• Chinese Journal of Lasers
  • Vol. 49, Issue 12, 1201004 (2022)
Jiaxing Heng1, Xi Feng1, Pei Liu1, and Zhaowei Zhang1、2、*
Author Affiliations
  • 1School of Optical & Electronic Information, Huazhong University of Science & Technology, Wuhan 430074, Hubei, China
  • 2Wuhan National Laboratory for Optoelectronics, Huazhong University of Science & Technology, Wuhan 430074, Hubei, China
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    DOI: 10.3788/CJL202249.1201004 Cite this Article Set citation alerts
    Jiaxing Heng, Xi Feng, Pei Liu, Zhaowei Zhang. Research Progress on Intracavity Spectral Broadening in Femtosecond Optical Parametric Oscillators[J]. Chinese Journal of Lasers, 2022, 49(12): 1201004 Copy Citation Text show less
    Dual-channel OPO[53]. (a) Schematic; (b) experimental setup; (c) idler spectra output during dual-channel operation
    Fig. 1. Dual-channel OPO[53]. (a) Schematic; (b) experimental setup; (c) idler spectra output during dual-channel operation
    Simulated signal bandwidth (-20 dB) and maximum pump pulse energy versus intracavity GDD[79]
    Fig. 2. Simulated signal bandwidth (-20 dB) and maximum pump pulse energy versus intracavity GDD[79]
    Measured signal spectra and bandwidths at different incident pump powers[79]. (a)-(e) Measured signal spectra at different incident pump powers, where the dashed line in figure (e) shows calculated phase-matching curve of 3 mm long PPLN crystal; (f) measured signal bandwidth versus incident pump power
    Fig. 3. Measured signal spectra and bandwidths at different incident pump powers[79]. (a)-(e) Measured signal spectra at different incident pump powers, where the dashed line in figure (e) shows calculated phase-matching curve of 3 mm long PPLN crystal; (f) measured signal bandwidth versus incident pump power
    Relationship between bandwidth of output signal bandwidth and nonlinear parameter deff2/n2 of nonlinear crystal by simulation[80]
    Fig. 4. Relationship between bandwidth of output signal bandwidth and nonlinear parameter deff2/n2 of nonlinear crystal by simulation[80]
    Signal spectra at different pump powers[80]. (a)-(d) Experimentally measured signal spectra at different pump powers, where the dashed line in figure (a) is phase matching curve of 3 mm long KTA; (e) simulated signal spectrum (solid line) and intracavity GDD (dashed line)
    Fig. 5. Signal spectra at different pump powers[80]. (a)-(d) Experimentally measured signal spectra at different pump powers, where the dashed line in figure (a) is phase matching curve of 3 mm long KTA; (e) simulated signal spectrum (solid line) and intracavity GDD (dashed line)
    Numerical simulation: output signal before and after pulse-compression[88]. (a)-(b) Signal pulse and spectrum without pulse-compression; (c)-(d) signal pulse (dashed line is the fitted hyperbolic secant curve) and spectrum with pulse-compression (the pump power was 0.7 W)
    Fig. 6. Numerical simulation: output signal before and after pulse-compression[88]. (a)-(b) Signal pulse and spectrum without pulse-compression; (c)-(d) signal pulse (dashed line is the fitted hyperbolic secant curve) and spectrum with pulse-compression (the pump power was 0.7 W)
    Jiaxing Heng, Xi Feng, Pei Liu, Zhaowei Zhang. Research Progress on Intracavity Spectral Broadening in Femtosecond Optical Parametric Oscillators[J]. Chinese Journal of Lasers, 2022, 49(12): 1201004
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