首页> 外文期刊>World Journal of Condensed Matter Physics >Interplay between Carrier Polarization, Spin-Orbit Coupling and Exchange Field on Anomalous Hall Conductivity in the Presence of Magnetic Impurity in Mn Doped GaAs
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Interplay between Carrier Polarization, Spin-Orbit Coupling and Exchange Field on Anomalous Hall Conductivity in the Presence of Magnetic Impurity in Mn Doped GaAs

机译:Mn掺杂GaAs中磁性杂质的载流子极化,自旋轨道耦合和交换场对反常霍尔电导率的相互作用

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We develop a model Hamiltonian to treat anomalous Hall conductivity in dilute magnetic semiconductor (DMS) of type (III, Mn, V) considering the impurity potentials (potential due to interaction of spin of carriers with localized spin of dopant (Mn) and coulomb like potential). Using equation of motion in Green function together with Quantum Kubo-formula of conductivity, the anomalous Hall conductivity is calculated as function of spin-orbit coupling, exchange field and carrier polarization. The calculated result shows that at low impurity concentration, the interplay between spin polarization of carriers, spin-orbit coupling and exchange fields is crucial for existence of anomalous Hall conductivity. The monotonic increment of anomalous Hall conductivity with exchange field is observed for strong spin-orbit coupling limit. In weak spin-orbit coupling limit, the magnitude of anomalous Hall conductivity increases parabolically with the spin-orbit coupling. Our results provide an important basis for understanding the interplay between the spin polarization, spin-orbit coupling, and exchange field on anomalous Hall conductivity at low impurity concentration. The findings are also a key step to realize dissipationless quantum transport without external magnetic field.
机译:考虑杂质势(由于载流子自旋与局部掺杂物(Mn)和库仑自旋的相互作用而引起的电势),我们开发了一种哈密顿量模型来处理类型(III,Mn,V)的稀磁半导体(DMS)中的异常霍尔电导率潜在)。结合格林函数运动方程和电导率的量子久保公式,计算了反常霍尔电导率与自旋轨道耦合,交换场和载流子极化的关系。计算结果表明,在低杂质浓度下,载流子自旋极化,自旋轨道耦合和交换场之间的相互作用对霍尔电导率异常的存在至关重要。对于强自旋轨道耦合极限,观察到霍尔电导率随交换场的单调递增。在弱的自旋轨道耦合极限下,异常霍尔电导率的大小随自旋轨道耦合抛物线地增加。我们的结果为理解自旋极化,自旋轨道耦合以及低杂质浓度下异常霍尔电导率交换场之间的相互作用提供了重要依据。这些发现也是在没有外部磁场的情况下实现无耗散量子传输的关键步骤。

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