• Advanced Photonics
  • Vol. 1, Issue 4, 046003 (2019)
Evgenii Narimanov*
Author Affiliations
  • Purdue University, School of Electrical and Computer Engineering, Birck Nanotechnology Center, West Lafayette, Indiana, United States
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    DOI: 10.1117/1.AP.1.4.046003 Cite this Article Set citation alerts
    Evgenii Narimanov. Ghost resonance in anisotropic materials: negative refractive index and evanescent field enhancement in lossless media[J]. Advanced Photonics, 2019, 1(4): 046003 Copy Citation Text show less

    Abstract

    We show that dielectric waveguides formed by materials with strong optical anisotropy support electromagnetic waves that combine the properties of propagating and evanescent fields. These “ghost waves” are created in tangent bifurcations that “annihilate” pairs of positive- and negative-index modes and represent the optical analogue of the “ghost orbits” in the quantum theory of nonintegrable dynamical systems. Ghost waves can be resonantly coupled to the incident evanescent field, which then grows exponentially through the anisotropic media—as in the case of negative index materials. As ghost waves are supported by transparent dielectric media, the proposed approach to electromagnetic field enhancement is free from the “curse” of material loss that is inherent to conventional negative index composites.
    kz=±12{(ϵx+ϵy)(ωc)2(1+ϵxϵz)qx2(1+ϵyϵz)qy2±[((ϵxϵy)(ωc)2+(1ϵxϵz)qx2(1ϵyϵz)qy2)2+4(1ϵxϵz)(1ϵyϵz)qx2qy2]12}12,(1)

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    ϵx<ϵz<ϵy,(2)

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    arctan(ϵxϵyϵyϵzϵzϵx)<φ<arctan(ϵyϵzϵzϵx),(3)

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    φarctan(qy/qx)(4)

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    φDarctan(ϵxϵy·ϵyϵzϵzϵx),(5)

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    ωD=c(ϵyϵx)ϵy(ϵzϵx)·qx,(6)

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    ωc=cϵyϵx(qx1ϵxϵz+qyϵyϵz1),(7)

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    kc=1ϵz(ϵyϵx)[ϵx(ϵzϵy)qx2+ϵy(ϵxϵz)qy2+(ϵx+ϵy)(ϵzϵx)(ϵyϵz)qxqy]1/2(8)

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    Szghost=0.(9)

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    Zx=ExHy,(10)

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    Zy=EyHx.(11)

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    Zx=ωckz·ϵz(cqω)2ϵz+(ϵxϵy)·(cqω)2ϵy(cqω)2(ckzω)2,(12)

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    Zy=ωckz·ϵz(cqω)2ϵz(ϵxϵy)·(cqω)2ϵx(cqω)2(ckzω)2,(13)

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    qqx2+qy2.(14)

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    κ0(κ++κ){κ+κ+ϵxϵyϵ0[qx2ϵy+qy2ϵx(ωsc)2]}+κ+κ[(1+ϵxϵ0)qx2+(1+ϵyϵ0)qy2(ϵx+ϵy)(ωsc)2]+{κ+2κ2+ϵxϵyϵ0κ02[qx2ϵy+qy2ϵx(ωsc)2]}=0,(15)

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    κ0=qx2+qy2ϵ0(ωsc)2,(16)

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    κ±=12{(1+ϵxϵz)qx2+(1+ϵyϵz)qy2(ϵx+ϵy)(ωsc)2±[((ϵxϵy)(ωsc)2+(1ϵxϵz)qx2(1ϵyϵz)qy2)2+4(1ϵxϵz)(1ϵyϵz)qx2qy2]12}12.(17)

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    E(r,t)=Eq(x,y)·exp(ikzziωt),(18)

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    B(r,t)=Bq(x,y)·exp(ikzziωt),(19)

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    Eq(x,y)=[ex·cos(qxx)sin(qyy),ey·sin(qxx)cos(qyy),ez·sin(qxx)sin(qyy)],(20)

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    Bq(x,y)=[bx·sin(qxx)cos(qyy),by·cos(qxx)sin(qyy),bz·cos(qxx)cos(qyy)].(21)

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    bx=cω(kzey+iqyez),(22)

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    by=cω(kzex+iqxez),(23)

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    bz=cω(iqyexiqxey),(24)

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    M(exeyez)=0,(25)

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    M[Δx(kz)qxqyikzqxqxqyΔy(kz)ikzqyikzqxikzqyΔz(kz)],(26)

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    Δx(κ)=ϵx(ωc)2qy2kz2,(27)

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    Δy(κ)=ϵy(ωc)2qx2kz2,(28)

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    Δz(κ)=ϵz(ωc)2qx2qy2.(29)

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    det(M)=0,(30)

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    ϵz·kz4[(ϵx+ϵy)·(ωc)2(ϵx+ϵz)·qx2(ϵy+ϵz)·qy2]·kz2+[ϵz(ωc)2qx2qy2][ϵxϵy(ωc)2ϵxqx2ϵyqy2]=0.(31)

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    k±2=12[(ϵx+ϵy)·(ωc)2ϵx+ϵzϵzqx2ϵy+ϵzϵzqy2±D],(32)

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    D=[(ϵxϵy)(ωc)2+ϵzϵxϵzqx2+ϵyϵzϵzqy2]2+4·(ϵxϵz)·(ϵyϵz)ϵz2qx2qy2.(33)

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    D(ωc)=0,(34)

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    ωc=cϵyϵx(1ϵxϵz·qx+ϵyϵz1·qy),(35)

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    kc=1ϵz(ϵyϵx)[ϵx(ϵzϵy)qx2+ϵy(ϵxϵz)qy2+(ϵzϵx)(ϵyϵz)(ϵx+ϵy)qxqy]1/2.(36)

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    k(ω2±)=0.(37)

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    ω2+=cqx2+qy2ϵz,(38)

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    ω2=cqx2ϵy+qy2ϵx.(39)

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    ωc<min(ω2+,ω2),(40)

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    qy=ϵxϵy·ϵyϵzϵzϵx·qx,(41)

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    φDarctanqyqx|ωD=arctanϵxϵy·ϵyϵzϵzϵx,(42)

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    ωD=c(ϵyϵx)ϵy(ϵzϵx)·qx(43)

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    =c(ϵyϵx)ϵx(ϵyϵz)·qy.(44)

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    E(r,t)=Eq(z)·exp(iqxx+iqyyiωt),(45)

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    B(r,t)=Bq(z)·exp(iqxx+iqyyiωt),(46)

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    Eq(z)={(ases+apep)eκ0z,z<0a+e+eκ+z+aeeκz,z>0,(47)

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    Bq(z)={(asbs+apbp)eκ0z,z<0b+b+eκ+z+bbeκz,z>0,(48)

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    es=(qy,qx,0),(49)

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    bs=cω(iκ0qx,iκ0qy,qx2+qy2),(50)

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    ep=[qx,qy,iκ0(qx2+qy2)],(51)

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    bp=iωϵ0cκ0(qy,qx,0),(52)

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    e±={iκ±qx[qy2Δy(κ±)],iκ±qy[qx2Δx(κ±)],Δx(κ±)·Δy(κ±)qx2qy2},(53)

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    b±=ωc{qy[ϵyΔx(κ±)ϵxqx2],qx[ϵxΔy(κ±)ϵyqy2],iqxqyκ±(ϵyϵx)}.(54)

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    ϵzEz(curlB)zqxByqyBx,(55)

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    N(asapa+a)=0,(56)

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    N=[iqyqxiκ+(qy2Δy+)κ(qy2Δy)iqxqyiκ+(qx2Δx+)κ(qx2Δx)0iq2ϵ0κ0ϵzΔx+Δy+qx2qy2ΔxΔyqx2qy2iq2κ0qxqy0(ϵyϵx)ω2κ+2c2(ϵyϵx)ω2κ2c2],(57)

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    Δx,y±Δx,y(κ±).(58)

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    ζ±=(Δx±Δy±qx2qy2)·a±.(59)

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    (α+αβ+β)·(ζ+ζ)=0,(60)

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    α±=ϵzϵ0+κ±κ0(ωc)2(ϵxqy2+ϵyqx2)q2(q2κ±2)Δx±Δy±qx2qy2,(61)

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    β±=κ±·κ0+κ±Δx±Δy±qx2qy2.(62)

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    det(α+αβ+β)=0,(63)

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    κ0(κ++κ)·{ϵxϵyϵ0[(ωc)2qx2ϵyqy2ϵx]κ+κ}+κ+κ[(ϵx+ϵy)(ωc)2ϵ0+ϵxϵ0qx2ϵ0+ϵyϵ0qy2]+{ϵxϵyϵ0κ02[(ωc)2qx2ϵyqy2ϵx]κ+2κ2}=0.(64)

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    Evgenii Narimanov. Ghost resonance in anisotropic materials: negative refractive index and evanescent field enhancement in lossless media[J]. Advanced Photonics, 2019, 1(4): 046003
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