Driving method for optical modulation device using ferroelectric liquid crystal

• US 5,255,110 A
• Filed: 03/08/1991
• Issued: 10/19/1993
• Est. Priority Date: 12/25/1985
• Status: Expired due to Fees

• Current Assignee: Canon Kabushiki Kaisha (Canon Inc.)
• Original Assignee: Canon Kabushiki Kaisha (Canon Inc.)
• Inventors: Inaba, Yutaka, Mouri, Akihiro, Kaneko, Shuzo, Kanbe, Junichiro, Toyono, Tsutomu
• Primary Examiner(s): Sikes, William L.
• Assistant Examiner(s): Duong, Tai V.
• Application Number:
  US07/666,893
• Time in Patent Office: 956 Days
• Field of Search: 350/333, 350/350 S, 340/784, 340/805, 359/56, 359/85, 359/100
• US Class Current: 345/97
• CPC Class Codes: G09G 2310/06 Details of flat display driving waveforms
• CPC Class Codes: G09G 2310/061 for resetting or blanking
• CPC Class Codes: G09G 2310/063 Waveforms for resetting the whole screen at once
• CPC Class Codes: G09G 2320/0209 Crosstalk reduction, i.e. to reduce direct or indirect influences of signals directed to a certain pixel of the displayed image on other pixels of said image, inclusive of influences affecting pixels in different frames or fields or sub-images which constitute a same image, e.g. left and right images of a stereoscopic display
• CPC Class Codes: G09G 3/3629 using liquid crystals having memory effects, e.g. ferroelectric liquid crystals
• CPC Class Codes: H01L 31/1884 Manufacture of transparent electrodes, e.g. TCO, ITO
• CPC Class Codes: Y02E 10/50 Photovoltaic [PV] energy

Abstract

An optical modulation device includes scanning electrodes and signal electrodes disposed opposite to and intersecting with the signal electrodes, and an optical modulation material disposed between the electrodes, a pixel being formed at each intersection of the electrodes and showing a contrast depending on the polarity of a voltage applied thereto. The device is driven by a method including, in a writing period for writing in all or prescribed pixels among the pixels on a selected scanning electrode, a first phase for applying a voltage of one polarity having an amplitude exceeding a first threshold voltage of the optical modulation material to the all or prescribed pixels, and a second phase for applying a voltage of the other polarity having an amplitude exceeding a second threshold voltage of the optical modulation material to a selected pixel and applying a voltage not exceeding the threshold voltages of the optical modulation material to the other pixels, respectively among the all or prescribed pixels. The maximum duration of a continually applied voltage of the same polarity applied to a pixel on a scanning electrode is 2.5 times the duration of the first phase in the writing period.

Claims

1. A driving method for an optical modulation device comprising scanning electrodes, signal electrodes disposed intersecting the scanning electrodes so as to form a pixel at each intersection of the scanning electrodes and signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes and assuming different orientation states when supplied with voltages of different polarities exceeding threshold voltages;

said driving method comprising the steps of;

writing in all or prescribed pixels on a selected scanning electrode of the scanning electrodes in a writing period including at least four phases;

applying voltages of mutually opposite polarities in the first phase and the last phase, having an amplitude not exceeding the threshold voltages of said optical modulation material, to all of the pixels on a nonselected scanning electrode; and

applying to said selected scanning electrode two voltage signals having the same amplitude and mutually opposite polarities, a voltage signal having a smaller amplitude than said same amplitude, and a voltage signal 0 voltage, respectively, with respect to the potential of a nonselected scanning electrode in the writing period including said at least four phases, wherein said voltage signal of 0 voltage is applied in the last phase of said at least four phases.

2. A driving method according to claim 1, wherein said smaller amplitude is one half of said same amplitude.

3. A driving method according to claim 1, further comprising the step of continually applying a voltage of a single polarity to a pixel on a scanning electrode, wherein the maximum duration of the continually applied voltage of the same polarity applied to the pixel on the scanning electrode is twice the duration of the first phase.

4. A driving method according to claim 1, wherein said optical modulation material comprises a ferroelectric liquid crystal.

5. A driving method according to claim 4, wherein said ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

6. A driving method according to claim 5, wherein said chiral smectic liquid crystal is disposed in a layer thin enough to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.

7. A driving method according to claim 1, further comprising the steps of:

applying a voltage of one polarity exceeding a first threshold voltage of the optical modulation material to said all or prescribed pixels in at least one phase of said at least four phases; and

applying a voltage of the other polarity exceeding a second threshold voltage of the optical modulation material to a selected pixel of said all or prescribed pixels in at least another phase.

8. An optical modulation apparatus comprising:

an optical modulation device comprising scanning electrodes, signal electrodes disposed intersecting the scanning electrodes so as to form a pixel at each intersection of the scanning electrodes and signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes and assuming a first stable optical state in response to a voltage of one polarity and a second stable optical state in response to a voltage of another polarity exceeding respective threshold voltages, and

(b) drive means for;

(b1) sequentially applying to the scanning electrodes a scanning selection signal comprising a pulse of one polarity in a first phase, a pulse of another polarity in a second phase and a pulse of said one polarity in a third phase, and

(b2) writing in pixels on a selected scanning electrode by,

in the first phase, applying to the signal electrodes a voltage signal which provides a voltage of one polarity simultaneously causing the first optical state at the pixels on the selected scanning electrode in combination with the scanning selection signal to erase the pixels on the selected scanning electrode,

in the second phase, selectively applying to the signal electrodes a pulse of one polarity or a pulse of another polarity which provides a voltage of another polarity causing the second optical state or a voltage maintaining the erased state respectively in combination with the scanning selection signal at associated pixels on the selected scanning electrode to write in the associated pixels, and

in the third phase, applying to the signal electrodes voltage signals which provide voltages respectively opposite to the voltages applied to the associated pixels on the selected scanning line in the second phase so as to retain the written states at the associated pixels,

the polarities of the pulses being defined with respect to a voltage applied to a non-selected scanning electrode, and

(b3) applying an alternating voltage to pixels on a non-selected scanning electrode so as to retain the written states of the pixels formed when they have been placed on a selected scanning electrode.

9. An optical modulation apparatus according to claim 8, wherein said optical modulation material comprises a ferroelectric liquid crystal.

10. An optical modulation apparatus according to claim 9, wherein said ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

11. An optical modulation apparatus according to claim 10, wherein said chiral smectic liquid crystal is disposed in a layer thin enough to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.