Ferroelectric liquid crystal optical device having temperature compensation

• US 4,902,107 A
• Filed: 05/15/1989
• Issued: 02/20/1990
• Est. Priority Date: 04/26/1985
• Status: Expired due to Term

• Current Assignee: Canon Kabushiki Kaisha (Canon Inc.)
• Original Assignee: Canon Kabushiki Kaisha (Canon Inc.)
• Inventors: Tsuboyama, Akira, Okada, Shinjiro, Enari, Masahiko, Taniguchi, Osamu
• Primary Examiner(s): Miller, Stanley D.
• Assistant Examiner(s): DUONG, TAI V
• Application Number:
  US07/352,609
• Time in Patent Office: 281 Days
• Field of Search: 350/331 T, 350/332, 350/333, 350/350 S, 350/337, 340/765, 340/784, 340/805, 340/811, 340/813
• US Class Current: 349/72
• CPC Class Codes: G02F 1/133382 Heating or cooling of liquid crystal cells other than for activation, e.g. circuits or arrangements for temperature control, stabilisation or uniform distribution over the cell
• CPC Class Codes: G09G 2310/06 Details of flat display driving waveforms
• CPC Class Codes: G09G 2320/041 Temperature compensation
• CPC Class Codes: G09G 3/3629 using liquid crystals having memory effects, e.g. ferroelectric liquid crystals
• CPC Class Codes: G09G 3/3681 suitable for passive matrices only
• CPC Class Codes: G09G 3/3692 suitable for passive matrices only

Abstract

A liquid crystal device, includes: (a) a liquid crystal cell includes a pair of base plates, and a ferroelectric smectic liquid crystal having a negative dielectric anisotropy, (b) a device for applying to the ferroelectric liquid crystal an alternating electric field capable of causing the crystal to assume at least two stable orientation states including a first stable orientation state and a second stable orientation state, (c) a device for changing the frequency or voltage value of the alternating electric field corresponding to a temperature change, (d) a device for selectively applying a first electric field for orienting the ferroelectric liquid crystal to the first stable orientation state and a second electric field for orienting the ferroelectric liquid crystal to the second stable orientation state, and (e) a device for detecting an optical difference between light rays having passed through the ferroelectric liquid crystal oriented to the first orientation state and light rays having passed through the ferroelectric liquid crystal oriented to the second orientation state.

Claims

1. A liquid crystal optical device, comprising:

(a) a liquid crystal cell comprising a matrix electrode structure composed of a first group of electrodes and a second group of electrodes intersecting the first group of electrodes with a ferroelectric smectic liquid crystal having a negative dielectric anisotropy disposed between the first and second groups of electrodes;

(b) means for applying a scanning selection signal to at least one electrode of the first group of electrodes and a scanning nonselection signal to at least one of the other of the first group of electrodes;

(c) means for applying information signals in parallel to the second group of electrodes, said information signals being repeated alternating electric fields;

such that repeated alternating electric fields are applied to at least some intersections of the first group of electrodes and the second group of electrodes so as to place the ferroelectric smectic liquid crystal in a bistable memory orientation state with an increased tilt angle;

(d) means for raising the frequency of the alternating electric field in accordance with a temperature increase in said liquid crystal cell; and

(e) means for detecting an optical difference between light rays which have passed through the ferroelectric smectic liquid crystal oriented to a plurality of different orientation states.

2. A liquid crystal optical device according to claim 1, wherein said means for detecting an optical difference is a polarizer having a polarization axis substantially in parallel with the molecular axis of the ferroelectric liquid crystal oriented to one of the plurality of different orientation states.

3. A liquid crystal optical device according to claim 1, wherein said means for detecting an optical difference comprises a pair of polarizers arranged in the form of cross nicols, one of the pair of polarizers having a polarization axis substantially parallel with the molecular axis of the ferroelectric liquid crystal oriented to one of the plurality of different orientation states.

4. A liquid crystal optical device according to claim 1, wherein said ferroelectric smectic liquid crystal is in chiral smectic C phase, H phase, I phase, G phase or F phase.

5. A liquid crystal optical device according to claim 1, wherein the frequency of said alternating electric field is in the range of 400 Hz to 100 KHz.

6. A liquid crystal optical device according to claim 1, wherein said alternating electric field is applied from the second group of electrodes to the intersections of the first group of electrodes and the second group of electrodes when said first group of electrodes are supplied with the scanning nonselection signal.

7. A liquid crystal optical device according to claim 1, wherein said alternating electric field is applied from the first group of electrodes to the intersections between the first group of electrodes and the second group of electrodes when said first group of electrodes are supplied with the scanning nonselection signal.

8. A liquid crystal optical device according to claim 1, wherein said means for raising the frequency of the alternating electric field corresponding to a temperature increase, comprises a temperature sensor and a variable frequency generator circuit.

9. A liquid crystal optical device according to claim 1, wherein said ferroelectric smectic liquid crystal shows cholesteric phase on a higher temperature side than the smectic phase.

10. A liquid crystal optical device according to claim 1, wherein the molecules of said ferroelectric smectic liquid crystal are arranged to form a spiral structure in absence of an electric field.

11. A liquid crystal optical device according to claim 1, wherein the molecules of said ferroelectric smectic liquid crystal are in an alignment state wherein the spiral structure is not formed in the absence of an electric field.