WO2016101339A1 - 液晶显示器 - Google Patents
液晶显示器 Download PDFInfo
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- WO2016101339A1 WO2016101339A1 PCT/CN2015/070080 CN2015070080W WO2016101339A1 WO 2016101339 A1 WO2016101339 A1 WO 2016101339A1 CN 2015070080 W CN2015070080 W CN 2015070080W WO 2016101339 A1 WO2016101339 A1 WO 2016101339A1
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- optical axis
- liquid crystal
- single optical
- axis phase
- compensation film
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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
- G02F1/133528—Polarisers
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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
- G02F1/13363—Birefringent elements, e.g. for optical compensation
-
- 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
- G02F1/13363—Birefringent elements, e.g. for optical compensation
- G02F1/133634—Birefringent elements, e.g. for optical compensation the refractive index Nz perpendicular to the element surface being different from in-plane refractive indices Nx and Ny, e.g. biaxial or with normal optical axis
-
- 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
- G02F1/13363—Birefringent elements, e.g. for optical compensation
- G02F1/133635—Multifunctional compensators
-
- 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
- G02F2413/00—Indexing scheme related to G02F1/13363, i.e. to birefringent elements, e.g. for optical compensation, characterised by the number, position, orientation or value of the compensation plates
- G02F2413/02—Number of plates being 2
-
- 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
- G02F2413/00—Indexing scheme related to G02F1/13363, i.e. to birefringent elements, e.g. for optical compensation, characterised by the number, position, orientation or value of the compensation plates
- G02F2413/04—Number of plates greater than or equal to 4
-
- 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
- G02F2413/00—Indexing scheme related to G02F1/13363, i.e. to birefringent elements, e.g. for optical compensation, characterised by the number, position, orientation or value of the compensation plates
- G02F2413/06—Two plates on one side of the LC cell
Definitions
- the present invention relates to a liquid crystal display, and more particularly to a liquid crystal display using a single optical axis phase compensation film.
- liquid crystal displays have gradually become mainstream displays due to the thinness and shortness of liquid crystal displays.
- various electronic devices on the market such as mobile phones, personal digital assistants, digital cameras, computer screens, laptop screens, etc., almost all adopt liquid crystal display screens as their display screens.
- the liquid crystal display includes a liquid crystal layer, and changes in the direction of rotation of the liquid crystal molecules in the liquid crystal layer by the electric field applied to the liquid crystal layer, thereby adjusting the transmittance of light passing through the liquid crystal layer.
- the liquid crystal material has a birefringence characteristic, that is, refractive indices different from each other along the long axis direction of the molecule and the short axis direction of the molecule. Therefore, the linearly polarized incident light passes through different paths of the liquid crystal layer to have different phases in its polarization direction, and thus the color characteristics and transmittance at the oblique viewing angle and at the frontal view may be different.
- the prior art proposes to add a compensation film to the liquid crystal panel.
- the compensation film is corrected by compensating for the phase difference of light in different directions, and the birefringence property of the liquid crystal molecules is compensated for symmetry.
- FIG. 1 is a dark state light leakage after compensation by a conventional single optical axis phase compensation film.
- the cloth simulation map, FIG. 2 is a simulation diagram of the full-view contrast distribution after being compensated by the single optical axis phase compensation film.
- 1 and 2 set the liquid crystal optical path difference ⁇ n ⁇ d to be 296.5 nm, the compensation value Ro of the A-type compensation film was 58 nm, the compensation value Rth was 220 nm, and the compensation value Rth of the C-type compensation film was 16 nm.
- the horizontal viewing area is more easily seen by the audience, so the contrast and sharpness of the horizontal viewing angle have a greater impact on the viewing effect. In contrast, the area of vertical viewing is less likely to be seen and has less impact on the audience.
- the liquid crystal display can define a dark state light leakage region in a vertical viewing angle region.
- the present invention discloses a liquid crystal display comprising a backlight; a first triacetate cellulose (TAC) film; a first polyvinyl alcohol (PVA) film; a first single optical axis phase compensation film that adjusts a thickness of the first single optical axis phase compensation film and adjusts a first refractive index corresponding to the light rays in the first direction, the second direction, and the third direction, respectively a second refractive index and a third refractive index to provide a first compensation value and a second compensation value; a second single optical axis phase compensation film that adjusts a thickness of the second single optical axis phase compensation film and Adjusting a fourth refractive index, a fifth refractive index, and a sixth refractive index corresponding to the light in the first direction, the second direction, and the third direction, respectively, to provide a third compensation value; a layer; a second PVA film; and a second TAC film.
- TAC triacetate cellulose
- PVA polyviny
- the liquid crystal layer has an optical path difference determined by (ne-no) ⁇ d, which is between 287.2 and 305.7 nm, wherein ne and no respectively represent extraordinary light of the liquid crystal layer.
- the refractive index and the ordinary refractive index, and d represents the thickness of the liquid crystal layer.
- the second compensation value is determined according to the first refractive index, the second refractive index, the third refractive index, and the thickness of the first single optical axis phase compensation film. .
- the second compensation value of the first single optical axis phase compensation film is between 208 and 281 nm.
- the liquid crystal molecules of the liquid crystal layer have a pretilt angle of 89 degrees.
- the third compensation value is determined according to the fourth refractive index, the fifth refractive index, the sixth refractive index, and the thickness of the second single optical axis phase compensation film. .
- the first single optical axis phase compensation film is an A-type compensation film, and an optical axis of the first single optical axis phase compensation film is parallel to a surface, and the second single optical axis phase
- the compensation film is a C-type compensation film, and the optical axis of the second single-axis phase compensation film is perpendicular to the surface.
- the liquid crystal display further includes a first pressure sensitive adhesive disposed between the first single optical axis phase compensation film and the liquid crystal layer.
- the liquid crystal display further includes a second pressure sensitive adhesive disposed between the second single optical axis phase compensation film and the liquid crystal layer.
- the first compensation value Ro A of the first single optical axis phase compensation film is controlled to be between 55 and 75 nm
- the second compensation value Rth b is controlled between 208 and 281 nm
- the present invention can improve the conventional single optical axis by appropriately setting the first compensation value Ro A of the first single optical axis phase compensation film, the second compensation value Rth A, and the third compensation value Rth C of the second single optical axis phase compensation film.
- the phase compensation film compensates for the problem of severe dark state light leakage in the horizontal viewing angle region, while increasing the contrast and sharpness of the horizontal viewing angle region.
- FIG. 1 is a simulation diagram of dark state light leakage distribution after compensation by a conventional single optical axis phase compensation film.
- FIG. 2 is a simulation diagram of full-view contrast distribution after being compensated by the single optical axis phase compensation film.
- FIG 3 is a schematic view of a preferred embodiment of a liquid crystal display of the present invention.
- FIG. 4 is a diagram showing the first compensation value Ro A and the second compensation value Rth A of the first single optical axis phase compensation film and the second single optical axis phase compensation film under the condition that the optical path difference of the liquid crystal layer is 287.2 nm.
- FIG. 5 is a diagram showing the first compensation value Ro A and the second compensation value Rth A of the first single optical axis phase compensation film and the second single optical axis phase compensation film under the condition that the optical path difference of the liquid crystal layer is 296.5 nm.
- FIG. 6 is a diagram showing the first compensation value Ro A and the second compensation value Rth A of the first single optical axis phase compensation film and the second single optical axis phase compensation film under the condition that the optical path difference of the liquid crystal layer is 305.7 nm.
- the liquid crystal optical path difference is 287.2 nm
- the first compensation value Ro A of the first single optical axis phase compensation film is 71 nm
- the second compensation value Rth A is 269 nm
- the second single optical axis phase compensation film is The three compensation value Rth C is a dark state light leakage distribution map under the condition of 16 nm.
- the three-compensation value Rth C is a full-view contrast distribution map at a condition of 16 nm.
- the liquid crystal optical path difference is 296.5 nm
- the first compensation value Ro A of the first single optical axis phase compensation film is 65 nm
- the second compensation value Rth A is 244 nm
- the second single optical axis phase compensation film is The three compensation value Rth C is a dark state light leakage distribution map at 52 nm.
- the liquid crystal optical path difference is 296.5 nm
- the first compensation value Ro A of the first single optical axis phase compensation film is 65 nm
- the second compensation value Rth A is 244 nm
- the second single optical axis phase compensation film is The three-compensation value Rth C is a full-view contrast distribution map at 52 nm.
- the three compensation value Rth C is a dark state light leakage distribution map under the condition of 87 nm.
- the three-compensation value Rth C is a full-view contrast distribution map at 87 nm.
- FIG. 3 is a schematic diagram of a preferred embodiment of the liquid crystal display 10 of the present invention.
- the liquid crystal display 10 includes a liquid crystal layer 16, a first polarizer 12, a second polarizer 14, and a backlight 18.
- the backlight 18 is used to generate light, and the liquid crystal layer 16 is bonded between the first polarizer 12 and the second polarizer 14 by a pressure sensitive adhesive (PSA) 2.
- PSA pressure sensitive adhesive
- the first polarizer 12 and the second polarizer 14 are used to deflect incident light, and the first optical axis of the first polarizer 12 is perpendicular to the second optical axis of the second polarizer 14.
- the first polarizer 12 includes a first polyvinyl alcohol (PVA) film 121 sandwiched between a first triacetate cellulose (TAC) film 122 and a first single optical axis phase compensation film 123. between.
- the second polarizer 14 includes a second polyvinyl alcohol film 141 sandwiched between the second single optical axis phase compensation film 142 and the second TAC film 143.
- the first single optical axis phase compensation film 123 is an A-type compensation film (A-plate) whose optical axis is parallel to the surface of the compensation film 123.
- the second single optical axis phase compensation film 142 is a C-type compensation film (C-plate) whose optical axis is perpendicular to the surface of the compensation film 142.
- the first single optical axis phase compensation film 123 is used to provide a first compensation value Ro A and a second compensation value Rth A
- the second single optical axis phase compensation film 142 is used to provide a third compensation value Rth C .
- the angle between the slow axis of the first single optical axis phase compensation film 123 and the absorption axis of the first PVA film 121 is 90 degrees
- the absorption axis of the second PVA film 141 is 0 degrees. How to determine the first compensation value, the second compensation value, and the third compensation value will be described below.
- the optical path difference of the liquid crystal layer 16 and the compensation values of the compensation films 123, 142 are all values corresponding to a wavelength equal to 550 nm.
- FIG. 4-6 illustrate the first compensation of different first single optical axis phase compensation films 123 under the condition that the optical path difference of the liquid crystal layer 16 is 287.2 nm, 296.5 nm, and 305.7 nm, respectively.
- the incident light emitted from the backlight 18 is distributed in a Lambertian distribution, and the central luminance is defined as 100 nit.
- the liquid crystal molecules of the liquid crystal layer 16 have a pretilt angle of 89 degrees.
- d represents the thickness of the liquid crystal layer 16.
- Ro A represents the first compensation value of the first single optical axis phase compensation film 123 in the XY plane
- Rth A represents the second compensation value of the first single optical axis phase compensation film 123 in the Z-axis direction
- Rth C represents the third compensation value of the second single optical axis phase compensation film 142 in the Z-axis direction
- Ro A , Rth A , and Rth C are determined by the following equations:
- Rth A [(Nx A +Ny A )/2-Nz A ] ⁇ D A Equation (2)
- Rth C [(Nx C +Ny C )/2-Nz C ] ⁇ D C Equation (3)
- Nx A , Ny A , and Nz A respectively represent the refractive indices corresponding to the X, Y, and Z axes of the Cartesian coordinate system when the light from the backlight 18 passes through the first single optical axis phase compensation film 123.
- Nx C , Ny C , and Nz C respectively represent the refractive indices corresponding to the X, Y, and Z axes of the Cartesian coordinate system when the light rays from the backlight 18 pass through the second single optical axis phase compensation film 142
- D A and D C indicate the thicknesses of the first single optical axis phase compensation film 123 and the second single optical axis phase compensation film 142, respectively.
- the pre-tilt angle is 89 degrees, 287.2nm ⁇ ⁇ n ⁇ d ⁇ 305.7nm, dark state light leakage is less than 0.2
- the corresponding compensation value range of the first single optical axis phase compensation film 123 and the second single optical axis phase compensation film 142 at nit that is, in the case where the optical path difference of the liquid crystal layer 16 is between 287.2 nm and 305.7 nm and the pretilt angle of the liquid crystal molecules of the liquid crystal layer 16 is 89 degrees, the liquid crystal display 10 can still be based on the first single optical axis phase compensation film.
- the first compensation value Ro A and the second compensation value Rth A of 123 and the third compensation value Rth C of the second single optical axis phase compensation film 142 suppress light leakage.
- the first compensation value Ro A , the second compensation value Rth A of the first single optical axis phase compensation film 123 and the third compensation value Rth C of the second single optical axis phase compensation film 142 are all incidents with a wavelength of 550 nm.
- the compensation value of the light when the compensation value is within the above range, can obtain an optimum compensation effect in the liquid crystal display device, and achieve the minimum dark state light leakage.
- FIG. 7 and FIG. 8 respectively show that the first compensation value Ro A of the first single optical axis phase compensation film 123 is 71 nm and the second compensation value Rth A when the liquid crystal optical path difference is 287.2 nm.
- the third compensation value Rth C of 269 nm and the second single optical axis phase compensation film 142 is a dark state light leakage distribution map and a full viewing angle contrast distribution map at a condition of 16 nm. 9 and FIG.
- the liquid crystal optical path difference is 296.5 nm
- the first compensation value Ro A of the first single optical axis phase compensation film 123 is 65 nm
- the second compensation value Rth A is 244 nm
- the second The third compensation value Rth C of the single optical axis phase compensation film 142 is a dark state light leakage distribution map and a full viewing angle contrast distribution map at 52 nm. 11 and FIG.
- the liquid crystal optical path difference is 305.7 nm
- the first compensation value Ro A of the first single optical axis phase compensation film 123 is 58 nm
- the second compensation value Rth A is 220 nm
- the second The third compensation value Rth C of the single optical axis phase compensation film 142 is a dark state light leakage distribution map and a full viewing angle contrast distribution map at 87 nm.
- the dark state light leakage compensated by the liquid crystal display according to the embodiment of the present invention is lower than the dark state light leakage after compensation by the single optical axis phase compensation film. Moreover, the compensated dark state light leakage is concentrated near the vertical viewing angle, and the light leakage range is concentrated in a small viewing angle range. Comparing FIG. 8 , FIG. 10 , FIG. 12 and FIG. 2 , it can be directly observed that the full-view contrast distribution compensated by the liquid crystal display according to the embodiment of the present invention is also superior to the full-view contrast ratio compensated by the existing single optical axis phase compensation film. The distribution, especially in the horizontal viewing area, is effectively improved.
- a person skilled in the art may obtain the first compensation value Ro A of the first single optical axis phase compensation film 123, the second compensation value Rth A, and the third compensation value Rth C of the second single optical axis phase compensation film 142, and then The refractive index or thickness of the first single optical axis phase compensation film 123 and the second single optical axis phase compensation film 142 are adjusted by Equations (1) to (3).
- the present invention sets the first compensation value Ro A of the first single optical axis phase compensation film 123, the second compensation value Rth A and the third compensation value of the second single optical axis phase compensation film 142.
- Rth C can improve the problem of severe dark state light leakage in the horizontal viewing angle region caused by the compensation of the traditional single optical axis phase compensation film, and increase the contrast and sharpness of the horizontal viewing angle region.
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Abstract
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Claims (17)
- 一种液晶显示器,其包含一背光源用来发出光线,包括:一第一三醋酸纤维素酯片基(triacetate cellulose,TAC)膜;一第一聚乙烯醇(Polyvinyl Alcohol,PVA)膜;一第一单光轴相位补偿膜,其通过调整所述第一单光轴相位补偿膜的厚度以及调整所述光线在第一方向、第二方向以及第三方向分别所对应的第一折射率、第二折射率以及第三折射率以提供一第一补偿值以及一第二相位差值;一液晶层;一第二单光轴相位补偿膜,其通过调整所述第二单光轴相位补偿膜的厚度以及调整所述光线在所述第一方向、所述第二方向以及所述第三方向分别所对应的第四折射率、第五折射率以及第六折射率以提供一第三补偿值;一第二PVA膜;以及一第二TAC膜,其中所述液晶显示器依据所述第一补偿值、所述第二补偿值以及所述第三补偿值控制其暗态大视角漏光,其中所述第一补偿值是依据以下方程序所决定:RoA=(NxA-NyA)×DA,RoA表示所述第一补偿值,NxA、NyA分别表示所述第一单光轴相位补偿膜在笛卡尔坐标系的X、Y轴上所对应的折射率,DA表示所述第一单光轴相位补偿膜的厚度,其中所述液晶层由(ne-no)×d决定的光程差,是介于287.2~305.7nm之间,其中ne和no分别表示所述液晶层的非寻常光折射率和寻常光折射率,d表示所述液晶层厚度,所述第一单光轴相位补偿膜的第一补偿值是介于55~75nm 之间,所述第一单光轴相位补偿膜的第二补偿值是介于208~281nm之间,所述第二单光轴相位补偿膜的第三补偿值是介于Y1nm~Y2nm之间,其中Y1=0.000193x3–0.1395x2+32.434x-2387.4以及Y2=-0.007242x2+2.378x-67.84,x表示所述第二补偿值。
- 如权利要求1所述的液晶显示器,其中所述第二补偿值是依据以下方程序所决定RthA=[(NxA+NyA)/2-NzA]×DA,其中RthA表示所述第二补偿值,NxA、NyA、NzA分别表示所述第一单光轴相位补偿膜在笛卡尔坐标系的X、Y、Z轴上所对应的折射率,DA表示所述第一单光轴相位补偿膜的厚度。
- 如权利要求1所述的液晶显示器,其中所述液晶层的液晶分子的预倾角(pretilt angle)是89度。
- 如权利要求1所述的液晶显示器,其中所述第三补偿值是依据所述第四折射率、所述第五折射率、所述第六折射率和所述第二单光轴相位补偿膜的厚度决定。
- 如权利要求1所述的液晶显示器,其中所述第一单光轴相位补偿膜是一A型补偿膜,所述第一单光轴相位补偿膜的光轴平行于表面,所述第二单光轴相位补偿膜是一C型补偿膜,所述第二单光轴相位补偿膜的光轴垂直于表面。
- 根据权利要求1所述的液晶显示器,其中所述液晶显示器进一步包括第一压敏胶,所述第一压敏胶设置于所述第一单光轴相位补偿膜与所述液晶层之间。
- 根据权利要求6所述的液晶显示器,其中所述液晶显示器进一步包括第二压敏胶,所述第二压敏胶设置于所述第二单光轴相位补偿膜与所述液晶层 之间。
- 一种液晶显示器,其包含一背光源用来发出光线,包括:一第一三醋酸纤维素酯片基(triacetate cellulose,TAC)膜;一第一聚乙烯醇(Polyvinyl Alcohol,PVA)膜;一第一单光轴相位补偿膜,其通过调整所述第一单光轴相位补偿膜的厚度以及调整所述光线在第一方向、第二方向以及第三方向分别所对应的第一折射率、第二折射率以及第三折射率以提供一第一补偿值以及一第二相位差值;一液晶层;一第二单光轴相位补偿膜,其通过调整所述第二单光轴相位补偿膜的厚度以及调整所述光线在所述第一方向、所述第二方向以及所述第三方向分别所对应的第四折射率、第五折射率以及第六折射率以提供一第三补偿值;一第二PVA膜;以及一第二TAC膜,其中所述液晶显示器依据所述第一补偿值、所述第二补偿值以及所述第三补偿值控制其暗态大视角漏光,其中所述第一补偿值是依据以下方程序所决定:RoA=(NxA-NyA)×DA,RoA表示所述第一补偿值,NxA、NyA分别表示所述第一单光轴相位补偿膜在笛卡尔坐标系的X、Y轴上所对应的折射率,DA表示所述第一单光轴相位补偿膜的厚度,其中所述第一单光轴相位补偿膜的第一补偿值是介于55~75nm之间。
- 如权利要求8所述的液晶显示器,其中所述液晶层由(ne-no)×d决定的光程差,是介于287.2~305.7nm之间,其中ne和no分别表示所述液晶层的 非寻常光折射率和寻常光折射率,d表示所述液晶层厚度。
- 如权利要求8所述的液晶显示器,其中所述第二补偿值是依据以下方程序所决定RthA=[(NxA+NyA)/2-NzA]×DA,其中RthA表示所述第二补偿值,NxA、NyA、NzA分别表示所述第一单光轴相位补偿膜在笛卡尔坐标系的X、Y、Z轴上所对应的折射率,DA表示所述第一单光轴相位补偿膜的厚度。
- 如权利要求10所述的液晶显示器,其中所述第一单光轴相位补偿膜的第二补偿值是介于208~281nm之间。
- 如权利要求8所述的液晶显示器,其中所述液晶层的液晶分子的预倾角(pretilt angle)是89度。
- 如权利要求1所述的液晶显示器,其中所述第三补偿值是依据所述第四折射率、所述第五折射率、所述第六折射率和所述第二单光轴相位补偿膜的厚度决定。
- 如权利要求13所述的液晶显示器,其中所述第二单光轴相位补偿膜的第三补偿值是介于Y1nm~Y2nm之间,其中Y1=0.000193x3–0.1395x2+32.434x-2387.4以及Y2=-0.007242x2+2.378x-67.84,x表示所述第二补偿值。
- 如权利要求8所述的液晶显示器,其中所述第一单光轴相位补偿膜是一A型补偿膜,所述第一单光轴相位补偿膜的光轴平行于表面,所述第二单光轴相位补偿膜是一C型补偿膜,所述第二单光轴相位补偿膜的光轴垂直于表面。
- 根据权利要求8所述的液晶显示器,其中所述液晶显示器进一步包括第一压敏胶,所述第一压敏胶设置于所述第一单光轴相位补偿膜与所述液晶层之间。
- 根据权利要求16所述的液晶显示器,其中所述液晶显示器进一步包括第二压敏胶,所述第二压敏胶设置于所述第二单光轴相位补偿膜与所述液晶层之间。
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US14/417,538 US9638958B2 (en) | 2014-12-25 | 2015-01-05 | Liquid crystal display |
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CN106019720B (zh) * | 2016-05-31 | 2020-02-14 | 京东方科技集团股份有限公司 | 一种显示用基板、显示装置和曲面显示装置 |
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GB2550305B (en) | 2021-02-24 |
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