Patent Application
20210165262
This application claims priority to Japanese application No. 2019-215093, filed on Nov. 28, 2019 and incorporated herein by reference.
The present invention relates to a phase difference compensation element, liquid crystal display device, and a projection image display device.
Recently, optical compensation techniques using phase difference compensation elements have been used for improving contrast and view angles of liquid crystal display devices. Example of such techniques include compensation of black level reduction in vertically aligned liquid crystal molecules. Moreover, proposed are an optical compensation method where a phase difference compensation element, such as crystal, is disposed to be parallel to a main plane of a liquid crystal panel to compensate a retardance due to pretilt angles of liquid crystal molecules, or retardance due to birefringence caused by oblique angle incident light, and a method where an organic material having birefringence, such as a polymer film, is disposed to be parallel to a main plane of a liquid crystal panel to perform optical compensation (see, for example, Japanese Patent Application Laid-Open (JP-A) No. 2005-172984, and Japanese Patent (JP-B) Nos. 4661510 and 4566275).
In a case where a method for processing monocrystal as a phase difference compensation element, in order to perform optical compensation considering particularly pretilt angles of liquid crystal molecules, it is necessary to cut the monocrystal out with a predetermined angle relative to a crystal axis thereof, and extremely high accuracy in cut-out of the material or polishing is important.
Therefore, a cost of such a phase difference compensation element is high. Moreover, it is not easy to control a crystal axis in a stretched film.
Therefore, proposed is a method where a phase difference compensation element itself is arranged to be tilted with respect to a main plane of a liquid crystal panel (see, for example, JP-A Nos. 2006-11298 and 2009-229804).
0.5<A/B<1.5 Formula (1)
0.5<A/B<1.5 Formula (1)
a first optical anisotropic layer that is a birefringent body including an inorganic material, where an optic axis of the birefringent body is orthogonal to the transparent substrate; and
0.5<A/B<1.5 Formula (1)
Embodiments of the present technology will be described in details according to the following order with reference to drawings.
The prior art of phase difference compensation elements is as described earlier. However, there is a concern that an internal space of a projector, which has been downsizing, may not be sufficient to arrange a phase difference compensation element to be tilted with respect to a main plane of a liquid crystal panel. Moreover, the phase difference compensation element tends to be deteriorated by heat or light of high brightness and high output, and therefore there is a problem in durability of the phase difference compensation element.
Accordingly, there is currently a need for a phase difference compensation element that can significantly reduce a space to be disposed, and has excellent durability.
The present invention aims to solve the above-described various problems existing in the art, and to achieve the following object. Specifically, the present invention has an object to provide a phase difference compensation element, which can significantly reduce a space to be disposed, and has excellent durability, a liquid crystal display device using the phase difference compensation element, and a projection image display device using the liquid crystal display device.
The present invention can solve the above-described various problems existing in the art, and can provide a phase difference compensation element, which can significantly reduce a space to be disposed, and has excellent durability, a liquid crystal display device using the phase difference compensation element, and a projection image display device using the liquid crystal display device.
The phase difference compensation element according to the present embodiment is a phase difference compensation element configured to compensate a residual retardance of a liquid crystal panel.
The phase difference compensation element includes a transparent substrate, a first optical anisotropic layer, and a second optical anisotropic layer.
In the present invention, the following formula (1) is satisfied:
0.5<A/B<1.5 Formula (1)
In the formula above, A is an average retardance of the phase difference compensation element with incident light tilted within the range of 5° towards a pretilt direction of liquid crystal molecules, i.e., an average retardance of the phase difference compensation element of incident light tilted by ±5° towards a pretilt direction of liquid crystal molecules of the liquid crystal panel disposed to face the phase difference compensation element, when a direction orthogonal to a main plane of the phase difference compensation element is determined as 0°; and B is an average retardance of the liquid crystal panel with incident light tilted within the range of 5° towards the pretilt direction of the liquid crystal molecules of the liquid crystal panel, i.e., an average retardance of the liquid crystal panel with incident light tilted by ±5° towards the pretilt direction of liquid crystal molecules of the liquid crystal panel, when a direction orthogonal to a main plane of the liquid crystal panel is determined as 0°.
Since the formula (1) is satisfied, a residual retardance of the liquid crystal panel can be compensated without tilting the phase difference compensation element with respect to the liquid crystal panel. Therefore, a space in which the phase difference compensation element is disposed can be significantly reduced.
In the present specification, the phrase “pretilt direction of liquid crystal molecules” means a direction along which liquid crystal molecules are pretilted in the liquid crystal panel disposed to face the phase difference compensation element (i.e. the direction for aligning the liquid crystal molecules). Moreover, the phrase “pretilt direction of liquid crystal molecules” with respect to the phase difference compensation element means the pretilt direction of the liquid crystal molecules in the liquid crystal panel to which the phase difference compensation element is disposed to face. For example, the pretilt direction of the liquid crystal molecules can be represented as the direction indicated with the symbol L in
Note that, the average retardance is an average value of retardance values obtained by measuring with incident light tilted within the range of 5° towards the pretilt direction of the liquid crystal molecules per 1° (i.e., tilted by −5°, −4°, −3°, −2°, −1°, 0°, 1°, 2°, 3°, 4°, and 5°.
Moreover, the retardance can be measured by a retardation measuring device RETS-100, available from Otsuka Electronic Co., Ltd.
The average retardance of the phase difference compensation element with incident light tilted within the range of 5 20 towards the pretilt direction of the liquid crystal molecules of the liquid crystal panel may be appropriately selected depending on the average retardance of the liquid crystal panel. For example, the average retardance of the phase difference compensation element is 1 nm or greater but 10 nm or less.
The average retardance of the liquid crystal panel with incident light tilted in the range of 5° towards the pretilt direction of the liquid crystal molecules therein is not particularly limited and may be appropriately selected depending on the intended purpose. For example, the average retardance of the liquid crystal panel is 1 nm or greater but 10 nm or less.
The first optical anisotropic layer includes an inorganic material.
The second optical anisotropic layer is a birefringent layer obtained by depositing an inorganic material.
Since the phase difference compensation element includes inorganic materials as constitutional materials, the phase difference compensation element has excellent durability.
The transparent substrate 11 is transparent to light of a wavelength range for use. The transparent substrate 11 has a high transmittance to light of a wavelength range for use. For example, a material of the transparent substrate 11 is an inorganic material. Examples of the inorganic material include glass, quartz, crystal, and sapphire. A shape of the transparent substrate 11 is typically a square, but the shape thereof is appropriately selected depending on the intended purpose. For example, a thickness of the transparent substrate 11 is preferably 0.1 mm or greater but 3.0 mm or less.
For example, the first optical anisotropic layer 15A is disposed to be in contact with a plane of the transparent substrate 11 opposite to the side of the second optical anisotropic layer 13.
The first optical anisotropic layer 15A includes an inorganic material.
The first optical anisotropic layer 15A functions as a C plate.
In the present specification, the C-plate is a birefringent body an optic axis of which is orthogonal to a plane of the transparent substrate. The optic axis is a direction along which birefringence does not occur, and a direction with which a phase difference (retardance) is 0.
For example, the antireflection layer 15B is optionally disposed to be in contact with a plane of the protective layer 14 opposite to the side of the second optical anisotropic layer 13.
For example, the first optical anisotropic layer 15A has an antireflection function in a desired wavelength range for use.
For example, the antireflection layer 15B has an antireflection function in a desired wavelength range for use.
The larger difference between the refractive index of the first oxide film 151 and the refractive index of the second oxide film 152 is more preferable. In view of availability of materials and film formability, the difference is preferably 0.5 or greater but 1.0 or less. The refractive index is, for example, a refractive index at a wavelength of 550 nm.
For example, the inorganic oxide films of the first antireflection layer 15A and the inorganic oxide films of the second antireflection layer 15B are each an oxide film including at least one selected from the group consisting of Ti, Si, Ta, Al, Ce, Zr, Nb, and Hf.
For example, the first optical anisotropic layer 15A and the antireflection layer 15B are each a multiple film where first oxide films 151 formed of niobium oxide (refractive index at wavelength of 550 nm: 2.3) having a relatively high refractive index, and second oxide films 152 formed of silicon oxide (refractive index at wavelength of 550 nm: 1.5) having a relatively low refractive index are alternately laminated.
Note that, the oxides constituting the first optical anisotropic layer 15A or the antireflection layer 15B may be nonstoichiometric. Specifically, an atomic ratio of constitutional elements of the oxide is not necessarily a simple whole number ratio. When an oxide film is formed by sputtering etc., the formed oxide is often nonstoichiometric. Moreover, an elemental ratio of the oxide of the formed film cannot be easily measured stably, thus it is difficult to determine an elemental ratio of the oxide.
Considering the oxide being nonstoichiometric, for example, the oxide including Nb is represented by the following formula.
NbOX (0<X≤2.5)
For example, the oxide including Si is represented by the following formula.
SiOY (0<Y<2)
A thickness of the first optical anisotropic layer 15A and a thickness of the antireflection layer 15B are not particularly limited and may be appropriately selected depending on the intended purpose. For example, the thickness thereof is 250 nm or greater but 2,300 nm or less. In the present specification, a thickness of a layer (film thickness) means an average film thickness.
The matching layer 12 is, for example, a multiple layer film where two or more inorganic oxide films having mutually different refractive indexes are laminated. The matching layer 12 is disposed between the transparent substrate 11 and the second optical anisotropic layer 13. The matching layer 12 is designed to cancel interface reflection light by interference, to thereby prevent reflection at an interface between the transparent substrate 11 and the second optical anisotropic layer 13. Specifically, the matching layer 12 is designed to cancel out reflected light at an interface between the transparent substrate 11 and the matching layer 12 and reflected light at an interference between the matching layer 12 and the second optical anisotropic layer 13.
For example, the matching layer 12 is formed of an oxide film including at least one selected from the group consisting of Ti, Si, Ta, Al, Ce, Zr, Nb, and Hf.
Note that, the oxides constituting the matching layer 12 may be nonstoichiometric. Specifically, an atomic ratio of constitutional elements of the oxide is not necessarily a simple whole number ratio. When an oxide film is formed by sputtering etc., the formed oxide is often nonstoichiometric.
A thickness of the matching layer 12 is not particularly limited and may be appropriately selected depending on the intended purpose. For example, the thickness of the matching layer 12 is 140 nm or greater but 240 nm or less.
The second optical anisotropic layer 13 is a birefringent layer obtained by depositing an inorganic material.
An angle formed between a direction along which the inorganic material is deposited in the birefringent layer and a surface of the transparent substrate is other than 90°.
For example, the birefringent layer includes an oblique angle vapor deposition film.
In the phase difference compensation element 10 illustrated in
The birefringent layer includes, for example, a plurality of birefringent films each formed of an inorganic material. The inorganic material is preferably a dielectric material. Examples of the inorganic material include an oxide including at least one selected from the group consisting of Si, Nb, Zr, Ti, La, Ta, Al, Hf, and Ce.
The inorganic material is preferably tantalum oxide (e.g., Ta2O5).
For example, the plurality of birefringent films constituting the birefringent layer may be formed of the same material or composition.
A retardance of each of the birefringent films is not particularly limited and may be appropriately selected depending on a liquid crystal panel for use.
A thickness of each birefringent film constituting the birefringent layer may be appropriately selected depending on a retardance to be compensate.
A thickness of the whole second optical anisotropic layer including the birefringent films is appropriately selected depending on a retardance to compensate. For example, the thickness of the second optical anisotropic layer is 50 nm or greater but 500 nm or less.
For example, the second optical anisotropic layer 13 has a structure where a plurality of the above-described birefringent films are deposited.
Each birefringent film is formed by depositing in the direction slanting relative to the normal line S, and an angle formed between the film formation direction of an inorganic material constituting the birefringent film and a surface of the transparent substrate is not 90°.
A method creating a state where an angle formed between the film formation direction of the inorganic material and the surface of the transparent substrate is not 90° is, for example, preferably a method where a deposition source is arranged in a position slanted relative to the normal line S and an oblique angle vapor deposition film is formed by oblique angle vapor deposition from the deposition source. When a birefringent layer is formed by performing oblique angle vapor deposition multiple times, the oblique angle vapor deposition is repeated with varying the deposition angle to thereby obtain a final birefringent layer.
As illustrated in
During the deposition process P1, as illustrated in
The protective layer 14 is formed of a dielectric film, and is disposed to be in contact with the oblique angle vapor deposition film of the second optical anisotropic layer 13. The presence of the protective layer 14 can prevent warping of the phase difference compensation element 10, and can improve humidity resistance of the oblique angle vapor deposition film.
The dielectric material of the protective layer 14 is not particularly limited and may be appropriately selected depending on the intended purpose, as long as the dielectric material can adjust stress applied to the phase difference compensation element 10, and can exhibit an effect of improving humidity resistance. Examples of such a dielectric material include oxide including at least one selected from the group consisting of Si, Ta, Ti, Al, Nb, and La, and MgF2.
A thickness of the protective layer 14 is not particularly limited and may be appropriately selected depending on the intended purpose. The thickness of the protective layer 14 is, for example, 10 nm or greater but 100 nm or less.
Next, a production method of the phase difference compensation element according to the present embodiment will be described. As a specific example of the production method of the phase difference compensation element, the production method of the phase difference compensation element having the configuration example illustrated in
First, a transparent substrate 11 is provided in Step S1.
Next, a matching layer 12, in which inorganic oxide films are laminated, is formed on the transparent substrate in order to prevent reflection at an interface between the second optical anisotropic layer 13 and the transparent substrate 11 in Step S2.
Next, a first optical anisotropic layer 15A [back antireflection (AR) layer] is formed on a surface of the transparent substrate 11, on which the matching layer 12 is not formed, in Step S3.
Next, a second optical anisotropic layer 13 is formed on the matching layer 12 by oblique angle vapor deposition in Step S4. As illustrated in
Next, the second optical anisotropic layer 13 is subjected to annealing at a temperature of 200° C. or higher but 600° C. or lower in Step S5. The second optical anisotropic layer 13 is subjected to annealing more preferably at a temperature of 300° C. or higher but 500° C. or lower, further more preferably 400° C. or higher but 500° C. or lower. As a result, properties of the second optical anisotropic layer 13 can be stabilized.
Next, a protective layer 14 is formed on the second optical anisotropic layer 13 in Step S6. When a film of SiO2 is formed as the protective layer 14, for example, tetraethoxysilane (TEOS) gas and O2 are preferably used as a material of SiO2, and a plasma CVD device is preferably used.
A SiO2 CVD film formed by a plasma CVD device uses a vaporized material gas for film formation different from physical vapor deposition, such as sputtering. Therefore, TEOS gas is relatively easily penetrated into gaps in the column structure to further improve adhesion of the protective layer 14 to the second optical anisotropic layer 13.
Next, a second antireflection layer 15B (surface AR layer) is formed on the protective layer 14 in Step S7.
Finally, scribe cutting is performed to obtain a size matched to a specification in Step S8.
According to the production method as described above, an optical element having excellent durability against light of high luminance and high output emitted from a laser light source etc. can be obtained.
The liquid crystal display device according to the present embodiment includes a liquid crystal panel and the above-described phase difference compensation element.
For example, the liquid crystal panel and the phase difference compensation element are disposed in the liquid crystal display device in a manner that a main plane of the liquid crystal panel is parallel to a main plane of the phase difference compensation element. Because of the arrangement as described, a space where the phase difference compensation element is disposed can be significantly reduced compared to a case where the phase difference compensation element is disposed to be oblique to the liquid crystal panel. In the present specification, “being parallel to” does not mean complete parallel, and the main plane of the phase difference compensation element may be tilted from the main plane of the liquid crystal panel as long as the space to be arranged can be significantly reduced. For example, the main plane of the phase difference compensation element may be tilted from the main plane of the liquid crystal panel in the range of 2° or less.
The liquid crystal display device includes at least a liquid crystal panel and the phase difference compensation element, and may further include other members, such as a first polarizing plate and a second polarizing plate.
The liquid crystal panel is not particularly limited. For example, the liquid crystal panel includes a substrate, and a VA-mode liquid crystal layer including liquid crystal molecules having pretilt relative to the orthogonal direction to the main surface of the substrate, and modulates the entered luminous flux entered. The VA-mode (vertical alignment mode) means a system where liquid crystal molecules aligned vertical (or with pretilt) to the substrate are moved using a longitudinal electric field in a vertical direction.
A first polarizing plate is a polarizing plate disposed at the inlet side of the liquid crystal panel, and a second polarizing plate is a polarizing plate disposed at the outlet side of the liquid crystal panel. The first polarizing plate and the second polarizing plate are preferably inorganic polarizing plates in view of durability.
A typical optical system will be described with reference to
The projection image display device according to the present embodiment includes a light source configured to emit light, a projection optical system configured to project modulated light, and the above-described liquid crystal display device.
The liquid crystal display device is disposed on an optical path between the light source and the projection optical system. The projection image display device is suitably used for projectors, such as a liquid crystal projector, and a liquid crystal on silicon (LCOS) projector.
Alight source is not particularly limited and may be appropriately selected depending on the intended purpose, as long as the light source is a member that emits light. For example, a laser light source that emits light of high luminance and high output can be used.
The wavelength of the laser light source is, for example, 455 nm.
The projection optical system is not particularly limited and may be appropriately selected depending on the intended purpose, as long as the projection optical system is a member for projecting modulated light. Examples of the projection optical system include a projection lens configured to project the modulated light onto a screen.
The projection image display device having the above-described structure can significantly reduce a space where the phase difference compensation element is disposed. Therefore, a small projection image display device can be constructed.
FIG.8 is a schematic view illustrating one example of the structure of the projection image display device according to the present embodiment. The projection image display device 115A is a so-called 3-panel liquid crystal projector, which displays a color image using 3 liquid crystal panels of red, green, and blue. As illustrated in
The light source 102 is configured to emit light-source light (white light) L including blue light LB, green light LG, and red light LR for forming an image display. Examples of the light source 102 include a halogen lamp, a metal halide lamp, and a xenon lamp.
The dichroic mirror 103 has a function of separating the light-source light L into blue light LB and light of other colors LRG. The dichroic mirror 104 has a function of separating the light passed LRG through the dichroic mirror 103 into red light LR and green light LG. The total reflection mirror 105 reflects the blue light LB separated by the dichroic mirror 103 towards the polarization beam splitter 106B.
The polarization beam splitters 106R, 106G, and 106B are prism-type polarized light separators disposed on optical paths of the red light LR, the green light LG, and the blue light LB, respectively. The polarization beam splitters 106R, 106G, and 106B have polarized light splitting surfaces 107R, 107G, and 107B, respectively. The polarization beam splitters 106R, 106G, and 106B have a function of splitting the entered light of each color into two polarized light components orthogonal to each other at the polarized light splitting surfaces 107R, 107G, and 107B, respectively. The polarized light splitting surfaces 107R, 107G, and 107B reflect one polarized light component (e.g., an S-polarized light component) and transmit the other polarized light component (e.g., a P-polarized light component).
The color light of the certain polarized light component (e.g., an S-polarized light component) separated by each of the polarized light splitting surfaces 107R, 107G, and 107B of the polarization beam splitters 106R, 106G, and 106B enters each of the liquid crystal display devices 101R, 101G, and 101B. The liquid crystal display devices 101R, 101G, and 101B are driven by driving voltage applied according to an image signal to modulate the incident light, and also have a function of reflecting the modulated light to the polarization beam splitters 106R, 106G, and 106B.
The phase difference compensation elements 10 and the 1/4-wave plates 113R, 113G, and 113B are disposed between the polarization beam splitters 106R, 106G, and 106B, and the liquid crystal panels of the liquid crystal display devices 101R, 101G, and 101B, respectively. The 1/4-wave plates 113R, 113G, and 113B each function as a 1/2-wave plate as the 1/4-wave plates 113R, 113G, and 113B allow to pass the light twice, i.e., when the light enters the liquid crystal panel, and when the light is emitted from the liquid crystal panel (for example, converting an S-polarized light component into a P-polarized light component). Moreover, the 1/4-wave plates 113R, 113G, and 113B have a function of suppressing a reduction of the contrast owing to the incident light angle dependency the polarization beam splitters 106R, 106G, and 106B have. The phase difference compensation elements 10 have a function of compensating the residual phase difference of the liquid crystal panels constituting the liquid crystal display devices 101R, 101G, and 101B, respectively. In one aspect, the phase difference compensation element 10 is the phase difference compensation element according to the present embodiment.
The beam-combining prism 108 has a function of combining color light of the certain polarized light components (e.g., P-polarized light components) emitted from the liquid crystal display devices 101R, 101G, and 101B and passed through the polarization beam splitter 106R, 106G, and 106B. The projection lens 109 has a function of projecting the synthesized light emitted from the beam-combining prism 108 towards the screen 110.
Next, an operation of the projection image display device 115A constituted in the above-described manner will be described.
First, white light L emitted from the light source 102 is split into blue light LB and other color light (red light and green light) LRB by a function of the dichroic mirror 103. The blue light LB is reflected to the polarization beam splitter 106B by a function of the total reflection mirror 105.
Meanwhile, other color light (red light and green light) LRG is further split into red light LR and green light LG by a function of the dichroic mirror 104. The split red light LR and green light LG enters the polarization beam splitters 106R and 106G, respectively.
The polarization beam splitters 106R, 106G, and 106B are configured to split the entered color light into two polarized light components orthogonal to each other by the polarized light splitting surfaces 107R, 107G, and 107B, respectively. The polarized light splitting surfaces 107R, 107G, and 107B reflect one polarized light component (e.g., an S-polarized light component) to the liquid crystal display devices 101R, 101G, and 101B. The liquid crystal display devices 101R, 101G, and 101B are driven by driving voltage applied according to an image signal, and modulate color light of the entered certain polarized light by pixel.
The liquid crystal display devices 101R, 101G, and 101B reflect the modulated color light to the polarization beam splitters 106R, 106G, and 106B, respectively. The polarization beam splitters 106R, 106G, and 106B only pass through the certain polarized light component (e.g., P-polarized light components) within the reflected light (modulated light) from the liquid crystal display devices 101R, 101G, and 101B, and emit towards the beam-combining prism 108.
The beam-combining prism 108 synthesize the color light of the certain polarized light components passed through the polarization beam splitters 106R, 106G, and 106B, and emits towards the projection lens 109. The projection lens 109 projects the synthesized light emitted from the beam-combining prism 108 to the screen 110. As a result, an image corresponding to the light modulated by the liquid crystal display devices 101R, 101G, and 101B is projected on the screen 110, and a desired image display is achieved.
Specific example of the present invention will be described hereinafter. However, the present invention is not limited to the example below. Note that, formed films are described as a SiO2 film and a Nb2O5 film for the matter of convenience, but the films are highly likely nonstoichiometric.
On one surface of a glass substrate (average thickness: 0.7 mm), Nb2O5 and SiO2 were alternately deposited by sputtering to form 5 layers in total, to thereby form a matching layer.
On the other surface of the glass substrate, subsequently, Nb2O5 and SiO2 were alternately deposited by sputtering to form 40 layers in total, to thereby form a first optical anisotropic layer. The layer structure was designed in a manner that retardance given to tilted incident light that was tilted by 15° from the direction orthogonal to the surface of the glass substrate was 15 nm. Moreover, the first optical anisotropic layer was imparted with an antireflection function. An optic axis of the obtained first optical anisotropic layer was orthogonal to the planar direction. Specifically, the first optical anisotropic layer functioned as a C-plate.
Subsequently, a deposition source was arranged in a position slanted relative to a normal line of the glass substrate by 70°, and oblique angle vapor deposition was performed using a deposition material prepared by adding TiO2 to Ta2O5, to thereby form a second optical anisotropic layer. As illustrated in
After the vapor deposition, annealing was performed at 400° C. to stabilize the properties of the second optical anisotropic layer. After the annealing, a SiO2 film was formed by plasma CVD using tetraethoxysilane (TEOS) gas and O2.
Subsequently, Nb2O5 and SiO2 were alternately deposited by sputtering to form 7 layers in total to thereby form an antireflection layer. As described above, a phase difference compensation element was produced.
A retardance of each of the produced phase difference compensation elements was measured with incident light tilted per 1° in the range of ±5° towards the pretilt direction of the liquid crystals, and an average values of the measured retardance values was calculated.
A liquid crystal panel whose average retardance with incident light tilted within the range of 5° towards a pretilt direction of liquid crystal molecules therein was 5 nm and each of the phase difference compensation elements (9 samples) of Example 1 were mounted in a liquid crystal projector, and contrast thereof was measured. The phase difference compensation element was disposed to be parallel to a main plane of the liquid crystal panel.
Note that, the contrast is an average value of values obtained by measuring at 9 points by means of an illuminometer T-10 available from KONICA MINOLTA, INC.
A liquid crystal panel whose average retardance with incident light tilted within the range of 5° towards a pretilt direction of liquid crystal molecules therein was 4 nm and each of the phase difference compensation elements (9 samples) of Example 1 were mounted in a liquid crystal projector, and contrast thereof was measured in the same manner as in Example 1.
The phase difference compensation element of the present invention can be suitably applied for a small projection image display device, because the phase difference compensation element can significantly reduce a space to be disposed, and has excellent durability.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2019-215093 | Nov 2019 | JP | national |
