2019
DOI: 10.1016/j.carbon.2019.08.020
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The novel graphene metasurfaces based on split-ring resonators for tunable polarization switching and beam steering at terahertz frequencies

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Cited by 64 publications
(29 citation statements)
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“…[19][20][21][22][23][24][25][26] Systems utilizing graphene could potentially provide the necessary functionalities. However, to achieve polarization conversion, symmetry breaking has to be introduced; this can be implemented geometrically, [15,[27][28][29] e.g., via patterned nanorectangles, [15] or by inducing anisotropy in the graphene conductivity, e.g., through the application of strong magnetic fields. [30] Alternatively, the tunable anisotropic conductivity of monolayer black phosphorus (BP), a 2D material with an inherent anisotropic crystalline structure, [24,31,32] can circumvent the above limitations, offering the desired tunability and wideband operation within the same system.…”
Section: Dynamic Control Of Light Chirality With Nanostructured Monol...mentioning
confidence: 99%
“…[19][20][21][22][23][24][25][26] Systems utilizing graphene could potentially provide the necessary functionalities. However, to achieve polarization conversion, symmetry breaking has to be introduced; this can be implemented geometrically, [15,[27][28][29] e.g., via patterned nanorectangles, [15] or by inducing anisotropy in the graphene conductivity, e.g., through the application of strong magnetic fields. [30] Alternatively, the tunable anisotropic conductivity of monolayer black phosphorus (BP), a 2D material with an inherent anisotropic crystalline structure, [24,31,32] can circumvent the above limitations, offering the desired tunability and wideband operation within the same system.…”
Section: Dynamic Control Of Light Chirality With Nanostructured Monol...mentioning
confidence: 99%
“…We use the Au gate bias voltage to change the working state of the graphene nanoribbons. According to the previous reports [26,40], we can know that there is almost no SPPs when the Fermi level of the graphene layer is 0. Since the graphene nanoribbons are off (Fermi level is 0) and the Fermi level of graphene rings are 1eV, the simulation results of the proposed device show two narrow filters which excited by the SPPs of graphene rings in the terahertz as shown in Fig.…”
Section: Model Constructionmentioning
confidence: 86%
“…As a two-dimensional material, graphene attracts considerable attention of researchers because of its unique optoelectronic properties [17][18][19][20][21]. Due to the semi-metallic properties of graphene, single-layer graphene can be processed into ribbon [22,23], disks [24,25], and split rings [26,27] that can also excite SPPs. The SPPs properties of graphene can be controlled by the Fermi level of graphene.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, based on the above two design strategies, it remains challenging to achieve a full 360 • phase modulation while maintaining high transmittance/reflectance. However, in most applications such as tuneable metalens [30,31], beam steering [32,33], switchable wave-plates [34][35][36] and polarisation control [37,38], dynamic phase modulation covering the full 360 • as well as high reflectance/transmittance are highly desirable. In order to tackle the challenge of the limited dynamic phase modulation range and relatively low reflectance/transmittance, Zhu et al [39] proposed and demonstrated a multiple resonance metasurface for providing 360 • phase variation in the microwave regime.…”
Section: Introductionmentioning
confidence: 99%