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首页> 外文期刊>Physical review, B >Instability analysis of spin-torque oscillator with an in-plane magnetized free layer and a perpendicularly magnetized pinned layer
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Instability analysis of spin-torque oscillator with an in-plane magnetized free layer and a perpendicularly magnetized pinned layer

机译:具有面内磁化自由层和垂直磁化固定层的自旋扭矩振荡器的不稳定性分析

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摘要

We study the theoretical conditions to excite a stable self-oscillation in a spin-torque oscillator with an in-plane magnetized free layer and a perpendicularly magnetized pinned layer in the presence of magnetic field pointing in an arbitrary direction. The linearized Landau-Lifshitz-Gilbert (LLG) equation is found to be inapplicable to evaluate the threshold between the stable and self-oscillation states because the critical current density estimated from the linearized equation is considerably larger than that found in the numerical simulation. We derive a theoretical formula of the threshold current density by focusing on the energy gain of the magnetization from the spin torque during a time shorter than a precession period. A good agreement between the derived formula and the numerical simulation is obtained. The condition to stabilize the out-of-plane self-oscillation above the threshold is also discussed.
机译:我们研究了在自旋扭矩振荡器中激发平面内磁化自由层和垂直磁化固定层的自激转矩的理论条件,该磁场存在指向任意方向的磁场。发现线性化的Landau-Lifshitz-Gilbert(LLG)方程不适用于评估稳态和自激振荡状态之间的阈值,因为从线性化方程估算的临界电流密度大大大于数值模拟中的临界电流密度。通过关注自旋转矩在比进动周期短的时间内磁化的能量增益,我们得出了阈值电流密度的理论公式。在推导的公式和数值模拟之间获得了良好的一致性。还讨论了将平面外自激稳定在阈值以上的条件。

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