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Correlation between the bias dependence of tunneling anisotropic magnetoresistance and tunneling magnetoresistance in a La_(0.67)Sr_(0.33)MnO_3-based magnetic tunnel junction

机译:基于La_(0.67)Sr_(0.33)MnO_3的磁性隧道结中隧道各向异性磁阻的偏置依赖性与隧道磁阻的相关性

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La_(0.67)Sr_(0.33)MnO_3 (LSMO) is one of the most promising oxide materials for spintronic devices due to its high Curie temperature (T_c〜370 K), colossal magnetoresistance , and its half-metallicity . The band structure of LSMO around the Fermi level E_F, specifically that at the LSMO / SrTiO_3 (STO) tunnel barrier interface, is known to be a complex mixture of the different J-band components, the up-spin eg and t_(2g) states. The t_(2g) states are located at 〜0.5 eV below E_F in the bulk, but are pushed up closer to E_F at the interface . Hence in LSMO, when the carrier energy is tuned between the interfacial e_gand t_(2g) bands, a sharp change of the angular dependence of the density of states (DOS) on the magnetization direction is expected, like in the quantum wells of ferromagnetic semiconductor GaMnAs [4].
机译:La_(0.67)Sr_(0.33)MnO_3(LSMO)由于其居里温度(T_c〜370 K)高,巨大的磁阻和半金属性而成为自旋电子器件中最有希望的氧化物材料之一。已知在费米能级E_F附近的LSMO的能带结构,特别是在LSMO / SrTiO_3(STO)隧道势垒界面处的能带结构,是由不同的J波段分量,例如上旋和t_(2g)组成的复杂混合物。状态。 t_(2g)状态在批量中位于E_F以下〜0.5 eV,但在接口处被向上推至更靠近E_F的位置。因此,在LSMO中,当在界面e_gand t_(2g)谱带之间调整载流子能量时,像铁磁半导体的量子阱一样,可以预期态密度(DOS)对磁化方向的角度依赖性的急剧变化。 GaMnAs [4]。

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    Department of Electrical Engineering and Information Systems The University of Tokyo Institute of Engineering Innovation The University of Tokyo;

    Department of Electrical Engineering and Information Systems The University of Tokyo;

    Department of Electrical Engineering and Information Systems The University of Tokyo Center for Spintronics Research Network (CSRN) The University of Tokyo;

    Department of Electrical Engineering and Information Systems The University of Tokyo Institute of Engineering Innovation The University of Tokyo Center for Spintronics Research Network (CSRN) The University of Tokyo;

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