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樊丽娜, 沙金巧, 曹召良. 亿博体育登陆[J]. 中国光学(中英文), 2024, 17(2): 493-500. doi: 10.37188/CO.EN-2023-0030
引用本文: 樊丽娜, 沙金巧, 曹召良. 亿博体育登陆[J]. 中国光学(中英文), 2024, 17(2): 493-500. doi: 10.37188/CO.EN-2023-0030
FAN Li-na, SHA Jin-qiao, CAO Zhao-liang. 亿博体育串子[J]. Chinese Optics, 2024, 17(2): 493-500. doi: 10.37188/CO.EN-2023-0030
Citation: FAN Li-na, SHA Jin-qiao, CAO Zhao-liang. 亿博体育串子[J]. Chinese Optics, 2024, 17(2): 493-500. doi: 10.37188/CO.EN-2023-0030

亿博体育登陆

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  • 中图分类号:O436.1;TN25

亿博体育串子

doi: 10.37188/CO.EN-2023-0030
Funds:Supported by Jiangsu Key Disciplines of the Fourteenth Five-Year Plan (No. 2021135); Key Research and De-Velopment Project of the Department of Science and Technology of Jilin Province (No. 20220203033SF)
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    Author Bio:

    Fan Li-na (1980—), female, Yuci city, Shanxi province, Ph.D., received her Ph.D. from the University of Shanghai for Science and Technology in 2020 and is mainly engaged in research on micro-nano optical devices. E-mail: [email protected]

    Corresponding author: [email protected]
  • 摘要:

    本文提出并展示了一种亿博体育登陆。通过优化光栅层厚度,使其能够在支持TE导模的同时抑制TM导模。本文设计的滤波器呈现出可调谐的单一反射峰, 峰值反射率理论上可达100%。当入射角改变时,共振波长可以由642.5 nm调节至484.6 nm。该反射峰是由一级衍射波与TE导模(基模)之间的共振效应所产生的。同样地,通过按比例增加光栅层的厚度和周期可实现应用于更高动态范围的可调谐滤波器。

  • Figure 1. Schematic diagram of 1D RWG in full conical mounting. The structural parameters are n H = 1.8, n L = 1.63, n s = 1.46, n c = 1.0, d = 102 nm, f = 0.5, and Λ = 440 nm

    Figure 2. Calculated reflection spectra with the incident angle variation when the TM-polarized wave irradiates 1D RWG in full conical mounting

    Figure 3. Internal electric field (E y ) profile for (a) λ R = 642.5 nm (θ = 0°); (b) λ R = 578.6 nm (θ = 40°); (c) λ R = 484.6 nm (θ = 80°)

    Figure 4. Calculated resonant positions based on the eigenvalue equation of fundamental TE guided mode at different incident angles

    Figure 5. Calculated resonant positions based on the eigenvalue equation of fundamental TE and TM guided modes at different incident angles

    Figure 6. Reflection spectra of equivalent multilayer stacks at different incident angles. (a) TE-polarized incidence; (b) TM-polarized incidence

    Figure 7. Resonant wavelength as a function of the incident angle

    Figure 8. Resonant wavelength as a function of the k value and the incident angle

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  • 收稿日期: 2023-11-19
  • 修回日期: 2023-12-05
  • 录用日期: 2023-12-29
  • 网络出版日期: 2024-01-09

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