• Chinese Journal of Lasers
  • Vol. 48, Issue 12, 1201003 (2021)
Yizhou Liu1, Wenchao Qiao1, Kong Gao1、2, Rong Xu2, Tianli Feng1、2, Meng Zhang1, Xun Li3, Yangyang Liang1、2, and Tao Li1、2、*
Author Affiliations
  • 1Laser Physics and Technology Laboratory, School of Information Science and Engineering, Shandong University, Qingdao, Shandong 266237, China
  • 2China Key Laboratory of Laser & Infrared System (Shandong University), Ministry of Education, Qingdao, Shandong 266237, China
  • 3State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics of CAS, Xi'an, Shaanxi 710119, China
  • show less
    DOI: 10.3788/CJL202148.1201003 Cite this Article Set citation alerts
    Yizhou Liu, Wenchao Qiao, Kong Gao, Rong Xu, Tianli Feng, Meng Zhang, Xun Li, Yangyang Liang, Tao Li. Development of High-Power Ultrafast Fiber Laser Technology[J]. Chinese Journal of Lasers, 2021, 48(12): 1201003 Copy Citation Text show less
    Development history of high power ultrafast fiber laser
    Fig. 1. Development history of high power ultrafast fiber laser
    Structure diagram of passive mode-locked fiber laser
    Fig. 2. Structure diagram of passive mode-locked fiber laser
    Distribution of research results of passively mode locked fiber laser oscillators[16-49]
    Fig. 3. Distribution of research results of passively mode locked fiber laser oscillators[16-49]
    Diagram of high power ultrafast laser system
    Fig. 4. Diagram of high power ultrafast laser system
    Measured autocorrelation trace of the compressed pulses with and without fine adjusting of dispersion of CFBG at 10 μJ pulse energy[68]
    Fig. 5. Measured autocorrelation trace of the compressed pulses with and without fine adjusting of dispersion of CFBG at 10 μJ pulse energy[68]
    Experimental results. (a) Pulse spectrum at the output of the amplifier; (b) autocorrelation trace of the amplifier pulses (inset: output beam profile) [71]
    Fig. 6. Experimental results. (a) Pulse spectrum at the output of the amplifier; (b) autocorrelation trace of the amplifier pulses (inset: output beam profile) [71]
    Experimental simulation results. (a) Gaussian spectrum; (b) parabolic spectrum; phase-profiles of (c) Gaussian spectrum and (d) parabolic spectrum at power levels corresponding to B-integrals of 3.5 rad and 16 rad, respectively; corresponding autocorrelation traces of (e) Gaussian spectrum and (f) parabolic spectrum at power levels corresponding to B-integrals of 3.5 rad and 16 rad, respectively[74]
    Fig. 7. Experimental simulation results. (a) Gaussian spectrum; (b) parabolic spectrum; phase-profiles of (c) Gaussian spectrum and (d) parabolic spectrum at power levels corresponding to B-integrals of 3.5 rad and 16 rad, respectively; corresponding autocorrelation traces of (e) Gaussian spectrum and (f) parabolic spectrum at power levels corresponding to B-integrals of 3.5 rad and 16 rad, respectively[74]
    High-power ultra-fast laser output. (a) Full power spectrum of single channel before compression and combined beam before and after compression; (b) measured and calculated transform-limited (TFL) non-collinear intensity autocorrelation (inset: output stretched pulse shape of the main amplifier) [77]
    Fig. 8. High-power ultra-fast laser output. (a) Full power spectrum of single channel before compression and combined beam before and after compression; (b) measured and calculated transform-limited (TFL) non-collinear intensity autocorrelation (inset: output stretched pulse shape of the main amplifier) [77]
    Schematic diagram of amplification technology. (a) Chirped pulse amplification; (b) divided pulse amplification; (c) pre-chirp managed amplification
    Fig. 9. Schematic diagram of amplification technology. (a) Chirped pulse amplification; (b) divided pulse amplification; (c) pre-chirp managed amplification
    Schematic construction of the 10.4 kW fiber laser system [77]
    Fig. 10. Schematic construction of the 10.4 kW fiber laser system [77]
    In recent years, high-power ultra-fast laser output parameters based on CPA, DPA, PCMA, and CPS technologies have been achieved. (a) Year-energy distribution diagram of 1 μm high-power ultrafast laser; (b) year-average power distribution diagram of 1 μm high-power ultrafast laser[80, 82-88, 90-112]
    Fig. 11. In recent years, high-power ultra-fast laser output parameters based on CPA, DPA, PCMA, and CPS technologies have been achieved. (a) Year-energy distribution diagram of 1 μm high-power ultrafast laser; (b) year-average power distribution diagram of 1 μm high-power ultrafast laser[80, 82-88, 90-112]
    Structure diagram of CPA system with average output power of 830 W[80]
    Fig. 12. Structure diagram of CPA system with average output power of 830 W[80]
    Experimental setup of DPA system [78]
    Fig. 13. Experimental setup of DPA system [78]
    Schematic construction of the high power Yb-fiber PCMA system [117]
    Fig. 14. Schematic construction of the high power Yb-fiber PCMA system [117]
    Experimental setup of CPS system with output pulse energy of 10 mJ [112]
    Fig. 15. Experimental setup of CPS system with output pulse energy of 10 mJ [112]
    Common nonlinear compression devices. (a) Multipass cell with quartz sheet; (b) multipass cell filled with noble gas
    Fig. 16. Common nonlinear compression devices. (a) Multipass cell with quartz sheet; (b) multipass cell filled with noble gas
    Yizhou Liu, Wenchao Qiao, Kong Gao, Rong Xu, Tianli Feng, Meng Zhang, Xun Li, Yangyang Liang, Tao Li. Development of High-Power Ultrafast Fiber Laser Technology[J]. Chinese Journal of Lasers, 2021, 48(12): 1201003
    Download Citation