2015
DOI: 10.1007/s11468-015-0028-x
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Gate-Tunable mid-Infrared Plasmonic Planar Band-Stop Filters Based on a Monolayer Graphene

Abstract: In this paper, the graphene ribbon bus waveguide side-coupled a coplanar short graphene strip, constructed on a monolayer graphene with substrates by spatially varying external gates, is proposed and investigated numerically by using the finite-difference time-domain (FDTD) method. Simulated results exhibit that the outstanding mid-infrared band-stop filtering effect is realized based on the edge mode resonance in the short strip acting as a perfect Fabry-Perot resonator. By changing the locations of gate volt… Show more

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Cited by 24 publications
(4 citation statements)
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“…In our simulations, the ultra-narrow graphene ribbon with a width of 10 nm [27,[43][44][45][46][47] supports SPPs in the mid-infrared region. The surface conductivity (σ g ) of graphene is supported by Kubo's formula [48]…”
Section: Geometry Modeling and Methods Of Analysismentioning
confidence: 66%
“…In our simulations, the ultra-narrow graphene ribbon with a width of 10 nm [27,[43][44][45][46][47] supports SPPs in the mid-infrared region. The surface conductivity (σ g ) of graphene is supported by Kubo's formula [48]…”
Section: Geometry Modeling and Methods Of Analysismentioning
confidence: 66%
“…Here, to simplify the theoretical model, the terahertz wave propagation and coupling losses are not considered. For the harmonic time dependence of e −jωt , the temporal normalised mode amplitudes a i of the ith cavity (i = 1, 2, 3, 4) can be described as [26,27] da…”
Section: Theory Analysismentioning
confidence: 99%
“…Here, to simplify the theoretical model, the terahertz wave propagation and coupling losses are not considered. For the harmonic time dependence of e −j ωt , the temporal normalised mode amplitudes a i of the i th cavity ( i = 1, 2, 3, 4) can be described as [26, 27] normaldainormaldt=(jωiκo,iκe,i)ai+normalejθiκe,iS+,in(i)+normalejθiκe,iS,in(i) where ω i represents the resonance frequency of the i th cavity, κ o , i is the decay rate of the field due to internal loss in the i th cavity, and κ e,i is the decay rate due to the energy escape into the waveguide, θ i is the phase of coupling coefficient. The decay rates satisfy the relationships κ o , i = ω i /(2 Q o , i ), κ e,i = ω i /(2 Q e,i ), Q o , i and Q e,i stand for the intrinsic and coupling quality factors of the i th cavity, respectively.…”
Section: Theory Analysismentioning
confidence: 99%
“…For example, tunable plasmonic devices using graphene insulator stacks in the near-infrared band were experimentally demonstrated [10]. A monolayer graphene structure with tunable gates in the mid-infrared range was proposed to support the fabrication of planar nano-integrated plasmonic circuits [11]. Simulations were performed to achieve perfect plasmonic absorption in the far-infrared band using a metal-graphene-insulator-metal structure [12].…”
Section: Introductionmentioning
confidence: 99%