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Charge pumping by magnetization dynamics in magnetic and semi-magnetic tunnel junctions with interfacial Rashba or bulk extrinsic spin-orbit couplings

机译:通过磁和半磁中的磁化动力学进行电荷泵浦   与界面Rashba或大量外在自旋轨道的隧道连接   联轴器

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摘要

We develop a time-dependent nonequilibrium Green function (NEGF) approach tothe problem of spin pumping by precessing magnetization in one of theferromagnetic layers within F/I/F magnetic tunnel junctions (MTJs) or F/I/Nsemi-MTJs in the presence of intrinsic Rashba spin-orbit coupling (SOC) at theF/I interface or the extrinsic SOC in the bulk of F layers of finite thickness(F-ferromagnet; N-normal metal; I-insulating barrier). To express thetime-averaged pumped charge current, or the corresponding dc voltage signal inopen circuits that was measured in recent experiments on semi-MTJs [T. Moriyamaet al., Phys. Rev. Lett. 100, 067602 (2008)], we construct a novel solution forthe double-time-Fourier-transformed NEGFs. The two energy arguments of NEGFs inthis representation are connected by the Floquet theorem describing multiphotonemission and absorption processes. Within this fully quantum-mechanicaltreatment of the conduction electrons, we find that: (i) only in the presenceof the interfacial Rashba SOC the non-zero dc pumping voltage in F/I/N semi-MTJcan emerge at the adiabatic level (i.e., proportional to microwave frequency);(ii) a unique signature of this charge pumping phenomenon, which disappears ifRashba SOC is not located with the precessing F layer, is dc pumping voltagethat changes sign as the function of the precession cone angle; (iii) unlikestandard spin pumping in the absence of SOCs, where one emitted or absorbedmicrowave photon is sufficient to match the exact solution in the framerotating with the magnetization, the presence of the Rashba SOC requires totake into account up to ten photons in order to reach the asymptotic value ofpumped charge current; (iv) disorder within F/I/F MTJs can enhance the dcpumping voltage in the quasiballistic transport regime; ...
机译:我们通过在存在F / I / F磁性隧道结(MTJ)或F / I / Nemi-MTJ的铁磁性层之一中进动磁化,开发了一种与时间有关的非平衡格林函数(NEGF)方法来解决自旋泵浦问题F / I界面处的本征Rashba自旋轨道耦合(SOC)或有限厚度的大部分F层(F铁磁体; N普通金属; I绝缘势垒)中的本征SOC。为了表示平均开路时间的抽运电荷电流或相应的直流电压信号,该电流是最近在半MTJ上进行的实验[T. Moriyamaet等,物理学。牧师100,067602(2008)],我们构建了经过两次傅立叶变换的NEGF的新颖解决方案。 NEGF在此表示中的两个能量论点通过描述多光发射和吸收过程的Floquet定理联系起来。在对传导电子进行完全量子力学处理的过程中,我们发现:(i)仅在存在界面Rashba SOC的情况下,F / I / N半MTJ中的非零直流泵浦电压才能出现在绝热水平(即, (ii)这种电荷抽运现象的独特特征是直流抽运电压,该电荷抽运现象的特征在于进动锥角的函数;如果Rashba SOC不在进动的F层中,则该电荷消失。 (iii)与没有SOC的标准自旋泵不同,在标准自旋泵中没有一个SOC时,一个发射或吸收的微波光子足以使框架旋转中的精确解与磁化相匹配,而Rashba SOC的存在需要考虑多达十个光子才能达到泵浦充电电流的渐近值; (iv)F / I / F MTJ内的混乱会提高准弹道运输制度中的倾销电压; ...

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