• High Power Laser Science and Engineering
  • Vol. 11, Issue 1, 010000e5 (2023)
Yanyan Li1, Beijie Shao1、2, Yujie Peng1、*, Junyu Qian1、2, Wenkai Li1, Xinliang Wang1, Xingyan Liu1, Xiaoming Lu1, Yi Xu1, Yuxin Leng1、*, and Ruxin Li1
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-intense Laser Science, Shanghai Institute of Optics and Fine Mechanics (SIOM), Chinese Academy of Sciences (CAS), Shanghai, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing, China
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    DOI: 10.1017/hpl.2022.44 Cite this Article Set citation alerts
    Yanyan Li, Beijie Shao, Yujie Peng, Junyu Qian, Wenkai Li, Xinliang Wang, Xingyan Liu, Xiaoming Lu, Yi Xu, Yuxin Leng, Ruxin Li. Ultra-broadband pulse generation via hollow-core fiber compression and frequency doubling for ultra-intense lasers[J]. High Power Laser Science and Engineering, 2023, 11(1): 010000e5 Copy Citation Text show less
    (a) Schematic of the laser system. PS: actuator; L: lens; BS: beam splitter; LS: linear stage; W: CaF2 window; CM: concave mirror; DM: dichroic mirror; BT: beam trap; WP: wedge pair. (b) The output beam profile of the HCF and (c) the near-field and (d) far-field beam profiles of the 910 nm beam.
    Fig. 1. (a) Schematic of the laser system. PS: actuator; L: lens; BS: beam splitter; LS: linear stage; W: CaF2 window; CM: concave mirror; DM: dichroic mirror; BT: beam trap; WP: wedge pair. (b) The output beam profile of the HCF and (c) the near-field and (d) far-field beam profiles of the 910 nm beam.
    (a) Spectrum profiles measured by a near-infrared spectrometer at different argon pressures; (b) energy stability of the output laser after the HCF system.
    Fig. 2. (a) Spectrum profiles measured by a near-infrared spectrometer at different argon pressures; (b) energy stability of the output laser after the HCF system.
    The SHG spectra with one single crystal and cascaded crystals.
    Fig. 3. The SHG spectra with one single crystal and cascaded crystals.
    (a) Spectra and spectral phase of the 910 nm laser: spectrum (pink filled) with a fiber spectrometer, spectrum (red solid) with a Wizzler device, measured spectral phase (black solid) and retrieved spectral phase (black dot). (b) Measured (golden filled) and FTL (red solid) pulse duration of the 910 nm pulse.
    Fig. 4. (a) Spectra and spectral phase of the 910 nm laser: spectrum (pink filled) with a fiber spectrometer, spectrum (red solid) with a Wizzler device, measured spectral phase (black solid) and retrieved spectral phase (black dot). (b) Measured (golden filled) and FTL (red solid) pulse duration of the 910 nm pulse.
    (a) Energy stability of the 910 nm laser; (b) spectrum stability of the 910 nm laser.
    Fig. 5. (a) Energy stability of the 910 nm laser; (b) spectrum stability of the 910 nm laser.
    (a) Third-order correlation curves of the initial pulse (black) and the 910 nm pulse (red); (b) third-order correlation curve of the laser pulse after a one-stage OPCPA system.
    Fig. 6. (a) Third-order correlation curves of the initial pulse (black) and the 910 nm pulse (red); (b) third-order correlation curve of the laser pulse after a one-stage OPCPA system.
    Yanyan Li, Beijie Shao, Yujie Peng, Junyu Qian, Wenkai Li, Xinliang Wang, Xingyan Liu, Xiaoming Lu, Yi Xu, Yuxin Leng, Ruxin Li. Ultra-broadband pulse generation via hollow-core fiber compression and frequency doubling for ultra-intense lasers[J]. High Power Laser Science and Engineering, 2023, 11(1): 010000e5
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