• Photonics Insights
  • Vol. 1, Issue 1, R02 (2022)
Shaojie Ma1, Biao Yang2, and Shuang Zhang1、3、*
Author Affiliations
  • 1Department of Physics, University of Hong Kong, Hong Kong, China
  • 2College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, China
  • 3Department of Electrical & Electronic Engineering, University of Hong Kong, Hong Kong, China
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    DOI: 10.3788/PI.2022.R02 Cite this Article Set citation alerts
    Shaojie Ma, Biao Yang, Shuang Zhang. Topological photonics in metamaterials[J]. Photonics Insights, 2022, 1(1): R02 Copy Citation Text show less

    Abstract

    Originally a pure mathematical concept, topology has been vigorously developed in various physical systems in recent years, and underlies many interesting phenomena such as the quantum Hall effect and quantum spin Hall effect. Its widespread influence in physics led the award of the 2016 Nobel Prize in Physics to this field. Topological photonics further expands the research field of topology to classical wave systems and holds promise for novel devices and applications, e.g., topological quantum computation and topological lasers. Here, we review recent developments in topological photonics but focus mainly on their realizations based on metamaterials. Through artificially designed resonant units, metamaterials provide vast degrees of freedom for realizing various topological states, e.g., the Weyl point, nodal line, Dirac point, topological insulator, and even the Yang monopole and Weyl surface in higher-dimensional synthetic spaces, wherein each specific topological nontrivial state endows novel metamaterial responses that originate from the feature of some high-energy physics.

    Story Video to the Review Article

    [DB]=[ɛ0ɛiγ/ciζ/cµ0µ][EH].

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    {U=iωL·I+qC+IR,U=dl·Eds·B/t,and{I=q˙=iωq,B/t=iωµ0H,

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    p=q·Sp=q·dlandm=iωq·Sm=I·ds.

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    q=Sp·E+iωµ0Sm·HL·(ω0ω2iωΓ).

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    P=pV=Sp(Sp·E)+iωµ0·Sp(Sm·H)LV·(ω0ω2iωΓ),M=m/V=iωSm(Sp·E)+ω2µ0·Sm(Sm·H)LV·(ω0ω2iωΓ).

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    ɛ=ɛbg·I+SpSpɛ0LV·(ω0ω2iωΓ),µ=µbg·I+(ω/c)2·SmSmɛ0LV·(ω0ω2iωΓ),γ=ζ=(ω/c)·SpSmɛ0LV·(ω0ω2iωΓ).

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    ik×Ψ±=±k0Ψ±,

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    H=kx·λx+ky·λy+kz·λzandHΨ±=±EΨ±,

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    λx=[00000i0i0],λy=[00i000i00],λz=[0i0i00000].

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    C±=12πFk·dS=±2.

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    H=ω0·I+i,jvijkjσi.

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    CWP=sgn[det(v)]=±1.

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    FWP=QWP·kk3.

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    F(k)=+F(k)withIS,F(k)=F(k)with time-reversal symmetry(TRS).

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    {Sp,red=[0,l,0]T,Sm,red=[A,0,0]T,and{Sp,blue=[l,0,0]T,Sm,blue=[0,A,0]T.

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    AWP(x)=ΔkWP(x)[1,1,0]·ax·|kWP,0|/2.

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    H=[v·kzv·(kxiky)Nv·(kx+iky)Nv·kz],NZ.

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    Sp,±=12·[l,±l,0]TandSm,±=[0,0,0]T.

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    HD=ωk0·I+i=13viki·Γi,

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    HY=ωk0·I+i=15viki·Γi,

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    ɛ^=[111ωpω2],µ^=[111ωpω2],γ^=[γxzγyzγxzγyz].

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    γ^Sm,ySm,z·[00cosψ4500sinψ45cosψ45sinψ450]·sinδ45.

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    [(ωγxyσxkzσy)·λ2(ωγzxσxkyσy)·λ5+(ωγyzσxkxσy)·λ7]·ΨEH=ω·12[(σ0+σz)·ɛ0ɛ^+(σ0σz)·µ0µ^]·ΨEH.

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    Sp,±=12·[l,±l,0]TandSm,±=12·[A,A,0]T.

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    Shaojie Ma, Biao Yang, Shuang Zhang. Topological photonics in metamaterials[J]. Photonics Insights, 2022, 1(1): R02
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