Control of Circular Photogalvanic Effect of Surface States in the Topological Insulator Bi<sub>2</sub>Te<sub>3</sub> via Spin Injection

Jinling Yu, Lijia Xia, Kejing Zhu, Qinggao Pan, Xiaolin Zeng, Yonghai Chen, Yu Liu, Chunming Yin, Shuying Cheng, Yunfeng Lai,

ACS Applied Materials & Interfaces · 2020 · 29 citations · 20 references

Abstract

The circular photogalvanic effect (CPGE) provides a method utilizing circularly polarized light to control spin photocurrent and will also lead to novel opto-spintronic devices. The CPGE of three-dimensional topological insulator Bi<sub>2</sub>Te<sub>3</sub> with different substrates and thicknesses has been systematically investigated. It is found that the CPGE current can be dramatically tuned by adopting different substrates. The CPGE current of the Bi<sub>2</sub>Te<sub>3</sub> films on Si substrates are more than two orders larger than that on SrTiO<sub>3</sub> substrates when illuminated by 1064 nm light, which can be attributed to the modulation effect due to the spin injection from Si substrate to Bi<sub>2</sub>Te<sub>3</sub> films, larger light absorption coefficient, and stronger inequivalence between the top and bottom surface states for Bi<sub>2</sub>Te<sub>3</sub> films grown on Si substrates. The excitation power dependence of the CPGE current of Bi<sub>2</sub>Te<sub>3</sub> films on Si substrates shows a saturation at high power especially for thicker samples, whereas that on SrTiO<sub>3</sub> substrates almost linearly increases with excitation power. Temperature dependence of the CPGE current of Bi<sub>2</sub>Te<sub>3</sub> films on Si substrates first increases and then decreases with decreasing temperature, whereas that on SrTiO<sub>3</sub> substrates changes monotonously with temperature. These interesting phenomena of the CPGE current of Bi<sub>2</sub>Te<sub>3</sub> films on Si substrates are related to the spin injection from Si substrates to Bi<sub>2</sub>Te<sub>3</sub> films. Our work not only intrigues new physics but also provides a method to effectively manipulate the helicity-dependent photocurrent via spin injection.

References

20