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Axially-symmetric sheared polymer network liquid crystals

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Abstract

An axially-symmetric sheared polymer network liquid crystal (SPNLC) device is demonstrated and its performances characterized. Through analyzing the structure of this axially-symmetric SPNLC, we constructed a 3-D model to explain the observed phenomena. The simulation results agree well with the experiment. Two potential applications of such an axially-symmetric SPNLC, namely tunable-focus negative lens and spatial polarization converter, are discussed.

©2005 Optical Society of America

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Supplementary Material (2)

Media 1: MPG (492 KB)     
Media 2: MPG (443 KB)     

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Figures (9)

Fig. 1.
Fig. 1. SPNLC structure observed under crossed polarizers.
Fig. 2.
Fig. 2. Voltage-dependent transmittance of the axially symmetric SPNLC cell. d=9 µm and λ=633 nm.
Fig. 3.
Fig. 3. Optical response time of the 9-µm axially-symmetric SPNLC: (a) rise time, and (b) decay time.
Fig. 4.
Fig. 4. (a) Top view and cross-section of the LC structure; (b) Measured gradient distribution of the phase retardation.
Fig. 5.
Fig. 5. Simulated pretilt angle distribution of the axially-symmetric SPNLC cell.
Fig. 6.
Fig. 6. Measured V-T curves at different positions of the axially-symmetric SPNLC cell.
Fig. 7.
Fig. 7. Measured response time at different positions of the axially-symmetric SPNLC cell.
Fig. 8.
Fig. 8. (a) A movie shows the real dynamic image of the axially-symmetric SPNLC cell (492KB), and (b) Simulation results (443KB).
Fig. 9.
Fig. 9. (a) Incident light with vertical linear polarization, (b) Rotationally symmetric half wave plate, and (c) Output light with polarization P=2 field.
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