Liquid crystal apparatus and driving method therefor

Abstract: A liquid crystal device is formed by a plurality of scanning electrodes, a plurality of data electrodes intersecting the scanning electrodes, and a bistable liquid crystal showing a first stable orientation state and a second stable orientation state disposed between the scanning electrodes and the data electrodes so as to form a pixel at each intersection of the scanning electrodes and the data electrodes. The liquid crystal device is driven according to a scheme wherein a pixel is written in a first orientation state (or at a gradation level k ) in two steps including: a first step of applying a prescribed voltage for causing the second orientation state to the pixel and then applying a voltage of at least V₁ (or a voltage Va) to the pixel, and a second step of applying a voltage of at least V₂ (or a voltage Vb) to the pixel, wherein V₁ (Va) denotes a threshold voltage required for converting a pixel in the second orientation state into the first orientation state (into the gradation level k ) after applying the prescribed voltage for causing the second orientation state to the pixel in the first orientation state, and V₂ (Vb) denotes a threshold voltage required for converting a pixel in the second orientation state into the first orientation state (into the gradation level k ) after applying the prescribed voltage for causing the second orientation state to the pixel in the second orientation state.

Description: FIELD OF THE INVENTION AND RELATED ART The present invention relates to a liquid crystal apparatus particularly a ferroelectric liquid crystal apparatus, and a liquid crystal driving method. Display devices using a ferroelectric liquid crystal have been known, including a type wherein a ferroelectric liquid crystal (hereinafter sometimes abbreviated as "FLC") is injected into a cell or panel formed by disposing a pair of glass plates each having an inner surface provided with a transparent electrode and an aligning treatment opposite to each other so that their inner surfaces face each other with a cell gap of about 1 - 3 microns therebetween (as disclosed in, e.g., Japanese Laid-Open Patent Application (JP-A) 61-94023). The above type of display device using a ferroelectric liquid crystal is characterized in that a ferroelectric liquid crystal has a spontaneous polarization causing a coupling with an external electric field available for switching and in that the switching can be caused depending on the polarity of the external electric field because the director ((longer) molecular axis direction) of each FLC molecule corresponds to the direction of its spontaneous polarization in a one-to-one correspondence. A ferroelectric liquid crystal is generally utilized in its chiral smectic (SmC*, SmH*, etc.) phase so that the liquid crystal molecular axes are disposed to show a twisted alignment in its bulk state but the twisting of the liquid crystal molecular axes can be released or suppressed by disposing the ferroelectric liquid crystal in a cell having a cell gap on the order of 01 - 3 microns as described above (N.A. Clark, et al., MCLC (1983), Vol. 94, p.p. 213 - 234). In an actual FLC cell or panel structure, a simple matrix-structure, e.g., as shown in Figures 3A and 3B may be adopted. Referring to Figures 3A and 3B, such an FLC cell or panel has a sectional structure as shown in Figure 3B and includes a pair of upper and lower glass substrates 31 each having ITO stripe electrodes 32, an SiO 2 insulating film 33 and a polyimide alignment film 34 disposed in this order thereon, a ferroelectric liquid crystal 36 disposed between the substrates, and a sealing member 35 sealing the periphery of the cell structure. The ITO stripe electrodes 32 are disposed on one substrate 31, e.g., in a pattern as shown in Figure 3B, so as to intersect with the stripe electrodes 32 on the other substrate 32. For matrix drive of FLC display devices, a line-sequential scanning scheme has been conventionally adopted, wherein an identical writing waveform is applied for providing one display state to a pixel regardless of whether the pixel has had either one of bistable molecular orientation states. In actual drive, however, it has been found that a state before a writing remarkably affects the threshold for the writing. More specifically, if it is assumed that V thW denotes a threshold for writing "white" in a "white" pixel after once clearing the pixel into "black" and V thB denotes a threshold for writing "white" in a "black" pixel after once clearing the pixel into "black", a relationship of V thB > V thW exhibits until a certain relaxation time lapses since the clearing into "black". Based on the phenomenon, when a drive voltage in the vicinity of the threshold is applied, the resultant display state can be different depending on whether the pixel in question has been in "white" state or "black" state before the writing. This is quite awkward for a display device. Further, in the case of displaying a halftone in a pixel for the purpose of a gradational display by voltage modulation, it is inevitable to set a voltage in the vicinity of the threshold depending on a pixel state before the writing, and the adverse effect of the phenomenon is serious. If the adverse effect is avoided by placing a wait time before the writing, a motion picture lacks its continuity, or a picture flickers in the case of a refresh drive. The US-A-4 932 759 discloses a liquid crystal driving apparatus and a method for driving the same, including a liquid crystal device comprising a plurality of scanning electrodes, a plurality of data electrodes intersecting said scanning electrodes, and a bistable liquid crystal showing a first stable orientation state and a second stable orientation state disposed between said scanning electrodes and said data electrodes so as to form a pixel at each intersection of said scanning electrodes and said data electrodes. Moreover, the described apparatus and method of driving the same includes 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 a pixel. Furthermore, document EP-A-0 214 857 describes a similar liquid crystal driving apparatus and a method for driving the same which uses a time sharing driving for obtaining grey levels and which additionally resets the respective pixels so as to bring them into a predetermined state. However, the above prior art documents are both silent with regard to the above described problems relating to the present invention. It is an object of the present invention to provide a liquid crystal driving apparatus and method which is suitable for gradational motion picture display free from flickering in case of refresh drive. This object is achieved by a liquid crystal driving method and apparatus as claimed in claims 1 and 2, respectively. Thus, particularly by taking into account the initial or previous state of a pixel as parameter for control of the pixel a gradation display as well as a high-speed motion picture display can be provided which is free from flickering in case of refresh drive. More particularly, even when in the first step, due to its previous state a pixel is not brought completely to its desired state, in the second step this desired gradational state is securely reached. As a result, the standing time from clearing to writing of a pixel can be optimally reduced and an intended gradation state can be displayed without depending on different initial states before writing by consecutively applying two voltage application steps. BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a schematic view for illustrating an embodiment of the liquid crystal driving method according to the present invention. Figures 2A and 2B are schematic views for illustrating another embodiment of the liquid crystal driving method according to the present invention. Figure 3A is a schematic sectional view of a conventional ferroelectric liquid crystal device, and Figure 3B is a schematic plan view showing an example of an electrode pattern thereof. Figure 4 is a block diagram of a drive circuit for generating drive signals for performing the liquid crystal driving method according to the present invention. Figure 5 is a waveform diagram showing an example of a driving waveform applied to a pixel for performing the liquid crystal driving method according to the present invention. Figure 6 is a graph showing a change with time of difference in switching threshold of a ferroelectric liquid crystal depending on a difference in state before writing. Figures 7A and 7B are waveform diagrams showing an example set of driving waveforms for the liquid crystal driving method according to the present invention. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS According to the present invention, voltage signals applied to the respective pixels of the liquid crystal device are divided and consecutively applied in steps 1 and 2, respectively, so that a desired state is reliably displayed in each pixel regardless of the state of the pixel before the writing. Particularly, in the case of a gradational display, a desired gradation level is stably written in the respective pixels without being affected by the previous state of each pixel. Further, a gradational state close to the desired level can be accomplished by performing the step 1 without having a wait time corresponding to the relaxation time in which the writing threshold affected by the previous states become substantially the same. Accordingly, it is possible to provide the display with a continuity, which is suitably applicable to a motion picture display and which is free from flickering in case of refresh drive. In the display device used in the present invention, a plurality of scanning electrodes and a plurality of data electrodes are disposed to intersect each other so as to receive the respective signals, and a liquid crystal showing a first orientation state and a second orientation state is disposed between the two types of electrodes so as to form a pixel at each intersection of the scanning electrodes and the data electrodes. The liquid crystal at each pixel is driven between the first and second orientation states. In order to provide the first orientation state at a certain pixel, the pixel is first supplied with a voltage sufficient to cause the second orientation state and then supplied with a voltage of at least V 1 which is a threshold voltage for converting a pixel in the second orientation state into the first orientation state after applying a clearing voltage for causing the second orientation state to the pixel in the first orientation state (Step 1), and then supplied with a voltage of at least V 2 which is a threshold voltage for converting a pixel in the second orientation state into the first orientation state after applying a clearing voltage for causing the second orientation state to the pixel in the second orientation state (Second step). As a result, in the first step, a pixel in the first orientation state is securely brought to the first orientation state and, in the second step, a pixel in the second orientation state is securely brought to the first orientation state even when the pixel is not brought to the first orientation state in the first step. In the case of a gradational display, in order to provide a desired gradation level K at a certain pixel, the pixel is first supplied with a voltage sufficient to cause the second orientation state completely and then supplied with a voltage Va which is a voltage capable of providing the gradation level K to a pixel completely in the second orientation state after applying a clearing voltage for causing the second orientation state to the pixel in the first orientation state (Step 1), and then supplied with a voltage Vb which is a voltage capable of providing the gradation level K to a pixel completely in the second orientation state after applying a clearing voltage for causing the second orientation to thee pixel in the second orientation state (Step 2). As a result, in the case where the certain pixel is at the gradation level K or closer to the complete first orientation state, the pixel is brought to the gradation level K in the first orientation state. On the other hand, in the case where the certain pixel is between the gradation level K and the complete second orientation state, the pixel is securely brought to the gradation level K in the second step even if the gradation level K is not provided in the first orientation state and remains to be between the gradation level K and the complete second orientation state. In the step 2, Va and Vb are ordinarily almost the same or closer to each other, a pixel at the gradation level K already in the first step does not change the gradation level. As a result, a desired gradation level can be stably written in a pixel without being affected by a previous display state of the pixel. Further, the step 1 may be performed to obtain a gradation level close to the desired gradation level without having a wait time within which Va and Vb become substantially the same value. Accordingly, the display is caused to acquire a continuity, thus being suitable for a motion picture display and free from flickering in the case of refresh drive. In the present invention, the first and second steps may be performed in this order one by one in successive two scanning times. The liquid crystal suitably used in the present invention may comprise a ferroelectric liquid crystal. As the ferroelectric liquid crystal, a liquid crystal compound or composition showing chiral smectic phase as disclosed in U.S. Patent Nos. 4561726, 4614609, 4589996, 4592858, 4596667, 4613209, etc., may be used. Hereinbelow, some embodiments of the present invention will be described with reference to the drawings. First embodiment In a specific example, a ferroelectric liquid crystal device was prepared in the following manner. An electrode plate was provided by coating a polished glass substrate with an ITO film having a sheet resistivity of about 40 ohm.-square by sputtering. Each electrode plate was further coated with a polyimde precursor liquid ("LQ-1802", mfd. by Hitachi Kasei K.K.), followed by curing and rubbing in one direction with a nylon fiber (about 0.3 mm-long)-planted cloth to form a polyimide-type alignment film. A pair of the class plates thus provided were fixed to each other so that their rubbing directions are identical to form a blank cell with a cell gap of about 1.4 micron. The blank cell was then filled with a liquid crystal A having a Ps (spontaneous polarization) of 6.6 nC/cm 2 , a Δε (dielectric anisotropy) of -0.3 and a tilt angle of 14.3 degrees, respectively at 30 °C, and showing the following phase transition series: Phase transition series (°C) Cryst.: crystal, SmC*: chiral smectic C phase, SmA: smectic A phase, Ch.: cholesteric phase, and Iso.: isotropic phase. The cell filled with the liquid crystal A heated in its isotropic phase was gradually cooled for alignment to form a liquid crystal device (cell or panel). Figure 4 is a block diagram of an embodiment of the liquid crystal apparatus according to the present invention including a liquid crystal cell or panel 41 thus prepared and a drive circuit therefor, which includes a drive power supply 42 for generating voltages supplied to the liquid crystal cell 41, segment-side drive IC 43 for applying voltages from the drive power supply 42 to data signal lines of the liquid crystal cell 41 as image data signals, a latch circuit 44, a segment-side S/R (shift register) 45, a common-side drive IC for applying a voltage from the drive power supply 42 to scanning signal lines of the liquid crystal cell 41 as a scanning signal, a common side S/R (shift register) 47, an image data source 48, and a controller 49 for controlling the segment-side S/R 45 and the common-side S/R 47 based on image data from the image data source 48. Figure 5 shows an example of a voltage signal (pixel signal) waveform conventionally applied to pixel of the liquid crystal cell 41 according the above arrangement. As a result, there can result a difference in writing threshold depending on whether a pixel to be written is in a "white" state or a "black" state before the writing. Figure 5 shows a waveform for clearing a pixel into "black" and then writing the pixel into "white", including a clearing pulse P1 into "black" and a writing pulse P2 for "white". Herein, the parameters are set such that ΔT = 40 µsec, Vi = 6.2 volts, T = 200 µsec and Ve = 26.0 volts. Vop denotes a prescribed switching voltage. In the period T, data signals for other scanning lines are applied. In the case of Figure 5, the switching threshold V th may cause changes as shown in Figure 6 depending on the length of the period T. Referring to Figure 6, the curve 61 connecting black spots () represents a change in threshold V thB for clearing a pixel in "black" state before writing into "black" and then writing "white", and the curve 62 connecting white spots (o) represents a change in threshold V thW for clearing a pixel in "white" state before writing into "black" and then writing "white". As is understood from Figure 6, a relationship of V thB - V thW > 1.0 holds for a relatively short period T. The difference in threshold cannot be ignored for writing by application of voltages in the neighborhood of the threshold and leads to a difficulty in display of gradation levels. A period T of about 44 msec is required in order that the difference between V thB and V thW can be ignored. During the period, flickering is caused even in a refresh drive, giving rise to a difficulty in a display device. Further, in the case of a gradational display, the difference can result in display gradation level amounting to about 5 - 10 %. In order to obviate the above-mentioned difficulties, a voltage application method including two steps is adopted in this embodiment as will be explained with reference to Figure 1. Figure 1 is a schematic view for illustrating a transition of states of four pixels a - d having different initial states. From the left to right in Figure 1, at A are shown initial states, at B are shown states after clearing into "black", at C are shown states after a first writing, and at D are shown states after a second writing for the pixels a - d, respectively. The pixels a - d are respectively assumed to have a square region having a threshold gradually increasing from the left side toward the right side. Such a threshold change within a pixel may be caused according to a cell gap change within the range of 1.0 - 1.4 micron for a pixel. This embodiment is constituted by two steps including a first step of from clearing into "black" up to application of a gradation data signal for the first time, and a second step of applying a gradation data signal for the second time. These results in differences as shown at C after the first writing of gradation data signals depending on the initial states before writing of the pixels at a - d. Now, a first-time gradation data signal is assumed to be an inversion signal for causing an inversion of, e.g., 50 % of pixel. In the first step (step 1), a clearing pulse P 1 (Ve = 26.0 volts) similar to one shown in Figure 5 for clearing into or toward "black" to form a state B and then, after a period of T = 200 µsec., a white-writing pulse P 2 (Vop = 13.7 volts) to effect a writing. In this instance, the pixels having the initial states b and c are completely written with intended data, whereas the pixels having the initial states a and d provide incompletely written states. This is a result of influence of a difference in threshold caused by a difference in state of pixels before writing as has been described hereinbefore. After the step 1, a writing (rewriting) in a second step (step 2) is performed after a lapse of time T 0 which is larger than a relaxation time T of approximately 44 msec (beyond which a difference in threshold disappears). In the step 2, the pixels a - d are initially at the states C . In this rewriting step, it is possible to either apply or not apply a clearing pulse for providing the states B , and the writing signal may have a switching threshold Vop (15.0 volts) from the "black" state. As a result of the above-described writing, even the pixels having the initial states a and d are completely written with 50 %-inversion data. In this instance, the pixels having the initials b and c which have been already written with complete gradation data also have the same switching threshold from the "black" state with respect to their black-written regions. As a result, all the pixels a - d are written at the same intended gradation level. According to this embodiment as described above, an intended gradation state can be displayed without depending on different initial states before writing by consecutively applying two voltage application steps of the step 1 and the step 2. Further, even at a stage after the step 1, the gradation data are written to some extent, so that the display can be provided with a continuity and may be applicable to a motion picture display compared with the case where a whole picture or screen is allowed to stand at the initial state of "white" or "black" for the above-mentioned relaxation time T. In other words, compared with a conventional scheme wherein a standing time of 40 msec or longer is required from clearing to writing, the standing time can be reduced to an order of microseconds or substantially omitted according to this embodiment. Further, if the steps 1 and 2 are divided into two consecutive frames each comprises scanning of all the scanning lines, an intended graditional picture can be displayed with an error of about 10 % in a step 1, followed by a step 2 providing a completely intended gradational picture free of error. In this instance, if the above frame scanning time is assumed to be 100 msec for example, the influence of the previous pixel states can be completely removed if the above-mentioned relaxation time is 100 msec or shorter. Further, even in a case where the relaxation time exceeds 100 msec., and the frame scanning time se shorter than the relaxation time (while this is not ideal), a much better display quality can be accomplished than in a conventional system wherein the pixels are merely caused to stand in a refresh operation. In the above described embodiment, pixels b and c having a lower threshold voltage for the desired gradation level are written in Step 1, but it is also possible to write pixels a and d having a higher threshold voltage for the desired gradation level in Step 1 if an additional step of clearing into "black" is placed before Step 2. Second embodiment This embodiment is directed to an application of the present invention to a binary state display. According to this embodiment, a display device (cell) comprising 400 scanning lines C 1 - C 400 and 640 data signal lines S 1 - S 640 as shown in Figure 2A is driven by applying driving voltages which are changed for each frame scanning (of 400 lines) so that steps 1 and 2 as described in the previous embodiment are performed are alternating frames as shown in Figure 2. The liquid crystal device structure is the same as in the first embodiment except that the cell gap is uniformly 1.4 micron. The device is subjected to application of a set of driving voltage waveforms as shown in Figures 7A and 7B, which include a scanning signal S, data signals I, pixel signals G (= S-I), ΔT = 40 µsec. a writing signal voltage Vop = 17.4 volts in Step 1, a writing signal voltage Vop = 16.1 volts in Step 2 and a clearing signal voltage Ve = 22.0 volts (for only in Step 1). This embodiment is effective for ensuring a reliable writing over a wide liquid crystal device (a panel rather than a cell) having a certain difference in operation temperature, which also results in a difference in switching threshold voltages so that an entire panel cannot be written by a single writing signal voltage. In a particular drive operation, an A4 size panel resulted in a temperature difference of 2 °C ranging from 34 °C to 36 °C due to a local difference in heat generated by the drive IC. In this case, the writing signal voltage Vop = 17.4 volts was suitable for driving at a temperature of 34 °C, and the writing signal voltage Vop = 16.1 volts was suitable for driving at a temperature of 36 °C. As a result of application of the above-described driving scheme using Ve = 22.0 volts and Vop = 17.4 volts in Step 1 and Vop = 16.1 volts in Step 2 to the A4 size panel having a temperature difference of 2 °C, a desired picture could be displayed over the entire panel. However, when the above A4 size panel was driven applying Figures 7A and 7B waveforms involving a single writing step using Ve = 22.0 volts and Vop = 17.4 volts or Vop = 16.1 volts, the A4 size panel caused a local disorder at a high-temperature part or a low-temperature part.

Claims: A liquid crystal driving method, comprising: providing a liquid crystal device comprising a plurality of scanning electrodes (C 1 -C 400 ), a plurality of data electrodes (S 1 -S 640 ) intersecting said scanning electrodes (C 1 -C 400 ), and a bistable liquid crystal (36) showing a first stable orientation state and a second stable orientation state disposed between said scanning electrodes (C 1 -C 400 ) and said data electrodes (S 1 -S 640 ) so as to form a pixel at each intersection of said scanning electrodes and said data electrodes, said method being characterized by the writing steps for causing the first orientation state in a pixel including: a first step of applying a prescribed voltage (Ve) for causing the second orientation state to the pixel and then applying a first voltage V 1st to the pixel, and a second step of applying a second voltage V 2nd to the pixel, wherein said first voltage V 1st and said second voltage V 2nd are at least V 1 and at least V 2 , respectively, or V a and V b , respectively, wherein V 1 denotes a threshold voltage (V thW ) required for converting a pixel in the second orientation state into the first orientation state after applying said prescribed voltage (V e ) for causing the second orientation state to the pixel in the first orientation state, and V 2 denotes a threshold voltage (V thB ) required for converting a pixel in the second orientation state into the first orientation state after applying the prescribed voltage (V e ) for causing the second orientation state to the pixel in the second orientation state, V a denotes a voltage required for converting a pixel completely in the second orientation state into the gradation level k after applying the prescribed voltage (V e ) for causing the second orientation state to the pixel completely in the first orientation state, and V b denotes a voltage required for converting a pixel completely in the second orientation state into the gradation level k after applying the prescribed voltage (V e ) for causing the second orientation state to the pixel completely in the second orientation state, and the first step is performed at a time when V 1 < V 2 or Va < Vb, respectively, and the second step is performed at a time when V 1 and V 2 or Va and Vb, respectively, are substantially identical to each other. A liquid crystal driving apparatus, comprising: a liquid crystal device comprising a plurality of scanning electrodes (C 1 -C 400 ), a plurality of data electrodes (S 1 -S 640 ) intersecting said scanning electrodes (C 1 -C 400 ), and a bistable liquid crystal (36) showing a first stable orientation state and a second stable orientation state disposed between said scanning electrodes (C 1 -C 400 ) and said data electrodes (S 1 -S 640 ) so as to form a pixel at each intersection of said scanning electrodes and said data electrodes, said apparatus being characterized by drive means (42 - 49) for causing the first orientation state in a pixel in two steps including: a first step of applying a prescribed voltage (Ve) for causing the second orientation state to the pixel and then applying a first voltage V 1st to the pixel, and a second step of applying a second voltage V 2nd to the pixel, wherein said first voltage V 1st and said second voltage V 2nd are at least V 1 and at least V 2 , respectively, or V a and V b , respectively, wherein V 1 denotes a threshold voltage (V thW ) required for converting a pixel in the second orientation state into the first orientation state after applying said prescribed voltage (V e ) for causing the second orientation state to the pixel in the first orientation state, and V 2 denotes a threshold voltage (V thB ) required for converting a pixel in the second orientation state into the first orientation state after applying the prescribed voltage (V e ) for causing the second orientation state to the pixel in the second orientation state, V a denotes a voltage required for converting a pixel completely in the second orientation state into the gradation level k after applying the prescribed voltage (V e ) for causing the second orientation state to the pixel completely in the first orientation state, and V b denotes a voltage required for converting a pixel completely in the second orientation state into the gradation level k after applying the prescribed voltage (V e ) for causing the second orientation state to the pixel completely in the second orientation state, and the first step is performed at a time when V 1 < V 2 or Va < Vb, respectively, and the second step is performed at a time when V 1 and V 2 or Va and Vb, respectively, are substantially identical to each other. A method or apparatus according to claim 1 or 2, characterized in that said first and second steps are performed in this order respectively in successive two scanning times for the pixel. A method or apparatus according to claim 1 or 2, characterized in that said liquid crystal (36) is a ferroelectric liquid crystal.

Inventors: OKADA SHINJIRO, OKADA, SHINJIRO
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1991
Main classification: G09G3
IPC codes: G02F1, G09G3