He Chuan, Zhao Qiyi, Huang Yuanyuan, Zhu Lipeng, Zhang Sujuan, Bai Jintao, Xu Xinlong
Shaanxi Joint Lab of Graphene, State Key Lab Incubation Base of Photoelectric Technology and Functional Materials, International Collaborative Center on Photoelectric Technology and Nano Functional Materials, Institute of Photonics & Photon-Technology , Northwest University , Xi'an 710069 , China.
School of Science , Xi'an University of Posts & Telecommunications , Xi'an 710121 , China.
J Phys Chem Lett. 2019 May 2;10(9):2090-2100. doi: 10.1021/acs.jpclett.9b00217. Epub 2019 Apr 16.
Light-frequency conversion based on two-dimensional (2D) materials is of great importance for modern nano- and integrated photonics. Herein, we report both the intrinsic (from the pure WX (X = S, Se, and Te)) and extrinsic (from the interface of graphene/WX) second-order nonlinear coefficient tensor from graphene/WX van der Waals (vdW) heterostructures by first-principles calculations. The prominent peaks in the dispersion relation of the intrinsic second-order nonlinear coefficient in monolayer WX are due to the Van Hove singularity in the high-symmetry point or along the high-symmetry line with high joint density of states. The enhanced nonlinear optical response in the infrared band can be achieved in graphene/WS vdW heterostructures, resulting from the interlayer charge transfer between graphene and WS. The value of the intrinsic second-order nonlinear coefficients of graphene/WSe vdW heterostructures is 1.5 times larger than that of pure monolayer WSe at the band gap energy of monolayer WSe because of the enhanced carrier generation after the heterostructure formation. Different from pure monolayer WX, azimuthal angle-dependent second harmonic generation from graphene/WX vdW heterostructures exhibits extraordinary rotational symmetry at different photon energies, which can be used to deduce the extrinsic second-order nonlinear coefficient. These results pave the way for the nonlinear optical coefficient design based on 2D heterostructures for nonlinear nanophotonics and integrated devices.
基于二维(2D)材料的光频率转换对于现代纳米光子学和集成光子学至关重要。在此,我们通过第一性原理计算报道了石墨烯/WX范德华(vdW)异质结构的本征(来自纯WX(X = S、Se和Te))和非本征(来自石墨烯/WX界面)二阶非线性系数张量。单层WX中本征二阶非线性系数色散关系中的显著峰值归因于高对称点或沿具有高态密度的高对称线的范霍夫奇点。石墨烯/WS vdW异质结构中可以实现红外波段增强的非线性光学响应,这是由于石墨烯和WS之间的层间电荷转移。由于异质结构形成后载流子产生增强,石墨烯/WSe vdW异质结构的本征二阶非线性系数值在单层WSe的带隙能量处比纯单层WSe大1.5倍。与纯单层WX不同,石墨烯/WX vdW异质结构的方位角相关二次谐波产生在不同光子能量下表现出非凡的旋转对称性,这可用于推导非本征二阶非线性系数。这些结果为基于二维异质结构的非线性纳米光子学和集成器件的非线性光学系数设计铺平了道路。