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Spin-torque driven magnetization dynamics in a nanocontact setup for low external fields: Numerical simulation study

机译:用于低外部磁场的纳米接触装置中自旋扭矩驱动的磁化动力学:数值模拟研究

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We present numerical simulation studies of the slcady-state magnetization dynamics driven by a spin-polarized current in a point-contact geometry for the case of a relatively large contact diameter (D_c=80 nm) and small external field (H=30 Oe). We show that under these conditions the magnetization dynamics is qualitatively different from the dynamics observed for small contacts in large external fields. In particular, the "bullet" mode with a relatively homogeneous mode core, which was the dominating localized mode for small contacts, is not found here. Instead, all localized oscillation modes observed in simulations correspond to different motion kinds of vortex-antivortex (V-AV) pairs. These modes include rotation of pairs with the V-AV distance d~D_c and creation/annihilation of much smaller (satellite) V-AV pairs. We also show that for our geometry the Oersted field has a qualitative effect on the magnetization dynamics of a free layer. This effect offers (in principle) a possibility to control magnetization dynamics by a suitable electric contact setup, adjusted to produce a desired Oersted field. Finally, we demonstrate that when the magnetization dynamics of the "fixed" layer-induced by the magnetodipolar interaction with the "free" layer-is taken into account, the threshold current for the oscillation onset is drastically reduced and new types of localized modes appear. In conclusion, we show that our simulations reproduce semiquantitatively several important features of the magnetization dynamics in a point-contact system for low external fields reported experimentally.
机译:对于接触直径较大(D_c = 80 nm)和外部磁场较小(H = 30 Oe)的情况,我们对点接触几何形状中的自旋极化电流驱动的滑态磁化动力学进行了数值模拟研究。我们表明,在这些条件下,磁化动力学在质量上不同于在大外部磁场中观察到的小接触的动力学。特别是,这里没有找到具有相对均质模式核心的“子弹”模式,该模式是小触点的主要局部模式。取而代之的是,在仿真中观察到的所有局部振荡模式都对应于涡-反涡(V-AV)对的不同运动类型。这些模式包括旋转V-AV距离为d〜D_c的对,以及创建/歼灭更小的(卫星)V-AV对。我们还表明,对于我们的几何形状,奥斯特场对自由层的磁化动力学具有定性影响。这种效果(原则上)提供了通过适当的电触点设置来控制磁化动力学的可能性,调整该设置以产生所需的奥斯特场。最后,我们证明,当考虑到由与“自由”层的磁偶极相互作用引起的“固定”层的磁化动力学时,振荡开始的阈值电流将大大降低,并且出现了新型的局部模式。总之,我们表明,我们的模拟半定量地再现了针对点接触系统中低外部磁场的磁化动力学的几个重要特征,这些特征是通过实验报道的。

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