ABSTRACT
Hyperbolic metamaterials have recently been widely investigated in nanophotonics systems. Here, we propose an alternating graphene/${{\rm SiO}_2}$SiO2 multilayer structure as an anisotropic medium with hyperbolic dispersion. When in-plane and out-of-plane effective permittivity is negative and positive, respectively, the incident beam (transverse magnetic polarization wave) can be split into two subwavelength beams, and a dark hollow beam can be achieved for circularly polarized incidence. Also, the size of the dark hollow beam can be tuned by changing the Fermi level. Our method is believed to be used as a tunable optical tweezer for controlling molecules.
ABSTRACT
Herein, we present a tunable multifunctional reflection polarizer, based on a graphene metasurface, which is composed of an array of cross double-ellipse graphene patches. A dual band of linear-to-linear (LTL) polarization conversions is achieved due to the superimposition of the two reflection components with a near 0° or 180° phase difference, in the mid-infrared region. By carefully choosing the parameters, linear-to-circular polarization conversion and broadband of LTL polarization conversion (about 0.7 THz) are also realized. Also, the tunable responses of the proposed reflection polarizer are discussed under a different Fermi energy and electron scattering time. It is believed that our proposed polarizer can be widely used for multifunctional and tunable polarization conversion.
ABSTRACT
Graphene surface plasmon (GSP) superlenses, induced from the negative refraction, have recently been demonstrated in various two-dimensional photonic crystal systems. However, inplane GSP superlenses have never been reported in a one-dimensional (1D) photonic crystal system. Here, we propose a graphene-Si/SiO2 system, by transferring a graphene sheet on the tilted 1D subwavelength silicon/silica gratings. By discussing the dispersion relations of the inplane GSP in this system, the GSP negative refraction is found in the mid-infrared region. When the tilted angle, working wavelength, and Fermi level are set to be 60°, 11.22 µm, and 0.2 eV, respectively, the off-axis subwavelength focusing has the best resolution, and the full width at half-maximum (FWHM) of the image is 0.0091λ (102.1 nm). Further, we investigate the effects of the Fermi level on the superlens frequency range, and the image's FWHM, the broadband, and the deep subwavelength superlens are achieved. The full-wave numerical simulations are conducted by the finite element method. Our findings can be applied to the manipulation of inplane GSP propagation and biological imaging.
