• Photonics Research
  • Vol. 9, Issue 4, 477 (2021)
Junyu Qian1、2、†, Pengfei Wang1、2、†, Yujie Peng1、*, Yanyan Li1, Beijie Shao1、2, Hongpeng Su1、2, Xinlin Lv1、2, Ding Wang1, Yuxin Leng1、3, and Ruxin Li1、4
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 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3e-mail: lengyuxin@mail.siom.ac.cn
  • 4e-mail: ruxinli@mail.shcnc.ac.cn
  • show less
    DOI: 10.1364/PRJ.415794 Cite this Article Set citation alerts
    Junyu Qian, Pengfei Wang, Yujie Peng, Yanyan Li, Beijie Shao, Hongpeng Su, Xinlin Lv, Ding Wang, Yuxin Leng, Ruxin Li. Pulse combination and compression in hollow-core fiber for few-cycle intense mid-infrared laser generation[J]. Photonics Research, 2021, 9(4): 477 Copy Citation Text show less
    Schematic of the 4 μm OPCPA system and the HCF-based CBC system. KTA, KTiOAsO4 crystal; DL, delay line; HWP, half-wave plate; TFP, thin film polarizer; DM, dichroic mirror; T, telescope; W, CaF2 window; IR, image relay; BS, beam splitter; RM, roof mirror; G, grating; KEPM, knife edge prism mirror; L, lens; Kr, krypton.
    Fig. 1. Schematic of the 4 μm OPCPA system and the HCF-based CBC system. KTA, KTiOAsO4 crystal; DL, delay line; HWP, half-wave plate; TFP, thin film polarizer; DM, dichroic mirror; T, telescope; W, CaF2 window; IR, image relay; BS, beam splitter; RM, roof mirror; G, grating; KEPM, knife edge prism mirror; L, lens; Kr, krypton.
    (a) Spectra measured by MOZZA and (b) corresponding temporal profiles measured by SHG-FROG at different krypton pressures. (c) Spectral evolution throughout increasing gas pressures output from the HCF measured by SHG-FROG. (d) The measured compressed pulse durations with 2 mm CaF2 (blue curve), corresponding FTL duration (green curve), and estimated FTL duration (red curve) for different krypton pressures. Dashed line represents 26 fs, corresponding to two optical cycles for 4 μm laser pulse.
    Fig. 2. (a) Spectra measured by MOZZA and (b) corresponding temporal profiles measured by SHG-FROG at different krypton pressures. (c) Spectral evolution throughout increasing gas pressures output from the HCF measured by SHG-FROG. (d) The measured compressed pulse durations with 2 mm CaF2 (blue curve), corresponding FTL duration (green curve), and estimated FTL duration (red curve) for different krypton pressures. Dashed line represents 26 fs, corresponding to two optical cycles for 4 μm laser pulse.
    Temporal and spectral characterizations of the compressed pulse. (a) Measured and (b) reconstructed SHG-FROG traces. (c) Blue curve, pulse temporal profile of 22.9 fs duration (FWHM); green curve, retrieved phase. (d) Blue curve, reconstructed spectrum of SHG-FROG; red curve, directly measured spectrum by MOZZA; green curve, retrieved phase.
    Fig. 3. Temporal and spectral characterizations of the compressed pulse. (a) Measured and (b) reconstructed SHG-FROG traces. (c) Blue curve, pulse temporal profile of 22.9 fs duration (FWHM); green curve, retrieved phase. (d) Blue curve, reconstructed spectrum of SHG-FROG; red curve, directly measured spectrum by MOZZA; green curve, retrieved phase.
    (a) Beam profiles before the lens L7. Beam profiles at the focal plane of L7 with the relative phase of the individual pulses (b) Δϕ=π and (c) Δϕ=0. (d) Beam profiles at the HCF output window. The beam profile is measured by a pyroelectric thermal camera (PyroCAM IV) with a resolution of 80 μm. (e) Michelson-type interferometer for the measurement of temporal coherence of the compressed pulse and (f) the measured interference fringes. (g) Michelson-type interferometer for the measurement of spatial coherence of the compressed pulse and (h) the measured interference fringes. D, D-shape mirror; DL, delay line; BS, beam splitter.
    Fig. 4. (a) Beam profiles before the lens L7. Beam profiles at the focal plane of L7 with the relative phase of the individual pulses (b) Δϕ=π and (c) Δϕ=0. (d) Beam profiles at the HCF output window. The beam profile is measured by a pyroelectric thermal camera (PyroCAM IV) with a resolution of 80 μm. (e) Michelson-type interferometer for the measurement of temporal coherence of the compressed pulse and (f) the measured interference fringes. (g) Michelson-type interferometer for the measurement of spatial coherence of the compressed pulse and (h) the measured interference fringes. D, D-shape mirror; DL, delay line; BS, beam splitter.
    Junyu Qian, Pengfei Wang, Yujie Peng, Yanyan Li, Beijie Shao, Hongpeng Su, Xinlin Lv, Ding Wang, Yuxin Leng, Ruxin Li. Pulse combination and compression in hollow-core fiber for few-cycle intense mid-infrared laser generation[J]. Photonics Research, 2021, 9(4): 477
    Download Citation