Acta Optica Sinica, Volume. 42, Issue 23, 2306001(2022)
Photodarkening Effect of 5 kW Near-Single-Mode Fiber Laser Oscillator
Fig. 2. Output characteristics of fiber laser oscillator under forward pump condition. (a) Output power and optical-to-optical conversion efficiency varying with pump power; (b) optical spectrum at pump power of 1.644 kW; (c) time-domain signals recorded by photoelectric detector at P1 and P2; (d) Fourier spectra in frequency domain corresponding to time-domain signals at P1 and P2
Fig. 3. Output characteristics of fiber laser oscillator under backward pump condition. (a) Output power and optical-to-optical conversion efficiency varying with pump power; (b) optical spectrum at pump power of 4 kW; (c) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at pump power of 4 kW
Fig. 4. Output characteristics of fiber laser oscillator under bidirectional pump condition. (a) Output power and optical-to-optical conversion efficiency varying with pump power; (b) optical spectrum at pump power of 5 kW; (c) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at pump power of 5 kW
Fig. 5. Measurement result of beam quality of output laser with different powers under bidirectional pump condition
Fig. 6. Output characteristics of fiber laser oscillator under full power working. (a) Output power of fiber laser oscillator varying with operating time under full power working; (b) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at stageⅠ; (c) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at stage
Fig. 7. Comparison of output characteristics of fiber laser oscillator before and after long-time full power working. (a) Output power varying with optical-to-optical conversion efficiency varying with pump power before and after long-time working; (b) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at pump power of 6.512 kW; (c) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at pump power of 6.556 kW
Fig. 8. Output characteristics of fiber laser oscillator under bidirectional pump condition after adjusting forward and backward pump power ratio. (a) Output power and optical-to-optical conversion efficiency varying with pump power; (b) optical spectrum at pump power of 5 kW; (c) time-domain signal recorded by photoelectric detector and corresponding Fourier spectrum in frequency domain at pump power of 5 kW
Fig. 9. Output power of fiber laser oscillator varying with operating time under second full power working
Fig. 10. Comparison of output power and conversion efficiency of fiber laser oscillator before and after photodarkening effect. (a)(d) Output power and optical-to-optical conversion efficiency varying with pump power; (b)(e) time-domain signals; (c)(f) Fourier spectra in frequency domain corresponding to time-domain signals
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Peng Wang, Baolai Yang, Hanwei Zhang, Xiaoming Xi, Chen Shi, Xiaolin Wang, Xiaojun Xu, Lü Pin. Photodarkening Effect of 5 kW Near-Single-Mode Fiber Laser Oscillator[J]. Acta Optica Sinica, 2022, 42(23): 2306001
Category: Fiber Optics and Optical Communications
Received: Apr. 11, 2022
Accepted: Jun. 4, 2022
Published Online: Dec. 14, 2022
The Author Email: Zhang Hanwei (zhanghanwei100@163.com)