• Photonics Research
  • Vol. 5, Issue 2, 113 (2017)
Yong-Pan Gao1, Tie-Jun Wang1, Cong Cao2, and Chuan Wang1、*
Author Affiliations
  • 1State Key Laboratory of Information Photonics and Optical Communications and School of Science, Beijing University of Posts and Telecommunications, Beijing 100876, China
  • 2School of Ethnic Minority Education, Beijing University of Posts and Telecommunications, Beijing 100876, China
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    DOI: 10.1364/PRJ.5.000113 Cite this Article Set citation alerts
    Yong-Pan Gao, Tie-Jun Wang, Cong Cao, Chuan Wang. Gap induced mode evolution under the asymmetric structure in a plasmonic resonator system[J]. Photonics Research, 2017, 5(2): 113 Copy Citation Text show less

    Abstract

    The modulation of resonance features in microcavities is important to applications in nanophotonics. Based on the asymmetric whispering-gallery modes (WGMs) in a plasmonic resonator, we theoretically studied the mode evolution in an asymmetric WGM plasmonic system. Exploiting the gap or nano-scatter in the plasmonic ring cavity, the symmetry of the system will be broken and the standing wave in the cavity will be tunable. Based on this asymmetric structure, the output coupling rate between the two cavity modes can also be tuned. Moreover, the proposed method could further be applied for sensing and detecting the position of defects in a WGM system.
    H=ω(acwacw+accwaccw)+g(accwacw+acwaccw+acwacw+accwaccw),(1)

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    dacwdt=1i[acw,H]κ0+κout2acwκinacwin,(2)

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    daccwdt=1i[accw,H]κ0+κout2accwκinaccwin.(3)

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    dacwdt=i[(ω+g)acw+gaccw]κ0+κout2acwκinacwin,(4)

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    daccwdt=i[(ω+g)accw+gacw]κ0+κout2accwκinaccwin.(5)

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    g=αf2(r)ω2Vc,α=Vpϵpϵmϵp+2ϵm.(6)

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    [i(Δ2g)+κout+κ02]a++κina+in=0,(7)

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    (iΔ+κout+κ02)a+κinain=0,(8)

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    t=1κout(λ,θ)κinββ2+g2,β=i(Δg)+κ0+κout2.(9)

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    t=1ϕ(λ,θ)κinββ2+g2.(10)

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    E(θ)=E0sin(θ+φ1(θscatter)+φ2(λ)).(11)

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    ××Eμεk2E=0,E(x,y,z)=E(x,y)eikzz.(12)

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    E(θ)=E0sin(θ+θscatter+107πλ2+0.15),(13)

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    ϕ(θ,λ)=sin(θ+θscatter+πλ1072+0.15).(14)

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    T=|1ϕ(λ,θ)κinββ2+g2|2,β=i(Δ+g)+κ0+κout2,ϕ(θ,λ)=sin(θ+θscatter+πλ1072+0.15).(15)

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    Yong-Pan Gao, Tie-Jun Wang, Cong Cao, Chuan Wang. Gap induced mode evolution under the asymmetric structure in a plasmonic resonator system[J]. Photonics Research, 2017, 5(2): 113
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