US20120280953A1 - Display device - Google Patents
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- US20120280953A1 US20120280953A1 US13/461,805 US201213461805A US2012280953A1 US 20120280953 A1 US20120280953 A1 US 20120280953A1 US 201213461805 A US201213461805 A US 201213461805A US 2012280953 A1 US2012280953 A1 US 2012280953A1
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- compensation film
- display device
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/133524—Light-guides, e.g. fibre-optic bundles, louvered or jalousie light-guides
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/0001—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings specially adapted for lighting devices or systems
- G02B6/0011—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings specially adapted for lighting devices or systems the light guides being planar or of plate-like form
- G02B6/0033—Means for improving the coupling-out of light from the light guide
- G02B6/005—Means for improving the coupling-out of light from the light guide provided by one optical element, or plurality thereof, placed on the light output side of the light guide
- G02B6/0053—Prismatic sheet or layer; Brightness enhancement element, sheet or layer
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1334—Constructional arrangements; Manufacturing methods based on polymer dispersed liquid crystals, e.g. microencapsulated liquid crystals
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/13356—Structural association of cells with optical devices, e.g. polarisers or reflectors characterised by the placement of the optical elements
- G02F1/133562—Structural association of cells with optical devices, e.g. polarisers or reflectors characterised by the placement of the optical elements on the viewer side
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/1336—Illuminating devices
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/137—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/13793—Blue phases
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- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/137—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/139—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent
- G02F1/1393—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on orientation effects in which the liquid crystal remains transparent the birefringence of the liquid crystal being electrically controlled, e.g. ECB-, DAP-, HAN-, PI-LC cells
Definitions
- the invention relates to a display device, and more particularly to a liquid crystal display device.
- blue phase liquid crystal displays characterized by fast response speed have been developed in the industry pertinent to displays.
- a positive blue phase liquid crystal material is applied, a transverse electric field is required for operation, such that the positive blue phase liquid crystal material can function as a light valve.
- positive blue phase liquid crystal molecules in the blue phase LCD are driven by adopting the electrode design of an in-plane switching (IPS) display module.
- IPS in-plane switching
- the invention provides a display device capable of solving issues of low transmittance and high driving voltage when blue phase liquid crystals are applied in a conventional IPS display module.
- the invention provides a display device including a light source module, a display module, a turning optical film, a first compensation film, and a second compensation film.
- the light source module generates a directional light.
- the display module is disposed above the light source module, and the display module includes a first substrate, a second substrate, and a display medium.
- the first substrate has a first inner surface and a first outer surface.
- the second substrate is disposed opposite to the first substrate and has a second inner surface and a second outer surface.
- the display medium is disposed between the first substrate and the second substrate and is optically isotropic.
- the display medium is optically anisotropic when driven with an electric field.
- the directional light is not perpendicular to the first outer surface when the directional light enters the display module, and the directional light is not perpendicular to the second outer surface when the directional light exits the display module.
- the turning optical film is disposed on the second outer surface of the second substrate of the display module.
- the turning optical film has an incident surface and an output surface.
- the directional light enters the turning optical film from the incident surface, and exits the turning optical film from the output surface so as to form an output light.
- an included angle is between the output light and the output surface.
- the first compensation film is disposed on the first outer surface of the first substrate.
- the second compensation film is disposed between the second substrate and the turning optical film.
- the compensation films are disposed between the top polarizer and bottom polarizer.
- the configuration of the compensation films can adjust the polarization state of the directional light entering the display module, such that the polarization state of the directional light matches the absorption axis direction of the top polarizer. Accordingly, light leakage can be minimized and the contrast ratio and viewing angle of the display device can be enhanced.
- FIG. 1 is a schematic cross-sectional view of a display device according to an embodiment of the invention.
- FIG. 2A is a schematic view of an optically isotropic display medium without an electric field.
- FIG. 2B is a schematic view of an optically anisotropic display medium in an electric field.
- FIG. 3A and FIG. 3B are schematic cross-sectional views of a display device according to an embodiment of the invention.
- FIG. 4A is a schematic cross-sectional view of a first optical film in a display device according to an embodiment of the invention.
- FIG. 4B is a perspective view of the first optical film depicted in FIG. 4A .
- FIG. 5A is a schematic cross-sectional view of a second optical film in a display device according to an embodiment of the invention.
- FIG. 5B is a perspective view of the second optical film depicted in FIG. 5A .
- FIG. 6A is schematic cross-sectional view of an optical film in a display device according to an embodiment of the invention.
- FIG. 6B is a perspective view of the optical film depicted in FIG. 6A .
- FIG. 7 is an optical path diagram of light passing through a first optical film, a second optical film, and a turning optical film according an embodiment of the invention.
- FIG. 8A is schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.
- FIG. 8B is a perspective view of the optical film depicted in FIG. 8A .
- FIG. 9A is schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.
- FIG. 9B is a perspective view of the optical film depicted in FIG. 9A .
- FIG. 10A is schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.
- FIG. 10B is a perspective view of the optical film depicted in FIG. 10A .
- FIG. 11 and FIG. 12 are schematic cross-sectional views of a display device according to embodiments of the invention.
- FIG. 13 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance.
- FIGS. 14A and 14B are relational diagrams of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a light angle.
- FIG. 15 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance.
- FIG. 16 is a relational diagram of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a transmittance.
- FIG. 17 depicts the measurement results of a hysteresis phenomenon from a transverse electric field driving blue phase liquid crystals of a conventional IPS display module.
- FIG. 18 depicts the measurement results of a hysteresis phenomenon from a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals.
- FIG. 19 is a relational diagram between display medium thickness and voltage for a display device according to an embodiment of the invention.
- FIG. 20 is a relational diagram between voltage and transmittance under different display thickness conditions for a display device according to an embodiment of the invention.
- FIG. 21 is a schematic cross-sectional view of a display device according to a first embodiment of the invention.
- FIG. 22 is a perspective view of a light source module and a display module in a display device according to an embodiment of the invention.
- FIG. 23 is a schematic view of a Poincaré sphere of a compensation process during a dark state when a display device according to the first embodiment of the invention employs compensation films.
- FIG. 24 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 1.
- FIG. 25 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 2.
- FIG. 26 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 3.
- FIG. 27 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 4.
- FIG. 28 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 5.
- FIG. 29 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 6.
- FIG. 30 is a schematic cross-sectional view of a display device according to a second embodiment of the invention.
- FIG. 31 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the second embodiment of the invention employs compensation films.
- FIG. 32 is a contour map of the contrast ratios measured on the display device of FIG. 30 with the parameter setting of Table 7.
- FIG. 33 is a schematic cross-sectional view of a display device according to a third embodiment of the invention.
- FIG. 34 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the third embodiment of the invention employs compensation films.
- FIG. 35 is a contour map of the contrast ratios measured on the display device of FIG. 33 with the parameter setting of Table 8.
- FIG. 36 is a contour map of the contrast ratios measured on the display device of FIG. 33 with the parameter setting of Table 9.
- FIG. 37 is a schematic cross-sectional view of a display device according to a fourth embodiment of the invention.
- FIG. 38 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fourth embodiment of the invention employs compensation films.
- FIG. 39 is a contour map of the contrast ratios measured on the display device of FIG. 37 with the parameter setting of Table 10.
- FIG. 40 is a schematic cross-sectional view of a display device according to a fifth embodiment of the invention.
- FIG. 41 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films.
- FIG. 42 is a contour map of the contrast ratios measured on the display device of FIG. 40 with the parameter setting of Table 11.
- FIG. 43 is a contour map of the bright state measurements on the display device of FIG. 40 with the parameter setting of Table 11.
- FIG. 44 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films.
- FIG. 45 is a contour map of the contrast ratios measured on the display device of FIG. 40 with the parameter setting of Table 12.
- FIG. 46 is a contour map of the bright state measurements on the display device of FIG. 40 with the parameter setting of Table 12.
- FIG. 47 is a schematic cross-sectional view of a display device according to a sixth embodiment of the invention.
- FIG. 48 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the sixth embodiment of the invention employs compensation films.
- FIG. 49 is a contour map of the contrast ratios measured on the display device of FIG. 47 with the parameter setting of Table 13.
- FIG. 50 is a contour map of the bright state measurements on the display device of FIG. 47 with the parameter setting of Table 13.
- FIG. 51 is a schematic cross-sectional view of a display device according to a seventh embodiment of the invention.
- FIG. 52 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the seventh embodiment of the invention employs compensation films.
- FIG. 53 is a contour map of the contrast ratios measured on the display device of FIG. 51 with the parameter setting of Table 14.
- FIG. 54 is a contour map of the bright state measurements on the display device of FIG. 51 with the parameter setting of Table 14.
- FIG. 1 is a schematic cross-sectional view of a display device according to an embodiment of the invention.
- a display device 100 of the present embodiment includes a display module P, a light source module B, and a turning optical film 25 .
- the display module P includes a first substrate 21 b, a second substrate 21 a, and a display medium 20 .
- the first substrate 21 b has an inner surface S 1 and an outer surface S 2 , and a pixel array 22 b is disposed on the inner surface S 1 of the first substrate 21 b.
- the first substrate 21 b may be made of glass, quartz, an organic polymer, or other suitable materials.
- the pixel array 22 b includes a plurality of scan lines, a plurality of data lines, and a plurality of pixel units.
- Each of the pixel units includes an active element and a pixel electrode electrically connected to the active element.
- the active element of the pixel unit is electrically connected to a corresponding data line and a corresponding scan line.
- the active element may a bottom-gate thin film transistor (TFT) or a top-gate TFT.
- the second substrate 21 a is disposed opposite to the first substrate 21 b, and the second substrate 21 a has an inner surface S 3 and an outer surface S 4 . Moreover, an opposite electrode 22 a is disposed on the inner surface S 3 of the second substrate 21 a.
- the second substrate 21 a may also be made of glass, quartz, an organic polymer, or other suitable materials.
- the opposite electrode 22 a completely covers the inner surface S 3 of the second substrate 21 a.
- the opposite electrode 22 a is a transparent electrode
- a material of the transparent electrode includes a metal oxide such as indium tin oxide (ITO), indium zinc oxide (IZO), aluminum tin oxide (ATO), aluminum zinc oxide (AZO), indium germanium zinc oxide, other suitable metal oxides, or a stacked layer having at least two of the above materials.
- ITO indium tin oxide
- IZO indium zinc oxide
- ATO aluminum tin oxide
- AZO aluminum zinc oxide
- indium germanium zinc oxide other suitable metal oxides, or a stacked layer having at least two of the above materials.
- a color filter array may be disposed on the first substrate 21 b or the second substrate 21 a, so that the display module P can display color images.
- the invention is not limited thereto.
- the display medium 20 is disposed between the pixel array 22 b of the first substrate 21 b and the opposite electrode 22 a of the second substrate 21 a. Moreover, the display medium 20 is optically isotropic when no electric field is applied thereto, as shown in FIG. 2A .
- the display medium 20 is optically anisotropic when a perpendicular electric field 201 is applied thereto, as shown in FIG. 2B .
- the display medium 20 displays properties of optical isotropy.
- the display medium 20 displays properties of optical anisotropy.
- the display medium 20 includes blue phase liquid crystals, such as polymer-stabilized blue phase liquid crystals or polymer-stabilized isotropic phase liquid crystals. Since the display medium 20 switches between optically isotropic and optically anisotropic by the generation of electric fields, such that the display medium 20 functions as a light valve, the response speed of this type of display medium 20 is preferably faster than the twisting response speed of the conventional twisted nematic liquid crystal molecules.
- the light source module B is disposed below the outer surface S 2 of the first substrate 21 b of the display module P. Moreover, the light source module B generates a directional light 281 . In other words, the directional light 281 projects along a specific projected direction and distributes within a specific angle. In the present embodiment, the directional light 281 is concentrated within a specific range. That is, the directional light 281 has directionality and is not like the conventional scattered light source with light spreading in all directions without any directionality.
- the light source module B is, for example, a side incident type light source module, including a light guide plate 26 a and a light source 26 b. It should be appreciated that the light source module B may further include elements such as an optical film set and a frame. In the present embodiment, the side incident type light source module is used as an example for description, although the invention is not limited thereto. According to other embodiments, the light source module B may be a light source module having other forms, such as the direct type light source module, for example.
- the display medium 20 is optically anisotropic when no electric field is applied thereto, therefore, when the pixel array 22 b of the display module P and the opposite electrode 22 a form the perpendicular electric field 201 therebetween, the display medium 20 not only display properties of optical anisotropy, but the display medium 20 is also vertically aligned along the perpendicular electric field 201 , as shown in FIGS. 1 and 2B .
- the propagating direction of the light from the light source module B has a specific design as illustrated below.
- the directional light 281 generated by the light source module B propagates along an incident direction D 1 when the directional light 281 enters the display module P. Moreover, the incident direction D 1 is not perpendicular to the outer surface S 2 of the first substrate 21 b. In other words, the directional light 281 generated by the light source module B does not perpendicularly enter into the display module P, but the directional light 281 is incident at a specific inclination angle into the display module P. In order for the directional light 281 generated by the light source module B to exit the light source module B at a specific angle, special optical microstructures can be designed on the light guide plate 26 a.
- a layer of optical film having special optical microstructures may be disposed on the light guide plate 26 a. Accordingly, when the light generated by the light source 26 b passes the light guide plate 26 a (or optical film), the propagating direction of the light changes, such that the directional light 281 generated by the light source module B exits at the specific inclination angle. According to the present embodiment, since the directional light 281 generated by the light source module B exits at the specific inclination angle, therefore, an included angle ⁇ 1 between the incident direction D 1 of the directional light 281 and the outer surface S 2 of the first substrate 21 b is 5° ⁇ 45°, for example.
- an inclination angle ⁇ 1 ′ of the directional light 281 generated by the light source module B is 45° ⁇ 85°, for example.
- the inclination angle ⁇ 1 ′ refers to the included angle between the incident direction D 1 of the directional light 281 and a perpendicular axial line V.
- a directional light 282 is formed.
- the directional light 282 in the display module P maintains the same direction when passing through the display medium 20 .
- the directional light 281 generated by the light source module B becomes the directional light 282 when entering the display medium 20 .
- the directional light 282 propagates along an incident direction D 2 not perpendicular to the inner surface S 1 of the first substrate 21 b. Therefore, the included angle ⁇ between the incident direction D 2 of the directional light 282 and the inner surface S 1 of the first substrate 21 b is not equal to 90°.
- the included angle ⁇ between the incident direction D 2 of the directional light 282 and the inner surface S 1 of the first substrate 21 b is 5° ⁇ 45°, for example.
- an included angle between the propagating direction D 3 and a surface (output surface) of the turning optical film 25 is substantially 60° ⁇ 120°.
- the output light 283 exits the turning optical film 25 perpendicularly. Therefore, the included angle between the propagating direction D 3 and the surface (output surface) of the turning optical film is substantially 90°, such that the output light 283 received by a user's eye 29 is a light propagating along the normal direction. Accordingly, an included angle ⁇ 2 between the propagating direction D 3 of the output light 283 and the surface (output surface) of the turning optical film 25 is substantially equal to 90°.
- a first optical film 24 b may be further disposed on the outer surface S 2 of the first substrate 21 b, such that the directional light 282 maintains the same propagating or transmitting direction as much as possible before entering the display medium 20 .
- a second optical film 24 a may be further disposed on the outer surface S 4 of the second substrate 21 a.
- the first optical film 24 b is disposed on the outer surface S 2 of the first substrate 21 b.
- the first optical film 24 b has a plurality of first optical structures T 1 .
- the first optical structures T 1 allow the directional light 281 passing through the first optical structures T 1 without generating total reflection. That is, the directional light 281 directly passes through the first optical structures T 1 of the first optical film 24 b. If the directional light 281 is not being totally reflected or refracted when directly passing through the first optical structures T 1 of the first optical film 24 b, optical loss of the directional light 281 caused by the first optical film 24 b can be minimized. In other words, optical loss of the directional light 281 at the interface of air and the first substrate 21 b due to reflection can be reduced. Accordingly, the directional light 281 can pass through the first optical film 24 b in the same propagating direction as much as possible.
- the first optical film 24 b has a first surface S 5 and a second surface S 6 opposite to the first surface S 5 .
- the first surface S 5 faces the light source module B
- the second surface S 6 faces the outer surface S 2 of the first substrate 21 b
- the first optical structures T 1 are disposed on the first surface S 5 . That is, the second surface S 6 of the first optical film 24 b is a smooth plane, although the invention is not limited thereto.
- the first optical structures T 1 on the first surface S 5 of the first optical film 24 B can cause the directional light 281 of the light source module B to pass through the first optical film 24 b as directly as possible.
- the first optical structures T 1 are grooves having a first side wall W 1 and a second side wall W 2 , as shown in FIG. 4A .
- the incident direction D 1 is substantially perpendicular to the first side wall W 1
- the incident direction D 1 is substantially parallel to the second side wall W 2 .
- the first side wall W 1 of the grooves T 1 is a short side wall
- the second side wall W 2 is a long side wall.
- the short side wall W 1 is substantially perpendicular to the incident direction D 1 .
- a refractive index of the first optical film 24 b is close to a refractive index of the first substrate 21 b.
- a width p 1 of the first optical structures (grooves) T 1 is approximately 5 ⁇ m ⁇ 100 ⁇ m.
- An included angle ⁇ 4 between the first side wall W 1 of the first optical structures (grooves) T 1 and the perpendicular axial line V is approximately 5° ⁇ 45°.
- An included angle ⁇ 3 between the second side wall W 2 of the first optical structures (grooves) T 1 and the perpendicular axial line V is approximately 45° ⁇ 85°.
- the second optical film 24 b is disposed on the outer surface S 4 of the second substrate 21 a.
- the second optical film 24 a has a plurality of second optical structures T 2 .
- the second optical structures T 2 allows the directional light 282 passing through the second optical structures T 2 without generating total reflection. That is, the directional light 282 directly passes through the second optical structures T 2 of the second optical film 24 a. If the directional light 282 is not being totally reflected or refracted when directly passing through the second optical structures T 2 of the second optical film 24 a, optical loss of the directional light 282 caused by the second optical film 24 a can be minimized. In other words, optical loss of the directional light 282 at the interface of air and the second optical film 24 a due to reflection can be reduced. Accordingly, the directional light 282 can exit the second optical film 24 a in the same transmitting direction as much as possible.
- the second optical film 24 a has a first surface S 7 and a second surface S 8 opposite to the first surface S 7 .
- the first surface S 7 faces the outer surface S 4 of the second substrate 21 a, and the second optical structures T 2 are disposed on the second surface S 8 . That is, the first surface S 7 of the second optical film 24 a is a smooth plane, although the invention is not limited thereto.
- the second optical structures T 2 on the second surface S 8 of the second optical film 24 a can cause the directional light 282 to pass through the second optical film 24 a as directly as possible.
- the second optical structures T 2 are grooves having a first side wall W 3 and a second side wall W 4 , as shown in FIG. 5A .
- the incident direction D 2 of the directional light 282 when passing through the second optical film 24 a is perpendicular to the first side wall W 3
- the incident direction D 2 is parallel to the second side wall W 4 .
- the first side wall W 3 is a short side wall
- the second side wall W 4 is a long side wall.
- the short side wall W 3 is substantially perpendicular to the incident direction D 2 of the directional light 282 .
- a refractive index of the second optical film 24 a is close to a refractive index of the second substrate 21 a. Accordingly, when the directional light 282 passes through the second optical structures (grooves) T 2 , the directional light 282 can directly pass through the short side wall W 3 without generating total reflection or refraction, such that the directional light 282 can pass through the second optical film 24 a as directly as possible.
- a width p 2 of the second optical structures (grooves) T 2 is approximately 5 ⁇ m ⁇ 100 ⁇ m.
- An included angle ⁇ 6 between the first side wall W 3 of the second optical structures (grooves) T 2 and the perpendicular axial line V is approximately 5° ⁇ 45°.
- An included angle ⁇ 5 between the second side wall W 4 of the second optical structures (grooves) T 2 and the perpendicular axial line V is approximately 45° ⁇ 85°.
- the turning optical film 25 is disposed on the second optical film 24 a.
- the turning optical film 25 has a plurality of tuning optical structures T 3 , such that the directional light 282 is totally reflected by the tuning optical structures T 3 to form the output light 283 .
- an included angle between the propagating direction D 3 after the output light 283 passes through the turning optical film 25 and a surface (output surface) S 10 of the turning optical film 25 is 60° ⁇ 120°.
- the propagating direction D 3 after the output light 283 passes through the turning optical film 25 is substantially perpendicular to the surface (output surface) S 10 of the turning optical film 25 .
- the directional light 282 is totally reflected by the tuning optical structures T 3 of the turning optical film 25 as much as possible to form the output light 283 .
- the tuning optical structures T 3 of the turning optical film 25 is designed mainly to redirect the propagating or transmitting direction of the directional light 281 and 282 emitted from the light source module B after passing through the turning optical film 25 .
- the output light 283 can exit the turning optical film 25 perpendicularly to be received by the user's eye 29 .
- the turning optical film 25 has a first surface S 9 (also referred to as the incident surface) and a second surface S 10 (also referred to as the output surface) opposite to the first surface S 9 .
- the first surface S 9 faces the outer surface S 4 of the second substrate 21 a, and the tuning optical structures T 3 are disposed on the first surface S 9 .
- the second surface S 10 of the turning optical film 25 is a smooth plane, although the invention is not limited thereto.
- the directional light 282 is totally reflected by the tuning optical structures T 3 of the turning optical film 25 by the first surface S 9 , so as to form the output light 283 .
- the tuning optical structures T 3 are grooves having a first side wall W 5 and a second side wall W 6 , as shown in FIG. 6A .
- the first side wall W 5 and the second side wall W 6 of the grooves T 3 are planar side walls.
- an included angle ⁇ 7 between the first side wall W 5 and the perpendicular axial line V is approximately 5° ⁇ 60°
- an included angle ⁇ 8 between the second side wall W 6 and the perpendicular axial line V is approximately 15° ⁇ 45°.
- a width p 3 of the optical structures (grooves) T 3 is approximately 5 ⁇ m ⁇ 100 ⁇ m.
- FIG. 7 the optical paths of the directional light 281 and 282 passing through the first optical film 24 b, second optical film 24 a, and the turning optical film 25 are illustrated.
- the optical paths of the directional light 281 , the directional light 282 , and the output light 283 respectively passing through the first optical film 24 b, the second optical film 24 a, and the turning optical film 25 only the first optical film 24 b, the second optical film 24 a, and the turning optical film 25 are drawn in FIG. 7 . That is, the display module P and other film layers are omitted in the drawing.
- the directional light 281 passes through the first optical film 24 b as directly as possible without generating total reflection or refraction.
- the directional light 282 then passes through the second optical film 24 a also as directly as possible without generating total reflection or refraction.
- the directional light 282 is then totally reflected as much as possible by the tuning optical structures T 3 of the turning optical film 25 , so as to form the output light 283 .
- the display device 100 of the present embodiment may further include a bottom polarizer 23 b and a top polarizer 23 a.
- the bottom polarizer 23 b is disposed between the first substrate 21 b and the first optical film 24 b
- the top polarizer 23 a is disposed between the second substrate 21 a and the second optical film 24 a.
- Dichroic polymer films such as polyvinyl-alcohol-based films may be adopted for the bottom polarizer 23 b and the top polarizer 23 a.
- An included angle between a transmission axis of the bottom polarizer 23 b and a transmission axis of the top polarizer 23 a may be 5° ⁇ 175°.
- the display module P of the present embodiment further includes a compensation film 231 and a diffusion film 27 .
- the compensation film 231 is disposed between the bottom polarizer 23 b and the top polarizer 23 a.
- the compensation film 231 is disposed between the bottom polarizer 23 b and the first substrate 21 b as an example for description.
- a compensation film (not drawn) may also be disposed between the top polarizer 23 a and the second substrate 21 a.
- the compensation film 231 may be disposed between the bottom polarizer 23 b and the first substrate 21 b, and the compensation film (not drawn) may be disposed between the top polarizer 23 a and the second substrate 21 a.
- the configuration of the compensation film 23 a can enhance the contrast ratio of the display module P as well as the viewing angle.
- the diffusion film 27 is disposed above the top polarizer 23 a, so that a diffusion effect is generated when the output light 283 passes through the diffusion film 27 , thereby achieving preferable display quality for the display module P.
- the use of the diffusion film 27 is not necessary in the invention.
- the display medium 20 of the display module P of the present embodiment is driven by the perpendicular electric field 201 between the pixel array 22 b and the opposite electrode 22 a, the low transmittance and high driving voltage issues of the conventional IPS display module can be resolved.
- the incident direction D 2 of the directional light 281 and the directional light 282 generated by the light source module B in the present embodiment are not perpendicular to the surface of the first substrate 21 b when entering the display medium 20 , the display medium 20 is still birefringent to the directional light 282 of the light source module B when the display medium 20 is driven and becomes optically anisotropic. Accordingly, the display module P can display images.
- the top polarizer 23 a is disposed between the second substrate 21 a and the second optical film 24 a. Thereby, the effect from the second optical film 24 a and the turning optical film 25 on the polarization state of the directional light 282 is minimized.
- the invention is not limited thereto. According to other embodiments, the top polarizer 23 a may also be disposed above the second optical film 24 a or the turning optical film 25 , as shown in FIG. 3A .
- the second optical film 24 b may be omitted in the display module P, as shown in FIG. 3B . Accordingly, the effect from the second optical film 24 a on the polarization state of the directional light 282 is minimized.
- the invention is not limited thereto.
- the optical film 25 of the display module P are shown in FIGS. 6A and 6B , for example.
- the invention is not limited thereto.
- the optical film 25 of the display device 100 may also adopt other forms or structures, as further elaborated below.
- FIG. 8A is a schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.
- FIG. 8B is a perspective view of the optical film depicted in FIG. 8A .
- the tuning optical structures T 3 ′ of the optical film 25 in the present embodiment are grooves
- a first side wall W 5 ′ of the optical structures (grooves) T 3 is a curved side wall
- a second side wall W 6 ′ of the optical structures (grooves) T 3 ′ is a planar side wall.
- the directional light 282 when the directional light 282 enters the optical film 25 , the directional light 282 is totally reflected by the first side wall (curved side wall) W 5 ′ of the tuning optical structures T 3 ′ so as to form the output light 283 , such that the output light 283 can exit the turning optical film 25 perpendicularly.
- the first side wall W 5 ′ is a curved side wall, besides the directional light 282 generating total reflection at the first side wall (curved side wall) W 5 ′, a part of the output light 283 generated by total reflection has an incident angle that is less than a total reflection angle.
- a width p 4 of the optical structures (grooves) T 3 ′ is approximately 5 ⁇ m ⁇ 100 ⁇ m.
- each tuning optical structure T 3 ′ in the turning optical film 25 of the embodiment depicted in FIGS. 8A and 8B has the same pattern.
- the optical structures of the turning optical film 25 may have different patterns, as shown in FIGS. 9A and 9B .
- FIG. 9A is a schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.
- FIG. 9B is a perspective view of the optical film depicted in FIG. 9A .
- each tuning optical structure T 3 ′ of the turning optical film 25 has a planar side wall and a curved side wall, but the radii of curvature of the curved side walls of the tuning optical structures T 3 ′ are not all the same.
- a radius of curvature of the curved side wall W 5 ′ of the tuning optical structure T 3 ′ in the present embodiment is different than a radius of curvature of a curved side wall W 5 ′′.
- the tuning optical structure T 3 ′ having the curved side wall W 5 ′ with the larger radius of curvature is alternatively arranged with the optical structure T 3 ′ having the curved side wall W 5 ′ with the smaller radius of curvature.
- FIG. 10A is a schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.
- FIG. 10B is a perspective view of the optical film depicted in FIG. 10A .
- each tuning optical structure T 3 ′ of the turning optical film 25 has a planar side wall and a curved side wall, and the curved side wall of each tuning optical structure T 3 ′ has a plurality of radii of curvature. The radii of curvature of the curved side wall progressively decrease as the bottom of the groove T 3 ′ is approached.
- the first side wall of the grooves T 3 ′ in the turning optical film 25 is a curved side wall, including a curved side walls W 5 - 1 and a curved side wall W 5 - 2 .
- the radius of curvature of the curved side wall W 5 - 1 is smaller than the radius of curvature of the curved side wall W 5 - 2 .
- the present embodiment uses two different curvatures for the curved side walls W 5 - 1 and W 5 - 2 as an illustrative example, although in actuality the first side wall of the grooves T 3 ′ in the turning optical film 25 is a continuous curved surface.
- the output light 283 can be refracted out of the optical film 25 after being reflected to the curved side wall W 5 - 1 . Since the radius of curvature of the curved side wall W 5 - 1 progressively decreases as the bottom of the grooves T 3 ′ is approached, an included angle between a tangent of the curved side wall W 5 - 1 and the transmission direction of the output light 283 also decreases gradually. Accordingly, the output light 283 can be easily refracted out of the optical film 25 after being reflected to this area.
- the curved side wall W 5 - 1 having the smaller radius of curvature can refract more output light 283 out the optical film 25 at this area.
- the divergence angle and distribution of light from the turning optical film 25 depicted in FIGS. 10A and 10B is wider and broader than those of the embodiment illustrated in FIGS. 8A and 8B .
- FIG. 11 and FIG. 12 are schematic cross-sectional views of a display device according to embodiments of the invention.
- the embodiment shown in FIGS. 11 and 12 is similar to the embodiment shown in FIG. 1 , and thus identical components denoted with the same numerals and will not be repeated herein.
- a difference between the embodiments in FIGS. 11 and 1 lies in that, a pixel array 221 b has a slit alignment pattern 60 , and a protruding alignment pattern 70 is disposed on an opposite electrode 221 a.
- the distribution of a perpendicular electric field 202 changes and multi-domain alignment is achieved for the display medium 20 , accordingly.
- a difference between the embodiments in FIGS. 12 and 1 lies in that, the pixel array 221 b has the slit alignment pattern 60 , and the opposite electrode 221 a has a slit alignment pattern 80 .
- the distribution of the perpendicular electric field 202 can also be changed by configuring the slit alignment pattern 60 on the pixel array 221 b and the slit alignment pattern 80 on the opposite electrode 221 a, thereby achieving multi-domain alignment for the display medium 20 .
- alignment patterns e.g. slit alignment patterns or protruding alignment patterns
- the invention is not limited thereto.
- alignment patterns e.g. slit alignment patterns or protruding alignment patterns
- alignment patterns may only be disposed on the pixel array 221 b
- alignment patterns e.g. slit alignment patterns or protruding alignment patterns
- the combination of alignment patterns on the pixel array 221 b and the opposite electrode 221 a is also not limited to the embodiments depicted in FIGS. 11 and 12 .
- the protruding alignment pattern may be disposed on the pixel array 221 b and the slit alignment pattern may be disposed on the opposite electrode 221 a, or the protruding alignment pattern may be disposed on the pixel array 221 b and the protruding alignment pattern may be disposed on the opposite electrode 221 a
- the display device has lower driving voltage and preferable transmittance compared to the conventional IPS display device
- several examples with comparison to the conventional IPS display device are set forth below.
- FIG. 13 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance.
- the horizontal axis of FIG. 13 represents voltage (V), while the vertical axis represents the transmittance of the display module.
- V voltage
- the driving voltage needs to reach 52 V to achieve a preferable transmittance. That is, the driving voltage needs to reach 52 V in order for the display module to have a Kerr constant of 12.68 nm/V 2 .
- FIGS. 14A and 14B are relational diagrams of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a light angle.
- the horizontal axis of FIGS. 14A and 14B represent an inclination angle of light from a light source module (e.g. the angle ⁇ 1 ′ depicted in FIG. 1 ), and the vertical axis represents voltage (V).
- a display medium thickness (also referred to as the cell gap) of the display module in this display device is 3.5 ⁇ m, and the display module of FIG. 14A has a Kerr constant of 12.68 nm/V 2 .
- the driving voltage (below 15 V) needed by the display module of FIG. 14A is far lower than the driving voltage (52 V) needed by the IPS display module of FIG. 13 .
- the driving voltage thereof decreases.
- a display medium thickness (also referred to as the cell gap) of the display module in this display device is 5 ⁇ m, and the display module of FIG. 14B has the same Kerr constant of 12.68 nm/V 2 .
- the driving voltage (below 18 V) needed by the display module of FIG. 14B is far lower than the driving voltage (52 V) needed by the IPS display module of FIG. 13 .
- the driving voltage thereof decreases.
- FIG. 15 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance.
- the horizontal axis of FIG. 15 represents voltage (V), while the vertical axis represents the transmittance of the display module.
- a laser light of 633 nm serves as the light from the light source module, and the laser light enters the IPS display module perpendicularly.
- the display module has the greatest transmittance when the driving voltage reaches 193 Vrms.
- FIG. 16 is a relational diagram of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a transmittance.
- the horizontal axis of FIG. 16 represents voltage (V), while the vertical axis represents the transmittance of the display module.
- the 633 nm laser light serves as the light from the light source module
- t represents the display medium thickness (also referred to as the cell gap)
- ⁇ represents the light inclination angle (angle ⁇ 1 ′ depicted in FIG. 1 ) of the light source module.
- angle ⁇ 1 ′ depicted in FIG. 1
- Blue phase liquid crystals typically exhibit the hysteresis phenomeon.
- hysteresis usually needs to be suppressed or reduced to prevent the hysteresis of the blue phase liquid crystals from affecting the gray level control accuracy of the display module.
- FIG. 17 depicts the measurement results of a hysteresis phenomenon from a transverse electric field driving blue phase liquid crystals of a conventional IPS display module.
- FIG. 18 depicts the measurement results of a hysteresis phenomenon from a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals.
- the hysteresis phenomenon of blue phase liquid crystals can be measured by gradually increasing voltage to measure the voltage and transmittance curves M and M′, and by gradually decreasing voltage to measure the voltage and transmittance curves N and N′. The voltage difference between the two curves M and N (M′ and N′) under a half transmittance condition is then calculated.
- the voltage difference between the curves M and N ( FIG. 17 ) under the half transmittance condition is significantly greater than the voltage difference between the curves M′ and N′ ( FIG. 18 ) under the half transmittance condition. Therefore, the blue phase liquid crystals of the conventional IPS display module driven by the transverse electric field exhibit high hysteresis.
- FIG. 19 is a relational diagram between display medium thickness and voltage for a display device according to an embodiment of the invention.
- the horizontal axis in FIG. 19 represents the display medium thickness (also referred to as the cell gap), and the vertical axis represents voltage (V).
- the 550 nm laser light serves as the light from the light source module
- ⁇ represents the light inclination angle (angle ⁇ 1 ′ depicted in FIG. 1 ) of the light source module
- the four curves in FIG. 19 can all allow the display module to have a Kerr constant of 10.2 nm/V 2 .
- the required driving voltage is also reduced.
- FIG. 20 is a relational diagram between voltage and transmittance under different display medium thickness conditions for a display device according to an embodiment of the invention.
- the horizontal axis of FIG. 20 represents voltage (V), while the vertical axis represents the transmittance.
- the display medium thickness also referred to as the cell gap
- the 550 nm laser light serves as the light from the light source module
- the light inclination angle (angle ⁇ 1 ′ depicted in FIG. 1 ) of the light source module is 70°.
- the driving voltage of the display device according to an embodiment of the invention is related to the display medium thickness.
- the display medium of the display module is driven by the perpendicular electric field generated between the pixel array and the electrode layer.
- the display medium since the incident direction of the light generated by the light source module when entering the display medium is not perpendicular to the inner surface of the first substrate, the display medium remains birefringent to the light from the light source module when the display medium is driven to be optically anisotropic. Accordingly, since the display device according to an exemplary embodiment can adopt the perpendicular electric field to drive the display medium, the issues of low transmittance and high driving voltage from conventionally using the transverse electric field to drive the blue phase liquid crystals can be resolved.
- the display device can further include a plurality of compensation films, which can be configured to enhance the display quality of the display device.
- Embodiments 1-7 provided below to further illustrate the advantages of configuring the compensation films. It should be noted that, the embodiments provided below are similar to the embodiment shown in FIG. 1 , and thus identical components denoted with the same numerals and will not be repeated herein. The omitted portions can be referenced to the earlier embodiments. The differences between the embodiments are further described below.
- FIG. 21 is a schematic cross-sectional view of a display device according to a first embodiment of the invention.
- the display device 100 a includes a first compensation film 28 b and a second compensation film 28 a, and does not include the compensation film 231 .
- the first compensation film 28 b is disposed on the outer surface S 2 of the first substrate 21 b
- the second compensation film 28 a is disposed between the second substrate 21 a and the turning optical film 25 .
- the bottom polarizer 23 b is disposed on the outer surface S 2 of the first substrate 21 b
- the top polarizer 23 a is disposed on the outer surface S 4 of the second substrate 21 a.
- the bottom polarizer 23 b is disposed between the first compensation film 28 b and the first optical film 24 b.
- the top polarizer 23 a is disposed between the second compensation film 28 a and the second optical film 24 a
- the second optical film 24 a is disposed between the turning optical film 25 and the top polarizer 23 a.
- the directional light 282 passes through the bottom polarizer 23 b, the first compensation film 28 b, the second compensation film 28 a, and the top polarizer 23 a in sequence.
- the first compensation film 28 b and the second compensation film 28 a may be used to adjust the polarization state of the directional light 282 located in the display module P, such that the polarization state of the directional light 282 after adjustment matches the absorption axis direction of the top polarizer 23 a.
- the light leakage generated when the directional light 282 forms the output light 283 can be reduced, and the contrast ratio of the display device 100 a in the dark state can be further enhanced.
- a Poincaré sphere is used to illustrate the compensation process of the first compensation film 28 b and the second compensation film 28 a.
- a polar angle ⁇ and an orientation angle ⁇ are used for the definitions below.
- FIG. 22 is a perspective view of a light source module and a display module in the display device according to an embodiment of the invention.
- the orientation angle ⁇ is an included angle between a projection line on the XY plane of an arbitrary direction D 4 and the X direction.
- the polar angle ⁇ is an included angle between the arbitrary direction D 4 and the Z direction.
- FIG. 23 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the first embodiment of the invention employs compensation films.
- the polar angle ⁇ of the directional light 282 is 70° and the orientation angle ⁇ is 270°
- an effective angle between the bottom polarizer 23 b and the top polarizer 23 a changes. Therefore, a transmissive state P 1 of the directional light 282 and a state A 1 of the absorption axis of the top polarizer 23 a are separated, thereby causing the light leakage.
- the first compensation film 28 b can rotate the polarization state of the directional light 282 from the state P 1 to a state P 0
- the second compensation film 28 a can rotate the polarization state of the directional light 282 from the state P 0 to the state A 1 . Accordingly, after the directional light 282 passes through the first compensation film 28 b and the second compensation film 28 a, the polarization state of the directional light 282 can be rotated from the state P 1 to the state A 1 , and thereby prevent light leakage.
- Table 1 tabulates a parameter setting data of each component in the display device 100 a, in which Nz denotes the ratio of refractive index anisotropy, and Nz can be represented by the following equation:
- Nz ( n x ⁇ n z )/( n x ⁇ n y )
- FIG. 24 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 1.
- the four contour lines from outside to inside respectively represents the contour lines of contrast ratios 100, 200, 500, and 1000.
- the viewing cone of contrast ratio greater than 1000:1 is approximately 20°, and the 20° viewing cone is sufficient for the straight directional light 282 in the vertical field switching blue phase LCD.
- the front diffusion film 27 or the turning optical film 25 can be used to diffuse the straight backlight source, so as to achieve the wide viewing angle.
- the invention is not limited thereto. An example of other parameter settings is provided below to optimize the contrast ratio.
- Table 2 tabulates a parameter setting data of each component in the display device 100 a.
- FIG. 25 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 2.
- the contour line area of contrast ratio 1000:1 in FIG. 25 is greater than the contour line area of contrast ratio 1000:1 in FIG. 24 .
- the smaller polar angle of the incident light results in higher driving voltage.
- Table 3 tabulates a parameter setting data of each component in the display device 100 a.
- FIG. 26 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 3.
- FIG. 27 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 4.
- FIG. 27 illustrates the contour lines of the optimized contrast ratio for an incident light with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°.
- FIG. 28 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 5.
- FIG. 28 illustrates the contour lines of the optimized contrast ratio for an incident light with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°.
- FIG. 29 is a contour map of the contrast ratios measured on the display device of FIG. 21 with the parameter setting of Table 6.
- FIG. 29 illustrates the contour lines of the optimized contrast ratio for an incident light with a polar angle ⁇ of 60° and an orientation angle ⁇ of 270°.
- FIG. 30 is a schematic cross-sectional view of a display device according to a second embodiment of the invention.
- a display device 100 b of the present embodiment is similar to the display device 100 a of the first embodiment.
- a difference therebetween lies in that, the display device 100 b further includes a third compensation film 31 b and a fourth compensation film 31 a.
- the third compensation film 31 b is disposed between the first compensation film 28 b and the bottom polarizer 23 b
- the fourth compensation film 31 a is disposed between the second compensation film 28 a and the top polarizer 23 a.
- the third compensation film 31 b and the fourth compensation film 31 a are respectively a biaxial compensation film, for example.
- the third compensation film 31 b and the fourth compensation film 31 a may be designed in accordance with different orientation angle ⁇ , so as to compensate for an angular difference between the top polarizer 23 a and the bottom polarizer 23 b.
- the directional light 282 passes through the bottom polarizer 23 b, the third compensation film 31 b, the first compensation film 28 b, the second compensation film 28 a, the fourth compensation film 31 a, and the top polarizer 23 a in sequence.
- FIG. 31 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the second embodiment of the invention employs compensation films.
- a P 2 state is shifted from a P 1 state.
- the P 2 state represents a polarization state when the orientation angle ⁇ is 300°
- the P 1 state represents a polarization state when the orientation angle ⁇ is 270°.
- the third compensation film 31 b can rotate the polarization state from the state P 2 to the state P 1 .
- the first compensation film 28 b and the second compensation film 28 a can then rotate the polarization state from the state P 1 to a state A 1 .
- the fourth compensation film 31 a can then rotate the polarization state from the state A 1 to a state A 2 matching the absorption axis of the top polarizer 23 a.
- Table 7 tabulates a parameter setting data of each component in the display device 100 b.
- FIG. 32 is a contour map of the contrast ratios measured on the display device of FIG. 30 with the parameter setting of Table 7.
- FIG. 33 is a schematic cross-sectional view of a display device according to a third embodiment of the invention.
- a display device 100 c of the present embodiment is similar to the display device 100 b of the second embodiment.
- a difference therebetween lies in that, in the display device 100 c, the third compensation film 31 b is disposed between the first compensation film 28 b and the first substrate 21 b, and the fourth compensation film 31 a is disposed between and the second compensation film 28 a and the second substrate 21 a.
- the third compensation film 31 b and the fourth compensation film 31 a are respectively a biaxial compensation film, for example.
- the third compensation film 31 b and the fourth compensation film 31 a may be designed in accordance with different orientation angles ⁇ , so as to compensate for an angular difference between the top polarizer 23 a and the bottom polarizer 23 b.
- the directional light 282 passes through the bottom polarizer 23 b, the first compensation film 28 b, the third compensation film 31 b, the fourth compensation film 31 a, the second compensation film 28 a, and the top polarizer 23 a in sequence.
- FIG. 34 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the third embodiment of the invention employs compensation films.
- the first compensation film 28 b can rotate a polarization state from a state P 1 to a state P 0 .
- the third compensation film 31 b then rotates the polarization state from a linear polarization state of the state P 0 to a circular polarization state of a state C 1 .
- the fourth compensation film 31 a then rotates the polarization state from the circular polarization state of the state C 1 to the linear polarization state of the state P 0 .
- the second compensation film 28 a then rotates the polarization state from the state P 0 to a state A 1 matching the absorption axis of the top polarizer 23 a. Since circularly polarized light is not affected by the orientation angles of the blue phase liquid crystal materials, circularly polarized light can improve the viewing angle of the VFS blue phase LCD.
- Table 8 tabulates a parameter setting data of each component in the display device 100 c.
- FIG. 35 is a contour map of the contrast ratios measured on the display device of FIG. 33 with the parameter setting of Table 8.
- FIG. 36 is a contour map of the contrast ratios measured on the display device of FIG. 33 with the parameter setting of Table 9.
- FIG. 36 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle ⁇ of 60° and an orientation angle ⁇ of 270°.
- FIG. 37 is a schematic cross-sectional view of a display device according to a fourth embodiment of the invention.
- a display device 100 d of the present embodiment is similar to the display device 100 b of the second embodiment.
- a difference therebetween lies in that, in the display device 100 d, the bottom polarizer 23 b is a wire-grid polarizer, for example.
- the first compensation film 28 b, the second compensation film 28 a, the third compensation film 31 b, and the fourth compensation film 31 a are all disposed between the top polarizer 23 a and the wire-grid bottom polarizer 23 b.
- the directional light 282 passes through the wire-grid bottom polarizer 23 b, the third compensation film 31 b, the first compensation film 28 b, the second compensation film 28 a, the fourth compensation film 31 a, and the top polarizer 23 a in sequence.
- FIG. 38 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fourth embodiment of the invention employs compensation films.
- an orientation angle ⁇ of the absorption axis of the wire-grid bottom polarizer 23 b is 90°
- an orientation angle ⁇ of the absorption axis of the top polarizer 23 a is 0°.
- the third compensation film 31 b does not change the polarization state when the orientation angle ⁇ is 270°.
- the first compensation film 28 b rotates the linear polarization state of the state P 0 to a circular polarization state of a state C 1 .
- the second compensation film 28 a rotates the circularly polarized light from the state C 1 to a state A 0 matching the absorption axis of the top polarizer 23 a. Accordingly, a preferable dark state performance can be achieved.
- the orientation angle ⁇ of the directional light 282 is not the same (e.g. 300°)
- the polarization state P 1 shifts from the polarization state P 0 .
- the third compensation film 31 b can employ different orientation angles ⁇ (e.g. from 225° to 315°) in order to rotate the state P 1 back to the state P 0 .
- the first compensation film 28 b and the second compensation film 28 a then rotate the polarization state from the state P 0 to a state P 2 through the state C 1 .
- the fourth compensation film 31 a then polarizes the linearly polarized light from the state P 2 to a state A 1 matching the absorption axis of the top polarizer 23 a.
- FIG. 39 is a contour map of the contrast ratios measured on the display device of FIG. 37 with the parameter setting of Table 10.
- FIG. 39 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°.
- the wire-grid bottom polarizer 23 b has a favorable extinction ratio, preferably high and broad contour lines can be obtained. Moreover, the wire-grid bottom polarizer 23 b is not sensitive to the incident light 281 angle and has minimal diffusion effect. Therefore, the wire-grid bottom polarizer 23 b is suitable for the VFS blue phase LCD.
- FIG. 40 is a schematic cross-sectional view of a display device according to a fifth embodiment of the invention.
- a display device 100 e of the present embodiment is similar to the display device 100 b of the second embodiment.
- a difference therebetween lies in that, in the display device 100 e, the top polarizer 23 a is disposed between the turning optical film 25 and the diffusion film 27 , and the fourth compensation film 31 a includes an A-plate compensation film 31 a - 1 and a C-plate compensation film 31 a - 2 .
- the first compensation film 28 b, the second compensation film 28 a, and the third compensation film 31 b are biaxial compensation films.
- the third compensation film 31 b is disposed between the bottom polarizer 23 b and the first compensation film 28 b
- the first optical film 24 b is disposed between the third compensation film 31 b and the first compensation film 28 b.
- the fourth compensation film 31 a is disposed between the second compensation film 28 a and the top polarizer 23 a
- the second optical film 24 a is disposed between the fourth compensation film 31 a and the top polarizer 23 a.
- the A-plate compensation film 31 a - 1 in the fourth compensation film 31 a is disposed between the C-plate compensation film 31 a - 2 and the second optical film 24 a.
- the directional light 282 passes through the bottom polarizer 23 b, the third compensation film 31 b, the first optical film 24 b, the first compensation film 28 b, the second compensation film 28 a, the C-plate compensation film 31 a - 2 , the A-plate compensation film 31 a - 1 , and the second optical film 24 a in sequence.
- the output light 283 is formed after the directional light 282 passes through the turning optical film 25 , and then the output light 283 passes through the top polarizer 23 a.
- FIG. 41 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films.
- the orientation angles ⁇ of the bottom polarizer 23 b and the top polarizer 23 a are respectively 0° and 90°.
- the polarization state of the directional light 281 is a state P 0 .
- the orientation angle ⁇ of the directional light 281 changes (e.g. 300°)
- the polarization state of the directional light 281 shifts from the state P 0 to a state P 1 .
- the third compensation film 31 b does not change the polarization state P 0 when the orientation angle ⁇ is 270°, but when the orientation angle ⁇ is 200°, the polarization state changes from the state P 1 to the state P 0 .
- the first compensation film 28 b rotates the linearly polarized light from the state P 0 to a circularly polarized light of of a state C 1 .
- the second compensation film 28 a rotates the circularly polarized light from the state C 1 to the linearly polarized light of of the state P 0 .
- the C-plate compensation film 31 a - 2 is designed to rotate the polarization state from the state P 0 to a state P 2
- the A-plate compensation film 31 a - 1 is used to rotate the polarization state from the state P 2 to a state A 1 matching the absorption axis of the top polarizer 23 a.
- FIG. 42 is a contour map of the contrast ratios measured on the display device of FIG. 40 with the parameter setting of Table 11.
- FIG. 42 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°, in which the contour lines from outside to inside respectively represents the contour lines of contrast ratios 100, 200, 500, and 1000.
- FIG. 43 is a contour map for the bright state measurements on the display device of FIG. 40 with the parameter setting of Table 11, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.2, 0.25, 0.3, 0.35, and 0.4.
- FIG. 44 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films.
- the third compensation film 31 b is used in different orientation angles to compensate the polarization state from the state P 1 to the state P 0 .
- the first compensation film 28 b shifts the state P 0 to the state P 2 .
- the second compensation film 28 a shifts the state P 2 back to the state P 0 .
- the C-plate compensation film 31 a - 2 shifts the state P 0 to a state P 3
- the A-plate compensation film 31 a - 1 shifts the state P 3 to the state A 1 matching the absorption axis of the top polarizer 23 a.
- FIG. 45 is a contour map of the contrast ratios measured on the display device of FIG. 40 with the parameter setting of Table 12.
- FIG. 45 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°, in which the contour lines from outside to inside respectively represents the contour lines of contrast ratios 100, 200, 500, and 1000.
- FIG. 46 is a contour map for the bright state measurements on the display device of FIG. 40 with the parameter setting of Table 12, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.2, 0.25, 0.3, 0.35, and 0.4.
- the bright state area in FIG. 43 is larger than the bright state area in FIG. 46 .
- the foregoing result is because during the compensation process of FIG. 41 , the polarization state of the directional light 282 in the blue phase liquid crystal materials is circularly polarized. Since the circularly polarized light is not affected by the orientation angle, the contour lines of the contrast ratio can be improved.
- FIG. 47 is a schematic cross-sectional view of a display device according to a sixth embodiment of the invention.
- a display device 100 f of the present embodiment is similar to the display device 100 e of the fifth embodiment.
- a difference therebetween lies in that, in the display device 100 f, the third compensation film 31 b is disposed between the bottom polarizer 23 b and the first compensation film 28 b, and the bottom polarizer 23 b is disposed between the first optical film 24 b and the third compensation film 31 b.
- the fourth compensation film 31 a is disposed between the second compensation film 28 a and the top polarizer 23 a, and the second optical film 24 a is disposed between the fourth compensation film 31 a and the top polarizer 23 a.
- the first compensation film 28 b, the second compensation film 28 a, and the third compensation film 31 b are biaxial compensation films.
- the fourth compensation film 31 a includes the A-plate compensation film 31 a - 1 and the C-plate compensation film 31 a - 2 .
- the directional light 282 passes through the bottom polarizer 23 b, the third compensation film 31 b, the first compensation film 28 b, the second compensation film 28 a, the C-plate compensation film 31 a - 2 , the A-plate compensation film 31 a - 1 , and the second optical film 24 a in sequence.
- the output light 283 is formed after the directional light 282 passes through the turning optical film 25 , and then the output light 283 passes through the top polarizer 23 a.
- FIG. 48 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the sixth embodiment of the invention employs compensation films.
- a polar angle of the directional light 281 is 70° and an orientation angle ⁇ is 270°, for example.
- the polarization state of the directional light 282 is a state P 0 .
- the orientation angle ⁇ of the directional light 282 changes, such as when the orientation angle ⁇ becomes 300°, the polarization state of the directional light 282 shifts from the state P 0 to a state P 1 .
- the third compensation film 31 b does not change the polarization state P 0 when the orientation angle ⁇ is 270°, but when the orientation angle ⁇ is 300°, the polarization state of the polarized light can be changed from the state P 1 to the state P 0 .
- the first compensation film 28 b shifts a linearly polarized light of the state P 0 to a circularly polarized light of a state C 1 .
- the second compensation film 28 a shifts the circularly polarized light of the state C 1 to the state P 0 .
- the absorption axis of the top polarizer 23 a is shifted to the state A 1 .
- the C-plate compensation film 31 a - 2 shifts the directional light 282 from the state P 0 to a state P 2
- the A-plate compensation film 31 a - 1 shifts from the state P 2 to the state A 1 matching the absorption axis of the top polarizer 23 a.
- FIG. 49 is a contour map of the contrast ratios measured on the display device of FIG. 47 with the parameter setting of Table 13.
- FIG. 49 illustrates the contour lines of the optimized contrast ratio for an incident light 282 with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°, in which the contour lines from outside to inside respectively represents the contour lines of contrast ratios 100, 200, 500, and 1000.
- FIG. 50 is a contour map for the bright state measurements on the display device of FIG. 47 with the parameter setting of Table 13, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.2, 0.25, 0.3, 0.35, and 0.4.
- the ideal maximum transmittance after passing the bottom polarizer 23 b and the top polarizer 23 a is 0.5.
- FIG. 51 is a schematic cross-sectional view of a display device according to a seventh embodiment of the invention.
- a display device 100 g of the present embodiment is similar to the display device 100 a of the first embodiment.
- a difference therebetween lies in that, in the display device 100 g, the bottom polarizer 23 b is an O-type polarizer, and the top polarizer 23 a is an E-type polarizer, for example.
- the absorption axis of the O-type polarizer follows an orientation angle ⁇ of 0°.
- the c-axis (i.e. transmission axis) of the E-type polarizer follows the orientation angle ⁇ of 0°.
- the top polarizer 23 a (E-type polarizer) transmits the extraordinary ray and absorbs the ordinary ray.
- the top polarizer 23 a (E-type polarizer) weakens light which is not perpendicular to any transmission direction of the c-axis.
- the first compensation film 28 b and the second compensation film 28 a are disposed between the top polarizer 23 a and the bottom polarizer 23 b.
- FIG. 52 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the seventh embodiment of the invention employs compensation films.
- the polarization state of the directional light 181 after passing through the bottom polarizer 23 b is a state P 1 .
- the first compensation film 28 b rotates a linearly polarized light from the state P 1 to a circularly polarized light of of a state C 1 . Since circularly polarized light is not affected by the orientation angles, circularly polarized light is applied in the display medium 20 to improve the contrast ratio and bright state performance.
- the second compensation film 28 a shifts the circularly polarized light of the state C 1 to a state A 1 matching the absorption axis of the top polarizer 23 a, in which the display medium 20 is optically isotropic and no voltage is applied.
- FIG. 53 is a contour map of the contrast ratios measured on the display device of FIG. 51 with the parameter setting of Table 14.
- FIG. 53 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle ⁇ of 70° and an orientation angle ⁇ of 270°, in which the contour lines from outside to inside respectively represents the contour lines of contrast ratios 500, 1000, 2000, and 5000.
- FIG. 54 is a contour map for the bright state measurements on the display device of FIG. 51 with the parameter setting of Table 14, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.1, 0.15, 0.2, 0.25, 0.3, 0.35, and 0.4.
- compensation films are disposed between the top and bottom polarizers in the display device according to an exemplary embodiment of the invention.
- the configuration of the compensation films can adjust the polarization state of the directional light entering the display module, such that the polarization state of the directional light matches the absorption axis direction of the top polarizer. Accordingly, light leakage can be minimized and the contrast ratio of the display device can be enhanced.
- the configuration of the compensation films can convert the polarization state of the directional light from the linear polarization state to the circular polarization state for transmission in the display medium. Since the circularly polarized light is not affected by the orientation angle, the viewing angle of the display device can be increased.
Abstract
A display device including a display module, a light source module, a turning optical film, a first compensation film and a second compensation film is provided. The display module includes a first substrate, a second substrate and a display medium. The light source module generates directional light. The display module is disposed above the light source module. The second substrate is disposed opposite to the first substrate. The display medium is disposed between the first substrate and the second substrate and is optically isotropic. The turning optical film is disposed on the second substrate of the display module. The directional light enters the turning optical film and then exits the turning optical film to form an output light. The first compensation film is disposed on the first outer surface of the first substrate. The second compensation film is disposed between the second substrate and the turning optical film.
Description
- This application claims the priority benefits of U.S. provisional application Ser. No. 61/481,295, filed on May 2, 2011 and Taiwan application serial no. 101114566, filed on Apr. 24, 2012. The entirety of each of the above-mentioned patent applications is hereby incorporated by reference herein and made a part of this specification.
- 1. Field of the Invention
- The invention relates to a display device, and more particularly to a liquid crystal display device.
- 2. Description of Related Art
- With vigorous development of display technologies, consumers' requirements for favorable performance of displays have been increasing. Specifically, consumers have high demands for the response time of the displays in addition to the requirements for resolution, contrast ratio, viewing angle, grey level inversion, and color saturation.
- To satisfy said requirements, blue phase liquid crystal displays (LCDs) characterized by fast response speed have been developed in the industry pertinent to displays. For instance, when a positive blue phase liquid crystal material is applied, a transverse electric field is required for operation, such that the positive blue phase liquid crystal material can function as a light valve. At this current stage, positive blue phase liquid crystal molecules in the blue phase LCD are driven by adopting the electrode design of an in-plane switching (IPS) display module.
- However, in the electrode design of a typical IPS display module, many regions above the electrodes do not have transverse electric fields. Consequently, a plurality of liquid crystal molecules in the blue phase LCD cannot be properly driven, such that the transmittance of the display module is low. Although the transmittance of the IPS display module can be enhanced by increasing the driving voltage, the resulting excess power consumption is unfavorable. Accordingly, improving the low transmittance and high driving voltage of the blue phase LCD demand attention from research and developers. Moreover, further enhancement of the contrast ratio and viewing angle of the blue phase LCD is needed.
- The invention provides a display device capable of solving issues of low transmittance and high driving voltage when blue phase liquid crystals are applied in a conventional IPS display module.
- The invention provides a display device including a light source module, a display module, a turning optical film, a first compensation film, and a second compensation film. The light source module generates a directional light. The display module is disposed above the light source module, and the display module includes a first substrate, a second substrate, and a display medium. The first substrate has a first inner surface and a first outer surface. The second substrate is disposed opposite to the first substrate and has a second inner surface and a second outer surface. The display medium is disposed between the first substrate and the second substrate and is optically isotropic. The display medium is optically anisotropic when driven with an electric field. The directional light is not perpendicular to the first outer surface when the directional light enters the display module, and the directional light is not perpendicular to the second outer surface when the directional light exits the display module. The turning optical film is disposed on the second outer surface of the second substrate of the display module. The turning optical film has an incident surface and an output surface. The directional light enters the turning optical film from the incident surface, and exits the turning optical film from the output surface so as to form an output light. Moreover, an included angle is between the output light and the output surface. The first compensation film is disposed on the first outer surface of the first substrate. The second compensation film is disposed between the second substrate and the turning optical film.
- In the display device according to an exemplary embodiment of the invention, the compensation films are disposed between the top polarizer and bottom polarizer. The configuration of the compensation films can adjust the polarization state of the directional light entering the display module, such that the polarization state of the directional light matches the absorption axis direction of the top polarizer. Accordingly, light leakage can be minimized and the contrast ratio and viewing angle of the display device can be enhanced.
- In order to make the aforementioned and other features and advantages of the invention more comprehensible, embodiments accompanying figures are described in detail below.
- The accompanying drawings are included to provide further understanding, and are incorporated in and constitute a part of this specification. The drawings illustrate exemplary embodiments and, together with the description, serve to explain the principles of the invention.
-
FIG. 1 is a schematic cross-sectional view of a display device according to an embodiment of the invention. -
FIG. 2A is a schematic view of an optically isotropic display medium without an electric field. -
FIG. 2B is a schematic view of an optically anisotropic display medium in an electric field. -
FIG. 3A andFIG. 3B are schematic cross-sectional views of a display device according to an embodiment of the invention. -
FIG. 4A is a schematic cross-sectional view of a first optical film in a display device according to an embodiment of the invention. -
FIG. 4B is a perspective view of the first optical film depicted inFIG. 4A . -
FIG. 5A is a schematic cross-sectional view of a second optical film in a display device according to an embodiment of the invention. -
FIG. 5B is a perspective view of the second optical film depicted inFIG. 5A . -
FIG. 6A is schematic cross-sectional view of an optical film in a display device according to an embodiment of the invention. -
FIG. 6B is a perspective view of the optical film depicted inFIG. 6A . -
FIG. 7 is an optical path diagram of light passing through a first optical film, a second optical film, and a turning optical film according an embodiment of the invention. -
FIG. 8A is schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention. -
FIG. 8B is a perspective view of the optical film depicted inFIG. 8A . -
FIG. 9A is schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention. -
FIG. 9B is a perspective view of the optical film depicted inFIG. 9A . -
FIG. 10A is schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention. -
FIG. 10B is a perspective view of the optical film depicted inFIG. 10A . -
FIG. 11 andFIG. 12 are schematic cross-sectional views of a display device according to embodiments of the invention. -
FIG. 13 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance. -
FIGS. 14A and 14B are relational diagrams of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a light angle. -
FIG. 15 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance. -
FIG. 16 is a relational diagram of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a transmittance. -
FIG. 17 depicts the measurement results of a hysteresis phenomenon from a transverse electric field driving blue phase liquid crystals of a conventional IPS display module. -
FIG. 18 depicts the measurement results of a hysteresis phenomenon from a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals. -
FIG. 19 is a relational diagram between display medium thickness and voltage for a display device according to an embodiment of the invention. -
FIG. 20 is a relational diagram between voltage and transmittance under different display thickness conditions for a display device according to an embodiment of the invention. -
FIG. 21 is a schematic cross-sectional view of a display device according to a first embodiment of the invention. -
FIG. 22 is a perspective view of a light source module and a display module in a display device according to an embodiment of the invention. -
FIG. 23 is a schematic view of a Poincaré sphere of a compensation process during a dark state when a display device according to the first embodiment of the invention employs compensation films. -
FIG. 24 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 1. -
FIG. 25 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 2. -
FIG. 26 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 3. -
FIG. 27 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 4. -
FIG. 28 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 5. -
FIG. 29 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 6. -
FIG. 30 is a schematic cross-sectional view of a display device according to a second embodiment of the invention. -
FIG. 31 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the second embodiment of the invention employs compensation films. -
FIG. 32 is a contour map of the contrast ratios measured on the display device ofFIG. 30 with the parameter setting of Table 7. -
FIG. 33 is a schematic cross-sectional view of a display device according to a third embodiment of the invention. -
FIG. 34 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the third embodiment of the invention employs compensation films. -
FIG. 35 is a contour map of the contrast ratios measured on the display device ofFIG. 33 with the parameter setting of Table 8. -
FIG. 36 is a contour map of the contrast ratios measured on the display device ofFIG. 33 with the parameter setting of Table 9. -
FIG. 37 is a schematic cross-sectional view of a display device according to a fourth embodiment of the invention. -
FIG. 38 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fourth embodiment of the invention employs compensation films. -
FIG. 39 is a contour map of the contrast ratios measured on the display device ofFIG. 37 with the parameter setting of Table 10. -
FIG. 40 is a schematic cross-sectional view of a display device according to a fifth embodiment of the invention. -
FIG. 41 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films. -
FIG. 42 is a contour map of the contrast ratios measured on the display device ofFIG. 40 with the parameter setting of Table 11. -
FIG. 43 is a contour map of the bright state measurements on the display device ofFIG. 40 with the parameter setting of Table 11. -
FIG. 44 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films. -
FIG. 45 is a contour map of the contrast ratios measured on the display device ofFIG. 40 with the parameter setting of Table 12. -
FIG. 46 is a contour map of the bright state measurements on the display device ofFIG. 40 with the parameter setting of Table 12. -
FIG. 47 is a schematic cross-sectional view of a display device according to a sixth embodiment of the invention. -
FIG. 48 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the sixth embodiment of the invention employs compensation films. -
FIG. 49 is a contour map of the contrast ratios measured on the display device ofFIG. 47 with the parameter setting of Table 13. -
FIG. 50 is a contour map of the bright state measurements on the display device ofFIG. 47 with the parameter setting of Table 13. -
FIG. 51 is a schematic cross-sectional view of a display device according to a seventh embodiment of the invention. -
FIG. 52 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the seventh embodiment of the invention employs compensation films. -
FIG. 53 is a contour map of the contrast ratios measured on the display device ofFIG. 51 with the parameter setting of Table 14. -
FIG. 54 is a contour map of the bright state measurements on the display device ofFIG. 51 with the parameter setting of Table 14. -
FIG. 1 is a schematic cross-sectional view of a display device according to an embodiment of the invention. With reference toFIG. 1 , adisplay device 100 of the present embodiment includes a display module P, a light source module B, and a turningoptical film 25. - The display module P includes a
first substrate 21 b, asecond substrate 21 a, and adisplay medium 20. - The
first substrate 21 b has an inner surface S1 and an outer surface S2, and apixel array 22 b is disposed on the inner surface S1 of thefirst substrate 21 b. Thefirst substrate 21 b may be made of glass, quartz, an organic polymer, or other suitable materials. According to the present embodiment, thepixel array 22 b includes a plurality of scan lines, a plurality of data lines, and a plurality of pixel units. Each of the pixel units includes an active element and a pixel electrode electrically connected to the active element. Moreover, the active element of the pixel unit is electrically connected to a corresponding data line and a corresponding scan line. The active element may a bottom-gate thin film transistor (TFT) or a top-gate TFT. - The
second substrate 21 a is disposed opposite to thefirst substrate 21 b, and thesecond substrate 21 a has an inner surface S3 and an outer surface S4. Moreover, anopposite electrode 22 a is disposed on the inner surface S3 of thesecond substrate 21 a. Thesecond substrate 21 a may also be made of glass, quartz, an organic polymer, or other suitable materials. Theopposite electrode 22 a completely covers the inner surface S3 of thesecond substrate 21 a. According to the present embodiment, theopposite electrode 22 a is a transparent electrode, and a material of the transparent electrode includes a metal oxide such as indium tin oxide (ITO), indium zinc oxide (IZO), aluminum tin oxide (ATO), aluminum zinc oxide (AZO), indium germanium zinc oxide, other suitable metal oxides, or a stacked layer having at least two of the above materials. - It should be noted that, a color filter array may be disposed on the
first substrate 21 b or thesecond substrate 21 a, so that the display module P can display color images. However, the invention is not limited thereto. - The
display medium 20 is disposed between thepixel array 22 b of thefirst substrate 21 b and theopposite electrode 22 a of thesecond substrate 21 a. Moreover, thedisplay medium 20 is optically isotropic when no electric field is applied thereto, as shown inFIG. 2A . Thedisplay medium 20 is optically anisotropic when a perpendicularelectric field 201 is applied thereto, as shown inFIG. 2B . In other words, when no electric field is generated between thepixel array 22 b and theopposite electrode 22 a, thedisplay medium 20 displays properties of optical isotropy. When the perpendicularelectric field 201 is generated between thepixel array 22 b and theopposite electrode 22 a, thedisplay medium 20 displays properties of optical anisotropy. According to the present embodiment, thedisplay medium 20 includes blue phase liquid crystals, such as polymer-stabilized blue phase liquid crystals or polymer-stabilized isotropic phase liquid crystals. Since thedisplay medium 20 switches between optically isotropic and optically anisotropic by the generation of electric fields, such that thedisplay medium 20 functions as a light valve, the response speed of this type ofdisplay medium 20 is preferably faster than the twisting response speed of the conventional twisted nematic liquid crystal molecules. - The light source module B is disposed below the outer surface S2 of the
first substrate 21 b of the display module P. Moreover, the light source module B generates adirectional light 281. In other words, the directional light 281 projects along a specific projected direction and distributes within a specific angle. In the present embodiment, thedirectional light 281 is concentrated within a specific range. That is, thedirectional light 281 has directionality and is not like the conventional scattered light source with light spreading in all directions without any directionality. The light source module B is, for example, a side incident type light source module, including alight guide plate 26 a and alight source 26 b. It should be appreciated that the light source module B may further include elements such as an optical film set and a frame. In the present embodiment, the side incident type light source module is used as an example for description, although the invention is not limited thereto. According to other embodiments, the light source module B may be a light source module having other forms, such as the direct type light source module, for example. - Since the
display medium 20 is optically anisotropic when no electric field is applied thereto, therefore, when thepixel array 22 b of the display module P and theopposite electrode 22 a form the perpendicularelectric field 201 therebetween, thedisplay medium 20 not only display properties of optical anisotropy, but thedisplay medium 20 is also vertically aligned along the perpendicularelectric field 201, as shown inFIGS. 1 and 2B . In order for the vertically aligned opticallyanisotropic display medium 20 to be birefringent to the light from the light source module B, in the present embodiment, the propagating direction of the light from the light source module B has a specific design as illustrated below. - According to the present embodiment, the
directional light 281 generated by the light source module B propagates along an incident direction D1 when thedirectional light 281 enters the display module P. Moreover, the incident direction D1 is not perpendicular to the outer surface S2 of thefirst substrate 21 b. In other words, thedirectional light 281 generated by the light source module B does not perpendicularly enter into the display module P, but thedirectional light 281 is incident at a specific inclination angle into the display module P. In order for thedirectional light 281 generated by the light source module B to exit the light source module B at a specific angle, special optical microstructures can be designed on thelight guide plate 26 a. Alternatively, a layer of optical film having special optical microstructures may be disposed on thelight guide plate 26 a. Accordingly, when the light generated by thelight source 26 b passes thelight guide plate 26 a (or optical film), the propagating direction of the light changes, such that thedirectional light 281 generated by the light source module B exits at the specific inclination angle. According to the present embodiment, since thedirectional light 281 generated by the light source module B exits at the specific inclination angle, therefore, an included angle θ1 between the incident direction D1 of thedirectional light 281 and the outer surface S2 of thefirst substrate 21 b is 5°˜45°, for example. In other words, an inclination angle θ1′ of thedirectional light 281 generated by the light source module B is 45°˜85°, for example. The inclination angle θ1′ refers to the included angle between the incident direction D1 of thedirectional light 281 and a perpendicular axial line V. - Accordingly, after the direction light 281 enters the display module P at the inclination angle θ1′, a
directional light 282 is formed. Thedirectional light 282 in the display module P maintains the same direction when passing through thedisplay medium 20. In other words, thedirectional light 281 generated by the light source module B becomes thedirectional light 282 when entering thedisplay medium 20. Moreover, thedirectional light 282 propagates along an incident direction D2 not perpendicular to the inner surface S1 of thefirst substrate 21 b. Therefore, the included angle θ between the incident direction D2 of thedirectional light 282 and the inner surface S1 of thefirst substrate 21 b is not equal to 90°. According to the present embodiment, the included angle θ between the incident direction D2 of thedirectional light 282 and the inner surface S1 of thefirst substrate 21 b is 5°˜45°, for example. - After the directional light 282 passes through the
display medium 20 and thesecond substrate 21 a, thedirectional light 282 is guided by the turningoptical film 25 to form anoutput light 283 propagating along a propagating direction D3. Moreover, an included angle between the propagating direction D3 and a surface (output surface) of the turningoptical film 25 is substantially 60°˜120°. In the present embodiment, theoutput light 283 exits the turningoptical film 25 perpendicularly. Therefore, the included angle between the propagating direction D3 and the surface (output surface) of the turning optical film is substantially 90°, such that theoutput light 283 received by a user'seye 29 is a light propagating along the normal direction. Accordingly, an included angle θ2 between the propagating direction D3 of theoutput light 283 and the surface (output surface) of the turningoptical film 25 is substantially equal to 90°. - In the present embodiment, a first
optical film 24 b may be further disposed on the outer surface S2 of thefirst substrate 21 b, such that thedirectional light 282 maintains the same propagating or transmitting direction as much as possible before entering thedisplay medium 20. Moreover, in order for thedirectional light 282 to maintain the same propagating or transmitting direction as much as possible after exiting thedisplay medium 20, a secondoptical film 24 a may be further disposed on the outer surface S4 of thesecond substrate 21 a. - With reference to
FIGS. 1 , 4A, and 4B, the firstoptical film 24 b is disposed on the outer surface S2 of thefirst substrate 21 b. To be specific, the firstoptical film 24 b has a plurality of first optical structures T1. Moreover, the first optical structures T1 allow thedirectional light 281 passing through the first optical structures T1 without generating total reflection. That is, thedirectional light 281 directly passes through the first optical structures T1 of the firstoptical film 24 b. If thedirectional light 281 is not being totally reflected or refracted when directly passing through the first optical structures T1 of the firstoptical film 24 b, optical loss of thedirectional light 281 caused by the firstoptical film 24 b can be minimized. In other words, optical loss of thedirectional light 281 at the interface of air and thefirst substrate 21 b due to reflection can be reduced. Accordingly, thedirectional light 281 can pass through the firstoptical film 24 b in the same propagating direction as much as possible. - According to the present embodiment, the first
optical film 24 b has a first surface S5 and a second surface S6 opposite to the first surface S5. The first surface S5 faces the light source module B, the second surface S6 faces the outer surface S2 of thefirst substrate 21 b, and the first optical structures T1 are disposed on the first surface S5. That is, the second surface S6 of the firstoptical film 24 b is a smooth plane, although the invention is not limited thereto. Moreover, the first optical structures T1 on the first surface S5 of the first optical film 24B can cause thedirectional light 281 of the light source module B to pass through the firstoptical film 24 b as directly as possible. - According to the present embodiment, the first optical structures T1 are grooves having a first side wall W1 and a second side wall W2, as shown in
FIG. 4A . The incident direction D1 is substantially perpendicular to the first side wall W1, and the incident direction D1 is substantially parallel to the second side wall W2. To be specific, in the first optical structures (grooves) T1 of the present embodiment, the first side wall W1 of the grooves T1 is a short side wall, and the second side wall W2 is a long side wall. Moreover, the short side wall W1 is substantially perpendicular to theincident direction D 1. Furthermore, a refractive index of the firstoptical film 24 b is close to a refractive index of thefirst substrate 21 b. Accordingly, when the directional light 281 passes through the first optical structures (grooves) T1, thedirectional light 281 can directly pass through the short side wall W1 without generating total reflection or refraction, such that thedirectional light 281 can pass through the firstoptical film 24 b as directly as possible. In the present embodiment, a width p1 of the first optical structures (grooves) T1 is approximately 5 μm˜100 μm. An included angle θ4 between the first side wall W1 of the first optical structures (grooves) T1 and the perpendicular axial line V is approximately 5°˜45°. An included angle θ3 between the second side wall W2 of the first optical structures (grooves) T1 and the perpendicular axial line V is approximately 45°˜85°. - With reference to
FIGS. 1 , 5A, and 5B, the secondoptical film 24 b is disposed on the outer surface S4 of thesecond substrate 21 a. To be specific, the secondoptical film 24 a has a plurality of second optical structures T2. Moreover, the second optical structures T2 allows thedirectional light 282 passing through the second optical structures T2 without generating total reflection. That is, thedirectional light 282 directly passes through the second optical structures T2 of the secondoptical film 24 a. If thedirectional light 282 is not being totally reflected or refracted when directly passing through the second optical structures T2 of the secondoptical film 24 a, optical loss of thedirectional light 282 caused by the secondoptical film 24 a can be minimized. In other words, optical loss of thedirectional light 282 at the interface of air and the secondoptical film 24 a due to reflection can be reduced. Accordingly, thedirectional light 282 can exit the secondoptical film 24 a in the same transmitting direction as much as possible. - According to the present embodiment, the second
optical film 24 a has a first surface S7 and a second surface S8 opposite to the first surface S7. The first surface S7 faces the outer surface S4 of thesecond substrate 21 a, and the second optical structures T2 are disposed on the second surface S8. That is, the first surface S7 of the secondoptical film 24 a is a smooth plane, although the invention is not limited thereto. Moreover, the second optical structures T2 on the second surface S8 of the secondoptical film 24 a can cause thedirectional light 282 to pass through the secondoptical film 24 a as directly as possible. - According to the present embodiment, the second optical structures T2 are grooves having a first side wall W3 and a second side wall W4, as shown in
FIG. 5A . The incident direction D2 of thedirectional light 282 when passing through the secondoptical film 24 a is perpendicular to the first side wall W3, and the incident direction D2 is parallel to the second side wall W4. To be specific, in the second optical structures (grooves) T2 of the present embodiment, the first side wall W3 is a short side wall, and the second side wall W4 is a long side wall. Moreover, the short side wall W3 is substantially perpendicular to the incident direction D2 of thedirectional light 282. Furthermore, a refractive index of the secondoptical film 24 a is close to a refractive index of thesecond substrate 21 a. Accordingly, when the directional light 282 passes through the second optical structures (grooves) T2, thedirectional light 282 can directly pass through the short side wall W3 without generating total reflection or refraction, such that thedirectional light 282 can pass through the secondoptical film 24 a as directly as possible. In the present embodiment, a width p2 of the second optical structures (grooves) T2 is approximately 5 μm˜100 μm. An included angle θ6 between the first side wall W3 of the second optical structures (grooves) T2 and the perpendicular axial line V is approximately 5°˜45°. An included angle θ5 between the second side wall W4 of the second optical structures (grooves) T2 and the perpendicular axial line V is approximately 45°˜85°. - With reference to
FIGS. 1 , 6A, and 6B, the turningoptical film 25 is disposed on the secondoptical film 24 a. The turningoptical film 25 has a plurality of tuning optical structures T3, such that thedirectional light 282 is totally reflected by the tuning optical structures T3 to form theoutput light 283. Moreover, an included angle between the propagating direction D3 after the output light 283 passes through the turningoptical film 25 and a surface (output surface) S10 of the turningoptical film 25 is 60°˜120°. In the present embodiment, the propagating direction D3 after the output light 283 passes through the turningoptical film 25 is substantially perpendicular to the surface (output surface) S10 of the turningoptical film 25. That is, thedirectional light 282 is totally reflected by the tuning optical structures T3 of the turningoptical film 25 as much as possible to form theoutput light 283. In other words, the tuning optical structures T3 of the turningoptical film 25 is designed mainly to redirect the propagating or transmitting direction of thedirectional light optical film 25. Thereby, theoutput light 283 can exit the turningoptical film 25 perpendicularly to be received by the user'seye 29. - According to the present embodiment, the turning
optical film 25 has a first surface S9 (also referred to as the incident surface) and a second surface S10 (also referred to as the output surface) opposite to the first surface S9. The first surface S9 faces the outer surface S4 of thesecond substrate 21 a, and the tuning optical structures T3 are disposed on the first surface S9. That is, the second surface S10 of the turningoptical film 25 is a smooth plane, although the invention is not limited thereto. Thedirectional light 282 is totally reflected by the tuning optical structures T3 of the turningoptical film 25 by the first surface S9, so as to form theoutput light 283. - According to the present embodiment, the tuning optical structures T3 are grooves having a first side wall W5 and a second side wall W6, as shown in
FIG. 6A . In the present embodiment, the first side wall W5 and the second side wall W6 of the grooves T3 are planar side walls. To be specific, in the optical structures (grooves) T3 of the present embodiment, an included angle θ7 between the first side wall W5 and the perpendicular axial line V is approximately 5°˜60°, and an included angle θ8 between the second side wall W6 and the perpendicular axial line V is approximately 15°˜45°. Therefore, when thedirectional light 282 enters theoptical film 25, thedirectional light 282 is totally reflected by the first side wall W5 of the tuning optical structures T3 so as to form theoutput light 283, such that theoutput light 283 can exit the turningoptical film 25 perpendicularly. In the present embodiment, a width p3 of the optical structures (grooves) T3 is approximately 5 μm˜100 μm. - In
FIG. 7 , the optical paths of thedirectional light optical film 24 b, secondoptical film 24 a, and the turningoptical film 25 are illustrated. In order to clearly depict the optical paths of thedirectional light 281, thedirectional light 282, and theoutput light 283 respectively passing through the firstoptical film 24 b, the secondoptical film 24 a, and the turningoptical film 25, only the firstoptical film 24 b, the secondoptical film 24 a, and the turningoptical film 25 are drawn inFIG. 7 . That is, the display module P and other film layers are omitted in the drawing. - As shown in
FIG. 7 , the directional light 281 passes through the firstoptical film 24 b as directly as possible without generating total reflection or refraction. Thedirectional light 282 then passes through the secondoptical film 24 a also as directly as possible without generating total reflection or refraction. Thedirectional light 282 is then totally reflected as much as possible by the tuning optical structures T3 of the turningoptical film 25, so as to form theoutput light 283. By using the afore-described configuration of the firstoptical film 24 b, the secondoptical film 24 a, and the turningoptical film 25, light from the light source module B can obliquely enter into the display module P and then exit the turningoptical film 25 along the normal direction. - With reference to
FIG. 1 , besides the display module P, the light source module B, and the turningoptical film 25, thedisplay device 100 of the present embodiment may further include abottom polarizer 23 b and atop polarizer 23 a. Thebottom polarizer 23 b is disposed between thefirst substrate 21 b and the firstoptical film 24 b, and thetop polarizer 23 a is disposed between thesecond substrate 21 a and the secondoptical film 24 a. Dichroic polymer films, such as polyvinyl-alcohol-based films may be adopted for thebottom polarizer 23 b and thetop polarizer 23 a. An included angle between a transmission axis of thebottom polarizer 23 b and a transmission axis of thetop polarizer 23 a may be 5°˜175°. - Moreover, in order to achieve favorable display quality for the display module P, the display module P of the present embodiment further includes a
compensation film 231 and adiffusion film 27. Thecompensation film 231 is disposed between thebottom polarizer 23 b and thetop polarizer 23 a. In the present embodiment, thecompensation film 231 is disposed between thebottom polarizer 23 b and thefirst substrate 21 b as an example for description. In other words, a compensation film (not drawn) may also be disposed between thetop polarizer 23 a and thesecond substrate 21 a. Alternatively, thecompensation film 231 may be disposed between thebottom polarizer 23 b and thefirst substrate 21 b, and the compensation film (not drawn) may be disposed between thetop polarizer 23 a and thesecond substrate 21 a. The configuration of thecompensation film 23 a can enhance the contrast ratio of the display module P as well as the viewing angle. Moreover, thediffusion film 27 is disposed above thetop polarizer 23 a, so that a diffusion effect is generated when the output light 283 passes through thediffusion film 27, thereby achieving preferable display quality for the display module P. However, the use of thediffusion film 27 is not necessary in the invention. - Accordingly, since the
display medium 20 of the display module P of the present embodiment is driven by the perpendicularelectric field 201 between thepixel array 22 b and theopposite electrode 22 a, the low transmittance and high driving voltage issues of the conventional IPS display module can be resolved. Moreover, since the incident direction D2 of thedirectional light 281 and thedirectional light 282 generated by the light source module B in the present embodiment are not perpendicular to the surface of thefirst substrate 21 b when entering thedisplay medium 20, thedisplay medium 20 is still birefringent to thedirectional light 282 of the light source module B when thedisplay medium 20 is driven and becomes optically anisotropic. Accordingly, the display module P can display images. - In the embodiment depicted in
FIG. 1 , thetop polarizer 23 a is disposed between thesecond substrate 21 a and the secondoptical film 24 a. Thereby, the effect from the secondoptical film 24 a and the turningoptical film 25 on the polarization state of thedirectional light 282 is minimized. However, the invention is not limited thereto. According to other embodiments, thetop polarizer 23 a may also be disposed above the secondoptical film 24 a or the turningoptical film 25, as shown inFIG. 3A . - Moreover, according to another embodiment, the second
optical film 24 b may be omitted in the display module P, as shown inFIG. 3B . Accordingly, the effect from the secondoptical film 24 a on the polarization state of thedirectional light 282 is minimized. However, the invention is not limited thereto. - Furthermore, in the embodiment depicted in
FIG. 1 , theoptical film 25 of the display module P are shown inFIGS. 6A and 6B , for example. However, the invention is not limited thereto. According to other embodiments, theoptical film 25 of thedisplay device 100 may also adopt other forms or structures, as further elaborated below. -
FIG. 8A is a schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.FIG. 8B is a perspective view of the optical film depicted inFIG. 8A . With reference toFIGS. 8A and 8B , the tuning optical structures T3′ of theoptical film 25 in the present embodiment are grooves, a first side wall W5′ of the optical structures (grooves) T3 is a curved side wall, and a second side wall W6′ of the optical structures (grooves) T3′ is a planar side wall. Therefore, when thedirectional light 282 enters theoptical film 25, thedirectional light 282 is totally reflected by the first side wall (curved side wall) W5′ of the tuning optical structures T3′ so as to form theoutput light 283, such that theoutput light 283 can exit the turningoptical film 25 perpendicularly. It should be noted that, since the first side wall W5′ is a curved side wall, besides thedirectional light 282 generating total reflection at the first side wall (curved side wall) W5′, a part of theoutput light 283 generated by total reflection has an incident angle that is less than a total reflection angle. Therefore, after the part of theoutput light 283 is reflected to the first side wall (curved side wall) W5′, the part of theoutput light 283 is refracted out of theoptical film 25. Therefore, when the curved side wall is adopted for the first side wall W5′ of the optical structures (grooves) T3′, the included angle between the propagating direction of theoutput light 283 and the output surface can be 60°˜120°. That is, theoutput light 283 can be diffused when emitted, thereby enhancing the image quality. In the present embodiment, a width p4 of the optical structures (grooves) T3′ is approximately 5 μm˜100 μm. - In the embodiment depicted in
FIGS. 8A and 8B , the radaii of curvature of the curved side walls W5′ of all the tuning optical structures T3′ in the turningoptical film 25 are the same. Therefore, each tuning optical structure T3′ in the turningoptical film 25 of the embodiment depicted inFIGS. 8A and 8B has the same pattern. However, the invention is not limited thereto. According to other embodiments, the optical structures of the turningoptical film 25 may have different patterns, as shown inFIGS. 9A and 9B . -
FIG. 9A is a schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.FIG. 9B is a perspective view of the optical film depicted inFIG. 9A . With reference toFIGS. 9A and 9B , in the present embodiment, each tuning optical structure T3′ of the turningoptical film 25 has a planar side wall and a curved side wall, but the radii of curvature of the curved side walls of the tuning optical structures T3′ are not all the same. For example, a radius of curvature of the curved side wall W5′ of the tuning optical structure T3′ in the present embodiment is different than a radius of curvature of a curved side wall W5″. Moreover, the tuning optical structure T3′ having the curved side wall W5′ with the larger radius of curvature is alternatively arranged with the optical structure T3′ having the curved side wall W5′ with the smaller radius of curvature. -
FIG. 10A is a schematic cross-sectional view of an optical film in a display device according to another embodiment of the invention.FIG. 10B is a perspective view of the optical film depicted inFIG. 10A . With reference toFIGS. 10A and 10B , in the present embodiment, each tuning optical structure T3′ of the turningoptical film 25 has a planar side wall and a curved side wall, and the curved side wall of each tuning optical structure T3′ has a plurality of radii of curvature. The radii of curvature of the curved side wall progressively decrease as the bottom of the groove T3′ is approached. For example, the first side wall of the grooves T3′ in the turningoptical film 25 is a curved side wall, including a curved side walls W5-1 and a curved side wall W5-2. Moreover, the radius of curvature of the curved side wall W5-1 is smaller than the radius of curvature of the curved side wall W5-2. In order to facilitate the description, the present embodiment uses two different curvatures for the curved side walls W5-1 and W5-2 as an illustrative example, although in actuality the first side wall of the grooves T3′ in the turningoptical film 25 is a continuous curved surface. - Based on the above, when the
directional light 282 enters the turningoptical film 25, besides thedirectional light 282 generating total reflection at the curved side walls W5-1 and W5-2, a part of theoutput light 283 can be refracted out of theoptical film 25 after being reflected to the curved side wall W5-1. Since the radius of curvature of the curved side wall W5-1 progressively decreases as the bottom of the grooves T3′ is approached, an included angle between a tangent of the curved side wall W5-1 and the transmission direction of theoutput light 283 also decreases gradually. Accordingly, theoutput light 283 can be easily refracted out of theoptical film 25 after being reflected to this area. That is, the curved side wall W5-1 having the smaller radius of curvature can refractmore output light 283 out theoptical film 25 at this area. In other words, the divergence angle and distribution of light from the turningoptical film 25 depicted inFIGS. 10A and 10B is wider and broader than those of the embodiment illustrated inFIGS. 8A and 8B . -
FIG. 11 andFIG. 12 are schematic cross-sectional views of a display device according to embodiments of the invention. The embodiment shown inFIGS. 11 and 12 is similar to the embodiment shown inFIG. 1 , and thus identical components denoted with the same numerals and will not be repeated herein. A difference between the embodiments inFIGS. 11 and 1 lies in that, apixel array 221 b has a slitalignment pattern 60, and a protrudingalignment pattern 70 is disposed on anopposite electrode 221 a. By configuring theslit alignment pattern 60 on thepixel array 221 b and the protrudingalignment pattern 70 on theopposite electrode 221 a, the distribution of a perpendicularelectric field 202 changes and multi-domain alignment is achieved for thedisplay medium 20, accordingly. Similarly, a difference between the embodiments inFIGS. 12 and 1 lies in that, thepixel array 221 b has the slitalignment pattern 60, and theopposite electrode 221 a has a slitalignment pattern 80. The distribution of the perpendicularelectric field 202 can also be changed by configuring theslit alignment pattern 60 on thepixel array 221 b and theslit alignment pattern 80 on theopposite electrode 221 a, thereby achieving multi-domain alignment for thedisplay medium 20. - Although the embodiments depicted in
FIGS. 11 and 12 configure alignment patterns (e.g. slit alignment patterns or protruding alignment patterns) on thepixel array 221 b and theopposite electrode 221 a, the invention is not limited thereto. According to other embodiments, alignment patterns (e.g. slit alignment patterns or protruding alignment patterns) may only be disposed on thepixel array 221 b, or alignment patterns (e.g. slit alignment patterns or protruding alignment patterns) may only be disposed in theopposite electrode 221 a. The combination of alignment patterns on thepixel array 221 b and theopposite electrode 221 a is also not limited to the embodiments depicted inFIGS. 11 and 12 . In other words, the protruding alignment pattern may be disposed on thepixel array 221 b and the slit alignment pattern may be disposed on theopposite electrode 221 a, or the protruding alignment pattern may be disposed on thepixel array 221 b and the protruding alignment pattern may be disposed on theopposite electrode 221 a - In order to illustrate that the display device according to an exemplary embodiment has lower driving voltage and preferable transmittance compared to the conventional IPS display device, several examples with comparison to the conventional IPS display device are set forth below.
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FIG. 13 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance. With reference toFIG. 13 , the horizontal axis ofFIG. 13 represents voltage (V), while the vertical axis represents the transmittance of the display module. As shown inFIG. 13 , when the conventional IPS display module drives the blue phase liquid crystals, the driving voltage needs to reach 52 V to achieve a preferable transmittance. That is, the driving voltage needs to reach 52 V in order for the display module to have a Kerr constant of 12.68 nm/V2. -
FIGS. 14A and 14B are relational diagrams of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a light angle. The horizontal axis ofFIGS. 14A and 14B represent an inclination angle of light from a light source module (e.g. the angle θ1′ depicted inFIG. 1 ), and the vertical axis represents voltage (V). - With reference to
FIG. 14A , a display medium thickness (also referred to as the cell gap) of the display module in this display device is 3.5 μm, and the display module ofFIG. 14A has a Kerr constant of 12.68 nm/V2. As shown inFIG. 14A , the driving voltage (below 15 V) needed by the display module ofFIG. 14A is far lower than the driving voltage (52 V) needed by the IPS display module ofFIG. 13 . Moreover, in the display device ofFIG. 14A , when the inclination angle of light from the light source module increases, the driving voltage thereof decreases. - With reference to
FIG. 14B , a display medium thickness (also referred to as the cell gap) of the display module in this display device is 5 μm, and the display module ofFIG. 14B has the same Kerr constant of 12.68 nm/V2. As shown inFIG. 14B , the driving voltage (below 18 V) needed by the display module ofFIG. 14B is far lower than the driving voltage (52 V) needed by the IPS display module ofFIG. 13 . Similarly, in the display device ofFIG. 14B , when the inclination angle of light from the light source module increases, the driving voltage thereof decreases. -
FIG. 15 is a relational diagram of a voltage of a transverse electric field driving blue phase liquid crystals of a conventional IPS display module and a transmittance. With reference toFIG. 15 , the horizontal axis ofFIG. 15 represents voltage (V), while the vertical axis represents the transmittance of the display module. InFIG. 15 , a laser light of 633 nm serves as the light from the light source module, and the laser light enters the IPS display module perpendicularly. As shown inFIG. 15 , the display module has the greatest transmittance when the driving voltage reaches 193 Vrms. -
FIG. 16 is a relational diagram of a voltage of a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals and a transmittance. With reference toFIG. 16 , the horizontal axis ofFIG. 16 represents voltage (V), while the vertical axis represents the transmittance of the display module. InFIG. 16 , the 633 nm laser light serves as the light from the light source module, t represents the display medium thickness (also referred to as the cell gap), and θ represents the light inclination angle (angle θ1′ depicted inFIG. 1 ) of the light source module. As shown inFIG. 16 , under combinations of different display medium thicknesses (also referred to as the cell gap) and different light inclination angles, four relational curves of voltage and transmittance can be obtained. However, in the four curves, the driving voltages required for the display module to achieve the highest transmittance condition are all far lower than the driving voltage (193 Vrms) needed by the conventional IPS display module. - Blue phase liquid crystals typically exhibit the hysteresis phenomeon. When blue phase liquid crystals are applied in the display medium of the display device, hysteresis usually needs to be suppressed or reduced to prevent the hysteresis of the blue phase liquid crystals from affecting the gray level control accuracy of the display module.
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FIG. 17 depicts the measurement results of a hysteresis phenomenon from a transverse electric field driving blue phase liquid crystals of a conventional IPS display module.FIG. 18 depicts the measurement results of a hysteresis phenomenon from a perpendicular electric field of a display device according to an embodiment of the invention driving blue phase liquid crystals. Generally speaking, the hysteresis phenomenon of blue phase liquid crystals can be measured by gradually increasing voltage to measure the voltage and transmittance curves M and M′, and by gradually decreasing voltage to measure the voltage and transmittance curves N and N′. The voltage difference between the two curves M and N (M′ and N′) under a half transmittance condition is then calculated. As the voltage difference between the two curves M and N (M′ and N′) increases, the hysteresis phenomenon is more apparent. On the other hand, as the voltage difference between the two curves M and N (M′ and N′) decreases, the hysteresis phenomenon is less apparent. - As shown in
FIGS. 17 and 18 , the voltage difference between the curves M and N (FIG. 17 ) under the half transmittance condition is significantly greater than the voltage difference between the curves M′ and N′ (FIG. 18 ) under the half transmittance condition. Therefore, the blue phase liquid crystals of the conventional IPS display module driven by the transverse electric field exhibit high hysteresis. -
FIG. 19 is a relational diagram between display medium thickness and voltage for a display device according to an embodiment of the invention. The horizontal axis inFIG. 19 represents the display medium thickness (also referred to as the cell gap), and the vertical axis represents voltage (V). InFIG. 19 , the 550 nm laser light serves as the light from the light source module, θ represents the light inclination angle (angle θ1′ depicted inFIG. 1 ) of the light source module, and the four curves inFIG. 19 can all allow the display module to have a Kerr constant of 10.2 nm/V2. As shown inFIG. 19 , as the display medium thickness (also referred to as the cell gap) decreases, the required driving voltage is also reduced. -
FIG. 20 is a relational diagram between voltage and transmittance under different display medium thickness conditions for a display device according to an embodiment of the invention. The horizontal axis ofFIG. 20 represents voltage (V), while the vertical axis represents the transmittance. InFIG. 20 , the display medium thickness (also referred to as the cell gap) are respectively 1, 2, and 5 μm, the 550 nm laser light serves as the light from the light source module, and the light inclination angle (angle θ1′ depicted inFIG. 1 ) of the light source module is 70°. As shown inFIG. 20 , the driving voltage of the display device according to an embodiment of the invention is related to the display medium thickness. - Based on the above, in the display device according to an embodiment of the invention, the display medium of the display module is driven by the perpendicular electric field generated between the pixel array and the electrode layer. In particular, since the incident direction of the light generated by the light source module when entering the display medium is not perpendicular to the inner surface of the first substrate, the display medium remains birefringent to the light from the light source module when the display medium is driven to be optically anisotropic. Accordingly, since the display device according to an exemplary embodiment can adopt the perpendicular electric field to drive the display medium, the issues of low transmittance and high driving voltage from conventionally using the transverse electric field to drive the blue phase liquid crystals can be resolved.
- Moreover, the display device according to an exemplary embodiment can further include a plurality of compensation films, which can be configured to enhance the display quality of the display device. Embodiments 1-7 provided below to further illustrate the advantages of configuring the compensation films. It should be noted that, the embodiments provided below are similar to the embodiment shown in
FIG. 1 , and thus identical components denoted with the same numerals and will not be repeated herein. The omitted portions can be referenced to the earlier embodiments. The differences between the embodiments are further described below. -
FIG. 21 is a schematic cross-sectional view of a display device according to a first embodiment of the invention. With reference toFIG. 21 , a difference between adisplay device 100 a and the embodiment ofFIG. 1 lies in that, thedisplay device 100 a includes afirst compensation film 28 b and asecond compensation film 28 a, and does not include thecompensation film 231. To be specific, thefirst compensation film 28 b is disposed on the outer surface S2 of thefirst substrate 21 b, and thesecond compensation film 28 a is disposed between thesecond substrate 21 a and the turningoptical film 25. - In the present embodiment, the
bottom polarizer 23 b is disposed on the outer surface S2 of thefirst substrate 21 b, and thetop polarizer 23 a is disposed on the outer surface S4 of thesecond substrate 21 a. According to the present embodiment, thebottom polarizer 23 b is disposed between thefirst compensation film 28 b and the firstoptical film 24 b. Thetop polarizer 23 a is disposed between thesecond compensation film 28 a and the secondoptical film 24 a, and the secondoptical film 24 a is disposed between the turningoptical film 25 and thetop polarizer 23 a. According to the present embodiment, the directional light 282 passes through thebottom polarizer 23 b, thefirst compensation film 28 b, thesecond compensation film 28 a, and thetop polarizer 23 a in sequence. - According to the present embodiment, the
first compensation film 28 b and thesecond compensation film 28 a may be used to adjust the polarization state of thedirectional light 282 located in the display module P, such that the polarization state of thedirectional light 282 after adjustment matches the absorption axis direction of thetop polarizer 23 a. Thereby, the light leakage generated when the directional light 282 forms theoutput light 283 can be reduced, and the contrast ratio of thedisplay device 100 a in the dark state can be further enhanced. - In order to further describe the effects of the
first compensation film 28 b and thesecond compensation film 28 a, a Poincaré sphere is used to illustrate the compensation process of thefirst compensation film 28 b and thesecond compensation film 28 a. To clearly define the directions of thedirectional light 281 and thedirectional light 282, as well as the absorption axis angles of thetop polarizer 23 a, thebottom polarizer 23 b, thefirst compensation film 28 b, and thesecond compensation film 28 a, a polar angle θ and an orientation angle Φ are used for the definitions below. -
FIG. 22 is a perspective view of a light source module and a display module in the display device according to an embodiment of the invention. With reference toFIG. 22 , with the center of the display module P as reference, the orientation angle Φ is an included angle between a projection line on the XY plane of an arbitrary direction D4 and the X direction. The polar angle θ is an included angle between the arbitrary direction D4 and the Z direction. For example, the polar angle θ of a direction D5 is 90° and the orientation angle Φ is 0°; the polar angle θ of a direction D6 is 90° and the orientation angle Φ is 90°; the polar angle θ of a direction D7 is 90° and the orientation angle Φ is 180°; and the polar angle θ of a direction D8 is 90° and the orientation angle Φ is 270°. -
FIG. 23 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the first embodiment of the invention employs compensation films. With reference toFIG. 23 , when the polar angle θ of thedirectional light 282 is 70° and the orientation angle Φ is 270°, an effective angle between thebottom polarizer 23 b and thetop polarizer 23 a changes. Therefore, a transmissive state P1 of thedirectional light 282 and a state A1 of the absorption axis of thetop polarizer 23 a are separated, thereby causing the light leakage. According to the present embodiment, thefirst compensation film 28 b can rotate the polarization state of the directional light 282 from the state P1 to a state P0, and thesecond compensation film 28 a can rotate the polarization state of the directional light 282 from the state P0 to the state A1. Accordingly, after the directional light 282 passes through thefirst compensation film 28 b and thesecond compensation film 28 a, the polarization state of thedirectional light 282 can be rotated from the state P1 to the state A1, and thereby prevent light leakage. - Table 1 tabulates a parameter setting data of each component in the
display device 100 a, in which Nz denotes the ratio of refractive index anisotropy, and Nz can be represented by the following equation: -
Nz=(n x −n z)/(n x −n y) - in which is nx the x-axis refractive index, ny the y-axis refractive index, nz the z-axis refractive index, d(nx−ny) is the phase difference, and the incident light refers to the
directional light 281.FIG. 24 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 1. -
TABLE 1 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 45° First Compensation Film Φ = 38.5° Nz = 0.54 d(nx − ny) = 256 nm Second Compensation Film Φ = −38.5° Nz = 0.54 d(nx − ny) = 256 nm Top Polarizer Φ = −45° - With reference to
FIG. 24 , the four contour lines from outside to inside respectively represents the contour lines ofcontrast ratios FIG. 24 , the viewing cone of contrast ratio greater than 1000:1 is approximately 20°, and the 20° viewing cone is sufficient for the straightdirectional light 282 in the vertical field switching blue phase LCD. In order to widen the viewing angle, thefront diffusion film 27 or the turningoptical film 25 can be used to diffuse the straight backlight source, so as to achieve the wide viewing angle. However, the invention is not limited thereto. An example of other parameter settings is provided below to optimize the contrast ratio. - Table 2 tabulates a parameter setting data of each component in the
display device 100 a.FIG. 25 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 2. -
TABLE 2 Incident Light θ = 60° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 45° First Compensation Film Φ = 42° Nz = 0.63 d(nx − ny) = 260 nm Second Compensation Film Φ = −42° Nz = 0.63 d(nx − ny) = 260 nm Top Polarizer Φ = −45° - The contour line area of contrast ratio 1000:1 in
FIG. 25 is greater than the contour line area of contrast ratio 1000:1 inFIG. 24 . However, the smaller polar angle of the incident light results in higher driving voltage. - Table 3 tabulates a parameter setting data of each component in the
display device 100 a.FIG. 26 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 3. -
TABLE 3 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 40° First Compensation Film Φ = 36° Nz = 0.506 d(nx − ny) = 259 nm Second Compensation Film Φ = −36° Nz = 0.506 d(nx − ny) = 259 nm Top Polarizer Φ = −40° - Table 4 tabulates a parameter setting data of each component in the
display device 100 a.FIG. 27 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 4.FIG. 27 illustrates the contour lines of the optimized contrast ratio for an incident light with a polar angle θ of 70° and an orientation angle Φ of 270°. -
TABLE 4 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 30° First Compensation Film Φ = 29.75° Nz = 0.399 d(nx − ny) = 272 nm Second Compensation Film Φ = −29.75° Nz = 0.399 d(nx − ny) = 272 nm Top Polarizer Φ = −30° - Table 5 tabulates a parameter setting data of each component in the
display device 100 a.FIG. 28 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 5.FIG. 28 illustrates the contour lines of the optimized contrast ratio for an incident light with a polar angle θ of 70° and an orientation angle Φ of 270°. -
TABLE 5 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 30° First Compensation Film Φ = 31° Nz = 0.44 d(nx − ny) = 264 nm Second Compensation Film Φ = −31° Nz = 0.44 d(nx − ny) = 264 nm Top Polarizer Φ = −30° - Table 6 tabulates a parameter setting data of each component in the
display device 100 a.FIG. 29 is a contour map of the contrast ratios measured on the display device ofFIG. 21 with the parameter setting of Table 6.FIG. 29 illustrates the contour lines of the optimized contrast ratio for an incident light with a polar angle θ of 60° and an orientation angle Φ of 270°. -
TABLE 6 Incident Light θ = 60° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 30° First Compensation Film Φ = 32.5° Nz = 0.4775 d(nx − ny) = 264.5 nm Second Compensation Film Φ = −32.5° Nz = 0.4775 d(nx − ny) = 264.5 nm Top Polarizer Φ = −30° -
FIG. 30 is a schematic cross-sectional view of a display device according to a second embodiment of the invention. With reference toFIG. 30 , adisplay device 100 b of the present embodiment is similar to thedisplay device 100 a of the first embodiment. A difference therebetween lies in that, thedisplay device 100 b further includes athird compensation film 31 b and afourth compensation film 31 a. Thethird compensation film 31 b is disposed between thefirst compensation film 28 b and thebottom polarizer 23 b, and thefourth compensation film 31 a is disposed between thesecond compensation film 28 a and thetop polarizer 23 a. - According to the present embodiment, the
third compensation film 31 b and thefourth compensation film 31 a are respectively a biaxial compensation film, for example. Thethird compensation film 31 b and thefourth compensation film 31 a may be designed in accordance with different orientation angle Φ, so as to compensate for an angular difference between thetop polarizer 23 a and thebottom polarizer 23 b. According to the present embodiment, the directional light 282 passes through thebottom polarizer 23 b, thethird compensation film 31 b, thefirst compensation film 28 b, thesecond compensation film 28 a, thefourth compensation film 31 a, and thetop polarizer 23 a in sequence. -
FIG. 31 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the second embodiment of the invention employs compensation films. With reference toFIG. 31 , in the present embodiment, a P2 state is shifted from a P1 state. The P2 state represents a polarization state when the orientation angle Φ is 300°, and the P1 state represents a polarization state when the orientation angle Φ is 270°. In the present embodiment, thethird compensation film 31 b can rotate the polarization state from the state P2 to the state P1. Thefirst compensation film 28 b and thesecond compensation film 28 a can then rotate the polarization state from the state P1 to a state A1. Thefourth compensation film 31 a can then rotate the polarization state from the state A1 to a state A2 matching the absorption axis of thetop polarizer 23 a. - Table 7 tabulates a parameter setting data of each component in the
display device 100 b.FIG. 32 is a contour map of the contrast ratios measured on the display device ofFIG. 30 with the parameter setting of Table 7. -
TABLE 7 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 30° Third Compensation Film Φ = 25.75° Nz = 0.851 d(nx − ny) = 281.5 nm First Compensation Film Φ = 29.72° Nz = 0.3984 d(nx − ny) = 272 nm Second Compensation Film Φ = −29.72° Nz = 0.3984 d(nx − ny) = 272 nm Fourth Compensation Film Φ = −25.75° Nz = 0.851 d(nx − ny) = 281.5 nm Top Polarizer Φ = −30° -
FIG. 33 is a schematic cross-sectional view of a display device according to a third embodiment of the invention. With reference toFIG. 33 , adisplay device 100 c of the present embodiment is similar to thedisplay device 100 b of the second embodiment. A difference therebetween lies in that, in thedisplay device 100 c, thethird compensation film 31 b is disposed between thefirst compensation film 28 b and thefirst substrate 21 b, and thefourth compensation film 31 a is disposed between and thesecond compensation film 28 a and thesecond substrate 21 a. - According to the present embodiment, the
third compensation film 31 b and thefourth compensation film 31 a are respectively a biaxial compensation film, for example. Thethird compensation film 31 b and thefourth compensation film 31 a may be designed in accordance with different orientation angles Φ, so as to compensate for an angular difference between thetop polarizer 23 a and thebottom polarizer 23 b. According to the present embodiment, the directional light 282 passes through thebottom polarizer 23 b, thefirst compensation film 28 b, thethird compensation film 31 b, thefourth compensation film 31 a, thesecond compensation film 28 a, and thetop polarizer 23 a in sequence. -
FIG. 34 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the third embodiment of the invention employs compensation films. With reference toFIG. 34 , in the present embodiment, thefirst compensation film 28 b can rotate a polarization state from a state P1 to a state P0. Thethird compensation film 31 b then rotates the polarization state from a linear polarization state of the state P0 to a circular polarization state of a state C1. Thefourth compensation film 31 a then rotates the polarization state from the circular polarization state of the state C1 to the linear polarization state of the state P0. Thesecond compensation film 28 a then rotates the polarization state from the state P0 to a state A1 matching the absorption axis of thetop polarizer 23 a. Since circularly polarized light is not affected by the orientation angles of the blue phase liquid crystal materials, circularly polarized light can improve the viewing angle of the VFS blue phase LCD. - Table 8 tabulates a parameter setting data of each component in the
display device 100 c.FIG. 35 is a contour map of the contrast ratios measured on the display device ofFIG. 33 with the parameter setting of Table 8. -
TABLE 8 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 45° First Compensation Film Φ = 40° Nz = 0.575 d(nx − ny) = 256 nm Third Compensation Film Φ = 90° Nz = 0.5 d(nx − ny) = 137 nm Fourth Compensation Film Φ = 0° Nz = 0.5 d(nx − ny) = 137 nm Second Compensation Film Φ = −40° Nz = 0.575 d(nx − ny) = 256 nm Top Polarizer Φ = −45° - Table 9 tabulates a parameter setting data of each component in the
display device 100 c.FIG. 36 is a contour map of the contrast ratios measured on the display device ofFIG. 33 with the parameter setting of Table 9.FIG. 36 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle θ of 60° and an orientation angle Φ of 270°. -
TABLE 9 Incident Light θ = 60° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 45° First Compensation Film Φ = 42° Nz = 0.63 d(nx − ny) = 260 nm Third Compensation Film Φ = 90° Nz = 0.5 d(nx − ny) = 137 nm Fourth Compensation Film Φ = 0° Nz = 0.5 d(nx − ny) = 137 nm Second Compensation Film Φ = −42° Nz = 0.63 d(nx − ny) = 260 nm Top Polarizer Φ = −45° -
FIG. 37 is a schematic cross-sectional view of a display device according to a fourth embodiment of the invention. With reference toFIG. 37 , adisplay device 100 d of the present embodiment is similar to thedisplay device 100 b of the second embodiment. A difference therebetween lies in that, in thedisplay device 100 d, thebottom polarizer 23 b is a wire-grid polarizer, for example. - In the present embodiment, the
first compensation film 28 b, thesecond compensation film 28 a, thethird compensation film 31 b, and thefourth compensation film 31 a are all disposed between thetop polarizer 23 a and the wire-grid bottom polarizer 23 b. According to the present embodiment, the directional light 282 passes through the wire-grid bottom polarizer 23 b, thethird compensation film 31 b, thefirst compensation film 28 b, thesecond compensation film 28 a, thefourth compensation film 31 a, and thetop polarizer 23 a in sequence. -
FIG. 38 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fourth embodiment of the invention employs compensation films. With reference toFIG. 38 , in the present embodiment, an orientation angle Φ of the absorption axis of the wire-grid bottom polarizer 23 b is 90°, and an orientation angle Φ of the absorption axis of thetop polarizer 23 a is 0°. After the directional light 282 passes through the wire-grid bottom polarizer 23 b, thedirectional light 282 rotates from a state P1 to a linear polarization state of a state P0. - The
third compensation film 31 b does not change the polarization state when the orientation angle Φ is 270°. Thefirst compensation film 28 b rotates the linear polarization state of the state P0 to a circular polarization state of a state C1. Thesecond compensation film 28 a rotates the circularly polarized light from the state C1 to a state A0 matching the absorption axis of thetop polarizer 23 a. Accordingly, a preferable dark state performance can be achieved. - However, when the orientation angle Φ of the
directional light 282 is not the same (e.g. 300°), the polarization state P1 shifts from the polarization state P0. Here, thethird compensation film 31 b can employ different orientation angles Φ (e.g. from 225° to 315°) in order to rotate the state P1 back to the state P0. Thefirst compensation film 28 b and thesecond compensation film 28 a then rotate the polarization state from the state P0 to a state P2 through the state C1. Thefourth compensation film 31 a then polarizes the linearly polarized light from the state P2 to a state A1 matching the absorption axis of thetop polarizer 23 a. - Table 10 tabulates a parameter setting data of each component in the
display device 100 d.FIG. 39 is a contour map of the contrast ratios measured on the display device ofFIG. 37 with the parameter setting of Table 10.FIG. 39 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle θ of 70° and an orientation angle Φ of 270°. -
TABLE 10 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 90° Third Compensation Film Φ = 90° Nz = 0.81 d(nx − ny) = 317.35 nm First Compensation Film Φ = 45° Nz = 0.5 d(nx − ny) = 137 nm Second Compensation Film Φ = −45° Nz = 0.5 d(nx − ny) = 137 nm Fourth Compensation Film Φ = 0° Nz = 0.81 d(nx − ny) = 317.35 nm Top Polarizer Φ = 0° - Since the wire-
grid bottom polarizer 23 b has a favorable extinction ratio, preferably high and broad contour lines can be obtained. Moreover, the wire-grid bottom polarizer 23 b is not sensitive to the incident light 281 angle and has minimal diffusion effect. Therefore, the wire-grid bottom polarizer 23 b is suitable for the VFS blue phase LCD. -
FIG. 40 is a schematic cross-sectional view of a display device according to a fifth embodiment of the invention. With reference toFIG. 40 , adisplay device 100 e of the present embodiment is similar to thedisplay device 100 b of the second embodiment. A difference therebetween lies in that, in thedisplay device 100 e, thetop polarizer 23 a is disposed between the turningoptical film 25 and thediffusion film 27, and thefourth compensation film 31 a includes an A-plate compensation film 31 a-1 and a C-plate compensation film 31 a-2. - According to the present embodiment, the
first compensation film 28 b, thesecond compensation film 28 a, and thethird compensation film 31 b are biaxial compensation films. Thethird compensation film 31 b is disposed between thebottom polarizer 23 b and thefirst compensation film 28 b, and the firstoptical film 24 b is disposed between thethird compensation film 31 b and thefirst compensation film 28 b. Moreover, thefourth compensation film 31 a is disposed between thesecond compensation film 28 a and thetop polarizer 23 a, and the secondoptical film 24 a is disposed between thefourth compensation film 31 a and thetop polarizer 23 a. Specifically, the A-plate compensation film 31 a-1 in thefourth compensation film 31 a is disposed between the C-plate compensation film 31 a-2 and the secondoptical film 24 a. According to the present embodiment, the directional light 282 passes through thebottom polarizer 23 b, thethird compensation film 31 b, the firstoptical film 24 b, thefirst compensation film 28 b, thesecond compensation film 28 a, the C-plate compensation film 31 a-2, the A-plate compensation film 31 a-1, and the secondoptical film 24 a in sequence. Theoutput light 283 is formed after the directional light 282 passes through the turningoptical film 25, and then the output light 283 passes through thetop polarizer 23 a. -
FIG. 41 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films. With reference toFIG. 41 , in the present embodiment, the orientation angles Φ of thebottom polarizer 23 b and thetop polarizer 23 a are respectively 0° and 90°. According to the present embodiment, for thedirectional light 281 having a polar angle θ of 70° and an orientation angle Φ of 270° as an incident angle, when the directional light 281 passes through thebottom polarizer 23 b, the polarization state of thedirectional light 281 is a state P0. However, when the orientation angle Φ of the directional light 281 changes (e.g. 300°), the polarization state of thedirectional light 281 shifts from the state P0 to a state P1. - In the present embodiment, the
third compensation film 31 b does not change the polarization state P0 when the orientation angle Φ is 270°, but when the orientation angle Φ is 200°, the polarization state changes from the state P1 to the state P0. Thefirst compensation film 28 b rotates the linearly polarized light from the state P0 to a circularly polarized light of of a state C1. Thesecond compensation film 28 a rotates the circularly polarized light from the state C1 to the linearly polarized light of of the state P0. Since the polarization state may change with the turningoptical film 25 corresponding to thetop polarizer 23 a, therefore, the C-plate compensation film 31 a-2 is designed to rotate the polarization state from the state P0 to a state P2, and the A-plate compensation film 31 a-1 is used to rotate the polarization state from the state P2 to a state A1 matching the absorption axis of thetop polarizer 23 a. - Table 11 tabulates a parameter setting data of each component in the
display device 100 e, in which no is the fast axis refractive index, ne is the slow axis refractive index, and d is the thickness.FIG. 42 is a contour map of the contrast ratios measured on the display device ofFIG. 40 with the parameter setting of Table 11.FIG. 42 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle θ of 70° and an orientation angle Φ of 270°, in which the contour lines from outside to inside respectively represents the contour lines ofcontrast ratios FIG. 43 is a contour map for the bright state measurements on the display device ofFIG. 40 with the parameter setting of Table 11, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.2, 0.25, 0.3, 0.35, and 0.4. -
TABLE 11 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 0° Third Compensation Film Φ = 0° Nz = 0.756 d(nx − ny) = 254 nm First Compensation Film Φ = −45° Nz = 0.501 d(nx − ny) = 137.5 nm Second Compensation Film Φ = 45° Nz = 0.501 d(nx − ny) = 137.5 nm C-Plate Compensation Film no = 1.5095 ne = 1.511 d = 48 μm A-Plate Compensation Film Φ = 0° no = 1.5095 ne = 1.511 d = 70 μm Top Polarizer Φ = 90° - However, the invention is not limited thereto. Another type of compensation process described below may be adopted by using the framework of the present embodiment.
-
FIG. 44 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the fifth embodiment of the invention employs compensation films. With reference toFIG. 44 , in the present embodiment, thethird compensation film 31 b is used in different orientation angles to compensate the polarization state from the state P 1 to the state P0. Thefirst compensation film 28 b shifts the state P0 to the state P2. Thesecond compensation film 28 a shifts the state P2 back to the state P0. The C-plate compensation film 31 a-2 shifts the state P0 to a state P3, and the A-plate compensation film 31 a-1 shifts the state P3 to the state A1 matching the absorption axis of thetop polarizer 23 a. - Table 12 tabulates a parameter setting data of each component in the
display device 100 e.FIG. 45 is a contour map of the contrast ratios measured on the display device ofFIG. 40 with the parameter setting of Table 12.FIG. 45 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle θ of 70° and an orientation angle Φ of 270°, in which the contour lines from outside to inside respectively represents the contour lines ofcontrast ratios FIG. 46 is a contour map for the bright state measurements on the display device ofFIG. 40 with the parameter setting of Table 12, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.2, 0.25, 0.3, 0.35, and 0.4. -
TABLE 12 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 0° Third Compensation Film Φ = 0° Nz = 0.756 d(nx − ny) = 254 nm First Compensation Film Φ = 112.5° Nz = 0.6738 d(nx − ny) = 275 nm Second Compensation Film Φ = 22.5° Nz = 0.9328 d(nx − ny) = 275 nm C-Plate Compensation Film no = 1.5095 ne = 1.511 d = 65 μm A-Plate Compensation Film Φ = 0° no = 1.5095 ne = 1.511 d = 70 μm Top Polarizer Φ = 90° - As shown in
FIGS. 43 and 46 , the bright state area inFIG. 43 is larger than the bright state area inFIG. 46 . The foregoing result is because during the compensation process ofFIG. 41 , the polarization state of thedirectional light 282 in the blue phase liquid crystal materials is circularly polarized. Since the circularly polarized light is not affected by the orientation angle, the contour lines of the contrast ratio can be improved. -
FIG. 47 is a schematic cross-sectional view of a display device according to a sixth embodiment of the invention. With reference toFIG. 47 , adisplay device 100 f of the present embodiment is similar to thedisplay device 100 e of the fifth embodiment. A difference therebetween lies in that, in thedisplay device 100 f, thethird compensation film 31 b is disposed between thebottom polarizer 23 b and thefirst compensation film 28 b, and thebottom polarizer 23 b is disposed between the firstoptical film 24 b and thethird compensation film 31 b. - According to the present embodiment, the
fourth compensation film 31 a is disposed between thesecond compensation film 28 a and thetop polarizer 23 a, and the secondoptical film 24 a is disposed between thefourth compensation film 31 a and thetop polarizer 23 a. In the present embodiment, thefirst compensation film 28 b, thesecond compensation film 28 a, and thethird compensation film 31 b are biaxial compensation films. Moreover, thefourth compensation film 31 a includes the A-plate compensation film 31 a-1 and the C-plate compensation film 31 a-2. According to the present embodiment, the directional light 282 passes through thebottom polarizer 23 b, thethird compensation film 31 b, thefirst compensation film 28 b, thesecond compensation film 28 a, the C-plate compensation film 31 a-2, the A-plate compensation film 31 a-1, and the secondoptical film 24 a in sequence. Theoutput light 283 is formed after the directional light 282 passes through the turningoptical film 25, and then the output light 283 passes through thetop polarizer 23 a. -
FIG. 48 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the sixth embodiment of the invention employs compensation films. With reference toFIG. 48 , in the present embodiment, a polar angle of thedirectional light 281 is 70° and an orientation angle Φ is 270°, for example. After the backlight passes through thebottom polarizer 23 b, the polarization state of thedirectional light 282 is a state P0. When the orientation angle Φ of the directional light 282 changes, such as when the orientation angle Φ becomes 300°, the polarization state of thedirectional light 282 shifts from the state P0 to a state P1. Thethird compensation film 31 b does not change the polarization state P0 when the orientation angle Φ is 270°, but when the orientation angle Φ is 300°, the polarization state of the polarized light can be changed from the state P1 to the state P0. Thefirst compensation film 28 b shifts a linearly polarized light of the state P0 to a circularly polarized light of a state C1. Thesecond compensation film 28 a shifts the circularly polarized light of the state C1 to the state P0. By using the turningoptical film 25 for depolarization, the absorption axis of thetop polarizer 23 a is shifted to the state A1. The C-plate compensation film 31 a-2 shifts the directional light 282 from the state P0 to a state P2, and the A-plate compensation film 31 a-1 shifts from the state P2 to the state A1 matching the absorption axis of thetop polarizer 23 a. - Table 13 tabulates a parameter setting data of each component in the
display device 100 f.FIG. 49 is a contour map of the contrast ratios measured on the display device ofFIG. 47 with the parameter setting of Table 13.FIG. 49 illustrates the contour lines of the optimized contrast ratio for an incident light 282 with a polar angle θ of 70° and an orientation angle Φ of 270°, in which the contour lines from outside to inside respectively represents the contour lines ofcontrast ratios FIG. 50 is a contour map for the bright state measurements on the display device ofFIG. 47 with the parameter setting of Table 13, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.2, 0.25, 0.3, 0.35, and 0.4. The ideal maximum transmittance after passing thebottom polarizer 23 b and thetop polarizer 23 a is 0.5. -
TABLE 13 Incident Light θ = 70° Φ = 270° λ = 550 nm Bottom Polarizer Φ = 0° Third Compensation Film Φ = 0° Nz = 0.568 d(nx − ny) = 209.6 nm First Compensation Film Φ = −45° Nz = 0.501 d(nx − ny) = 137.5 nm Second Compensation Film Φ = 45° Nz = 0.501 d(nx − ny) = 137.5 nm C-Plate Compensation Film no = 1.5095 ne = 1.511 d = 40 μm A-Plate Compensation Film Φ = 0° no = 1.5095 ne = 1.511 d = 60 μm Top Polarizer Φ = 90° -
FIG. 51 is a schematic cross-sectional view of a display device according to a seventh embodiment of the invention. With reference toFIG. 51 , adisplay device 100 g of the present embodiment is similar to thedisplay device 100 a of the first embodiment. A difference therebetween lies in that, in thedisplay device 100 g, thebottom polarizer 23 b is an O-type polarizer, and thetop polarizer 23 a is an E-type polarizer, for example. - Typically speaking, the absorption axis of the O-type polarizer follows an orientation angle Φ of 0°. Moreover, the c-axis (i.e. transmission axis) of the E-type polarizer follows the orientation angle Φ of 0°. Compared to the
bottom polarizer 23 b (O-type polarizer), thetop polarizer 23 a (E-type polarizer) transmits the extraordinary ray and absorbs the ordinary ray. Thetop polarizer 23 a (E-type polarizer) weakens light which is not perpendicular to any transmission direction of the c-axis. According to the present embodiment, thefirst compensation film 28 b and thesecond compensation film 28 a are disposed between thetop polarizer 23 a and thebottom polarizer 23 b. -
FIG. 52 is a schematic view of a Poincaré sphere for a compensation process during a dark state when a display device according to the seventh embodiment of the invention employs compensation films. With reference toFIG. 52 , in the present embodiment, the polarization state of the directional light 181 after passing through thebottom polarizer 23 b is a state P1. Thefirst compensation film 28 b rotates a linearly polarized light from the state P1 to a circularly polarized light of of a state C1. Since circularly polarized light is not affected by the orientation angles, circularly polarized light is applied in thedisplay medium 20 to improve the contrast ratio and bright state performance. After the directional light 282 passes through thedisplay medium 20 materials, thesecond compensation film 28 a shifts the circularly polarized light of the state C1 to a state A1 matching the absorption axis of thetop polarizer 23 a, in which thedisplay medium 20 is optically isotropic and no voltage is applied. - Table 14 tabulates a parameter setting data of each component in the
display device 100 g.FIG. 53 is a contour map of the contrast ratios measured on the display device ofFIG. 51 with the parameter setting of Table 14.FIG. 53 illustrates the contour lines of the optimized contrast ratio for an incident light 281 with a polar angle θ of 70° and an orientation angle Φ of 270°, in which the contour lines from outside to inside respectively represents the contour lines ofcontrast ratios 500, 1000, 2000, and 5000.FIG. 54 is a contour map for the bright state measurements on the display device ofFIG. 51 with the parameter setting of Table 14, in which the contour lines from outside to inside respectively represents the contour lines of transmittances 0.1, 0.15, 0.2, 0.25, 0.3, 0.35, and 0.4. -
TABLE 14 Incident Light θ = 70° Φ = 270° λ = 550 nm O-Type Polarizer Φ = 0° First Compensation Film Φ = −45° Nz = 0.5 d(nx − ny) = 137.5 nm Second Compensation Film Φ = 45° Nz = 0.5 d(nx − ny) = 137.5 nm C-Axis of the E-Type Polarizer Φ = 0° - In view of the foregoing, compensation films are disposed between the top and bottom polarizers in the display device according to an exemplary embodiment of the invention. The configuration of the compensation films can adjust the polarization state of the directional light entering the display module, such that the polarization state of the directional light matches the absorption axis direction of the top polarizer. Accordingly, light leakage can be minimized and the contrast ratio of the display device can be enhanced. Moreover, the configuration of the compensation films can convert the polarization state of the directional light from the linear polarization state to the circular polarization state for transmission in the display medium. Since the circularly polarized light is not affected by the orientation angle, the viewing angle of the display device can be increased.
- It will be apparent to those skilled in the art that various modifications and variations can be made to the structure of the invention without departing from the scope or spirit of the invention. In view of the foregoing, it is intended that the invention cover modifications and variations of this invention provided they fall within the scope of the following claims and their equivalents.
Claims (27)
1. A display device, comprising:
a light source module generating a directional light;
a display module disposed above the light source module, the display module comprising:
a first substrate having a first inner surface and a first outer surface;
a second substrate disposed opposite to the first substrate and having a second inner surface and a second outer surface; and
a display medium disposed between the first substrate and the second substrate and is optically isotropic, wherein the display medium is optically anisotropic when driven with an electric field, the directional light is not perpendicular to the first outer surface when the directional light enters the display module, and the directional light is not perpendicular to the second outer surface when the directional light exits the display module;
a turning optical film disposed on the second outer surface of the second substrate of the display module, the turning optical film having an incident surface and an output surface, the directional light entering the turning optical film from the incident surface and exiting the turning optical film from the output surface so as to form an output light, wherein an included angle is between the output light and the output surface;
a first compensation film disposed on the first outer surface of the first substrate; and
a second compensation film disposed between the second substrate and the turning optical film.
2. The display device as claimed in claim 1 , further comprising:
a first optical film disposed on the first outer surface of the first substrate, the first optical film having a plurality of first optical structures allowing the directional light passing through the first optical structures without generating total reflection; and
a second optical film disposed on the second outer surface of the second substrate, wherein the second optical film has a plurality of second optical structures substantially allowing the directional light passing through the first optical structures without generating total reflection.
3. The display device as claimed in claim 2 , further comprising:
a bottom polarizer disposed on the first outer surface of the first substrate; and
a top polarizer disposed on the second outer surface of the second substrate.
4. The display device as claimed in claim 3 , wherein the bottom polarizer is disposed between the first compensation film and the first optical film, the top polarizer is disposed between the second compensation film and the second optical film, and the second optical film is disposed between the turning optical film and the top polarizer.
5. The display device as claimed in claim 4 , wherein an orientation angle of the first compensation film is 20°˜50° and Nz is 0.35˜0.75; and an orientation angle of the second compensation film is −20°˜−50° and Nz is 0.35˜0.75.
6. The display device as claimed in claim 3 , further comprising:
a third compensation film disposed between the first compensation film and the bottom polarizer; and
a fourth compensation film disposed between the second compensation film and the top polarizer; and
7. The display device as claimed in claim 6 , wherein the third compensation film and the fourth compensation film are respectively a biaxial compensation film.
8. The display device as claimed in claim 7 , wherein an orientation angle of the first compensation film is 20°˜40° and Nz is 0.25˜0.55; an orientation angle of the second compensation film is −20°˜−40° and Nz is 0.25˜0.55; an orientation angle of the third compensation film is 15°˜35° and Nz is 0.75˜0.95; and an orientation angle of the fourth compensation film is −15°˜−35° and Nz is 0.75˜0.95.
9. The display device as claimed in claim 6 , wherein the bottom polarizer is a wire-grid polarizer.
10. The display device as claimed in claim 9 , wherein an orientation angle of the first compensation film is 30°˜60° and Nz is 0.35˜0.65; an orientation angle of the second compensation film is −30°˜−60° and Nz is 0.35˜0.65; an orientation angle of the third compensation film is −10°˜10° and Nz is 0.71˜0.91; and an orientation angle of the fourth compensation film is 80°˜100° and Nz is 0.71˜0.91.
11. The display device as claimed in claim 3 , further comprising:
a third compensation film disposed between the first compensation film and the first substrate; and
a fourth compensation film disposed between the second compensation film and the second substrate.
12. The display device as claimed in claim 11 , wherein the third compensation film and the fourth compensation film are respectively a biaxial compensation film.
13. The display device as claimed in claim 12 , wherein an orientation angle of the first compensation film is 25°˜55° and Nz is 0.45˜0.75; an orientation angle of the second compensation film is −25°˜−55° and Nz is 0.47˜0.67; an orientation angle of the third compensation film is 80°˜100° and Nz is 0.4˜0.6; and an orientation angle of the fourth compensation film is −10°˜10° and Nz is 0.4˜0.6.
14. The display device as claimed in claim 3 , wherein the first compensation film and the second compensation film are respectively a biaxial compensation film.
15. The display device as claimed in claim 14 , further comprising:
a third compensation film disposed between the bottom polarizer and the first compensation film, and the first optical film is disposed between the third compensation film and the first compensation film; and
a fourth compensation film disposed between the second compensation film and the top polarizer, and the second optical film is disposed between the fourth compensation film and the top polarizer.
16. The display device as claimed in claim 15 , wherein the turning optical film is disposed between the second optical film and the top polarizer.
17. The display device as claimed in claim 16 , wherein the third compensation film is a biaxial compensation film, and the fourth compensation film comprises an A-plate compensation film and a C-plate compensation film.
18. The display device as claimed in claim 17 , wherein an orientation angle of the first compensation film is 100°˜125° and Nz is 0.55˜0.8; an orientation angle of the second compensation film is 10°˜35° and Nz is 0.8˜1.0; an orientation angle of the third compensation film is −10°˜10° and Nz is 0.6˜0.8; an orientation angle of the A-plate compensation film is −10°˜10°, no is 1.4˜1.6, and ne is 1.4˜1.6; and no of the C-plate compensation film is 1.4˜1.6 and ne is 1.4˜1.6.
19. The display device as claimed in claim 14 , further comprising:
a third compensation film disposed between the bottom polarizer and the first compensation film, and the bottom polarizer is disposed between the first optical film and the third compensation film; and
a fourth compensation film disposed between the second compensation film and the top polarizer, and the second optical film is disposed between the fourth compensation film and the top polarizer.
20. The display device as claimed in claim 19 , wherein the turning optical film is disposed between the second optical film and the top polarizer.
21. The display device as claimed in claim 20 , wherein the third compensation film is a biaxial compensation film, and the fourth compensation film comprises an A-plate compensation film and a C-plate compensation film.
22. The display device as claimed in claim 21 , wherein an orientation angle of the first compensation film is −35°˜−55° and Nz is 0.4˜0.6; an orientation angle of the second compensation film is 35°˜55° and Nz is 0.4˜0.6; an orientation angle of the third compensation film is −10°˜10° and Nz is 0.45˜0.65; an orientation angle of the A-plate compensation film is −10°˜10°, no is 1.4˜1.6, and ne is 1.4˜1.6; and no of the C-plate compensation film is 1.4˜1.6 and ne is 1.4˜1.6.
23. The display device as claimed in claim 3 , wherein the bottom polarizer comprises an O-type polarizer, and the top polarizer comprises an E-type polarizer.
24. The display device as claimed in claim 23 , wherein an orientation angle of the first compensation film is −35°˜−55° and Nz is 0.4˜0.6; and an orientation angle of the second compensation film is 35°˜55° and Nz is 0.4˜0.6.
25. The display device as claimed in claim 1 , wherein the included angle is 60°˜120°.
26. The display device as claimed in claim 25 , wherein the included angle is 90°.
27. The display device as claimed in claim 1 , further comprising a diffusion film disposed on the turning optical film.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US13/461,805 US20120280953A1 (en) | 2011-05-02 | 2012-05-02 | Display device |
Applications Claiming Priority (4)
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US201161481295P | 2011-05-02 | 2011-05-02 | |
TW101114566 | 2012-04-24 | ||
TW101114566A TWI465805B (en) | 2012-04-24 | 2012-04-24 | Display device |
US13/461,805 US20120280953A1 (en) | 2011-05-02 | 2012-05-02 | Display device |
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US20120280953A1 true US20120280953A1 (en) | 2012-11-08 |
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ID=47261439
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
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US13/244,284 Expired - Fee Related US8804067B2 (en) | 2011-05-02 | 2011-09-24 | Display device |
US13/461,805 Abandoned US20120280953A1 (en) | 2011-05-02 | 2012-05-02 | Display device |
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US13/244,284 Expired - Fee Related US8804067B2 (en) | 2011-05-02 | 2011-09-24 | Display device |
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CN (1) | CN102759818B (en) |
TW (1) | TWI465803B (en) |
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US11137637B2 (en) | 2017-01-18 | 2021-10-05 | Boe Technology Group Co., Ltd. | Display device with liquid crystal prism |
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Also Published As
Publication number | Publication date |
---|---|
TWI465803B (en) | 2014-12-21 |
US20120307178A1 (en) | 2012-12-06 |
TW201245815A (en) | 2012-11-16 |
CN102759818B (en) | 2015-03-25 |
US8804067B2 (en) | 2014-08-12 |
CN102759818A (en) | 2012-10-31 |
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