• Chinese Optics Letters
  • Vol. 21, Issue 1, 010003 (2023)
Wanxia Huang*, Yabo Zhang, Yuan Pei, Maosheng Wang, Fenghua Shi, and Kuanguo Li
Author Affiliations
  • Anhui Key Laboratory of Optoelectric Materials Science and Technology, School of Physics and Electronic Information, Anhui Normal University, Wuhu 241002, China
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    DOI: 10.3788/COL202321.010003 Cite this Article Set citation alerts
    Wanxia Huang, Yabo Zhang, Yuan Pei, Maosheng Wang, Fenghua Shi, Kuanguo Li. Effects of propagation phase on the coupling of plasmonic optical modes[J]. Chinese Optics Letters, 2023, 21(1): 010003 Copy Citation Text show less

    Abstract

    The temporal coupled-mode theory (TCMT) has made significant progress in recent years, and is widely applied in explaining a variety of optical phenomena. In this paper, the optical characteristics of the metasurface composed of nano-bars and nano-rings are simulated. The simulation results are well explained by TCMT under the coupled basis vector. However, when the structural asymmetry is large, the fitting of results shows that the total radiation loss is not conservative, in contradiction to the requirement of traditional TCMT. We solved this inconsistency by introducing the propagation phase into the near-field coupling term of TCMT. The studies show that, unlike the local mode near the exceptional point which corresponds to the radiation loss of the bright mode, the global mode near the diabolic point is closely related to the propagation phase. Furthermore, the structure near the diabolic point shows characteristic cross-coupling with the change of period. This study proposes a new theoretical framework for comprehending the interaction of light and matter and offers some guiding implications for the application of TCMT to a variety of related domains.
    A=1TR.

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    H^0|Ψp=2πfp|Ψp,

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    H^0|Ψq=2πfq|Ψq,

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    12πddt(apaq)=i[(fp+κppκpqκqpfq+κqq)i(γp00γq)](apaq)(γp000)(apaq)+(kp1kp200)(S1+S2+),

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    (S1S2)=(S110S120S210S220)(S1+S2+)+(d1p0d2p0)(apaq),

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    S120=S210=2nn+1,S220=S110=n1n+1.

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    f˜=f¯Δf˜.

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    M=(ΔfΔf˜(ΔfΔf˜)2+κpq2Δf+Δf˜(Δf+Δf˜)2+κpq2κpq(ΔfΔf˜)2+κpq2κpq(Δf+Δf˜)2+κpq2).

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    12πddt(a˜+a˜)=i(f˜+00f˜)(a˜+a˜)+(γ˜++γ˜+X˜X˜γ˜+γ˜)(a˜+a˜)+(k˜+1k˜+2k˜1k˜2)(S10+S20+).

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    (S10S20)=(S110S120S210S220)(S10+S20+)+(d˜1+d˜1d˜2+d˜2+)(a˜+a˜).

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    X˜=κpqγp/(2Δf˜),

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    γ˜=γp(Δf˜+Δf)/2Δf˜,

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    γ˜+=γp(Δf˜Δf)/2Δf˜,

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    γ˜=γp+γq2(γqγp)Δf2Δf˜,

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    γ˜+=γp+γq2+(γqγp)Δf2Δf˜.

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    γ˜++γ˜=γp,

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    γ˜++γ˜=γp+γq.

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    κpq=f˜+f˜2γp(γp+γ˜+γ˜)(γpγ˜++γ˜),

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    κqq=[f˜++f˜fpfq+f˜+f˜γp(γ˜γ˜+)]/2,

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    κpp=[f˜++f˜fpfqf˜+f˜γp(γ˜γ˜+)]/2.

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    t=2nn+12nn+1(γ˜W˜+γ˜+W˜+2γ˜γ˜+W˜W˜+)/(1γ˜γ˜+W˜W˜+),

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    12πddt(apaq)=i[(fp+κppeiακpqeiβκpqeiβfq+κqqeiα)i(γp00γq)](apaq)(γp000)(apaq)+(kp1kp2kq1kq2)(S10+S20+)=i[(fp+κppcosακpqcosβκpqcosβfq+κqqcosα)i(γp00γq)](apaq)(γp+κppsinακpqsinβκpqsinβκqqsinα)(apaq)+(kp1kp2kq1kq2)(S10+S20+),

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    f˜=f¯Δf˜.

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    M˜=(Δf+Δf˜2κpqΔf+Δf˜2κpq11).

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    (γ˜X˜X˜γ˜+)M1(γp+κppsinακpqsinβκpqsinβκqqsinα)M=(B11B12B21B22),

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    B11=Δf(γp+κppsinακqqsinα)+Δf˜(γp+κppsinα2κpqsinβ+κqqsinα)2Δf˜,

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    B12=κpqcosβ(γpκppsinα+κqqsinα)2Δf˜,

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    B21=κpqcosβ(γpκppsinα+κqqsinα)Δf˜2Δfsinβcosβ,

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    B22=Δf(γpκppsinα+κqqsinα)+Δf˜(γp+κppsinα+2κpqsinβ+κqqsinα)2Δf˜.

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    2Δfsinβcosβ=0.

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    γ˜+=(γpγq)Δf2Δf˜+γp+γq2,

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    γ˜=γp+γq2(γpγq)Δf2Δf˜.

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    γ˜++γ˜=γp+κppsinα+κqqsinα,

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    γ˜++γ˜=γp+γq.

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    tanα=γ˜++γ˜γpf˜+f˜+fpfq.

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    κpp=12[γ˜++γ˜γpsinαγpcosα(γpcosα)24sinαcosα(γ˜γ˜+)(f˜+f˜)2sinαcosα],

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    κqq=12[γ˜++γ˜γpsinα+γpcosα(γpcosα)24sinαcosα(γ˜γ˜+)(f˜+f˜)2sinαcosα],

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    κpq=12{(f˜f˜+)2[γpcosα(γpcosα)24sinαcosα(γ˜γ˜+)(f˜f˜+)2sinα]2}0.5.

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    Wanxia Huang, Yabo Zhang, Yuan Pei, Maosheng Wang, Fenghua Shi, Kuanguo Li. Effects of propagation phase on the coupling of plasmonic optical modes[J]. Chinese Optics Letters, 2023, 21(1): 010003
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