High Power Laser Science and Engineering, Volume. 6, Issue 2, 02000e23(2018)
Linear angular dispersion compensation of cleaned self-diffraction light with a single prism
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).
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.
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.
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.
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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
Received: Nov. 2, 2017
Accepted: Feb. 9, 2018
Published Online: Jul. 4, 2018
The Author Email: Jun Liu (jliu@siom.ac.cn)