不同厚度垂直铁磁纳米点的热激活磁开关模式

N. A. Wibowo, Cahya Handoyo, L. R. Sasongko
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引用次数: 4

摘要

即使已经成功地应用热脉冲通过随机化磁化来降低矫顽力,以这种方式刺激磁反转,但在书写过程中磁开关场消耗的效率仍然是实现HAMR技术的一个令人兴奋的研究领域。HAMR存储介质的一个显著的几何特性是纳米点的厚度,这可能与写入场缩小问题有关。此外,热波动导致磁化转换过程具有概率性。这种磁开关概率决定了写入场的大小。本文旨在用数值方法研究介质厚度变化对磁化过程的影响,特别是在高温下。将纳米点建模为具有单轴各向异性的平行六面体,将其视为不存在相邻纳米点扰动场的磁隔离系统。采用仿真方法对当前热辅助磁记录中的矫顽力和写入场消耗两种观点进行了评价。矫顽力是通过在热平衡状态下向周围诱导一个线性增加到2特斯拉的2.5 ns的磁场来测量的。在计算写入场消耗时,磁场诱导纳米点时产生略低于居里温度的热场脉冲。这些方案的研究基于Landau-Lifshift-Gilbert方程,该方程在计算热波动效应时符合涨落-耗散定理。此外,还考虑了与温度相关的材料参数,如磁饱和度、磁各向异性和交换相互作用。在室温下,矫顽力场和成核场对纳米点厚度高度敏感。在热辅助下,所选厚度在10 nm和100 nm处的写入场分别为0.110T和0.125 T。这些写作成绩明显低于媒体的强制性。对于两种厚度,都观察到零场磁化反转现象,这是由H = 0时开关概率的存在所表明的。数值研究表明,在居里点附近的加热辅助下,即使在没有驱动磁场的情况下,具有选定厚度和磁性参数的纳米点也可能被磁化。伴随着这个结果,需要完全磁化的磁场感应仅在亚特斯拉-大约是矫顽力场的十分之一。在热辅助磁化过程中,磁矩的随机化在畴壁成核并传播到单个磁化畴之前启动了开关动态。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermally Activated Magnetic Switching Mode for Various Thicknesses of Perpendicularly Ferromagnetic Nano-dot
Even applying thermal pulse has been succeeded to reduce the coercivity through randomization the magnetization in such a way stimulate the magnetic reversion, the efficiency of magnetic switching field consumption in writing process still turns out to be an exciting research field to implement the HAMR technology. One of the remarkable geometric properties of HAMR storage media that can be correlated to the writing field reduction issue is the nano-dot thickness. Furthermore, thermal fluctuation causes the magnetization switching process to be probabilistic. This magnetic switching probability determines the magnitude of the writing field. This paper aims to investigate the impact of changes in media thickness on the magnetization process in particular at high temperatures numerically. Nano-dot was modeled as a parallelepiped with uniaxial anisotropy which was regarded as a magnetically isolated system where no disturbance field of neighboring nano-dots. Simulation arrangements were implemented to evaluate the two viewpoints in the current heat-assisted magnetic recording, either coercivity, as well as writing field consume. Coercivity was gauged by inducing a magnetic field which linearly increased up to 2 Tesla for 2.5 ns at thermal equilibrium to the surrounding. In evaluating writing field consume, thermal field pulse which just below the Curie temperature was generated while the magnetic field inducing the nano-dot. These schemes investigations were based on the Landau-Lifshift- Gilbert equation which accommodates the fluctuation-dissipation theorem in calculating thermal fluctuation effect. Also, temperature dependent material parameters such as magnetic saturation, magnetic anisotropy, and exchange interaction, were taken into account. At room temperature, the coercive and nucleation fields are highly sensitive to the nano-dot thickness. Under thermal assistance, the writing field for 10 nm and 100 nm of the chosen thicknesses are 0.110 T and 0.125 T respectively. These writing grades are significantly lower than the coercivity of the media. For both thicknesses, zero field magnetization reversal phenomena are observed as indicated by the existences of the switching probabilities at H = 0. This numerical study showed that using the heating assistance close to the Curie point, nanodots with the chosen thicknesses and magnetic parameters were probably to be magnetized even no driven magnetic field. Along with this result, magnetic field induction which required to utterly magnetizing was only in the sub-Tesla - about a tenth of the coercive field. During magnetization processes under thermal assistance, randomization of magnetic moments initiated the switching dynamic before the domain wall was nucleated and propagated to reach a single magnetized domain.
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