Ferroelectric liquid crystal device and process for production thereof

Abstract: A ferroelectric liquid crystal device of a cell structure having a suppressed increase of cell thickness along a cell side is constituted by disposing a ferroelectric liquid crystal between a pair of electrode plates each sequentially provided with an electrode, an insulating film and an alignment film on a substrate. The alignment film is provided with a surface unevenness for suppressing a liquid crystal movement causing the increase in cell thickness. The surface unevenness is provided to the alignment film directly or to the insulating film below the alignment film, e.g., by wet forming the relevant film by using at least two solvents having different boiling points or dispersing fine particles within the relevant film, optionally followed by removal of the fine particles.

Description: FIELD OF THE INVENTION AND RELATED ART The present invention relates to a ferroelectric liquid crystal device and a process for production thereof, more particularly to a ferroelectric liquid crystal device having a cell structure with improved driving characteristics and a process for production thereof. A display device of the type which controls transmission of light in combination with a polarizing device by utilizing the refractive index anisotropy of ferroelectric liquid crystal molecules has been proposed by Clark and Lagerwall (U.S. Patent No. 4,367,924, etc.). The ferroelectric liquid crystal has generally chiral smectic C phase (SmC*) of H phase (SmH*) of a non-helical structure and, under this state, shows a property of taking either one of a first optically stable state and a second optically stable state responding to an electrical field applied thereto and maintaining such a state in the absence of an electrical field, namely bistability, and also has a rapid response to the change in electrical field. Thus, it is expected to be utilized in a high speed and memory type display device and particularly to provide a large-area, high-resolution display. For an optical modulating device by use of a liquid crystal having such bistability to exhibit desirable driving characteristics, it is required that the liquid crystal disposed between a pair of substrates should be in such a molecular alignment state that conversion between the above two stable states may occur effectively irrespective of the application of an electrical field. Further, in a liquid crystal device utilizing birefringence of a liquid crystal, the transmittance under right angle cross nicols is given by the following equation: I/I 0 = sin 2 4 sin 2 (Δnd/λ)π, wherein I 0 : incident light intensity, I: transmitted light intensity, : tilt angle, Δn: refractive index anisotropy, d: thickness of the liquid crystal layer, λ: wavelength of the incident light. The tilt angle  in the above-mentioned non-helical structure is recognized as a half of an angle between the average molecular axis directions of liquid crystal molecules in a twisted alignment in a first orientation state and a second orientation state. According to the above equation, it is shown that a tilt angle  of 22.5 degrees provides a maximum transmittance and the tilt angle in a non-helical structure for realizing bistability should desirably be as close as possible to 22.5 degrees. A method for aligning a ferroelectric liquid crystal should desirably be such that molecular layers each composed of a plurality of molecules of a smectic liquid crystal are aligned uniaxially along their normals, and it is desirable to accomplish such an alignment state by a rubbing treatment which requires only a simple production step. As an alignment method for a ferroelectric liquid crystal, particularly a chiral smectic liquid crystal in a non-helical structure, one disclosed in U.S. Patent No. 4,561,726 has been known for example. However, there has been found a problem that, when such a ferroelectric liquid crystal device of a cell structure is continually driven for a long time, the thickness along a cell side is gradually increased to show a pale yellow tint. If such yellowing occurs on one side of a display cell, the display image quality is impaired. The occurrence of the yellowing is not limited to on a monochromatic image display but also causes a deviation in color balance on a color display, thus hindering a high-quality image display. Incidentally, such a display device is provided with an electrode matrix comprising scanning electrodes and data electrodes for multiplexing drive of a chiral smectic liquid crystal including sequential application of a scanning signal to the scanning electrodes and application of data signals to the data electrodes in synchronism with the scanning signal. Further, according to our experiments, it has been found that a tile angle  (an angle shown in Figure 6 as described below) in a ferroelectric liquid crystal with a non-helical structure obtained by alignment with an alignment control film of the prior art has become smaller as compared with a tilt angle H ○ (the angle H ○ is a half of the apex angle of the cone shown in Figure 5 as described below) in the ferroelectric liquid crystal having a helical structure. Particularly, the tilt angle  in a ferroelectric liquid crystal with a non-helical structure obtained by alignment with alignment control films of the prior art was found to be generally on the order of 3 - 8 degrees, and the transmittance at that time was at most about 3 to 5 %. Thus, according to Clark and Lagerwall, the tilt angle in a ferroelectric liquid crystal with a non-helical structure realizing bistability should have the same angle as the tilt angle in the ferroelectric liquid crystal having a helical structure, but in fact the tilt angle  in a non-helical structure is smaller than the tilt angle H ○ in a helical structure. More specifically, it has been found that the tilt angle  in a non-helical structure becomes smaller than the tilt angle H ○ because of a twist alignment of liquid crystal molecules in the non-helical structure. Thus, in a ferroelectric liquid crystal having a non-helical structure, liquid crystal molecules are aligned with a twist from a molecular axis adjacent to an upper substrate to a molecular axis adjacent to a lower substrate continuously at a certain twist angle. This leads to a phenomenon that the tilt angle  in the non-helical structure is smaller than the tilt angle H ○ in the helical structure. Incidentally, there has been also proposed a ferroelectric liquid crystal device wherein an AC electric field is applied to change an alignment state (Japanese Laid-Open Patent Application (JP-A) 62-161123). By the application, the tilt angle  in the non-helical structure can be increased, and the alignment or C-directors between the substrates can be changed from a twist alignment to a parallel alignment (uniform alignment) having almost identical C-directors. As a result, the transmittance in the dark state under cross nicols can be lowered to provide a higher contrast. In the Patent Abstracts of Japan, vol. 15, no. 165 (P-1195), and JP-A-3 033 722, as well as in US-A-5 076 671 which is assumed to contain the same disclosure as JP-A-3 033 722, there is disclosed a liquid crystal device including a pair of substrates each having an electrode, an insulating film having an uneveness, an orientation controlling film being provided on at least one of the substrates through a base layer and having a uniaxial orientation processing axis, and a ferroelectric smectic liquid crystal which is disposed between the substrates. SUMMARY OF THE INVENTION An object of the present invention is to minimize the increase in cell thickness within a liquid crystal cell using a ferroelectric liquid crystal. A further object of the present invention is to suppress the liquid crystal movement in a ferroelectric liquid crystal device, thus preventing the yellowing due to a cell thickness increase or the occurrence of a void. Another object of the present invention is to provide a ferroelectric liquid crystal device wherein the movement of liquid crystal molecules during a long term drive of the device to provide an improved reliability of display characteristics, such as high contrast and freeness from persistence or after-image. A further object of the invention is to provide a ferroelectric liquid crystal device wherein the local change in cell thickness during drive is prevented, and a process for producing the device. Another object of the invention is to provide a process for producing an alignment control film having an unevenness of optimum shape, size and density to minimize the liquid crystal movement while retaining the good alignment characteristic. A further object of the invention is to provide a ferroelectric liquid crystal device with a large tilt angle  in a non-helical structure of a chiral smectic liquid crystal, which can realize a display showing a high contrast image free from persistence. A further object of the invention is to provide a ferroelectric liquid crystal device with an improved device structure by which a latitude of material selection is increased to allow a simple production process at low temperatures which is good at productivity and has a broader latitude of selection of other materials for, e.g., color filter. According to the present invention, there is provided a ferroelectric liquid crystal device according to claim 1. According to the invention, there is further provided a ferroelectric liquid crystal device according to claim 2. According to the invention, there is provided a process for producing a ferroeletric liquid crystal device according to claim 9. According to the invention, there is further provided a process for producing a ferroelectric liquid crystal device according to claim 10. These and other objects, features and advantages of the present invention will become more apparent upon a consideration of the following description of the preferred embodiments of the present invention taken in conjunction with the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Figures 1A and 1B are explanatory views for illustrating a cell thickness increase along a cell side in relation with liquid crystal movement directions. Figure 2 is an explanatory view for illustrating an alignment state occurring in a chiral smectic liquid crystal used in the invention. Figures 3A and 3B are explanatory views for illustrating changes in director orientation according to various positions between substrates in C1 alignment and C2 alignment, respectively. Figure 4 is a front view of a conventional liquid crystal display apparatus when it is driven for a long time for displaying a fixed pattern. Figure 5 is a perspective view showing schematically an alignment of a chiral smectic liquid crystal having a helical structure. Figure 6 is a perspective view showing schematically an alignment state of a chiral smectic liquid crystal having a non-helical structure. Figures 7, 8 and 9 are schematic sectional views of three embodiments of the liquid crystal device (cell) according to the invention. Figure 10 is a schematic sectional view showing an alignment state of a chiral smectic liquid crystal aligned according to the present invention. Figure 11 is an illustration of C-director alignments in a uniform alignment state. Figure 12 is an illustration of C-director alignments in a splay alignment state. Figures 13A and 13B are plan views illustrating tilt angles  in a uniform alignment state and a splay alignment state, respectively. Figure 14 is a sectional view showing a charge distribution, a direction of a spontaneous polarization P S and a direction of a reverse electric field Vrev. Figure 15 is a schematic plan view illustrating changes in tilt angle  during and after application of an electric field. Figures 16 and 17 are graphs showing optical response characteristics according to a conventional device and the present invention, respectively. Figure 18 is a waveform diagram illustrating driving waveforms used in an embodiment of the present invention. DESCRIPTION OF THE PREFERRED EMBODIMENTS We have analyzed the yellowing caused by the increase in cell thickness at the cell side. According to our study, the increase in cell thickness at the cell side is recognized to be caused by a pressure increase which in turn is caused by movement of liquid crystal molecules in a particular direction due to driving. Presumably, such a force causing the liquid crystal molecule movement may be attributable to an electrodynamic effect caused by perturbation of liquid crystal molecule dipole moments in an AC-like electric field caused by continuation of drive pulses. Further, according to our experiments, the directions 22a and 22b of the liquid crystal movement are determined in relation with the rubbing direction 20 and the average liquid crystal molecular axis position 21a or 21b as shown in Figure 1A. As the moving direction of liquid crystal molecules is related with the rubbing direction, the above-mentioned phenomenon is assumed to depend on the pre-tilt state at the substrate surfaces. Referring to Figures 1A and 1B, reference numeral 21a (or 21b in a reverse orientation state) denotes an average molecular axis (director) orientation. When the liquid crystal molecules (described herein as having a negative spontaneous polarization) are oriented to provide the average molecular axis 21a and are supplied with a certain strength of AC electric field not causing a switching to the orientation state 21b, the liquid crystal molecules are liable to move in the direction of an arrow 22a in the case where the substrates are provided with rubbing axes extending in parallel and in the same direction 20. This liquid crystal movement phenomenon depends on an alignment state in the cell. More specifically, this phenomenon hardly occurs in C2 alignment but is remarkably observed in C1 alignment and uniform alignment described hereinafter. The two alignment states C1 and C2 may be explained by a difference in chevron structure of smectic layers as shown in Figure 2. Referring to Figure 2, reference numeral 31 denotes a smectic layer showing ferroelectricity, 32 denotes a C1 alignment region, and 33 denotes a C2 alignment region. A smectic liquid crystal generally has a layer structure and causes a shrinkage of layer pitch when it is transformed from SmA (smectic A) phase into SmC (smectic C) phase or SmC* (chiral smectic C) phase, to result in a structure accompanied with a bending of layers between the upper and lower substrates 14a and 14b (chevron structure) as shown in Figure 2. The bending of the layers 31 can be caused in two ways corresponding to the C1 and C2 alignment as shown. As is well known, liquid crystal molecules at the substrate surfaces are aligned to form a certain angle α (pre-tilt) as a result of rubbing in a direction A in such a manner that their heads (leading ends) in the rubbing direction are up (or away) from the substrate surfaces 11a and 11b. Because of the pre-tilt, the C1 and C2 alignment states are not equivalent to each other with respect to their elastic energy, and a transition between these states can be caused at a certain temperature or when supplied with a mechanical stress. When the layer structure shown in Figure 2 is viewed in plan as shown in the upper part of Figure 2, a boundary 34 of transition from C1 alignment (32) to C2 alignment (33) in the rubbing direction A looks like a zigzag lightning and is called a lightning defect, and a boundary 35 of transition from C2 alignment (33) to C1 alignment (32) forms a broad and moderate curve and is called a hairpin defect. When FLC is disposed between a pair of substrates 14a and 14b and placed in an alignment state satisfying a relationship of H < α + δ (1) , wherein α denotes a pretilt angle of the FLC, H ○ denotes a tilt angle (a half of cone angle), and δ denotes an angle of inclination of SmC* layer, there are four states each having a chevron structure in the C1 alignment state. These four C1 alignment states are different from the known C1 alignment state. Further, two among the four C1 alignment states form bistable states (uniform alignment). Herein, two states among the four C1 states giving an apparent tilt angle  a therebetween in the absence of an electric field satisfying a relationship of H >  a > H /2 (2) are inclusively referred to as a uniform state. In the uniform state, the directors are believed to be not twisted between the substrates in view of optical properties thereof. Figure 3A is a schematic view illustrating director positions between the substrates in the respective states in C1 alignment. More specifically, at 51 - 54 are respectively shown changes in director positions between the substrates in the form of projections of directors onto cone bottoms as viewed from each bottom. At 51 and 52 is shown a splay state, and at 53 and 54 is shown a director arrangement which is believed to represent a uniform alignment state. As is understood from Figure 3A, at 53 and 54 representing a uniform state, the molecule position (director) is different from that in the splay state either at the upper substrate or lower substrate. Figure 3B shows two states in C2 alignment between which no switching is observed at the boundaries but an internal switching is observed. The uniform state in C1 alignment provides a larger tilt angle  a and thus a higher brightness and a higher contrast than the conventionally used bistable state in C2 alignment. However, in a ferroelectric liquid crystal having a uniform alignment state based on the condition of H > a > H /2 , the above-mentioned problem of the yellowing due to the liquid crystal movement is liable to occur. In an actual liquid crystal cell, the liquid crystal movement occurs as shown in Figure 1A. For example, when the liquid crystal molecules in the entire cell are placed in a state providing an average molecular axis direction 21a, the liquid crystal molecules in the cell are liable to move under AC application in the direction of the arrow 22, i.e., from the right to the left in the figure. As a result, the cell thickness in a region 23 is increased gradually to show a yellowish tint. If the liquid crystal molecules are placed in a state providing an average molecular axis 21b, the liquid crystal movement under AC application is caused in the reverse direction 22b. In either case, the liquid crystal movement is caused in a direction perpendicular to the rubbing direction, i.e., in the direction of extension of smectic layers. According to another experiment of ours, when a ferroelectric liquid crystal cell 60 including a ferroelectric liquid crystal of a non-helical structure in a high pretilt alignment state in a cell region defined by a sealant 69 is driven by a driver including a scanning electrode driver circuit 62 and a data electrode driver circuit 64 to continuously write in a white (61) or black (63) fixed pattern as shown in Figure 4, liquid crystal molecules are caused to move in different directions B and C in parallel with the extension direction of chiral smectic C layers and perpendicular to the rubbing direction A corresponding to the molecular positions for displaying a white display state (region 61) and a black display state (region 63), respectively. As a result, at the destination sides of the liquid crystal molecular movement, the liquid crystal layer is caused to have an increased thickness while enlarging the cell gap to form portions 65 colored in pale yellow (yellowing). On the opposite sides of the liquid crystal molecular movement, voids 67 lacking liquid crystal molecules are formed. These phenomena are caused most noticeably in the neighborhood of the seal 69 and propagated toward the inside of the cell. As described above, we have found that the liquid crystal movement in one direction is caused in a long term of drive to cause a slight change in cell thickness, thus resulting in yellowing or color deviation adversely affecting the display characteristics. More specifically, in the destination side in the liquid crystal movement direction, the cell thickness is liable to be increased to result in a yellowish tint. On the opposite side, a state with a less amount of liquid crystal results to cause a disorder in alignment. Accordingly, a liquid crystal device causing these phenomena as a result of long term drive shows a uniformity in display performance which is much worse than the initial state, thus being accompanied with a problem in reliability. The above-mentioned change in cell thickness cause further difficulties including changes in drive voltage threshold characteristics and adverse effects to durability of the liquid crystal device in a long term of continuous drive. As a result of further study, we have found that the liquid crystal movement in a planar direction is effectively suppressed by providing a fine surface unevenness pattern to an alignment control layer formed on an electrode plate, so that the above-mentioned problem of cell thickness increase on a cell side can be solved. Further, we have also found that a specific unevenness pattern (or dimples) provided to the alignment control layer surface can result in a homogeneous alignment with a remarkably suppressed liquid crystal movement. In other words, we have found that the liquid crystal behavior strongly depends on the physical states of the substrate boundary, i.e., the surfaces of alignment control films, and the liquid crystal movement is remarkably suppressed by an appropriate size of unevenness provided to the alignment control film surfaces. As stated above, in order for an optical modulation device utilizing bistability to exhibit desirable driving characteristics, it is important that the liquid crystal disposed between a pair of substrates should be in such an alignment state that conversion between two stable states may occur effectively irrespective of the application of an electric field, i.e., in a good uniaxial alignment state. Further, in order to realize a switching device having a high luminance and a high speed, it is necessary to use a ferroelectric liquid crystal having a large spontaneous polarization. However, in case where a thick alignment film and/or a high-impedance insulating film is used, a large spontaneous polarization can cause a reverse electric field, which can remarkably impair switching characteristic and even cause a failure in operation as a display device in some cases. This should require a caution. Our experiments have also revealed that too large a decrease in alignment control film thickness so as to reduce the influence of the reverse electric field can impair the homogeneity of ferroelectric liquid crystal alignment, thus causing a failure in function as a display device in some cases. The above described objects of the present invention can be accomplished by forming an unevenness at the surface of an insulating layer constituting a layer beneath an alignment film More specifically, in the present invention, a prescribed unevenness is formed at the surface of an insulating layer to prevent or decrease the liquid crystal movement, thereby preventing or decreasing the occurrence of the yellowing or occurrence of voids in a cell due to the cell thickness change to provide a ferroelectric liquid crystal device showing a high contrast and little change in display characteristic with time. Further, in the present invention, the unevenness in the insulating layer may be produced in a process which is simple and also good at reproducibility. In the present invention, the unevenness may be formed by incorporating fine particles in a layer forming an insulating film and then forming an alignment film on the insulating film or by further rubbing the alignment film to remove the tine particles from the insulating layer to form an unevenness at the surface of the insulating film or alignment film. These are preferred embodiments and may be appropriately combined as desired. The unevenness thus formed can vary to some extent depending on factors, such as liquid crystal material used, alignment film material, thicknesses of alignment film and insulating layer, cell gap and conditions for driving the liquid crystal device, but may preferably be as follows. The unevenness formed in the insulating layer may preferably have a width of 0.1 - 20 µm, a difference in height (as formed between an adjacent pair of convexity and concavity) of 10-200 nm (100 - 2000 Å), more preferably 10-50 nm (100 - 500 Å). In case where the unevenness is composed of individual convexities or/and concavities, the unevenness may preferably be formed at a pitch of at most 100 nm (1000 Å), more preferably 10-100 nm (100 - 1000 Å), and the convexities or concavities may preferably be formed at a density of at least 2500/mm 2 . If the average difference in height formed in the insulating layer exceeds 50 nm (500 Å), the liquid crystal alignment is liable to be disordered because of too large an unevenness while it can depend on the thickness of the alignment film formed thereon. On the other hand, if the average difference in height is below 10 nm (100 Å), the effect thereof can be insufficient by forming an alignment film thereon in some cases. If the unevenness pitch is below 10 nm (100 Å), the effect can be insufficient in some cases. If the pitch exceeds 100 nm (1000 Å), the unevenness distribution is sparse, and the effect thereof can be insufficient in some cases. In the case where fine particles are incorporated in the insulating layer, the fine particles may preferably have an average particle size (diameter) D satisfying D < 50 di, more preferably D < 2di, further preferably D > di/2, wherein di denotes the thickness of the insulating layer, which may be a desired thickness but may preferably be about 30 nm (30 Å) - 1 µm, more preferably 4-200 nm (40 - 2000 Å). The degree of unevenness formed in the insulating layer is closely related with the unevenness of the alignment film formed thereon and is therefore an important factor, but the unevenness formed at the surface of the alignment film directly affect the performance and is therefore more important. The unevenness formed at the surface of the alignment film may preferably have a difference in height of at most 50 nm (500 Å), more preferably 2-50 nm (20 - 500 Å), further preferably 2-30 nm (20 - 300 Å), and may preferably be formed at a pitch of at most 100 nm (1000 Å), more preferably 10-100 nm (100 - 1000 Å), and a density of 10000/mm 2 , more preferably 10 4 - 2x10 7 /mm 2 . The unevenness may have an arbitrary shape but may preferably comprises concavities in the form of dimples or convexities in the form of dots, semispheres or domes because these shapes can be easily formed by using fine particles. Similarly, circular concavities or convexities are also preferred. The thickness of the alignment film may be set to show an appropriate degree of function of preventing or suppressing the liquid crystal movement while showing a sufficient alignment effect and may preferably be 3 nm (30 Å) - 1 µm, more preferably be 5-100 nm (50 - 1000 Å), further preferably at most 10 nm (100 Å). The dimples or concavities formed may have a depth Dd satisfying da < Dd < 100da with respect to the thickness da of the alignment film. The present invention is most effective when applied to a liquid crystal device using a ferroelectric liquid crystal, particularly a ferroelectric liquid crystal showing a larger pretilt angle, more specifically of at least 5 degrees, more preferably at least 10 degrees, further preferably at least 15 degrees. The operation of a ferroelectric liquid crystal is explained with reference to schematic perspective views of liquid crystal cells as shown in Figures 5 and 6. Figure 5 is a schematic illustration of a ferroelectric liquid crystal cell (device) for explaining operation thereof. Reference numerals 521a and 521b denote substrates (glass plates) on which a transparent electrode of, e.g., In 2 O 3 , SnO 2 , ITO (indium-tin-oxide), etc., is disposed, respectively. A liquid crystal of an SmC*-phase (chiral smectic C phase) or SmH*-phase (chiral smectic H phase) in which liquid crystal molecular layers 522 are aligned perpendicular to surfaces of the glass plates is hermetically disposed therebetween. Full lines 523 show liquid crystal molecules. Each liquid crystal molecule 523 has a dipole moment (P ⊥ ) 524 in a direction perpendicular to the axis thereof. The liquid crystal molecules 523 continuously form a helical structure in the direction of extension of the substrates. When a voltage higher than a certain threshold level is applied between electrodes formed on the substrates 521a and 521b, a helical structure of the liquid crystal molecule 523 is unwound or released to change the alignment direction of respective liquid crystal molecules 523 so that the dipole moment (P ⊥ ) 524 are all directed in the direction of the electric field. The liquid crystal molecules 523 have an elongated shape and show refractive anisotropy between the long axis and the short axis thereof. Accordingly, it is easily understood that when, for instance, polarizers arranged in a cross nicol relationship, i.e., with their polarizing directions crossing each other, are disposed on the upper and the lower surfaces of the glass plates, the liquid crystal cell thus arranged functions as a liquid crystal optical modulation device of which optical characteristics vary depending upon the polarity of an applied voltage. Further, when the liquid crystal cell is made sufficiently thin (e.g., 0.1 - 3 microns), the helical structure of the liquid crystal molecules is unwound to provide a non-helical structure even in the absence of an electric field, whereby the dipole moment assumes either of the two states, i.e., Pa in an upper direction 534a or Pb in a lower direction 534b as shown in Figure 6, thus providing a bistable condition. When an electric field Ea or Eb higher than a certain threshold level and different from each other in polarity as shown in Figure 6 is applied to a cell having the above-mentioned characteristics, the dipole moment is directed either in the upper direction 534a or in the lower direction 534b depending on the vector of the electric field Ea or Eb. In correspondence with this, the liquid crystal molecules are oriented in either of a first stable state 533a and a second stable state 533b. A first advantage attained by using such a ferroelectric liquid crystal cell is that the response speed is quite fast, and a second advantage is that the orientation of the liquid crystal shows bistability. The second advantage will be further explained, e.g., with reference to Figure 6. When the electric field Ea is applied to the liquid crystal molecules, they are oriented in the first stable state 533a. This state is stably retained even if the electric field is removed. On the other hand, when the electric field Eb of which direction is opposite to that of the electric field Ea is applied thereto, the liquid crystal molecules are oriented to the second stable state 533b, whereby the directions of molecules are changed. This state is similarly stably retained even if the electric field is removed. Further, as long as the magnitude of the electric field Ea or Eb being applied is not above a certain threshold value, the liquid crystal molecules are placed in the respective orientation states. Hereinbelow, some embodiments of the ferroelectric liquid crystal device according to the present invention will be described. Figures 8 and 9 are schematic sectional views of embodiments of the ferroelectric liquid crystal device (cell) according to the present invention. In the present invention, the ferroelectric liquid crystal may be used in a chiral smectic phase, more specifically in chiral smectic C phase (SmC*), H phase (SmH*), I phase (SmI*), K phase (SmK*), G phase (SmG*) or F phase (SmF*). Details of ferroelectric liquid crystals are described, e.g., in Journal De Physique Letters 36 (L-69), 1975, "Ferroelectric Liquid Crystals"; Applied Physics Letters 36 (11), 1980, "Submicro Second Bi-stable Electrooptic Switching in Liquid Crystals"; Solid State Physics (Kotai Butsuri), 16 (141), 1981, "Liquid Crystal"; U.S. Patents Nos. 4,561,726, 4,589,996, 4,592,858, 4,596,676, 4,613,209, 4,614,609, and 4,62,165. Ferroelectric liquid crystals disclosed in these references may be used in the present invention. A particularly preferred class of ferroelectric liquid crystal may include those showing cholesteric phase on a higher temperature side, which may for example include a pyrimidine-based mixture liquid crystal showing the following phase transition series. The ferroelectric liquid crystal device shown in Figure 8 may be obtained by dispersing spacer beads 1714 of, e.g., silica or alumina on the alignment control layer of either one of the pair of electrode plates 1712a and 1712b, then combining the electrode plates so that the uniaxial alignment directions provided to the alignment control layers 1713a and 1713b are substantially parallel and in the same direction as shown (or substantially parallel and in the opposite direction), and bonding the electrode plates with an optional particulate adhesive used in combination with the spacer beads 1714 and with an epoxy adhesive for sealing the periphery to form a blank cell having an injection port. Then, the cell is filled with a liquid crystal 1717 as described above heated to a temperature preferably giving cholesteric phase or a higher temperature phase and, after sealing the injection port, is cooled to a temperature giving the chiral smectic phase. Hereinbelow, an embodiment of the liquid crystal device using an insulating film containing fine particles is described. Figure 9 is a schematic sectional view of such an embodiment. Referring to Figure 9, the device includes substrates (glass plates) 2211a and 2211b coated with transparent electrodes 2212a and 2212b, respectively, of, e.g., In 2 O 3 or ITO (indium tin oxide) and then with 5-200 nm (50 to 2000 Å)-thick insulating films 2213a and 2213b (of, e.g., Ti - Si) and with 5-100 nm (50 to 1000 Å)-thick alignment films 2214a and 2214b, respectively. In this embodiment, the insulating layers 2213a and 2213b contain fine particles 2218 of, e.g., silica and alumina. The alignment films 2214a and 2214b have been rubbed in directions A which are parallel and in the same direction. Between the substrates 2211a and 2211b is disposed a ferroelectric chiral smectic liquid crystal 2215. The spacing between the substrates 2211a and 2211b is set to a small value (e.g., 0.1 - 3 µm) sufficient to suppress the formation of a helical structure of the chiral smectic liquid crystal so that the chiral smectic liquid crystal 2215 is placed in a bistable alignment state. The sufficiently small spacing for the liquid crystal 2215 is held by spacer beads 2216 (of e.g., silica or alumina) disposed between the alignment films 2214a and 2214b. The entire cell is sandwiched between polarizers 2217a and 2217b. The alignment films used in the present invention are not specifically limited but may preferably comprise a polyimide or polyamide, e.g., as represented by the following formula (1) and (2): wherein A denotes a tetravalent organic residue group, and R 1 and R 2 denote an alkyl or fluoroalkyl group each having 1 - 10 carbon atoms with the proviso that R 1 and R 2 may be the same or different; wherein B denotes a divalent organic residue group, and R 3 and R 4 denote an alkyl or fluoroalkyl group each having 1 - 10 carbon atoms with the proviso that R 3 and R 4 may be the same or different. In order to form the insulating film, a solution at a concentration of 0.01 - 40 wt. % is formed by using a solvent, such as hexylene glycol, n-butyl cellosolve and iso-propyl alcohol, and applied onto a substrate by a method, such as spinner coating, spray coating or roller coating. In this instance, tine particles are dispersed in the solution by ball milling or ultrasonic dispersion in advance. The coating on the substrate may be pre-baked for evaporation of the solvent at 60 - 150 °C for about 10 min., irradiated with ultraviolet rays and then baked for about 1 hour to 250 - 350 °C. The insulating layer may have a thickness on the order of 3 nm (30 Å) - 1 µm, preferably 5-200 nm (50 - 2000 Å). The thus formed insulating film is provided with a minute unevenness, which may function like columns formed by oblique evaporation to align liquid crystal molecules along inclined sides thereof. This may be the reason why a high contrast alignment is obtained thereby. In order to form the alignment film, a solution at a concentration of 0.01 - 40 wt. % is formed by using a solvent, such as dimethylformamide, dimethylacetamide, dimethyl sulfoxide, and N-methyl-2-pyrrolidone, and applied onto a substrate by a method, such as spinner coating, spray coating or roller coating, followed by heating at 100 - 300 °C, preferably 150 - 250 °C, to form an alignment film. The alignment film is then subjected to rubbing with, e.g., cloth. Figure 10 is a schematic sectional view showing an alignment state of liquid crystal molecules attained by using a polyamide complex alignment film in the liquid crystal device according to the present invention, and Figure 10 is a view showing alignment of corresponding C-directors. Reference numerals 2551a and 2551b in Figure 10 denote upper and lower substrates, respectively. Numeral 2550 denotes a molecular layer composed of liquid crystal molecules 2552, and liquid crystal molecules 2552 are aligned so as to change their positions along the bottom face 2554 (circular) of a cone 2553. Figure 11 more specifically shows a change in C-directors. Referring to Figure 11, at U 1 are shown C-directors 2581 (each being a projection of a molecular long axis onto an imaginary plane perpendicular to the normal to a molecular layer 2550) in one stable orientation state, and at U 2 are shown C-directors 2581 in the other stable orientation state. On the other hand, an alignment state attained by a conventional rubbing-treated polyimide film may be represented by a C-director diagram of Figure 12, which shows an alignment state wherein molecular axes are twisted in a large degree from the upper substrate 2551a to the lower substrate 2551b to provide a smaller tilt angle . Figure 13A is a schematic plan view illustrating a tilt angle  in an alignment state where C-directors 2581 assume a state shown in Figure 11 (referred to as "uniform alignment state"), and Figure 13B is a schematic plan view illustrating a tilt angle  in an alignment state where C-directors 2581 assume a state shown in Figure 12 (referred to as "splay alignment state"). In these figures, reference numeral 2560 denotes a rubbing axis provided to the above-mentioned fluorine-containing polyimide film, numeral 2561a denotes an average molecular axis in the orientation state U 1 , numeral 2561b denotes an average molecular axis in the orientation state U 2 , numeral 2562a denotes an average molecular axis in the orientation state S 1 , and numeral 2562b denotes an average molecular axis in the orientation state S 2 . The average molecular axes 2561a and 2561b can be switched to each other by applying voltages of mutually opposite polarities. Similar switching is caused between the average molecular axes 2562a and 2562b. Next, the effectiveness of the uniform alignment state with respect to a delay in optical response (after-image) due to a reverse electric field Vrev is explained. If the capacitance of an insulating layer constituting a liquid crystal cell is denoted by Ci, the capacitance of a liquid crystal layer is denoted by C LC and the spontaneous polarization of the liquid crystal is denoted by P S , Vrev causing after-image is expressed by the following equation. Vrev = 2P S /(Ci+C LC ) Figure 14 is a schematic sectional view illustrating changes in charge distribution direction of P S and direction of the reverse electric field in a liquid crystal cell. At Figure 14(a), there is shown a distribution of ⊕ and ⊖ charges in a memory state before application of a pulse electric field, where the spontaneous polarization is directed from ⊕ charges to ⊖ charges. At Figure 14(b) is shown a state immediately after removal of a pulse electric field, when the direction of the spontaneous polarization P S is opposite to that shown at Figure 14(a) (thus, the liquid crystal molecules are inverted from one stable orientation state to the other orientation state) but the distribution of the ⊕ and ⊖ charges is similar to that shown at Figure 14(a), so that a reverse electric field Vrev is generated as indicated by an arrow shown at Figure 14(b). The reverse electric field Vrev disappears in a short time to provide a distribution of ⊕ and ⊖ charges as shown at Figure 14(c). Figure 15 is a plan view showing a change in optical response in a splay alignment state given by a conventional polyimide alignment film in terms of a change in tilt angle . Referring to Figure 15, at the time of application of a pulse electric field, the orientation of liquid crystal molecules is changed from an average molecular axis S(A) in a splay alignment state to be overshot to an average molecular axis U 2 in a uniform alignment state close to that providing a maximum tilt angle H ○ along a path denoted by an arrow X 1 , and immediately after the removal of the pulse electric field, the orientation is changed along a path denoted by an arrow X 2 to an average molecular axis S(B) in a splay alignment state providing a decreased tilt angle  due to the action of the reverse electric field Vrev shown at Figure 14(b). Then, as the reverse electric field Vrev attenuates as shown at Figure 14(c), the orientation is changed along a path denoted by an arrow X 3 to an average molecular axis S(C) in a splay alignment state providing a stable orientation state having a somewhat increased tilt angle . The resultant optical response in this case is shown in Figure 16. In the alignment state given by using the polyimide film obtained by using a naphthalenetetracarboxylic acid of the present invention, the average molecular axes S(A), S(B) and S(C) in the splay alignment state shown in Figure 15 are not caused but it is possible to form an alignment state with an average molecular axis giving a tilt angle  which is close to a maximum tilt angle H ○ . An optical response at this time according to the present invention is shown in Figure 17. Figure 17 shows that a delay in optical response causing after-image is obviated and a high contrast in memory states is caused. The alignment film in the present invention is not restricted to a specific structure but may include polyimides prepared in the following manner as preferred examples. Examples of the tetracarboxylic acid component constituting the polyimide may include: pyromellitic dianhydride, biphenyltetracarboxylic dianhydride, naphthalenetetracarboxylic dianhydride, and cyclobutanetetracarboxylic dianhydride. Examples of the diamine component may include bis[4-(aminophenoxy)phenyl] compounds represented by the following formula (I): wherein R 1 and R 2 denote fluoroalkyl chain groups represented by CF 3 (CF 2 ) m (CH 2 ) L -, (L ≧ 0, m ≧ 0) with the proviso that R 1 and R 2 may be the same or different. The liquid crystal material used in the present invention may preferably be one showing a phase transition from isotropic phase through cholesteric phase and smectic A phase into chiral smectic C phase in the course of temperature decrease. Particularly, a chiral smectic liquid crystal showing a helical pitch of 0.8 µm (micron) or longer in cholesteric phase (measured at a mid temperature in the cholesteric range). Preferred examples of such a liquid crystal material may include liquid crystal materials (1) - (5) below comprising the following liquid crystals "LC-1", "80B" and "80SI*" in the indicated proportions by weight. Liquid crystal material (1) (LC-1) 90 /(80B) 10 (2) (LC-1) 80 /(80B) 20 (3) (LC-1) 70 (80B) 30 (4) (LC-1) 60 /(80B) 40 (5) (80SI*) 100 Hereinbelow, the present invention will be described with respect to some specific examples. Example 1 Figure 7 is a schematic sectional view of an embodiment of the liquid crystal cell according to the present invention. Referring to Figure 7, the liquid crystal cell includes a pair of an upper substrate 1011a and a lower substrate 1011b disposed in parallel with each other and provided with, e.g., about 40-300 nm (400 to 3000 Å)-thick transparent electrodes 1012a and 1012b. Between the upper substrate 1011a and the lower substrate 1011b is disposed a ferroelectric liquid crystal 1015, preferably a ferroelectric smectic liquid crystal disposed in a non-helical structure providing at least two stable states. On the transparent electrodes 1012a and 1012b, e.g., 10-300 nm (100 to 3000 Å)-thick insulating films 1013a and 1013b, respectively, are disposed. On the insulating films 1013a and 1013b are further disposed, e.g., 5-100 nm (50 to 1000 Å)-thick alignment control films 1014a and 1014b, respectively. The alignment control films may generally comprise a polymer but may preferably be one providing a high pretilt angle, e.g., one comprising a fluorine-containing polyimide. In this specific example, the liquid crystal cell was prepared by forming transparent ITO electrodes 1012a and 1012b on glass substrates 1011a and 1011b and further thereon insulating films of wet application-baking type, which were formed by disposing 200 nm (2000 Å)-dia. silica beads (available from Ube Nitto Kasei K.K.) in a mixture solution of an organic titanium compound and an organic silicon compound to form a coating liquid and applying the coating liquid onto the transparent electrodes by Angstromer in a thickness of 100 nm (1000 Å), followed by baking at 300 °C. Incidentally, it is also possible to dispose a tantalum oxide by sputtering below the above insulating film to provide a two-layer structure. Thereon, a 1 %-NMP solution of a polyimide precursor ("LQ-1802", mfd. by Hitachi Kasei K.K.) was applied by a spinner and baked at 270 °C for 1 hour, followed by rubbing. Two substrates treated in this way were applied to each other with a 1.5 µm gap held therebetween so that their rubbing directions were parallel and in the same direction, to form a cell. The cell was then filled with a pyrimidine-based liquid crystal showing the following phase transition series. tilt angle H ○ = 14 degrees layer inclination angle δ = 11 degrees apparent tilt angle  a = 11 degrees. The alignment control film formed in the cell provided a pretilt angle α of 17 degrees. Thus, the cell satisfied the relationships (1) and (2), and the C1 uniform alignment was developed stably. Then, the entire cell was brought to an orientation state providing the average molecular axis direction 21 in Figure 1A and then subjected to application for 7 hours of rectangular wave signals having a pulse width (Δt) of 25 µsec, a voltage amplitude Vpp of 40 volts and a duty ratio of 1/2. Thereafter, the cell thickness in the region 23 in Figure 1B was measured and found to show only an increase of about 10 % with respect to the initial value. Example 2 A liquid crystal cell was prepared in the same manner as in Example 1 except that 500 nm (5000 Å)-dia. particles ("Microgel, mfd. by Nippon Paint K.K.) were used for preparing the insulating films, and subjected to the same evaluation, whereby the cell thickness increase was only about 5 % with respect to the initial thickness. Comparative Example For comparison with Examples 1 and 2, a liquid crystal cell was prepared in the same manner except that no fine particles were mixed in preparation of the insulating films, and subjected to the same evaluation, whereby the cell thickness increase in the region 23 of Figure 1B was about 30 % with respect to the initial thickness. Example 3 Figure 8 is a schematic sectional view of another embodiment of the liquid crystal cell according to the present invention. Referring to Figure 8, the liquid crystal cell includes a pair of an upper substrate 1711a and a lower substrate 1711b disposed in parallel with each other and provided with, e.g., about 40-200 nm (400 to 2000 Å)-thick transparent electrodes 1712a and 1712b. Between the upper substrate 1711a and the lower substrate 1711b is disposed a ferroelectric liquid crystal 1717, preferably a ferroelectric smectic liquid crystal disposed in a non-helical structure providing at least two stable states. On the transparent electrodes 1712a and 1712b, e.g., 10-200 nm (100 to 2000) Å-thick insulating films 1718a and 1718b, respectively, are disposed. The insulating films 1718a and 1718b may preferably be formed by an insulating material of wet application-baking type. More specifically, it is possible to use a mixture solution of an organic titanium compound and an organic silicon compound. The mixture solution may be applied by printing as by Angstromer, etc., dried at about 150°C and baked at 300°C to form an insulating film. The fine particles 1719 are dispersed at the surface of the insulating films 1718a and 1718b and may comprise fine particles of inorganic materials, such as silica and titania, or organic materials, such as acrylic resins and polystyrene. The fine particles 1719 may preferably have an average diameter Dp satisfying da < Dp < 100da with respect to the thickness da of alignment control films 1713a and 1713b formed on the insulating films, more specifically in the range of 50 nm ≦ Dp ≦ 5000 nm with respect to the alignment control film thickness da in the range of 10 nm ≦ da ≦ 100 nm. The fine particles 1719 may preferably be dispersed at a density of 0.1 - 10 pieces/µm 2 , more preferably 0.5 - 5 pieces/µm 2 . In order to enhance the insulating between the pair of substrates, it is possible to insert an additional inorganic oxide insulating film layer of, e.g., 20-300 nm (200 - 3000 Å) in thickness, e.g., by sputtering, between the insulating film 1718 (and/or 1718b) and the transparent electrode 1712a (and/or 1712b). After the baking of the insulating films 1718a and 1718b, the alignment control films 1713a and 1713b may be formed thereon, e.g., as a 1 to 100 nm (10 to 1000 Å)-thick film of an organic polymer, such as a polyimide. The alignment control films 1713a and 1713b may be rubbed in directions which are almost parallel and in the same direction. The spacing between the substrates may be held by, e.g., silica beads 1714 having an average particle size of about 1.5 µm (0.1 - 3.5 µm, in general) and a particulate adhesive 1715. The periphery of the cell is sealed by a sealant 1716. In a specific example, a liquid crystal cell was prepared in the above-described manner. Then, the entire cell was brought to an orientation state providing the average molecular axis direction 21 in Figure 1A and then subjected to application for 7 hours of rectangular wave signals having a pulse width (Δt) of 25 µsec, a voltage amplitude Vpp of 40 volts and a duty ratio of 1/2. Thereafter, the cell thickness (gap) in the region 23 in Figure 1B was measured and found to show only an increase of about 10 % with respect to the initial value. Example 4 Two 1.1 mm-thick glass plates each provided with 100 nm (1000 Å)-thick ITO electrodes were coated with a 6.0 wt. % insulating film-forming solution (of Ti/Si = 1/1) containing silica fine particles with an average diameter of 50 nm (500 Å) dispersed in advance therein by printing using an extender plate with a roughness of 16 µm, followed by prebaking at 100 °C for about 10 min., irradiation with ultraviolet rays and baking at 300 °C for 1 hour, to form a 90 nm (900 Å)-thick insulating film. Then, the insulating film on each substrate was coated with a 2.0 wt. % solution of a polyamide represented by the following structural formula 30-1 in a solvent mixture of N-methyl-pyrrolidone/n-butyl cellosolve (= 2/1) by spin coating, followed by baking at 220 °C for about 1 hour to form a 25 nm (250 Å)-thick film, which was then rubbed in one direction with a nylon-planted cloth. Onto one of the substrates thus treated, alumina beads of about 1.5 µm in average diameter were dispersed, and the other substrate was applied thereto so that their rubbing directions were parallel and in the same direction, to form a blank cell. The blank cell was then filled with ferroelectric smectic liquid crystal ("CS-1014" trade name; available from Chisso K.K.) in isotropic phase under vacuum and, after sealing, was gradually cooled from isotropic phase at a rate of 0.5 °C/min. to about 30 °C, whereby an alignment was effected. The "CS-1014" liquid crystal in the cell showed the following phase transition series: ISO 80.5°C / Ch. 69 / SmA 50 / SmC*. The above-prepared liquid crystal cell was sandwiched between a pair of 90 degrees-cross nicol polarizers to provide a liquid crystal device and was supplied with a pulse of 50 µsec and 30 V. Then, the cross nicol polarizers were set at the extinction position (providing the darkest state), and the transmittance through the liquid crystal device at this time was measured by a photo-multiplier. Then, a pulse of 50 µsec and -30 V was applied to the device, and the transmittance (brightest state) at this time was measured in the same manner, whereby the following data were obtained. Tilt angle  = 15 degrees, transmittance in the brightest state = 32 %, transmittance in the darkest state = 1.3 %, contrast ratio = 25:1. The delay in optical response causing after-image was 0.3 sec or less. The liquid crystal device was subjected to multiplexing drive for display using driving waveforms shown in Figure 18, whereby a high-quality display with a high contrast was attained. Further, after an image display of a prescribed character image, the whole picture area was erased into "white", whereby no after-image was recognized. Referring to Figure 18, at S N , S N+1 and S N+2 are shown voltage waveforms applied to scanning lines, at I is shown a voltage waveform applied to a representative date line, and at (I-S N ) is shown a combined voltage waveform applied to the data line I and the scanning line S N . In the above embodiment, the drive was performed under the conditions of V 0 = 5 - 8 volts and ΔT = 20 - 70 µsec. Example 5 A liquid crystal cell was prepared in the same manner as in Example 4 except that a 20 nm (200 Å)-thick insulating film was formed by applying a 6.0 wt. % insulating film-forming solution (of Ti/Si = 1/1) containing silica fine particles with an average diameter of 15 nm (150 Å) dispersed in advance therein by printing using an extender plate of 5 µm, and an alignment film of a polyimide represented by the following formula 31-1 was formed through baking at 270 °C. The liquid crystal cell was subjected to the same test as in Example 4, whereby results including a contrast ratio of 23:1 and a delay in optical response of 0.2 sec were obtained. As a result of the same multiplexing display drive test as in Example 4, similarly good results were obtained with respect to contrast and after-image. Example 6 A liquid crystal cell was prepared in the same manner as in Example 4 except that a 20 nm (200 Å)-thick insulating film was formed by applying a 6.0 wt. % insulating film-forming solution (of Ti/Si = 1/1) containing silica fine particles with an average diameter of 15 nm (150 Å) dispersed in advance therein by printing using an extender plate of 5 µm. The liquid crystal cell was subjected to the same test as in Example 4, whereby results including a contrast ratio of 24:1 and a delay in optical response of 0.3 sec were obtained. As a result of the same multiplexing display drive test as in Example 4, similarly good results were obtained with respect to contrast and after-image. Comparative Example (1) For comparison with Examples 4 - 6, a liquid crystal cell was prepared in the same manner as in Example 4 except that the insulating film was formed without inclusion of the fine particles. The liquid crystal cell was subjected to the same test as in Example 4, whereby results including a contrast ratio of 14:1 and a delay in optical response to 2.1 sec were obtained. As a result of the same multiplexing display drive test as in Example 4, the contrast was lower than those in Examples 4 - 6, and, after-image was recognized. (2) For further, comparison, a liquid crystal cell was prepared in the same manner as in Example 5 except that a 90 nm (900 Å)-thick insulating film was formed by using an extender plate of 16 µm. The liquid crystal cell was subjected to the same test as in Example 4, whereby results including a contrast ratio of 12:1 and a delay in optical response of 2.5 sec were obtained. As a result of the same multiplexing display drive test as in Example 4, the contrast was lower than those in Examples 4 - 6, and, after-image was recognized. As described above, through improvement in physical and chemical surface states of the alignment films, the liquid crystal device according to the present invention can provide a display characteristic with good contrast and suppress the phenomenon of liquid crystal molecular movement occurring in a long term drive, thus being able to retain good and uniform display characteristics for a long term. Further, according to the present invention, it is possible to suppress liquid crystal molecular movement during drive by forming an unevenness at the surface of the insulating film, thus remarkably decreasing color change due to an increase in cell thickness along a cell side and retaining a stable alignment state within a long term drive. Moreover, according to the present invention, it is possible to reduce the liquid crystal movement within a cell and improve the display quality by incorporating fine particles within or at the surface of the insulating film. Further, according to the present invention, prescribed spherical fine particles are disposed at the surface of an insulating film, whereby the liquid crystal movement was reduced and the cell thickness increase at a cell side is reduced to prevent yellowing, while retaining a good alignment characteristic. Further, in the present invention, an unevenness is provided at the surface of an insulating film disposed below the alignment control film, so that the liquid crystal movement can be suppressed while retaining a good alignment characteristic without a substantial adverse effect to the alignment of the liquid crystal. Further, in the present invention, inorganic fine particles may be dispersed on a first insulating layer and then a second insulating layer may be formed by vacuum deposition, so that a shadowing effect of the inorganic fine particles can be effectively utilized for dimple formation. Thus, it is possible to optimize the effect of suppressing the yellowing and occurrence of void due to reduction in liquid crystal movement. Further, according to the present invention, the liquid crystal movement is suppressed and the cell thickness fluctuation is less liable, so that yellowing along a cell side can be prevented and a high-quality image display apparatus or recording apparatus can be provided. Further, according to the present invention, it is possible to realize a stable C1 uniform alignment, thus being able to realize an image display which shows a higher luminance and a higher contrast than those obtained by utilizing bistable states in a conventional C2 alignment. Further, according to the present invention, the latitude of selection of alignment film material is enlarged, so that a material, such as polyamide, not requiring a higher temperature treatment can also be used and the productivity can be improved. Further, the resultant liquid crystal device provides a high quality display as represented by a high contrast between bright and dark states, particularly a very high contrast during a multiplexing drive, and freeness from ugly after-image or persistence. Incidentally, the particles to be incorporated within or disposed at the surface of an insulating film need not be silica beads but can comprise particles of any materials which are resistant to the baking temperature, e.g., 300 °C. Further, the various embodiments of the present invention set forth above can be provided or combined with each other within the scope of the present invention as defined in the claims.

Claims: A ferroelectric liquid crystal device, comprising: a cell including a pair of substrates (1011a, 1011b) each having thereon an electrode (1012a, 1012b) for driving a liquid crystal (1015) and disposed opposite to each other, at least one the substrates (1011a, 1011b) further having on the electrode (1012a, 1012b) at least one layer of an insulating film (1013a, 1013b) and an alignment control film (1014a, 1014b) subjected to a uniaxial aligning treatment, and a ferroelectric liquid crystal (1015) sandwiched between the pair of oppositely disposed substrates (1011a, 1011b), characterized in that at least one of the insulating films contains fine particles (1019) dispersed therein and that the fine particles have a diameter D satisfying di/2 < D < 50 di with respect to the thickness di of said insulating film. A ferroelectric liquid crystal device, comprising: a cell including a pair of substrates (1711a, 1711b; 2211a, 2211b) each having thereon an electrode (1712a, 1712b; 2212a, 2212b) for driving a liquid crystal (1717; 2215) and disposed opposite to each other, at least one of the substrates (1711a, 1711b; 2211a, 2211b) further having on the electrode (1712a, 1712b; 2212a, 2212b) at least one layer of an insulating film (1718a, 1718b; 2213a, 2213b) and an alignment control film (1713a, 1713b; 2214a, 2214b) subjected to a uniaxial aligning treatment, and a ferroelectric liquid crystal (1717; 2215) sandwiched between the pair of oppositely disposed substrates (1711a, 1711b; 2211a, 2211b), characterized in that a plurality of fine particles (1719; 2218) having a diameter Dp are dispersed at the surface of the insulating film (1718a, 1718b; 2213a, 2213b), satisfying a relationship of da < Dp < 100 da with respect to the thickness da of said alignment control film (1713a, 1713b; 2214a, 2214b) formed on said insulating film (1718a, 1718b; 2213a, 2213b). A device according to claim 1 or 2, wherein said ferroelectric liquid crystal is in an alignment state satisfying H < α + δ , wherein α denotes a pretilt angle, H ○ denotes a tilt angle and δ denotes an inclination angle of chiral smectic C phase. A device according to any of the preceding claims, wherein said ferroelectric liquid crystal is in an alignment state providing at least two stable states of optical axes which form angle 2Θ a therebetween satisfying H > Θ a > H /2 , wherein H ○ denotes a tilt angle of the ferroelectric liquid crystal. A device according to any of the preceding claims, wherein said alignment film comprises a polyimide represented by the following formula (1): wherein A denotes a tetravalent organic residue group, and R 1 and R 2 denote an alkyl or fluoroalkyl group each having 1 to 10 carbon atoms with the proviso that R 1 and R 2 may be the same different. A device according to any of the preceding claims, wherein said alignment film comprises a polyamide represented by the following formula (2): wherein B denotes a divalent organic residue group, and R 3 and R 4 denote an alkyl or fluoroalkyl group each having 1 to 10 carbon atoms with the proviso that R 3 and R 4 may be the same different. A device according to Claim 1 or 2, wherein spacer beads (1017; 1714; 2216) are dispersed and sandwiched between the pair of substrates (1011a, 1011b; 1711a, 1711b; 2211a, 2211b). A device according to Claim 1 or 2, wherein a spacing between the pair of Substrates (1011a, 1011b; 1711a, 1711b) is held by spacer beads (1017; 1714) and an adhesive (1715) disposed between the pair of substrates (1011a, 1011b; 1711a, 1711b). A process for producing a ferroelectric liquid crystal device according to claim 1 or any one of claims 3 to 8 when dependant on claim 1, comprising the steps: providing a cell including a pair of substrates (1011a, 1011b) each having thereon an electrode (1012a, 1012b) for driving a liquid crystal (1015) and disposing them opposite each other; providing at least one layer of an insulating film (1013a, 1013b), in which fine particles (1019) having a diameter D satisfying di/2 < D < 50 di with respect to the thickness di of said insulating film are dispersed, and an alignment control film (1014a, 1014b) subjected to uniaxial alignment treatment, to the electrode (1012a, 1012b) of at least one of the substrates (1011a, 1011b); providing a ferroelectric liquid crystal (1015) between the pair of substrates. A process for producing a ferroelectric liquid crystal device according to claim 2 or any one of claims 3 to 8 when dependent on claim 2, comprising the steps of: providing a cell including a pair of substrates (1711a, 1711b; 2211a, 2211b) each having thereon an electrode (1712a, 1712b; 2212a, 2212b) for driving a liquid crystal (1717; 2215) and disposing them opposite to each other; providing at least one layer of an insulating film (1718a, 1718b; 2213a, 2213b), at the surface of which a plurality of fine particles (1719; 2218) having a diameter Dp are dispersed, satisfying a relationship of da < Dp < 100 da with respect to the thickness da of said alignment control film (1713a, 1713b; 2214a, 2214b) formed on said insulating film (1718a, 1718b; 2213a, 2213b), and an alignment control film (1713a, 1713b; 2214a, 2214b) subjected to uniaxial alignment treatment, to the electrode (1712a, 1712b; 2212a, 2212b) of at least one of the substrates (1711a, 1711b; 2211a, 2211b); providing a ferroelectric liquid crystal (1717; 2215) between the pair of substrates. A process according to claim 9 or 10, wherein the step of providing the insulating film comprises the step of applying a coating liquid. A process according to claim 10, wherein the step for forming the insulating layer (1718a, 1718b; 2213a, 2213b) on each substrate (1711a, 1711b; 2211a, 2211b) comprises: a first step of forming a first insulating layer on a substrate surface (1711a, 1711b; 2211a, 2211b) provided with a group of electrodes (1712a, 1712b; 2212a, 2212b) for liquid crystal drive, a second step of dispersing inorganic fine particles having a diameter of at most 1 µm on the substrate surface (1711a, 1711b; 2211a, 2211b) provided with the first insulating layer, and a third step of forming a second insulating layer on the substrate surface (1711a, 1711b; 2211a, 2211b) provided with the inorganic fine particles. A process according to claim 12, wherein the groups of electrodes (1712a, 1712b; 2212a, 2212b) formed on the pair of substrates constitute data electrodes and scanning electrodes, respectively. A process according to claim 12, wherein the second insulating layer is formed by vacuum deposition.

Inventors: ASAOKA MASANOBU, HANYU YUKIO, HOTTA YOSHIO, KODERA YASUTO, KOJIMA MAKOTO, MIHARA TADASHI, NAKAMURA KATSUTOSHI, ONUMA KENJI, TAKAO HIDEAKI, TANIGUCHI OSAMU, WADA TAKATSUGU, ASAOKA, MASANOBU, HANYU, YUKIO, HOTTA, YOSHIO, KODERA, YASUTO, KOJIMA, MAKOTO, MIHARA, TADASHI, NAKAMURA, KATSUTOSHI, ONUMA, KENJI, TAKAO, HIDEAKI, TANIGUCHI, OSAMU, WADA, TAKATSUGU, ASAOKA, MASANOBU, C/O CANON KABUSHIKI KAISHA, HANYU, YUKIO, C/O CANON KABUSHIKI KAISHA, Hotta, Yoshio, c/o Canon Kabushiki Kaisha, Kodera, Yasuto, c/o Canon Kabushiki Kaisha, Kojima, Makoto, c/o Canon Kabushiki Kaisha, MIHARA, TADASHI, C/O CANON KABUSHIKI KAISHA, NAKAMURA, KATSUTOSHI, C/O CANON KABUSHIKI KAISHA, Onuma, Kenji, c/o Canon Kabushiki Kaisha, Takao, Hideaki, c/o Canon Kabushiki Kaisha, TANIGUCHI, OSAMU, C/O CANON KABUSHIKI KAISHA, Wada, Takatsugu, c/o Canon Kabushiki Kaisha
Applicants: CANON KK, CANON KABUSHIKI KAISHA
Application year: 1992
Main classification: G02F1
IPC codes: G02F1, B82B1