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Proceedings of Topical Meeting on Optoinformatics (pdf-format, 1.21 ...

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SAINT-PETERSBURG, October 17 – 20, 2005 47<br />

The replicated hologram is obtained by the next technique, first a digital patter by<br />

computer simulati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> a Fourier hologram (figure 3) generated later with lithographic<br />

tools this is photoreduced to obtaining gray-scale transmissi<strong>on</strong> masks. The soluti<strong>on</strong> (Point<br />

4 KERR ®¨ modifiable resin) is poured by Spin coater <strong>on</strong> commune substrate then the mask<br />

is aligner with the layer resin that is cured by exposure to UV light, finally the mass takes<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g>f and the hologram pattern is transferred <strong>on</strong>to layer substrate without some develop<br />

process after that the hologram is rec<strong>on</strong>structed (figure 5).<br />

Figure 3. Microstructure Fourier<br />

Hologram<br />

Figure 4. Object used to obtain<br />

digital hologram<br />

Figure 5. Diffracti<strong>on</strong> pattern<br />

optical rec<strong>on</strong>structi<strong>on</strong><br />

Figure 7 shows the diffracti<strong>on</strong> efficiency <str<strong>on</strong>g>of</str<strong>on</strong>g> an absorpti<strong>on</strong> hologram as a functi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the<br />

energy. The diffracti<strong>on</strong> efficiency increased in functi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> the UV irradiance expositi<strong>on</strong>,<br />

the maximum efficiency is obtained at 40 sec<strong>on</strong>ds exposure time that corresp<strong>on</strong>d a 0.29<br />

joules/cm 2 <str<strong>on</strong>g>of</str<strong>on</strong>g> energy this is 82.7%, after that decrease.<br />

80<br />

Diffracti<strong>on</strong> efficiency(%)<br />

60<br />

40<br />

20<br />

0<br />

0.00 0.05 0.10 0.15 0.20 0.25 0.30 0.35 0.40 0.45<br />

Energy (Joules/cm 2 )<br />

Figure 6. Diffracti<strong>on</strong> pattern <str<strong>on</strong>g>of</str<strong>on</strong>g> a single grating<br />

Figure 7. Diffracti<strong>on</strong> efficiency <str<strong>on</strong>g>of</str<strong>on</strong>g> the grating array<br />

“The Point 4 KERR ® ” is a composite resin, this have a organic phase (matrix), the disperse<br />

phase (filler), and the interfacial phase coupling agent. This resin can be used as layer film<br />

and the method present in this paper is simple and faster for obtaining a replayed<br />

hologram.<br />

1. Tani Y, New technology <str<strong>on</strong>g>of</str<strong>on</strong>g> composite resins developed in Japan, Trans. Sec<strong>on</strong>d Int<br />

Cog Dent Mater 1993, 54-61.<br />

2. Ruyter IE, Oysaed H. Composite for use in posterior teeth: Compositi<strong>on</strong> and<br />

c<strong>on</strong>versi<strong>on</strong>, J Biomed mater Res 1987, 21(1), 11-23.<br />

3. Hosada H. Yamada, Inokoshi S. SEM and elemental analysis <str<strong>on</strong>g>of</str<strong>on</strong>g> composites resins. J<br />

Prosthet Dent 1990, 64(6), 669-676.<br />

4. Svetlana S. and Dejan P. Relief hologram replicati<strong>on</strong> using a dental composite as an<br />

embossing tool, Optics Express 2005, 13(7), 2747-2754.<br />

5. A Guide for using Point 4 Optimized Particle Composite System, Keer Corpotati<strong>on</strong>.

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