High Power Laser Science and Engineering, Volume. 7, Issue 2, 02000e32(2019)
High-repetition-rate, high-peak-power 1450 nm laser source based on optical parametric chirped pulse amplification
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.
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
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).
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
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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
Special Issue: HIGH ENERGY DENSITY PHYSICS AND HIGH POWER LASERS
Received: Sep. 20, 2018
Accepted: Apr. 8, 2019
Published Online: May. 29, 2019
The Author Email: Yuxin Leng (lengyuxin@mail.siom.sc.cn)