Patent Application
20140204318
The present disclosure relates to the field of liquid crystal display (LCD), and more particularly to an LCD device, and a method for arranging polarizers of the LCD device.
In a liquid crystal display (LCD) device, an LCD panel may not normally display an image without polarization of a polarizer. The polarizer absorbs light that is perpendicular to a polarization axes, only permits the light in a direction of the polarization axes to pass, and converts natural light into linearly polarized light. Because the polarizer is made of a material that is in a film or plate form, the polarizer is also called a polarizing film or a polarizing plate.
Vertical alignment (VA) display mode refers to the relative VA display mode of liquid crystal (LC) molecules and substrates. Since the VA display mode has various characteristics such as having a wide viewing angle, high contrast, and no need of a friction alignment, the VA display mode is a common display mode for a thin film transistor LCD (TFT-LCD) for a large-size television TV.
Generally speaking, the LCD device in the VA display mode is in the normal black mode when the voltage is not applied, namely the first polarizer and the second polarizer are vertically laminated. Thus, in a dark state, a display brightness of the LCD device is very low, which makes high contrast. Moreover, the dark state occurs when pixels are damaged, which appears as a dark spot on the LCD panel, and slightly affects an image display, otherwise appears as a bright spot on the LCD panel, and greatly affects the image display.
However, in manufacturing the large-size LCD devices, the vertical lamination of the first polarizer and the second polarizer may be limited by material. At present, the polarizers manufactured by a polarizer manufacturing equipment are in a coil form, and are cut into an appropriate size in accordance with a size of LCD panels as required. A width of the polarizers in the coil form, at present, is limited, for example, if a length of the LCD panel is L and a width of the LCD panel is W, and a maximum width of the polarizers in the coil form is W, the first polarizer with the length of L and the width of W is obtained by cutting off the polarizers in the coil form. However, because the absorption axes of the second polarizer and the absorption axes of the first polarizer are arranged perpendicular to each other, an appropriate size of second polarizer may not be obtained. Therefore, when the length L of the LCD panel exceeds the width of the polarizers in the coil form, one of the two polarizers, which are vertically laminated, may not cover the total LCD panel because the width of the polarizers may not meet the requirement that the polarizers in the coil form may not be cut into two polarizers which have the same size and have the absorption axes which are perpendicular to each other. Optionally, a mode of splicing polarizers can be used to achieve the vertical lamination of the first polarizer and the second polarizer. However, a bright line may be produced at a spliced position, which is an unacceptable situation in a process of manufacturing LCD panels. Thus, the large-size LCD panels exceeding the width of the polarizers may not normally achieve a normal black mode in accordance with existing structures. Therefore, the problem needs to be solved urgently
In view of the above-described problems, an aim of the present disclosure is to provide a large-size LCD panel of a liquid crystal display (LCD) device can normally achieve a normal black mode.
The aim of the present discourse is achieved by the following technical scheme.
An LCD device comprises an LCD panel, a first polarizer arranged on a first side of the LCD panel, a second polarizer arranged on a second side of the LCD panel, and a λ/2 wave plate arranged between the first polarizer and the second polarizer.
An absorption axes of the first polarizer is in parallel with an absorption axes of the second polarizer.
In one example, a compensation value of an entire waveband of the λ/2 wave, plate is ½ of a corresponding wavelength of light, which increases a contrast of the LCD panel of the LCD device.
In one example, the λ/2 wave plate is arranged between the first polarizer and the LCD panel.
In one example, the λ/2 wave plate is arranged between the second polarizer and the LCD panel
In one example, an included angle between a slow axes of the λ/2 wave plate and the absorption axes of the first polarizer is 45°, and the included angle between the slow axes of the λ/2 wave plate and the absorption axes of the second polarizer is 45°, which increases the contrast of the LCD panel.
In one example, the included angle between the slow axes of the λ/2 wave plate and the absorption axes of the first polarizer is 135° and the included angle between the slow axes of the λ/2 wave plate and the absorption axes of the second polarizer is 135°.
A method for arranging polarizers of the LCD device comprises:
A: arranging a λ/2 wave plate on a first side of the LCD panel;
B: arranging a first polarizer and a second polarizer on two sides of the LCD panel to make an absorption axes of the first polarizer is in parallel with an absorption axes of the second polarizer.
In one example, a compensation value of an entire waveband of the λ/2 wave plate is ½ of a corresponding wavelength of light.
In the present disclosure, because the absorption axes of the first polarizer and the second polarizer are arranged in parallel, a width of the polarizers is sufficiently applied to the large-size LCD panel, and light passing through the first polarizer and the λ/2 wave plate is absorbed by the second polarizer, the λ/2 wave plate is arranged between the first polarizer and the second polarizer, the LCD device is able to display the normal black mode.
Legends: 100. LCD panel, 101. first polarizer, 102. second polarizer, 103. first compensation film, 104. second compensation film, 105. λ/2 wave plate.
The present disclosure provides a large-size liquid crystal display (LCD) device that is made of an existing polarizer material and is able to normally display a normal black mode. In the present disclosure, because an absorption axes of a first polarizer and a second polarizer of the LCD device are arranged in parallel, a width of the polarizers is sufficiently applied to a large-size LCD panel, and light passing through the first polarizer and a λ/2 wave plate is absorbed by the second polarizer, the λ/2 wave plate is arranged between the first polarizer and the second polarizer, the LCD device is able to display the normal black mode. Optionally, the present disclosure is also applicable to normal-sized LCD devices. For the normal-sized LCD devices, only the polarizers arranged in parallel are manufactured for a standard size without additionally manufacturing one of the polarizers having absorption axes that are in parallel with each other.
The present disclosure is further described in detail in accordance with the figures and the examples.
As shown in
In the example, the λ/2 wave plate 105 may be arranged between the second polarizer 102 and the LCD panel 100 as well because the λ/2 wave plate 105 is used to enable the polarized light passing through the first polarizer 102 to produce λ/2 phase delay.
The present disclosure will further be described in details by simulating an existing polarizer structure of the LCD device and a polarizer structure of the example.
A simulation is performed in the example by using the LCD Master simulation software.
Simulation setting is as follows:
LC setting:
1: Set a pretilt angle: 89°;
2: Define 4domain LC azimuth: 45°, 135°, 225°, and 315°.
Light source setting:
1: Simulate to use Blue-YAG LED spectrum
2: Define central brightness: 100 nit
3: Light source distribution is Lambert's distribution
For the condition of setting same experimental parameters, the existing polarizer structure and the polarizer structure of the example are simulated, and the results are as follows:
A dark state brightness, a bright state brightness, and a contrast of the existing polarizer (POL) structure in normal black mode are as follows:
If the POL structure of the example, namely the structure shown in
It can be seen that when the slow axes of the wave plate is parallel or perpendicular to the absorption axes of the POL, the LCD device is in a bright state and a normal white mode at 0V, and the LCD device is in a normal black mode at 7V, When the included angle between the slow axes of the λ/2 wave plate and the absorption axes of the POL is 45° or 135°, the LCD device is in the normal black mode. However, the brightness is slightly high at 0V which makes con frost of the LCD panel be low.
This is because of the slight variation of the wave plate used in the simulation corresponding to compensation values (Ro) of different wavelengths of the light. The parameters of the existing λ/2 wave plate are as follows
Thus, we simulate a requirement of the required λ/2 wave plate.
The relationship between compensation values Ro, Rth and refractive index N, and thickness d is as follows:
Ro=(Nx−Ny)*d
Rth=[(Nx+Ny)/2−Nz]*d
Take 650 nm as an example, we design different λ/2 Re corresponding to the 650 nm.
Therefore, the λ/2 wave plate has the characteristics shown in
As shown in the Table below, When all the compensation values of the λ/2 wave plate corresponding to the wavelength of the light of each waveband are ½ of the wavelength of the light of the waveband, the simulated results of the LCD device of the example are as follows:
It can be seen that using, the parameters of the novel λ/2 wave plate to perform simulation may really and effectively reduce the brightness in the dark state, and may effectively increase the contrast without sacrificing the brightness in the bright state. The novel λ/2 wave plate may be obtained by the formula . In accordance with the formula, the novel λ/2 wave plate may achieve the parameters by simultaneously changing the refractive index Nx, Ny, and thickness d of the novel λ/2 wave plate. In a process of manufacturing the wave plate, the refractive index Nx, Ny, and the thickness d of the wave plate are adjusted to enable the parameters of the wave plate to be coincident with or approximate to the parameters shown in
The present disclosure is described in detail in accordance with the above contents with the specific preferred examples. However, this present disclosure is not limited to the specific examples. For the ordinary technical personnel of the technical field of the present disclosure, on the premise of keeping the conception of the present disclosure, the technical personnel can also make simple deductions or replacements, and all of which should be considered to belong to the protection scope of the present disclosure.
| Number | Date | Country | Kind |
|---|---|---|---|
| 201310021316.4 | Jan 2013 | CN | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/CN2013/071903 | 2/26/2013 | WO | 00 | 3/15/2013 |
