Phase-matched second-harmonic generation in hybrid polymer-LN waveguides

doi:10.1088/1674-1056/ac6edc

中国物理B ›› 2022, Vol. 31 ›› Issue (10): 104208-104208.doi: 10.1088/1674-1056/ac6edc

所属专题： SPECIAL TOPIC — Optical field manipulation

• SPECIAL TOPIC—Optical field manipulation • 上一篇下一篇

Phase-matched second-harmonic generation in hybrid polymer-LN waveguides

Zijie Wang(王梓杰)¹, Bodong Liu(刘伯东)¹, Chunhua Wang(王春华)^2,†, and Huakang Yu(虞华康)^1,3,‡

1. School of Physics and Optoelectronics, South China University of Technology, Guangzhou 510641, China;
2. School of Electrical Engineering and Intelligentization, Dongguan University of Technology, Dongguan 523808, China;
3. China-Singapore International Joint Research Institute, Guangzhou Knowledge City, Guangzhou 510663, China

收稿日期:2022-02-23 修回日期:2022-04-22 出版日期:2022-10-16 发布日期:2022-09-24
通讯作者: Chunhua Wang, Huakang Yu E-mail:wangch0515@163.com;hkyu@scut.edu.cn
基金资助:
Project supported by the National Natural Science Foundation of China (Grant Nos. 91850107 and 12174116), the National Key Research and Development Program of China (Grant No. 2018YFA0306200), Guangdong Innovative and Entrepreneurial Research Team Program (Grant No. 2016ZT06C594), the Key Program of Guangzhou Scientific Research Special Project (Grant No. 201904020013), the Science and Technology Project of Guangdong Province, China (Grant No. 2020B010190001), and the Fundamental Research Funds for the Central Universities.

Phase-matched second-harmonic generation in hybrid polymer-LN waveguides

Zijie Wang(王梓杰)¹, Bodong Liu(刘伯东)¹, Chunhua Wang(王春华)^2,†, and Huakang Yu(虞华康)^1,3,‡

1. School of Physics and Optoelectronics, South China University of Technology, Guangzhou 510641, China;
2. School of Electrical Engineering and Intelligentization, Dongguan University of Technology, Dongguan 523808, China;
3. China-Singapore International Joint Research Institute, Guangzhou Knowledge City, Guangzhou 510663, China

Received:2022-02-23 Revised:2022-04-22 Online:2022-10-16 Published:2022-09-24
Contact: Chunhua Wang, Huakang Yu E-mail:wangch0515@163.com;hkyu@scut.edu.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant Nos. 91850107 and 12174116), the National Key Research and Development Program of China (Grant No. 2018YFA0306200), Guangdong Innovative and Entrepreneurial Research Team Program (Grant No. 2016ZT06C594), the Key Program of Guangzhou Scientific Research Special Project (Grant No. 201904020013), the Science and Technology Project of Guangdong Province, China (Grant No. 2020B010190001), and the Fundamental Research Funds for the Central Universities.

摘要/Abstract

摘要： Here we propose a hybrid polymer-LN waveguide for achieving phase-matched second-harmonic generation (SHG). From the aspect of super-mode theory, the geometric parameters of the hybrid semi-nonlinear waveguide were optimized to utilize both symmetric (even) and antisymmetric (odd) modes of the pump and SHG waves so as to facilitate phase matching with large modal overlap. Phase matching between a fundamental even (TE₀₀-like) mode at 1320 nm and a fundamental odd (TE₀₁-like) mode at 660 nm was found with a calculated modal overlap integral of 0.299, while utilizing the largest nonlinear coefficient d₃₃, and achieving an efficient calculated normalized conversion efficiency of 148% W^-1·cm^-2. Considering the fabrication feasibility of such hybrid waveguide with features including etchless, large dimension, and low structural sensitivity, we believe our findings would provide a useful reference for future on-chip efficient nonlinear conversion devices.

关键词: nonlinear waveguides, super-mode theory, phase matching, second harmonic generation

Abstract: Here we propose a hybrid polymer-LN waveguide for achieving phase-matched second-harmonic generation (SHG). From the aspect of super-mode theory, the geometric parameters of the hybrid semi-nonlinear waveguide were optimized to utilize both symmetric (even) and antisymmetric (odd) modes of the pump and SHG waves so as to facilitate phase matching with large modal overlap. Phase matching between a fundamental even (TE₀₀-like) mode at 1320 nm and a fundamental odd (TE₀₁-like) mode at 660 nm was found with a calculated modal overlap integral of 0.299, while utilizing the largest nonlinear coefficient d₃₃, and achieving an efficient calculated normalized conversion efficiency of 148% W^-1·cm^-2. Considering the fabrication feasibility of such hybrid waveguide with features including etchless, large dimension, and low structural sensitivity, we believe our findings would provide a useful reference for future on-chip efficient nonlinear conversion devices.

Key words: nonlinear waveguides, super-mode theory, phase matching, second harmonic generation

中图分类号: (Nonlinear waveguides)

42.65.Wi

42.82.-m (Integrated optics) 52.35.Mw (Nonlinear phenomena: waves, wave propagation, and other interactions (including parametric effects, mode coupling, ponderomotive effects, etc.)) 42.65.-k (Nonlinear optics)

Zijie Wang(王梓杰), Bodong Liu(刘伯东), Chunhua Wang(王春华), and Huakang Yu(虞华康). Phase-matched second-harmonic generation in hybrid polymer-LN waveguides[J]. 中国物理B, 2022, 31(10): 104208-104208.

Zijie Wang(王梓杰), Bodong Liu(刘伯东), Chunhua Wang(王春华), and Huakang Yu(虞华康). Phase-matched second-harmonic generation in hybrid polymer-LN waveguides[J]. Chin. Phys. B, 2022, 31(10): 104208-104208.

参考文献

[1] Boyd R W 2003 Nonlinear Optics, 3rd edn. (New York: Academic Press) pp. 96—104
[2] Shen Y R 1984 The principles of nonlinear optics (New York: John Wiley & Sons) pp. 14—35
[3] Alibart O, D'Auria V, De Micheli M, Doutre F, Kaiser F, Labonte L, Lunghi T, Picholle E and Tanzilli S 2016 J. Opt. 18 104001
[4] Guo X, Ying Y B and Tong L M 2014 Acc. Chem. Res. 47 656
[5] Koos C, Vorreau P, Vallaitis T, Dumon P, Bogaerts W, Baets R, Esembeson B, Biaggio I, Michinobu T, Diederich F, Freude W and Leuthold J 2009 Nat. Photon. 3 216
[6] Subbaraman H, Xu X, Hosseini A, Zhang X, Zhang Y, Kwong D and Chen R T 2015 Opt. Express 23 2487
[7] Moss D J, Morandotti R, Gaeta A L and Lipson M 2013 Nat. Photon. 7 597
[8] Hui H, Jin Y, Li G and Sohler W 2012 Proc. SPIE 8431 84311D
[9] Boes A, Corcoran B, Chang L, Bowers J and Mitchell A 2018 Laser Photon. Rev. 12 1700256
[10] Kong Y F, Bo F, Wang W W, Zheng D H and Xu J J 2020 Adv. Mater. 32 1806452
[11] Lin J T, Bo F, Cheng Y and Xu J J 2020 Photon. Res. 8 1910
[12] Hu X P, Xu P and Zhu S N 2013 Photon. Res. 1 171
[13] Ma F, Liang L Y, Chen J P, Gao Y, Zheng M Y, Xie X P, Liu H, Zhang Q and Pan J W 2018 J. Opt. Soc. Am. B - Opt. Phys. 35 2096
[14] Rao S V, Moutzouris K and Ebrahimzadeh M 2004 J. Opt. A-Pure. Appl. Opt. 6 569
[15] Fiore A, Janz S, Delobel L, Vander Meer P, Bravetti P, Berger V, Rosencher E and Nagle J 1998 Appl. Phys. Lett. 72 2942
[16] Foster M A, Turner A C, Michal L and Gaeta A L 2008 Opt. Express 16 1300
[17] Lin J T, Yao N, Hao Z Z, Zhang J H, Mao W B, Wang M, Chu W, Wu R B, Fang Z and Qiao L 2019 Phys. Rev. Lett. 122 173903
[18] Wang L, Wang C, Wang J, Fang B, Zhang M, Gong Q, Marko L and Xiao Y F 2018 Opt. Lett. 43 2917
[19] Liang H X, Luo R, He Y, Jiang H W and Lin Q 2017 Optica 4 1251
[20] Fang Z W, Yao N, Wang M, Lin J T, Zhang J H, Wu R B, Qiao L L, Fang W, Lu T and Cheng Y 2017 Int. J. Optomechatron. 11 47
[21] Lin Z, Liang X, Loncar M, Johnson S G and Rodriguez A W 2016 Optica 3 233
[22] Lin J T, Xu Y X, Ni J L, Wang M, Fang Z W, Qiao L L, Fang W and Cheng Y 2016 Phys. Rev. Appl. 6 014002
[23] Guo X, Zou C L and Tang H X 2016 Optica 3 1126
[24] Guo X, Zou C L, Jung H and Tang H X 2016 Phys. Rev. Lett. 117 123902
[25] Kuo P S, Bravo-Abad J and Solomon G S 2014 Nat. Commun. 5 4109
[26] Buckley S, Radulaski M, Biermann K and Vukovi J 2013 Appl. Phys. Lett. 103 211117
[27] Pernice W, Xiong C, Schuck C and Tang H X 2012 Appl. Phys. Lett. 100 153901
[28] Levy J S, Foster M A, Gaeta A L and Lipson M 2011 Opt. Express 19 11415
[29] Wang L, Zhang X Q and Chen F 2021 Laser Photon. Rev. 15 2100409
[30] Luo R, He Y, Liang H, Li M and Lin Q 2019 Laser Photon. Rev. 13 1800288
[31] Yu Z J, Xi X, Ma J W, Tsang H K and Sun X K 2019 Optica 6 1342
[32] Zou C L, Cui J M, Sun F W, Xiong X, Zou X B, Han Z F and Guo G C 2015 Laser Photon. Rev. 9 114
[33] Yu Y, Yu Z J, Wang L and Sun X K 2021 Adv. Opt. Mater. 9 2100060
[34] Fang B, Gao S L, Wang Z Z, Zhu S N and Li T 2021 Chin. Opt. Lett. 19 060004
[35] Haus H A, Huang W P and Snyder A W 1989 Opt. Lett. 14 1222
[36] Kapon E, Katz J and Yariv A 1984 Opt. Lett. 9 125
[37] Snyder A W and Young W R 1978 J. Opt. Soc. Am. 68 297
[38] Liu B D, Yu H K, Li Z Y and Tong L M 2019 J. Opt. Soc. Am. B - Opt. Phys. 36 2650
[39] Dong P, Upham J, Jugessur A and Kirk A G 2006 Opt. Express 14 2256
[40] Dong P and Kirk A G 2004 Phys. Rev. Lett. 93 133901
[41] Luo R, He Y, Liang H X, Li M X and Lin Q 2018 Optica 5 1006
[42] Zhu C Y, Chen Y P, Li G Z, Ge L C, Zhu B, Hu M N and Chen X F 2017 Chin. Opt. Lett. 15 091901

Phase-matched second-harmonic generation in hybrid polymer-LN waveguides

Phase-matched second-harmonic generation in hybrid polymer-LN waveguides

RichHTML

PDF (PC)

赞

可视化

摘要/Abstract

引用本文

使用本文

参考文献

相关文章 15

Metrics

本文评价

推荐阅读 0

[1]	Qianyu Qi(齐倩玉), Yaowei Li(李耀威), Ting Liu(刘婷), Peiqing Zhang(张培晴),Shixun Dai(戴世勋), and Tiefeng Xu(徐铁峰). Design of a coated thinly clad chalcogenide long-period fiber grating refractive index sensor based on dual-peak resonance near the phase matching turning point[J]. 中国物理B, 2023, 32(1): 14204-014204.
[2]	Hui Xu(徐慧), Ziqi Li(李子琦), Chi Pang(逄驰), Rang Li(李让), Genglin Li(李庚霖), Sh. Akhmadaliev, Shengqiang Zhou(周生强), Qingming Lu(路庆明), Yuechen Jia(贾曰辰), and Feng Chen(陈峰). Second harmonic generation from precise diamond blade diced ridge waveguides[J]. 中国物理B, 2022, 31(9): 94209-094209.
[3]	Hongbao Yao(姚洪宝), Er-Jia Guo(郭尔佳), Chen Ge(葛琛), Can Wang(王灿), Guozhen Yang(杨国桢), and Kuijuan Jin(金奎娟). Photon-interactions with perovskite oxides[J]. 中国物理B, 2022, 31(8): 88106-088106.
[4]	Hao Wang(王浩), Liang Qiao(乔亮), Zu-Ying Zheng(郑祖应), Hong-Bo Hao(郝宏波), Tao Wang(王涛), Zheng Yang(杨正), and Fa-Shen Li(李发伸). Microwave absorption properties regulation and bandwidth formula of oriented Y₂Fe₁₇N_3-δ@SiO₂/PU composite synthesized by reduction-diffusion method[J]. 中国物理B, 2022, 31(11): 114206-114206.
[5]	Rong Ye(叶荣), Huining Dong(董会宁), Xianyun Wu(吴显云), and Xiang Gao(高翔). Phase matched scanning optical parametric chirped pulse amplification based on pump beam deflection[J]. 中国物理B, 2021, 30(10): 104209-104209.
[6]	何烜坚, 贾俊, 焦高锋, 陈丽清, 袁春华, 张卫平. A two-mode squeezed light based on a double-pump phase-matching geometry[J]. 中国物理B, 2020, 29(7): 74207-074207.
[7]	刘振, 贾维国, 王红玉, 汪洋, 门克内木乐, 张俊萍. Effect of dark soliton on the spectral evolution of bright soliton in a silicon-on-insulator waveguide[J]. 中国物理B, 2020, 29(6): 64212-064212.
[8]	高敏, 杨峰, 崔学武, 王瑞. Geometrical optics-based ray field tracing method for complex source beam applications[J]. 中国物理B, 2018, 27(4): 40401-040401.
[9]	彭英楠, 张金伟, 王兆华, 朱江峰, 李德华, 魏志义. Generation of 15 W femtosecond laser pulse from a Kerr-lens mode-locked Yb: YAG thin-disk oscillator[J]. 中国物理B, 2016, 25(9): 94207-094207.
[10]	孙经纬, 王湘晖, 常胜江, 曾明, 张娜. Second harmonic generation of metal nanoparticles under tightly focused illumination[J]. 中国物理B, 2016, 25(3): 37803-037803.
[11]	张宁华, 滕浩, 黄杭东, 田文龙, 朱江峰, 吴红萍, 潘世烈, 方少波, 魏志义. Generation of femtosecond laser pulses at 396 nm in K₃B₆O₁₀Cl crystal[J]. 中国物理B, 2016, 25(12): 124204-124204.
[12]	田文龙, 王兆华, 朱江峰, 魏志义. Tunable femtosecond near-infrared source based on a Yb:LYSO-laser-pumped optical parametric oscillator[J]. 中国物理B, 2016, 25(1): 14207-014207.
[13]	张解放, 金美贞, 何纪达, 楼吉辉, 戴朝卿. Dynamics of optical rogue waves in inhomogeneous nonlinear waveguides[J]. 中国物理B, 2013, 22(5): 54208-054208.
[14]	常建华, 孙青, 葛益娴, 王婷婷, 陶在红, 张闯. Mid-IR dual-wavelength difference frequency generation in uniform grating PPLN using index dispersion control[J]. 中国物理B, 2013, 22(12): 124204-124204.
[15]	陈伟, 孟洲, 周会娟. Phase-matching analysis of four-wave mixing induced by modulation instability in a single-mode fiber[J]. 中国物理B, 2012, 21(9): 94215-094215.