• Laser & Optoelectronics Progress
  • Vol. 60, Issue 16, 1600003 (2023)
Yuheng Xu1,2, Cheng Qiu1,*, Yongyi Chen1,3,**, Ye Wang1,4..., Lei Liang1, Peng Jia1, Li Qin1, Yongqiang Ning1 and Lijun Wang1|Show fewer author(s)
Author Affiliations
  • 1State Key Laboratory of Luminescence and Application, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, Jilin, China
  • 2Daheng College, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Jlight Semiconductor Technology Co., Ltd., Changchun 130102, Jilin, China
  • 4School of Opto-Electronic Engineering, Changchun University of Science and Technology, Changchun 130022, Jilin, China
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    DOI: 10.3788/LOP222487 Cite this Article Set citation alerts
    Yuheng Xu, Cheng Qiu, Yongyi Chen, Ye Wang, Lei Liang, Peng Jia, Li Qin, Yongqiang Ning, Lijun Wang. Research Progress of High-Speed and Wide-Tuned Frequency Swept Lasers for Optical Coherence Tomography Applications[J]. Laser & Optoelectronics Progress, 2023, 60(16): 1600003 Copy Citation Text show less
    OCT principle
    Fig. 1. OCT principle
    SS-OCT principle
    Fig. 2. SS-OCT principle
    Development of SS-OCT and its main frequency swept lasers
    Fig. 3. Development of SS-OCT and its main frequency swept lasers
    Schematic of polyhedral rotating mirror frequency swept light source[41]
    Fig. 4. Schematic of polyhedral rotating mirror frequency swept light source[41]
    Structure of blazed grating tunable laser[42]
    Fig. 5. Structure of blazed grating tunable laser[42]
    Structure of volume Bragg grating tunable laser[43]
    Fig. 6. Structure of volume Bragg grating tunable laser[43]
    Double-cavity polyhedral rotating mirror swept frequency light source[45]
    Fig. 7. Double-cavity polyhedral rotating mirror swept frequency light source[45]
    Structure comparison between traditional ring cavity frequency swept laser and FDML laser[51]
    Fig. 8. Structure comparison between traditional ring cavity frequency swept laser and FDML laser[51]
    Structural diagram of FDML frequency swept light source[53]
    Fig. 9. Structural diagram of FDML frequency swept light source[53]
    Structure diagram of FFP-TF[54]
    Fig. 10. Structure diagram of FFP-TF[54]
    FDML structure with dual SOA[55]
    Fig. 11. FDML structure with dual SOA[55]
    Output spectrum of FDML fenquency swept laser with DSF and ordinary single-mode fiber[57]
    Fig. 12. Output spectrum of FDML fenquency swept laser with DSF and ordinary single-mode fiber[57]
    Schematic of buffer FDML structure [58]
    Fig. 13. Schematic of buffer FDML structure [58]
    4× buffer stage FDML laser[59]
    Fig. 14. 4× buffer stage FDML laser[59]
    Structure diagram of harmonic FDML[60]
    Fig. 15. Structure diagram of harmonic FDML[60]
    FDML laser based on polyhedral rotating mirror filter [63]
    Fig. 16. FDML laser based on polyhedral rotating mirror filter [63]
    Structure diagram of MEMS-VCSEL[65]
    Fig. 17. Structure diagram of MEMS-VCSEL[65]
    Process flow chart of InP-based MEMS-VCSEL [71]
    Fig. 18. Process flow chart of InP-based MEMS-VCSEL [71]
    1050-nm electrically pumped MEMS-VCSEL[72]
    Fig. 19. 1050-nm electrically pumped MEMS-VCSEL[72]
    Structural diagram of SG-DBR[76]
    Fig. 20. Structural diagram of SG-DBR[76]
    Diagram of vernier tuning principle
    Fig. 21. Diagram of vernier tuning principle
    Schematic of simulated SG-DBR structure[78]
    Fig. 22. Schematic of simulated SG-DBR structure[78]
    SSG-TTG tunable double guide laser [80]
    Fig. 23. SSG-TTG tunable double guide laser [80]
    Schematic of DS-DBR grating structure[82]
    Fig. 24. Schematic of DS-DBR grating structure[82]
    DCG-DBR tuning current-wavelength diagram[85]
    Fig. 25. DCG-DBR tuning current-wavelength diagram[85]
    Structural diagram of SSG-DBR[87]
    Fig. 26. Structural diagram of SSG-DBR[87]
    Performance index of swept laserPerformance index of SS-OCTTypical value
    Scan rateImaging speed100 kHz27
    Center wavelengthAxial resolution,lateral resolution1060 nm28
    Tuning rangeAxial resolution70 nm29
    Dynamic coherence lengthImaging depth10 mm30
    Output powerSignal-to-noise ratio,sensitivity11 mW31
    Table 1. Corresponding relationship between performance index of frequency swept light source and SS-OCT
    Type of swept laserTuning rangeScan rateOutput power
    External cavity330 nm3250 kHz3377 W34
    FDML160 nm275.2 MHz35200 mW35
    MEMS-VCSEL150 nm36800 kHz3730 mW37
    VT-DBR60 nm38100 kHz3930 mW40
    Table 2. The latest performance index of four swept lasers
    YearUnitMethodPerformance indexReference
    2003Harvard Medical School & Wellman Laboratories for PhotomedicineUsing polygon mirror as filter for the first time

    Scan rate:15.7 kHz;

    tuning range:75 nm

    29
    2005Harvard Medical School & Wellman Laboratories for PhotomedicineUsing dual SOAs to broaden tuning range

    Scan rate:20 kHz;

    tuning range:145 nm

    45
    2009University of Central FloridaUsing blazed grating to achieve tuning

    Center wavelength:

    2000 nm;

    tuning range:161 nm

    46
    2019University of Central FloridaUsing volume Bragg grating and lens group

    Tuning range:103 nm;

    output power:48 W

    50
    2022Fraunhofer IOSB Inst Optron Syst Technol & ImageUsing volume Bragg grating and Tm3+∶Ho3+-codoped free-space single-oscillator fiber laser

    Center wavelength:

    2090 nm;

    tuning range:200 nm;

    output power:77 W

    34
    Table 3. Representative research progresses of external cavity frequency swept laser
    YearUnitMethodPerformance indexReference
    2006Massachusetts Institute of TechnologyAll optical modes are stored in the long cavity up to several kilometers

    Scan rate:290 kHz;

    tuning range:105 nm

    53
    2009Ludwig Maximilian UniversityUsing faraday rotating mirror to reduce the cavity length

    Scan rate:570 kHz;

    tuning range:95 nm

    60
    2012LightLab ImagingUsing dispersion compensation module(DCM)to reduce dispersion

    Scan rate:200 kHz;

    tuning range:105 nm;

    output power:35 mW

    30
    2012Ludwig Maximilian UniversityUsing four buffer stage to increase scan rate

    Scan rate:1.6 MHz;

    tuning range:100 nm

    59
    2018Ludwig Maximilian UniversityUsing improved FBG,SOA,and FP cavity

    Tuning range:143 nm;

    scan rate:1.67 MHz

    28
    Table 4. Representative research progresses of FDML frequency swept laser
    YearUnitMethodPerformance indexReference
    1999CoretekUsing strain compensated multiple quantum wells and using stable cavity to realize low diffraction loss cavity

    Tuning range:50 nm;

    SMSR:50 dB

    67
    2003Hochschule Darmstadt University of Applied ScienceUsing electric pumping structure and introducing buried tunnel junction

    Tuning range:40 nm;

    SMSR:32 dB

    70
    2009Research Center for Advanced Science and Technology,The University of TokyoUsing movable silicon mirror with a high resonance frequency to increase scan rate

    Scan rate:500 kHz;

    tuning range:55 nm;

    SMSR:60 dB

    71
    2012Praevium ResearchThe thin optical pump active region structure and the wide gain bandwidth InP based multi quantum well active region are combined with the wide bandwidth fully oxidized GaAs based mirrors through wafer bonding

    Scan rate:500 kHz;

    tuning range:150 nm

    36
    2020Praevium ResearchThe strain compensated InGaAsP gain region is combined with a fully oxidized back mirror to achieve a wide tuning range

    Scan rate:800 kHz;

    tuning range:100 nm;output power:30 mW

    37
    Table 5. Representative research progresses of MEMS-VCSEL frequency swept laser
    YearUnitMethodPerformance indexReference
    1993University of CaliforniaFirst using sampling grating as two side grating

    Tuning range:57 nm;

    SMSR:30 dB

    78
    1993NTT Photoelectric LaboratoryUsing super structure grating instead of sampling grating to widen the tuning range

    Tuning range:105 nm;

    SMSR:35 dB

    79
    2003BookhamDesigning digital supermodel DBR to improve tuning

    Tuning range:40 nm;

    SMSR:40 dB

    82
    2004BookhamDesigning phase grating DBR to achieve flatness output

    Tuning range:35 nm;

    SMSR:40 dB

    84
    2008Wuhan National Laboratory of OptoelectronicsDesigning digital concatenated grating DBR to achieve flatness output and wide tuning range

    Tuning range:54 nm;

    SMSR:40 dB

    85
    2019JDSUSG-DBR produced by JDSU,which represents the SG-DBR with high performance at present

    Tuning range:60 nm;

    SMSR:30 dB;

    output power:10 mW

    38
    Table 6. Representative research progresses of DBR frequency swept laser
    TypeTechnical maturityCostScan rateTuning rangeOutput powerSwept linearity
    External cavityhighhighlowhighhighmiddle
    FDMLmiddlehighmiddlemiddlemiddlelow
    MEMS-VCSELhighmiddlemiddlemiddlelowmiddle
    VT-DBRlowlowhighlowlowhigh
    Table 7. Performance indexes of different types of swept frequency light sources
    Yuheng Xu, Cheng Qiu, Yongyi Chen, Ye Wang, Lei Liang, Peng Jia, Li Qin, Yongqiang Ning, Lijun Wang. Research Progress of High-Speed and Wide-Tuned Frequency Swept Lasers for Optical Coherence Tomography Applications[J]. Laser & Optoelectronics Progress, 2023, 60(16): 1600003
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