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Spin configurations in hard/soft coupled bilayer systems: Transitions from rigid magnet to exchange-spring

机译:硬/软耦合双层系统中的自旋配置:从刚性磁体到交换弹簧的过渡

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摘要

We investigate equilibrium properties of an exchange-spring magnetic system constituted of a soft layer (e.g., Fe) of a given thickness on top of a hard magnetic layer (e.g., FePt). The magnetization profile M(z) as a function of the atomic position ranging from the bottom of the hard layer to the top of the soft layer is obtained in two cases with regard to the hard layer: (i) in the case of a rigid interface (the FePt layer is a single layer), the profile is obtained analytically as the exact solution of a sine-Gordon equation with Cauchy's boundary conditions. Additional numerical simulations also confirm this result. Asymptotic expressions of M(z) show a linear behavior near the bottom and the top of the soft layer. In addition, a critical value of the number of atomic planes in the soft layer, that is necessary for the onset of spin deviations, is obtained in terms of the anisotropy and exchange coupling between the adjacent plane in the soft layer, (ii) In the case of a relaxed interface (the FePt layer is a multilayer), the magnetization profile is obtained numerically for various Fe and FePt films thicknesses and applied field.
机译:我们研究了交换弹簧磁系统的平衡特性,该交换弹簧磁系统由在硬磁层(例如FePt)上具有给定厚度的软层(例如Fe)构成。在两种情况下,对于硬质层,可以获得从硬质层的底部到软质层的顶部的原子位置的函数的磁化曲线M(z):(i)刚性时界面(FePt层是单层),则通过解析得到作为具有Cauchy边界条件的正弦Gordon方程的精确解的轮廓。其他数值模拟也证实了这一结果。 M(z)的渐近表达式在软层的底部和顶部附近显示线性行为。另外,根据各向异性和软层中相邻平面之间的交换耦合,获得了自旋偏差开始所必需的,软层中原子平面数目的临界值,(ii)在界面松弛的情况下(FePt层是多层的),对于不同的Fe和FePt膜厚度和施加的磁场,可以通过数值获得磁化曲线。

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