• High Power Laser Science and Engineering
  • Vol. 7, Issue 2, 02000e32 (2019)
Pengfei Wang1、2, Beijie Shao1、2, Hongpeng Su1、2, Xinlin Lv1、2, Yanyan Li1, Yujie Peng1, and Yuxin Leng1、†
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.1017/hpl.2019.19 Cite this Article Set citation alerts
    Pengfei Wang, Beijie Shao, Hongpeng Su, Xinlin Lv, Yanyan Li, Yujie Peng, Yuxin Leng. High-repetition-rate, high-peak-power 1450 nm laser source based on optical parametric chirped pulse amplification[J]. High Power Laser Science and Engineering, 2019, 7(2): 02000e32 Copy Citation Text show less
    Schematic of the OPCPA setup. DL, delay line; TFP, thin film polarizer at 1064 nm; DM, dichroic mirror; BS, beam splitter; HWP, half-wave plate; WLC, white-light continuum; Sa, sapphire; RM, roof mirror; IR, image relay; OAP, off-axis parabolic mirror; VDF, variable density filter; T, telescope; PC, computer.
    Fig. 1. Schematic of the OPCPA setup. DL, delay line; TFP, thin film polarizer at 1064 nm; DM, dichroic mirror; BS, beam splitter; HWP, half-wave plate; WLC, white-light continuum; Sa, sapphire; RM, roof mirror; IR, image relay; OAP, off-axis parabolic mirror; VDF, variable density filter; T, telescope; PC, computer.
    Spectrum evolution through the OPCPA system. Insert, near-field beam profile after the second KTA crystal, as measured by a pyroelectric thermal camera (PyroCAM) with a spatial resolution of $80~\unicode[STIX]{x03BC}\text{m}$.
    Fig. 2. Spectrum evolution through the OPCPA system. Insert, near-field beam profile after the second KTA crystal, as measured by a pyroelectric thermal camera (PyroCAM) with a spatial resolution of $80~\unicode[STIX]{x03BC}\text{m}$.
    Energy fluctuation of compressed pulses at 1450 nm.
    Fig. 3. Energy fluctuation of compressed pulses at 1450 nm.
    Temporal characterization of the compressed pulse. (a) Measured and (b) retrieved SHG-FROG traces; (c) reconstructed pulse envelope (blue), which is 60 fs (FWHM), phase (green) and its TL pulse (red); (d) reconstructed spectrum (blue), phase (green) and measured spectrum (red) obtained by a near-infrared spectrometer (NIR-Quest from Ocean Optics).
    Fig. 4. Temporal characterization of the compressed pulse. (a) Measured and (b) retrieved SHG-FROG traces; (c) reconstructed pulse envelope (blue), which is 60 fs (FWHM), phase (green) and its TL pulse (red); (d) reconstructed spectrum (blue), phase (green) and measured spectrum (red) obtained by a near-infrared spectrometer (NIR-Quest from Ocean Optics).
    (a) Amplified signal energy as a function of pump energy (seed energy fixed) of the first (insert) and the second OPA stages. (Black) Seed energy fixed at $30~\unicode[STIX]{x03BC}\text{J}$. (Red) Seed energy fixed at $55~\unicode[STIX]{x03BC}\text{J}$. (b) Amplified signal (black dots) and idler (red dots) energies as functions of pump energy in the second OPA stage (the energy of the first amplified signal is fixed at 4.9 mJ).
    Fig. 5. (a) Amplified signal energy as a function of pump energy (seed energy fixed) of the first (insert) and the second OPA stages. (Black) Seed energy fixed at $30~\unicode[STIX]{x03BC}\text{J}$. (Red) Seed energy fixed at $55~\unicode[STIX]{x03BC}\text{J}$. (b) Amplified signal (black dots) and idler (red dots) energies as functions of pump energy in the second OPA stage (the energy of the first amplified signal is fixed at 4.9 mJ).
    Pengfei Wang, Beijie Shao, Hongpeng Su, Xinlin Lv, Yanyan Li, Yujie Peng, Yuxin Leng. High-repetition-rate, high-peak-power 1450 nm laser source based on optical parametric chirped pulse amplification[J]. High Power Laser Science and Engineering, 2019, 7(2): 02000e32
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