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Anatomy of electrical signals and dc-voltage line shape in spin-torque ferromagnetic resonance

机译:旋转扭矩铁磁谐振中电信号和直流电压线形状的解剖

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摘要

The electrical detection of spin-torque ferromagnetic resonance (st-FMR) is becoming a popular method for measuring the spin-Hall angle of heavy metals (HM). However, various sensible analysis on the same material with either the same or different experimental setups yielded different spin-Hall angles with large discrepancy, indicating some missing ingredients in our current understanding of st-FMR. Here we carry out a careful analysis of electrical signals of the st-FMR in a HM/ferromagnet (HM/FM) bilayer with an arbitrary magnetic anisotropy. The FM magnetization is driven by two radio-frequency (rf) forces: the rf Oersted field generated by an applied rf electric current and the so called rf spin-orbit torque from the spin current flowing perpendicularly from the HM to the FM due to the spin-Hall effect. By using the universal form of the dynamic susceptibility matrix of magnetic materials at the st-FMR, the electrical signals, originated from the anisotropic magnetoresistance, anomalous Hall effect, and inverse spin-Hall effect are analyzed and dc-voltage line shapes near the st-FMR are obtained. Angular dependence of dc voltage is given for two setups. A way of experimentally extracting the spin-Hall angle of a HM is proposed.
机译:旋转扭矩铁磁谐振(ST-FMR)的电检测成为测量重金属旋转厅(HM)的旋转厅角度的流行方法。然而,具有相同或不同实验设置的相同材料的各种明智分析产生了具有大的旋转霍尔角,具有大的差异,表明我们目前对ST-FMR的理解中缺失的成分。在这里,我们仔细分析了HM /铁磁性(HM / FM)双层的ST-FMR的电信号,其具有任意磁各向异性。 FM磁化​​由两个射频(RF)力驱动:由所施加的RF电流产生的RF型磁场和所谓的RF自旋轨道扭矩从旋转电流从HM垂直于FM流过到FM的旋转电流旋转霍尔效果。通过在ST-FMR处使用动态敏感性矩阵的通用形式,分析了来自各向异性磁阻,异常霍尔效应和逆旋转厅效应的电信号,并在ST附近的直流电压线形状-FMR获得。对于两个设置,给出了直流电压的角度依赖性。提出了一种实验提取HM的旋转厅角的方法。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2019年第6期|064424.1-064424.11|共11页
  • 作者单位

    Hong Kong Univ Sci & Technol Phys Dept Kowloon Clear Water Bay Hong Kong Peoples R China|HKUST Shenzhen Res Inst Shenzhen 518057 Peoples R China;

    Nanjing Univ Natl Lab Solid State Microstruct 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China|Nanjing Univ Dept Phys 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China;

    Nanjing Univ Natl Lab Solid State Microstruct 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China|Nanjing Univ Dept Phys 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China|Nanjing Univ Collaborat Innovat Ctr Adv Microstruct 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China;

    Nanjing Univ Natl Lab Solid State Microstruct 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China|Nanjing Univ Dept Phys 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China|Nanjing Univ Collaborat Innovat Ctr Adv Microstruct 22 Hankou Rd Nanjing 210093 Jiangsu Peoples R China;

    Hong Kong Univ Sci & Technol Phys Dept Kowloon Clear Water Bay Hong Kong Peoples R China|HKUST Shenzhen Res Inst Shenzhen 518057 Peoples R China;

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