2016
DOI: 10.1088/0022-3727/49/32/32lt01
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Dually guided-mode-resonant graphene perfect absorbers with narrow bandwidth for sensors

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Cited by 38 publications
(29 citation statements)
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“…To overcome this problem, various physical mechanisms [ 18 43 ] to enhance absorption of graphene in the visible region have been proposed, which include strong photon localization on the defect layer in one-dimensional (1D) photonic crystals [ 18 , 28 , 33 , 38 ], total internal reflection [ 19 , 20 , 23 , 27 ], surface plasmon resonances [ 21 , 22 , 30 , 31 , 33 ], evanescent diffraction orders of the arrays of metal nanoparticles [ 34 ], and critical coupling to guided mode resonances [ 25 , 26 , 32 , 34 , 35 , 37 , 39 41 ]. Besides the absorption enhancement in graphene, achieving multiband and broadband light absorption in graphene is also important for some graphene-based optoelectronic devices from a practical point of view.…”
Section: Introductionmentioning
confidence: 99%
“…To overcome this problem, various physical mechanisms [ 18 43 ] to enhance absorption of graphene in the visible region have been proposed, which include strong photon localization on the defect layer in one-dimensional (1D) photonic crystals [ 18 , 28 , 33 , 38 ], total internal reflection [ 19 , 20 , 23 , 27 ], surface plasmon resonances [ 21 , 22 , 30 , 31 , 33 ], evanescent diffraction orders of the arrays of metal nanoparticles [ 34 ], and critical coupling to guided mode resonances [ 25 , 26 , 32 , 34 , 35 , 37 , 39 41 ]. Besides the absorption enhancement in graphene, achieving multiband and broadband light absorption in graphene is also important for some graphene-based optoelectronic devices from a practical point of view.…”
Section: Introductionmentioning
confidence: 99%
“… where β is the propagation wavenumber along the guiding direction, k 0 is the free-space wavenumber, n eff is the effective refractive index of the mode inside the core, m is the diffraction order, λ 0 is the free-space wavelength and Λ is the grating period. Writing an analytical expression for the phase-matching condition in Device I is cumbersome because our grating diffracts incoming waves in not only the x-direction but also in the y-direction, as opposed to the explicitly used devices with 1D grating 44 – 51 does. Therefore, the guided-mode’s propagation direction is not simply the x-direction as in Device 0.…”
Section: Resultsmentioning
confidence: 99%
“…The difference between two methods is the structures where GMRs are excited. The third method is to couple graphene to the GMRs of photonic crystal slabs (PhCs) 43 or 1-dimensional photonic crystals (1DPCs), excited by sub-wavelength grating (SWG) couplers 44 , 45 . The guided-mode leaks out evanescent waves to graphene.…”
Section: Introductionmentioning
confidence: 99%
“…The FoM of the HRA is relatively small due to the large FWHM. However, the sensitivity of the HRA is comparable with many other nanostructures, such as waveguide gratings [43][44][45] and plasmonic absorbers [46,47] in the visible and near-infrared region, and there is a good linearity between the absorption peak and the refractive index of the background. Therefore, dual-band absorption enhancement of the HRA may be suitable for sensing-related applications.…”
Section: Resultsmentioning
confidence: 96%