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Switching Distributions for Perpendicular Spin-Torque Devices Within the Macrospin Approximation

机译:Macrospin逼近内垂直自旋扭矩设备的开关分布

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We model “soft” error rates for writing (WSER) and for reading (RSER) for spin-torque memory devices that have a free layer with easy axis perpendicular to the film plane by solving the Fokker-Planck equation for the probability distribution of the angle that the free layer magnetization makes with the normal to the plane of the film. We obtain: 1) an exact, closed form, analytical expression for the zero-temperature switching time as a function of initial angle; 2) an approximate analytical expression for the distribution function of the direction of the magnetization and the exponential decay of the WSER as a function of the time the current is applied; 3) comparison of the approximate analytical expressions for the distribution function and WSER to numerical solutions of the Fokker-Planck equation; 4) an approximate analytical expression for the distribution function and WSER for the case in which the pinned layer is not collinear with the perpendicular free layer; 5) an approximate analytical expression for the linear increase in RSER with current applied for reading; 6) comparison of the approximate analytical formula for the RSER to the numerical solution of the Fokker-Planck equation; and 7) confirmation of the accuracy of the Fokker-Planck solutions by comparison with results of direct simulation using the single-macrospin Landau-Lifshitz-Gilbert equations with a random fluctuating field in the short-time regime for which the latter is practical. We find that the WSER decays at long times as $exp[-2(i-1)tau]$ where the reduced time $tau$ is related to the switching time, Gilbert damping and precession frequency through $tau=alphaomega_{0}t$, and the reduced current $i$ is th- ratio of the applied current to the critical current density for switching $i=overline{I}/I_{0}$ . This exponentially decaying tail in WSER is not easily reduced by tilting the pinned layer magnetization.
机译:我们通过求解Fokker-Planck方程来求解自旋扭矩存储设备的“软”错误写入率(WSER)和读取错误率(RSER),该自旋扭矩存储设备的自由层的易轴垂直于胶片平面。自由层磁化强度与薄膜平面法线所成的角度。我们获得:1)零温度切换时间与初始角度的函数的精确的闭合形式解析表达式; 2)磁化方向分布函数和WSER的指数衰减随电流施加时间的近似解析表达式; 3)将分布函数和WSER的近似解析表达式与Fokker-Planck方程的数值解进行比较; 4)在固定层与垂直自由层不共线的情况下,分布函数和WSER的近似解析表达式; 5)随着电流的增加,RSER线性增加的近似解析表达式; 6)将RSER的近似解析公式与Fokker-Planck方程的数值解进行比较;和7)通过与单随机宏Landau-Lifshitz-Gilbert方程在短时间范围内具有随机波动场的直接仿真结果进行比较,从而确认Fokker-Planck解的准确性。我们发现WSER长时间以$ exp [-2(i-1)tau] $衰减,其中减少的时间$ tau $与切换时间,吉尔伯特阻尼和进动频率相关,通过$ tau = alphaomega_ {0} t $,减小的电流$ i $是施加电流与用于切换$ i = overline {I} / I_ {0} $的临界电流密度的比率。通过倾斜固定层的磁化强度,不容易减少WSER中呈指数衰减的尾部。

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