Patent Grant
7684005
The present invention relates to a liquid crystal display apparatus, and, more particularly, to an active matrix liquid crystal display apparatus.
Various examples of liquid crystal display apparatus are disclosed, for example, in Japanese Patent Publication No. 63-21907 (1988), UP, WO91/10936 and Japanese Patent Application Laid-Open No. 6-222397 (1994), in which a pair of comb electrodes are used to apply an electric field to a liquid crystal in a direction parallel to the surface of a substrate. However, in a display system of this type wherein the direction of an electric field applied to the liquid crystal is controlled to be parallel with the surface of a substrate by using active elements (hereinafter referred to as a horizontal electric field type), no consideration is given to the characteristic of the light source required to decrease the power consumption of the whole liquid crystal display apparatus. Further, no consideration is given to the configuration of the liquid crystal display apparatus required to suppress color shift in response to the application of a voltage thereto and to prevent a color defect s from occurring.
In the establishment of a horizontal electric field, opaque electrodes are provided in a display pixel portion in order to produce an electric field substantially in parallel with the surface of the substrate. As compared with the prior art type of display panel wherein an electric field is applied in a direction substantially vertical to the surface of the substrate by using a transparent electrode, the aperture ratio may be deteriorated and the brightness under a bright state may be reduced. Accordingly, it is necessary to use a high-intensity light source in the horizontal electric field producing type of display panel.
Because the display mode effective for a liquid crystal display apparatus of the horizontal electric field type is a double refraction mode, the transmittance T can be generally expressed by the following equation (1):
where, To designates a coefficient and is determined mainly by the transmittance of the polarizer used in the liquid crystal panel, θ designates the angle between an effective optical axis in the liquid crystal layer and a transmittance axis for polarized light, d designates the thickness of the liquid crystal layer, Δn designates the anisotropy of the refractive index of the liquid crystal layer, and λ denotes the wavelength of light. Because the transmittance of the liquid crystal display apparatus has essentially a maximum value at a certain wavelength, the liquid crystal display elements are colored. One solution to the above equation is a value which satisfies a condition wherein the peak wavelength becomes equal to the maximum wavelength 555 nm for luminous efficiency under a retardation of 0 order, that is, (πd·Δn/555)=π/2. In this case, the transmittance falls suddenly on the short wavelength side of the peak wavelength, and it decreases gradually on the long wavelength side. Therefore, the liquid crystal display elements are colored yellow. As a result, it is required to use a light source with the color of a cold color family which represents a complementary color to yellow. In other words, it is required to use a light source with a high color-temperature characteristic.
In general, a fluorescent lamp is used as a light source for a liquid crystal display apparatus. Because the luminous efficiency of the fluorescent lamp in a short wavelength region is less than that in a long wavelength region, the brightness may be reduced, and so a large consumption of power is required to obtain a high brightness. Since the normal voltage of the battery must be maintained for a long time, for example, in a note book type personal computer or personal digital assistance, it is required to avoid any increase in the power consumption.
Now, the display operation of a liquid crystal display apparatus of the horizontal electric field type can be obtained in the double refraction mode, and the transmittance T can be generally expressed by the following equation (2):
T=T0·sin22θ·sin2 [(π·deff·Δn)/λ] (2)
where, T0 designates a coefficient and is determined mainly by the transmittance of the polarizer used in the liquid crystal panel, θ designates the angle between an effective optical axis in the liquid crystal layer and a transmittance axis for polarized light, deff designates the thickness of the liquid crystal layer, Δ denotes the anisotropy of the refractive index of the liquid crystal layer, and λ designates the wavelength of light. Further, the product of deff and Δ is referred to as retardation. Here, the thickness deff of the liquid crystal layer is not the thickness of the whole liquid crystal layer, but the thickness of the liquid crystal layer in which the direction of alignment is changed when a voltage is applied.
In general, the molecules of the liquid crystal in the vicinity of the boundary surface of a liquid crystal layer do not change the alignment direction due to the effect of anchoring at the boundary surface even if a voltage is applied. Accordingly, when the thickness of the whole liquid crystal layer sandwiched between the substrates equals deff, deff<dLC always is maintained between the thickness dLC and deff. It is estimated that the difference between dLC and deff equals about 20 nm to 40nm.
As clearly seen from the above equation (2), the transmittance of the liquid crystal display panel takes a maximum value at a specific wavelength (peak wavelength). Therefore, the liquid crystal display element is easily colored, in other words, it is easy to be unnecessarily colored.
Generally, the liquid crystal panel is constructed so that the peak wavelength may become equal to the maximum wavelength 555 nm for luminous efficiency, that is, (πd·Δn/555)=π/2. At this time, the liquid crystal display element is colored yellow, because the spectral transmittance falls suddenly on the short wavelength side of the peak wavelength, and it decreases gradually on the long wavelength side.
The extent of coloring extremely changes with the application of a voltage to the liquid crystal. As the magnitude of the voltage value changes from the minimum voltage required for display to the medium tone display voltage and then to the maximum voltage, the color tone is gradually changed. Therefore, the display state of colors is extremely deteriorated.
Because the difference between the thickness of the liquid crystal layers appears as a change in the peak wavelength in the birefringence mode, the local and abnormal thickness of the liquid crystal display layer causes display defects, such as variations in the intensity and/or color tone, which are different from those in its surrounding area.
An object of the present invention is to provide an improved liquid crystal display apparatus, in which a low power consumption and a fine display characteristic are compatible with each other.
Another object of the present invention is to provide an improved liquid crystal display apparatus which can suppress color shift caused by the application of a voltage and reduce the occurrence of a color defect due to a local difference in thickness in the liquid crystal layer.
A liquid crystal display apparatus according to the present invention comprises a liquid crystal panel having a pair of substrates, a plurality of electrodes formed on at least one of said pair of electrodes and a liquid crystal layer sandwiched between said pair of substrates, and a light source provided on one surface of said liquid crystal panel. The light source has a luminous characteristic with the chromaticity of a warm color family and said liquid crystal panel has a characteristic of spectral transmittance with the chromaticity of a cold color family. Thereby, the color of said light source can be compensated.
The warm color family includes colors with a reddish hue, such as yellow or orange, in contradistinction with “white” illuminated from the standard illuminant C. The cold color family includes colors with a bluish hue in contradistinction with “white” illuminated from the standard illuminant C. While an illuminant with a color of the warm color family has a transmittance which is low at a shorter wavelength, for an illuminant with a color of the cold color family, the transmittance is low at a longer wavelength. Therefore, by combining them, it becomes possible to transmit light almost uniformly in the visible region. As a result, the display of the whole liquid crystal display apparatus approaches “white”, as illuminated from the standard illuminant C.
The reason why the power consumption is reduced by using the present invention is as follows. The fluorescent lamp with a color of the warm color family tends to consume less electric power than one with a color of the cold color family while obtaining the same intensity. In general, it is assumed that the power consumption of a fluorescent lamp with a color temperature of 6000K is 1, the power consumption required to obtain the same intensity results in a 5% increase in a fluorescent lamp with a color temperature of 8000K and a 10% increase in one with a temperature of 10000K, but a 5% decrease in one with a temperature of 4000K. For example, in order to compensate the color in a liquid crystal display element colored in yellow, by using a fluorescent lamp with a color temperature more than the 6770K of the white standard illuminant C, it is necessary to use an illuminant with a color temperature of preferably more than 10000K. For example, if an electric power of 2 watts is consumed by using a fluorescent lamp with a color temperature of 8700K in the liquid crystal display apparatus of the horizontal electric field type, an electric power of 2.06 watts is consumed when a fluorescent lamp with a color temperature of 10000K is used. However, if the fluorescent lamp with a color temperature of 6000K lower than that of the white standard illuminant C is used, the power consumption is 1.87 watts, and if one with 4000K is used, it becomes 1.79 watts.
The illuminant with a color of the warm color family may be made by changing the kind of fluorescent materials being used and their mixing ratio. A narrow band emission type fluorescent lamp can be made by mixing the materials selected from each of the following A, B and C groups. The A group has an emission peak in the range of 450 nm to 490 nm, and includes the following materials:
There are three methods to realize a liquid crystal display apparatus of the cold color family.
The threshold voltage Ec in the liquid crystal display apparatus is expressed by the following equation:
where, dLC designates the thickness of the liquid crystal layer, K2 represents an elastic constant, Δ∈ designates the anisotropy of a dielectric constant of the liquid crystal, and ∈ denotes a dielectric constant for a vacuum. As dLC is reduced, the threshold voltage shifts to a higher voltage. By setting the thickness of the liquid crystal to be thin at a pixel portion where red is displayed, it becomes possible to shift red, that is, a voltage-transmittance characteristic in a long wavelength region to a higher voltage side. Thereby, the transmittance at the long wavelength region for each voltage is suppressed, and thus it becomes possible to make a liquid crystal display. apparatus in which the transmittance in the short wavelength region is larger. In order to suppress sufficiently the transmittance in the high wavelength region and hold a color balance, it is preferable that the change in thickness of the liquid crystal is suppressed within the range of 0.1 μm to 1 μm. For example, it is possible to reduce dLC by thickening the film at a portion of the color filter where red is displayed. It may be possible to thicken the film at a portion of the color filter where blue is displayed more than dLC at portions lo where red and green are displayed. Also, in this case, it is preferable that the change in the thickness of the liquid crystal layer is within the range of 0.1 μm to 15 μm.
The illuminant used in accordance with the present invention has a maximum value of at least one intensity in each range from 400 nm to 500 nm, from 500 nm to 600 nm and from 600 nm to 700 nm of said light source, and the liquid crystal panel has a characteristic of spectral transmittance required to satisfy the relation, x>y>z, where x equals a value of the transmittance at the wavelength which shows the maximum value of the intensity in the range from 400 nm to 500 nm, y denotes a value of the transmittance at the wavelength which shows the maximum value of the intensity in the range from 500 nm to 600 nm, and z denotes a value of the transmittance at the wavelength which shows the maximum value of the intensity in the range from 600 nm to 700 nm. Thus, it is possible to suppress the color shift caused by the change in the applied voltage and to provide a liquid crystal display apparatus having a fine display characteristic.
The reason why a fine display characteristic can be obtained will be explained hereinafter.
As described above, the liquid crystal display apparatus is generally operated in a birefringent mode. Its transmittance is expressed in the equation (2). Accordingly, the liquid crystal display apparatus has a spectral transmittance which has its maximum value at a certain wavelength, suddenly decreases on the shorter wavelength side, and gradually decreases on the longer wavelength side. It is assumed that the peak wavelength is around 550 nm. The transmittance suddenly decreases in the range of 400 nm to 500 nm, which is in a blue region. As the brightness of the liquid crystal panel increases, the dependence of the transmittance on the wavelength becomes remarkable. Accordingly, this is the factor which causes the color shift according to a change in the applied voltage.
When the thickness of the liquid crystal layer at a certain portion is locally different from other portions in the liquid crystal display apparatus, the transmittance of blue at the portion remarkably changes and a color defect may occur. Accordingly, it should be noted that it is important to suppress any sudden decrease of the transmittance in the short wavelength region of the peak wavelength or the blue region. In order to suppress a sudden decrease of the transmittance in the short wavelength region, it is effective to shift the peak wavelength to the short wavelength side by setting the wavelength λ to be shorter than 550 nm under the condition of deff·Δn(λ)=λ/2.
The more the wavelength λ is spaced from the peak wavelength, the more the extent of the decrease of the transmittance increases. It is, therefore, possible to suppress a sudden decrease of the transmittance in the short wavelength region by setting the peak wavelength to the shorter wavelength side. It is also important to suppress a sudden decrease of the transmittance at the wavelength of emission from the illuminant being used.
In general, a narrow band emission type fluorescent lamp is used for the illuminant of the liquid crystal display apparatus. Such a fluorescent lamp uses materials which have a luminescence peak at each spectrum region of red (R), green (G) and blue (B).
The following group has an emission peak in the range of 450 nm to 490 nm corresponding to blue, and includes the following materials:
The luminescence characteristic of the narrow band emission type fluorescent lamp made with fluorescent materials selected from each of the above groups is as follows. The spectrum corresponding to blue is within the range of 450 nm to 490 nm, the spectrum corresponding to green is in the vicinity of 545 nm, and the spectrum corresponding to red is within the range of 610 nm to 630 nm.
Therefore, the characteristic of the spectrum transmittance which should be taken into consideration in the liquid crystal panel using the above narrow band emission type fluorescent lamp is as follows. It should have the range of 450 nm to 490 nm as a blue region, the range in the vicinity of 545 nm as a green region, and the range of 610 nm to 630 nm as a red region.
Accordingly, the most effective characteristic of the transmittance to suppress color shift and/or color defects in the liquid crystal panel has a maximum value in the wavelength region of 450 nm to 490 nm. The retardation deff·Δn(A) should be set to be less than 0.245 μm (λ=490 nm) to fit the peak of the transmittance to the above wavelength region. Further, it is necessary to use a liquid crystal material which has a small anisotropy Δn of refractive index and a thin liquid crystal layer to reduce the retardation deff·Δn.
As described above, it is important to fit the characteristic of the luminescence at the short wavelength region of the illuminant to the peak of the transmittance of the liquid crystal panel. Here, the spectral transmittance does not mean the spectral characteristic after passing through a color filter, etc., but refers to the characteristic of the transmittance of the liquid crystal panel itself.
While the peak wavelength of the transmittance may change a little by using a certain color filter, it is possible to ignore its effect during actual use. The most important point in accordance with the present invention resides in the relationship between the peak of the intensity of the illuminant and the transmittance of the liquid crystal panel.
The magnitude of the anisotropy Δn of the refractive index of the liquid crystal changes according to temperature. If the temperature of the liquid crystal panel changes due to the environment of the place where the display apparatus is used, the set value of the retardation deff·Δn may change.
In a liquid crystal in which the anisotropy Δn of the refractive index is relatively small, the change in the anisotropy Δn itself of its refractive index becomes small. In addition, if the thickness deff is also small, the change in the product deff·Δn of the thickness and the anisotropy becomes smaller. Accordingly, by using the above liquid crystal, it is possible to obtain an expansion of the margin of the temperature, and thus suppress any change in the retardation deff·Δn.
a) and 4(b) are side-sectional views each showing one pixel portion of the liquid crystal display panel of the horizontal electric field type.
c) and 4(d) are front views of the panels of
a) and 7(b) each show an shows the emission characteristic of an illuminant.
a) and 8(b) each show an the emission characteristic of an illuminant.
a) shows the spectral transmittance of the liquid crystal display panel when a drive voltage is applied.
b) shows a luminescence spectrum obtained by using a light source.
Embodiments of the liquid crystal display apparatus according to the present invention will be explained hereinafter with reference to the attached drawings.
Firstly, the configuration and the principle of operation of a liquid crystal display element of the horizontal electric field type will be explained with reference to
In
Because there are a pair of polarizers and a pair of boundary surfaces, respectively, an upper one and a lower one, the relevant angles are expressed as ΦP1, ΦP2, ΦLC1, and ΦLC2, respectively, if necessary. Further, the longitudinal axis 10 of the molecule of liquid crystal is oriented in the same direction as that of rubbing due to an alignment control film.
Secondly, the configuration and the principle of operation of a liquid crystal display panel of the horizontal electric field type will be explained with reference to
a) and 4(b) are side-sectional views each showing one pixel portion of the liquid crystal display panel of the horizontal electric field type, and
The molecules of liquid crystal are alignment-controlled according to a rubbing direction 10 of the alignment control film 5 when a voltage is not applied.
The angle ΦLC is controlled so as to satisfy the relation, 45°<|ΦLC|□90° in consideration of the dielectric positive anisotropy. In this example, the directions of alignment of the molecules of the liquid crystal on the upper and lower boundary surfaces are parallel to each other, namely, ΦLC1=ΦLC2.
When a voltage with a predetermined polarity is applied, and thus an electric field 9 is produced, the molecules of liquid crystal change their directions to align with the direction of the electric field 9, as shown in
This operation may be normally performed even if the composition of the liquid crystal has a negative dielectric anisotropy. In this case, it should be noted that the state of original alignment must be set to 0°<|ΦLC|□45°.
Referring now to
a) shows the spectral transmittance of this liquid crystal display panel when a drive voltage is applied, and
A nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +9.0, and the anisotropy of the refractive index is 0.082 (589 nm, 20° C.). The gap d between cells equals 3.8 μm. As a result, dLC·Δn equals 0.31 μm, and deff·Δn equals 0.28 μm.
The liquid crystal display apparatus may also be provided with an edge light type back-light unit using a cold cathode fluorescent lamp as a light source having a color temperature of 11000K and the luminescence spectrum shown in
When the light source is changed to an edge light type back-light unit with a color temperature of 5885K, a power of 1.8 Watts is consumed in the light source unit.
A color filter 24 is provided on the substrate opposite to the substrate having transistor elements, as shown in
In one example, a nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +7.3, and the anisotropy of the refractive index is 0.074 (589 nm, 20° C.). The gap d between cells equals 3.2 μm in such a state that spherical polymer beads are scattered and sandwiched between the substrates and the liquid crystal is sealed in. As a result, d·Δn equals 0.24 μm.
In another example, a nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +9.0, and the anisotropy of the refractive index is 0.082 (589nm, 20° C.). The gap d between cells equals 3.7 μm in such a state that spherical polymer beads are scattered and sandwiched between the substrates and the liquid crystal is sealed in. As a result, dLC·Δn equals 0.30 μm, and deff·Δn equals about 0.27 μm. A phase plate is attached between the upper substrate and the polarizer, so that the angle ΦF1 of the optical axis may become parallel with the upper substrate, in other words, QF1=ΦP1=75°. The phase plate is made of poly carbonate and has a retardation of 595 nm (550 nm). The liquid crystal display panel is provided with an edge light type back-light unit using a cold cathode fluorescent lamp as a light source. The light source s has a color temperature of 4348K and the luminescence spectrum shown in
A striped color filter 24 with three colors, R, G, B, is provided on the substrate 7 opposite to the substrate having transistor elements, as shown in
The thickness of the film of the color filter was about 2 μm at the B and G pixels, and about 2.5 μm at the R pixels. The difference between these thicknesses remains as a level difference of about 0.3 μm after spin-coating the flat film. The level difference represents the difference of thickness between the liquid crystal layers. The edge light type back light unit, which was used for the liquid crystal display panel, included a cold cathode fluorescent lamp with a color temperature of 4703K.
In another example, the thickness of the film of the color filter was about 2 μm at the G and R pixels and about 1.5 μm at the B pixels. The thickness of the liquid crystal layer was about 3.8 μm at the G and R pixels, and about 4.1 μm at the B pixels. An edge light type back light unit, which was used for the liquid crystal display panel, included a cold cathode fluorescent lamp with a color temperature of 4703K.
In a further example, the thickness of the film of the color filter was about 2 μm at the G pixels, about 1.5 μm at the B pixels and about 2.5 μm at the R pixels. The thickness of the liquid crystal layer was about 4.2 μm at the G pixels, about 3.9 μm at the R pixels, and about 3.9 μm at the B pixels. An edge light type back light unit, which was used for the liquid crystal display panel, included a cold cathode fluorescent lamp with a color temperature of 4348K.
In a still further example, the thickness of the film of the color filter was about 2 μm at the G and R pixels, and about 1.5 μm at the B pixels. The thickness of the liquid crystal layer was about 4.5 μm at the G and R pixels, and about 4.2 μm at the B pixels. A phase difference film made of poly-carbonate, which has a retardation of 997 nm (550 nm), was inserted between the upper substrate and the polarizer, and it was attached so that the angle ΦF1 of its delay-phase axis was parallel with the upper polarizer, that is, ΦF1=ΦP1=75°. An edge light type back light unit, which was used for the liquid crystal display panel, included a cold cathode fluorescent lamp with a color temperature of 4348K.
In these figures, reference numeral 14 designates a thin film transistor, which has pixel electrodes (source electrodes) 4, signal electrodes (drain electrodes) 3, a scanning electrode (gate electrode) 12, and amorphous silicon 13. A common electrode 1 and the scanning electrode 12 are formed by patterning the same metal layer formed on the glass substrate. The signal electrodes 3 and the pixel electrodes 4 are formed by patterning the same metal layer formed on a gate insulating layer 2. A load capacitance 16 is formed by allowing the insulating layer 2 to sandwich between the pixel electrodes 4 and the common electrode 1.
In
The width of each electrode is determined as follows. In the electrodes used as a wiring electrode bridging a plurality of pixels, that is, the scanning electrode 12, the signal electrode 3 and the wiring portion (parallel with the scanning electrode, and in a horizontal direction in
The width of the pixel electrode 4 formed independently for each pixel and the longitudinally extending portion of the common electrode 1 are respectively set to be 9 μm. The common electrode 1 and the signal electrode 3 are partially superposed on each other (by 1 μm) through the insulating layer. Thereby, it becomes unnecessary to provide a black matrix in a direction parallel with the signal electrode 3. Accordingly, there is provided only a black matrix 22 which can shield the light in the direction of the scanning electrode. In addition, a color filter 24 is provided only on the surface of one substrate.
While the black matrix 22 is provided on the substrate in which the electrodes are formed, it may be possible to provide the black matrix on the opposing substrate. These electrodes can be formed in a conventional way.
In the example of
Further, a surface-flattening insulating layer 27 is provided between the alignment control film 5 and gate insulating layer 2. The material for the surface-flattening insulating layer 27 is SiO2 or SiN, the same as the gate insulating layer 2. However, it may be possible to use other suitable materials.
The width of each electrode is determined as follows.
In the electrodes used as a wiring electrode bridging between a plurality of pixels, that is, the scanning electrode 12, the signal electrode 3 and the wiring portion (parallel with the scanning electrode, and in a horizontal direction in
The width of the pixel electrode 4 formed independently for each pixel and the longitudinally extending portion of the common electrode 1 are set to be 5 μm and 6 μm, respectively.
Because the width of the electrode is narrow in this example, the possibility of breaks is increased due to the mixing of foreign particles. In
A scanning signal voltage, an image signal voltage and a timing signal are supplied from a power circuit (not shown) and a controller 19, and then the display operation responsive to the active matrix drive is started.
Embodiments of the present invention will be explained hereinafter.
In
A nemuatic liquid crystal composition is inserted between the substrates 7, of which the anisotropy of the dielectric constant is positive, +12.0, and the anisotropy of the refractive index is 0. 079 (589 nm, 20° C.). The gap d between cells equals 3.02 μm due to the fact that spherical polymer beads are scattered and sandwiched between the substrates and the liquid crystal is sealed in. As a result, the thickness of the whole liquid crystal layer dLC becomes equal to the gap d (3.02 μm). The value of dLC·Δn (589 nm) equals 0.239 μm, and from the wavelength dependence characteristic of the anisotropy of the refractive index, dLC·Δn (490 nm) equals 0.244 μm. As a result, deff·Δn (490 nm) equals about 0.22 μm.
The pair of substrates 7 are sandwiched by two polarizers 8. The polarization axis of one substrate is set to satisfy ΦP1=75°, and the polarization axis of the other substrate is set to satisfy ΦP2=−15°. Thereby, the liquid crystal display panel 23 shown in
As shown in
It may be possible to from the back-light unit by using a plurality of fluorescent lamps, and preferably, to provide a prism sheet between the polarizer 33 and the lower substrate 8.
In order to obtain a display closest to the achromatic color from the characteristics of the color of the liquid crystal display panel 23 itself, except for the color filter, the color temperature of the illuminant is determined. Its color temperature is 5885K.
The spectrum characteristic of the back-light is shown in
As seen from
A nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +9.0, and the anisotropy of the refractive index is 0.082 (589 nm, 20° C.). The gap d, between cells equals 3.83 μm.
In this comparison example, dLC·Δn (589 nm) equals 0.310 μm, and dLC·Δn (490 nm) equals 0.321 μm. As a result, deff·Δn (490 nm) equals about 0.30 μm. This value is out of the present invention.
This liquid crystal display panel is provided with an edge light type back-light unit using a cold cathode fluorescent lamp as a light source. The light source has a color temperature 6818K. The characteristic of the spectral transmittance in a light state of the liquid crystal display apparatus without the color filter is as shown in
As seen from the comparison example 1, the color is shifted as the dark state is shifted into the light state in the liquid crystal display apparatus using the liquid crystal display panel in which the transmittance at the short wavelength is reduced. According to this comparison example, it is difficult to suppress the color shift in the color display and the coloring in the black and white display, and thus the quality of the displayed image essentially deteriorates.
In the comparison example 2, a nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +9.0, and the anisotropy of the refractive index is 0.082 (589 nm, 20° C.). The gap d between cells equals 4.26 μm.
In this comparison example, dLC·Δn (589 nm) equals 0.345 μm, and dLC·Δn (490 nm) equals 0.357 μm. As a result, deff·Δn (490 nm) becomes equal to about 0.33 μm. This value is also outside of the present invention. It is understood that the transmittance for blue light is reduced.
This liquid crystal display panel is provided with an edge light type back-light unit using a cold cathode fluorescent lamp as a light source. The light source has a color temperature 6818K. A trail appears on the chromaticity coordinates until a voltage of the liquid crystal display apparatus is switched from OFF (a dark state) to ON (a light state) as shown in
The change in the characteristics caused by the local change in the thickness of the liquid crystal will be explained with reference to various embodiments and comparison examples.
The liquid crystal display apparatus has two substrates, one of which has a color filter with B, G and R pixels on its surface. A nemnatic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +12.0, and the anistropy of the refractive index is 0.079 (589 nm, 20° C.). The gap d between cells is formed by scattering spherical polymer beads and sandwiching them between the substrates. The gap is adjusted to d=2.87 μm by selecting the radius of the beads.
In this comparison example, dLC·Δn (589 nm) equals 0.227 μm and dLC·Δn (490 nm) equals 0.232 μm. As a result, deff·Δn (490 nm) equals about 0.21 μm. This value is out of the present invention.
The liquid crystal display panel is provided with a back-light unit as a light source which has a color temperature of 6818K.
The liquid crystal display apparatus has two substrates, one of which has a color filter with B, G and R pixels on its surface. A nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +12.0, and the anisotropy of the refractive index is 0.079 (589 nm, 20° C.). The gap d between cells is formed by scattering spherical polymer beads and sandwiching them between the substrates. The gap is adjusted to d=3.17 μm by selecting a radius of the beads which is different from that in embodiment A.
In this embodiment B, dLC·Δn (589 nm) equals 0.250 μm and dLC·Δn (490 nm) equals 0.256 μm. As a result, deffΔn (490 nm) equals about 0.23 μm.
The liquid crystal display panel is provided with a back-light unit as a light source which has a color temperature of 4703K.
The liquid crystal display apparatus has two substrates, one of which has a color filter with B, G and R pixels on its surface. A nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +9.0, and the anisotropy of the refractive index is 0.082 (589 nm, 20° C.). The gap d, between cells is adjusted to d=3.83 μm.
In this comparison example, dLC·Δn (589 nm) equals 0.314 μm, and dLC·Δn (490 nm) equals 0.321 μm. As a result, deff·Δn (490 nm) equals about 0.30 μm. This value is out of the present invention.
The liquid crystal display panel is provided with a back-light unit as a light source which has a color temperature of 6818K.
The liquid crystal display apparatus has two substrates, one of which has a color filter with B, G and R pixels on its surface. A nematic liquid crystal composition is inserted between the substrates, of which the anisotropy of the dielectric constant is positive, +9.0, and the anisotropy of the refractive index is 0.082 (589 nm, 20° C.). The gap d between cells is adjusted to d=4.26 μm.
In this comparison example, dLC·Δn (589 nm) equals 0.349 μm, and dLC·Δn (490 nm) equals 0.357 μm. As a result, deff·Δn (490 nm) equals about 0.33 μm. This value is also out of the present invention.
The liquid crystal display panel in the comparison example D is provided with a back-light unit as a light source which has a color temperature of 6818K.
As should be clearly understand from the above description, there is a difference of 10% in the gap between the embodiments A and B, and between the comparison examples C and D. Accordingly, it is possible to estimate the color shift caused by the change in the thickness deff (□d) of the liquid crystal layer, that is, the gap margin.
In general, the value of the color difference ΔEuv* allowable in the same liquid crystal display panel is around 3 in such a liquid crystal display apparatus.
Referring now to
While, as clearly understood from the characteristic shown by the dotted line of
In the embodiments of the present invention, it is understood that even if there is a difference of 10% in the gap between the embodiments A and B in the same display panel, a color defect is not evident in this case, and it is possible to obtain a sufficient margin for the change in the gap.
The reason for the occurrence of a color difference in the embodiments of the present invention and the comparison examples will be explained from the view point of the difference in the passing characteristic for the colors, R, G and B.
The following fact is clarified from these figures.
In the embodiments of the present invention shown in
In
It is important to maintain the relationship of the transmittance between the three wavelengths of the colors R, G and B to a predetermined state.
The predetermined state refers to a state wherein transmittance in the wavelength of the longest wave among the spectra corresponding to blue of the emission spectra of the back-light is always larger than that in the wavelengths 545 nm (green) and 630 nm (red).
Accordingly, the present invention must satisfy the condition that the above relationship is always maintained.
| Number | Date | Country | Kind |
|---|---|---|---|
| 7-273921 | Oct 1995 | JP | national |
| 8-114739 | May 1996 | JP | national |
This is a continuation of U.S. application Ser. No. 11/299,699, filed Dec. 13, 2005, now U.S. Pat. No. 7,433,012, which is a continuation of U.S. application Ser. No. 10/629,711, filed Jul. 30, 2003, now U.S. Pat. No. 7,209,211, which is a continuation of U.S. application Ser. No. 09/572,375, filed May 18, 2000, now U.S. Pat. No. 6,621,538, which is a continuation of U.S. application Ser. No. 08/740,008, filed Oct. 23, 1996, now U.S. Pat. No. 6,137,560, the subject matter of which is incorporated by reference herein.
| Number | Name | Date | Kind |
|---|---|---|---|
| 4345249 | Togashi | Aug 1982 | A |
| 4550436 | Freeman | Oct 1985 | A |
| 4632514 | Ogawa et al. | Dec 1986 | A |
| 4697884 | Amstutz | Oct 1987 | A |
| 4909604 | Kobayashi | Mar 1990 | A |
| 4973137 | Kozaki | Nov 1990 | A |
| 5048933 | Asano | Sep 1991 | A |
| 5089906 | Ohnishi | Feb 1992 | A |
| 5119216 | Wada | Jun 1992 | A |
| 5124825 | Asano | Jun 1992 | A |
| RE33987 | Suzawa | Jul 1992 | E |
| 5130834 | Kano | Jul 1992 | A |
| 5132825 | Miyadera | Jul 1992 | A |
| 5139340 | Okumura | Aug 1992 | A |
| 5211463 | Kalmanash | May 1993 | A |
| 5414542 | Kawagishi | May 1995 | A |
| 5532854 | Fergason | Jul 1996 | A |
| 5541750 | Seong | Jul 1996 | A |
| 5745200 | Kikuchi | Apr 1998 | A |
| 5757524 | Rupp | May 1998 | A |
| 5841498 | Baur et al. | Nov 1998 | A |
| 7209211 | Utsumi et al. | Apr 2007 | B2 |
| Number | Date | Country |
|---|---|---|
| 63-21907 | May 1988 | JP |
| 02-013926 | Jan 1990 | JP |
| 3-233518 | Oct 1991 | JP |
| 03-233518 | Oct 1991 | JP |
| 04-057011 | Feb 1992 | JP |
| 04-181219 | Jun 1992 | JP |
| 4-181219 | Jun 1992 | JP |
| 6-222397 | Aug 1994 | JP |
| 08-082715 | Mar 1996 | JP |
| 08-094848 | Apr 1996 | JP |
| 08-095015 | Apr 1996 | JP |
| 08-106010 | Apr 1996 | JP |
| 08-068997 | Jun 1996 | JP |
| 9110936 | Jul 1991 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20090040438 A1 | Feb 2009 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | 11299699 | Dec 2005 | US |
| Child | 12244181 | US | |
| Parent | 10629711 | Jul 2003 | US |
| Child | 11299699 | US | |
| Parent | 09572375 | May 2000 | US |
| Child | 10629711 | US | |
| Parent | 08740008 | Oct 1996 | US |
| Child | 09572375 | US |
