Driving method for optical modulation device

• US 4,932,759 A
• Filed: 12/23/1986
• Issued: 06/12/1990
• Est. Priority Date: 12/25/1985
• Status: Expired due to Term

• 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): Miller, Stanley D.
• Assistant Examiner(s): DUONG, TAI V
• Application Number:
  US06/945,578
• Time in Patent Office: 1,267 Days
• Field of Search: 350/332, 350/333, 350/350 S, 340/784, 340/805, 340/811, 340/802
• US Class Current: 345/97
• CPC Class Codes: G09G 2310/06 Details of flat display driving waveforms
• 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

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 so as to provide a matrix of pixels as a whole and having 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 the respective pixels on a selected scanning electrode: at least two repeating sets of phases, each set of phases comprising a state-determining phase for determining the contrast of a pixel and an auxiliary phase for not determining the contrast of the pixel.

Claims

1. A driving method for an optical modulation device comprising scanning electrodes and signal electrodes disposed opposite to and intersecting with the signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes, having a pixel at each intersection of the scanning electrodes and the signal electrodes so as to form a matrix of pixels and exhibiting contrast depending on the magnitude and polarity of a voltage applied to each pixel of the matrix;

said driving method comprising the step of writing on respective pixels on a selected scanning electrode in a writing period defined by application of a scanning selection signal voltage to the selected scanning electrode, the writing period comprising a former half period and a latter half period which is subsequent to the former half period, the former half period comprising a first state-determining phase for causing a selected one of the respective pixels on the selected scanning electrode to assume one optical state of two optical states and a first auxiliary phase prior to the first state-determining phase for causing the selected one of the respective pixels to assume a second optical state, and the latter half period comprising a second state-determining phase for causing at least a remaining non-selected one of the respective pixels on the selected scanning electrode to assume the second optical state and a second auxiliary phase prior to the second state-determining phase for causing the remaining non-selected pixels to assume the one optical state, and supplying both the pixel selected in the latter half period and the pixels non-selected in the former half period with an alternating voltage to maintain their optical state.

2. A driving method according to claim 1, wherein said writing step further comprises the steps of applying different voltages to the pixels on the selected scanning electrode at each of the first and second state-determining phases, and applying the different voltages to the pixels on the selected scanning electrode at each of the first and second auxiliary phases.

3. A driving method according to claim 1, wherein said writing step further comprises the step of applying alternating voltages to the pixels on a nonselected scanning electrode throughout the writing period including the first and second state-determining phases and the first and second auxiliary phases.

4. A driving method according to claim 1, wherein said writing step further comprises the step of applying a first voltage signal to a selected signal electrode at the first state-determining phase and applying a second voltage signal to the a remaining non-selected signal electrodes at the second state-determining phase, the first and second voltage signals being signals of mutually different voltages.

5. A driving method according to claim 4, wherein the first and second voltage signals are of mutually opposite polarities with respect to the voltage level of a nonselected scanning electrode.

6. A driving method according to claim 1, wherein said writing step comprises the steps of applying a voltage signal exceeding a threshold voltage of the optical modulation material to a selected pixel among the pixels on a selected scanning electrode at one of the state-determining phases, and simultaneously applying a voltage not exceeding the threshold voltage to the remaining non-selected pixels on the selected scanning electrode.

7. A driving method according to claim 1, wherein said writing step comprises the step of continually applying a voltage of the same polarity to a pixel on a scanning electrode, wherein the duration of the continually applied voltage of the same polarity applied to the pixel on the scanning electrode does not exceed twice the duration of the first or second state-determining phases.

8. A driving method according to claim 1, wherein said writing step further comprises the step of applying, in the writing period, a first voltage to a selected pixel on the selected scanning electrode at the first state-determining phase, the first voltage having a polarity opposite to that of the voltage applied to the selected pixel at the first auxiliary phase and a second voltage to the remaining non-selected pixels on the selected scanning electrode at the second state-determining phase, the second voltage having a polarity opposite to the voltage applied to the remaining non-selected pixels at the second auxiliary phase.

9. A driving method according to claim 8, wherein the voltages applied at the first and second auxiliary phases exceed a threshold voltage of the optical modulation material.

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

11. A driving method according to claim 10, wherein the ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

12. A driving method according to claim 10, wherein the chiral smectic liquid crystal is disposed in a layer sufficiently thin to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.

13. A driving method for an optical modulation device comprising scanning electrodes and signal electrodes disposed opposite to and intersecting with the signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes, having a pixel at each intersection of the scanning electrodes and the signal electrodes so as to form a matrix of pixels and exhibiting contrast depending on the magnitude and polarity of a voltage applied to each pixel of the matrix;

said driving method comprising the steps of;

applying to a selected pixel on a selected scanning electrode a voltage of one polarity having an amplitude exceeding a first threshold voltage of the optical modulation material at a first auxiliary phase, and a voltage of the other polarity having an amplitude exceeding a second threshold voltage at a first state-determining phase after the first auxiliary phase;

applying to a nonselected pixel on the selected scanning electrode a voltage of the other polarity having an amplitude exceeding the second threshold voltage at a second auxiliary phase after the first state-determining phase, and a voltage of the one polarity exceeding the first threshold voltage at a second state-determining phase after the second auxiliary phase; and

applying to the nonselected pixel on the selected scanning electrode a voltage not exceeding the threshold voltages of the optical modulation material throughout a period including the first auxiliary and state-determining phases while the selected pixel on the selected scanning electrode is supplied with the voltage of one polarity having an amplitude exceeding the first threshold voltage and the voltage of the other polarity having an amplitude exceeding the second threshold voltage.

14. A driving method according to claim 13, wherein said optical modulation material comprises a ferroelectric liquid crystal.

15. A driving method according to claim 14, wherein said ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

16. A driving method according to claim 15, wherein said chiral smectic liquid crystal is disposed in a layer sufficiently thin to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.

17. A driving method for an optical modulation device comprising scanning electrodes and signal electrodes disposed opposite to and intersecting with the signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes, having a pixel at each intersection of the scanning electrodes and the signal electrodes so as to form a matrix of pixels and exhibiting contrast depending on the magnitude and polarity of a voltage applied to each pixel of the matrix;

said driving method comprising the steps of;

applying to a selected pixel on a selected scanning electrode a voltage of one polarity having a first duration and an amplitude sufficient to exceed a threshold of the optical modulation material in a first phase, a voltage of the other polarity having a second duration and an amplitude insufficient to exceed the threshold in a second phase and third phase, and a voltage of 0 in a fourth phase; and

applying to a nonselected pixel on the selected scanning electrode a voltage of the other polarity having a duration and an amplitude sufficient to exceed the threshold in the third phase, a voltage of the one polarity having a duration and an amplitude insufficient to exceed the threshold voltage in the first and fourth phases, and a voltage of 0 in the second phase, wherein the first, second, third and fourth phases are sequential in that order.

18. A driving method according to claim 17, wherein the optical modulation material comprises a ferroelectric liquid crystal.

19. A driving method according to claim 18, wherein the ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

20. A driving method according to claim 19, wherein the 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.

21. An optical modulation apparatus comprising:

an optical modulation device comprising scanning electrodes and signal electrodes disposed opposite to and intersecting with said signal electrodes, and an optical modulation material disposed between said scanning electrodes and said signal electrodes, having a pixel at each intersection of said scanning electrodes and said signal electrodes so as to provide a matrix of pixels and exhibiting contrast depending on the magnitude and polarity of a voltage applied to each pixel of said matrix;

an optical detection means; and

a driving unit for applying to a selected pixel on a selected scanning electrode a voltage of one polarity having an amplitude exceeding a first threshold voltage of said optical modulation material at a first auxiliary phase, and a voltage of the other polarity having an amplitude exceeding a second threshold voltage at a first state-determining phase after the first auxiliary phase; and

applying to a nonselected pixel on said selected scanning electrode a voltage of the other polarity having an amplitude exceeding the second threshold voltage at a second auxiliary phase after the first state-determining phase and a voltage of said one polarity exceeding the first threshold voltage at a second state-determine phase after the second auxiliary phase,

wherein an alternating voltage not exceeding the first or second threshold voltages is supplied to said selected pixel during the second auxiliary phase and the second state-determining phase and the non-selected pixel during the first auxiliary phase and the first state-determining phase.

22. An optical modulation apparatus according to claim 21, wherein said optical modulation material comprises a ferroelectric liquid crystal.

23. An optical modulation apparatus according to claim 22, wherein said ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

24. An optical modulation apparatus according to claim 23, wherein said chiral smectic liquid crystal is disposed in a layer sufficiently thin to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.

25. An optical modulation device, comprising:

scanning electrodes and signal electrodes disposed opposite to and intersecting with the signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes, having a pixel at each intersection of the scanning electrodes and the signal electrodes so as to form a matrix of pixels exhibiting contrast depending on the magnitude and polarity of a voltage applied thereto;

an optical detection means; and

a driving unit for driving the matrix of pixels by steps of;

applying to a selected pixel on a selected scanning electrode a voltage of one polarity having a first duration and an amplitude sufficient to exceed a threshold of said optical modulation material in a first phase, a voltage of the other polarity having a second duration and amplitude insufficient to exceed the threshold in a second and third phase, and a voltage of 0 in a fourth phase, and

applying to a non-selected pixel on said selected scanning electrode a voltage of the other polarity having a third duration and an amplitude sufficient to exceed the threshold in the third phase, a voltage of the one polarity having a fourth duration and an amplitude insufficient to exceed the threshold in the first and fourth phases and a voltage of 0 in the second phase, wherein the first, second, third and fourth phases are sequential in that order.

26. An optical modulation apparatus according to claim 25, wherein said optical modulation material comprises a ferroelectric liquid crystal.

27. An optical modulation apparatus according to claim 26, wherein said ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

28. An optical modulation apparatus according to claim 27, wherein said chiral smectic liquid crystal is disposed in a layer sufficiently thin to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.

29. An optical modulation apparatus comprising:

an optical modulation device comprising scanning electrodes and signal electrodes disposed opposite to and intersecting with the signal electrodes, and an optical modulation material disposed between the scanning electrodes and the signal electrodes, having a pixel at each intersection of the scanning and the signal electrodes so as to provide a matrix of pixels exhibiting contrast depending on the magnitude and polarity of a voltage applied thereto;

an optical detection means; and

a driving unit for driving said optical modulation device by (i) applying to a selected pixel on a selected scanning electrode a first bipolar pulse causing said selected pixel to assume one optical state during the former half of a period during which pulses are applied to said pixels and a second bipolar pulse which maintains the one optical state of said selected pixel during the latter half of the period; and

(ii) applying to a nonselected pixel on said selected scanning electrode a third bipolar pulse not changing the optical state of said nonselected pixel during the former half of the period and a fourth bipolar pulse causing said nonselected pixel to assume the other optical state during the latter half of the period.

30. An optical modulation apparatus according to claim 29, wherein said first, second, third, and fourth bipolar pulses are respectively balanced bipolar pulses.

31. An optical modulation apparatus according to claim 30, wherein said optical modulation material comprises a ferroelectric liquid crystal.

32. An optical modulation apparatus according to claim 31, wherein said ferroelectric liquid crystal comprises a chiral smectic liquid crystal.

33. An optical modulation apparatus according to claim 32, wherein said chiral smectic liquid crystal is disposed in a layer sufficiently thin to release the helical structure of the chiral smectic liquid crystal in the absence of an electric field.