Fig. 1. Pictures of rainbow holographic master masks. (a) Light pillar rainbow holographic master masks; (b) plain rainbow holographic master masks
Fig. 2. Microstructures of different plain rainbow holographic materials with enlargement of 24000 times. (a)-(d) Planar figures of micro-structures of plain rainbow holographic master masks A, B, C, and D; (e)-(h) solid figures of micro-structures of plain rainbow holographic master masks A, B, C, and D
Fig. 3. Visual appearance and microstructures at different positions of light pillar rainbow holographic material. (a) Visual appearance; (b) microstructures at different positions
Fig. 4. Diagrams of geometric measurement conditions of different spectrophotometers. (a) Multi-angle spectrophotometer; (b) 45/0 spectrophotometer
Fig. 5. Measurement results of multi-angle spectrophotometer in condition of 45/0. (a)-(d) Spectral intensity from plain rainbow holographic master masks A, B, C, and D in the directions of 0°-45°; (e)-(h) spectral intensity from plain rainbow holographic master masks A, B, C, and D in the directions of 50°-90°
Fig. 6. Results of SpectroEye measurement for each plain rainbow holographic master mask. (a) Mask A; (b) mask B; (c) mask C; (d) mask D
Fig. 7. Diagram of diffraction direction of incident light
[8] Fig. 8. Results of the SpectroEye measurement for the light pillar rainbow holographic master masks
Fig. 9. Spectral power distribution of scanner’s light source
Fig. 10. Schematic of scanning optical path of scanner
Fig. 11. Colors of different plain rainbow holographic master masks versus rotation angle. (a) Mask A; (b) mask B; (c) mask C; (d) mask D
Fig. 12. Relationship between grating constant and incident angle for plain rainbow holographic materials
Plain rainbow master mask | λ1 | d1 | λ2 | d2 |
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A | 0.69-0.71 | 0.99±0.01 | 0.48-0.49 | 0.97±0.01 | B | 0.60-0.62 | 0.87±0.02 | 0.38-0.40 | 0.78±0.01 | C | 0.59-0.60 | 0.84±0.01 | 0.41-0.42 | 0.83±0.01 | D | 0.68-0.70 | 0.98±0.01 | 0.49-0.50 | 0.99±0.01 |
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Table 1. Grating constants corresponding to different peak wavelengthsμm
Plain rainbow master mask | d /μm | Color |
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0°-5° | 5°-40° | 40°-45° | 50°-80° | 85°-90° |
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A (D) | 1.01-1.05 | Blue | Rainbow | Red+Green | Rainbow | Blue | B (C) | 0.84-0.85 | Blue | Rainbow | Blue+Green | Rainbow | Blue |
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Table 2. Scanning color informations of different plain rainbow holographic master masks
Plain rainbow master mask | d /μm | Diffraction maximum wavelength /nm |
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0°-5° (85°-90°) | 40°-45° |
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A | 1.00 | 406.7-484.8 | 575.2-685.6 | B | 0.85 | 345.7-412.1 | 488.8-583.1 | C | 0.85 | 345.7-412.1 | 488.8-583.1 | D | 1.00 | 406.7-484.8 | 575.2-685.6 |
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Table 3. Results of diffraction maximum wavelength of different plain rainbow holographic master masks
Waveband /nm | Color sense |
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380-470 | Blue | 470-500 | Cyan | 500-530 | Green | 530-560 | Yellow-Green | 560-590 | Yellow | 590-620 | Orange | 620-700 | Red |
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Table 4. Color senses corresponding to different wavebands
Plain rainbow master mask | i /(°) | Grating constant /μm | d(range) /μm | d /μm |
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0° (position) | 45° (position) |
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Blue(380-470 nm) | Yellow-Green+Yellow(530-590 nm) | Blue-Green+Green(470-530 nm) | A, D | 24 | 0.93-1.16 | 0.92-1.03 | — | 0.93-1.03 | 0.98±0.05 | 29 | 0.78-0.97 | 0.77-0.86 | — | B, C | 24 | NaN | — | 0.82-0.92 | 0.82-0.92 | 0.87±0.05 | 29 | 0.78-0.97 | — | 0.69-0.77 |
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Table 5. Calculated grating constants of plain rainbow holographic materials in directions of 0° and 45°
Position | i /(°) | d |
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0.85 μm | 0.95 μm | 1.0 μm | 1.1 μm | 1.2 μm | 1.3 μm |
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0° | 25 | | 0.402 | 0.423 | 0.465 | 0.507 | 0.549 | 30 | 0.425 | 0.475 | 0.500 | 0.550 | 0.600 | 0.650 | 45° | 25 | 0.508 | 0.568 | 0.598 | 0.657 | 0.717 | 0.778 | 30 | 0.601 | 0.672 | 0.707 | 0.778 | 0.424 | 0.460 |
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Table 6. Grating constants of plain rainbow holographic master masks at different wavelengths