State Key Laboratory of Optical Technologies on Nano-Fabrication and Micro-Engineering, Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu, 610209, China.
College of Physics, Sichuan University, Chengdu, 610064, China.
Nanoscale. 2023 Jul 6;15(26):11155-11162. doi: 10.1039/d3nr01497e.
Polaritons - material excitation coupled with light - are thought to hold the potential for the extreme control of light down to the atomic length scale because of their high field confinement and sub-wavelength scales. For practical applications, it is essential but still a formidable challenge to manipulate polaritons with high efficiency and a wide tunable range. These obstacles may be overcome by the topology of polaritons. In photonic systems composed of graphene/α-MoO heterostructures, the topology of the hybrid polariton characterized by the isofrequency curve can transform from open hyperbolas to closed ellipse-like curves, driven by the carrier concentrations of graphene. The electronic tunability of such topological polaritons offers a unique platform for two-dimensional energy transfer. Here, by introducing local gates to obtain a tunable spatial carrier density profile in the graphene/α-MoO heterostructure, the phase of the polariton is predicted to be efficiently tuned from 0 to 2π . Remarkably, the reflectance and transmittance through the gap between local gates can also be modulated from 0 to 1 with high efficiency, where the device length can be less than 100 nm. The modulation is achieved owing to the dramatic changes in the wave vector of polaritons near the topological transition point. The proposed structures not only have direct applications in two-dimensional optics such as total reflectors, phase (amplitude) modulators, and optical switches but also can serve as an important component for complex nano-optical devices.
极化激元——与光耦合的物质激发——被认为具有在原子长度尺度上极端控制光的潜力,因为它们具有高场限制和亚波长尺度。对于实际应用,高效率和宽可调谐范围地操控极化激元是至关重要的,但仍然是一个艰巨的挑战。这些障碍可以通过极化激元的拓扑结构来克服。在由石墨烯/α-MoO 异质结构组成的光子系统中,由等频曲线表征的混合极化激元的拓扑结构可以通过石墨烯的载流子浓度从开放的双曲型转变为封闭的椭圆型曲线。这种拓扑极化激元的电子可调谐性为二维能量转移提供了一个独特的平台。在这里,通过引入局部栅极在石墨烯/α-MoO 异质结构中获得可调谐的空间载流子密度分布,可以有效地将极化激元的相位从 0 调谐到 2π。值得注意的是,通过局部栅极之间的间隙的反射率和透射率也可以以高效率从 0 调制到 1,其中器件长度可以小于 100nm。这种调制是由于在拓扑相变点附近极化激元的波矢发生剧烈变化而实现的。所提出的结构不仅在二维光学中具有直接应用,如全反射镜、相位(幅度)调制器和光开关,而且还可以作为复杂纳米光学器件的重要组成部分。