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Carrier-impurity spin transfer dynamics in paramagnetic II-VI diluted magnetic semiconductors in the presence of a wave-vector-dependent magnetic field

机译:顺磁性II-VI稀释的载体杂质自旋转移动力学   存在依赖于波矢量的磁性的磁性半导体   领域

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摘要

Quantum kinetic equations of motion for carrier and impurity spins inparamagnetic II-VI diluted magnetic semiconductors in a $\mathbf{k}$-dependenteffective magnetic field are derived, where the carrier-impurity correlationsare taken into account. In the Markov limit, rates for the electron-impurityspin transfer can be derived for electron spins parallel and perpendicular tothe impurity spins corresponding to measurable decay rates in Kerr experimentsin Faraday and Voigt geometry. Our rigorous microscopic quantum kinetictreatment automatically accounts for the fact that, in an individual spinflip-flop scattering process, a spin flip of an electron is necessarilyaccompanied by a flop of an impurity spin in the opposite direction and thecorresponding change of the impurity Zeeman energy influences the final energyof the electron after the scattering event. This shift in the electron energiesafter a spin flip-flop scattering processes, which usually has been overlookedin the literature, turns out to be especially important in the case ofextremely diluted magnetic semiconductors in an external magnetic field. As aspecific example for a $\mathbf{k}$-dependent effective magnetic field theeffects of a Rashba field on the dynamics of the carrier-impurity correlationsin a Hg$_{1-x-y}$Cd$_y$Mn$_x$Te quantum well are described. It is found that,although accounting for the Rashba interaction in the dynamics of thecorrelations leads to a modified $\mathbf{k}$-space dynamics, the timeevolution of the total carrier spin is not significantly influenced.Furthermore, a connection between the present theory and the description ofcollective carrier-impurity precession modes is presented.
机译:推导了依赖于$ \ mathbf {k} $的有效磁场中,顺磁性II-VI稀释的顺磁性II-VI稀释磁性半导体中载流子和杂质自旋的量子动力学方程,其中考虑了载流子与杂质的相关性。在马尔可夫极限中,对于与法拉第和Voigt几何学中的Kerr实验中可测量的衰减速率相对应的平行和垂直于杂质自旋的电子自旋,可以导出电子杂质自旋转移的速率。我们严格的微观量子动力学处理自动解释了以下事实:在单个自旋触发器散射过程中,电子的自旋翻转必然伴随着相反方向的杂质自旋翻转,并且杂质塞曼能量的相应变化会影响电子的自旋翻转。散射事件后电子的最终能量。在自旋触发器散射过程之后,电子能量的这种偏移在文献中通常被忽略,在外部磁场中极度稀释的磁性半导体的情况下,这一点变得尤为重要。作为依赖于$ \ mathbf {k} $的有效磁场的一个特定示例,Rashba场对Hg $ _ {1-xy} $ Cd $ _yyMn $ x $ Te中载流子-杂质相关动力学的影响描述量子阱。研究发现,尽管考虑了相关动力学中的拉什巴相互作用,导致修正了$ \ mathbf {k} $-空间动力学,但是总载流子自旋的时间演化并没有受到明显的影响。给出了载流子-杂质联合进动模式的理论和描述。

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