Photonics Research, 2019, 7 (11): 11001340, Published Online: Nov. 1, 2019
Dual waveband generator of perfect vector beams Download: 654次
Figures & Tables
Fig. 1. Schematic of the experimental setup. GT prism, Glan–Taylor prism; HWP, half wave plate; QWP 1 , QWP 2 , and QWP 3 , quarter wave plates; PBS, polarized beam splitter; M 1 , M 2 , M 3 , and M 4 , mirrors; SPP, spiral phase plate; S 1 and S 2 , 5% (mole fraction) MgO : LiNbO 3 ; DM, dichroic mirror; L 1 and L 2 , lens with focal length f = 200 mm ; SF 1 and SF 2 , spatial filters; CCD 1 and CCD 2 , charge coupled devices. Insets (a) and (b) represent the spatial intensity and polarization distributions of the simulated FF and SH PV beams, respectively.
Fig. 2. (a) and (b) The simulated and experimental intensity distributions of the FF PV beams with TC l = 1 . (a1)–(a9) Simulated intensity profile of the FF PV beams when the GT prism has different polarization angles (0°, 20°, 40°, 60°, 80°, 100°, 120°, 140°, 160°) with respect to the positive horizontal direction. (b1)–(b9) are the corresponding experimental results.
Fig. 3. (a) and (b) The simulated and experimental intensity distributions of the PV beams at the SH waveband. (a1)–(a9) Simulated intensity profiles of the generated PV beams when the GT prism has different polarization angles (0°, 20°, 40°, 60°, 80°, 100°, 120°, 140°, 160°) with respect to the positive horizontal direction. (b1)–(b9) are the corresponding experimental results.
Fig. 4. First and third rows are, respectively, the experimental results of the FF PV beams with δ / 2 + 2 γ = π / 3 and δ / 2 + 2 γ = 2 π / 3 . The second and fourth rows are, respectively, the SH PV beam patterns corresponding to the FF ones. Arrows in the figures show the polarization angles (0°, 45°, 90°, 135°) of the GT prism with respect to the positive horizontal direction.
Hui Li, Haigang Liu, Xianfeng Chen. Dual waveband generator of perfect vector beams[J]. Photonics Research, 2019, 7(11): 11001340.