US4036553A
Expired / Lapsed
US
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Method of controlling an optical characteristic
Assignee: Commissariat à l'Énergie Atomique et Aux Énergies Alternatives
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Filing: 1975-03-03
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Granted: 1977-07-19
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Expires: 1995-03-03
Abstract
Abstract The invention relates to a method of controlling an optical characteristic of a material and it is concerned also with devices and image-forming means for carrying out the method. The method of control is particularly advantageous in devices comprising a plurality of points distributed in the form of a matrix. The optical characteristic K of the material is controlled by an energization having a magnitude G for a duration t, the values G and t being so selected as a function of the time response K (G, t) of the characteristic K at an energization stage of magnitude G that K (G O , t O ) is equal to K O .
Inventors
- 👤 Joseph Borel
- 👤 Jean-Claude Deutsch
- 👤 Guy Labrunie
- 👤 Jacques Robert
Bibliographic Details
Application Number
—
Jurisdiction
US
Data Source
google_patents
Last Synchronized
2026-10-25 16:00
CPC Classifications
G; G09; G09F; G09F9/00; G09F9/30; G09F9/37; G09F9/372; G02; G02F; G02F1/00; G02F1/01; G02F1/13; G02F1/133; G02F1/13306; Y; Y10; Y10S; Y10S359/00; Y10S359/90
Claims Analysis
Total Claims: 3
Claim 1
Independent Claim
238 words
A method of controlling the optical index of the points of a liquid crystal layer to a desired value n 0 , said layer comprising a plurality of points, with an electric field, the application of an electric field of amplitude E 0 at a point causing the appearance of an electric field of amplitude E' 0 at some of the adjacent points, comprising the steps of: determining the transitory response n (E,t) of the liquid crystal index n at an electric field of amplitude E,t being the duration of application of said electric field, selecting a pair of values E 0 and t 0 from said transitory response so that the index n (E 0 , t 0 ) at said point obtained after the application of an electric field of amplitude E 0 for a duration t 0 is equal to a desired value n 0 , and so that the index n (E' 0 , t 0 ) at said adjacent points obtained under the influence of the electric field of amplitude E' 0 for said duration t 0 differs only slightly from the index value before the electric field is applied and applying to said liquid crystal at said points, said electrical field of amplitude E 0 for a duration t 0 , to obtained said desired value n 0 at said points and to maintain unchanged the optical index at said adjacent points.
Claim 2
Independent Claim
238 words
A method of controlling the optical index of the points of a liquid crystal layer to a desired value n 0 , said layer comprising a plurality of points, with an electric field, the application of an electric field of amplitude E 0 at a point causing the appearance of an electric field of amplitude E' 0 at some of the adjacent points, comprising the steps of: determining the transitory response n (E,t) of the liquid crystal index n at an electric field of amplitude E,t being the duration of application of said electric field, selecting a pair of values E 0 and t 0 from said transitory response so that the index n (E 0 , t 0 ) at said point obtained after the application of an electric field of amplitude E 0 for a duration t 0 is equal to a desired value n 0 , and so that the index n (E' 0 , t 0 ) at said adjacent points obtained under the influence of the electric field of amplitude E' 0 for said duration t 0 differs only slightly from the index value before the electric field is applied and applying to said liquid crystal at said points, said electrical field of amplitude E 0 for a duration t 0 , to obtained said desired value n 0 at said points and to maintain unchanged the optical index at said adjacent points.
Claim 3
Dependent Claim
59 words
A method as set forth in claim 1, characterized in that the optical index of the points of said plurality is controlled sequentially, the time taken for controlling all the points being less than the time needed for said index of the liquid crystal to resume its value at rest after the electric field has ceased to be applied.
References Cited (Backward Citations)
No citation records indexed.
USPTO Annuity & Maintenance Windows
| Annuity Stage | Window Opens | Payment Deadline | Surcharge Period Until | Estimated Fee | Status |
|---|---|---|---|---|---|
| 3.5 Years (Year 4) | 1980-07-18 | 1981-01-17 | 1981-07-19 | $2000.00 | Window Closed / Lapsed |
| 7.5 Years (Year 8) | 1984-07-18 | 1985-01-17 | 1985-07-19 | $3760.00 | Window Closed / Lapsed |
| 11.5 Years (Year 12) | 1988-07-18 | 1989-01-17 | 1989-07-19 | $7700.00 | Window Closed / Lapsed |