• High Power Laser Science and Engineering
  • Vol. 6, Issue 2, 02000e23 (2018)
Xiong Shen1、2, Peng Wang1、2, Jun Liu1、3、*, and Ruxin Li1、3
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3IFSA Collaborative Innovation Center, Shanghai Jiao Tong University, Shanghai 200240, China
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    DOI: 10.1017/hpl.2018.12 Cite this Article Set citation alerts
    Xiong Shen, Peng Wang, Jun Liu, Ruxin Li. Linear angular dispersion compensation of cleaned self-diffraction light with a single prism[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e23 Copy Citation Text show less
    Experimental setup for self-diffraction signal generation and temporal contrast measurement. BS: beam splitter; M1–M6: reflective mirrors; CL1, CL2: plane-convex cylindrical lenses, mm; P1: 0.15 mm thick fused silica plate; A: aperture; CM1: cylindrical reflective mirror, mm; C1: spherical concave reflective mirror, mm; C2: spherical convex reflective mirror, mm; VND: 2 mm thick variable neutral-density filter; P2: 1 mm thick fused silica plate; correlator: third-order cross-correlator (Amplitude Technologies Inc., Sequia 800).
    Fig. 1. Experimental setup for self-diffraction signal generation and temporal contrast measurement. BS: beam splitter; M1–M6: reflective mirrors; CL1, CL2: plane-convex cylindrical lenses,  mm; P1: 0.15 mm thick fused silica plate; A: aperture; CM1: cylindrical reflective mirror,  mm; C1: spherical concave reflective mirror,  mm; C2: spherical convex reflective mirror,  mm; VND: 2 mm thick variable neutral-density filter; P2: 1 mm thick fused silica plate; correlator: third-order cross-correlator (Amplitude Technologies Inc., Sequia 800).
    The temporal contrast of the input pulse and the generated first-order SD signal. The inset is an enlarged part of the curves from ps to 3 ps.
    Fig. 2. The temporal contrast of the input pulse and the generated first-order SD signal. The inset is an enlarged part of the curves from  ps to 3 ps.
    Scheme of angular dispersion generation.
    Fig. 3. Scheme of angular dispersion generation.
    (a) The spectra of the incident pulse and the first-order SD signal ; (b) the spectra at 30 different positions, the inset shows the center wavelengths measured at each position.
    Fig. 4. (a) The spectra of the incident pulse and the first-order SD signal ; (b) the spectra at 30 different positions, the inset shows the center wavelengths measured at each position.
    Scheme of angular dispersion compensation.
    Fig. 5. Scheme of angular dispersion compensation.
    (a) Scheme of prism dispersion; (b) the relationship between the incident angle and the dispersion angle of pulses with nm and nm; (c) spectra of compensated SD signal.
    Fig. 6. (a) Scheme of prism dispersion; (b) the relationship between the incident angle and the dispersion angle of pulses with  nm and  nm; (c) spectra of compensated SD signal.
    Xiong Shen, Peng Wang, Jun Liu, Ruxin Li. Linear angular dispersion compensation of cleaned self-diffraction light with a single prism[J]. High Power Laser Science and Engineering, 2018, 6(2): 02000e23
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