Author Affiliations
1Key Lab of Modern Manufacture Quantity Engineering, School of Mechanical Engineering, Hubei University of Technology, Wuhan 430068, Hubei , China2School of Science, Hubei University of Technology, Wuhan 430068, Hubei , Chinashow less
Fig. 1. Schematic diagram of SLM filling structure
Fig. 2. Schematic diagrams of orthogonal phase grating.(a) Radial binary grating; (b) axial binary grating; (c) orthogonal phase grating
Fig. 3. Profile of orthogonal phase grating
Fig. 4. Orthogonal phase grating structure diagrams. (a) Orthogonal phase grating; (b) element structure of orthogonal grating
Fig. 5. Orthogonal grating results and their diffraction light intensity. (a) Orthogonal phase grating; (b) diffraction pattern of orthogonal phase grating
Fig. 6. Schematic diagrams of orthogonal phase grating with different grey levels. (a) Structural diagram of orthogonal phase gratings with different gray grades; (b) one-dimensional distribution of orthogonal phase grating
Fig. 7. Orthogonal phase gratings with different period and corresponding diffraction patterns. (a) Orthogonal phase gratings with different periods; (b) diffraction patterns corresponding to orthogonal phase gratings with different periods
Fig. 8. Orthogonal phase gratings with different phase modulation depth and corresponding diffraction patterns. (a) Structural diagrams of orthogonal phase gratings with different phase modulation depths; (b) diffraction patterns corresponding to orthogonal phase gratings with different phase modulation depth
Fig. 9. Variation of relative intensity of different diffraction orders varying with grey level
Fig. 10. Variation of diffraction efficiency of 1st order light varying with grey level
Fig. 11. Experimental results of diffraction for orthogonal phase gratings with different phase modulation depth
Fig. 12. Experimental results of relative intensity of different diffraction orders varying with grey level
| Intensity calculated by Eqs.(9)-(11) | Intensity calculated by Fourier transform |
---|
0 order | (0,1)order | (1,1)order | 0 order | (0,1)order | (1,1)order |
---|
0 | 1.0000 | 0 | 0 | 1.0000 | 0 | 0 | 0.25π | 0.8902 | 0.0148 | 0.006 | 0.8908 | 0.0147 | 0.0060 | 0.5π | 0.6250 | 0.0507 | 0.0205 | 0.6270 | 0.0502 | 0.0205 | 0.75π | 0.3598 | 0.0865 | 0.0351 | 0.3633 | 0.0858 | 0.0351 | π | 0.2500 | 0.1013 | 0.0411 | 0.2540 | 0.1005 | 0.0411 | 1.25π | 0.3598 | 0.0865 | 0.0351 | 0.3633 | 0.0858 | 0.0351 | 1.5π | 0.6250 | 0.0507 | 0.0205 | 0.6270 | 0.0502 | 0.0205 | 1.75π | 0.8902 | 0.0148 | 0.0060 | 0.8908 | 0.0147 | 0.0060 | 2π | 1.0000 | 0 | 0 | 1.0000 | 0 | 0 |
|
Table 1. Intensity of different orders calculated by Eqs. (9)-(11) and Fourier transform
| Intensity |
---|
Calculated by Eq.(18) | Experimental result |
---|
0 | 1.000 | 1.000 | 0.25π | 0.892 | 0.889 | 0.50π | 0.630 | 0.630 | 0.75π | 0.369 | 0.371 | π | 0.260 | 0.255 | 1.25π | 0.369 | 0.375 | 1.50π | 0.630 | 0.621 | 1.75π | 0.892 | 0.885 | 2.00π | 1.000 | 0.925 |
|
Table 2. Intensity of zero-orders calculated by Eq. (18) and experiments