• Advanced Photonics
  • Vol. 5, Issue 4, 046001 (2023)
Karim Achouri*, Ville Tiukuvaara, and Olivier J. F. Martin
Author Affiliations
  • Institute of Electrical and Microengineering, École Polytechnique Fédérale de Lausanne, Nanophotonics and Metrology Laboratory, Lausanne, Switzerland
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    DOI: 10.1117/1.AP.5.4.046001 Cite this Article Set citation alerts
    Karim Achouri, Ville Tiukuvaara, Olivier J. F. Martin. Spatial symmetries in nonlocal multipolar metasurfaces[J]. Advanced Photonics, 2023, 5(4): 046001 Copy Citation Text show less

    Abstract

    We propose a framework that connects the spatial symmetries of a metasurface to its material parameter tensors and its scattering matrix. This provides a simple and universal way to effortlessly determine the properties of a metasurface scattering response, such as chirality or asymmetric transmission, and which of its effective material parameters should be taken into account in the prospect of a homogenization procedure. In contrast to existing techniques, this approach does not require any a priori knowledge of group theory or complicated numerical simulation schemes, hence making it fast, easy to use and accessible. Its working principle consists in recursively solving symmetry-invariance conditions that apply to dipolar and quadrupolar material parameters, which include nonlocal interactions, as well as the metasurface scattering matrix. The overall process thus only requires listing the spatial symmetries of the metasurface. Using the proposed framework, we demonstrate the existence of multipolar extrinsic chirality, which is a form of chiral response that is achieved in geometrically achiral structures sensitive to field gradients, even at normal incidence.
    [DB]=[ϵ¯¯ξ¯¯ζ¯¯μ¯¯]·[EH],

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    ϵ¯¯=ϵ¯¯T,μ¯¯=μ¯¯T,ζ¯¯=ξ¯¯T,

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    E=Λ¯¯·E,(3a)

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    H=1jωϵ0(Λ¯¯·)×(Λ¯¯·E)=det(Λ¯¯)Λ¯¯·H,(3b)

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    D=Λ¯¯·D,(4a)

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    B=det(Λ¯¯)Λ¯¯·B.(4b)

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    ϵ¯¯=Λ¯¯·ϵ¯¯·Λ¯¯T,(5a)

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    μ¯¯=Λ¯¯·μ¯¯·Λ¯¯T,(5b)

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    ξ¯¯=det(Λ¯¯)Λ¯¯·ξ¯¯·Λ¯¯T,(5c)

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    ζ¯¯=det(Λ¯¯)Λ¯¯·ζ¯¯·Λ¯¯T,(5d)

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    D=ϵ0E+P+·Q¯¯,(6a)

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    B=μ0(H+M+·S¯¯),(6b)

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    [PiMiQilSil][χeeijχemijχeeijkχemijkχmeijχmmijχmeijkχmmijkQeeiljQemiljQeeiljkQemiljkSmeiljSmmiljSmeiljkSmmiljk]·[EjHjkEjkHj],

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    Ti=aΛijTj,(8a)

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    Tij=aΛimΛjkTmk,(8b)

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    Tijk=aΛilΛjmΛknTlmn,(8c)

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    Tijkl=aΛimΛjnΛkoΛlpTmnop,(8d)

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    Ti=aΛijTj,(9a)

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    Tij=aΛimΛjkTmk,(9b)

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    Tijk=aΛilΛjmΛknTlmn,(9c)

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    Tijkl=aΛimΛjnΛkoΛlpTmnop,(9d)

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    ϵ¯¯=[ϵxxϵxyϵxzϵxyϵyyϵyzϵxzϵyzϵzz],

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    ϵ¯¯=[ϵxx000ϵyyϵyz0ϵyzϵzz].

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    ϵ¯¯=[ϵxx000ϵyy000ϵzz].

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    ϵ¯¯=[ϵxx000ϵxx000ϵzz],

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    S¯¯=[R11R12T13T14R21R22T23T24T31T32R33R34T41T42R43R44],

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    Λ¯¯=Rz(ϕ)·Λ¯¯·Rz(ϕ)T,

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    S¯¯=M¯¯·[bS¯¯+(1b)S¯¯T]·M¯¯1,

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    c1={1,if  Λxz=Λyz=0,0,otherwise,(17a)

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    c2={1,if  Λ¯¯·y=±R¯¯z(ϕ)T·R¯¯z(ϕ)·y,0,otherwise.(17b)

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    M¯¯=[a¯¯+a¯¯a¯¯a¯¯+],

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    a¯¯+=c2(1+Λzz)[Λyy00Λxx]+(1c)I¯¯t,(19a)

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    a¯¯=c2(1Λzz)[Λyy00Λxx],(19b)

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    M¯¯C4,z=[0100100000010010].

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    E={(xEy+yEx)/2,(xEz+zEx)/2,(yEz+zEy)/2,xEx,yEy,zEz},

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    S¯¯=[R11R12T13T14R12R22T14T24T13T14R11R12T14T24R12R22].

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    S¯¯=[R110T1300R220T24T130R1100T240R22].

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    S¯¯=[R11R12T13T14R12R22T14T24T13T14R11R12T14T24R12R22].

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    S¯¯=[R110T1300R220T24T130R1100T240R22].

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    S¯¯=[R110T1300R220T24T310R3300T420R44].

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    S¯¯=[R11R12T13T14R12R22T23T24T13T23R33R34T14T24R34R44].

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    S¯¯=[R110T1300R110T13T130R1100T130R11],

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    S¯¯=[R11R12T13T14R12R11T14T13T13T14R11R12T14T13R12R11].

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    Λ¯¯=I¯¯2nn,

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    σx=[100010001],(31a)

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    σy=[100010001],(31b)

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    σz=[100010001].(31c)

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    Rx(θ)=[1000cosθsinθ0sinθcosθ],(32a)

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    Ry(θ)=[cosθ0sinθ000sinθ0cosθ],(32b)

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    Rz(θ)=[cosθsinθ0sinθcosθ0001].(32c)

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    CN,i=Ri(2πN).

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    Karim Achouri, Ville Tiukuvaara, Olivier J. F. Martin. Spatial symmetries in nonlocal multipolar metasurfaces[J]. Advanced Photonics, 2023, 5(4): 046001
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