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arXiv 2109.03476cond-mat.mes-hall

非平衡磁纳米结中自旋弛豫的动力学

Dynamics of spin relaxation in nonequilibrium magnetic nanojunctions

Rudolf Smorka, Michael Thoss, Martin Žonda

AI总结:

本文结合经典自旋动力学与层级运动方程方法研究非平衡磁纳米结,发现自旋弛豫率随耦合强度呈非单调变化并在中等耦合处出现最大值,同时证明短链耦合半无限导线可精确模拟大型开放系统,并揭示了直流偏压下自旋弛豫的共振特征及其展宽机制。

摘要:

我们采用一种将经典自旋动力学与用于传导电子量子动力学的层级运动方程技术相结合的数值方法,研究磁纳米结中的非平衡现象。我们的关注点在于自旋动力学,其中我们观察到自旋弛豫率作为局域自旋与传导电子之间耦合强度的函数表现出非单调行为。值得注意的是,我们在中等耦合强度处识别出一个明显的最大值,我们将其归因于一种竞争,这种竞争涉及经典自旋与电子之间耦合影响的增强,以及费米能级处局域态密度减小的影响。此外,我们证明了一个大型开放系统的自旋动力学可以通过耦合到半无限金属导线的短链来精确模拟。在受到外部直流电压作用的磁结情形中,我们观察到自旋弛豫中的共振特征,反映了系统的电子能谱。经典自旋的进动在电子能谱中产生了额外的边带能量,这反过来导致了电压中增强阻尼范围的展宽。

英文摘要:

We investigate nonequilibrium phenomena in magnetic nano-junctions using a numerical approach that combines classical spin dynamics with the hierarchical equations of motion technique for quantum dynamics of conduction electrons. Our focus lies on the spin dynamics, where we observe non-monotonic behavior in the spin relaxation rates as a function of the coupling strength between the localized spin and conduction electrons. Notably, we identify a distinct maximum at intermediate coupling strength, which we attribute to a competition that involves the increasing influence of the coupling between the classical spin and electrons, as well as the influence of decreasing local density of states at the Fermi level. Furthermore, we demonstrate that the spin dynamics of a large open system can be accurately simulated by a short chain coupled to semi-infinite metallic leads. In the case of a magnetic junction subjected to an external DC voltage, we observe resonant features in the spin relaxation, reflecting the electronic spectrum of the system. The precession of classical spin gives rise to additional side energies in the electronic spectrum, which in turn leads to a broadened range of enhanced damping in the voltage.

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