JPH0220829A - Liquid crystal display device - Google Patents

Liquid crystal display device

Info

Publication number
JPH0220829A
JPH0220829A JP63170538A JP17053888A JPH0220829A JP H0220829 A JPH0220829 A JP H0220829A JP 63170538 A JP63170538 A JP 63170538A JP 17053888 A JP17053888 A JP 17053888A JP H0220829 A JPH0220829 A JP H0220829A
Authority
JP
Japan
Prior art keywords
liquid crystal
anisotropy
display device
voltage
crystal display
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
Application number
JP63170538A
Other languages
Japanese (ja)
Inventor
Hideshi Yoshida
秀史 吉田
Takeshi Kamata
豪 鎌田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP63170538A priority Critical patent/JPH0220829A/en
Publication of JPH0220829A publication Critical patent/JPH0220829A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To cancel a change in the state of light, to eliminate coloring at the time of slanting view, and to make a display with good view angle characteristics by canceling the effect of the polarizing operation of liquid crystal by a compensating layer when a voltage is applied to the liquid crystal. CONSTITUTION:The compensating layer 42 has refractive index anisotropy and the axial direction of the anisotropy is 90 deg. to the direction in a plane of liquid crystal molecules of the liquid crystal 40, which is sandwiched between a couple of polarizing plates 41a and 41b. The compensating layer 42 polarizes the state of light passed through the liquid crystal 40 by 90 deg. to cancel the effect of the polarizing operation of the liquid crystal 40 when a voltage is applied to the liquid crystal 40. The product DELTAn.d of the anisotropy DELTAn of the liquid crystal 40 and cell thickness (d) of the layer 42 varies by variation in the DELTAn.d of the liquid crystal 40 which is viewed slantingly. Consequently, no coloring occurs even when viewed slantingly and a display is made with good view angle characteristics.

Description

【発明の詳細な説明】 (概要〕 電圧非印加時において、垂直配向された液晶セルを一対
の偏光板で挟持する構成の液晶表示装置に関し、 斜めから見ても色がつかず、視角特性よく表示できるこ
とを目的とし、 屈折率の異方性を有し、該異方性の軸方向が液晶の液晶
分子の平面上における方向と90°をなす補fi層を、
液晶に重ね、該補f!i層と液晶とを重ねたものを一対
の偏光板で挟持した構成とする。
[Detailed Description of the Invention] (Summary) This invention relates to a liquid crystal display device having a configuration in which a vertically aligned liquid crystal cell is sandwiched between a pair of polarizing plates when no voltage is applied, which does not appear colored even when viewed from an angle and has good viewing angle characteristics. For the purpose of display, a compensatory layer having refractive index anisotropy and the axis direction of the anisotropy making 90 degrees with the plane direction of the liquid crystal molecules of the liquid crystal,
Superimposed on the LCD, the supplementary f! It has a structure in which an i-layer and a liquid crystal are stacked and sandwiched between a pair of polarizing plates.

〔産業上の利用分野〕[Industrial application field]

本発明は、電圧非印加時において垂直配向された液晶セ
ルを一対の偏光板で挟持する構成(DAP (Defo
rmation of A Iigned  Phas
es )方式)の液晶表示装置に関する。
The present invention has a configuration in which a vertically aligned liquid crystal cell is sandwiched between a pair of polarizing plates when no voltage is applied (DAP (Def
rmation of A Igned Phas
es ) type) liquid crystal display device.

近年、単純マトリクス方式の白黒表示液晶パネルの開発
が盛んに行なわれており、特に、大容量表示可能で、高
品位の表示可能な液晶表示装置の実現が要求されている
In recent years, simple matrix monochrome display liquid crystal panels have been actively developed, and in particular there is a demand for a liquid crystal display device capable of displaying a large capacity and high quality.

(従来の技術〕 第4図は従来装置の動作を説明する図を示し、同図(A
>は電圧非印加時、同図(B)は電圧印加時である。同
図(A)において、光1は偏光板2(偏光方向aが、液
晶部4の液晶分子の平面上における方向すに対して45
°の角度をもつ)を通過して直線偏光3とされ、液晶部
4に至る。液晶部4はそれぞれ透明電極(図示せず)を
形成したガラス基板5+ 、52の間に液晶6を設けら
れており、液晶6は初期状!21(透明電極よりの電圧
非印加時)において液晶分子が垂直配向(厳密に゛は僅
かな角度例えば右側に傾ぎをもつ)されており、後述の
電圧印加時に液晶分子が倒れる、いわゆる負の誘電率異
方性を有するものである。液晶部4に入った直線偏光3
は液晶6の屈折率の異方性の効果を受けずにそのままの
状態(直線偏光7)で通過し、しかる後偏光板8で遮断
され、黒表示となる。
(Prior art) Figure 4 shows a diagram explaining the operation of a conventional device.
> is when no voltage is applied, and (B) in the same figure is when voltage is applied. In the same figure (A), the light 1 is transmitted through the polarizing plate 2 (the polarization direction a is 45° with respect to the direction on the plane of the liquid crystal molecules of the liquid crystal section 4).
(with an angle of .degree.), becomes linearly polarized light 3, and reaches the liquid crystal section 4. In the liquid crystal section 4, a liquid crystal 6 is provided between glass substrates 5+ and 52 on which transparent electrodes (not shown) are formed, respectively, and the liquid crystal 6 is in its initial state! 21 (when no voltage is applied from the transparent electrode), the liquid crystal molecules are vertically aligned (strictly speaking, ゛ is tilted at a slight angle, for example, to the right), and when a voltage is applied, which will be described later, the liquid crystal molecules fall, which is the so-called negative alignment. It has dielectric constant anisotropy. Linearly polarized light 3 entering liquid crystal section 4
The light passes through as it is (linearly polarized light 7) without being affected by the anisotropy of the refractive index of the liquid crystal 6, and is then blocked by the polarizing plate 8, resulting in a black display.

一方、F1図(B)において、液晶部4の液晶6は透明
電極より電圧を印加されることにより液晶分子が右側に
倒れ、これにより、直線偏光3は液晶6の屈折率の異方
性の効果を受け、つまり、屈折率の異方性へ〇とセル厚
dとの積Δn−dによって偏光状態が変えられ、直線偏
光3と直線方向の偏光方向をもつ直線偏光9となる。直
線偏光9は偏光板2に対してクロスニコルの偏光板8を
そのまま通過し、白表示となる。
On the other hand, in Fig. F1 (B), the liquid crystal molecules of the liquid crystal 6 in the liquid crystal section 4 are tilted to the right by applying a voltage from the transparent electrode, and as a result, the linearly polarized light 3 is caused by the anisotropy of the refractive index of the liquid crystal 6. In other words, the polarization state is changed by the product Δn-d of the anisotropy of the refractive index and the cell thickness d, resulting in linearly polarized light 3 and linearly polarized light 9 having a linear polarization direction. The linearly polarized light 9 passes through the crossed Nicol polarizing plate 8 as it is with respect to the polarizing plate 2, resulting in a white display.

このように、垂直配向された液晶6に電圧をかけてその
液晶分子を倒すことにより、光のスイッチングを行ない
、白黒表示を行なう。これをDAP方式と称す。
In this way, by applying a voltage to the vertically aligned liquid crystal 6 and tilting the liquid crystal molecules, light switching is performed and a black and white display is performed. This is called the DAP method.

(発明が解決しようとする課題) 上記従来の装置では、パネルを真正面から見ている限り
では特に問題ないが、斜めから見た時は実質的に液晶6
のセル厚dが大きくなったのと同じことになり、液晶6
に予め設定されている初期のΔn−dの値が変化してし
まう。このため、直線偏光3の偏光状態を変化させる力
が初期に比して大きく働き、この結果、色がついて見え
、特に、白表示時において自立ら、表示品位が低下する
問題点があった。
(Problems to be Solved by the Invention) In the conventional device described above, there is no particular problem as long as the panel is viewed from the front, but when viewed from an angle, the liquid crystal
This is the same as increasing the cell thickness d of the liquid crystal 6.
The initial value of Δn-d, which is set in advance, changes. For this reason, the force that changes the polarization state of the linearly polarized light 3 acts more strongly than in the initial state, and as a result, there is a problem in that the display quality is degraded, especially when displaying white, and the display appears colored.

本発明は、斜めから見ても色がつかず、視角特性よく表
示できる液晶表示装置を提供することを目的とする。
SUMMARY OF THE INVENTION An object of the present invention is to provide a liquid crystal display device that can display images with good viewing angle characteristics without being colored even when viewed from an angle.

〔課題を解決するための手段〕[Means to solve the problem]

第1図は本発明の原理図を示す。同図中、40は負の誘
電率異方性を有する液晶、41a、41bは一対の偏光
板である。42は補償層で、屈折率の異方性を有し、該
異方性の軸方向が液晶40の液晶分子の平面上における
方向と90°をなすもので、液晶40に重ねてなる。補
償層42と液晶40とを重ねたものを上記一対の偏光板
41a。
FIG. 1 shows a diagram of the principle of the present invention. In the figure, 40 is a liquid crystal having negative dielectric constant anisotropy, and 41a and 41b are a pair of polarizing plates. Reference numeral 42 denotes a compensation layer which has anisotropy in refractive index, the axial direction of the anisotropy making an angle of 90° with the plane direction of the liquid crystal molecules of the liquid crystal 40, and is superimposed on the liquid crystal 40. The pair of polarizing plates 41a is formed by overlapping the compensation layer 42 and the liquid crystal 40.

41bで挟持してなる。41b.

(作用) 本発明では、補償層42は液晶40を通過した光の状態
を90°偏光する働きをもち、つまり、特に、液晶40
に電圧が印加されている時の液晶40の偏光作用の効果
を打消すように働く。従って、斜めから見て液晶40の
Δn−dが変化した分だけ[42のΔn−dも変化し、
これらは光の状態の変化を相殺する。
(Function) In the present invention, the compensation layer 42 has the function of polarizing the state of light passing through the liquid crystal 40 by 90°.
It acts to cancel the polarization effect of the liquid crystal 40 when a voltage is applied to the liquid crystal 40. Therefore, when viewed from an angle, the Δn-d of the liquid crystal 40 changes as much as the Δn-d of the liquid crystal 40 changes,
These compensate for changes in light conditions.

〔実施例〕〔Example〕

第2図は本発明の一実施例の構成図を示す。同図中、2
0は液晶表示パネルで、ガラス基板21、マトリクス状
透明電極22a、22b、配向剤23、液晶24、ガラ
ス基板25、シール材26にて構成されている。液晶2
4は誘電率εの異方性Δεが負(電圧非印加時に垂直配
向で、電圧印加時に液晶分子が倒れる)のネマティック
液晶であり、セル厚は例えば5μ■である。液晶24は
屈折率の異方性Δnとセル厚dとの積が約0,25μl
に設定されている。配向剤23は垂直配向のクロム錯体
と水平配向のポリイミド樹脂との混合物であり、ラビン
グにより液晶24が揃って僅かに右側に傾くようにして
あり、又、液晶24の液晶分子の平面上における方向は
偏光板27の偏光方向に対して45°である。
FIG. 2 shows a configuration diagram of an embodiment of the present invention. In the same figure, 2
0 is a liquid crystal display panel, which is composed of a glass substrate 21, matrix-like transparent electrodes 22a and 22b, an alignment agent 23, a liquid crystal 24, a glass substrate 25, and a sealing material 26. LCD 2
4 is a nematic liquid crystal whose anisotropy Δε of dielectric constant ε is negative (liquid crystal molecules are vertically aligned when no voltage is applied, and fall when a voltage is applied), and the cell thickness is, for example, 5 μι. The product of the refractive index anisotropy Δn and the cell thickness d of the liquid crystal 24 is approximately 0.25 μl.
is set to . The alignment agent 23 is a mixture of a vertically aligned chromium complex and a horizontally aligned polyimide resin, and by rubbing, the liquid crystal 24 is aligned and tilted slightly to the right, and the direction of the liquid crystal molecules of the liquid crystal 24 on the plane is adjusted. is 45° with respect to the polarization direction of the polarizing plate 27.

偏光板27.28は偏光板27に対して例えば平行ニコ
ルであり、偏光方向は液晶24の液晶分子の平面上の方
向Cに対して45°の角度をもつ。
The polarizing plates 27 and 28 are, for example, Nicol parallel to the polarizing plate 27, and the polarization direction is at an angle of 45° with respect to the direction C on the plane of the liquid crystal molecules of the liquid crystal 24.

29は補償層で、例えば透明なポリマ等の延伸フィルム
で、屈折率の異方性Δnとフィルム厚dとの積が液晶2
4と同じ約0.25μmに設定されており、屈折率の異
方性Δnの軸neの方向は、液晶24の液晶分子の平面
上の方向すに対して90゜の角度をもつ。
29 is a compensation layer, for example, a stretched film made of transparent polymer, etc., and the product of the refractive index anisotropy Δn and the film thickness d is the liquid crystal 2.
The direction of the axis ne of the refractive index anisotropy Δn is at an angle of 90° with respect to the plane direction of the liquid crystal molecules of the liquid crystal 24.

第3図は本発明装置の動作を説明する図を示し、同図(
A)は電圧非印加時、同図(B)は電圧印加時である。
FIG. 3 shows a diagram explaining the operation of the device of the present invention.
A) is when no voltage is applied, and (B) is when no voltage is applied.

同図(A)において、光1は偏光板27(偏光方向aが
、液晶24の液晶分子の平面上における方向すに対して
45°の角度をもつ)を通過して直線偏光30とされ、
液晶24に至る。
In the same figure (A), light 1 passes through a polarizing plate 27 (the polarization direction a has an angle of 45° with respect to the direction on the plane of the liquid crystal molecules of the liquid crystal 24) and becomes linearly polarized light 30,
The liquid crystal 24 is reached.

液晶24は初期状!g(電圧)1°印加時)において液
晶分子が垂直配向(厳密には僅かな角度例えば右側に傾
きをもつ)されており、後述の電圧印加時に液晶分子が
倒れる、いわゆる負の誘電重責方性を有するものである
。液晶24に入った直線偏光30は液晶24の屈折率の
異方性の効果を受けずにそのままの状態(直a偏光31
)で通過し、しかる後補償層29に入る。直線偏光31
は補償層29を通過する時に屈折率の異方性の効果によ
って偏光方向が90°変えられ(補償層29の屈折率の
異方性の軸neが直線偏光31と45°の角度にあるた
め)、直線偏光32として出射する。
LCD 24 is in its initial state! g (voltage) applied at 1°), the liquid crystal molecules are vertically aligned (strictly speaking, tilted at a slight angle, for example, to the right), and the liquid crystal molecules fall when a voltage is applied, which will be described later, resulting in so-called negative dielectric gravity. It has the following. The linearly polarized light 30 that has entered the liquid crystal 24 remains as it is without being affected by the anisotropy of the refractive index of the liquid crystal 24 (the linearly polarized light 31
) and then enters the compensation layer 29. Linear polarized light 31
When passing through the compensation layer 29, the polarization direction is changed by 90° due to the effect of refractive index anisotropy (because the axis ne of the refractive index anisotropy of the compensation layer 29 is at an angle of 45° with the linearly polarized light 31). ), the light is emitted as linearly polarized light 32.

そして、直線偏光32は偏光板28で遮断され、黒表示
となる。
Then, the linearly polarized light 32 is blocked by the polarizing plate 28, resulting in a black display.

一方、同図(B)において、液晶24は電圧を印加され
ることにより液晶分子が右側に倒れ、これにより、直線
偏光30は液晶24の屈折率の異方性の効果を受け、つ
まり、屈折率の異方性Δnとセル厚dとの積Δn−d(
=約0.25 μr* ) t、−よって偏光状態が変
えられ、直線偏光30と直角方向の偏光方向をもつ直線
偏光33となる。この場合、液晶24のΔn−dが0.
23 μm 〜0.27μmの範囲にあるとき、直線偏
光33は直線偏光30と直角になる。直線偏光33は補
償層29(Δn−dが0.23 μm 〜0.27 μ
+1の範囲にある)を通過する時、前述の電圧非印加時
と同時に屈折率の異方性の効果によって偏光方向が90
’変えられ、直線偏光34(直線偏光30と同じ)とさ
れ、偏光板28をそのまま通過し、白表示となる。
On the other hand, in the same figure (B), when the liquid crystal 24 is applied with a voltage, the liquid crystal molecules tilt to the right, and as a result, the linearly polarized light 30 is affected by the anisotropy of the refractive index of the liquid crystal 24, that is, it is refracted. The product of the rate anisotropy Δn and the cell thickness d Δn−d(
= approximately 0.25 μr*) t, - Therefore, the polarization state is changed and becomes linearly polarized light 33 having a polarization direction perpendicular to linearly polarized light 30. In this case, Δn-d of the liquid crystal 24 is 0.
In the range of 23 μm to 0.27 μm, linearly polarized light 33 is perpendicular to linearly polarized light 30. The linearly polarized light 33 is connected to the compensation layer 29 (Δn-d is 0.23 μm to 0.27 μm
+1 range), the polarization direction changes to 90° due to the effect of refractive index anisotropy at the same time as when no voltage is applied.
' is changed to linearly polarized light 34 (same as linearly polarized light 30), and passes through the polarizing plate 28 as it is, resulting in a white display.

ここで、電圧印加時における補償層29の補償作用につ
いて考えてみる。屈折率の異方性Δnと厚さdとの積Δ
n−dが等しい液晶24及び補償wa29は異方性の方
向が90°ずれており、このような構成では、補tri
層29は液晶24の偏光作用の効果を打消し、直線偏光
34は直線偏光31と同一となるように働く。従って、
斜めから見て液晶24の△n−dが変化した分だけ補f
aff129のΔn−dも変化し、これらは光の状態の
変化を相殺し、斜めから見た時色がつくことを防止でき
る。この場合、真正面に対して約30°の(従来は約1
5°)の斜めから見た場合まで色つき現象なく見ること
ができ、従来よりも視角特性よく表75できる。
Let us now consider the compensation effect of the compensation layer 29 when voltage is applied. Product Δ of refractive index anisotropy Δn and thickness d
The anisotropic directions of the liquid crystal 24 and the compensation wa 29 with the same n−d are shifted by 90 degrees, and in such a configuration, the compensation tri
The layer 29 counteracts the polarizing effect of the liquid crystal 24 so that the linearly polarized light 34 is identical to the linearly polarized light 31. Therefore,
Compensate f by the amount that △n-d of the liquid crystal 24 changes when viewed from an angle.
The Δn-d of the aff129 also changes, which cancels out changes in the state of light and prevents color from appearing when viewed from an angle. In this case, the angle of about 30 degrees (conventionally about 1
It can be seen without coloring even when viewed from an angle of 5 degrees, and the viewing angle characteristics are better than before.

〔発明の効果〕〔Effect of the invention〕

以上説明した如く、本発明によれば、特に液晶に電圧が
印加されている時に補償層によって液晶の偏光作用の効
果を打消すように働き、これにより、光の状態の変化を
相殺し、斜めから見た時に色はつかず、視角特性よく表
示できる。
As explained above, according to the present invention, the compensation layer works to cancel the polarizing effect of the liquid crystal, especially when a voltage is applied to the liquid crystal, thereby canceling out changes in the state of light and When viewed from above, no color appears and the display has good viewing angle characteristics.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の原理図、 第2図は本発明の一実施例の構成図、 第3図は本発明装置の動作を説明する図、第4図は従来
装置の動作を説明する図である。 図において、 20は液晶パネル、 24.40は液晶、 27.28.41a、41bは偏光板、29.42は補
償層、 30.31.32.33は直線偏光 を示す。
Fig. 1 is a diagram of the principle of the present invention, Fig. 2 is a block diagram of an embodiment of the present invention, Fig. 3 is a diagram explaining the operation of the device of the present invention, and Fig. 4 is a diagram explaining the operation of the conventional device. It is. In the figure, 20 is a liquid crystal panel, 24.40 is a liquid crystal, 27.28.41a and 41b are polarizing plates, 29.42 is a compensation layer, and 30.31.32.33 is linearly polarized light.

Claims (3)

【特許請求の範囲】[Claims] (1)負の誘電率異方性を有する液晶(40)を一対の
偏光板(41a)(41b)で挟持した構成の液晶表示
装置において、 屈折率の異方性を有し、該異方性の軸方向が上記液晶(
40)の液晶分子の平面上における方向と90゜をなす
補償層(42)を、上記液晶(40)に重ね、該補償層
(42)と上記液晶(40)とを重ねたものを上記一対
の偏光板(41a)(41b)で挾持してなることを特
徴とする液晶表示装置。
(1) In a liquid crystal display device having a configuration in which a liquid crystal (40) having negative dielectric constant anisotropy is sandwiched between a pair of polarizing plates (41a) (41b), having an anisotropy of refractive index, the anisotropy If the axis direction of the polarity is the above liquid crystal (
A compensation layer (42) forming an angle of 90 degrees with the plane direction of the liquid crystal molecules of 40) is stacked on the liquid crystal (40), and the stack of the compensation layer (42) and the liquid crystal (40) is stacked as the pair. A liquid crystal display device characterized in that it is sandwiched between polarizing plates (41a) and (41b).
(2)該液晶(40)は電圧非印加時において液晶分子
が揃つて一方向に傾いて略垂直に配向されており、 該偏光板(41a)(41b)の偏光方向は該液晶(4
0)の液晶分子の平面上における方向と45゜をなすこ
と特徴とする請求項1記載の液晶表示装置。
(2) In the liquid crystal (40), when no voltage is applied, the liquid crystal molecules are aligned and tilted in one direction and are oriented substantially vertically, and the polarization direction of the polarizing plates (41a) and (41b) is the same as that of the liquid crystal (40).
2. The liquid crystal display device according to claim 1, wherein the liquid crystal display device forms an angle of 45° with respect to the plane direction of the liquid crystal molecules of 0).
(3)該補償層(42)はポリマの延伸フィルムである
ことを特徴とする請求項1記載の液晶表示装置。
(3) The liquid crystal display device according to claim 1, wherein the compensation layer (42) is a stretched polymer film.
JP63170538A 1988-07-08 1988-07-08 Liquid crystal display device Pending JPH0220829A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63170538A JPH0220829A (en) 1988-07-08 1988-07-08 Liquid crystal display device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63170538A JPH0220829A (en) 1988-07-08 1988-07-08 Liquid crystal display device

Publications (1)

Publication Number Publication Date
JPH0220829A true JPH0220829A (en) 1990-01-24

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JP63170538A Pending JPH0220829A (en) 1988-07-08 1988-07-08 Liquid crystal display device

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Country Link
JP (1) JPH0220829A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03118450U (en) * 1990-03-15 1991-12-06
WO2015019997A1 (en) * 2013-08-08 2015-02-12 学校法人東京理科大学 Method for improving optical response and liquid crystal display device using same

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5092756A (en) * 1973-12-15 1975-07-24

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5092756A (en) * 1973-12-15 1975-07-24

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03118450U (en) * 1990-03-15 1991-12-06
WO2015019997A1 (en) * 2013-08-08 2015-02-12 学校法人東京理科大学 Method for improving optical response and liquid crystal display device using same
JP5866068B2 (en) * 2013-08-08 2016-02-17 学校法人東京理科大学 Method for improving optical response and liquid crystal display device using the same
CN105452947A (en) * 2013-08-08 2016-03-30 学校法人东京理科大学 Method for improving optical response and liquid crystal display device using same
KR20160041913A (en) * 2013-08-08 2016-04-18 갓코호우징 도쿄리카다이가쿠 Method for improving optical response and liquid crystal display device using same
US9575363B2 (en) 2013-08-08 2017-02-21 Tokyo University Of Science Foundation Method for improving optical response and liquid crystal display device using same

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