• High Power Laser Science and Engineering
  • Vol. 11, Issue 2, 02000e18 (2023)
Xin Zeng1、2, Shuzhen Cui2, Huawei Jiang2, Bowen Ruan1、2, Xin Cheng1、2, Jiaqi Zhou2, Zhiquan Lin1、2, Xuezong Yang1, Weibiao Chen1、2, and Yan Feng1、2、*
Author Affiliations
  • 1Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou, China
  • 2Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai, China
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    DOI: 10.1017/hpl.2023.28 Cite this Article Set citation alerts
    Xin Zeng, Shuzhen Cui, Huawei Jiang, Bowen Ruan, Xin Cheng, Jiaqi Zhou, Zhiquan Lin, Xuezong Yang, Weibiao Chen, Yan Feng. Single-frequency upconverted laser generation by phase summation[J]. High Power Laser Science and Engineering, 2023, 11(2): 02000e18 Copy Citation Text show less
    The concept of phase summation in SFG for single-frequency upconverted laser generation. The spectral and phase evolutions at different stages of the laser are schematically illustrated.
    Fig. 1. The concept of phase summation in SFG for single-frequency upconverted laser generation. The spectral and phase evolutions at different stages of the laser are schematically illustrated.
    The experimental setup includes two phase-modulated seed lasers, a two-stage Raman fiber amplifier and a frequency mixing unit. EOM, electro-optic phase modulator; WDM, wavelength division multiplexer.
    Fig. 2. The experimental setup includes two phase-modulated seed lasers, a two-stage Raman fiber amplifier and a frequency mixing unit. EOM, electro-optic phase modulator; WDM, wavelength division multiplexer.
    Spectra of the fundamental lasers. (a) Spectra of two single-frequency and phase-modulated lasers measured with the FPI. (b) Optical spectra of the seed lasers and main amplifier.
    Fig. 3. Spectra of the fundamental lasers. (a) Spectra of two single-frequency and phase-modulated lasers measured with the FPI. (b) Optical spectra of the seed lasers and main amplifier.
    Power curves of the fundamental Raman amplifier and upconverted single-frequency laser by sum-frequency generation. (a) The output and backward light power of the Raman fiber amplifier as a function of 1120 nm pump power. (b) The power and conversion efficiency of the single-frequency upconverted laser as a function of the fundamental laser power. Insert: spectrum of the generated 590.3 nm laser.
    Fig. 4. Power curves of the fundamental Raman amplifier and upconverted single-frequency laser by sum-frequency generation. (a) The output and backward light power of the Raman fiber amplifier as a function of 1120 nm pump power. (b) The power and conversion efficiency of the single-frequency upconverted laser as a function of the fundamental laser power. Insert: spectrum of the generated 590.3 nm laser.
    The spectral evolution of upconverted lasers at different phase offsets between sinusoidal signals. (a) The simulated spectra of upconverted lasers. (b) The measured spectra with the FPI. The intensity is normalized by the intensity of the single-frequency case.
    Fig. 5. The spectral evolution of upconverted lasers at different phase offsets between sinusoidal signals. (a) The simulated spectra of upconverted lasers. (b) The measured spectra with the FPI. The intensity is normalized by the intensity of the single-frequency case.
    Spectra of upconverted output. (a) The fine spectrum and FPI scan signal of the single-frequency upconverted laser with phase-modulated fundamental lasers at output power of 17.3 W. (b) The fine spectrum and FPI scan signal of the upconverted single-frequency laser without phase modulation.
    Fig. 6. Spectra of upconverted output. (a) The fine spectrum and FPI scan signal of the single-frequency upconverted laser with phase-modulated fundamental lasers at output power of 17.3 W. (b) The fine spectrum and FPI scan signal of the upconverted single-frequency laser without phase modulation.
    Xin Zeng, Shuzhen Cui, Huawei Jiang, Bowen Ruan, Xin Cheng, Jiaqi Zhou, Zhiquan Lin, Xuezong Yang, Weibiao Chen, Yan Feng. Single-frequency upconverted laser generation by phase summation[J]. High Power Laser Science and Engineering, 2023, 11(2): 02000e18
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