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氮化镓光波导的损耗特性分析与工艺优化研究

尹慧萍 李文迪 冯萧萧 秦飞飞 施政 王永进 李欣

尹慧萍, 李文迪, 冯萧萧, 秦飞飞, 施政, 王永进, 李欣. 氮化镓光波导的损耗特性分析与工艺优化研究[J]. 中国光学(中英文). doi: 10.37188/CO.2024-0188
引用本文: 尹慧萍, 李文迪, 冯萧萧, 秦飞飞, 施政, 王永进, 李欣. 氮化镓光波导的损耗特性分析与工艺优化研究[J]. 中国光学(中英文). doi: 10.37188/CO.2024-0188
YIN Hui-ping, LI Wen-di, FENG Xiao-xiao, QIN Fei-fei, SHI Zheng, WANG Yong-jin, LI Xin. Loss characteristics analysis and process optimization of gallium nitride optical waveguide[J]. Chinese Optics. doi: 10.37188/CO.2024-0188
Citation: YIN Hui-ping, LI Wen-di, FENG Xiao-xiao, QIN Fei-fei, SHI Zheng, WANG Yong-jin, LI Xin. Loss characteristics analysis and process optimization of gallium nitride optical waveguide[J]. Chinese Optics. doi: 10.37188/CO.2024-0188

氮化镓光波导的损耗特性分析与工艺优化研究

cstr: 32171.14.CO.2024-0188
基金项目: 国家自然科学基金(No. 62274096,No. 62204127);江苏省高等学校基础科学(自然科学)研究重大项目(No. 22KJA510003);江苏省自然科学基金(No. BK20210593)
详细信息
    作者简介:

    尹慧萍(2001—),女,硕士研究生,2022年于南京邮电大学获得学士学位,现为南京邮电大学通信与信息工程学院硕士,主要从事III族氮化物光电子器件和可见光通信方面的研究。E-mail:1222014634@njupt.edu.cn

    李 欣(1984—),女,博士,2013年于西安交通大学获得博士学位,现为南京邮电大学通信与信息工程学院副教授,主要从事III族氮化物光电子器件和可见光通信方面的研究。E-mail:lixin1984@njupt.edu.cn

  • 中图分类号: TN929.1

Loss characteristics analysis and process optimization of gallium nitride optical waveguide

Funds: Supported by National Natural Science Foundation of China (No. 62274096, No. 62204127), Key Project of the Natural Science Foundation of the Jiangsu Higher Education Institutions of China (No. 22KJA510003) and Jiangsu Province Natural Science Foundation (No. BK20210593)
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  • 摘要:

    本文利用基于光束传播方法(Beam Propagation Method,BPM)的有限元仿真模型研究了氮化镓(GaN)平面光波导的传输损耗特性,针对传统GaN波导损耗较大的问题提出了工艺优化方案。通过构建完整的传输损耗模型,系统分析了波导几何参数对传输特性的影响,重点研究了顶部刻蚀和背后减薄两种优化工艺的改善效果。研究表明,这两种工艺均可显著降低波导传输损耗:顶部刻蚀工艺可将损耗从2.29 dB/mm降至0.19 dB/mm,背后减薄工艺可降至0.24 dB/mm。此外,本文还量化分析了制造工艺引入的侧壁夹角和表面粗糙度等缺陷对传输损耗的影响,并通过参数优化确定了实现可见光单模传输的关键结构尺寸。研究成果为设计和制备低损耗GaN平面光波导提供了理论依据和工艺指导。

     

  • 图 8  氮化镓波导的光场传输模式分析(波导横截面)(a) 初始模型,(b) 顶部刻蚀工艺去除平板层,(c) 背后减薄工艺去除平板层,(d) 波导宽度150 nm高度100 nm实现单模传输,(e) 波导宽度100 nm高度150 nm实现单模传输

    Figure 8.  Analysis of light field transmission mode of GaN waveguide (waveguide cross section) (a) initial model, (b) top etching process removes the flat layer, (c) back thinning process removes the flat layer, (d) single-mode transmission achieved by waveguide width 150 nm and height 100 nm, (e) single-mode transmission with waveguide width 100 nm and height 150 nm

    图 1  (a) 顶部刻蚀GaN平面光波导的加工流程图,(b) 背后减薄GaN平面光波导的加工流程图,(c) 两种GaN平面光波导的横截面示意图

    Figure 1.  (a) the processing flow chart of the etched GaN planar optical waveguide at the top, (b) the processing flow chart of the thinned GaN planar optical waveguide at the back, and (c) the cross-sectional diagram of the two types of GaN planar optical waveguide

    图 2  初始模型下GaN平面光波导的折射率分布图

    Figure 2.  Refractive index distribution of GaN planar optical waveguides under the initial model

    图 3  GaN平面光波导的相对光功率分布(波导传输方向)(a) 初始模型,(b) 顶部刻蚀工艺去除脊型波导下方平板层,(c) 背后减薄工艺去除脊型波导下方平板层

    Figure 3.  Relative light output distribution of GaN planar optical waveguide (waveguide transmission direction) (a) initial model, (b) top etching process removes the lower flat layer of ridge waveguide, and (c) back thinning process removes the lower flat layer of ridge waveguide

    图 4  两种不同工艺下随平板层厚度变化的氮化镓波导传输损耗

    Figure 4.  GaN waveguide transmission loss with plate thickness under two different processes

    图 5  两种不同工艺下随侧壁夹角变化的氮化镓波导传输损耗

    Figure 5.  GaN waveguide transmission loss as a function of sidewall angle for two different processes

    图 6  两种不同工艺下随粗糙度变化的氮化镓波导传输损耗

    Figure 6.  Transmission loss of GaN waveguide as a function of roughness for two different processes

    图 7  两种不同工艺下随波导宽度变化的氮化镓波导传输损耗

    Figure 7.  GaN waveguide transmission loss as a function of waveguide width for two different processes

    图 9  两种不同工艺下随可见光信号的波长变化的氮化镓波导传输损耗

    Figure 9.  The GaN waveguide transmission loss as a function of the wavelength of the visible light signal under two different processes

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出版历程
  • 收稿日期:  2024-10-10
  • 录用日期:  2024-12-17
  • 网络出版日期:  2025-02-26

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