• Photonics Research
  • Vol. 12, Issue 4, 638 (2024)
Jiaju Wu1、†, Jingguang Chen2、†, Xin Qi1, Zhiwei Guo1, Jiajun Wang2, Feng Wu3, Yong Sun1, Yunhui Li1, Haitao Jiang1、4、*, Lei Shi2、5、*, Jian Zi2, and Hong Chen1
Author Affiliations
  • 1MOE Key Laboratory of Advanced Micro-Structured Materials, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 2State Key Laboratory of Surface Physics, Key Laboratory of Micro- and Nano-Photonic Structures (Ministry of Education) and Department of Physics, Fudan University, Shanghai 200433, China
  • 3School of Optoelectronic Engineering, Guangdong Polytechnic Normal University, Guangzhou 510665, China
  • 4e-mail: jiang-haitao@tongji.edu.cn
  • 5e-mail: lshi@fudan.edu.cn
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    DOI: 10.1364/PRJ.515969 Cite this Article Set citation alerts
    Jiaju Wu, Jingguang Chen, Xin Qi, Zhiwei Guo, Jiajun Wang, Feng Wu, Yong Sun, Yunhui Li, Haitao Jiang, Lei Shi, Jian Zi, Hong Chen. Observation of accurately designed bound states in the continuum in momentum space[J]. Photonics Research, 2024, 12(4): 638 Copy Citation Text show less

    Abstract

    Bound states in the continuum (BICs) in artificial photonic structures have received considerable attention since they offer unique methods for the extreme field localization and enhancement of light-matter interactions. Usually, the symmetry-protected BICs are located at high symmetric points, while the positions of accidental BICs achieved by tuning the parameters will appear at some points in momentum space. Up to now, to accurately design the position of the accidental BIC in momentum space is still a challenge. Here, we theoretically and experimentally demonstrate an accurately designed accidental BIC in a two-coupled-oscillator system consisting of bilayer gratings, where the optical response of each grating can be described by a single resonator model. By changing the interlayer distance between the gratings to tune the propagation phase shift related to wave vectors, the position of the accidental BIC can be arbitrarily controlled in momentum space. Moreover, we present a general method and rigorous numerical analyses for extracting the polarization vector fields to observe the topological properties of BICs from the polarization-resolved transmission spectra. Finally, an application of the highly efficient second harmonic generation assisted by quasi-BIC is demonstrated. Our work provides a straightforward strategy for manipulating BICs and studying their topological properties in momentum space.
    H=(ω1κκω2)i(γ1γ1γ2eiφγ1γ2eiφγ2),

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    ω±=ω0±κiγ(1±eiφ),

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    Re(ω±)=ω0±(κ+γsinφ),Im(ω±)=γ(1±cosφ).

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    φ=k0ndcosθ=mπ(mis an integer),

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    q=12πCdk·kϕ(k),

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    S0=|tpptp|2+|tsp|2,S1=|tpptp|2|tsp|2,S2=2Re[(tpptp)tsp*],S3=2Im[(tpptp)tsp*].

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    P(2ω)=vχ(2)(r,ω)[Eloc(r,ω)]2dV.

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    [PxSHPySHPzSH]=2ε0[0000d22d31d31d31d33000d220d22d3100][Ex2Ey2Ez22EyEz2ExEz2ExEy].

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    s+=(00Epu+0)=I0eiϕ0(0010).(B1)

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    s=I0eiϕ0S(0010),(B2)

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    S=C=(rsts00tsrs0000rptp00tprp),(B3)

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    S=(rsstssrsptsptssrsstsprsprpstpsrpptpptpsrpstpprpp).(B4)

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    s=I0eiϕ0S(rsptsprpptpp).(B5)

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    Ed=I0eiϕ0(tsptpp).(B6)

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    Ed·t^=[(t^·s^)tsp+(t^·p^)tpp]I0eiϕ0,(B7)

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    I=I0|(t^·s^)tsp+(t^·p^)tpp|2.(B8)

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    Tp=|(t^·s^)tsp+(t^·p^)tpp|2.(B9)

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    S˜0=Tpp+Tsp=|tpp|2+|tsp|2,S˜1=TppTsp=|tpp|2|tsp|2,S˜2=2Re(tpptsp*),S˜3=2Im(tpptsp*),(B10)

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    S0=|tpptp|2+|tsp|2,S1=|tpptp|2|tsp|2,S2=2Re[(tpptp)tsp*],S3=2Im[(tpptp)tsp*].(B11)

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    ϕsp=12arg(S1+iS2).(B12)

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    φ=ϒ+arctan(tanϕspcosθ).(B13)

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    Jiaju Wu, Jingguang Chen, Xin Qi, Zhiwei Guo, Jiajun Wang, Feng Wu, Yong Sun, Yunhui Li, Haitao Jiang, Lei Shi, Jian Zi, Hong Chen. Observation of accurately designed bound states in the continuum in momentum space[J]. Photonics Research, 2024, 12(4): 638
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