JP2006163070A - Retardation plate, liquid crystal panel, and projection-type display device - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a retardation plate which can perform proper optical compensation at the temperature in a use condition, and to provide a liquid crystal panel and a projection-type display device which can improve contrast in the utilization condition. <P>SOLUTION: The intersection angle of optical axes of a first retardation plate and a second retardation plate is formed so as to be different in a plane, at room temperature. When the intersection angle A3 of the optical axes at the central part is set at 90°, the intersection angles B3 and D3 of the optical axes on one diagonal line are set at <90°, and the intersection angles C3 and E3 of the optical axes on the other diagonal line are set at >90°. The intersection angle of the optical axes at the central part at the room temperature is varied from the intersection angles of the optical axes at the four corners on the diagonal lines. When the projection-type projector is operated, namely when the temperature of the retardation plate rises, the intersection angles of the optical axes is substantially is made to coincide in the plane. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

  The present invention relates to a retardation plate and a liquid crystal panel used for, for example, a projection display device, and a projection display device provided with the liquid crystal panel.

  A liquid crystal projector device is known in which light output from a light source is modulated by, for example, a transmissive liquid crystal panel to form image light, and the image light is projected onto a screen or the like.

  On the other hand, in a direct-view type liquid crystal panel used for a notebook personal computer or the like, it is assumed that a plurality of users view the same screen from a position having a certain angle. The structure is taken into consideration.

  As an example, the viewing angle characteristics are improved by correcting the optical characteristics of the direct-view liquid crystal panel using a discotic liquid crystal, a rod-shaped liquid crystal, or other retardation film having three-dimensional birefringence.

  By the way, in a liquid crystal projector device that uses a liquid crystal panel as a light valve that modulates light emitted in the optical axis direction of the reflector of the lamp and projects it onto a screen with a projection type optical system, There was no need to improve the viewing angle of the panel.

  However, in the above liquid crystal projector apparatus, the linearly polarized light emitted from the incident side polarizing plate becomes elliptically polarized light by the liquid crystal panel that modulates the video signal due to the reasons described below, and leakage occurs in the outgoing side polarizing plate, thereby reducing the black level. The contrast decreases.

  In general, the liquid crystal molecules of the liquid crystal panel have a pretilt angle of 2 ° to 8 °, for example. This is the angle of the initial molecular alignment given with respect to the alignment treatment direction applied to the surface of the liquid crystal panel substrate in order to guide the direction in which the liquid crystal molecules tilt when a driving voltage is applied.

  Due to the effect of the pretilt angle, the incident light is disturbed in polarization with an angle to the liquid crystal panel surface. This relates to the anisotropy of the refractive index of liquid crystal molecules. That is, due to the anisotropy of the refractive index of the liquid crystal, the phase of the major axis component of the liquid crystal molecule is delayed, so that the linearly polarized incident light is between the slow axis component and the fast axis component of the liquid crystal molecule. A phase difference (optical distortion) is generated in the light, resulting in elliptically polarized light.

  In addition, with respect to light inclined with respect to a certain azimuth angle with respect to the display surface of the liquid crystal panel, the transmittance decreases as the applied voltage value increases, and the transmittance increases again with a specific voltage value as a boundary. Then, gradually decline. Further, for light inclined with respect to a certain azimuth angle, the transmittance does not decrease even when the applied voltage is increased, and black may remain floating.

  As described above, linearly polarized light incident from various directions changes depending on liquid crystal molecules, and the elliptically polarized light changes according to the incident direction. That is, the polarization state of the light after passing through the liquid crystal panel is a sum of polarization changes caused by a number of liquid crystal molecules in different directions.

  As a result, light vertically incident on the liquid crystal panel is kept linearly polarized light, but light incident obliquely to a certain degree is disturbed to become elliptically polarized light corresponding to the incident light. For this reason, leakage due to elliptically polarized light occurs in the polarizing plate on the output side of the liquid crystal panel, so that the transmittance of black display increases and the contrast characteristics of the liquid crystal panel deteriorate.

Actually, the angle component of the irradiation light with respect to the liquid crystal panel of the liquid crystal projector device is mainly light of 5 ° to 15 °. In other words, the irradiation light contains almost no light that enters perpendicularly, and most of the incident light is incident at an angle, so that the polarization state changes under the influence of the pretilt angle of the liquid crystal molecules. As means for solving this problem, a phase difference plate is disclosed that cancels out the phase difference between the slow phase and the fast phase due to the pretilt of liquid crystal molecules, that is, compensates for optical distortion of the liquid crystal layer. (See Patent Document 1).
JP 2001-42314 A

  Since the retardation plate disclosed in Patent Document 1 is manufactured by using a stretching method, the in-plane optical axes all face the same direction. In a direct-view liquid crystal display, the operating temperature is almost room temperature. However, in the case of a projection type liquid crystal projector, the operating temperature becomes a high temperature such as 60 ° C., for example.

  Therefore, the optical axis of the retardation layer is shifted. In particular, the unevenness of contrast occurs due to the deviation of the optical axis at the in-plane end of the retardation layer. That is, the black characteristic of the image projected on the screen changes as it operates. In particular, a change in black characteristics appears remarkably at the four corners of the screen, causing a problem in image characteristics.

  A first object of the present invention is to provide a retardation plate capable of performing appropriate optical compensation at a temperature in use.

  A second object of the present invention is to provide a liquid crystal panel and a projection display device that can improve contrast by including a phase difference plate capable of performing appropriate optical compensation at a temperature in use. is there.

  In order to achieve the above object, the retardation plate of the present invention has a substrate and a retardation layer formed on the substrate, and the retardation layer has different in-plane optical axes in different directions at room temperature. It is defined so that the in-plane optical axes are aligned when raised to a predetermined temperature.

  In the retardation plate of the present invention, the retardation layer is formed in a direction in which the optical axis in the plane is different at room temperature. Here, when the retardation plate is irradiated with light, the temperature of the retardation plate rises in the use state, and the optical axis of the retardation layer is determined by the difference in the linear expansion coefficient between the retardation layer material and the substrate material The direction of changes. In the present invention, it is defined that the optical axes of the retardation layers are aligned in the plane at the temperature in use.

  In order to achieve the above object, a retardation plate of the present invention includes a substrate, a first retardation layer and a second retardation layer formed on the substrate, and the first and second retardation layers. The phase difference layer is defined such that the crossing angles of the optical axes in the plane are different at room temperature, and the crossing angles in the plane substantially coincide with each other when the temperature rises to a predetermined temperature. is there.

  In the retardation plate of the present invention described above, the first and second retardation layers are formed so that the crossing angles of the optical axes in the plane are different at room temperature. Here, when the phase difference plate is irradiated with light, the temperature of the phase difference plate rises in the use state, and the first and second differences are caused by the difference in the linear expansion coefficient between the material of the phase difference layer and the material of the substrate. The direction of the optical axis of the retardation layer changes. In the present invention, the crossing angles of the optical axes of the first and second retardation layers are defined so as to substantially coincide with each other at the temperature in use.

In order to achieve the above object, a liquid crystal panel according to the present invention includes a liquid crystal layer, two substrates arranged outside the liquid crystal layer, a first retardation layer and a second retardation layer formed on the substrate. The first and second retardation layers are formed in different angles at the normal temperature in the plane, and when the temperature rises to a predetermined temperature, the first and second retardation layers are formed in the plane. The crossing angles are defined so as to substantially match.

In the above-described liquid crystal panel of the present invention, the first and second retardation layers are formed so that the crossing angles of the optical axes in the plane are different from each other at room temperature, and the in-plane when the temperature rises to a predetermined temperature. It is defined that the crossing angles substantially coincide.
For this reason, in use, uneven retardation in the plane of the first and second retardation layers is suppressed, and uniform optical compensation is performed in the plane of the liquid crystal layer.

  In order to achieve the above object, a projection display device of the present invention includes a light source, a liquid crystal panel that modulates light from the light source, and a projection unit that projects light modulated by the liquid crystal panel. The liquid crystal panel includes two substrates disposed outside the liquid crystal layer, and a first retardation layer and a second retardation layer formed on the substrate, and the first and second retardation layers are provided. The phase difference layer is defined such that the crossing angles of the optical axes in the plane are different at room temperature, and the crossing angles in the plane substantially coincide with each other when the temperature rises to a predetermined temperature. is there.

In the projection display device of the present invention, the first and second retardation layers are formed so that the crossing angles of the optical axes in the plane are different at room temperature, and the predetermined temperature, that is, the temperature at the time of projection. Is defined so that the in-plane crossing angles substantially coincide with each other.
For this reason, at the time of projection, the retardation unevenness in the planes of the first and second retardation layers is suppressed, and uniform optical compensation is performed in the plane of the liquid crystal layer.

According to the retardation plate of the present invention, appropriate optical compensation can be performed at the temperature in use.
According to the liquid crystal panel and the projection display device of the present invention, the contrast can be improved by providing the retardation plate capable of performing appropriate optical compensation at the temperature in use.

  Embodiments of the present invention will be described below with reference to the drawings. The following content will be described mainly by taking a liquid crystal projector using a TN (Twisted Nematic) -LCD mode as an example. However, the present invention is not limited to the TN-LCD mode, and can also be used in a VA (Vertical Alignment) -LCD mode and a STN (Super Twisted Nematic) -LCD mode.

<Optical axis of retardation plate>
First, problems of the conventional high contrast projection type liquid crystal projector will be described.

  As shown in FIGS. 1A and 1B, a black display projected by a high-contrast liquid crystal projector provided with a conventional retardation plate may have bright and dark portions on the diagonal line. is there. One reason for this poor quality is thought to be the retardation plate.

  The retardation plate is often formed of two or more retardation layers. Normally, chromatic dispersion (reverse dispersion) that increases retardation (retardation value; characteristic of retardation plate expressed by product of birefringence and thickness) toward the longer wavelength side is required for the retardation plate. Since the wavelength dispersion of the polymer material constituting the retardation layer tends to decrease toward the longer wavelength side with only one layer, reverse dispersion is achieved by using two retardation layers (or retardation plates). To get. For example, in the TN-LCD mode, the optical axes of the two retardation layers often have an intersection angle of about 90 ° at room temperature (room temperature) when stacked.

  As shown in FIG. 2, at the room temperature (room temperature: 25 ° C.), the crossing angle of the optical axes of each phase difference plate is substantially the same at the center (A1) and the four corners (B1, C1, D1, E1). ing. However, when a phase difference plate is installed on the projector and projected, the temperature of the phase difference plate rises to about 40 ° C. to 60 ° C. due to the influence of the projection light. As the temperature rises, the optical axis of the phase difference plate is shifted as shown in FIG. 3 (a) or FIG. 3 (b). That is, the angles at the four corners are smaller or larger than the angles at room temperature.

  For example, as shown in FIG. 3A, when the optical axis crossing angle A2 at the central portion is 90 °, the optical axis crossing angles B2 and D2 are smaller than 90 °. The angles of C2 and E2 increase. As shown in FIG. 3B, when the optical axis angle A2 ′ at the center is 90 °, the optical axis angles B2 ′ and D2 ′ are larger than 90 °. The angles C2 ′ and E2 ′ become smaller.

  The phenomenon described above is considered to occur because the linear expansion coefficient of the substance forming the retardation layer and the substrate supporting the retardation layer are different. That is, the optical axis of the retardation layer is shifted due to the difference in linear expansion coefficient between the material constituting the retardation layer and the substrate.

  Therefore, due to the difference in the coefficient of linear expansion between the material constituting the retardation layer and the substrate, the conventional technique has a phenomenon in which a black display having a bright portion and a dark portion on the diagonal line occurs.

  Due to the difference in the linear expansion coefficient, the optical axis of the in-plane end portion of the retardation layer is shifted, and unevenness of contrast occurs. That is, as the temperature rises, the optical axis of the phase difference plate changes, so that the black characteristics change significantly at the four corners of the screen, causing problems in image characteristics.

<Configuration of retardation plate>
In order to solve the above problems, in the present embodiment, a configuration of a retardation plate as described below will be described as an example. The configuration of the phase difference plate is roughly divided into three types as shown in FIGS.

  One is a method in which the retardation film 1a and the retardation film 1b are used in combination as shown in FIGS. 4 (a) and 4 (b).

  The retardation film 1a includes a substrate 2a made of a transparent glass substrate or the like, an alignment film 3a formed on the substrate 2a, and a first retardation layer 4a formed on the alignment film 3a. The direction of the optical axis of the first retardation layer 4a is adjusted according to the alignment treatment applied to the alignment film 3a. The alignment film 3a is formed of, for example, a photo-alignment film that can be aligned by light irradiation. The first retardation layer 4a is formed of, for example, a liquid crystal polymer.

  The retardation film 1b includes a substrate 2b made of a transparent glass substrate or the like, an alignment film 3b formed on the substrate 2b, and a second retardation layer 4b formed on the alignment film 3b. The materials of the alignment film 3b and the second retardation layer 4b are the same as those of the alignment film 3a and the first retardation layer 4a.

  In the retardation plate 1 shown in FIG. 5, a first retardation layer 4a is formed on one surface of one substrate 2 via an alignment film 3a. Further, an alignment film 3b, a second retardation layer 4b, This is an example in which are stacked.

  In the retardation plate 1 shown in FIG. 6, a first retardation layer 4a is formed on one surface of one substrate 2 via an alignment film 3a, and a second phase is formed on the other surface of the substrate 2 via an alignment film 3b. In this example, a retardation layer 4b is formed.

  The retardation plates 1a and 1b are used, for example, disposed outside the liquid crystal panel or attached to the liquid crystal panel. In the case of the phase difference plate 1, the substrate 2 may be a substrate of a liquid crystal panel. Alternatively, the phase difference plate 1 may be attached to a liquid crystal panel or may be disposed outside the liquid crystal panel.

  In the present embodiment, each of the retardation layers 4a and 4b is formed in a direction in which the in-plane optical axes are different at room temperature. Here, in the phase difference layers 4a and 4b, the direction in which the refractive index generally increases is called the slow axis, and the direction perpendicular to the slow axis is called the fast axis. Here, the slow axis is called the optical axis. The fast axis may be the optical axis.

  FIG. 7A is a schematic diagram showing the direction of the optical axis of the first retardation layer 4a at room temperature, and FIG. 7B is a schematic diagram showing the direction of the optical axis of the second retardation layer 4b at room temperature. FIG.

  The first retardation layer 4a is formed in a direction in which the optical axes Ax2, Ax3, Ax4, and Ax5 in the peripheral portion are different from the reference optical axis Ax1 at normal temperature with the vertical optical axis Ax1 in the central portion as the reference optical axis. ing. For example, the optical axes Ax2 and Ax3 existing in one diagonal direction are formed to be shifted in the rotation direction (clockwise) R with respect to the reference optical axis Ax1. The optical axes Ax4 and Ax5 existing in the other diagonal direction are formed so as to be shifted in the rotational direction (counterclockwise) L with respect to the reference optical axis Ax1.

  The second retardation layer 4b is formed in a direction in which the optical axes Bx2, Bx3, Bx4, and Bx5 in the peripheral portion are different from the reference optical axis Bx1 at room temperature with the horizontal optical axis Bx1 in the central portion as the reference optical axis. ing. For example, the optical axes Bx2 and Bx3 existing in one diagonal direction are formed so as to be shifted in the rotation direction (counterclockwise) L with respect to the reference optical axis Bx1. The optical axes Bx4 and Bx5 existing in the other diagonal direction are formed so as to be shifted in the rotation direction (clockwise) R with respect to the reference optical axis Bx1.

  As a result, the crossing angle of the optical axes of the first retardation layer 4a and the second retardation layer 4b is as shown in FIG.

  That is, at normal temperature, when the optical axis crossing angle A3 at the center is set to 90 °, the optical axis crossing angles B3 and D3 on one diagonal line are set to be smaller than 90 °, The crossing angles C3 and E3 of the optical axes on the diagonal line are set to be larger than 90 °.

  Alternatively, as shown in FIG. 8B, when the crossing angle A3 ′ of the optical axes at the center is set to 90 °, the crossing angles B3 ′ and D3 ′ of the optical axes on one diagonal line are set to 90. When it is preferable to set the angle larger than °, the crossing angles C3 ′ and E3 ′ of the optical axes on the other diagonal line are made smaller than 90 °.

  At room temperature, as shown in FIGS. 8A and 8B, by changing the crossing angle of the optical axes at the center and the crossing angles of the optical axes at the four corners on the diagonal line, That is, when the temperature of the phase difference plate rises, the crossing angles of the optical axes are substantially matched within the plane as shown in FIGS. 9 (a) and 9 (b).

  As described above, the shift of the optical axis of the retardation layer accompanying the temperature rise is particularly noticeable in the diagonal direction. For this reason, it is preferable that the optical axes at the four corners located at least on the diagonal are different from the optical axis at the center. The direction of the optical axis other than the portion located on the diagonal line may be defined in the middle between the central portion and the four corners, or may be set to be the same as the central portion. For example, when an optical alignment film is used as the alignment films 3a and 3b, the direction of the optical axis in the plane of the retardation layer can be adjusted in many kinds. However, when the alignment is performed by a normal rubbing process, it is difficult to adjust the direction of the optical axis in the plane in various ways from the viewpoint of throughput, and it is preferable to change only the optical axes at the four corners.

  In any case, the crossing angles of the peripheral parts, particularly the four corners, are preliminarily shifted from the reference crossing angle at room temperature, and the crossing angles of the optical axes in the peripheral part are substantially matched with the reference crossing angle at the temperature in use.

  When the retardation plate according to the present embodiment is used in a projection-type liquid crystal display device, a high-quality and high-contrast image without unevenness is actually displayed at the temperature in use as shown in FIG. I was able to.

<Production method of retardation plate>
An example of a method for producing the retardation plate will be described. In this example, a method for manufacturing the retardation film 1a shown in FIG. 4A will be described as an example.

  First, the board | substrate 2a used for a phase difference plate is produced. For example, a transparent insulating substrate is prepared as the substrate 2a. In the case of being manufactured integrally with the liquid crystal panel, a transparent insulating substrate with a switching element such as a TFT element or a transparent electrode may be used.

  Next, an alignment film 3a is applied on the substrate 2a. The alignment film 3a is preferably a photocurable alignment film. In the exposure process for forming the photo-alignment film, a plurality of exposure processes may be performed, or in one photomask, the orientation directions of regions corresponding to the four corners of one retardation plate may be changed. .

  Next, a retardation layer material is applied on the alignment film. For example, a liquid crystal polymer is used as the retardation layer material. In the liquid crystal polymer, liquid crystal molecules are aligned according to the alignment direction of the alignment film. Thereby, the phase difference plate 1a having a plurality of optical axes in the plane can be produced. The manufacturing method of the retardation film 1b is the same as that of the retardation film 1a. The phase difference plate 1a and the phase difference plate 1b may be bonded together.

  In this case, the retardation of each phase difference layer 4a, 4b with respect to the normal direction is preferably 80 nm or less. In addition, it is preferable that the direction of the optical axis (alignment axis) of each of the retardation layers 4a and 4b differs from the optical axis of at least the central part in the plane of the liquid crystal layer by 0.5 ° to 5 °. This is because the change of the optical axis was confirmed in the above angle range as the temperature increased.

  In the production of the retardation film 1 shown in FIGS. 5 and 6, the alignment film 3b and the second retardation layer 4b may be formed on the same substrate.

  With the retardation plate according to the present embodiment, the value of the crossing angle of the in-plane optical axes at room temperature can be changed, and the in-plane optical axes can be aligned at the projection temperature. As a result, the retardation plate according to the present embodiment can uniformly compensate the optical distortion of the liquid crystal layer in the plane.

<Configuration of liquid crystal panel and light modulation means>
Next, an optical modulation unit configured by combining the above retardation plate and a liquid crystal panel will be described with reference to FIGS. 11 and 12. FIG.

  In FIG. 11A, in the light modulation means 10a having the polarizing plate 11 on the incident side, the liquid crystal panel 12, and the polarizing plate 13 on the output side, the phase difference plate 1a and the phase difference plate 1b according to this embodiment are It is an example installed before and after the liquid crystal panel 12. Dustproof glasses 12a and 12b exist outside the liquid crystal panel 12 used in the projection display device. Inside the dust-proof glasses 12a and 12b, although not shown, there are a liquid crystal layer and a pair of substrates sandwiching the liquid crystal layer. All the light rays incident on the pixels of the liquid crystal panel 12 are optically modulated in each pixel, and are enlarged and projected onto the screen 15 by the projection lens 14.

  Further, for example, the configuration shown in FIG. In the light modulation means 10b, two retardation plates 1a and 1b are installed between the liquid crystal panel 12 provided with the dust-proof glasses 12a and 12b and the polarizing plate 13 on the emission side. Alternatively, retardation plates 1a and 1b may be installed between the liquid crystal panel 12 and the polarizing plate 11 on the incident side.

  Further, as shown in FIG. 12A, a retardation layer may be formed in the liquid crystal panel 12 instead of installing a retardation plate as an independent component. For example, in the light modulation means 10c, the first retardation layer 4a is formed inside the dustproof glass 12a of the liquid crystal panel 12, and the second retardation layer 4b is formed inside the dustproof glass. In this case, an alignment film for restricting the optical axis of each of the retardation layers 4a and 4b is formed between the dust-proof glasses 12a and 12b, or between an inner substrate (not shown).

  Further, as in the light modulation means 10d shown in FIG. 12B, two retardation layers 4a and 4b may be formed inside the emission-side dust-proof glass 12b in the liquid crystal panel 12. Alternatively, two retardation layers 4 a and 4 b may be formed inside the dust-proof glass 12 a on the incident side in the liquid crystal panel 12.

  In addition to the structure shown in the figure, the two retardation layers 4a and 4b may be formed outside the dust-proof glasses 12a and 12b of the liquid crystal panel 12 via an alignment film. In this case, one retardation layer may be formed on each dustproof glass 12a, 12b, or two retardation layers may be formed only on one dustproof glass. It can also be used for liquid crystal panels equipped with microlenses.

  As shown in FIGS. 11 and 12, by using the phase difference plate or the phase difference layer of the present invention, a high contrast and high quality projected image can be obtained.

<Configuration of liquid crystal projector>
Next, a projection type liquid crystal display device configured using any one of the light modulation means 10a to 10d will be described.

  FIG. 13 is a diagram showing an example of the overall configuration of the projection type liquid crystal display device of the present embodiment. The projection type liquid crystal display device 20 of this embodiment is a so-called three-plate type projection type liquid crystal display device that displays an image using three transmissive liquid crystal panels. However, the present invention is not limited to a three-plate projection type liquid crystal display device, and can also be used for a so-called single-plate type projection liquid crystal display device that displays an image using a single transmissive liquid crystal panel. Details will be described below.

  In the three-plate projection type liquid crystal display device, light modulation means 10R, 10G, and 10B are installed for each color of red (R), green (G), and blue (B). The configuration of the light modulators 10R, 10G, and 10B corresponds to any of the light modulators 10a to 10d described with reference to FIGS.

  In the projection type liquid crystal display device 20 shown in FIG. 13, the lamp 22 has a light emitting portion 22b at the focal position of the reflector 22a, and the light emitted from the lamp 22 is light substantially parallel to the optical axis of the reflector 22a. Is emitted forward from the opening.

  In the rear stage of the lamp 22, a similar external shape that is substantially equal to the aspect ratio of the illuminated area (corresponding to an effective aperture for performing light modulation for pixel formation) of the liquid crystal panel in the light modulation means 10R, 10G, and 10B. For example, and a multi-lens array 24 in which a plurality of lens cells are formed so as to face the lens cells of the multi-lens array 23. Is arranged. The light condensed by the multi-lens arrays 23 and 24 is polarized by the polarization conversion block 25 into light having a predetermined polarization direction. That is, the non-polarized light (P-polarized wave + S-polarized wave) emitted from the lamp 22 passes through the polarization conversion block 25 and thereby has a predetermined polarization direction (for example, P) corresponding to the light modulation means 10R, 10G, 10B. Polarized light).

  The light converted into, for example, a P-polarized wave by the polarization conversion block 25 is incident on a plano-convex lens 26 arranged at the subsequent stage of the polarization conversion block 25. The plano-convex lens 26 condenses the light from the polarization conversion block 25 and efficiently irradiates the light modulation means 10R, 10G, and 10B.

  The light emitted from the plano-convex lens 26, that is, white light, first enters the dichroic mirror 27 that passes the red light R, where the red light R passes and the green G and blue light B are reflected. The red light R transmitted through the dichroic mirror 27 is guided by the mirror 28 to the light modulation means 10R via the plano-convex lens 29 with the traveling direction being bent by 90 °, for example.

  On the other hand, the green light G and the blue light B reflected by the dichroic mirror 27 enter the dichroic mirror 30 that transmits the blue light B, and are separated into the green light G and the blue light B. That is, the green light G is reflected and guided to the light modulation means 10G via the plano-convex lens 31. The blue light B passes through the dichroic mirror 30 and travels straight, and is guided to the light modulation means 10B via the relay lens 32, the mirror 33, the relay lens 34, the mirror 35, and the plano-convex lens 36.

  Each color light light-modulated by the light modulation means 10R, 10G, 10B enters the cross prism 37, respectively. The cross prism 37 has an outer shape formed by, for example, joining a plurality of glass prisms. Interference filters 37a and 37b having predetermined optical characteristics are formed on the joint surfaces of the glass prisms. For example, the interference filter 37a is configured to reflect red light R and transmit green light G. The interference filter 37b is configured to reflect the blue light B and transmit the green light G. Therefore, the red light R is reflected by the interference filter 37a, and the blue light B is reflected by the interference filter 37b in the direction of the projection lens 38. Then, the green light G reaches the projection lens 38 by passing through the interference filters 37a and 37b, where each color light is combined into one optical axis.

  In the projection-type liquid crystal display device according to the above-described embodiment, by providing the retardation layer or the retardation plate according to the above-described embodiment, it is possible to obtain a high-quality display with high contrast and no contrast unevenness. it can. In particular, by using a liquid crystal panel provided with retardation layers 4a and 4b instead of a retardation plate as a single component, the projection type liquid crystal display device can be miniaturized.

The present invention is not limited to the description of the above embodiment.
The retardation plate or retardation layer of the present invention is similarly applied not only to a projection type liquid crystal display device using a TN-LCD type liquid crystal panel or a VA-LCD type liquid crystal panel, but also to a direct view type liquid crystal panel. be able to.
In addition, various modifications can be made without departing from the scope of the present invention.

It is a figure for demonstrating the contrast nonuniformity which generate | occur | produces with a temperature rise. It is a figure which shows an example of the optical axis design of the conventional phase difference layer. It is a figure for demonstrating the change of the optical axis of the phase difference layer in the temperature at the time of projection. It is a figure for demonstrating the structure of the phase difference plate which concerns on this embodiment. It is a figure which shows the other structural example of a phase difference plate. It is a figure which shows the other structural example of a phase difference plate. It is a figure which shows the direction of the optical axis in normal temperature of each phase difference layer. It is a figure which shows the crossing angle of the optical axis of two phase difference layers in normal temperature. It is a figure which shows the crossing angle of the optical axis of two phase difference layers in projection temperature. It is a figure for demonstrating the effect of the phase difference plate which concerns on this embodiment. It is a figure which shows the structure of the liquid crystal panel which concerns on this embodiment. It is a figure which shows the structure of the liquid crystal panel which concerns on this embodiment. It is a figure which shows the structure of the projection type display apparatus which concerns on this embodiment.

Explanation of symbols

1, 1a, 1b ... retardation plate, 2 ... substrate, 2a ... first substrate, 2b ... second substrate, 3a, 3b ... alignment film, 4a ... first retardation layer, 4b ... second position Phase difference layer, 10a, 10b, 10c, 10d ... light modulation means, 11 ... polarizing plate, 12 ... liquid crystal panel, 12a ... dust-proof glass, 12b ... dust-proof glass, 13 ... polarizing plate, 14 ... projection lens, 15 ... screen, 20 Projection type display device, 22: Lamp, 22a: Reflector, 22b ... Light emitting unit, 23, 24 ... Multi lens array, 25 ... Polarization conversion block, 26 ... Plano-convex lens, 27 ... Dichroic mirror, 28 ... Mirror, 29 ... Flat Convex lens, 30 ... Dichroic mirror, 31 ... Plano-convex lens, 32 ... Relay lens, 33 ... Mirror, 34 ... Relay lens, 35 ... Mirror, 36 ... Plano-convex lens, 37 ... Cross prism, 37 ... interference filter, 37b ... interference filter, 38 ... projection lens

Claims (17)

A substrate,
A retardation layer formed on the substrate;
The retardation layer is formed such that the in-plane optical axes are formed in different directions at room temperature, and the in-plane optical axes are aligned when the in-plane optical axes are raised to a predetermined temperature. The retardation layer is formed in a direction different from the reference optical axis at normal temperature with the optical axis in the central portion as a reference optical axis, and when the optical axis in the peripheral portion rises to a predetermined temperature, The phase difference plate of Claim 1. It was prescribed | regulated so that the direction of an optical axis might align with the said reference | standard optical axis. The phase difference plate according to claim 2, wherein the retardation layer is formed such that an optical axis of a peripheral portion located in a diagonal direction of an outer shape of the retardation layer is different from the reference optical axis at room temperature. In the first diagonal direction, the optical axis of the peripheral portion of the retardation layer is shifted in the first rotation direction with respect to the reference optical axis, and the second diagonal direction intersects the first diagonal line. The phase difference plate according to claim 3, wherein the phase difference plate is formed so as to be shifted in a second rotation direction opposite to the first rotation direction with respect to the reference optical axis. A substrate,
A first retardation layer and a second retardation layer formed on the substrate;
The first and second retardation layers are formed such that the crossing angles of the optical axes in the plane are different at room temperature, and the crossing angles in the plane substantially coincide with each other when the temperature rises to a predetermined temperature. Retardation plate specified in 1. The first and second retardation layers are formed so that the crossing angle in the peripheral part is different from the reference crossing angle at normal temperature, with the crossing angle in the central part being a reference crossing angle, and the temperature has risen to a predetermined temperature. The retardation plate according to claim 5, wherein the crossing angle of the peripheral portion is defined so as to substantially coincide with the reference crossing angle. In the first and second retardation layers, the crossing angle of the optical axes of the peripheral portions located in the diagonal direction of the outer shape of the first and second retardation layers is different from the reference crossing angle at room temperature. The phase difference plate according to claim 6 formed. The intersection angle of the peripheral portion is formed so as to be larger than the reference intersection angle in a first diagonal direction and smaller than the reference intersection angle in a second diagonal direction intersecting with the first diagonal line. The phase difference plate according to claim 7. A liquid crystal layer;
Two substrates disposed outside the liquid crystal layer;
A first retardation layer and a second retardation layer formed on the substrate;
The first and second retardation layers are formed such that the crossing angles of the optical axes in the plane are different at room temperature, and the crossing angles in the plane substantially coincide with each other when the temperature rises to a predetermined temperature. LCD panel specified in 1. The first and second retardation layers are formed so that the crossing angle in the peripheral part is different from the reference crossing angle at normal temperature, with the crossing angle in the central part being a reference crossing angle, and the temperature has risen to a predetermined temperature. The liquid crystal panel according to claim 9, wherein the intersection angle of the peripheral portion is defined so as to substantially coincide with the reference intersection angle. In the first and second retardation layers, the crossing angle of the optical axes of the peripheral portions located in the diagonal direction of the outer shape of the first and second retardation layers is different from the reference crossing angle at room temperature. The liquid crystal panel according to claim 10 formed. The intersection angle of the peripheral portion is formed so as to be larger than the reference intersection angle in a first diagonal direction and smaller than the reference intersection angle in a second diagonal direction intersecting with the first diagonal line. The liquid crystal panel according to claim 11. 10. The liquid crystal panel according to claim 9, wherein the first and second retardation layers are formed to have different crossing angles of optical axes in a plane within an angle range within 5 ° at room temperature. 10. The liquid crystal panel according to claim 9, wherein the first and second retardation layers are formed so that retardation in a normal direction is not less than 10 nm and not more than 80 nm in a plane. The first retardation layer is formed on one of the two substrates,
The liquid crystal panel according to claim 9, wherein the second retardation layer is formed on the other substrate. The liquid crystal panel according to claim 9, wherein both the first retardation layer and the second retardation layer are formed on one of the two substrates. A light source;
A liquid crystal panel that modulates light from the light source;
Projecting means for projecting light modulated by the liquid crystal panel;
The liquid crystal panel has two substrates disposed outside the liquid crystal layer, and a first retardation layer and a second retardation layer formed on the substrate,
The first and second retardation layers are formed such that the crossing angles of the optical axes in the plane are different at room temperature, and the crossing angles in the plane substantially coincide with each other when the temperature rises to a predetermined temperature. Projection type display device specified in 1.

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