Author Affiliations
1School of Physics and Engineering, Zhengzhou University, Zhengzhou 450001, China2Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang 621900, China3School of Optoelectronic Information, University of Electronic Science and Technology of China, Chengdu 610054, Chinashow less
Fig. 1. Transmittance for SZPs with the topological charge p=1 in (a) the (x, y) coordinate system and (b) the (r2, θ) coordinate system. Transmittance for ALFSZPs with the topological charge p=1 in (c) the (x, y) coordinate system and (d) the (r2, θ) coordinate system.
Fig. 2. Schematic diagram of diffraction by the ALFSZPs.
Fig. 3. (a) The calculated axial irradiance of conventional SZPs; (b) the calculated axial irradiance of ALFSZPs with focal depths from 450 to 550 mm, Δf=100 mm, N=699, and Δd=0.0858 μm2; (c) the calculated axial irradiance of ALFSZPs with focal depths from 475 to 525 mm, Δf=50 mm, N=699, and Δd=0.0429 μm2; (d) the calculated axial irradiance of ALFSZPs with focal depths from 475 to 525 mm, Δf=50 mm, N=349, and Δd=0.0858 μm2.
Fig. 4. (a), (b), and (c) Calculated diffraction patterns of ALFSZPs at the positions of 450, 500, and 550 mm. (d), (e), and (f) Calculated diffraction patters of conventional SZPs with the same parameters at the positions of 450, 500, and 550 mm.
Fig. 5. ALFSZPs with different integer topological charges and axial irradiances from 450 to 550 mm. (a), (b) The topological charge p=0. (c), (d) The topological charge p=1. (e), (f) The topological charge p=2.