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Stabilization of the easy-cone magnetic state in free layers of magnetic tunnel junctions

机译:易锥磁能在磁隧道结的自由层中稳定

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The influence of temperature, FeCoB layer thickness, and insertion of ultrathin metal spacers (Ta and W) on the magnetic anisotropy of MgO/FeCoB/MgO free layers has been explored by means of ferromagnetic resonance. The second-order contribution to the perpendicular magnetic anisotropy (PMA), stemming from the fluctuations of the first-order term, accounts for the onset of an easy-cone magnetic state in the course of the transition from the in-plane to out-of-plane magnetization. Since the second-order term is small, the easy-cone state is stable only within a narrow range of free-layer thicknesses and temperatures, where the interfacial first-order PMA term gets counterbalanced by the magnetostatic term. We have found that the insertion of metallic spacers in the middle of the FeCoB layer noticeably widens the range of thicknesses and temperatures for obtaining the easy-cone state. We show that the W spacer outperforms its Ta counterpart in this enhancement, albeit increasing the magnetization damping due to a higher degree of alloying with FeCoB. A physical mechanism of the easy-cone stabilization is proposed. It considers a variation of the local saturation magnetization (M-S) and, notably, Curie temperature (T-C) near the MgO/FeCoB interface versus the distance to the metal spacer (or the capping) layer. The larger M-S and T-C values near MgO provide more thermal stability to the first-order PMA (k(s1)), while the lower M-S and T-C ones near the spacer layer result in a faster drop of the magnetostatic term with temperature. As a result, the effective PMA field exhibits a thermal stabilization effect that can be exploited to stabilize the easy-cone anisotropy. Alongside the improved conditions for setting an easy cone in the MgO/FeCoB/MgO free layers, we demonstrate that an easy-cone configuration with an almost temperature-independent opening angle can be obtained using a MgO/FeCoB(1.6 nm)/Ta free layer.
机译:通过铁磁共振探索了温度,Fecob层厚度和超薄金属间隔物(Ta和W)对MgO / Fecob / MgO自由层的磁各向异性的影响。对垂直磁各向异性(PMA)的二阶贡献,源于一阶项的波动,考虑到从面内到外的过渡过程中易锥磁状态的开始。平面磁化。由于二阶项很小,但易锥形状态仅在窄范围内稳定的自由层厚度和温度,其中界面一阶PMA术语通过磁稳定术语进行平衡。我们已经发现,在FECOB层的中间插入金属间隔物明显加宽为获得易锥状态的厚度和温度范围。我们表明,W间隔物在这种增强中优于其TA对应物,尽管由于具有较高的Fecob,因此由于较高程度的合金化而增加磁化阻尼。提出了一种易锥稳定的物理机制。它考虑了局部饱和磁化强度(M-S)的变化,特别是MgO / FECOB界面附近的居里温度(T-C)与与金属间隔物(或封端)层的距离相比。 MgO附近的较大的M-S和T-C值为一阶PMA提供了更多的热稳定性(K(S1)),而间隔层附近的下部M-S和T-C导致静磁术近的磁延时,温度较快。结果,有效的PMA场表现出热稳定效果,其可以被利用以稳定易锥形各向异性。除了在MgO / Fecob / MgO自由层中设置容易锥体的改进条件,我们证明可以使用MgO / Fecob(1.6nm)/ Ta自由地获得具有几乎温度无关的开口角度的易锥形配置层。

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