JP2006323417A - Liquid crystal device and projection type display apparatus - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a liquid crystal device 100 capable of obtaining a high contrast ratio within incident angle of light source light with respect to a light modulation means of a projection type display apparatus. <P>SOLUTION: The liquid crystal device 100 includes a liquid crystal panel 60 operating in twisted nematic mode. A first optical compensation sheet 70 is disposed on the light incident side of the liquid crystal panel 60 and a second optical compensation sheet 80 is disposed on the light emission side thereof. The respective optical compensation sheets 70, 80 are constituted by subjecting liquid crystal molecules exhibiting negative refractive index anisotropy to hybrid alignment, and are arranged so that the retardation in the normal direction is made to be ≥10 nm and ≤30 nm, and fast axis directions 71, 81 intersect each other at an angle that is not right angle when seeing from respective normal directions. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

  The present invention relates to a liquid crystal device and a projection display device.

  A liquid crystal device is used as light modulation means in a projection display device such as a liquid crystal projector. A liquid crystal device is configured by sandwiching a liquid crystal layer between a pair of substrates. Electrodes for applying an electric field to the liquid crystal layer are formed inside the pair of substrates. An alignment film that regulates the alignment state of the liquid crystal molecules is formed inside the electrode. Then, image light is formed on the basis of the change in the orientation of the liquid crystal molecules between when the non-selection voltage is applied and when the selection voltage is applied.

A projection display device using a conventional liquid crystal device has a contrast ratio of a projected image of only about 1: 500, and a contrast ratio of a projection display device using a mechanical shutter such as DMD (registered trademark) is 1: 3000. It was inferior in comparison. The cause is the viewing angle characteristic of the liquid crystal device. In the first place, the light source light incident on the light modulation means of the projection display device is not completely parallel light.
However, since the liquid crystal device used as the light modulator has an incident angle dependency, this causes a reduction in the contrast ratio of the projected image.

Therefore, an optical compensator is used to compensate for the incident angle dependency of the liquid crystal device. This optical compensator is obtained by hybrid-aligning discotic liquid crystal exhibiting negative refractive index anisotropy (see, for example, Patent Document 1 and Non-Patent Document 1). Due to this hybrid orientation, the optical compensator has a slow axis and a fast axis when viewed from the normal direction. Therefore, the optical compensator has a phase difference in the normal direction.
FIG. 13 is a graph showing the viewing angle dependence of the phase difference in the optical compensator described in Patent Document 1. As can be seen from FIG. 13, the phase difference when the viewing angle with respect to the optical compensator is 0 °, that is, the phase difference in the normal direction of the optical compensator is about 40 nm. Patent Document 2 discloses an example in which the phase difference in the normal direction of the optical compensator is 70 nm and 80 nm.

A first optical compensation plate is disposed outside the light incident side substrate of the liquid crystal panel, and a second optical compensation plate is disposed outside the light emission side substrate. The first optical compensation plate and the second optical compensation plate are fast axis directions when viewed from the normal direction of each optical compensation plate (that is, the orientation regulating direction of the discotic liquid crystal, and are indicated by an arrow 71 in FIG. (X-axis direction) is arranged so as to substantially coincide with the alignment regulating direction of the alignment film in the corresponding substrate. In addition, since the alignment regulating directions of the respective substrates of the liquid crystal panel are substantially orthogonal, the alignment regulating directions of the respective optical compensators are also arranged to be substantially orthogonal.
JP-A-8-50206 Japanese Patent Laid-Open No. 9-15687 Hiroyuki Mori, “Liquid Crystal Display Introductory Lecture 11: TFT-LCD Viewing Angle Expansion Technology Using Discotic Optical Compensation Films”, Liquid Crystal, Japanese Liquid Crystal Society, January 25, 2002, Vol. 6, No. 1, p84 -92

  However, the optical compensation plate was originally developed for a direct-view type liquid crystal panel, and is designed to obtain a high contrast ratio in a wide viewing angle range. On the other hand, the incident angle of the light source light with respect to the light modulation means of the projection display device is at most about 12 ° polar angle. A projection image is formed by the incident light in the narrow angle range. Therefore, it is desired to develop a liquid crystal device that can obtain a higher contrast ratio in the narrow viewing angle range.

  By the way, when an electric field is applied to the liquid crystal layer of the liquid crystal panel, the liquid crystal molecules near the center of the liquid crystal layer are vertically aligned, but the liquid crystal molecules near the alignment film are not completely vertically aligned. Therefore, the liquid crystal panel when an electric field is applied has a slight phase difference even when observed from the normal direction. This phase difference causes light leakage in black display and reduces the contrast ratio in the normal direction of the liquid crystal panel.

  The present invention has been made to solve the above problems, and provides a liquid crystal device capable of obtaining a high contrast ratio within the range of the incident angle of light source light with respect to the light modulation means of a projection display device. With the goal. It is another object of the present invention to provide a projection display device that can obtain a high contrast ratio in a projected image.

In order to solve the above problems, a liquid crystal device of the present invention includes a liquid crystal panel in which a liquid crystal layer is sandwiched between a pair of substrates, and the liquid crystal panel operates in a twisted nematic mode. An optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy is disposed outside one substrate, and a phase difference in the normal direction of the optical compensator is 10 nm or more and 30 nm or less. It is characterized by that.
According to this configuration, the phase difference in the normal direction in the liquid crystal panel can be compensated by the optical compensator. Thereby, it is possible to prevent light leakage in black display, and a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

In addition, the first optical compensation plate is arranged outside one of the pair of substrates, and the second optical compensation plate is arranged outside the other substrate of the pair of substrates. Preferably, the first optical compensation plate and the second optical compensation plate are arranged such that the fast axes when viewed from the respective normal directions intersect at an angle other than a right angle.
According to this configuration, the phase difference of the liquid crystal layer on one substrate side in the liquid crystal panel is compensated by the first optical compensator, and the phase difference of the liquid crystal layer on the other substrate side is compensated by the second optical compensator. The Then, by causing the fast axes of the first optical compensation plate and the second optical compensation plate to intersect at a non-perpendicular angle, it becomes possible to generate a phase difference in the normal direction as the entire optical compensation plate. The normal phase difference in the panel can be compensated. Therefore, a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

The first optical compensation plate is arranged outside one of the pair of substrates, and the second optical compensation plate is arranged outside the first optical compensation plate, The second optical compensator is disposed such that a surface having a smaller angle formed by the optical axis of the liquid crystal molecules and the normal direction of the second optical compensator faces the first optical compensator. In addition, the first optical compensation plate and the second optical compensation plate may be arranged such that the fast axes when viewed from the respective normal directions intersect at an angle other than a right angle.
Also with this configuration, the phase difference of the liquid crystal layer on one substrate side in the liquid crystal panel is compensated by the first optical compensator, and the phase difference of the liquid crystal layer on the other substrate side is compensated by the second optical compensator. . Further, it becomes possible to compensate for the phase difference in the normal direction in the liquid crystal panel, and a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

The first optical compensation plate and the second optical compensation plate are preferably arranged outside the substrate on the light emitting side of the pair of substrates.
According to this configuration, since the first optical compensation plate and the second optical compensation plate are arranged away from the light source, the heat from the light source is reduced by the amount far from the light source and the amount of light reduced by the aperture ratio of the liquid crystal device. Deterioration due to influence can be suppressed.

Further, the fast axis of one of the first optical compensation plate and the second optical compensation plate is parallel to the orientation regulating direction of the substrate corresponding to the optical compensation plate. It is desirable that they are arranged as follows.
According to this configuration, when viewed from the normal direction of each optical compensation plate by adjusting only the arrangement of either one of the first optical compensation plate and the second optical compensation plate Can be crossed at non-normal angles.

In addition, the projection contrast of the liquid crystal device is within a range where an intersection angle between the fast axis of the first optical compensator and the fast axis of the second optical compensator is in a range of 91 ° to 110 °. It is desirable that the angle has the maximum ratio.
According to this configuration, it is possible to balance the compensation of the phase difference in the normal direction in the liquid crystal panel and the compensation of the phase difference in a range where the polar angle from the normal direction is small. Therefore, a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

On the other hand, a projection display device according to the present invention is characterized in that the above-described liquid crystal device is provided as light modulation means.
In the projection display device, the incident angle of the light source light with respect to the light modulation means is about 12 ° polar angle, and the projection image is constituted by the incident light. The liquid crystal device described above can compensate for a phase difference in a range where the normal direction and polar angle of the liquid crystal panel are small, and light leakage in black display can be prevented. Therefore, a high contrast ratio can be obtained in the projected image.

Embodiments of the present invention will be described below with reference to the drawings. In each drawing used for the following description, the scale of each member is appropriately changed to make each member a recognizable size.
In the present specification, the liquid crystal layer side of each component of the liquid crystal device is referred to as an inner side, and the opposite side is referred to as an outer side. “When a non-selection voltage is applied” and “when a selection voltage is applied” are respectively “when the applied voltage to the liquid crystal layer is close to the threshold voltage of the liquid crystal” and “the applied voltage to the liquid crystal layer is It means “when sufficiently high compared to the threshold voltage”.

[First Embodiment]
First, a liquid crystal device according to a first embodiment of the present invention will be described with reference to FIGS. The liquid crystal device according to the first embodiment includes a liquid crystal panel in which a liquid crystal layer is sandwiched between a pair of substrates, an optical compensator disposed on the outer side of the liquid crystal panel, and an outer side of the optical compensator. A polarizing plate. In the present embodiment, an active matrix transmissive liquid crystal panel using a thin film transistor (hereinafter referred to as TFT) element as a switching element will be described as an example.

(Equivalent circuit)
FIG. 1 is an equivalent circuit diagram of a liquid crystal panel. Pixel electrodes 9 are formed on a plurality of dots arranged in a matrix to form an image display area of the transmissive liquid crystal panel. Further, a TFT element 30 which is a switching element for performing energization control to the pixel electrode 9 is formed on the side of the pixel electrode 9. A data line 6 a is electrically connected to the source of the TFT element 30. Image signals S1, S2,..., Sn are supplied to each data line 6a. The image signals S1, S2,..., Sn may be supplied to each data line 6a in this order, or may be supplied for each group to a plurality of adjacent data lines 6a.

The scanning line 3 a is electrically connected to the gate of the TFT element 30. Scan signals G1, G2,..., Gm are supplied to the scanning line 3a in pulses at a predetermined timing. The scanning signals G1, G2,..., Gm are applied sequentially to the respective scanning lines 3a in this order.
Further, the pixel electrode 9 is electrically connected to the drain of the TFT element 30. When the TFT elements 30 serving as switching elements are turned on for a certain period by the scanning signals G1, G2,..., Gm supplied from the scanning line 3a, the image signals S1, S2,. , Sn are written into the liquid crystal of each pixel at a predetermined timing.

  The predetermined level image signals S1, S2,..., Sn written in the liquid crystal are held for a certain period by a liquid crystal capacitor formed between the pixel electrode 9 and a common electrode described later. In order to prevent the retained image signals S1, S2,..., Sn from leaking, a storage capacitor 17 is formed between the pixel electrode 9 and the capacitor line 3b, and is arranged in parallel with the liquid crystal capacitor. . Thus, when a voltage signal is applied to the liquid crystal, the alignment state of the liquid crystal molecules changes depending on the applied voltage level. As a result, the light incident on the liquid crystal is modulated to enable gradation display.

(Planar structure)
FIG. 2 is an explanatory diagram of a planar structure of the liquid crystal panel. In the liquid crystal panel of this embodiment, a rectangular pixel electrode 9 made of a transparent conductive material such as indium tin oxide (hereinafter referred to as ITO) is formed on the TFT array substrate (the outline is indicated by a broken line 9a). Are arranged in a matrix. A data line 6 a, a scanning line 3 a, and a capacitor line 3 b are provided along the vertical and horizontal boundaries of the pixel electrode 9. In the present embodiment, the region where each pixel electrode 9 is formed is a dot, and the display can be performed for each dot arranged in a matrix.

  The TFT element 30 is formed around a semiconductor layer 1a made of a polysilicon film or the like. A data line 6 a is electrically connected to a source region (described later) of the semiconductor layer 1 a through a contact hole 5. Further, the pixel electrode 9 is electrically connected to the drain region (described later) of the semiconductor layer 1 a through the contact hole 8. On the other hand, a channel region 1a 'is formed in a portion of the semiconductor layer 1a facing the scanning line 3a. The scanning line 3a functions as a gate electrode in a portion facing the channel region 1a '.

  The capacitance line 3b is a data line from the intersection of the main line portion (that is, the first region formed along the scanning line 3a in plan view) extending in a substantially straight line along the scanning line 3a and the data line 6a. And a protruding portion (that is, a second region extending along the data line 6 a when viewed in a plan view) protruding toward the front side (upward in the drawing) along 6 a. In addition, a first light shielding film 11a is formed in a region indicated by a diagonal line rising to the right in FIG. Then, the protruding portion of the capacitor line 3b and the first light shielding film 11a are electrically connected through the contact hole 13 to form a storage capacitor to be described later.

(Cross-section structure)
FIG. 3 is an explanatory diagram of a cross-sectional structure of the liquid crystal panel, and is a side cross-sectional view taken along the line AA ′ of FIG. As shown in FIG. 3, the liquid crystal panel 60 of the present embodiment is mainly composed of a TFT array substrate 10, a counter substrate 20 disposed so as to face the TFT array substrate 10, and a liquid crystal layer 50 sandwiched therebetween. Yes. The TFT array substrate 10 is mainly composed of a substrate body 10A made of a translucent material such as glass or quartz, a TFT element 30, a pixel electrode 9, an alignment film 16 and the like formed inside thereof. One counter substrate 20 is mainly composed of a substrate body 20A made of a light-transmitting material such as glass or quartz, and a common electrode 21 and an alignment film 22 formed inside thereof.

  On the surface of the TFT array substrate 10, a first light shielding film 11a and a first interlayer insulating film 12, which will be described later, are formed. A semiconductor layer 1a is formed on the surface of the first interlayer insulating film 12, and a TFT element 30 is formed around the semiconductor layer 1a. A channel region 1a 'is formed in a portion of the semiconductor layer 1a facing the scanning line 3a, and a source region and a drain region are formed on both sides thereof. Since the TFT element 30 adopts an LDD (Lightly Doped Drain) structure, a high concentration region having a relatively high impurity concentration and a relatively low concentration region (LDD) in the source region and the drain region, respectively. Region). That is, a low concentration source region 1b and a high concentration source region 1d are formed in the source region, and a low concentration drain region 1c and a high concentration drain region 1e are formed in the drain region.

  A gate insulating film 2 is formed on the surface of the semiconductor layer 1a. Then, a scanning line 3a is formed on the surface of the gate insulating film 2, and a part thereof constitutes a gate electrode. A second interlayer insulating film 4 is formed on the surfaces of the gate insulating film 2 and the scanning line 3a. A data line 6a is formed on the surface of the second interlayer insulating film 4, and the data line 6a is electrically connected to the high-concentration source region 1d through a contact hole 5 formed in the second interlayer insulating film 4. ing. Further, a third interlayer insulating film 7 is formed on the surfaces of the second interlayer insulating film 4 and the data line 6a. Then, a pixel electrode 9 is formed on the surface of the third interlayer insulating film 7, and the pixel electrode 9 becomes a high-concentration drain region through a contact hole 8 formed in the second interlayer insulating film 4 and the third interlayer insulating film 7. 1e is electrically connected. Further, an alignment film 16 made of polyimide or the like is formed so as to cover the pixel electrode 9. The surface of the alignment film 16 is rubbed or the like so that the alignment direction of the liquid crystal molecules when a non-selection voltage is applied can be regulated.

  In the present embodiment, the first storage capacitor electrode 1f is formed by extending the semiconductor layer 1a. Further, the gate insulating film 2 is extended to form a dielectric film, and the capacitor line 3b is disposed on the surface thereof to form a second storage capacitor electrode. Thus, the above-described storage capacitor 17 is configured.

  The first light shielding film 11 a is formed on the surface of the TFT array substrate 10 corresponding to the formation region of the TFT element 30. The first light shielding film 11a prevents light incident on the liquid crystal panel from entering the channel region 1a ′, the low concentration source region 1b, and the low concentration drain region 1c of the semiconductor layer 1a. The first light-shielding film 11a is electrically connected to the previous-stage or subsequent-stage capacitor line 3b through a contact hole 13 formed in the first interlayer insulating film 12. Accordingly, the first light shielding film 11a functions as a third storage capacitor electrode, and a new storage capacitor is formed between the first storage capacitor electrode 1f and the first interlayer insulating film 12 as a dielectric film.

  On the other hand, a second light shielding film 23 is formed on the surface of the counter substrate 20 corresponding to the formation region of the data lines 6 a, the scanning lines 3 a, and the TFT elements 30. The second light shielding film 23 prevents light incident on the liquid crystal panel from entering the channel region 1a ', the low concentration source region 1b, and the low concentration drain region 1c of the semiconductor layer 1a. Further, a common electrode 21 made of a conductor such as ITO is formed on almost the entire surface of the counter substrate 20 and the second light shielding film 23. Further, an alignment film 22 made of polyimide or the like is formed on the surface of the common electrode 21. The surface of the alignment film 22 is rubbed or the like so that the alignment direction of the liquid crystal molecules when a non-selection voltage is applied can be regulated.

A liquid crystal layer 50 made of nematic liquid crystal is sandwiched between the TFT array substrate 10 and the counter substrate 20. The nematic liquid crystal molecules exhibit a positive dielectric anisotropy, and are horizontally aligned when a non-selection voltage is applied and vertically aligned when a selection voltage is applied. Nematic liquid crystal molecules exhibit positive refractive index anisotropy, and the product (retardation) Δnd of the birefringence and the liquid crystal layer thickness is, for example, about 0.40 μm (60 ° C.).
Note that the alignment regulation direction by the alignment film 16 of the TFT array substrate 10 and the alignment regulation direction by the alignment film 22 of the counter substrate 20 are arranged in a twisted state of about 90 ° as shown by arrows 67 and 68 in FIG. Has been. Thereby, the liquid crystal panel 60 of the present embodiment is configured to operate in a twisted nematic mode.

(Polarizer)
FIG. 4 is an exploded perspective view of the liquid crystal device according to the first embodiment. The liquid crystal device 100 of the present embodiment includes the above-described liquid crystal panel 60, optical compensation plates 70 and 80 disposed outside the liquid crystal panel 60, and polarizing plates 62 and 64 disposed outside the optical compensation plates 70 and 80. And is composed of. The optical compensators 70 and 80 and the polarizing plates 62 and 64 are mounted on a support substrate 78 (see FIG. 5) made of a light-transmitting material having high thermal conductivity such as sapphire glass or quartz, and a liquid crystal panel. It is spaced from 60.

  As shown in FIG. 4, a polarizing plate 62 is disposed on the light incident side of the liquid crystal panel 60, and a polarizing plate 64 is disposed on the light emitting side. Each of the polarizing plates 62 and 64 has a function of absorbing linearly polarized light in the absorption axis direction and transmitting linearly polarized light in the transmission axis direction. And each polarizing plate 62 and 64 is arrange | positioned so that each absorption axis and transmission axis may be orthogonal. The light emitting side polarizing plate 64 is arranged such that the absorption axis 65 or the transmission axis thereof substantially coincides with the alignment regulating direction 68 of the alignment film on the light emitting side substrate of the liquid crystal panel 60. The light incident side polarizing plate 62 is arranged such that the absorption axis 63 or the transmission axis thereof substantially coincides with the alignment regulating direction 67 of the alignment film on the light incident side substrate of the liquid crystal panel 60.

When light enters the liquid crystal device 100 from below the polarizing plate 62, only linearly polarized light that matches the transmission axis of the polarizing plate 62 is transmitted through the polarizing plate 62. In the liquid crystal panel 60 when the non-selection voltage is applied, the liquid crystal molecules are horizontally aligned in a spiral shape. Therefore, the linearly polarized light incident on the liquid crystal panel 60 is rotated about 90 ° and emitted from the liquid crystal panel 60. Since this linearly polarized light coincides with the transmission axis of the polarizing plate 64, it passes through the polarizing plate 64. Therefore, white display is performed on the liquid crystal panel 60 when the non-selection voltage is applied (normally white mode). Further, in the liquid crystal panel 60 when the selection voltage is applied, the liquid crystal molecules are vertically aligned (see FIG. 6). Therefore, the linearly polarized light incident on the liquid crystal panel 60 is emitted from the liquid crystal panel 60 without being rotated.
Since this linearly polarized light is orthogonal to the transmission axis of the polarizing plate 64, it does not pass through the polarizing plate 64. Therefore, black display is performed on the liquid crystal panel 60 when the selection voltage is applied.

(Optical compensation plate)
In this embodiment, the first optical compensation plate 70 is disposed outside the light incident side substrate of the liquid crystal panel 60, and the second optical compensation plate 80 is disposed outside the light emission side substrate.

  FIG. 5 is a side sectional view of the optical compensation plate. The first optical compensation plate 70 is obtained by providing an alignment film (not shown) on a support 72 made of triacetylcellulose (TAC) or the like and forming a discotic compound layer 74 such as a triphenylene derivative on the alignment film. is there. The alignment film is made of polyvinyl alcohol (PVA) or the like, and its surface is subjected to rubbing or the like so that the alignment direction of the liquid crystal molecules can be regulated. On the other hand, the discotic compound layer 74 has an optical structure in which the inclination angle of the optical axis of the refractive index ellipsoid showing negative uniaxiality is continuously changed in the film thickness direction. Such a hybrid alignment structure can be obtained by applying a liquid crystalline discotic compound on the support 72 and aligning and curing at a constant temperature. The discotic compound exhibits a tilt angle of 0 to 15 ° on the support 72 side and a tilt angle of 20 to 60 ° on the opposite side. In addition, the orientation regulation direction 71 of the discotic liquid crystal is defined as the X-axis direction. The X-axis direction is the fast axis direction when the optical compensator is viewed from the normal direction. As such a first optical compensation plate 70, specifically, a WV film made by Fuji Photo Film can be adopted. The second optical compensator is also configured in the same manner as the first optical compensator 70 described above.

  FIG. 6 is an explanatory diagram of optical compensation. The nematic liquid crystal sealed in the liquid crystal panel 60 exhibits optically positive uniaxiality. That is, the refractive index in the direction of the optical axis 66 is larger than the refractive index in the other direction, and the refractive index ellipsoid becomes a rugby ball type. When a selection voltage is applied to the nematic liquid crystal of the liquid crystal panel 60, the liquid crystal molecules are vertically aligned from the center to the end in the thickness direction of the liquid crystal layer. Here, the refractive index ellipsoid of the rugby ball type becomes an ellipse when observed from an oblique direction, and the difference between the major axis and the minor axis becomes birefringence. This phase difference when observed from an oblique direction causes light leakage in black display, which lowers the contrast ratio of the liquid crystal panel and deteriorates the viewing angle characteristic.

  On the other hand, the discotic liquid crystal constituting the first optical compensation plate 70 is optically negative uniaxial. That is, the refractive index in the direction of the optical axis 76 is smaller than the refractive index in the other direction, and the refractive index ellipsoid has a disk shape. Here, if the optical axis 76 of the disc-shaped refractive index ellipsoid 75 in the first optical compensator 70 is arranged in parallel with the optical axis 66 of the rugby ball-type refractive index ellipsoid 65 in the liquid crystal panel 60, the optical axis 76 can be obtained. Therefore, the birefringence effect of the refractive index ellipsoid 65 can be canceled. Therefore, as shown in FIG. 4, the first optical compensation plate 70 is arranged so that the alignment regulation direction 71 of the alignment film in the first optical compensation plate 70 substantially coincides with the alignment regulation direction 67 of the alignment film in the liquid crystal panel 60. To do. As shown in FIG. 6, the surface with the larger angle formed by the optical axis 76 of the liquid crystal molecules 75 in the first optical compensation plate 70 and the normal line of the first optical compensation plate 70 (that is, the liquid crystal molecules 75 are vertically aligned. The first optical compensator 70 is arranged so that the surface 70 a facing the liquid crystal panel 60. As a result, as indicated by an arrow in FIG. 6, the optical axis of the negative refractive index ellipsoid constituting the first optical compensation plate 70 is different from the optical axis of the positive refractive index ellipsoid constituting the liquid crystal panel 60. Arranged in parallel. Therefore, it is possible to almost completely compensate for the phase difference when observed from all directions. Therefore, light leakage during black display can be prevented, the contrast ratio of the liquid crystal panel can be improved, and the viewing angle characteristics can be improved.

  By the way, when a selection voltage is applied to the nematic liquid crystal of the liquid crystal panel 60, the liquid crystal molecules near the center of the liquid crystal layer are vertically aligned, but the liquid crystal molecules near the alignment film are strongly anchored and are not completely vertically aligned. Therefore, the liquid crystal panel 60 when the selection voltage is applied has a slight phase difference even when observed from the normal direction. This phase difference causes light leakage in black display, and reduces the contrast ratio in the normal direction of the liquid crystal panel 60.

  On the other hand, the discotic liquid crystal molecules of the optical compensators 70 and 80 have a hybrid orientation in which the tilt angle of the optical axis of the refractive index ellipsoid continuously changes in the film thickness direction. Due to this hybrid orientation, each of the optical compensators 70 and 80 has a slow axis and a fast axis when viewed from the normal direction. That is, the alignment regulating directions (X-axis directions) 71 and 81 of the alignment films in the optical compensation plates 70 and 80 are fast axes, and the direction orthogonal to the alignment regulating directions 71 and 81 is a slow axis. As a result, the optical compensator has a phase difference in the normal direction. Accordingly, the inventors of the present application have found that the phase difference in the normal direction of the liquid crystal panel 60 is compensated by the phase difference in the normal direction of the optical compensators 70 and 80.

  FIG. 7 is a graph showing the relationship between the phase difference of the optical compensator and the projection contrast ratio. The contrast ratio of the projection image by the projection display device was calculated by changing the phase difference in the normal direction of each optical compensator. In FIG. 7, the phase difference (retardation) in the normal direction of each optical compensation plate is changed from 5 to 80 nm by changing the thickness of each optical compensation plate. The light emitted to the liquid crystal panel is equivalent to the light from the light source used in a normal projection display device, has the maximum intensity in the normal direction of the liquid crystal panel, and has an intensity of 1 at a polar angle of 12 °. It has the extent of being reduced to / 10.

When the fast axis directions of the first optical compensation plate and the second optical compensation plate are orthogonal to each other, the phase differences in the respective normal directions cancel each other. The phase difference in the direction becomes 0, and the phase difference in the normal direction of the liquid crystal panel cannot be compensated.
Therefore, the first optical compensator and the second optical compensator set to have various phase differences are crossed with respect to the fast axis direction at an angle other than orthogonal, so that the optical compensator as a whole is positioned in the normal direction. A phase difference was generated. Specifically, as shown in FIG. 4, when the absorption axis angle of the light incident side polarizing plate 62 is set to 0 °, the fast axis direction (orientation regulating direction) 71 of the first optical compensation plate 70 is set to 0 °. In the liquid crystal panel 60, the alignment restriction direction 67 of the light incident side substrate is set to 0 °, the alignment restriction direction 68 of the light emission side substrate is set to 90 °, and the absorption axis angle of the light emission side polarizing plate 64 is set to 90 °. 2. The fast axis direction (orientation regulating direction) 81 of the optical compensator 80 was changed within a range of 91 ° to 110 °. When the fast axis direction 81 of the second optical compensator 80 is different from the alignment regulating direction 68 of the light emission side substrate in the liquid crystal panel 60, the phase difference when the liquid crystal panel 60 is observed from an oblique direction. Compensation may be incomplete. Therefore, the fast axis direction 81 of the second optical compensation plate 80 is arranged at an angle at which the contrast ratio of the projected image by the projection display device is maximized. This makes it possible to balance the compensation for the phase difference in the normal direction in the liquid crystal panel and the compensation for the phase difference in a range where the polar angle from the normal direction is small.

  As shown in FIG. 7, when there is no optical compensator (that is, when the phase difference in the normal direction of the optical compensator is zero), the projection contrast ratio is 480. Further, when a conventional optical compensator in which the phase difference in the normal direction of each optical compensator is 40 nm is used, the projection contrast ratio is 930. On the other hand, when the phase difference in the normal direction of each optical compensator is 10 to 30 nm, the projection contrast ratio exceeds 1200. In particular, when the phase difference in the normal direction of each optical compensation plate is 20 nm, the projection contrast ratio exceeds 1500. When the phase difference in the normal direction of each optical compensator is 10 nm, 20 nm, 30 nm, and 40 nm, the angle in the fast axis direction of the second optical compensator that can optimize the projection contrast ratio is 103.5, respectively. °, 97.2 °, 95.6 ° and 95.5 °.

FIG. 8 is an isocontrast ratio curve of the liquid crystal device, FIG. 8A shows a case where the phase difference in the normal direction of each optical compensator is 20 nm, and FIG. 8B shows a normal line of each optical compensator. This is the case where the direction phase difference is 40 nm. In each figure, the horizontal axis and the vertical axis are polar angles with the normal direction of the liquid crystal panel as the center, and the contrast ratio is expressed in common logarithm. The comparison between the case where the phase difference between the normal direction of 20nm and 40nm for the optical compensation plate, it is wide viewing angle in the case of 40nm (e.g., a region where the contrast ratio exceeds 10 ² is wide), but It can be seen that in the polar angle range of 12 °, the contrast ratio is higher in the case of 20 nm. As described above, the incident angle of the light source light with respect to the light modulation means of the projection display device is at most about 12 ° polar angle, and a projection image is constituted by the incident light. Therefore, the projection contrast ratio (1560) of the projection type display device configured using a liquid crystal panel having a phase difference of 20 nm in the normal direction of each optical compensator is a projection type configured using a liquid crystal panel having a phase difference of 40 nm. This is higher than the projection contrast ratio (930) of the display device.

  In the present embodiment, the configuration is such that the phase difference in the normal direction of each optical compensation plate is 10 nm or more and 30 nm or less. According to this configuration, the phase difference in the range where the normal direction and the polar angle of the liquid crystal panel are small can be compensated by each optical compensator. As a result, light leakage during black display can be prevented, and the contrast ratio in a range where the normal direction and polar angle of the liquid crystal panel are small can be improved. Note that the incident angle of the light source light with respect to the light modulation means of the projection display device is at most about 12 ° polar angle, and the projected image is constituted by the incident light. Therefore, the contrast ratio of the projected image can be improved by configuring the projection display device using the liquid crystal device of the present embodiment.

[Second Embodiment]
Next, a liquid crystal device according to a second embodiment of the present invention will be described with reference to FIGS. In the liquid crystal device according to the first embodiment shown in FIG. 4, the first optical compensation plate 70 and the second optical compensation plate 80 are disposed on both sides of the liquid crystal panel 60. On the other hand, the second embodiment shown in FIG. 9 is different in that the first optical compensation plate 70 and the second optical compensation plate 80 are arranged only on the light emitting side of the liquid crystal panel 60. Note that detailed description of portions having the same configuration as in the first embodiment is omitted.

  FIG. 9 is an exploded perspective view of the liquid crystal device according to the second embodiment. In the present embodiment, the second optical compensation plate 80 is disposed outside the substrate on the light emission side of the liquid crystal panel 60, and the first optical compensation plate 70 is disposed outside the second optical compensation plate 80. The alignment regulating direction 81 of the alignment film in the second optical compensator 80 is arranged so as to substantially coincide with the alignment regulating direction 68 of the alignment film in the light emitting side substrate of the liquid crystal panel 60. On the other hand, the orientation regulation direction 71 in the first optical compensation plate 70 is optimized to an angle at which the contrast ratio of the projected image by the projection display device is maximized. Specifically, when the absorption axis angle of the light incident side polarizing plate 62 is set to 0 °, the alignment regulating direction 67 of the light incident side substrate in the liquid crystal panel 60 is 0 °, and the alignment regulating direction 68 of the light emitting side substrate is set. 90 °, the fast axis direction (orientation regulating direction) 71 of the second optical compensation plate 80 is set to 90 °, the absorption axis angle of the light output side polarizing plate 64 is set to 90 °, and the advance of the first optical compensation plate 70 is set. The phase axis direction (orientation regulation direction) 71 was changed within the range of −20 ° to −1 °. Then, the fast axis direction 71 of the first optical compensator 70 is arranged at an angle at which the contrast ratio of the projected image by the projection display device is maximized.

  FIG. 10 is a side sectional view of the optical compensator arranged in a stacked manner. In the present embodiment, the first optical compensation plate 70 is mounted on the surface of the support substrate 78, and the second optical compensation plate 80 is further disposed on the surface of the first optical compensation plate 70. As described above, the first optical compensation plate 70 and the second optical compensation plate 80 are disposed in the liquid crystal device in a state of being mounted on the single support substrate 78.

  FIG. 11 is an explanatory diagram of optical compensation. The second optical compensation plate 80 is disposed so that the surface 80 a having a larger angle between the optical axis 86 of the liquid crystal molecules 85 and the normal line of the second optical compensation plate 80 faces the liquid crystal panel 60. The first optical compensation plate 70 is disposed so that the surface 70 b having a smaller angle formed by the optical axis 76 of the liquid crystal molecules 75 and the normal line of the first optical compensation plate 70 faces the second optical compensation plate 80. Has been.

  As described above, the first optical compensation plate 70 disposed on the light incident side of the liquid crystal panel 60 in the first embodiment shown in FIG. 4 is emitted from the second optical compensation plate 80 in the second embodiment shown in FIG. It is in a state of being translated to the side. Accordingly, as indicated by an arrow in FIG. 11, the light of the refractive index ellipsoid constituting the first optical compensation plate 70 and the second optical compensation plate 80 with respect to the optical axis of the refractive index ellipsoid constituting the liquid crystal panel 60. The axes are arranged in parallel.

  And the phase difference (retardation) of the normal direction of each optical compensation board 70 and 80 was changed to 5-80 nm by changing the thickness of each optical compensation board 70 and 80. FIG. As a result, the relationship between the phase difference in the normal direction of each of the optical compensators 70 and 80 and the projection contrast ratio showed the same tendency as in the first embodiment shown in FIG. That is, the projection contrast ratio without the optical compensator was 480, and the projection contrast ratio was 1010 when the phase difference in the normal direction of each optical compensator was 40 nm. On the other hand, when the phase difference in the normal direction of each optical compensator is 10 to 30 nm, the projection contrast ratio exceeds 1200, and particularly when the phase difference in the normal direction of each optical compensator is 20 nm. The projection contrast ratio reached 1600. When the phase difference in the normal direction of each optical compensator is 10 nm, 20 nm, 30 nm, and 40 nm, the angle in the fast axis direction of the first optical compensator 70 that can optimize the projection contrast ratio is −23, respectively. °, -10.4 °, -8 ° and -7 °.

  As described above, in the second embodiment, similarly to the first embodiment, the phase difference in the normal direction and the polar angle of the liquid crystal panel can be compensated by each optical compensator. As a result, light leakage during black display can be prevented, and the contrast ratio in a range where the normal direction and polar angle of the liquid crystal panel are small can be improved. And the contrast ratio of a projection image can be improved by comprising a projection type display apparatus using the liquid crystal device of this embodiment.

  In the second embodiment, as shown in FIG. 10, the first optical compensation plate 70 and the second optical compensation plate 80 are disposed in the liquid crystal device in a state of being mounted on one support substrate 78. The number of used can be reduced. The support substrate 78 is made of a light-transmitting material having a high thermal conductivity such as sapphire or non-alkali glass. However, the sapphire has a large phase difference, and the alkali-free glass also causes a phase difference due to heat. However, in the second embodiment, since the number of the support substrates 78 used can be reduced, the influence due to the phase difference of the support substrates 78 can be reduced. The above-mentioned projection contrast ratio is generally higher than that of the first embodiment, which is considered to be due to the effect that the influence of the phase difference of the support substrate 78 is reduced. Thereby, light leakage in black display is reduced, and the contrast ratio of the liquid crystal device can be improved. In addition, the attenuation of light by the support substrate 78 can be reduced, and the brightness of the emitted light can be ensured. Furthermore, space can be saved and the manufacturing cost of the liquid crystal device can be reduced.

  In the second embodiment, as shown in FIG. 9, the first optical compensation plate 70 and the second optical compensation plate 80 are disposed only on the light exit side of the liquid crystal panel 60. The optical compensator 80 is disposed away from a light source (not shown), and the amount of light is attenuated by the liquid crystal panel, so that it is not easily affected by heat. Therefore, compared with the first embodiment, thermal degradation of the first optical compensation plate 70 and the second optical compensation plate 80 can be suppressed.

[Projection type display device]
Next, a projection type display device which is a specific example of the electronic apparatus of the present invention will be described with reference to FIG. FIG. 12 is a schematic configuration diagram showing a main part of the projection display device. This projection type display device includes the liquid crystal device according to each of the above-described embodiments as light modulation means.

  In FIG. 12, 810 is a light source, 813 and 814 are dichroic mirrors, 815, 816 and 817 are reflection mirrors, 818 is an incident lens, 819 is a relay lens, 820 is an exit lens, and 822, 823 and 824 are liquid crystal devices of the present invention. 825 is a cross dichroic prism, and 826 is a projection lens. The light source 810 includes a lamp 811 such as a metal halide and a reflector 812 that reflects the light of the lamp.

  The dichroic mirror 813 transmits red light contained in white light from the light source 810 and reflects blue light and green light. The transmitted red light is reflected by the reflection mirror 817 and is incident on the light modulation means 822 for red light. The green light reflected by the dichroic mirror 813 is reflected by the dichroic mirror 814 and is incident on the light modulating means 823 for green light. Further, the blue light reflected by the dichroic mirror 813 passes through the dichroic mirror 814. For blue light, in order to prevent light loss due to a long optical path, a light guide means 821 comprising a relay lens system including an incident lens 818, a relay lens 819, and an exit lens 820 is provided. Blue light is incident on the light modulating means 824 for blue light through the light guiding means 821.

  The three color lights modulated by the respective light modulation means are incident on the cross dichroic prism 825. The cross dichroic prism 825 is formed by bonding four right-angle prisms. A dielectric multilayer film that reflects red light and a dielectric multilayer film that reflects blue light are formed in an X shape at the interface. Yes. These dielectric multilayer films combine the three color lights to form light representing a color image. The synthesized light is projected onto the screen 827 by the projection lens 826 which is a projection optical system, and the image is enlarged and displayed.

In addition, since the light from the lamp 811 in the light source 810 is converted into substantially parallel light by the reflector 812, the incident angle of the light source light with respect to the light modulation means 822, 823, and 824 is about 12 ° at the maximum. A projection image is formed by the incident light.
Here, if the liquid crystal device according to each of the above-described embodiments is used as the light modulators 822, 823, and 824, the contrast ratio can be improved in the normal direction and in a small range of polar angles. Therefore, the contrast ratio of the image projected on the screen 827 can be improved.

  Another specific example of the electronic device of the present invention is a mobile phone. This mobile phone includes the liquid crystal device according to each of the above-described embodiments or modifications thereof in a display unit. Other electronic devices include, for example, an IC card, a video camera, a personal computer, a head mounted display, a fax machine with a display function, a digital camera finder, a portable TV, a DSP device, a PDA, an electronic notebook, and an electric bulletin board. And advertising announcement displays.

  It should be noted that the technical scope of the present invention is not limited to the above-described embodiment, and includes those in which various modifications are made to the above-described embodiment without departing from the spirit of the present invention. For example, in the embodiment, a liquid crystal device including a TFT as a switching element has been described as an example. However, a two-terminal element such as a thin film diode may be employed as the switching element. In the embodiment, the transmissive liquid crystal device has been described as an example. However, the liquid crystal device of the present invention can be applied to a reflective or transflective liquid crystal device. Furthermore, although the three-plate projection display device has been described as an example of the electronic apparatus, the liquid crystal device of the present invention can be applied to a single-plate projection display device or a direct-view display device.

It is an equivalent circuit diagram of a liquid crystal panel. It is explanatory drawing of the planar structure of a liquid crystal panel. It is explanatory drawing of the cross-section of a liquid crystal panel. It is a disassembled perspective view of the liquid crystal device of 1st Embodiment. It is side surface sectional drawing of an optical compensation board. It is explanatory drawing of optical compensation. It is a graph showing the relationship between the phase difference of an optical compensator, and a projection contrast ratio. It is an iso-contrast ratio curve of a liquid crystal device. It is a disassembled perspective view of the liquid crystal device of 2nd Embodiment. It is side surface sectional drawing of the optical compensation board laminated | stacked and arrange | positioned. It is explanatory drawing of optical compensation. It is a block diagram which shows the principal part of a projection type display apparatus. It is a graph which shows the viewing angle dependence of the phase difference of an optical compensator.

Explanation of symbols

  60 liquid crystal panel 70 first optical compensator 71 orientation regulating direction (fast axis direction) 80 second optical compensator 81 orientation regulating direction (fast axis direction) 100 liquid crystal device

In order to solve the above problems, a liquid crystal device of the present invention includes a twisted nematic mode liquid crystal panel in which a liquid crystal layer is sandwiched between a pair of substrates, a light source that irradiates light to the liquid crystal panel, and the light source side of the liquid crystal panel A first optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy disposed outside the substrate, and the outside of the substrate opposite to the light source side of the liquid crystal panel And a second optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy disposed on the first optical compensator, wherein the first optical compensator comprises the liquid crystal molecules The surface with the smaller angle formed by the optical axis and the normal line of the first optical compensator is disposed on the light source side, and the second optical compensator includes the optical axis of the liquid crystal molecules and the second optical compensator. Large angle with normal of optical compensator The first surface is arranged on the light source side, and the first optical compensation plate and the second optical compensation plate each have a phase difference of 10 nm or more and 30 nm or less when viewed from the normal direction. The fast axes when viewed from the respective normal directions are arranged so as to intersect at an angle other than a right angle.
According to this configuration, the phase difference of the liquid crystal layer on one substrate side in the liquid crystal panel is compensated by the first optical compensator, and the phase difference of the liquid crystal layer on the other substrate side is compensated by the second optical compensator. The Then, by causing the fast axes of the first optical compensation plate and the second optical compensation plate to intersect at a non-perpendicular angle, it becomes possible to generate a phase difference in the normal direction as the entire optical compensation plate. The normal phase difference in the panel can be compensated. Therefore, a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

In addition, a twisted nematic mode liquid crystal panel in which a liquid crystal layer is sandwiched between a pair of substrates, a light source that irradiates light to the liquid crystal panel, and negative refraction disposed outside the substrate on the light source side of the liquid crystal panel A first optical compensator obtained by hybrid alignment of liquid crystal molecules exhibiting refractive index anisotropy and a liquid crystal molecule exhibiting negative refractive index anisotropy disposed outside the first optical compensator are hybrid aligned. The first optical compensation plate has a small angle formed between the optical axis of the liquid crystal molecules and the normal line of the first optical compensation plate. The second optical compensator is disposed on the light source side, and the surface of the second optical compensator having the larger angle formed by the optical axis of the liquid crystal molecule and the normal line of the second optical compensator is the light source side. And the optical axis of the liquid crystal molecule A surface having a smaller angle with the normal direction of the second optical compensation plate is disposed to face the first optical compensation plate, and the first optical compensation plate and the second optical compensation are arranged. The plates are set so that the phase difference when viewed from the normal direction is 10 nm or more and 30 nm or less, and the fast axes when viewed from the respective normal directions intersect at an angle that is not perpendicular. It is arranged.
Also with this configuration, the phase difference of the liquid crystal layer on one substrate side in the liquid crystal panel is compensated by the first optical compensator, and the phase difference of the liquid crystal layer on the other substrate side is compensated by the second optical compensator. . Further, it becomes possible to compensate for the phase difference in the normal direction in the liquid crystal panel, and a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

A liquid crystal panel of a twisted nematic mode in which a liquid crystal layer is sandwiched between a pair of substrates; a light source that irradiates light to the liquid crystal panel; and an outer side of the substrate opposite to the light source side of the liquid crystal panel. A second optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy, and liquid crystal molecules exhibiting negative refractive index anisotropy disposed outside the second optical compensator A first optical compensator formed by hybrid orientation of the liquid crystal device, wherein the second optical compensator is an optical axis of the liquid crystal molecules and a normal line of the first optical compensator. A surface having a larger angle is disposed on the light source side, and the first optical compensation plate has a smaller angle formed by the optical axis of the liquid crystal molecule and the normal line of the second optical compensation plate. Is disposed on the light source side and the surface is the second The first optical compensation plate and the second optical compensation plate are arranged opposite to the optical compensation plate, and the phase difference when viewed from the normal direction is set to 10 nm or more and 30 nm or less. The fast axes when viewed from the respective normal directions are arranged so as to intersect at a non-right angle.
According to this configuration, since the first optical compensation plate and the second optical compensation plate are arranged away from the light source, the heat from the light source is reduced by the amount far from the light source and the amount of light reduced by the aperture ratio of the liquid crystal device. Deterioration due to influence can be suppressed.

In order to solve the above problems, a liquid crystal device of the present invention includes a twisted nematic mode liquid crystal panel in which a liquid crystal layer is sandwiched between a pair of substrates, a light source that irradiates light to the liquid crystal panel, and the light source side of the liquid crystal panel A first optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy disposed outside the substrate, and the outside of the substrate opposite to the light source side of the liquid crystal panel And a second optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy disposed on the first optical compensator, wherein the first optical compensator comprises the liquid crystal molecules The surface with the smaller angle formed by the optical axis and the normal line of the first optical compensator is disposed on the light source side, and the second optical compensator includes the optical axis of the liquid crystal molecules and the second optical compensator. Large angle with normal of optical compensator The first surface is arranged on the light source side, and the first optical compensation plate and the second optical compensation plate each have a phase difference of 10 nm or more and 30 nm or less when viewed from the normal direction. The fast axes when viewed from the respective normal directions are arranged so as to intersect at an angle other than a right angle.
According to this configuration, the phase difference of the liquid crystal layer on one substrate side in the liquid crystal panel is compensated by the first optical compensator, and the phase difference of the liquid crystal layer on the other substrate side is compensated by the second optical compensator. The Then, by causing the fast axes of the first optical compensation plate and the second optical compensation plate to intersect at a non-perpendicular angle, it becomes possible to generate a phase difference in the normal direction as the entire optical compensation plate. The normal phase difference in the panel can be compensated. Therefore, a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

In addition, a twisted nematic mode liquid crystal panel in which a liquid crystal layer is sandwiched between a pair of substrates, a light source that irradiates light to the liquid crystal panel, and negative refraction disposed outside the substrate on the light source side of the liquid crystal panel A first optical compensator obtained by hybrid alignment of liquid crystal molecules exhibiting refractive index anisotropy and a liquid crystal molecule exhibiting negative refractive index anisotropy disposed outside the first optical compensator are hybrid aligned. The first optical compensation plate has a small angle formed between the optical axis of the liquid crystal molecules and the normal line of the first optical compensation plate. The second optical compensator is disposed on the light source side, and the surface of the second optical compensator having the larger angle formed by the optical axis of the liquid crystal molecule and the normal line of the second optical compensator is the light source side. And the optical axis of the liquid crystal molecule A surface having a smaller angle with the normal direction of the second optical compensation plate is disposed to face the first optical compensation plate, and the first optical compensation plate and the second optical compensation are arranged. The plates are set so that the phase difference when viewed from the normal direction is 10 nm or more and 30 nm or less, and the fast axes when viewed from the respective normal directions intersect at an angle that is not perpendicular. It is arranged.
Also with this configuration, the phase difference of the liquid crystal layer on one substrate side in the liquid crystal panel is compensated by the first optical compensator, and the phase difference of the liquid crystal layer on the other substrate side is compensated by the second optical compensator. . Further, it becomes possible to compensate for the phase difference in the normal direction in the liquid crystal panel, and a high contrast ratio can be obtained within the range of the incident angle of the light source light with respect to the light modulation means of the projection display device.

A liquid crystal panel of a twisted nematic mode in which a liquid crystal layer is sandwiched between a pair of substrates; a light source that irradiates light to the liquid crystal panel; and an outer side of the substrate opposite to the light source side of the liquid crystal panel. A second optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy, and liquid crystal molecules exhibiting negative refractive index anisotropy disposed outside the second optical compensator A first optical compensator formed by hybrid orientation of the liquid crystal device, wherein the second optical compensator is an optical axis of the liquid crystal molecules and a normal line of the second optical compensator. A surface having a larger angle is disposed on the light source side, and the first optical compensator is a surface having a smaller angle formed by the optical axis of the liquid crystal molecule and the normal line of the first optical compensator. Is disposed on the light source side and the surface is the second The first optical compensation plate and the second optical compensation plate are arranged opposite to the optical compensation plate, and the phase difference when viewed from the normal direction is set to 10 nm or more and 30 nm or less. The fast axes when viewed from the respective normal directions are arranged so as to intersect at a non-right angle.
According to this configuration, since the first optical compensation plate and the second optical compensation plate are arranged away from the light source, the heat from the light source is reduced by the amount far from the light source and the amount of light reduced by the aperture ratio of the liquid crystal device. Deterioration due to influence can be suppressed.

Claims (7)

A liquid crystal device comprising a liquid crystal panel having a liquid crystal layer sandwiched between a pair of substrates, the liquid crystal panel operating in a twisted nematic mode,
An optical compensator formed by hybrid alignment of liquid crystal molecules exhibiting negative refractive index anisotropy is disposed outside at least one substrate in the liquid crystal panel,
A liquid crystal device, wherein a phase difference in a normal direction of the optical compensator is 10 nm or more and 30 nm or less. The first optical compensation plate is arranged outside one of the pair of substrates, and the second optical compensation plate is arranged outside the other substrate of the pair of substrates,
The first optical compensation plate and the second optical compensation plate are arranged so that the fast axes when viewed from the respective normal directions intersect at an angle that is not perpendicular. Item 2. A liquid crystal device according to item 1. The first optical compensation plate is disposed outside one of the pair of substrates, and the second optical compensation plate is disposed outside the first optical compensation plate,
The second optical compensator has a surface having a smaller angle formed between the optical axis of the liquid crystal molecule and the normal direction of the second optical compensator facing the first optical compensator. Arranged,
The first optical compensation plate and the second optical compensation plate are arranged so that the fast axes when viewed from the respective normal directions intersect at an angle that is not perpendicular. Item 2. A liquid crystal device according to item 1. 4. The liquid crystal device according to claim 3, wherein the first optical compensation plate and the second optical compensation plate are disposed outside the substrate on the light emission side of the pair of substrates. 5. The fast axis of any one of the first optical compensation plate and the second optical compensation plate is parallel to the orientation regulating direction of the substrate corresponding to the optical compensation plate. The liquid crystal device according to claim 2, wherein the liquid crystal device is disposed in a liquid crystal device. The intersection angle between the fast axis of the first optical compensator and the fast axis of the second optical compensator is in the range of 91 ° to 110 °, and the projection contrast ratio of the liquid crystal device is 6. The liquid crystal device according to claim 2, wherein the angle is a maximum angle. 7. A projection display device comprising the liquid crystal device according to claim 1 as light modulation means.

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