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Spin-Current Control by Induced Electric-Polarization Reversal in Ni/hBN/Ni Magnetic Tunnel Junction: A Cross-Correlation Materials

机译:Ni / hBN / Ni磁性隧道结中通过感应电极化反转的自旋电流控制:互相关材料

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In a typical magnetic tunnel junction (MTJ), resistance is controlled by the magnetic alignment of upper and lower ferromagnetic materials. Anti-parallel (parallel) configuration of upper and lower ferromagnetic materials gives high (low) resistance. Here, we propose additional degree of freedom on MTJ. Within anti-parallel configuration (APC), spin-filtering effect occurs depending on the polarization of the insulator layer. We considered an ab-initio study of MTJ consisting of hexagonal boron nitride (hBN) sandwiched between Ni(111) layers. A maximum of two pd-hybridization bonds stabilized the structure, with APC proving to be the most favorable magnetic alignment, in line with the results of previous experimental studies [1]. Within two pd-hybridizations structure, there are asymmetric and symmetric stacking arrangement with total energy difference ≈ 33 meV where the former has lower energy. In the case of symmetric stacking arrangement, our transmission probability result shows a typical functionality of magnetic tunnel junction. Meanwhile, in the asymmetric stacking arrangement, a structural deformation from a flat hBN plane to a rugged hBN plane occurs. The buckling direction is two-fold and can be tuned by applying an external electric field. When the buckling direction is switched, the induced dipole moment in the hBN layer is also switched to have a reversed dipole. On the other hand, an induced magnetic moment at an N site appears when the structural deformation leading N to move closer to one of the Ni atoms. Interestingly, the magnetic moment direction is switched by the position of the N layer in the resulting bi-stable state with electrical polarization when APC is chosen. The transmission probability calculation of asymmetric stacking arrangement exhibits a spin-filtering effect where the spin-polarized current is controlled by the electric field when a field-induced reversal of the polarization is realized.
机译:在典型的磁性隧道结(MTJ)中,电阻是通过上下铁磁材料的磁对准来控制的。上下铁磁材料的反平行(平行)配置可提供高(低)电阻。在这里,我们建议在MTJ上增加自由度。在反平行配置(APC)中,根据绝缘层的极化情况发生自旋滤波效应。我们考虑了由六方氮化硼(hBN)夹在Ni(111)层之间组成的MTJ的从头开始研究。与以前的实验研究结果一致,最多两个pd杂化键稳定了结构,其中APC被证明是最有利的磁取向。在两个pd杂化结构中,存在不对称和对称的堆叠结构,总能量差≈33 meV,其中前者的能量较低。在对称堆叠的情况下,我们的传输概率结果显示了磁性隧道结的典型功能。同时,在非对称堆叠布置中,发生从平坦的hBN平面到崎的hBN平面的结构变形。屈曲方向是双重的,可以通过施加外部电场来调整。当屈曲方向被切换时,hBN层中的感应偶极矩也被切换为具有反向偶极子。另一方面,当结构变形导致N移近一个Ni原子时,会在N位置出现感应磁矩。有趣的是,磁矩方向由N层的位置中所得到的双稳定状态的电偏振选择APC时切换。非对称堆叠结构的传输概率计算表现出自旋滤波效果,其中当实现电场感应的极化反转时,自旋极化电流由电场控制。

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