垂直极化纳米柱中的非相干自旋波激发

W. Jin, Y. Liu
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引用次数: 0

摘要

自旋转移机制是MRAM、可编程逻辑、微波振荡器等领域广泛研究的课题。对磁柱的微磁模拟表明,在没有磁场的情况下,可以激发出几到几十GHz的自旋波,在一定电流下,频率随自由层厚度的增加而减小,在一定厚度下,频率随电流密度的增加而增加。太大的电流激发混沌的自旋波。偏振片高度大于其宽度和长度,由于其形状各向异性,其磁化强度沿z方向固定。采用包含Slonzewski自旋传递转矩项的Landau-Lifshitz方程模拟了自由层的磁化激励。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Incoherent Spin-Wave Excitations in Nanopillars with Perpendicular Polarizers
Spin-transfer mechanism is the subject of extensive research for applications in MRAM, programmable logic, and microwave oscillators. Micromagnetic simulations on magnetic pillars in this work show that several to tens of GHz spin waves can be excited without magnetic fields, the frequency decreases with the free layer thickness increasing at a given current and increases with the current density increasing at a fixed thickness. Too large current excites chaotic spin-waves. The polarizer height is larger than its width and length so that its magnetization is fixed along the z direction due to shape anisotropy. The Landau-Lifshitz equation including the Slonzewski's spin-transfer torque term is employed to simulate the magnetization excitations of the free layer.
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