• Chinese Optics Letters
  • Vol. 17, Issue 1, 012501 (2019)
Zhengyang Bai1, Qi Zhang1, and Guoxiang Huang1、2、*
Author Affiliations
  • 1State Key Laboratory of Precision Spectroscopy, School of Physics and Material Science, East China Normal University, Shanghai 200062, China
  • 2NYU-ECNU Joint Institute of Physics at NYU-Shanghai, Shanghai 200062, China
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    DOI: 10.3788/COL201917.012501 Cite this Article Set citation alerts
    Zhengyang Bai, Qi Zhang, Guoxiang Huang. Nonlinear polaritons in metamaterials with plasmon-induced transparency [Invited][J]. Chinese Optics Letters, 2019, 17(1): 012501 Copy Citation Text show less

    Abstract

    Electromagnetically induced transparency (EIT), a typical quantum interference effect, has been extensively investigated in coherent atomic gases. In recent years, it has been recognized that the plasmonic analog of atomic EIT, called plasmon-induced transparency (PIT), is a fruitful platform for the study of EIT-like propagation and interaction of plasmonic polaritons. Many proposals have been presented for realizing PIT in various metamaterials, which possess many unique characters, including the suppression of absorption of electromagnetic radiation, the reduction of propagation velocity, etc. Especially, nonlinear PIT metamaterials, obtained usually by embedding nonlinear elements into meta-atoms, can be used to acquire an enhanced Kerr effect resulted from the resonant coupling between radiation and the meta-atoms and to actively manipulate structural and dynamical properties of plasmonic metamaterials. In this article, we review recent research progress in nonlinear PIT metamaterials, and elucidate their interesting properties and promising applications. In particular, we give a detailed description on the propagation and interaction of nonlinear plasmonic polaritons in metamaterials via PIT, which are promising for chip-scale applications in information processing and transmission.
    q¨1+γ1q˙1+ω02q1κ2q2=gE(r,t),(1)

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    q¨2+γ2q˙2+(ω0+Δ)2q2κ2q1=0,(2)

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    2E1c22Et2=1ε0c22Pt2,(3)

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    K=nDcδ+κ0gD2(δ)D1(δ)D2(δ)κ4.(4)

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    q¨2+γ2q˙2+(ω0+Δ)2q2κ2q1+αq22+βq23=0,(5)

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    iFz212K22Fτ12+c2ω0nD(2x12+2y12)F+ω02cnDχ(3)|F|2Fe2α¯z2+m1ω02cnDχ(2)GF=0.(6)

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    χ(2)=2Neg2κ6αϵ0(ω04κ4)|D1(δ)D2(δ)κ4|2,(7)

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    χ(3)=[4α2ω02ω04κ4+2α2D1(2δ)D1(2δ)D2(2δ)κ43β]×g3κ8Neϵ0[D1(δ)D2(δ)κ4]2|D1(δ)D2(δ)κ4|2.(8)

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    (2x12+2y12)G(1Vp21Vg2)2Gτ12χ(2)c22|F|2τ12e2α¯z2=0,(9)

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    χeff(3)=χ(3)+χSL(3),(10)

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    χSL(3)=m1(χ(2))2c2(1Vp21Vg2),(11)

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    i(z+α1)U12K22Uτ2W|U|2U=0,(12)

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    (it+d31)σ31+Ωc1σ21+Ωp1=0,(13a)

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    (it+d41)σ41+Ωc2σ21+Ωp2=0,(13b)

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    (it+d21)σ21+Ωc1*σ31+Ωc2*σ41=0,(13c)

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    i(z+1ct)Ωp1+κ13σ31=0,(13d)

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    i(z+1ct)Ωp2+κ14σ41=0,(13e)

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    Ka±(ω)=ωc+(κ14D3+κ13D4)±(κ14D3κ13D4)2+4κ13κ14|Ωc1Ωc2|22[|Ωc1|2(ω+d41)+|Ωc2|2(ω+d31)(ω+d21)(ω+d31)(ω+d41)].(14)

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    2q1t2+γ1q1t+ω12q1κ1q3=g1Ex,(15a)

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    2q2t2+γ2q2t+ω22q2κ2q3=g2Ey,(15b)

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    2q3t2+γ3q3t+ω32q3κ1q1κ2q2=0,(15c)

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    (it+d1)q˜1+κ12ωpq˜3+g12ωpEx=0,(16a)

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    (it+d2)q˜2+κ22ωpq˜3+g22ωpEy=0,(16b)

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    (it+d3)q˜3+κ12ωpq˜1+κ22ωpq˜2=0,(16c)

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    i(z+nDct)Ex+κ0q˜1=0,(16d)

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    i(z+nDct)Ey+κ0q˜2=0,(16e)

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    Km±(ω)=nDcω+κ0(R1gf2+R2gf1)±(R1gf2R2gf1)2+4κf12κf22gf1gf22[κf12(ω+d2)+κf22(ω+d1)(ω+d3)(ω+d1)(ω+d2)],(17)

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    η(L)=|G0+G0|2|G0+G0|2|exp(iK0+L)|2.(18)

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    2q3t2+γ3q3t+ω32q3κ2q1κ2q2+αq32+βq33=0,(19)

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    E(r,t)exκ1+eyκ2κ12+κ22[(Ueikpziωpt+c.c.)]+V,(20)

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    Ld2q+dt2+rdq+dt+q+CCMC02cos(ωct+ϕ)q=2El,(21a)

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    Ld2qdt2+rtdqdt+qC0CMC02cos(ωct+ϕ)q+=0,(21b)

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    dq˜+dt=(γ+iΔ)q˜++igE+iΩceiϕq˜,(22a)

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    dq˜dt=[γt+i(Δδ)]q˜+iΩceiϕq˜+,(22b)

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    i(z+nDct)E+12kp2E+κ0q˜+=0,(23)

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    E(r,t)=m,pump(r,φ,z)Emp(z,t),(24)

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    ump(r,φ)=Cmpw0(2rw0)|m|exp(r2w02)×Lp|m|(2r2w02)exp(imφ).(25)

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    q˜+(r,t)=m,pq˜+mp(z,t)ump(r,φ),(26a)

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    q˜(r,t)=m,pq˜mp(z,t)ump(r,φ),(26b)

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    [t+cnDcos2θ(t)z]Pmp(z,t)=0,(27)

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    Zhengyang Bai, Qi Zhang, Guoxiang Huang. Nonlinear polaritons in metamaterials with plasmon-induced transparency [Invited][J]. Chinese Optics Letters, 2019, 17(1): 012501
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