2017
DOI: 10.1126/sciadv.1701377
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Electrical access to critical coupling of circularly polarized waves in graphene chiral metamaterials

Abstract: Electric control of coupling in hybrid graphene/metamaterial system enables strong selective modulation of light polarization.

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Cited by 131 publications
(95 citation statements)
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References 49 publications
(55 reference statements)
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“…Due to the uncoupled nature of resonances for left-handed and right-handed circularly-polarized light, this method can be applied independently to left-handed and right-handed circular polarization. Using this formalism, the contribution of each mode of resonator into the complex transmission T is the following 55 : where ν n denotes the resonant frequencies of the metasurface, Γ r n and Γ i n are the radiation and intrinsic losses of the resonances respectively, and ϕ n represents the phase delay due to the thickness of the metasurface for each resonance mode. In our case, the transmission for RCP and LCP waves can be perfectly described by the system with four resonant frequencies (N = 4).…”
Section: Resultsmentioning
confidence: 99%
“…Due to the uncoupled nature of resonances for left-handed and right-handed circularly-polarized light, this method can be applied independently to left-handed and right-handed circular polarization. Using this formalism, the contribution of each mode of resonator into the complex transmission T is the following 55 : where ν n denotes the resonant frequencies of the metasurface, Γ r n and Γ i n are the radiation and intrinsic losses of the resonances respectively, and ϕ n represents the phase delay due to the thickness of the metasurface for each resonance mode. In our case, the transmission for RCP and LCP waves can be perfectly described by the system with four resonant frequencies (N = 4).…”
Section: Resultsmentioning
confidence: 99%
“…6(b). Recently, many graphene-meta-hybridized tunable metadevices were demonstrated in both the THz [120][121][122][123][124] and IR regimes [125][126][127][128][129][130][131], which exhibit diversified functionalities, such as tunable absorbers [120,123,130], phase modulators [128,129], active polarization controllers [124], and beam steering [131]. Unfortunately, the phase tuning ranges of these graphene-metasurfaces are all very limited.…”
Section: 4a Electrically Tunable Metasurfacesmentioning
confidence: 99%
“…Since chirality is inherently a three-dimensional (3D) phenomenon that requires coupling between the local electric and the magnetic dipoles [16,17], artificial constituents are usually designed with complex conformations [18], such as spiral with multiple helices [11,16,19], or near-field coupled multilayer metamaterials [20,21]. Polarity reversal of intrinsic chirality is usually accompanied by 3D structural reconfiguration of metamaterial constituents via various approaches [22][23][24], such as by integrating semiconductors (silicon) [18], phase change materials (Ge 2 Sb 2 Te 5 ) [25], graphene [26], magnesium [24], DNA scaffold [27], and MEMS actuators [11,19]. However, a structural reconfiguration usually demands intense stimuli, like large dosage of optical pump fluence (∼1 mJ/cm 2 ) [18], high voltage (∼350 V) [19], high temperature (180 ∘ C) [25], chemical reaction (hydrogenation) [24], or pneumatic control (10 Pa) [11] that limits the applications of these fascinating devices.…”
Section: Introductionmentioning
confidence: 99%