2016
DOI: 10.1088/2040-8978/18/4/044024
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Graphene, plasmons and transformation optics

Abstract: Here we study subwavelength gratings for coupling into graphene plasmons by means of an analytical model based on transformation optics that is not limited to very shallow gratings. We consider gratings that consist of a periodic modulation of the charge density in the graphene sheet, and gratings formed by this conductivity modulation together with a dielectric grating placed in close vicinity of the graphene. Explicit expressions for the dispersion relation of the plasmon polaritons supported by the system, … Show more

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Cited by 39 publications
(62 citation statements)
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“…Hence, it relates a simple flat and homogeneously biased graphene sheet in z-space to a periodically biased graphene monolayer in w-space. 28 In the above equation, γ is a scaling factor that yields the periodicity in z-space, w 0 represents the modulation strength and y 0 = w 0 e 2b −w 2 0 , where b is a parameter that represents the position of the graphene layer in the wspace. Figure 1(b) shows the conductivity modulation profile derived from the conformal transformation for different modulation strengths (plotted with solid lines).…”
Section: Graphene With 1d Conductivity Modulationmentioning
confidence: 99%
See 1 more Smart Citation
“…Hence, it relates a simple flat and homogeneously biased graphene sheet in z-space to a periodically biased graphene monolayer in w-space. 28 In the above equation, γ is a scaling factor that yields the periodicity in z-space, w 0 represents the modulation strength and y 0 = w 0 e 2b −w 2 0 , where b is a parameter that represents the position of the graphene layer in the wspace. Figure 1(b) shows the conductivity modulation profile derived from the conformal transformation for different modulation strengths (plotted with solid lines).…”
Section: Graphene With 1d Conductivity Modulationmentioning
confidence: 99%
“…Hence, it relates a simple flat and homogeneously biased graphene sheet in z-space to a periodically biased graphene monolayer in w-space. 28 In the above equation, γ is a scaling factor that yields the periodicity in z-space, w 0 represents the modulation strength and y 0 = 2, with {a 0 , a 1 } given by the Fourier expansion coefficients of the transformation 3. Hence, even though our analytical model in principle applies to conductivity modulations derived from the conformal transformation, it accurately describes the simple sinusoidal modulations given in Eq.…”
Section: Graphene With 1d Conductivity Modulationmentioning
confidence: 99%
“…We start by considering a plasmonic metasurface based on a graphene monolayer with spatially periodic conductivity [24,25]. The configuration we propose is sketched in Figure 1a.…”
Section: Introductionmentioning
confidence: 99%
“…Here, l and s are the chemical potential and the scattering time for electrons, respectively, with s ¼ ml=ev 2 F (m is the mobility and v F % 10 6 m/s the Fermi velocity). In this work, we use the parameters a = 76 GHz/X and c g = 1.5 THz, which correspond to l = 0.65 eV and m = 10 4 cm 2 /V s. The conductivity grating established via periodic doping allows for free space radiation to couple into the surface plasmons sustained by the graphene layer, which have much shorter wavelength [24][25][26][27][28][29][30][31][32][33][34]. Hence, the modulation period needs to be much smaller than the wavelength of incident radiation (k 0 ) 2pc).…”
Section: Introductionmentioning
confidence: 99%
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