Compact 2×2 parabolic multimode interference thermo–optic switches based on fluorinated photopolymer
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摘要
In this work, a dual-side parabolic structural(DSPS) multimode interference(MMI) thermo–optic(TO) waveguide switch is designed and fabricated by using novel low-loss fluorinated photopolymer materials. Comparing with the traditional dual-side linear structural(DSLS) MMI device, the effective length of the MMI coupling region proposed can be effectively reduced by 40%. The thermal stability of the waveguide material is analyzed, and the optical characteristics of the switching chip are simulated. The actual performances of the entire MMI switch are measured with an insertion loss of7 dB, switching power of 15 m W and an extinction ratio of 28 dB. In contrast to the traditional MMI optical switch, the new type of parabolic structural MMI TO waveguide switch exhibits lower power consumption and larger extinction ratio. The compact fluorinated polymer MMI TO switches are suitable well for realizing miniaturization, high-properties, and lower cost of photonic integrated circuits.
In this work, a dual-side parabolic structural(DSPS) multimode interference(MMI) thermo–optic(TO) waveguide switch is designed and fabricated by using novel low-loss fluorinated photopolymer materials. Comparing with the traditional dual-side linear structural(DSLS) MMI device, the effective length of the MMI coupling region proposed can be effectively reduced by 40%. The thermal stability of the waveguide material is analyzed, and the optical characteristics of the switching chip are simulated. The actual performances of the entire MMI switch are measured with an insertion loss of7 dB, switching power of 15 m W and an extinction ratio of 28 dB. In contrast to the traditional MMI optical switch, the new type of parabolic structural MMI TO waveguide switch exhibits lower power consumption and larger extinction ratio. The compact fluorinated polymer MMI TO switches are suitable well for realizing miniaturization, high-properties, and lower cost of photonic integrated circuits.
In this work, a dual-side parabolic structural(DSPS) multimode interference(MMI) thermo–optic(TO) waveguide switch is designed and fabricated by using novel low-loss fluorinated photopolymer materials. Comparing with the traditional dual-side linear structural(DSLS) MMI device, the effective length of the MMI coupling region proposed can be effectively reduced by 40%. The thermal stability of the waveguide material is analyzed, and the optical characteristics of the switching chip are simulated. The actual performances of the entire MMI switch are measured with an insertion loss of7 dB, switching power of 15 m W and an extinction ratio of 28 dB. In contrast to the traditional MMI optical switch, the new type of parabolic structural MMI TO waveguide switch exhibits lower power consumption and larger extinction ratio. The compact fluorinated polymer MMI TO switches are suitable well for realizing miniaturization, high-properties, and lower cost of photonic integrated circuits.
引文
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[3]Forni F,Shi Y,Tran N C,Boom H P A,Tangdiongga E and KoonenAM J 2018 J.Lightwave Technol.36 3444
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[5]Zhang Z J,Yang J B,He X,Han Y X,Zhang J J,Huang J,Chen D Band Xu S Y 2018 Opt.Commun.425 196
[6]Herbert D,Kumar S,Cristina L A,Mikael D,Guy L,Peter V,Jan Wand Dries V T 2018 IEEE Photon.Technol.Lett.30 1258
[7]Deng Y G,Yako M,Zhang Z Y and Wada K 2018 IEEE J.Sel.Top.Quantum Electron.24 8300505
[8]Huang B J,Tsai C T,Lin Y H,Cheng C H,Wang H Y,Chi Y C,Chang P H,Wu C I and Lin G R 2018 ACS Photon.5 2251
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[11]Shin J S,Park T H,Oh M C,Chu W S,Lee C H and Shin S Y 2015Opt.Express 23 17223
[12]Soref R A,Francesco D L and Vittorio M N P 2018 Opt.Express 2614879
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[16]Li H Q,Dong X Y and Li E 2013 Opt.&Laser Technol.47 366
[17]Liang Y X,Zhao M S,Luo Y Q,Gu Y Y,Zhang Y,Wang L H,Han XY and Wu Z L 2016 Opt.Eng.55 117102
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[19]Ghanshyam S,Ashok S and Seema V 2013 IETE J.Res.59 479
[20]Xiao H F,Deng L,Zhao G L,Liu Z L,Meng Y H,Guo X N,Liu G P,Liu S,Ding J F and Tian Y H 2017 J.Opt.19 025802
[21]Zhang S C,Ji W,Yin R,Li X,Gong Z Y and Lv L Y 2018 IEEE Photon.Technol.Lett.30 107
[22]Le D T,Truong C D and Le T T 2017 Opt.Commun.387 148
[23]Chaudhuri R R,Amarachukwu N E,Youngsik S and Seo S W 2018Opt.Commun.418 1
[24]Han H L,Le H,Zhang X P,Liu A,Lin T Y,Chen Z,Lv H B,Lu M H,Liu X P and Chen Y F 2018 Opt.Express 26 25602
[25]Zhang Z D,Ma L J,Gao F,Zhang Y J,Tang J,Cao H L,Zhang B Z,Wang J C,Yan S B and Xue C Y 2017 Chin.Phys.B 26 124212
[26]Zhang Z D,Zhao Y N,Lu D,Xiong Z H and Zhang Z Y 2012 Acta Phys.Sin.61 187301(in Chinese)
[27]Yu Y Y,Sun X Q,Ji L T,He G B,Wang X B,Yi Y J,Chen C M,Wang F and Zhang D M 2016 Chin.Phys.B 25 054101
[28]Kim J P,Lee W Y,Kang J W,Kwon S K,Kim J J and Lee J S 2001Macromolecules 34 7817
[29]He G B,Ji L T and Gao Y 2017 Opt.Commun.402 422
[30]Wang J H,Chen C M,Zheng Y,Wang X B,Yi Y J,Sun X Q,Wang Fand Zhang D M 2017 Chin.Phys.B 26 024212
[31]Supaat A S M,Ibrahim M H,Mohammad A B,Kassim N M and Ghazali N E 2008 Am.J.Appl.5 1552
[32]Alvaro R,Ana G,Antoine B,Amadeu G and Pablo S 2016 Opt.Express24 191
[33]Wang S P and Dai D X 2018 Opt.Lett.43 2531
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