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基于绝缘体上硅的微环谐振器由于成本低、结构紧凑和集成度高等优点, 是构成波分复用器、调制器以及光开关等的核心器件. 然而, 该类器件由于芯层与覆盖层间的高折射率差, 具有较大的偏振相关性, 在诸多使用偏振无关器件的应用中受到限制. 本文基于亚波长光栅和三明治结构设计了一种偏振无关微环谐振器, 通过改变三明治结构中低折射率层SiNx的折射率, 同时结合耦合区亚波长光栅的结构参数优化, 最终消除微环谐振器的偏振相关性. 运用三维有限时域差分法进行建模仿真, 对器件的结构参数进行了优化. 结果表明, 器件在TE和TM偏振模时的3-dB带宽均小于0.8 nm, 插入损耗均小于0.8 dB, 微环半径仅为10 µm, 并且在谐振波长1552.26 nm附近的两个自由频谱区内实现了偏振无关. 与常见的微环谐振器相比, 本文所提出的器件尺寸小、损耗低, 可用于构成偏振无关的密集波分复用器, 在未来的集成光路中具有较高的应用价值.Ring resonator fabricated on a silicon-on-insulator is versatile in optical integration, which can be used to realize filters, modulators and switches. However, silicon-on-insulator is difficult to control the polarization dependence, and thus its application is greatly limited. The polarization dependence of the ring resonator is caused mainly by two factors: the coupling coefficients of the coupling region at the same wavelength for the two orthogonal polarization modes are different, and the birefringence effect of curved waveguide results in the different resonant wavelengths of TE and TM polarization modes. When the coupling region polarization independence and the resonant wavelength polarization independence are simultaneously satisfied, the polarization independence of the ring resonator can be realized. In this paper, a new type of polarization-insensitive ring resonator on a silicon-on-insulator is designed based on subwavelength grating and sandwiched structure. Firstly, by adjusting the duty cycle of the subwavelength grating and the refractive index of SiNx in the coupling region, polarization independence of the coupling region is achieved. Secondly, the refractive index of SiNx in curved waveguides is designed to make the resonance wavelengths for orthogonal polarization modes equal. Thirdly, the parameters of the coupling region are optimized to reduce the insertion loss. The three-dimensional finite-difference time-domain method is used for simulation. The results show that the radius of the ring is only 10 μm, the 3-dB bandwidth of the device is less than 0.8 nm, and the insertion loss is lower than 0.8 dB. It has potential applications in the future dense wavelength division multiplexing systems.
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Keywords:
- microring resonators /
- polarization-insensitive /
- subwavelength grating /
- sandwiched structure
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[14] Chen Y, Joines W T 2003 Opt. Commun. 228 319Google Scholar
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Wang J L, Chen Z Y, Chen H M 2020 Acta Phys. Sin. 69 054206Google Scholar
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Zhang F L, Zhai S, Pan J, Feng J J 2020 Chin. J. Lasers 43 1Google Scholar
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图 1 基于SWG和三明治结构的偏振无关微环谐振器结构示意图 (a) 俯视图; (b) 波导横截面示意图; (c) 基于SWG和三明治结构的耦合区三维结构示意图; (d) 耦合区Si层俯视图; (e) 耦合区SiNx层俯视图
Fig. 1. Schematic configuration of the polarization insensitive ring resonator based on SWG and sandwiched structure: (a) Top view; (b) cross section of the waveguide; (c) three-dimensional schematic configuration of the polarization insensitive coupling region based on subwavelength grating slot waveguides and sandwiched structure; (d) top view of Si layer in coupling region; (e) top view of SiNx layer in coupling region.
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[1] Lee J M, Park S, Kim G 2008 Opt. Commun. 281 4302Google Scholar
[2] Sang-Ngern S, Roeksabutr A 2006 IEEE Asia Pacific Conference on Circuits and Systems Singapore, December 4–7, 2006 p1907
[3] Heyn P D, Coster J D, Verheyem P, Lepage G, Pantouvaki M, Absil P, Bogaerts W, Campenhout J V, Thourhout D V 2013 J. Lightwave Technol. 31 2785Google Scholar
[4] Chao I F, Lee C H, Chung Y H 2019 4th International Conference on Intelligent Green Building and Smart Grid (IGBSG) Yichang, China, September 6–9, 2019 p30
[5] Kudo M, Ohta S, Taguchi E, Fujisawa T, Sakamoto T, Matsui T, Tsujikawa K, Nakajima K, Saitoh K 2019 Opt. Commun. 433 168Google Scholar
[6] Balaji V R, Murugan M, Robinson S 2016 International Conference on Wireless Communications, Signal Processing and Networking (WiSPNET) Chennai, India, March 23–25, 2016 p33
[7] Libertino S, Coffa S, Saggio M 2000 Mater. Sci. Semicond. Process. 3 375Google Scholar
[8] Vlasov Y, Mcnab S 2004 Opt. Express 12 1622Google Scholar
[9] Xu Q F, Fattal D, Beausoleil R G 2008 Opt. Express 16 4309Google Scholar
[10] Barwicz T, Watts M R, Popovi M A, Rakich P T, Socci L, Krtner F X, Ippen E P, Smith H I 2007 Nat. Photonics 1 57Google Scholar
[11] Xu D X, Janz S, Cheben P 2006 IEEE Photonics Technol. Lett. 18 343Google Scholar
[12] Geng M M 2016 Laser Optoelectron. Prog. 53 182Google Scholar
[13] Wang X D, Li Y Q, Quan X L, Cheng X L 2019 Conference on Lasers and Electro-Optics (CLEO) Munich, Germany, June 23–27, 2019 JTh2 A.64
[14] Chen Y, Joines W T 2003 Opt. Commun. 228 319Google Scholar
[15] Kaalund C J 2004 Opt. Commun. 237 357Google Scholar
[16] Little B E, Chu S T, Haus H A, Foresi J, Laine J P 1997 J. Lightwave Technol. 15 998Google Scholar
[17] Lee C C, Chen H L, Hsu J C, Tien C L 1999 Appl. Opt. 38 2078Google Scholar
[18] 邹祥云, 苑进社, 蒋一祥 2012 物理学报 61 148106Google Scholar
Zou X Y, Yuan J S, Jiang Y X 2012 Acta Phys. Sin. 61 148106Google Scholar
[19] 汪静丽, 陈子玉, 陈鹤鸣 2020 物理学报 69 054206Google Scholar
Wang J L, Chen Z Y, Chen H M 2020 Acta Phys. Sin. 69 054206Google Scholar
[20] Shi Y J, Shang H P, Sun D G 2018 Opt. Commun. 410 211Google Scholar
[21] 张福领, 翟珊, 潘俊, 冯吉军 2020 中国激光 43 1Google Scholar
Zhang F L, Zhai S, Pan J, Feng J J 2020 Chin. J. Lasers 43 1Google Scholar
[22] 柳襄怀, 薛滨, 郑志宏, 周祖尧, 邹世昌 1989 半导体学报 1989 457Google Scholar
Liu X H, Xue B, Zheng Z H, Zhou Z Y, Zhou S Z 1989 J. Semicond. 1989 457Google Scholar
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