Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force

doi:10.1088/1674-1056/23/12/124211

›› 2014, Vol. 23 ›› Issue (12): 124211-124211.doi: 10.1088/1674-1056/23/12/124211

• ELECTROMAGNETISM, OPTICS, ACOUSTICS, HEAT TRANSFER, CLASSICAL MECHANICS, AND FLUID DYNAMICS • 上一篇下一篇

Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force

廖莎莎, 闵书存, 董建绩

Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan 430074, China

收稿日期:2014-05-08 修回日期:2014-06-10 出版日期:2014-12-15 发布日期:2014-12-15
基金资助:
Project supported by the National Natural Science Foundation of China (Grant Nos. 60901006 and 11174096), the National Basic Research Program of China (Grant No. 2011CB301704), the Program for New Century Excellent Talents in Ministry of Education of China (Grant No. NCET-11-0168), and the Foundation for the Author of National Excellent Doctoral Dissertation of China (Grant No. 201139).

Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force

Liao Sha-Sha (廖莎莎), Min Shu-Cun (闵书存), Dong Jian-Ji (董建绩)

Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan 430074, China

Received:2014-05-08 Revised:2014-06-10 Online:2014-12-15 Published:2014-12-15
Contact: Dong Jian-Ji E-mail:jjdong@mail.hust.edu.cn
Supported by:
Project supported by the National Natural Science Foundation of China (Grant Nos. 60901006 and 11174096), the National Basic Research Program of China (Grant No. 2011CB301704), the Program for New Century Excellent Talents in Ministry of Education of China (Grant No. NCET-11-0168), and the Foundation for the Author of National Excellent Doctoral Dissertation of China (Grant No. 201139).

摘要/Abstract

摘要： Integrated optical pulse shaper opens up possibilities for realizing the ultra high-speed and ultra wide-band linear signal processing with compact size and low power consumption. We propose a silicon monolithic integrated optical pulse shaper using optical gradient force, which is based on the eight-path finite impulse response. A cantilever structure is fabricated in one arm of the Mach–Zehnder interferometer (MZI) to act as an amplitude modulator. The phase shift feature of waveguide is analyzed with the optical pump power, and five typical waveforms are demonstrated with the manipulation of optical force. Unlike other pulse shaper schemes based on thermo–optic effect or electro–optic effect, our scheme is based on a new degree of freedom manipulation, i.e., optical force, so no microelectrodes are required on the silicon chip, which can reduce the complexity of fabrication. Besides, the chip structure is suitable for commercial silicon on an insulator (SOI) wafer, which has a top silicon layer of about 220 nm in thickness.

关键词: pulse shaping, arbitrary waveform generation, optical grant force

Abstract: Integrated optical pulse shaper opens up possibilities for realizing the ultra high-speed and ultra wide-band linear signal processing with compact size and low power consumption. We propose a silicon monolithic integrated optical pulse shaper using optical gradient force, which is based on the eight-path finite impulse response. A cantilever structure is fabricated in one arm of the Mach–Zehnder interferometer (MZI) to act as an amplitude modulator. The phase shift feature of waveguide is analyzed with the optical pump power, and five typical waveforms are demonstrated with the manipulation of optical force. Unlike other pulse shaper schemes based on thermo–optic effect or electro–optic effect, our scheme is based on a new degree of freedom manipulation, i.e., optical force, so no microelectrodes are required on the silicon chip, which can reduce the complexity of fabrication. Besides, the chip structure is suitable for commercial silicon on an insulator (SOI) wafer, which has a top silicon layer of about 220 nm in thickness.

Key words: pulse shaping, arbitrary waveform generation, optical grant force

中图分类号: (Ultrafast processes; optical pulse generation and pulse compression)

42.65.Re

42.79.Gn (Optical waveguides and couplers) 42.50.Wk (Mechanical effects of light on material media, microstructures and particles) 42.79.Sz (Optical communication systems, multiplexers, and demultiplexers?)

廖莎莎, 闵书存, 董建绩. Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force[J]. , 2014, 23(12): 124211-124211.

Liao Sha-Sha (廖莎莎), Min Shu-Cun (闵书存), Dong Jian-Ji (董建绩). Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force[J]. Chin. Phys. B, 2014, 23(12): 124211-124211.

参考文献 0


[1]	Weiner A W 2011 Opt. Commun. 284 3669 doi: 10.1016/j.optcom.2011.03.084

[2]	Fang X, Wang D N and Li S 2003 J. Opt. Soc. Am. B 20 1603 doi: 10.1364/JOSAB.20.001603

[3]	Khan M H, Shen H, Xuan Y, Zhao L, Xiao S, Leaird D E, Weiner A M and Qi M 2010 Nat. Photo. 4 117 doi: 10.1038/nphoton.2009.266

[4]	Dugan M, Tull J and Warren W 1997 J. Opt. Soc. Am. B 14 2348 doi: 10.1364/JOSAB.14.002348

[5]	Monsterleet A, Tonda-Goldstein S, Dolfi D, Huignard J, Sapé P and Chazelas J 2005 Electron. Lett. 41 332 doi: 10.1049/el:20057949

[6]	Shen M and Minasian R A 2004 IEEE Photon. Technol. Lett. 16 1155 doi: 10.1109/LPT.2004.824618

[7]	Jiang Z, Leaird D E and Weiner A M 2005 Opt. Express 13 10431 doi: 10.1364/OPEX.13.010431

[8]	Bortnik B, Poberezhskiy I Y, Chou J, Jalali B and Fetterman H R 2006 J. Lightwave Technol. 24 2752 doi: 10.1109/JLT.2006.875943

[9]	Huang C B, Leaird D E and Weiner A M 2007 Opt. Lett. 32 3242 doi: 10.1364/OL.32.003242

[10]	Dai Y, Chen X, Ji H and Xie S 2007 IEEE Photon. Technol. Lett. 19 1916 doi: 10.1109/LPT.2007.908430

[11]	Supradeepa V, Leaird D E and Weiner A M 2009 Opt. Express 17 25 doi: 10.1364/OE.17.000025

[12]	Miao H, Leaird D E, Langrock C, Fejer M M and Weiner A M 2009 Opt. Express 17 3381 doi: 10.1364/OE.17.003381

[13]	Supradeepa V, Leaird D E and Weiner A M 2009 Opt. Express 17 14434 doi: 10.1364/OE.17.014434

[14]	Kuo F M, Shi J W, Chiang H C, Chuang H P, Chiou H K, Pan C L, Chen N W, Tsai H J and Huang C B 2010 IEEE Photon. J. 2 719 doi: 10.1109/JPHOT.2010.2064160

[15]	Wang C and Yao J 2010 J. Lightwave Technol. 28 1652 doi: 10.1109/JLT.2010.2047093

[16]	Zhang A and Li C 2012 Opt. Express 20 23074 doi: 10.1364/OE.20.023074

[17]	Fontaine N, Scott R, Cao J, Karalar A, Jiang W, Okamoto K, Heritage J, Kolner B and Yoo S 2007 Opt. Lett. 32 865 doi: 10.1364/OL.32.000865

[18]	Jiang W, Soares F M, Seo S W, Baek J H, Fontaine N K, Broeke N K, Cao J, Yan J, Okamoto K and Olsson F 2008 in: National Fiber Optic Engineers Conference, Optical Society of America, 2008, p. JThA39

[19]	Scott R, Fontaine N, Yang C, Geisler D, Okamoto K, Heritage J and Yoo S 2008 Opt. Lett. 33 1068 doi: 10.1364/OL.33.001068

[20]	Geisler D J, Fontaine N K, He T, Scott R P, Paraschis L, Heritage J P and Yoo S 2009 Opt. Express 17 15911 doi: 10.1364/OE.17.015911

[21]	Shen H, Fan L, Varghese L T, Leaird D E, Weiner A M and Qi M 2010 in: Conference on Lasers and Electro-Optics, Optical Society of America, 2010, p. CMS2

[22]	Guo X, Zou C L, Ren X F, Sun F W and Guo G C 2012 Appl. Phys. Lett. 101 071114 doi: 10.1063/1.4746761

[23]	Long Y, Wang J, Li X, Zhu L, Gui C, Zhang Z and Du J 2013 in: IEEE Photonics Conference (IPC), 2013 p. 339

[24]	Rakich P T, Popovic M A and Wang Z 2009 Opt. Express 17 18116 doi: 10.1364/OE.17.018116

[25]	Ma J and Povinelli M L 2011 Opt. Express 19 10102 doi: 10.1364/OE.19.010102

Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force

Optical pulse shaper with integrated slab waveguide for arbitrary waveform generation using optical gradient force

PDF (PC)

赞

可视化

摘要/Abstract

引用本文

使用本文

参考文献 0

相关文章 11

Metrics

本文评价

推荐阅读 0

[1]	Wenjing Cheng(程文静), Yuan Li(李媛), Hongzhen Qiao(乔红贞), Meng Wang(王蒙), Shaoshuo Ma(马绍朔), Fangjie Shu(舒方杰), Chuanqi Xie(解传奇), and Guo Liang(梁果). Simulating the resonance-mediated (1+2)-three-photon absorption enhancement in Pr³⁺ ions by a rectangle phase modulation[J]. 中国物理B, 2022, 31(6): 63201-063201.
[2]	程文静, 梁果, 吴萍, 赵世华, 贾天卿, 孙真荣, 张诗按. Up-conversion luminescence tuning in Er³⁺-doped ceramic glass by femtosecond laser pulse at different laser powers[J]. 中国物理B, 2018, 27(12): 123201-123201.
[3]	齐大龙, 郑烨, 程文静, 姚云华, 邓联忠, 冯东海, 贾天卿, 孙真荣, 张诗按. Simulating resonance-mediated two-photon absorption enhancement in rare-earth ions by a rectangle phase modulation[J]. 中国物理B, 2018, 27(1): 13202-013202.
[4]	马秀荣, 梁裕卿, 王松, 张双根, 单云龙. Improving the intensity and efficiency of compressed echo in rare-earth-ion-doped crystal[J]. 中国物理B, 2016, 25(7): 70302-070302.
[5]	廖莎莎, 杨婷, 董建绩. On-chip optical pulse shaper for arbitrary waveform generation[J]. , 2014, 23(7): 73201-073201.
[6]	郑傲凌, 董建绩, 雷蕾, 杨婷, 张新亮. Diversity of photonic differentiators based on flexible demodulation of phase signals[J]. 中国物理B, 2014, 23(3): 33201-033201.
[7]	徐传彩, 姜澜, 冷妮, 刘鹏军. Selective triggering of phase change in dielectric by femtosecond pulse trains based on electron dynamics control[J]. Chin. Phys. B, 2013, 22(4): 45203-045203.
[8]	董建绩, 罗博文, 于源, 张新亮. Photonic generation of arbitrary waveforms based on incoherent wavelength-to-time mapping[J]. 中国物理B, 2012, 21(6): 68401-068401.
[9]	张诗按, 张晖, 王祖赓, 孙真荣. Selective excitation and suppression of coherent anti-Stokes Raman scattering by shaping femtosecond pulses[J]. 中国物理B, 2010, 19(4): 43201-043201.
[10]	张晖, 张诗按, 王祖赓, 孙真荣. Coherent control of non-resonant two-photon transition in molecular system[J]. 中国物理B, 2010, 19(11): 113208-113301.
[11]	张诗按, 王祖赓, 孙真荣. Quantum coherent control of two-photon transitions by square phase-modulation[J]. 中国物理B, 2008, 17(8): 2914-2918.