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Switchable Fresnel lens using polymer-stabilized liquid crystals

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Abstract

A switchable Fresnel zone plate lens is demonstrated using a polymer-stabilized liquid crystal. The fabrication process is relatively simple and the device can be operated below 10 volts with fast response time. Such a device works well for a linearly polarized light.

©2003 Optical Society of America

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Figures (8)

Fig. 1.
Fig. 1. Schematic representation of the photomask patterns and the corresponding LC arrangement of the PSLC Fresnel lens.
Fig. 2.
Fig. 2. Microscope images of the PSLC cell at (a) V=0, (b) 4 Vrms, (c) 7 Vrms, and (d) 10 Vrms. The LC cell is sandwiched between crossed polarizers.
Fig. 3.
Fig. 3. The experimental setup for studying the focusing properties of the PSLC Fresnel lens. L1: focal length 50 mm, L2: focal length 250 mm, and P: 30 µm pinhole.
Fig. 4.
Fig. 4. The observed laser beam images: (a) without LC sample, (b) with sample at V=0, and (c) with LC sample at 8 Vrms. λ=633 nm.
Fig. 5.
Fig. 5. The observed laser beam images (a) at V=0 and (b) at 8 Vrms. λ=633 nm. The CCD camera was 27 cm away from the sample
Fig. 6.
Fig. 6. Beam intensity profile measured by the CCD camera at V=8Vrms. The diameter of the Fresnel zone plate is 1 cm and the focal length is 50 cm.
Fig. 7.
Fig. 7. Beam intensity profiles at (a) V=0, (b) 8 Vrms, and (c) 20 Vrms. The diameter of the Fresnel zone plate is 1 cm and the focal length is 50 cm.
Fig. 8.
Fig. 8. The voltage-dependent diffraction efficiency of the PSLC Fresnel lens. LC: MLC-6252, cell gap d=5 µm, and monomer concentration 5%.
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