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Controllable spin polarization in a DMS quantum dot

机译:DMS量子点中的可控自旋极化

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摘要

The effects of electro-magnetic confining potentials and the s-d exchange interaction between substituted Mn ions and carriers on the spin polarization of carriers in an diluted magnetic semiconductor quantum dot are investigated within the framework of the effective-mass theory. The energy eigenvalues and wavefunctions of a single electron in the presence of an external magnetic field are studied by solving the one particle Schrodinger equation including the conventional Zeeman effect, the s-d exchange interaction and the electric confining potential which describes the dot. The eigenenergy structure for low lying states is strongly dependant on the relative sizes of the s-d exchange interactions and the conventional Zeeman energy splitting. When the spin splitting exceeds the cyclotron energy splitting, the Landau level overlappings occur so that the spin polarization of carriers is induced in low lying energy states. This spin polarization of carriers in the diluted magnetic semiconductor quantum dot can be controlled by changing the electro-magnetic confining potentials.
机译:在有效质量理论的框架内,研究了电磁约束势以及取代的Mn离子与载流子之间的s-d交换相互作用对稀磁半导体量子点中载流子自旋极化的影响。通过求解包括传统塞曼效应,s-d交换相互作用和描述点的电约束势的一个粒子薛定inger方程,研究了在存在外部磁场的情况下单个电子的能量本征值和波函数。低位态的本征能量结构在很大程度上取决于s-d交换相互作用和常规塞曼能量分裂的相对大小。当自旋分裂超过回旋加速器能量分裂时,会发生Landau能级重叠,从而在低能量状态下引起载流子的自旋极化。稀释的磁性半导体量子点中载流子的这种自旋极化可以通过改变电磁限制电位来控制。

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