JPH03245122A - Liquid crystal display device - Google Patents
Liquid crystal display deviceInfo
- Publication number
- JPH03245122A JPH03245122A JP2041019A JP4101990A JPH03245122A JP H03245122 A JPH03245122 A JP H03245122A JP 2041019 A JP2041019 A JP 2041019A JP 4101990 A JP4101990 A JP 4101990A JP H03245122 A JPH03245122 A JP H03245122A
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- picture element
- color
- transmittance
- gap thickness
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000004973 liquid crystal related substance Substances 0.000 title claims abstract description 29
- 210000002858 crystal cell Anatomy 0.000 claims abstract description 10
- 238000002834 transmittance Methods 0.000 abstract description 27
- 230000001681 protective effect Effects 0.000 abstract description 8
- 238000004040 coloring Methods 0.000 abstract description 7
- 239000003086 colorant Substances 0.000 abstract description 5
- 239000000758 substrate Substances 0.000 abstract description 3
- 239000011521 glass Substances 0.000 abstract description 2
- 238000000034 method Methods 0.000 description 6
- 230000000694 effects Effects 0.000 description 3
- 125000006850 spacer group Chemical group 0.000 description 3
- 239000004988 Nematic liquid crystal Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
Landscapes
- Liquid Crystal (AREA)
- Devices For Indicating Variable Information By Combining Individual Elements (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、液晶内の透過光の制御において画素ごとで固
有の波長の光を制御する際に、それぞれの画素において
最適な透過率を設定できる液晶表示装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention sets the optimum transmittance for each pixel when controlling light with a unique wavelength for each pixel in controlling transmitted light in a liquid crystal. The present invention relates to a liquid crystal display device that can be used.
従来の装置は、特開昭60−159830号公報に記載
のように、赤、緑、青の順にギャップ厚が小さくなるよ
うに変化させて、どの色に対しても電圧無印加時の透過
率を最小限におさえている。又、特開昭63−2910
31号公報に記載されている例では。As described in JP-A-60-159830, in the conventional device, the gap thickness is changed in the order of red, green, and blue, and the transmittance when no voltage is applied is determined for each color. is kept to a minimum. Also, JP-A-63-2910
In the example described in Publication No. 31.
一つの表示画素内で保護膜に段差を形成し、三種のギャ
ップ厚を設けることにより、色の違いによる透過率の差
を小さくしている。By forming steps in the protective film within one display pixel and providing three different gap thicknesses, differences in transmittance due to different colors are reduced.
前述の例は、色の違いによる液晶セルの光の透過率の差
を小さくシ、黒色表示時の色つきをなくすのに有効であ
る。本発明者らは、色の違いによる光の透過率の差を小
さくするための方法として。The above-mentioned example is effective in reducing the difference in light transmittance of the liquid crystal cell due to the difference in color, and in eliminating coloration when displaying black. The present inventors developed this method as a method for reducing the difference in light transmittance due to differences in color.
前述の方法よりさらに簡単な方法を提供する。Provides a simpler method than the previously described method.
本発明の目的は、液晶セルのカラー表示において黒色表
示時の色つきを最小にすることである。An object of the present invention is to minimize coloring during black display in color display of a liquid crystal cell.
上記課題は、液晶セルの一つの表示画素において二種類
以上のギャップ厚の異なる部分を形成することにより達
成できる。更に、本発明の態様を示せば以下の通りであ
る。The above object can be achieved by forming two or more types of portions with different gap thicknesses in one display pixel of a liquid crystal cell. Further aspects of the present invention are as follows.
(1)液晶セル内の、液晶の占める部分のギャップ厚を
一つの表示画素につき二種類以上変え、それぞれの表示
画素内におけるギャップ厚の異なる部分の面積の比を、
表示画素の色ごとに変化させた液晶表示素子。(1) The gap thickness of the portion occupied by the liquid crystal in the liquid crystal cell is varied in two or more types for each display pixel, and the ratio of the areas of the portions with different gap thicknesses in each display pixel is
A liquid crystal display element that changes the color of each display pixel.
(2)液晶セルの表示画素の色が、赤、緑、青の三原色
の場合、ギャップ厚を二種類設定し、ギャップ厚の大き
い部分の面積の比を、赤〉緑〉青の順とした液晶表示素
子。(2) When the colors of the display pixels of the liquid crystal cell are the three primary colors of red, green, and blue, two types of gap thickness were set, and the area ratio of the portion with the largest gap thickness was set in the order of red>green>blue. Liquid crystal display element.
更に、本発明で、ギャップ厚とは、通過光が通る液晶の
部分の長さのことを示す、ただし、液晶層の厚さを固定
するスペーサがある場合、その中を通る距離も含む。Furthermore, in the present invention, the gap thickness refers to the length of the portion of the liquid crystal through which the passing light passes; however, if there is a spacer that fixes the thickness of the liquid crystal layer, it also includes the distance passing through the spacer.
又、あるギャップ厚を持った部分の面積とは、ある一つ
の表示画素内の、指定のギャップ厚の液晶あるいはスペ
ーサを通過し、実際に表示される光が、保護膜を通過す
る範囲を示す。In addition, the area of a portion with a certain gap thickness refers to the area within a certain display pixel where light that passes through the liquid crystal or spacer with a specified gap thickness and is actually displayed passes through the protective film. .
液晶の透過率Tは次式で示される。 Transmittance T of liquid crystal is expressed by the following formula.
λ
ここで、Δnは液晶の屈折率異方性、dは液晶セルのギ
ャップ厚、λは透過光の波長である。λ Here, Δn is the refractive index anisotropy of the liquid crystal, d is the gap thickness of the liquid crystal cell, and λ is the wavelength of transmitted light.
Δnはほとんど波長依存がないため、透過率Tはλとd
の値によって決まる。ここで一つの表示画素におけるギ
ャップ厚を複数種(n種類)設け、それぞれd+(i=
1p n)とし、それぞれの面積の一画素全体の面積に
対する比をαt(i=1+n)とすると、一画素の平均
の透過率は次式で表せる。Since Δn has almost no wavelength dependence, the transmittance T is determined by λ and d
determined by the value of Here, a plurality of types (n types) of gap thickness in one display pixel are provided, and each d+(i=
1p n), and the ratio of each area to the entire area of one pixel is αt (i=1+n), then the average transmittance of one pixel can be expressed by the following equation.
λ
上式でλが異なると、Tの値も変化するが、適当なα1
の組を選ぶことにより、最適な透過率を選ぶ事が可能と
なる。λ If λ differs in the above equation, the value of T will also change, but an appropriate α1
By selecting the set of , it is possible to select the optimum transmittance.
以下、本発明の一実施例を第1図および第2図により説
明する。An embodiment of the present invention will be described below with reference to FIGS. 1 and 2.
第1図に、ツィステッド・ネマティック型液晶カラー表
示装置の液晶表示素子を示す。偏光板1゜ガラス基板2
.透明電極4.保護膜7.配向膜5゜カラーフィルタ(
赤)31.(緑)32.(青)33を第1図の様に配置
し、その間の空間に、ネマティック型液晶を注入するゆ
保護膜は、段差が形成されており、一つの表示画素を、
di とd2の二つのギャップ厚の部分に分けている。FIG. 1 shows a liquid crystal display element of a twisted nematic liquid crystal color display device. Polarizing plate 1゜Glass substrate 2
.. Transparent electrode 4. Protective film7. Alignment film 5° color filter (
Red) 31. (Green) 32. (Blue) 33 are arranged as shown in Figure 1, and nematic liquid crystal is injected into the space between them.The protective film has a step formed, and one display pixel is
It is divided into two gap thickness parts, di and d2.
ギャップ厚の厚い部分の面積の、一つの画素に対する割
合をαとすると、カラーフィルタ(赤)の画素では、α
B1緑はαG、青はαBと色ごとにαを変化させており
、αR〉αG〉αBという関係になっている。偏光板の
偏光方向は同一方向に配置しており、配向膜5は上と下
で、配向の方向が、90°、あるいは、それ以上の角度
を威すように設定している。If the ratio of the area of the thick gap part to one pixel is α, then for the pixel of the color filter (red), α
B1 green is αG, blue is αB, and α is changed for each color, and the relationship is αR>αG>αB. The polarizing plates are arranged in the same direction, and the upper and lower orientation films 5 are set so that the orientation direction is at an angle of 90° or more.
透明電極間に電圧を印加させた状態で、透過率は最大と
なり、電圧を無印加にすると、透過率は最小となる。し
かし、透過率は1式(1)、 (2)で示したように、
波長に依存する。第2図に透過率TとΔncl(Δn:
液晶の屈折率異方性、d:液晶セルのギャップ厚)の関
係を示す。λが異なるとTが零となるΔndも異なる事
がわかる。Δnは定数であるのである波長λの光の透過
率Tはギャップ厚dに依存することがわかる。ギャップ
厚に段差を設けず一種類にギャップ厚にした場合の波長
ごとの透過率を表1に示す。When a voltage is applied between the transparent electrodes, the transmittance is maximum, and when no voltage is applied, the transmittance is minimum. However, as shown in equations (1) and (2), the transmittance is
Depends on wavelength. Figure 2 shows the transmittance T and Δncl (Δn:
The relationship between the refractive index anisotropy of the liquid crystal (d: gap thickness of the liquid crystal cell) is shown. It can be seen that if λ differs, Δnd at which T becomes zero also differs. Since Δn is a constant, it can be seen that the transmittance T of light of wavelength λ depends on the gap thickness d. Table 1 shows the transmittance for each wavelength when one type of gap thickness is used without providing a step in the gap thickness.
表1に示す様にギャップ厚が一つのみの場合、透過率が
波長によって異なり、透過率の大きい波長によって色付
現象が起る。As shown in Table 1, when there is only one gap thickness, the transmittance varies depending on the wavelength, and a coloring phenomenon occurs depending on the wavelength with a large transmittance.
一方、第1図におけるdl、dzを、Δndt:0.4
40.Δndz=0.502 となるように設定し、
第1図に示すαR9αG、αBを表2に示す値を選ぶと
、各画素の透過率は表2に示す様に、赤は0.826%
、緑は0.803%、青は0.814%となり、最大値
と最小値の差は0.022%になる。この値は一種類の
ギャップ厚の場合に比べ、百分の−であり黒色表示時の
色付現象を非常に小さく抑えることができる。On the other hand, dl and dz in Fig. 1 are Δndt: 0.4
40. Set so that Δndz=0.502,
If the values shown in Table 2 are selected for αR9αG and αB shown in Figure 1, the transmittance of each pixel is 0.826% for red as shown in Table 2.
, green is 0.803%, blue is 0.814%, and the difference between the maximum and minimum values is 0.022%. This value is -100% lower than that in the case of one type of gap thickness, and the coloring phenomenon during black display can be suppressed to a very small level.
表 2
Δnd1.Δndz、 αR,aa、(!Bは次に述べ
る方法で決定する。第2図の一部を拡大したものを第3
図に示す。まずΔndによって決まる透過率Tの上限値
を決める。上限値を1%とすると第3図に示す破線■よ
り下の部分が許容範囲となる。Table 2 Δnd1. Δndz, αR, aa, (!B are determined by the method described below.
As shown in the figure. First, the upper limit value of the transmittance T determined by Δnd is determined. If the upper limit is 1%, the portion below the broken line ■ shown in FIG. 3 becomes the permissible range.
この場合、青色では、0.374≦Δnd≦0.444
、緑色では0.438≦Δnd≦0.519、赤色では
0.486≦Δnd≦0.576となる。この範囲で、
dl、daの二種類のギャップ厚は第3図に示すHaと
Haの重なる範囲、及びHaとHFIの重なる範囲のΔ
ndに対応する必要がある。なぜむらば、赤緑青の各画
素について透過率の平均値が1%以下であるためには、
赤・緑・青の波長に対して、dz、daのどちらかが透
過率が1%以下の必要があるからである。上限値を1%
とした特上に述べた事から、Δndx+ Δndzの範
囲は0.486≦Δndx≦0.519,0.438≦
Δndz≦0.444となる。透過率の上限値を0.8
4% とした時、第3図の破線■で示す様に。In this case, for blue, 0.374≦Δnd≦0.444
, 0.438≦Δnd≦0.519 for green, and 0.486≦Δnd≦0.576 for red. In this range,
The two gap thicknesses dl and da are determined by Δ in the overlapping range of Ha and Ha and the overlapping range of Ha and HFI shown in Figure 3.
It is necessary to correspond to nd. Why, in order for the average value of transmittance for each red, green, and blue pixel to be less than 1%,
This is because either dz or da needs to have a transmittance of 1% or less for red, green, and blue wavelengths. Upper limit value 1%
As mentioned above, the range of Δndx+ Δndz is 0.486≦Δndx≦0.519, 0.438≦
Δndz≦0.444. The upper limit of transmittance is set to 0.8
When it is set to 4%, as shown by the broken line ■ in Figure 3.
HaとHaの重なる範囲はΔnd=0.4406の一点
のみとなり、これ以上、上限値を下げることはできない
、そこで、Δndz=0.44と決めΔnd工の範囲は
、上限値が0.84%の時のHa とHRの重なる範囲
とし、計算した結果、0.489≦Δndx≦0.51
5 となった。式(3)の中のΔndz、 λは決定
しているので一画素の平均の透過率Tはαとdlの関数
と考えられ。The range where Ha and Ha overlap is only one point, Δnd = 0.4406, and the upper limit value cannot be lowered any further, so Δndz = 0.44 is decided, and the upper limit value of the range of Δnd is 0.84%. Assuming the overlapping range of Ha and HR when
It became 5. Since Δndz and λ in equation (3) are determined, the average transmittance T of one pixel can be considered as a function of α and dl.
次式のようにおける。In the following equation.
=f(α、d1)
・・・(5)青色の場合、Ts=f(αB、dl)は、
Δndtの範囲ではαB=Oの時、最小値0.814%
となるので、αB=0に決定する。黒色表示時の色付現
象をなくすためには、他のTR,TOがTaに近い程良
いので、
TFI: f (αR,dx)=0.814Ta= f
(αc、dx)=0.814となる。αRI aa、
dz (0,489≦Δndx≦0.51.5)を求め
る。この場合、筒便な方法として、Δndlの値として
、第3図に示すグラフの緑と赤のグラフの交点となる値
を選んだ。このようにして求まった値を表2に示す。=f(α, d1)
...(5) In the case of blue, Ts=f(αB, dl) is
In the range of Δndt, when αB=O, the minimum value is 0.814%
Therefore, it is determined that αB=0. In order to eliminate the coloring phenomenon during black display, the closer the other TR and TO are to Ta, the better, so TFI: f (αR, dx) = 0.814 Ta = f
(αc, dx)=0.814. αRI aa,
Find dz (0,489≦Δndx≦0.51.5). In this case, as a convenient method, a value at the intersection of the green and red graphs shown in FIG. 3 was selected as the value of Δndl. Table 2 shows the values determined in this way.
第4図に保護膜の形状の別の例を示す。第1図に示した
例は、段差が一つであるが、第4図の様に1段差を増や
しても、ギャップ厚の厚い部分と薄い部分の面積の比が
、第工図に示した場合と同じである限り、同等の効果を
得られる。一つの画素内の段差の間隔は、第4図に示す
様に必ずしも規則的である必要はない。FIG. 4 shows another example of the shape of the protective film. The example shown in Fig. 1 has one step, but even if one step is increased as shown in Fig. 4, the ratio of the area of the thick part to the thin part of the gap will be the same as shown in the drawing. As long as the situation is the same, you can get the same effect. The intervals between the steps within one pixel do not necessarily have to be regular as shown in FIG.
本発明によれば、カラー表示用液晶セルの一つの画素に
おけるギャップ厚を二種類以上設け、ギャップ厚の異な
る部分の面積の一画素全体の面積に対する比を画素の色
ごとに調節し、画素の色ごとの透過率の差を最小にし、
黒色表示時の色付現象を抑えることができる。According to the present invention, two or more types of gap thickness are provided in one pixel of a liquid crystal cell for color display, and the ratio of the area of the portion with different gap thickness to the area of the entire one pixel is adjusted for each pixel color. Minimize the difference in transmittance between colors,
Coloring phenomenon during black display can be suppressed.
第1図は本発明の一実施例である液晶カラー表示装置の
最小単位部の縦断面図、第2図は透過率TとΔndの関
係を、三種類の波長(赤、緑、青)についてグラフ化し
た説明図、第3図は第1図の一部を拡大した説明図、第
4図は本発明の他の実施例である液晶カラー表示装置の
最小単位部の縦断面図である。
l・・偏光板、2・・・ガラス基板、4・・・透明電極
、5・・・配向膜、6・・・液晶、7・・・保護膜、3
1・・・カラーフィルタ(赤)、32・・・カラーフィ
ルタ (緑)。
33・・・カラーフィルタ (青)。
図
V、3 口
賃 zI21
41ft
ρ576Figure 1 is a vertical cross-sectional view of the smallest unit of a liquid crystal color display device that is an embodiment of the present invention, and Figure 2 shows the relationship between transmittance T and Δnd for three wavelengths (red, green, and blue). FIG. 3 is a partially enlarged explanatory diagram of FIG. 1, and FIG. 4 is a vertical sectional view of the smallest unit of a liquid crystal color display device according to another embodiment of the present invention. l... Polarizing plate, 2... Glass substrate, 4... Transparent electrode, 5... Alignment film, 6... Liquid crystal, 7... Protective film, 3
1... Color filter (red), 32... Color filter (green). 33...Color filter (blue). Figure V, 3 Rent zI21 41ft ρ576
Claims (1)
一つの表示画素につき二種類以上変え、それぞれの表示
画素内におけるギャップ厚の異なる部分の面積の比を、
表示画素の色調ごとに変化させることを特徴とする液晶
表示装置。1. The gap thickness of the portion occupied by the liquid crystal in the liquid crystal cell is varied in two or more types for each display pixel, and the ratio of the areas of the portions with different gap thicknesses in each display pixel is
A liquid crystal display device characterized by changing the color tone of each display pixel.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2041019A JPH03245122A (en) | 1990-02-23 | 1990-02-23 | Liquid crystal display device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2041019A JPH03245122A (en) | 1990-02-23 | 1990-02-23 | Liquid crystal display device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH03245122A true JPH03245122A (en) | 1991-10-31 |
Family
ID=12596684
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2041019A Pending JPH03245122A (en) | 1990-02-23 | 1990-02-23 | Liquid crystal display device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH03245122A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0595155A2 (en) * | 1992-10-19 | 1994-05-04 | Canon Kabushiki Kaisha | Liquid crystal display device |
KR100252436B1 (en) * | 1997-04-23 | 2000-05-01 | 구본준 | Liquid crystal display device and method for making the same |
US6819379B2 (en) | 1997-12-26 | 2004-11-16 | Sharp Kabushiki Kaisha | Liquid crystal display device with light transmission and reflection regions |
US6900863B2 (en) | 1997-12-26 | 2005-05-31 | Sharp Kabushiki Kaisha | Liquid crystal display |
KR100483524B1 (en) * | 1997-08-25 | 2005-08-24 | 삼성전자주식회사 | Liquid crystal display device with uniform substrate spacing and manufacturing method |
JP2007206342A (en) * | 2006-02-01 | 2007-08-16 | Epson Imaging Devices Corp | Liquid crystal and electronic device |
-
1990
- 1990-02-23 JP JP2041019A patent/JPH03245122A/en active Pending
Cited By (23)
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EP0595155A3 (en) * | 1992-10-19 | 1994-10-19 | Canon Kk | Liquid crystal display device. |
EP0595155A2 (en) * | 1992-10-19 | 1994-05-04 | Canon Kabushiki Kaisha | Liquid crystal display device |
KR100252436B1 (en) * | 1997-04-23 | 2000-05-01 | 구본준 | Liquid crystal display device and method for making the same |
US6061106A (en) * | 1997-04-23 | 2000-05-09 | Lg Electronics Inc. | Liquid crystal display device having a liquid crystal layer with a varying thickness |
KR100483524B1 (en) * | 1997-08-25 | 2005-08-24 | 삼성전자주식회사 | Liquid crystal display device with uniform substrate spacing and manufacturing method |
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US7542116B2 (en) | 1997-12-26 | 2009-06-02 | Sharp Kabushiki Kaisha | Liquid crystal display |
US6819379B2 (en) | 1997-12-26 | 2004-11-16 | Sharp Kabushiki Kaisha | Liquid crystal display device with light transmission and reflection regions |
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