromagnetic spin chain, obtain an expression that depends exponentially on the square of the system size indicating a break-down of the Meyer-Neldel rule.

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