Author Affiliations
1Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China2National Laboratory on High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China3University of Chinese Academy of Sciences, Beijing 100049, Chinashow less
Fig. 1. (a) Structure of the LC binary mask (1 – anti-reflection coating, 2 – front glass substrate, 3 – anti-reflection coating, 4 – polyimide layer, 5 – LC molecule, 6 – azobenzene group, 7 – photoalignment layer, 8 – anti-reflection coating, 9 – rear glass substrate and 10 – anti-reflection coating) and (b) arrangement of LC molecules in a single pixel of two pixel types (1 – incident light, 2 – polarizer, 3 – P-polarized light, 4 – front glass substrate with coating polyimide, 5 – LC molecule, 6 – rear glass substrate with coating azobenzene, 7 – P-polarized light, 8 – polarizer, 9 – output light and 10 – S-polarized light).
Fig. 2. Fabrication process of the LC cell.
Fig. 3. Photolithography mask system (1 – light source, 2 – collimating lens, 3 – polarization beam splitter, 4 – LCOS, 5 – imaging system (1:1) and 6 – LC cell).
Fig. 4. Designed objective function $y=0.8x^{2}+0.2$. (a) Binary distribution of the mask; the unit pixel is $40~\unicode[STIX]{x03BC}\text{m}$. (b) Spatial distribution of the objective function.
Fig. 5. Beam shaping test system (1 – laser source, 2 – single mode fiber, 3 – fiber port, 4 – beam expander ($20\times$), 5 – polarization beam splitter, 6 – LC binary mask, 7 – polarization beam splitter, 8 – plano-convex lens, 9 – mirror, 10 – pinhole, 11 – mirror, 12 – plano-convex lens and 13 – CCD).
Fig. 6. Physical LC binary mask. (a) Boundary dimension of the physical LC binary mask. (b) Parabolic pixel distribution is observed in polarized white light. (c) Regional area of the pixel structure examined under a crossed polarizer microscope ($50\times$).
Fig. 7. Parabolic shaping of the LC binary mask (curve 1 is the designed objective function, curve 2 was tested at the completed mask; curve 3 is the transmission curve of the same tested mask, which has been stored for six months in a conventional storage).
Fig. 8. Square soft edge diaphragm of the LC binary mask.
Fig. 9. Logo picture of ‘SIOM’ (the size of the picture is 8 mm $\times$ 8 mm; (a) designed picture and (b) picture written on the LC cell).
Fig. 10. Results of written and erased situation. (a) First lithography. (b) Third lithography on the same LC cell. (c) Fifth lithography on the same LC cell. (d) Sixth lithography on the same LC cell. (e) The LC cell erased by a linearly polarized blue light of 10 mW for 5 minutes after the sixth writing. (f) The LC cell erased at the power of 10 mW for extra 3 hours after (e).
Substrate | Laser damage threshold@1064 nm, 10 ns, 1 Hz |
---|
K9 glass 1 | $62.5385~\text{J}/\text{cm}^{2}$ | K9 glass 2 | $62.9698~\text{J}/\text{cm}^{2}$ | Ultraclear float glass | $54.34~\text{J}/\text{cm}^{2}$ |
|
Table 1. Laser damage thresholds of the azobenzene-based photoalignment layers.
Material | Laser damage |
---|
| threshold@1064 nm, 10 ns, 1 Hz |
---|
LC ($d\sim 5~\unicode[STIX]{x03BC}\text{m}$) | $18~\text{J}/\text{cm}^{2}$ | Polyimide ($d=50~\text{nm}$) | $15~\text{J}/\text{cm}^{2}$ | Chemical anti-reflection film | $30~\text{J}/\text{cm}^{2}$ | Inorganic anti-reflection film | $15~\text{J}/\text{cm}^{2}$ | Glass substrate (K9) | $50~\text{J}/\text{cm}^{2}$ |
|
Table 2. Laser damage thresholds of the LC binary mask materials.