Chinese Journal of Lasers, Volume. 51, Issue 19, 1901007(2024)

Research Progress on High-Power Narrow-Linewidth Linearly Polarized Yb-Doped Fiber Lasers and Their Main Applications (Invited)

Yanshan Wang1,2, Xiaobo Yang1,2,3, Yujun Feng1,2, Wanjing Peng1,2, Hao Hu1,2, Tenglong Li1,2, Hang Liu1,2, Yao Wang1,2, Shengtao Lin1,2, Jiangcai Wei1,2, Jue Wang1,2, Yinhong Sun1,2, Yanhua Lu1,2, Yi Ma1,2、*, and Chun Tang1,2
Author Affiliations
  • 1Institute of Applied Electronics, China Academy of Engineering Physics, Mianyang 621900, Sichuan , China
  • 2National Key Laboratory of Advanced Lasers and High Power Microwaves, Mianyang 621900, Sichuan , China
  • 3Graduate School of CAEP, Beijing 100088, China
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    Figures & Tables(58)
    Structure diagram of 811 W single-frequency fiber laser[8]
    Signal power and reflectivity versus pump power[8]
    Structure diagram of 414 W single-frequency laser[9]
    Experimental structure of all-fiber single-frequency PM fiber amplifier[12]
    Structure diagram of linearly polarized single-frequency fiber amplifier based on 1018 nm fiber laser core-pumping[13]
    Cross section of Panda type polarization-maintaining fiber
    Structure and output power curve of narrow-linewidth PM laser[15]
    Experimental system of the 2.43 kW narrow-linewidth linearly polarized fiber laser[21]
    Structure diagram of 2 kW narrow-linewidth linearly-polarized amplifier[23]
    Laser power and PER versus pump power[28]
    System structure of spectrum broadening by optimization algorithm[54]
    Theoretical and experimental results[54]. (a) Optimized signal waveforms; (b) optimized spectrum
    Output characteristics[30]. (a) Laser power and PER versus pump power; (b) output spectra under different laser powers
    Experimental test results[34]. (a) Output power curve; (b) forward spectrum; (c) backward spectrum; (d) beam quality
    Experimental system structure of narrow-linewidth linearly polarized fiber amplifier[32]
    Output characteristics[32]. (a) Output spectra under different laser powers; (b) 3 dB linewidth and RMS linewidth versus output power
    Output characteristics of 3.96 kW narrow-linewidth linearly polarized amplifier[33]. (a) Output spectra under different laser powers; (b) linewidth versus laser power
    Output characteristics of 4.5 kW narrow-linewidth linearly polarized fiber amplifier[35]. (a) Backward powers under different laser powers; (b) output spectra under different laser powers; (c) PERs under different laser powers
    Output characteristics of 5 kW narrow-linewidth linearly polarized fiber amplifier[36]. (a) Backward powers under different laser powers; (b) PERs under different laser powers; (c) output spectra under maximum power
    Experimental system structure of 2 kW narrow linewidth linearly-polarized fiber amplifier[37]
    Experimental system structure of narrow-linewidth linearly polarized fiber amplifier with output power of 5 kW and linewidth of 10 GHz[38]
    Output characteristics[38]. (a) PER versus laser power; (b) output spectrum at maximum laser power
    Experimental structure and results[19]. (a) Structure of narrow-linewidth fiber amplifier based on adaptive polarization control; (b) P∕S polarized power and PER versus laser power
    Structure of narrow-linewidth fiber amplifier based on adaptive polarization control[20]
    Experimental system of 3.1 kW narrow-linewidth fiber laser[17]
    Linearly polarized fiber oscillatorbased onfiber Bragg grating (FBG) [55]
    Theoretical simulation results of PM 15/130 μm fiber loss for different linear polarization modes[56]
    Experimental system of kW 1030 nm narrow-linewidth linearly polarized fiber amplifier [43]
    Experimental system of 3 kW narrow-linewidth linearly polarized fiber amplifier [44]
    Experimental results[44]. (a) Output spectrum under 3.08 kW power; (b) SRS spectrum
    Experimental system of 4.6 kW narrow-linewidth linearly polarized fiber amplifier[46]
    Refractive index distribution of single-trench fiber[88]
    Longitudinal profile for core diameter of biconical tapered fiber[89]
    Cross section photograph and refractive index distribution of optical fiber[90]. (a) Cross section of partially doped fiber; (b) refractive index distribution
    Device diagram of coherent beam combining system, output time domain signal, and spot patterns[98]. (a) Device diagram of coherent beam combining system; (b) output time domain signal and spot patterns
    Experimental results of coherent beam combing with 20 kW level fiber laser[100]. (a) Long exposure pattern of far-field spot pattern in open loop; (b) long exposure pattern of far-field spot pattern in close loop
    Optical path diagram of coherent beam combiningsystem[102]
    Experimental results before and after phase locking[102]. (a) Before phase locking; (b) after phase locking
    Optical path diagram of coherent beam combiningsystem[95]
    Output power versus total laser power after beam combining [95]
    Power curves of four-channel amplifier and output power and efficiency curves after polarization coherent beam combining[96]. (a) Power curves of four-channel amplifier; (b) output power and efficiency curves after polarization coherent beam combining
    Optical path diagram of coherent beam combiningsystem [97]
    Absorption characteristics of copper at different wavelengths [107]
    Schematic of green fiber laser based on single-pass SHG[110]
    Output power and SHG conversion efficiency of 532 nm CW laser [110]
    Output power and SHG conversion efficiency of 532 nm QCW laser[110]
    Schematic of sub-ns fiber laser and its harmonic conversion system[111]
    SHG green laser power versus pump power at different linewidths[112]
    Schematic diagram of experimental setup[109]
    Calculated and experimental results under different crystal lengths[109]. (a) Normalized power versus wavelength under different crystal lengths; (b) frequency doubling efficiency and green light power versus fundamental frequency light power
    Simplified diagram of LIGO gravitational wave detector [114]
    Single frequency fiber amplifier based on cascaded amplification structure[115]
    Schematic diagram of 3 W single frequency fiber amplifier[116]
    • Table 1. Representative research results of high-power narrow-linewidth linear polarization fiber amplifier in past 10 years

      View table

      Table 1. Representative research results of high-power narrow-linewidth linear polarization fiber amplifier in past 10 years

      YearInstitution

      Seed

      type

      Configuration

      Power /

      kW

      Linewidth

      Beam quality factor

      M2

      PER /dBGFL/OPFLRef.
      2014Air Force Research LaboratorySFSBulk structure0.811<5 kHz1.2

      9.2 m/

      0 m

      8
      2017National University of Defense TechnologyAll-fiber structure0.41420 kHz1.34172.5 m/0.18 m9
      2019Laser Zendrum HannoverAll-fiber structure0.2kHz level19

      3 m/

      10
      2020Université de BordeauxAll-fiber structure0.365<30 kHz1.117

      2 m/

      0 m

      11
      2022South China University of TechnologyAll-fiber structure0.6513 kHz (3 dB)1.7142.5 m/0.3 m12
      2023National University of Defense TechnologyAll-fiber structure0.25<100 kHz1.1517

      1.85 m/

      0.2 m

      13
      2024National University of Defense TechnologyAll-fiber structure1.01<28 MHz1.1414
      2014Lockheed MartinPMSFSAll-fiber structure1.1412 GHz1.081615
      2015IPGWNS modulation, all-fiber structure1.0320 GHz1.1820

      ‒/

      2 m

      16
      2016MIT Lincoln LaboratoryPRBS modulation, bulk structure3.112 GHz (3 dB)1.1512

      3‒4 m/

      0 m

      17
      2016National University of Defense TechnologySinc modulation, all-fiber structure1.8945 GHz (3 dB)<1.315.5

      8.5 m/

      2.5 m

      18
      2017Institute of Applied ElectronicsWNS modulation, all-fiber structure0.966.5 GHz (3 dB)1.213

      15 m/

      19
      2017National University of Defense TechnologyWNS modulation, all-fiber structure, PC1.4345 GHz (3 dB)11.1

      15 m/

      4.5 m

      20
      2017National University of Defense TechnologyWNS modulation, all-fiber structure2.4367 GHz (3 dB)18.3

      9 m/

      4 m

      21
      2017IPGAll-fiber structure1.515 GHz<1.1208 m/2 m22
      2018IPGAll-fiber structure222 GHz<1.12010 m/3 m23
      2018National University of Defense TechnologySinc modulation, all-fiber structure1.087.6 GHz1.1414

      9 m/

      2.5 m

      24
      2019National University of Defense TechnologyWNS modulation, all-fiber structure0.8271.8 GHz (3 dB)<1.1512

      5.5 m/

      25
      2019Advanced Photonics Research Institute (GIST)PRBS modulation, all-fiber structure0.8186.6 GHz (3 dB)13

      8 m/

      26
      2019Institute of Applied ElectronicsWNS modulation, all-fiber structure1.513 GHz (3 dB)1.1413

      8 m/

      2.5 m

      27
      2019Institute of Applied ElectronicsWNS modulation, all-fiber structure2.6232 GHz (3 dB)1.2914

      9 m/

      3.5 m

      28
      2021Institute of Applied ElectronicsOS modulation, all-fiber structure3.2520 GHz (RMS)1.2215

      10 m/

      29
      2021Institute of Applied ElectronicsOS modulation, all-fiber structure3.623GHz (RMS)1.211530
      2021Research Center of Laser FusionWNS modulation, all-fiber structure3.2221.7 GHz1.21031
      2022Institute of Applied ElectronicsOS modulation, all-fiber structure4.45

      58 GHz (RMS)

      21 GHz (RMS)

      1.2617.732
      2022Institute of Applied ElectronicsOS modulation, all-fiber structure5.04

      53 GHz (3 dB)

      71 GHz (3 dB)

      1.2816.532
      2022National University of Defense TechnologyWNS modulation, all-fiber structure3.96164 GHz (3 dB)1.413.98.5 m/33
      2022Research Center of Laser FusionOS modulation, all-fiber structure310.6 GHz1.181434
      2022National University of Defense TechnologyWNS modulation, all-fiber structure4.5

      87 GHz

      (3 dB)

      1.510.310 m/35
      2023National University of Defense TechnologyWNS modulation, all-fiber structure5.02101 GHz (3 dB)11.814 m/36
      2023Ground Technology Research InstitutePRBS modulation, all-fiber structure2.01

      8 GHz

      (3 dB)

      1.3157.3 m/37
      2023Institute of Applied ElectronicsOS modulation, all-fiber structure5.029.93 GHz (RMS)1.262038
      2024Institute of Applied ElectronicsOS modulation, all-fiber structure3.29.7GHz (RMS)1.2920.3

      13 m/

      39
      2015Tianjin UniversityFOSAll-fiber structure0.5230 GHz (3 dB)1.118

      12.5 m/

      2.5 m

      40
      2018National University of Defense TechnologyAll-fiber structure1.01880 GHz (3 dB)1.2414

      8.5 m/

      1.5 m

      41
      2018Institute of Applied ElectronicsAll-fiber structure1.147 GHz1.25157 m/42
      2018Research Center of Laser FusionAll-fiber structure1

      37 GHz

      (3 dB)

      1.212

      7 m/

      1 m

      43
      2020Institute of Applied ElectronicsAll-fiber structure3.0853 GHz (3 dB)1.4512

      9 m/

      3 m

      44
      2023Huazhong University of Science and TechnologyAll-fiber structure3.258 GHz (3 dB)1.316.613 m/45
      2023Huazhong University of Science and TechnologyAll-fiber structure4.691 GHz (3 dB)1.31546
    • Table 2. Performance comparison of different phase modulation methods

      View table

      Table 2. Performance comparison of different phase modulation methods

      Modulation methodSpectral broadening propertySBS propertySystem complexity
      Sinc modulationSpectral linewidth is positively correlated with modulation frequency and depth and generally requires cascade modulation to obtain wider spectrumSBS threshold increases with increase of modulation frequency and modulation depthSingle-stage modulation is relatively simple, and cascade modulation will increase system complexity
      WNS modulationSpectral linewidth is positively correlated with modulation frequency and modulation depthSBS threshold increases with increase of modulation frequency and modulation depthGenerally, wide spectrum can be obtained by using single-stage modulation, and system is relatively simple
      PRBS modulationSpectral linewidth is approximately equal to modulation frequencySBS threshold is related to modulation depth and modulation frequency. When modulation frequency is certain, SBS threshold reaches maximum when modulation depth is π. Different fiber lengths need to correspond to different code lengthsRelatively simple
      Optimized signal modulationSpectral linewidth is proportional to modulation frequency and depth and correlated with signal waveformSBS threshold is positively correlated with modulation frequency and modulation depth. There is optimal signal waveform that can maximize SBS thresholdSignal waveform needs to be nonlinearly optimized, and system is complex
    • Table 3. Performance comparison of amplifiers based on different seed sources

      View table

      Table 3. Performance comparison of amplifiers based on different seed sources

      Seed typeSpectral broadening propertySBS propertySRS propertySystem complexity and cost
      SFSTime domain is stable, and there is no spectral broadening during amplificationLow SBS thresholdHigh SRS thresholdIt requires multistage amplification, special fiber design, or stress measurement for optical fibers. System is complex and high-cost
      PMSFSTime domain is stable, and there is no spectral broadening during amplificationSBS threshold is related to modulation method and modulation linewidthHigh SRS thresholdIt requires phase modulation and multistage amplification. System is complex and high-cost
      FOSTime domain is unstable, and there is spectral broadening in amplification processHigh SBS thresholdSRS threshold is positively correlated with time domain stability of FOSGenerally, only one stage amplification is required. System is simple and low-cost
    • Table 4. Representative application results of narrow-linewidth fiber lasers in coherent beam combining in past 10 years

      View table

      Table 4. Representative application results of narrow-linewidth fiber lasers in coherent beam combining in past 10 years

      YearInstitutionNumber of laser channelsSingle-laser parameterOutput powerRef.
      2014Northrop Grumman Aerospace Systems3

      M2: 1.22‒1.39

      PER: 12 dB‒18 dB

      Linewidth: 18 GHz

      2.4 kW[95]
      2015National University of Defense Technology45.02 kW[96]
      2016Air Force Research Laboratory5

      M2<1.1

      PER: 15 dB‒16 dB

      Linewidth: 8.8 GHz

      4.9 kW[97]
      2020National University of Defense Technology107Linewidth: single frequency51.7 mW[98]
      2020Civan Advanced Technologies Ltd.3216 kW[99]
      2021National University of Defense Technology1921.6 kW[100]
      2023Research Center of Laser FusionLinewidth: 40 GHz10.8 kW[101]
      2023National University of Defense Technology1027Linewidth: single frequency[102]
    • Table 5. Representative research results of fiber laser in frequency doubling to produce green light in past 10 years

      View table

      Table 5. Representative research results of fiber laser in frequency doubling to produce green light in past 10 years

      YearInstitutionFiber laser parameter

      CW/

      QCW

      Green laser wavelengthGreen laser powerConversion efficiencyRef.
      2014IPG

      M2<1.15

      PER:>20 dB

      Linewidth: 20 GHz

      CW532 nm356 W35%[110]
      2014IPG

      M2<1.15

      PER:>20 dB

      Linewidth: 20 GHz

      QCW532 nm

      Average power: 550 W

      Peak power: 1100 W

      52%[110]
      2015IPG

      M2<1.18

      PER:>20 dB

      Linewidth: 20 GHz

      QCW532 nm

      Average power: 700 W

      Peak power: 3.3 kW

      70%[16]
      2017Osaka UniversitySub-ns520 nm600 W67%[111]
      2020Coherent

      PER:>15 dB

      Linewidth: 45 GHz

      CW532 nm1 kW54%[112]
      2021Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences

      M2: 1.15

      PER:>15 dB

      Linewidth: 20 GHz

      CW532 nm321 W40.9%[113]
      2021Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences

      M2<1.1

      PER:>15 dB

      Linewidth: 20 GHz

      CW532 nm610 W56.27%[109]
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    Yanshan Wang, Xiaobo Yang, Yujun Feng, Wanjing Peng, Hao Hu, Tenglong Li, Hang Liu, Yao Wang, Shengtao Lin, Jiangcai Wei, Jue Wang, Yinhong Sun, Yanhua Lu, Yi Ma, Chun Tang. Research Progress on High-Power Narrow-Linewidth Linearly Polarized Yb-Doped Fiber Lasers and Their Main Applications (Invited)[J]. Chinese Journal of Lasers, 2024, 51(19): 1901007

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    Paper Information

    Category: laser devices and laser physics

    Received: Jun. 18, 2024

    Accepted: Oct. 6, 2024

    Published Online: Oct. 21, 2024

    The Author Email: Yi Ma (rufinecn@163.com)

    DOI:10.3788/CJL240982

    CSTR:32183.14.CJL240982

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