A double-layered type liquid-crystal display device

Abstract: The liquid-crystal display device comprises a multi-layered-type liquid crystal cell that is composed of first and second cell layers, said cell containing liquid-crystal molecules with a twisted nematic orientation therein, wherein the angle of twist of the liquid-crystal molecules in the first cell layer is opposite to that of twist of the liquid-crystal molecules in the second cell layer; the orientation of the liquid-crystal molecules in the first cell layer that is the nearest the second cell layer is at an angle of 70 o to 150 o to that of the liquid-crystal molecules in the second cell layer that is the nearest the first cell layer; and the angle of twist of the liquid-crystal molecules in the first cell layer is different from the angle of twist of the liquid-crystal molecules in the second cell layer, thereby producing a black-and-white display image with high contrast without giving rise to color and a colored display image with high contrast.

Description: 1. Field of the invention: This invention relates to a double-layered-type liquid-crystal display device with the use of a twisted nematic display process that can produce a black-and-white display image with high contrast without giving rise to color and a colored display image with high contrast. 2. Description of the prior art: Liquid-crystal display devices are now used in clocks, electronic calculating machines, computer terminals, as well as word processor displays, televisions, and a variety of other uses in many fields. Recently, there has been an extremely large demand for liquid-crystal display devices because of the changes to multicolor and full-color displays, which are already being made use of in the fields of graphic display and image display. Color displays that have been widely put into practical use are attained by a liquid-crystal cell with color filter layers. The liquid-crystal cell functions as a light-switcher, and produces various colors. The main kind of display mode is a twisted nematic (TN) display mode attained by a liquid-crystal cell in which the liquid-crystal molecules are twisted 90°C so that high contrast, etc., can be obtained. However, with this TN display mode, the dependence of the display characteristics on the wavelength of light is great, and it is not possible to achieve switching of light uniformly over the entire spectrum of visible light. In particular, with the normally closed display process in which the axes of absorbance of the two polarizers are in parallel, there is the problem that light leakages at the time of the application of voltage gives rise to color. With a color display device that causes light-switching by the use of a TN display that has this kind of a color filter layer, there are two main kinds of driving methods. One of them involves the active-matrix drive method that uses a liquid-crystal cell that has picture elements provided with non-linear devices such as diodes or switching elements such as thin-film transistors. The other method involves the duty drive method in which the liquid crystals of a liquid-crystal cell without picture elements are successively driven. With the latter method, the steepness in the vicinity of the threshold value of the optical characteristics of the liquid crystals is important; this is a problem with the TN displays that are now being used. In order to improve the optical characteristics so that steepness in the vicinity of the threshold value can be attained, it has been suggested that a supertwisted nematic (STN) process that gives liquid-crystal molecules that are twisted at angles of around 180°-270°C be used. With the STN process, the curve in the vicinity of the threshold value increases sharply, and even when the duty ratio increases, it is possible to obtain a high contrast ratio. However, because birefringence effects of liquid crystals are used, the dependence of the display characteristics on the wavelength is theoretically higher than with the TN display, so it is very difficult to adapt it for use in a full-color display. Also, EP-A2-0246842 and EP-A2-0320283 disclose liquid crystal devices having upper and lower polarizers and first and second liquid crystal cells disposed between the polarizers, the twist direction of the first liquid crystal cell being opposite to that of the second liquid crystal cell. Also, a supertwisted nematic liquid crystal layer is known from EP-A-O 131 216 in which the polariser axes angles must be selected to optimise contrast ratio. SUMMARY OF THE INVENTION The double-layered type liquid-crystal display device of this invention, which overcomes the above-discussed and numerous other disadvantages and deficiencies of the prior art, comprises a multi-layered-type liquid crystal cell that is composed of first and second cell layers, said cell containing liquid-crystal molecules with a twisted nematic orientation therein, wherein the direction of twist in the first cell layer is opposite to the direction of twist in the second cell layer; the orientation of the liquid-crystal molecules in the first cell layer nearest the second cell layer is at an angle (α) of 70° to 150° to that of the liquid-crystal molecules in the second cell layer nearest the first cell layer; and the angle of twist in the first cell layer is different from the angle of twist in the second cell layer, wherein said first cell layer has a voltage applying means (2), the angle of twist in said first cell layer is set to be in the range of 180° to 360° and the angle in said second cell layer is set to be in the range of 30° to 390°, characterized in that an angle (β) of the orientation of the liquid-crystal molecules of the first cell layer on the light-incident side to the polarizer is in the range of β = β o ± 20° in which β o is the value of β for which the maximum contrast is attained and an angle (ψ) between the polarizer and the detector is in the range of ψ=ψ o ± 20° in which ψ o is the value of ψ for which the maximum contrast is attained, or an angle (β) of the orientation of the liquid-crystal molecules of the first cell layer on the light-incident side to the polarizer is in the range of β=(Θ₁-180°)/2+10°±20° and an angle (ψ) between the polarizer and the detector is in the range of ψ=α+Θ₁-Θ₂±20° where Θ₁ and Θ₂ are the angles of twist in the first and second cell layers and the dependence of the value of the birefringence Δn₁ of the liquid-crystal layer in the first cell layer on the wavelength of light is larger than that of the value of the birefringence Δn₂ of the liquid crystal layer in the second cell layer on the wavelength of light. In a preferred embodiment, the relationship between the pitch P of twist in the cell layer and the thickness d of the liquid-crystal layer in said cell layer is as follows: ϑ/360° - 1/4 < d/p ≾ ϑ/360°, In a preferred embodiment, the relationship between the product Δn₁.d₁ of Δn₁ and the thickness d₁ of the liquid-crystal layer in the first cell layer and the product Δn₂.d₂ of Δn₂ and the thickness d₂ of the liquid-crystal layer in the second cell layer is represented by the following inequality: 0.7 < Δn₁.d₁/Δn₂.d₂ < 1.4. In a more preferred embodiment, the absolute value of each of the products Δn₁.d₁ and Δn₂.d₂ is in the range of 0.3 to 3.0. Thus, the invention described herein makes possible the objectives of providing a liquid-crystal display device that produces a black-and-white display image with high contrast without giving rise to colour and a coloured display image with high contrast. BRIEF DESCRIPTION OF THE DRAWINGS This invention may be better understood and its numerous objects and advantages will become apparent to those skilled in the art by reference to the accompanying drawings as follows: Figure 1 is a sectional view showing the fundamental cell structure of a double-layered-type liquid-crystal display device of this invention. Figures 2a and 2b, respectively, are diagrams showing twists of liquid-crystal molecules in the right and left direction. Figure 3 is of a characteristic curve showing the relationship between the angle of the orientation of the liquid-crystal molecules in the first cell layer in the vicinity of the second cell layer to the orientation of the liquid-crystal molecules in the second cell layer in the vicinity of the first cell layer and the contrast ratio. Figure 4 is of a characteristic curve showing the relationship between the angles ϑ₁ and ϑ₂ of twist of the liquid-crystal molecules in the first and second cell layers, respectively, and the contrast ratio of display images. Figure 5 is of a characteristic curve showing the relationship between the value of Δn₁ · d₁/Δn₂ · d₂ and the contrast ratio. Figure 6a is of characteristic curves showing the relationship between the applied voltage and the light transmittance with regard to the display device (ϑ₁ ϑ₂) of Figure 1 of this invention. Figure 6b is of characteristic curves showing the relationship between the applied voltage and the light transmittance with regard to a double-layered type TN-LCD (ϑ₁ ϑ₂). Figure 7 is of characteristic curves showing the relationship between the applied voltage and the light transmittance with regard to another double-layered display device of this invention. Figure 8 is of characteristic curves showing the relationship between the applied voltage and the light transmittance with regard to another double-layered display device of this invention. Figure 9 is of characteristic curves showing the relationship among the retardation Δn₁·d₁, the angle β of the orientation of the liquid-crystal molecules on the light-incidence side in the first cell layer to the polarizer, and the angle ψ of the light-detector to the polarizer at the time when a positive-type display is attained. Figure 10 is of characteristic curves showing the relationship among the value of Δn₁·d₁, the value of β, and the value of ψ at the time when a negative-type display is attained. DESCRIPTION OF THE PREFERRED EMBODIMENTS This invention provides a liquid-crystal display device, the fundamental double-layered cell structure of which is, as shown in Figure 1, composed of a first cell layer C₁ and a second cell layer C₂ that contains liquid-crystal molecules therein with a twisted nematic orientation. Each cell layer is composed of transparent substrates 1 of glass, acrylic resins, or the like, transparent conductive films 2 of ITO (a film that is mainly made of indium oxide), nesa film, or the like positioned on the substrate 1, orientation films 3 of inorganic film made of SiO₂, SiO, or the like or an organic film made of polyimide, polyvinyl alcohol, nylon, acrylic resins, or the like for the orientation of liquid-crystal molecules positioned on the substrates 1 and the transparent conductive films 2, and a polarizer 5a positioned on the back face of the substrate 1. Both ends of each cell layer are sealed by sealing substances 6. A liquid-crystal layer 4 is disposed in each of the cell layers C₁ and C₂. The transparent conductive films 2 act as electrodes when voltage is applied to the liquid-crystal layer 4 of the first cell layer C₁. The direction in which the liquid-crystal molecules of the liquid-crystal layer 4 in one cell layer are helically twisted is opposite to the direction in which the liquid-crystal molecules of the liquid-crystal layer 4 in the other cell layer. The directions of twist of the liquid-crystal molecules are set as shown in Figures 2a and 2b in which Figure 2a shows the twist of the liquid-crystal molecules in the right direction with regard to the direction in which light from a light source is incident upon the cell and Figure 2b shows twist of the liquid-crystal molecules in the left direction with regard to the light incidence direction. When an optically active substance is added to a nematic liquid crystal, the liquid-crystal molecules form a twisted structure. To cause the liquid-crystal molecules to give rise to a twist in the right direction, the substance that is represented by the following chemical structure is used as an optically active substance: To cause the liquid-crystal molecules to give rise to a twist in the left direction, cholesteryl nonanoate (Merck), S-811 (Merck), etc., are used as optically active substances. Figure 3 shows the relationship between the angles α of the orientation of the liquid-crystal molecules of the first cell layer C₁, that is nearest the second cell layer C₂ to the orientation of the liquid-crystal molecules of the second cell layer C₂ that is the nearest the first cell layer C and the contrast ratio, wherein the angles ϑ, and ϑ₂ of twist of the liquid-crystal molecules of the liquid-crystal layers in the first and second cell layers C₁ and C₂ are set as follows: ϑ₁ = 270° and ϑ₂ = 240°, and the values Δn₁·d₁ and Δn₂·d₂ (Δn₁ and Δn₂ being the birefringence of the liquid crystals in the first and second cell layers, respectively, and d₁ and d₂ being the thicknesses of the liquid-crystal layers in the first and second cell layers, respectively) of the liquid-crystal layers in the first and second cell layers are set as follows: Δn₁·d₁ = Δn₂·d₂ = 1.0 . It can be seen from Figure 3 that the value of α should be set to be 70° to 150° in order to obtain a contrast ratio that is around 1/2 times or more the maximum contrast ratio. With the angles ϑ₁ and ϑ₂ of twist of the liquid-crystal layers in the first cell layer (on which voltage is applied) C₁ and the second cell layer (that acts as a compensation cell layer) C₂, as shown in Figure 4, the contrast ratio at the time when the value of ϑ₁ is not equal to that of ϑ₂ (i.e., ϑ₁ ϑ₂ wherein ϑ₂ ϑ₁ -30°) is higher than that at the time when the value of ϑ₁ is equal to that of ϑ₂ (i.e., ϑ₁ = ϑ₂). In addition, by considering the display contrast and the visibility, as shown in Figure 4, the angle ϑ₁ of twist of the liquid-crystal molecules is preferably set to be in the range of about 180° to about 360° based on the relationship between the angle of twist and the contrast ratio. If the angle ϑ₁ of twist of the liquid-crystal molecules exceeds 360°, a domain appears in which the liquid crystals have their orientation disarrayed at the time of the application of voltage, resulting in a dispersion of light, which readily gives rise to a decrease in contrast. The angle ϑ₂ of twist of the liquid-crystal molecules in the compensation cell layer C₂ is preferably set to be a value that is different from the angle ϑ₁ of twist of the liquid-crystal molecules in the voltage-applied cell layer C₁, said value of ϑ₂ being in the range of about 30° to about 390°. Moreover, to obtain sharp threshold characteristics of contrast, the specific pitch P of the twist of liquid-crystal molecules in one cell layer with a voltage-applying means becomes very important. The ratio of the thickness d of the liquid-crystal layer to the pitch P of the twist of the liquid-crystal molecules, d/p, is preferably set by the use of experimental data as follows: ϑ/360° - 1/4 < d/p ≾ ϑ/360°, wherein ϑ is the angle of twist of liquid-crystal molecules. This requirement applies in the case where the pretilt angle of the liquid crystals is about 10° or less. In the case where the pretilt angle exceeds 10°, the range of this value of d/p becomes different. The liquid-crystal cell layers of this invention are constructed so that the following relationship can be satisfied because the maximum contrast ratio exists therein: 0.7 < Δn₁·d₁ /Δn₂·d₂ < 1.4 Moreover, in light of brightness and contrast ratio, the absolute value of each of Δn₁·d₁ and Δn₂·d₂ is preferably set to be in the range of 0.3 to 3.0. To prevent the display images produced by this liquid-crystal device from giving rise to color, the dependence of the value of Δn₁ of the liquid-crystal of the first cell layer C₁ on the wavelength of light is preferably sat to be larger than the dependence of the value of Δn₂ of the liquid crystal of the second cell layer C₂ on the wavelength of light. Example 1 Figure 1 shows the double-layered cell structure of a liquid-crystal display device (i.e., a double-layered-type TN-LCD) of this invention, in which the transparent substrate 1 is made of glass. A transparent conductive film 2 with a thickness of about 1500 Å is disposed on each of the glass substrates 1 of the first cell layer C₁ alone by vapor deposition of ITO and patterned by an etching technique. On the glass substrates 1 and the transparent conductive films 2, liquid-crystal-molecule orientation films 3 of polyimide are formed with a thickness of about 500 Å by a spin coating technique, the surfaces of which are treated by being rubbed with cloth, causing the liquid-crystal molecules to be in a twisted nematic orientation. The end portions of the cell layers are sealed by a sealing substance 6. As a liquid-crystal substance of the first cell Layer C₁, a nematic liquid crystal, EX-02 (Rodick), is used. As a liquid-crystal substance of the second cell layer C₂, a nematic liquid crystal, ZLI-3021-000 (Merck), is used. To the liquid-crystal layer 4 of the first cell layer C₁, 0.60 wt% of cholesteryl nonanoate is added and 0.90 wt% of CB15 is added to the liquid-crystal layer 4 of the second cell layer C₂. The angle of twist of the liquid-crystal molecules in the first cell layer C₁ is opposite to that of the liquid-crystal molecules in the second cell layer C₂, wherein ϑ₁ = 270° and ϑ₂ = 240°. The thicknesses of the liquid-crystal layers in the first and second cell layers C₁ and C₂ (i.e., the thicknesses of the cell layers C₁ and C₂) are 8 µm and 10 µm, i.e., d₁ = 8 µm and d₂ = 10 µm. The value of P₁ is 13 µm and the value of P₂ is 20 µm. The pretilt angle of the liquid crystals on the substrates 1 is about 8°. The angles α of the orientation of the liquid-crystal molecules of the first cell layer C, that is the nearest the second cell layer C₂ to the orientation of the liquid-crystal molecules of the second cell layer C₂ that is the nearest the first cell layer C₁ is about 90° (i.e., α = about 90°). The polarizer 5a and the detector 5b, which are made of an iodine-system polarizing board, are placed at an angle of about 30° therebetween (i.e., |ψ| = about 30°). Figures 6a and 6b show the dependence of the light transmittance on the applied voltage with regard to the double-layered-type TN-LCD of this invention and a reference standard double-layered-type TN-LCD (in which ϑ₁ = ϑ₂ = 270°), respectively, wherein the wavelengths λ used herein for red color, green color, and blue color are 610 nm, 550 nm, and 450 nm, respectively, indicating that at the time of the application of a voltage near the threshold value, the transmittance of the wavelength for each color in the double-layered-type cell is lower than that of the wavelength for each color in the reference standard cell (wherein ϑ₁ = ϑ₂) . This means that the double-layered-type cell can attain high contrast. Moreover, the dependence of the applied-voltage-transmittance characteristics on the wavelengths with regard to the double-layered-type cell is much smaller than that of the applied-voltage-transmittance characteristics on the wavelengths with regard to the reference standard cell, and thus, the double-layered-type cell can produce a distinct black-and-white display image of a positive-display type. Example 2 This example provides another liquid-crystal display device of this invention, which has the same structure as that of Example 1, except that 0.50 wt% of cholesteryl nonanoate is added to the liquid-crystal layer 4 of the first cell layer C₁ and 0.30 wt% of CBl5 is added to the liquid-crystal layer 4 of the second cell layer C₂, and moreover the angles ϑ₁ and ϑ₂ of twist of the liquid-crystal molecules in the first and second cell layers C₁ and C₂ are set to the values of 240° and 150°, respectively (i.e., ϑ₁ = 240° and ϑ₂ = 150°). The polarizer 5a and the detector 5b are placed at an angle of about 90°. The other conditions are the same as those of Example 1. Figure 7 shows the dependence of the light transmittance on the applied voltage with regard to the double-layered type TN-CLD of this invention, wherein the wavelengths λ examined herein are 610 nm for red, 550 nm for green, and 450 nm for blue. Figure 7 indicates that the transmittance characteristics of the wavelengths for red, green, and blue in the double-layered-type cell are sufficiently high and agree with each other, so that a bright, distinct black-and-white display image of the positive-display type can be attained without giving rise to color. Moreover, the said double-layered-type cell has sharp threshold characteristics, so that the said cell can produce a display image with high contrast. Example 3 This example provides another liquid-crystal display device of this invention, which has the same structure as that of Example 1, except that 0.50 wt% of cholesteryl nonanoate is added to the liquid-crystal layer 4 of the first cell layer C₁ and 1.08 wt% of CBl5 is added to the liquid-crystal layer 4 of the second cell layer C₂, and moreover the angles ϑ₁ and ϑ₂ of twist of the liquid-crystal molecules in the first and second cell layers C₁ and C₂ are set to the values of 240° and 270°, respectively (i.e., ϑ₁ = 240° and ϑ₂ = 270°). The polarizer 5a and the detector 5b are placed at an angle of 30° (i.e., |ψ|=30°). The other conditions are the same as those of Example 1. Figure 8 shows the dependence of the light transmittance on the applied voltage with regard to the double-layered type TN-CLD of this invention, wherein the wavelengths λ examined herein are 610 nm for red, 550 nm for green, and 450 nm for blue. Figure 8 indicates that the transmittance characteristics of the wavelengths for red, green, and blue in the double-layered-type cell are sufficiently high and agree with each other, so that a bright, distinct black-and-white display image of the positive-display type can be attained. In the above-mentioned examples, the polarizer 5a and the detector 5b are used to obtain a display image of the positive-display type. In order to attain excellent display characteristics, the positional conditions of the polarizer and the detector must be changed depending upon the value of retardation Δn₁·d₁, the difference in angles of twist between the liquid-crystal molecules in the first and second cell layers, and the difference in angles of the orientation between the liquid-crystal molecules of the first cell layer that is the nearest the second cell layer and the liquid-crystal molecules of the second cell layer that is the nearest the first cell layer. For example, Figure 9 shows the changes of the positional conditions of the polarizer and the detector depending upon the value of retardation Δn₁·d₁, wherein β is an angle of the orientation of the liquid-crystal molecules of the first cell layer on the light-incidence side to the polarizer, and ψ is on angle between the polarizer and the detector. In Figure 9, β and ψ are the optimum values at which the maximum contrast can be attained. The range that is suitable for display is that β = β₀ ± 20° (β₀; the optimum value of β) and ψ = ψ₀ + 20°(ψ; the optimum value of ψ). The angles ϑ₁ and ϑ₂ of twist of the liquid-crystal molecules in the first and second cell layers are 240° and 270°, respectively (i.e., ϑ₁ = 240° and ϑ₂ = 270°), and the angles α of the orientation between the liquid-crystal molecules of the first call layer that is the nearest the second cell layer and the liquid-crystal molecules of the second cell layer that is the nearest the first cell layer is 90° (i.e., α = 90°). In this manner, when the values of β and ψ are changed depending upon the value of retardation, a black-and-white display image with high contrast of the positive-display type can be obtained. In order to attain a display image of the negative-display type, the positional conditions at the polarizer 5a and the detector 5b must be changed depending upon the difference in angles of twist between the liquid-crystal molecules in the first and second cell layers, or the like. Figure 10 shown the changes of the positional conditions of the polarizer and the detector depending upon the value of Δn₁·d₁ at the time when a negative display is carried out. The values of ϑ₁ and ϑ₂ are set to be 240° and 270°, respectively (i.e., ϑ₁ =240° and ϑ₂=270°), and the value of α is set to be 90° (i.e., α=90°). In case of the negative display, the changes of β and ψ depending upon the value of Δn₁·d₁, are small. Moreover, when ϑ₁ is set at 240° (i.e., ϑ₁=240°), the optimum values of β and ψ at which the maximum contrast can be attained are as follows: β ≃40° and ψ ≃ α + ϑ₁-ϑ₂ . The range that is suitable for display is that β =40° ± 20° and ψ = α + ϑ₁ - ϑ₂ ±20° . The optimum values of β and ψ at the time when the value of ϑ₁ is in the range of 180° to 360° are represented as follows: β ≃(ϑ₁ - 180°)/2 +10° and ψ ≃ α + ϑ₁ - ϑ₂ . It was found that the range suitable for display is that β =(ϑ₁ -180°)/2 + 10° ± 20° and ψ = α + ϑ₁ - ϑ₂ + 20° . As mentioned above, by determining the values or β and ψ, a black-and-white display image with high contrast of the negative-display type can be obtained. Example 4 Inside the liquid-crystal cell layer with the transparent conductive films 2 of each of the display devices in the above-mentioned examples, color (red, green and blue) filter layers of a gelatin film are disposed. The display devices with the color filter layers are subjected to a single-multiplex drive, with the formation of a distinct, clear color image. Example 5 The liquid-crystal cells of this invention are used in place of a liquid-crystal panel with color filters that is provided with a TFT (Thin Film Transistor) as an active device, and are examined for color display tests by an active matrix drive. They produce a distinct and clear color image, so they are useful for full-color display and multi-color display. It is not intended that the scope of the claims appended hereto be limited to the description as set forth herein.

Claims: A liquid-crystal display device comprising: a multi-layered-type liquid crystal cell that is composed of first and second cell layers (C₁, C₂), said cell containing liquid-crystal molecules with a twisted nematic orientation therein, wherein the direction of twist in the first cell layer (C₁) is opposite to the direction of twist in the second cell layer (C₂); the orientation of the liquid-crystal molecules in the first cell layer (C₁) nearest the second cell layer (C₂) is at an angle (α) of 70° to 150° to that of the liquid-crystal molecules in the second cell layer (C₂) nearest the first cell layer (C₁); and the angle of twist in the first cell layer (C₁) is different from the angle of twist in the second cell layer (C₂), wherein said first cell layer (C₁) has a voltage applying means (2), the angle of twist in said first cell layer (C₁) is set to be in the range of 180° to 360° and the angle in said second cell layer (C₂) is set to be in the range of 30° to 390°, characterized in that an angle (β) of the orientation of the liquid-crystal molecules of the first cell layer (C₁) on the light-incident side to the polarizer (5a) is in the range of β = β o ± 20° in which β o is the value of β for which the maximum contrast is attained and an angle (ψ) between the polarizer (5a) and the detector (5b) is in the range of ψ = ψ o ± 20° in which ψ o is the value of ψ for which the maximum contrast is attained, or an angle (β) of the orientation of the liquid-crystal molecules of the first cell layer (C₁) on the light-incident side to the polarizer (5a) is in the range of β=(Θ₁-180°)/2+10°±20° and an angle (ψ) between the polarizer (5a) and the detector (5b) is in the range of ψ=α+Θ₁-Θ₂±20° where Θ₁ and Θ₂ are the angles of twist in the first and second cell layers (C₁, C₂) and the dependence of the value of the birefringence Δn₁ of the liquid-crystal layer in the first cell layer (C₁) on the wavelength of light is larger than that of the value of the birefringence Δn₂ of the liquid crystal layer in the second cell layer (C₂) on the wavelength of light. A liquid-crystal display device according to claim 1, wherein the relationship between the pitch P of twist in the cell layer and the thickness d of the liquid-crystal layer (4) in said cell layer is as follows: Θ/360° -1/4 < d/p ≦ Θ/360°. A liquid-crystal display device according to claim 1 or claim 2, wherein the relationship between the product Δn₁·d₁ of Δn₁ and the thickness d₁ of the liquid-crystal layer in the first cell layer and the product Δn₂·d₂ of Δn₂ and the thickness d₂ of the liquid-crystal layer in the second cell layer is represented by the following inequality: 0.7 < Δn₁·d₁ / Δn₂·d₂ < 1.4. A liquid crystal display device according to claim 3, wherein the absolute value of each of the products Δn₁·d₁ and Δn₂·d₂ is in the range of 0.3 to 3.0.

Inventors: HATANO AKITSUGU, HATANO, AKITSUGU
Applicants: SHARP KK, SHARP KABUSHIKI KAISHA
Application year: 1989
Main classification: G02F1
IPC codes: G02F1