Polymer dispersed liquid crystal film devices, and method of forming the same

• US 4,938,568 A
• Filed: 01/05/1988
• Issued: 07/03/1990
• Est. Priority Date: 01/05/1988
• Status: Expired due to Term

• Current Assignee: Delco Electronics Corporation (General Motors Company), General Motors Corporation (General Motors Company), Victor Company of Japan Limited (JVC Kenwood Corporation)
• Original Assignee: Hughes Aircraft Company (Rtx Corporation)
• Inventors: Smith, George W., Kohler, James L., Lackner, Anna M., Margerum, John D., Allison, Charles R., Vaz, Nuno A., Ramos, Elena
• Primary Examiner(s): Miller, Stanley D.
• Assistant Examiner(s): GROSS, ANITA P
• Application Number:
  US07/141,033
• Time in Patent Office: 910 Days
• Field of Search: 350/320, 350/347 V, 350/348, 350/351, 350/334, 427/213.3, 427/213.33, 427/213.34, 427/213.35
• US Class Current: 349/201
• CPC Class Codes: C09K 19/544 as dispersing or encapsulating medium around the liquid crystal
• CPC Class Codes: G02F 1/1334 based on polymer dispersed liquid crystals, e.g. microencapsulated liquid crystals
• CPC Class Codes: Y10S 359/90 Methods

Abstract

A method of forming a polymer dispersed liquid crystal (PDLC) film is disclosed which consists of forming a solution of LC dissolved in a monomer, photopolymerizing the solution to form a film having a dispersion of LC bubbles therein, establishing a correlation between the LC bubble size and selected characteristics of the film, selecting a LC bubble size corresponding to desired film characteristics, and controlling the conditions of photopolymerization to achieve said LC bubble size. The LC bubble size is controlled by means of the UV exposure intensity, exposure temperature, exposure wavelength, LC concentration and/or concentration of polymerization initiator. Correlations are noted between LC bubble size and the resulting film'"'"'s threshold and operating voltages for optical transmission, contrast ratio, absolute transmissivity and electro-optical response times. Special types of films, including in situ gratings and holograms, are obtained by periodically varying the conditions of polymerization over the film to produce a corresponding periodic spatial variation in the LC bubble size; different processes used to achieve this result are noted. Films with LC bubbles in a new size regime that significantly decreases the operating voltage threshold, and with gradients in the bubble size, are also disclosed.

Claims

1. A method of controlling the electro-optical properties of a polymer dispersed liquid crystal (LC) film, comprising:

forming a solution of a LC dissolved in a polymerizable monomer system,

photopolymerizing said solution to form a polymerized film having a dispersion of LC bubbles therein, and

spatially varying the conditions of polymerization over said film to spatially vary the sizes of said LC bubbles therein.

2. The method of claim 1, wherein said photopolymerization is accomplished by ultraviolet light exposure of said solution, and the conditions of polymerization are spatially varied by spatially varying the exposure intensity and/or exposure temperature over the film.

3. The method of claim 2, wherein the exposure intensity is spatially varied by exposing the film through a mask having a spatial variation in transmissivity.

4. The method of claim 3, wherein said mask is at least partially transmissive or said spatial variation in transmissivity, thereby enabling substantially the entire film to polymerize at generally the same time but at spatially varying polymerization rates corresponding to the spatial variation in mask transmissivity.

5. The method of claim 3, wherein the solution is polymerized in a two-step polymerization process comprising an exposure through said mask at one exposure intensity in one step, and an exposure without the mask at a different exposure intensity in another step.

6. The method of claim 2, wherein the exposure intensity is spatially varied in a periodic fashion to form diffraction gratings within the film.

7. The method of claim 2, wherein the solution is exposed by directing a pair of laser beams onto the solution at angles which produce a holographic interference pattern in the film.

8. The method of claim 2, wherein a spatial gradient is established in the exposure intensity to produce a corresponding spatial gradient in the LC bubble size within the film.

9. The method of claim 8, wherein said spatial gradient is established by employing a polymerization wavelength at which the components progressively absorb substantial amounts of the ultraviolet light during transit through said solution, resulting in larger LC bubbles in the back part of the film.