• High Power Laser and Particle Beams
  • Vol. 33, Issue 11, 111003 (2021)
Mengqiu Fan1、4, Shengtao Lin2, han Wu3, Wanguo Zheng1、*, and Zinan Wang2、*
Author Affiliations
  • 1Laser Fusion Research Center, CAEP, P. O. Box 919-988, Mianyang 621900, China
  • 2Key Laboratory of Optical Fiber Sensing and Communications of Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China
  • 3College of Electronics and Information Engineering, Sichuan University, Chengdu 610064, China
  • 4Graduate School of China Academy of Engineering Physics, Beijing 100088, China
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    DOI: 10.11884/HPLPB202133.210306 Cite this Article
    Mengqiu Fan, Shengtao Lin, han Wu, Wanguo Zheng, Zinan Wang. Research progress of random fiber lasers’ characteristics in time-frequency-spatial domain[J]. High Power Laser and Particle Beams, 2021, 33(11): 111003 Copy Citation Text show less
    A concept of the random distributed feedback fiber laser[5]
    Fig. 1. A concept of the random distributed feedback fiber laser[5]
    Randomly distributed feedback fiber laser configurations[5]
    Fig. 2. Randomly distributed feedback fiber laser configurations[5]
    Methods for solving the systems of differential equations of the Raman random fiber laser[14]
    Fig. 3. Methods for solving the systems of differential equations of the Raman random fiber laser[14]
    Lasing spectral characteristics of randomly distributed feedback fiber laser based on NLSE[11]
    Fig. 4. Lasing spectral characteristics of randomly distributed feedback fiber laser based on NLSE[11]
    Temporal and statistical characteristics of randomly distributed feedback fiber laser based on NLSE[11]
    Fig. 5. Temporal and statistical characteristics of randomly distributed feedback fiber laser based on NLSE[11]
    Output intensity characteristics of randomly distributed feedback fiber laser[35]
    Fig. 6. Output intensity characteristics of randomly distributed feedback fiber laser[35]
    Output temporal characteristics and statistical features of random fiber laser[36]
    Fig. 7. Output temporal characteristics and statistical features of random fiber laser[36]
    Temporal intensity dynamics and PDF of filtered random lasing radiations at different spectral locations[38]
    Fig. 8. Temporal intensity dynamics and PDF of filtered random lasing radiations at different spectral locations[38]
    Temporal signals and corresponding spectral densities of the RFL at maximal pump power[39]
    Fig. 9. Temporal signals and corresponding spectral densities of the RFL at maximal pump power[39]
    Normalized oscilloscope traces of the RRFL output by different pump[40]
    Fig. 10. Normalized oscilloscope traces of the RRFL output by different pump[40]
    Effect of bandwidth of ASE pump on random fiber laser[42]
    Fig. 11. Effect of bandwidth of ASE pump on random fiber laser[42]
    Characteristics of 1090 nm YRFL pump[43]
    Fig. 12. Characteristics of 1090 nm YRFL pump[43]
    Comparison between 1365 nm RFL pumped by 1090 YRFL and commercial 1365 nm fiber laser[43]
    Fig. 13. Comparison between 1365 nm RFL pumped by 1090 YRFL and commercial 1365 nm fiber laser[43]
    Spectrum evolution of random fiber laser based on Rayleigh scattering[13]
    Fig. 14. Spectrum evolution of random fiber laser based on Rayleigh scattering[13]
    Temporal dynamics of the generation spectra of the measured random fiber laser (the letters in (a) and (b) mark the same spectral lines)[46]
    Fig. 15. Temporal dynamics of the generation spectra of the measured random fiber laser (the letters in (a) and (b) mark the same spectral lines)[46]
    Real-time spectro-temporal evolution in the random fiber laser[47]
    Fig. 16. Real-time spectro-temporal evolution in the random fiber laser[47]
    Spectral correlations in the random fiber laser[47]
    Fig. 17. Spectral correlations in the random fiber laser[47]
    Statistical analysis of the intensity spectra and PDF P(I) of maximum intensities I with different pump power (erbium-doped RFL)[49]
    Fig. 18. Statistical analysis of the intensity spectra and PDF P(I) of maximum intensities I with different pump power (erbium-doped RFL)[49]
    Statistical analysis of the temporal intensity and PDF P(I) of maximum intensities Iwith different pump power (Raman RFL)[52]
    Fig. 19. Statistical analysis of the temporal intensity and PDF P(I) of maximum intensities Iwith different pump power (Raman RFL)[52]
    Optical images of the speckle pattern and the logo mask with different illumination sources[57]
    Fig. 20. Optical images of the speckle pattern and the logo mask with different illumination sources[57]
    Speckle formed after passing through a ground glass diffuser[59]
    Fig. 21. Speckle formed after passing through a ground glass diffuser[59]
    Schematic diagram of high power low spatial coherence random fiber laser based on MOPA configuration[60]
    Fig. 22. Schematic diagram of high power low spatial coherence random fiber laser based on MOPA configuration[60]
    Mengqiu Fan, Shengtao Lin, han Wu, Wanguo Zheng, Zinan Wang. Research progress of random fiber lasers’ characteristics in time-frequency-spatial domain[J]. High Power Laser and Particle Beams, 2021, 33(11): 111003
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