2014
DOI: 10.1016/j.photonics.2014.06.005
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Electromagnetic waves reflection, transmission and absorption by graphene–magnetic semiconductor–graphene sandwich-structure in magnetic field: Faraday geometry

Abstract: Electrodynamic properties of the graphene -magnetic semiconductor -graphene sandwich-structure have been investigated theoretically with taking into account the dissipation processes. Influence of graphene layers on electromagnetic waves propagation in graphene -semi-infinte magnetic semiconductor and graphene -magnetic semiconductor -graphene sandwich-structure has been analyzed. Frequency and field dependences of the reflectance, transmittance and absorbtance of electromagnetic waves by such structure have b… Show more

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Cited by 13 publications
(5 citation statements)
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“…A PC is shown schematically in Figure 1. As a magnetically active material, we have chosen a well-studied magnetic semiconductor CdCr 2 Se 4 , which combines the properties of a semiconductor (sufficiently high conductivity, can be pand n-type depending on the production method) and a magnetic (sufficiently high magnetization) [26]. This material is characterized by cyclotron and ferromagnetic resonances with a narrow width of the resonance curve, which significantly expands the possibilities of its practical application [27].…”
Section: Geometry and Materials Parameters Of A Photonic Cellmentioning
confidence: 99%
See 1 more Smart Citation
“…A PC is shown schematically in Figure 1. As a magnetically active material, we have chosen a well-studied magnetic semiconductor CdCr 2 Se 4 , which combines the properties of a semiconductor (sufficiently high conductivity, can be pand n-type depending on the production method) and a magnetic (sufficiently high magnetization) [26]. This material is characterized by cyclotron and ferromagnetic resonances with a narrow width of the resonance curve, which significantly expands the possibilities of its practical application [27].…”
Section: Geometry and Materials Parameters Of A Photonic Cellmentioning
confidence: 99%
“…where plasma and cyclotron frequencies are introduced ω p = 4πe 2 n 0 /m * ε l and ω c = eH 0 /m * c. For numerical modeling, we will use the parameters of the above p-type magnetic semiconductor: ε l 17.8 is the lattice part of the permittivity, n 0 and m * is the concentration of carriers n 0 = 6 • 10 14 cm −3 , their effective mass m * = 0.1 m e , ω ν = ω + iν, collision frequency ν = 10 11 s −1 [26,28]. The effective permittivity is ε ⊥ = ε − ε 2 a /ε taking into account the transverse orientation of the external magnetic field with respect to the wave vector (k ⊥ H 0 ).…”
Section: Geometry and Materials Parameters Of A Photonic Cellmentioning
confidence: 99%
“…Three optical phenomena of reflection, transmission, and absorption occur when sunlight is incident on the surface of a medium; and the sum of energies of reflected, transmitted, and absorbed light equals the energy of the incident light. 15 Design and preparation of various light absorbing materials with desired architectures are needed to increase solar energy utilization efficiency for solar-driven vapor generation. The ideal solar absorber collects the energy of the broad solar spectrum from ultraviolet to near-infrared with minimum reflection and transmission.…”
Section: Solar Absorptionmentioning
confidence: 99%
“…Multilayer graphenebased structures have a number of interesting properties, including waveguide ones [9,10]. Structures based on graphene and gyrotropic materials have features as well [11,12]. Recently we have shown influence of graphene coating on speckle-pattern rotation in gyrotropic optical fiber [13].…”
Section: Introductionmentioning
confidence: 99%