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Optical control of spin-polarized photocurrent in topological insulator thin films

机译:拓扑绝缘体薄膜中自旋极化光电流的光学控制

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摘要

Dirac electrons in topological insulators (TIs) provide one possible avenue to achieve control of photocurrents and spin currents without the need to apply external fields by utilizing characteristic spin-momentum locking. However, for TI crystals with electrodes it is actually difficult to characterize the net flow of spin-polarized photocurrents because of the coexistence of surface carriers and bulk carriers generated by optical excitations. We demonstrate here that the net flow directions of spin-polarized photocurrents in TI polycrystalline thin films without electrodes can be precisely and intentionally controlled by the polarization of the excitation pulse alone, which is characterized by performing time-domain terahertz (THz) wave measurements and time-resolved magneto-optical Kerr rotation measurements that are non-contact methods. We show that the amplitudes of s-polarized THz waves radiated from photocurrents under right- and left-circularly polarized excitations are inverted relative to one another. Moreover, we observe the inversion of time-resolved magneto-optical Kerr rotation signals between the two excitations. Our results will open the way as innovative methods to control spin-polarized electrons in optoelectronic and spintronic TI devices without the need to apply external fields.
机译:拓扑绝缘体(TI)中的狄拉克电子为实现控制光电流和自旋电流提供了一种可能的途径,而无需通过利用特有的自旋动量锁定来施加外部场。但是,对于带电极的TI晶体,由于光激发产生的表面载流子和体载流子并存,因此实​​际上很难表征自旋极化光电流的净流量。我们在这里证明,没有电极的TI多晶薄膜中自旋极化光电流的净流向可以仅通过激发脉冲的极化来精确而有意地控制,其特征在于执行时域太赫兹(THz)波测量和非接触式时间分辨磁光克尔旋转测量。我们表明,在右旋和左旋圆偏振激发下,从光电流辐射出的s极化THz波的振幅彼此相反。此外,我们观察到两次激励之间时间分辨的磁光克尔旋转信号的反转。我们的结果将为控制光电和自旋电子TI器件中的自旋极化电子而无需施加外部场的创新方法开辟道路。

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