• Photonics Research
  • Vol. 5, Issue 6, 543 (2017)
Limei Qi* and Chang Liu
Author Affiliations
  • School of Electronic Engineering, Beijing University of Posts and Telecommunications, Beijing 100876, China
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    DOI: 10.1364/PRJ.5.000543 Cite this Article Set citation alerts
    Limei Qi, Chang Liu, "Complex band structures of 1D anisotropic graphene photonic crystal," Photonics Res. 5, 543 (2017) Copy Citation Text show less

    Abstract

    The complex band structures of a 1D anisotropic graphene photonic crystal are investigated, and the dispersion relations are confirmed using the transfer matrix method and simulation of commercial software. It is found that the result of using effective medium theory can fit the derived dispersion curves in the low wave vector. Transmission, absorption, and reflection at oblique incident angles are studied for the structure, respectively. Omni-gaps exist for angles as high as 80° for two polarizations. Physical mechanisms of the tunable dispersion and transmission are explained by the permittivity of graphene and the effective permittivity of the multilayer structure.
    ϵg=[ϵg,t000ϵg,t000ϵg,].(1)

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    ϵg,t=1+jσ(ω)ϵ0ωa.(2)

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    σintra=je2kBTπ2(ωjΓ)[μckBT+2ln(eμckBT+1)],(3)

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    σinter=je24πln[2μc(ωjΓ)2μc+(ωjΓ)],(4)

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    (ExIHyI)=M1(ExIIHyII),(5)

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    M1=(cos(k1za)jη1sin(k1za)jη1sin(k1za)cos(k1za)),(6)

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    M2=(cos(k2zb)jη2sin(k2zb)jη2sin(k2zb)cos(k2zb)),(7)

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    HzxHxz=jωϵ0ϵg,tEy,(8)

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    Eyz=jωμ0Hx,(9)

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    Eyx=jωμ0Hz.(10)

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    2Eyz2+2Eyx2+k02ϵg,tEy=0.(11)

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    k1z2+k1x2=k02ϵg,t.(12)

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    M1=(cos(k1za)jη1sin(k1za)jη1sin(k1za)cos(k1za)),(13)

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    M2=(cos(k2zb)jη2sin(k2zb)jη2sin(k2zb)cos(k2zb)),(14)

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    M=M1M2=(cos(k1za)cos(k2zb)η2η1sin(k1za)sin(k2zb)jη2cos(k1za)sin(k2zb)jη1sin(k1za)cos(k2zb)jη2cos(k1za)sin(k2zb)jη1sin(k1za)cos(k2zb)cos(k1za)cos(k2zb)η1η2sin(k1za)sin(k2zb)).(15)

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    (ExIHyI)=MN(ExN+1HyN+1)=(m11m12m21m22)(ExN+1HyN+1),(16)

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    r=HyrIHyiI=m11η0+m12η0ηN+1m21m22ηN+1m11η0+m12η0ηN+1+m21+m22ηN+1,t=HytN+1HyiI=2η0m11η0+m12η0ηN+1+m21+m22ηN+1,(17)

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    R=|r|2,T=|t|2,A=1RT.(18)

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    cos(kzd)=12Tr(M)=cos(k1za)cos(k2zb)12(η1η2+η2η1)sin(k1za)sin(k2zb),(19)

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    f12(ω)cos2(kRd)f22(ω)sin2(kRd)=1real,(20)

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    f12(ω)cosh2(kId)+f22(ω)sinh2(kId)=1imaginary,(21)

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    kz2ϵxeff+kx2ϵzeff=k02(TM),(22)

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    kz2+kx2=ϵxeffk02(TE),(23)

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    ω2c2=kz2ϵxeff.(24)

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