Infrared and Laser Engineering, Volume. 52, Issue 5, 20220756(2023)

Approach to generation of flat optical frequency comb using cascaded phase modulator and intensity modulator

Yaohu Cui1, Zixiong Wang2、*, Yitong Xu2, Xunhe Zuo2, Yang Jiang3, Jinlong Yu2, and Zhanhua Huang1
Author Affiliations
  • 1School of Precision Instrument and Opto-Electronics Engineering, Tianjin University, Tianjin 300072, China
  • 2School of Electrical and Information Engineering, Tianjin University, Tianjin 300072, China
  • 3College of Physics, Guizhou University, Guiyang 550025, China
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    Figures & Tables(15)
    Schematic to generate flat OFC by using cascaded PM and IM
    Waveform of combined fundamental tone and third harmonic that drive the PM
    OFC in simulation, where the PM is driven by combined fundamental tone and third harmonic and the IM is driven by fourth harmonic
    OFC in simulation, where the combined fundamental tone, third and fifth harmonic drive both PM and IM
    Relationship between the flatness of optical frequency comb and the fixed phase of each microwave driving signal under case (b) of Tab. 1
    Modulation indices of all microwave driving signals when the phase of 3-GHz microwave signal that drives PM is fixed under case (b) of Tab. 1
    Modulation indices of all microwave driving signals when the phase of 9-GHz microwave signal that drives PM is fixed under case (b) of Tab. 1
    Modulation indices of all microwave driving signals when the phase of 12-GHz microwave signal that drives IM is fixed under case (b) of Tab.1
    Relationship between the flatness of optical frequency comb and the phase of each microwave driving signal under case (c) of Tab. 1
    Relationship between the flatness of optical frequency comb and the phase of each microwave driving signal under case (a) of Tab.1
    Relationship between the flatness of optical frequency comb and the phase of each microwave driving signal under case (d) of Tab.1
    Relationship between number of comb lines and flatness of the generated OFC
    Experiment setup of the generation for flat optical frequency comb by using cascaded phase modulator and intensity modulator
    OFC in experiment, where the PM is driven by fundamental tone and third harmonic and the IM is driven by fourth harmonic
    • Table 1. Combinations of harmonics for the generation of flat OFC

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      Table 1. Combinations of harmonics for the generation of flat OFC

      CaseCombined harmonics that drive PM Parameters of harmonics that drive PM Combined harmonics that drive IM Parameters of harmonics that drive IM Number of comb lines Flatness/dB
      (a)$ {f}_{0} $, $ 3{f}_{0} $$ {\;\beta }_{\mathrm{P}\mathrm{M},1}= $1.50 $ {\;\beta }_{\mathrm{P}\mathrm{M},3}= $1.20 $ {\varphi }_{\mathrm{P}\mathrm{M},1}= $1.75 $ {\varphi }_{\mathrm{P}\mathrm{M},3}= $5.93 $ 2{f}_{0} $$ {\;\beta }_{\mathrm{I}\mathrm{M},2}= $0.45 $ {\varphi }_{\mathrm{I}\mathrm{M},2}= $3.05 $ {\varphi }_{\mathrm{B}\mathrm{i}\mathrm{a}\mathrm{s}}= $3.23 90.59
      (b)$ {f}_{0} $, $ 3{f}_{0} $$ {\;\beta }_{\mathrm{P}\mathrm{M},1}= $1.48 $ {\;\beta }_{\mathrm{P}\mathrm{M},3}= $1.12 $ {\varphi }_{\mathrm{P}\mathrm{M},1}= $3.01 $ {\varphi }_{\mathrm{P}\mathrm{M},3}= $3.85 $ 4{f}_{0} $$ {\;\beta }_{\mathrm{I}\mathrm{M},4}= $1.06 $ {\varphi }_{\mathrm{I}\mathrm{M},4}= $3.09 $ {\varphi }_{\mathrm{B}\mathrm{i}\mathrm{a}\mathrm{s}}= $2.93 130.27
      (c)$ {f}_{0} $, $ 3{f}_{0} $$ {\;\beta }_{\mathrm{P}\mathrm{M},1}= $1.35 $ {\;\beta }_{\mathrm{P}\mathrm{M},3}= $0.92 $ {\varphi }_{\mathrm{P}\mathrm{M},1}= $3.32 $ {\varphi }_{\mathrm{P}\mathrm{M},3}= $5.20 $ {f}_{0} $, $ 3{f}_{0} $, $ 5{f}_{0} $$ {\;\beta }_{\mathrm{I}\mathrm{M},1}= $0.97 $ {\;\beta }_{\mathrm{I}\mathrm{M},3}= $0.63 $ {\;\beta }_{\mathrm{I}\mathrm{M},5}= $1.01 $ {\varphi }_{\mathrm{I}\mathrm{M},1}= $0.17 $ {\varphi }_{\mathrm{I}\mathrm{M},3}= $6.10 $ {\varphi }_{\mathrm{I}\mathrm{M},5}= $0.70 $ {\varphi }_{\mathrm{B}\mathrm{i}\mathrm{a}\mathrm{s}}= $3.13 170.45
      (d)$ {f}_{0} $, $ 3{f}_{0} $, $ 5{f}_{0} $$ {\;\beta }_{\mathrm{P}\mathrm{M},1}= $1.36 $ {\;\beta }_{\mathrm{P}\mathrm{M},3}= $1.02 $ {\;\beta }_{\mathrm{P}\mathrm{M},5}= $1.06 $ {\varphi }_{\mathrm{P}\mathrm{M},1}= $4.34 $ {\varphi }_{\mathrm{P}\mathrm{M},3}= $5.18 $ {\varphi }_{\mathrm{P}\mathrm{M},5}= $2.44 $ {f}_{0} $, $ 3{f}_{0} $, $ 5{f}_{0} $$ {\;\beta }_{\mathrm{I}\mathrm{M},1}= $0.29 $ {\;\beta }_{\mathrm{I}\mathrm{M},3}= $1.04 $ {\;\beta }_{\mathrm{I}\mathrm{M},5}= $0.87 $ {\varphi }_{\mathrm{I}\mathrm{M},1}= $5.82 $ {\varphi }_{\mathrm{I}\mathrm{M},3}= $0.84 $ {\varphi }_{\mathrm{I}\mathrm{M},5}= $0.80 $ {\varphi }_{\mathrm{B}\mathrm{i}\mathrm{a}\mathrm{s}}= $0.01 190.56
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    Yaohu Cui, Zixiong Wang, Yitong Xu, Xunhe Zuo, Yang Jiang, Jinlong Yu, Zhanhua Huang. Approach to generation of flat optical frequency comb using cascaded phase modulator and intensity modulator[J]. Infrared and Laser Engineering, 2023, 52(5): 20220756

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    Paper Information

    Category: Optical communication and sensing

    Received: Oct. 27, 2022

    Accepted: --

    Published Online: Jul. 4, 2023

    The Author Email: Wang Zixiong (wangzixiong@tju.edu.cn)

    DOI:10.3788/IRLA20220756

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