Tóbik Jaroslav, Cambel Vladimir, Karapetrov Goran
Institute of Electrical Engineering, Slovak Academy of Sciences, Dúbravská cesta 9, SK-841 04 Bratislava, Slovakia.
Department of Physics, Drexel University, 3141 Chestnut Street, Philadelphia, Pennsylvania 19104, USA.
Sci Rep. 2015 Jul 22;5:12301. doi: 10.1038/srep12301.
Strong interest in nanomagnetism stems from the promise of high storage densities of information through control of ever smaller and smaller ensembles of spins. There is a broad consensus that the Landau-Lifshitz-Gilbert equation reliably describes the magnetization dynamics on classical phenomenological level. On the other hand, it is not so evident that the magnetization dynamics governed by this equation contains built-in asymmetry in the case of broad topology sets of symmetric total energy functional surfaces. The magnetization dynamics in such cases shows preference for one particular state from many energetically equivalent available minima. We demonstrate this behavior on a simple one-spin model which can be treated analytically. Depending on the ferromagnet geometry and material parameters, this asymmetric behavior can be robust enough to survive even at high temperatures opening simplified venues for controlling magnetic states of nanodevices in practical applications. Using micromagnetic simulations we demonstrate the asymmetry in magnetization dynamics in a real system with reduced symmetry such as Pacman-like nanodot. Exploiting the built-in asymmetry in the dynamics could lead to practical methods of preparing desired spin configurations on nanoscale.
对纳米磁性的浓厚兴趣源于通过控制越来越小的自旋系综来实现高信息存储密度的前景。人们普遍认为,朗道 - 里夫希茨 - 吉尔伯特方程在经典唯象学层面上可靠地描述了磁化动力学。另一方面,在对称总能量泛函曲面的广泛拓扑集情况下,由该方程支配的磁化动力学是否包含内在不对称性并不那么明显。在这种情况下,磁化动力学从许多能量上等效的可用极小值中表现出对一种特定状态的偏好。我们在一个可以进行解析处理的简单单自旋模型上展示了这种行为。根据铁磁体的几何形状和材料参数,这种不对称行为甚至在高温下也可能足够稳健,从而为实际应用中控制纳米器件的磁态开辟了简化途径。通过微磁模拟,我们展示了在具有降低对称性的实际系统(如吃豆人状纳米点)中磁化动力学的不对称性。利用动力学中的内在不对称性可能会导致在纳米尺度上制备所需自旋构型的实用方法。