JP3363640B2 - Liquid crystal display - Google Patents

Liquid crystal display

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Publication number
JP3363640B2
JP3363640B2 JP01454695A JP1454695A JP3363640B2 JP 3363640 B2 JP3363640 B2 JP 3363640B2 JP 01454695 A JP01454695 A JP 01454695A JP 1454695 A JP1454695 A JP 1454695A JP 3363640 B2 JP3363640 B2 JP 3363640B2
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JP
Japan
Prior art keywords
liquid crystal
light
degrees
crystal cell
angle
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.)
Expired - Lifetime
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JP01454695A
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Japanese (ja)
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JPH08201794A (en
Inventor
剛 須崎
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.)
Sanyo Electric Co Ltd
Original Assignee
Tottori Sanyo Electric Co Ltd
Sanyo Electric Co Ltd
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Application filed by Tottori Sanyo Electric Co Ltd, Sanyo Electric Co Ltd filed Critical Tottori Sanyo Electric Co Ltd
Priority to JP01454695A priority Critical patent/JP3363640B2/en
Publication of JPH08201794A publication Critical patent/JPH08201794A/en
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Publication of JP3363640B2 publication Critical patent/JP3363640B2/en
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Description

【発明の詳細な説明】 【0001】 【産業上の利用分野】本発明は視角依存性が低い液晶表
示装置に関する。 【0002】 【従来の技術】従来より、液晶セルを用いた表示装置
(特開昭60−107020公報)においては、一定以
上のコントラストと明度が得られる視野角(観察方向)
が限定される。つまり正面から表示を観察しても暗い表
示になりやすく、大きい画面においては表示周辺部に対
して斜め方向から観察したことになるのでコントラスト
が低下したりコントラスト反転が生じるという欠点があ
った。この様な視野角の制限が大きいことを視角依存性
が高いという。 【0003】視角依存性が生じる理由としては、液晶分
子の捩れ(螺旋の向きや、ラビング方向によって決まる
液晶分子の螺旋開始位置など)に起因するものや、液晶
の複屈折異方性(光の通過方向によるレタデ−ションの
相違など)に起因するものや、偏光板の特性(光振動方
向の選択性の良否など)に起因するものや、液晶に光を
照射する光源の指向性に起因するものなどが挙げられ
る。 【0004】そして一般に、液晶表示装置においては上
記視角依存性を考慮し、最も表示の見易い位置が観察者
の通常視野範囲内に入るような設計、例えば画面中央の
法線方向付近のコントラストをその周囲に比べて高める
ような設計が行われている。 【0005】 【発明が解決しようとする課題】本願出願人は、上記種
々の理由によって液晶表示装置に発生する視角依存性に
対処するため、液晶セルの表面に特殊フィルムを貼付し
て視角依存性を改善する提案を行った(特願平6−25
6877号他)。 【0006】ところが、上記特殊フィルムは、例えば法
線(φ=0度)から所定方向に30度程度の範囲までの
入射光を散乱するように設定された特殊構造を有する高
分子薄膜フィルムからなり、図2に示すようにそれを介
して対象物を観察したとき、例えば視点から正面片方向
に0度〜30度の範囲は不透明状態、それ以外の範囲は
透明に見えるように、入射光を選択的に拡散する機能を
有し、特に、上記角度範囲の内外でヘイズ率(全光線透
過率に対する散乱光線透過率の割合)が急峻に変化する
(不透明状態から透明状態あるいはその逆に透明状態か
ら不透明状態に急峻に変化する)構成であったため、不
透明状態から透明状態、あるいはその逆に透明状態から
不透明状態への境界線部分が明確になり、境界線部分に
おける表示の連続性が損なわれて表示品位が低下すると
いう新たな問題が発生した。そこで、本発明はこれを解
消することを主な課題とする。 【0007】 【課題を解決するための手段】本発明は、所定の液晶層
を有する液晶セルと、該液晶セルの液晶層に光を導く光
導入手段と、前記液晶セルから出てきた光の内、所定の
角度範囲で入射する光を選択的に拡散する光拡散手段と
を具備し、前記光拡散手段は、入射角度に応じたヘイズ
率(全光線透過率に対する散乱光線透過率の割合)が最
小の角度領域と最大の角度領域の間に、入射角度に応じ
てヘイズ率が徐々に変化する角度領域を形成し、光拡散
手段を介して液晶セルの固定位置を見る視点を液晶セル
の上側から下側に移動させたときに、視線と法線の成す
角度が上20度から下10度程度の範囲において液晶セ
ルから出てくる光が光拡散手段のヘイズ率が徐々に増加
する入射角度領域に入り、上10度から下30度程度の
範囲において前記液晶セルから出てくる光が前記光拡散
手段のヘイズ率が最大の入射角度領域に入り、下30度
から下50度程度の範囲において液晶セルから出てくる
光が光拡散手段のヘイズ率が徐々に減少する入射角度領
域に入ることを特徴とする。 【0008】 【0009】 【作用】本発明によれば、液晶セルから出てきた光の
内、所定の角度範囲で入射する光を選択的に拡散する光
拡散手段を備えるので、液晶分子の捩れ、液晶の複屈折
異方性、偏光板の特性、光源の指向性などの影響を受け
て液晶から出てきた光の内、希望する方向の光を光拡散
手段によって選択して拡散することができ、視角依存性
を低くすることができる。 【0010】また、光拡散手段は、入射角度に応じたヘ
イズ率が最小の角度領域と最大の角度領域の間に、入射
角度に応じてヘイズ率が徐々に変化する角度領域を形成
したので、ヘイズ率の急峻な変化がなく、不透明状態か
ら透明状態、あるいはその逆に透明状態から不透明状態
へ徐々に変化させることができ、液晶セルの表示連続性
を保って表示品位の低下を防止することができる。 【0011】 【0012】 【実施例】図1は本発明の実施例の液晶表示装置の要部
の断面図で、1は所定の厚みの液晶層10を有する液晶
セル、2はその液晶セル1の液晶層10に略垂直な方向
の光を導く光導入手段、3は液晶セル1から出てきた光
を拡散する光拡散手段である。 【0013】液晶セル1は、例えば液晶分子が90〜2
70度の螺旋状に整列されたいわゆるツイストネマティ
ック液晶層10を、画素毎に電界を印加する電極12が
内面に直交するように設けられた基板11により支えて
いる。液晶セル1に偏光板13が必要なときは、基板1
1の外側前後に貼付されるのが簡単で好ましい。また、
基板11には、液晶分子に所定の配向を形成するための
配向膜14を液晶層10を挟むようにして形成している
が、基板11に直接ラビングして配向する場合は配向膜
14を省略することもできる。ここで、高コントラスト
が得られる領域が液晶セル1の所定領域、例えば法線方
向ないし下側方向(図2の観察方向参照)となるような
配向処理が行われる。 【0014】光導入手段2は、例えば上面全面に、頂角
が90〜100度前後の微小なプリズムを10〜数10
0μmピッチで形成したポリカ−ボネ−ト等のプラスチ
ック製レンズシ−トで構成され、平坦裏面から入射した
光を集光して指向性を高めた光とする機能を有する。ま
た、光導入手段2は、アクリル樹脂、光学ガラスのよう
な透明平板の中にシリコンとかエポキシ樹脂、塩化銀等
の屈折率の異なる透明材料によりマイクロレンズを形成
して構成してもよいし、扁平凸レンズアレイや、凸レン
ズアレイと凹レンズアレイの積層体、若しくは複数の凸
レンズアレイや凹レンズアレイの積層体で構成してもよ
い。 【0015】光導入手段2の裏側には、必要に応じて面
照明手段4を設けることができる。この面照明手段4
は、例えばアクリル樹脂平板のような導光板41と、導
光板41の側面に設けられた冷陰極管などからなる線状
光源42と、必要に応じて導光板41に設けられた表面
光拡散シート43や裏面反射シート44、若しくは線状
光源を覆う筒状反射シート(図示せず)などによって構
成することができる。ここで、表面光拡散シート43
は、光導入手段2と兼用することもできる。 【0016】光拡散手段3は、図2に示すように、液晶
セル1と同じ四角平面形状を成しており、所定の範囲、
例えば法線(φ=0度)と成す角度が上50度程度から
下20度程度の角度範囲の入射光を入射角度に応じた拡
散度合で拡散するように設定された特殊構造を有する高
分子薄膜フィルムからなる。そして、この光拡散手段3
は、光の入射角度を変化させた場合の全光線透過率に対
する散乱光線透過率の割合を示すヘイズ率(数値が大き
い程光拡散度合い高い)が、図4に示すように設定され
ている。すなわち、入射角度(法線と入射光の成す角
度)が下90度から下20度程度の角度領域におけるヘ
イズ率を最小のほぼ0%に設定し、入射光を拡散するこ
となく透過させて透明状態を呈し、入射角度が上10度
から上30度程度の角度領域におけるヘイズ率を最大の
ほぼ80%に設定し、入射光のほとんどを拡散させて不
透明状態を呈するようにしている。尚、光拡散手段3
は、不透明状態においては、透明状態と同じ程度の光透
過率を有するとともに、透過する光の殆どを拡散して明
るいスリガラス状の外観を呈する。さらに、上記ヘイズ
率が最小の角度領域から最大の角度領域間の入射角度が
下20度から上10度程度の角度領域(少なくとも20
度以上の角度領域を有する)におけるヘイズ率は、最小
値から最大値に徐々に単調増加しながら変化するように
設定し、また、入射角度が上30度から上50度程度の
角度領域におけるヘイズ率は、最大値から最小値に徐々
に単調減少しながら変化するように設定している。 【0017】この光拡散手段3を構成する高分子薄膜フ
ィルムは、内部に例えばブラインド状の相構造を有する
アクリル系樹脂成形品とすることがでる。この成形品の
内部構造は、光学顕微鏡によって観察した場合、表面観
察では畳目状に寸断されてはいるがある程度の長さの相
が形成され、縦断面観察ではフィルム表面から約50μ
mの深さからブラインド状に濃淡をもつ相構造が形成さ
れている。この様な相構造の間隔は、フィルム上部で約
2μm、照射面から約300μmの深さでは3〜4μm
になっており、深さ方向に沿って次第に間隔が広くなっ
ているが、これらは所望の光拡散方向、光拡散度に応じ
て設定すればよい。また、上記相構造の方向を変化させ
て光照射面に対する相構造の傾きを変化させると、不透
明状態の発現角度を自由に設定することができととも
に、樹脂成形時の紫外線強度もしくは紫外線下を通過さ
せる速度を制御することにより、入射角度に応じたヘイ
ズ率を自由に設定することができるので、光拡散する光
の入射角度範囲や入射角度に応じたヘイズ率を必要に応
じて設定することができる。さらにまた、相構造間には
大きな組成分布の違いがあり、屈折率を例えば、一方の
相では1.55、他方の相では1.51と、相間の屈折
率差を0.4と大きな値に設定することができた。これ
らの値は、フィルムの深さ方向どの位置でも同じ値を示
すように成形することができる。高分子薄膜フィルム中
で生じる上述した視角依存性のある光散乱は、前記相構
造と相構造間の屈折率差に大きく起因して制御できるも
のである。そして、この様な光拡散手段3を構成する高
分子薄膜フィルムを市販品で入手しようとすれば、住友
化学工業株式会社製の視界制御フィルム(製品名「ルミ
スティ−」)のシリーズに対して光学特性を指定して用
いることが好ましい。 【0018】この光拡散手段3は、液晶セル1の表面に
接着剤を用いて貼付されるが、その際、光拡散手段3を
液晶セル1の所定の視角依存方向に対応させて両者の位
置決めが行われる。視角依存性の原因としては、例え
ば、液晶分子の捩れ(螺旋の向きや、ラビング方向によ
って決まる液晶分子の螺旋開始位置など)に起因するも
のや、液晶の複屈折異方性(光の通過方向によるレタデ
−ションの相違など)に起因するものや、偏光板の特性
(光振動方向の選択性の良否など)に起因するものや、
液晶に光を照射する光源の指向性に起因するものの1
つ、もしくはその組み合わせが考えられるので、それら
を考慮して視角依存方向に対応した位置決めが行われ
る。本実施例においては、例えば観察者が液晶セル1の
下側から上側を見るときの視野角を広くするように改善
する場合を例示し、図2に示すように、視点を固定し光
拡散手段3を介して観察するとき、光拡散手段3の存在
によって、対象物が不透明状態に見える視線の範囲(斜
線で図示)が、視点を通る法線に対して上50度から下
20度程度の範囲となるように、光拡散手段3を位置決
めして液晶セル1に貼付している。特に、液晶セル1か
ら改善すべき視野角方向(観察者側方向)へ向かう光
が、光拡散手段3(主にそのヘイズ率最大角度領域)に
よって拡散されるように、光拡散手段3が位置決めされ
て液晶セル1に貼付けられる。ここで、光拡散手段3は
薄膜フィルムによって構成しているので、表示装置の薄
型化を図ることができるとともに、接着剤などを用いて
液晶セル1に簡単に貼付することができるので、構造の
簡素化を図ることができる。 【0019】このようにして光拡散手段3を液晶セル1
に貼付した結果、図3に示すように、光拡散手段3を介
して液晶セル1の固定位置を見る視点を液晶セル1の上
側から下側に移動させて液晶セル1を観察したとき、視
線と法線の成す角度が上90度から上20度程度の範囲
においては、液晶セル1から出てくる光が光拡散手段3
のヘイズ率が最小の入射角度領域に入り、視線と法線の
成す角度が上20度から下10度程度の範囲において
は、液晶セル1から出てくる光が光拡散手段3のヘイズ
率が徐々に増加する入射角度領域に入り、視線と法線の
成す角度が下10度から下30度程度の範囲において
は、液晶セル1から出てくる光が光拡散手段3のヘイズ
率が最大の入射角度領域に入り、視線と法線の成す角度
が下30度から下50度程度の範囲においては、液晶セ
ル1から出てくる光が光拡散手段3のヘイズ率が徐々に
減少する入射角度領域に入る。したがって、光拡散手段
3のヘイズ率が最大の入射角度領域の前後にヘイズ率が
徐々に変化する領域が存在し、その領域は少なくとも2
0度の角度領域に及ぶので、ヘイズ率が最大(不透明状
態)角度領域と最小(透明状態)角度領域の間における
ヘイズ率の急激な変化を防いで画像の連続性を維持する
ことができ、表示品質を良好に保つことができる。尚、
光拡散手段3を貼付した結果、液晶セル1から光拡散手
段3に入射する光のうち、入射角度が上10から上30
度程度の光の殆どと、その近辺の角度領域の光の一部が
選択的に拡散されるので、液晶セル1から出てくる光を
平均化して出力することができ、輝度やコントラストを
全体的に平坦化して周辺部の輝度やコントラストを増加
させることができる。ここで、ヘイズ率が最大ないし最
大角度領域が法線方向(一般に最も輝度やコントラスト
が高い)を外れているので、法線方向の輝度やコントラ
スト低下を防止することができる。 【0020】上記実施例は、下方向(表示面を法線の下
側から上側に視線を配して観察する場合)の視野角を改
善する場合を例にしたが、上方向(表示面を法線の上側
から下側に視線を配して観察する場合)の視野角を改善
するためには、光拡散手段3の上下を反転して液晶セル
1に貼付すればよい。しかし、右方向もしくは左方向の
視野角を改善するためには、光拡散手段3を90度左右
に回転して液晶セル1に貼付すればよいものの、良視野
方向を下側に設定している本実施例においては、上下方
向ほどには視野角の改善ができなかった。 【0021】尚、光拡散手段を貼付する液晶セルとして
は、STN方式に限らず、TFT方式、MIM方式のも
のも対象とすることができる。 【0022】 【発明の効果】本発明によれば、液晶セルから出てきた
光の内、所定の角度範囲で入射する光を選択的に拡散す
る光拡散手段を備えるので、液晶分子の捩れ、液晶の複
屈折異方性、偏光板の特性、光源の指向性などの影響を
受けて液晶から出てきた光の内、希望する方向の光を光
拡散手段によって選択して拡散することができ、視角依
存性を低くすることができる。 【0023】また、光拡散手段は、入射角度に応じたヘ
イズ率が最小の角度領域と最大の角度領域の間に、入射
角度に応じてヘイズ率が徐々に変化する角度領域を形成
したので、ヘイズ率の急峻な変化がなく、不透明状態か
ら透明状態、あるいはその逆に透明状態から不透明状態
へ徐々に変化させることができ、液晶セルの表示連続性
を保って表示品位の低下を防止することができる。 【0024】また、光拡散手段は、散乱光線透過率が最
大となる角度領域を液晶セルの所定の視角依存方向に対
応させて液晶セルの観察者側に配置したので、液晶セル
観察者側の良視野範囲を光拡散手段によって拡大するこ
とができる。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a liquid crystal display having low viewing angle dependence. 2. Description of the Related Art Conventionally, in a display device using a liquid crystal cell (Japanese Patent Application Laid-Open No. 60-107020), a viewing angle (observation direction) at which a certain level of contrast and brightness can be obtained.
Is limited. In other words, even if the display is viewed from the front, the display tends to be dark, and a large screen has a disadvantage that the contrast is reduced or the contrast is inverted because the image is viewed obliquely with respect to the peripheral portion of the display. Such a large restriction on the viewing angle is referred to as having a high viewing angle dependency. [0003] The viewing angle dependence is caused by the twist of liquid crystal molecules (such as the helix direction and the helical start position of the liquid crystal molecules determined by the rubbing direction), and the birefringence anisotropy of the liquid crystal (the light Due to the difference in retardation depending on the passing direction), due to the characteristics of the polarizing plate (such as the selectivity of the light vibration direction), or due to the directivity of the light source that irradiates the liquid crystal with light. And the like. In general, in the liquid crystal display device, in consideration of the above-described viewing angle dependency, a design in which a position where the display is most easily viewed falls within a normal visual field range of an observer, for example, a contrast near a normal direction in the center of the screen is adjusted. It is designed to be higher than the surroundings. The applicant of the present invention has applied a special film to the surface of a liquid crystal cell to deal with the viewing angle dependency that occurs in a liquid crystal display device due to the above various reasons. Made a proposal (Japanese Patent Application No. 6-25)
No. 6877). However, the above-mentioned special film is made of a polymer thin film having a special structure set so as to scatter incident light within a range of about 30 ° in a predetermined direction from a normal line (φ = 0 °). As shown in FIG. 2, when observing the target object through it, for example, the incident light is opaque in a range of 0 to 30 degrees in one direction from the viewpoint to the front in one direction, and the other range is transparent so as to be transparent. It has a function of selectively diffusing, and in particular, the haze ratio (the ratio of the scattered light transmittance to the total light transmittance) changes steeply inside and outside the above-mentioned angle range (from an opaque state to a transparent state or vice versa) From the opaque state to the transparent state, or vice versa, the boundary part from the transparent state to the opaque state becomes clear, and the display continues at the boundary part. A new problem occurs that is display quality is lowered impaired. Therefore, it is a main object of the present invention to solve this. SUMMARY OF THE INVENTION The present invention provides a liquid crystal cell having a predetermined liquid crystal layer, light introducing means for guiding light to the liquid crystal layer of the liquid crystal cell, and light A light diffusing means for selectively diffusing light incident within a predetermined angle range, wherein the light diffusing means has a haze ratio (a ratio of a scattered light transmittance to a total light transmittance) according to an incident angle. Between the minimum angle area and the maximum angle area, an angle area where the haze ratio gradually changes according to the incident angle is formed, and the viewpoint of viewing the fixed position of the liquid crystal cell through the light diffusing means is viewed from the liquid crystal cell. When the angle between the line of sight and the normal line is in the range of about 20 degrees to about 10 degrees when moved from the upper side to the lower side, the light coming out of the liquid crystal cell is incident upon the haze ratio of the light diffusing means, which gradually increases. Enter the angle range and range from upper 10 degrees to lower 30 degrees In the above, light coming out of the liquid crystal cell enters the incident angle region where the haze ratio of the light diffusing means is maximum, and light coming out of the liquid crystal cell falls within the range of about 30 degrees to about 50 degrees below. It is characterized in that the rate falls in an incident angle region where the rate gradually decreases. According to the present invention, there is provided a light diffusing means for selectively diffusing light incident from a liquid crystal cell within a predetermined angle range, thereby torsion of liquid crystal molecules. The light diffusing means can select and diffuse light in the desired direction from the light coming out of the liquid crystal under the influence of the birefringence anisotropy of the liquid crystal, the characteristics of the polarizing plate, the directivity of the light source, etc. It is possible to reduce the viewing angle dependency. Further, the light diffusing means forms an angle region where the haze ratio gradually changes according to the incident angle between the angle region where the haze ratio according to the incident angle is minimum and the angle region where the haze ratio is maximum according to the incident angle. There is no sharp change in the haze ratio, and it is possible to gradually change from an opaque state to a transparent state, or vice versa, from a transparent state to an opaque state, thereby maintaining the display continuity of the liquid crystal cell and preventing the display quality from deteriorating. Can be. FIG. 1 is a sectional view of a main part of a liquid crystal display device according to an embodiment of the present invention, wherein 1 is a liquid crystal cell having a liquid crystal layer 10 having a predetermined thickness, and 2 is a liquid crystal cell 1 thereof. The light introducing means 3 for guiding light in a direction substantially perpendicular to the liquid crystal layer 10 is a light diffusing means for diffusing light coming out of the liquid crystal cell 1. The liquid crystal cell 1 has, for example, 90 to 2 liquid crystal molecules.
A so-called twisted nematic liquid crystal layer 10 spirally aligned at 70 degrees is supported by a substrate 11 on which an electrode 12 for applying an electric field for each pixel is provided so as to be orthogonal to the inner surface. When the polarizing plate 13 is necessary for the liquid crystal cell 1, the substrate 1
It is simple and preferable to be attached to the front and back of the outside of 1. Also,
On the substrate 11, an alignment film 14 for forming a predetermined alignment on the liquid crystal molecules is formed so as to sandwich the liquid crystal layer 10. However, when the alignment is performed by directly rubbing the substrate 11, the alignment film 14 is omitted. Can also. Here, an alignment process is performed such that a region where a high contrast is obtained is a predetermined region of the liquid crystal cell 1, for example, a normal direction or a downward direction (see the observation direction in FIG. 2). The light introducing means 2 includes, for example, a fine prism having an apex angle of about 90 to 100 degrees on the entire upper surface.
It is composed of a lens sheet made of plastic such as polycarbonate formed at a pitch of 0 μm, and has a function of condensing light incident from the flat back surface and converting the light into light with improved directivity. Further, the light introducing means 2 may be formed by forming a microlens with a transparent material having a different refractive index such as silicon, epoxy resin or silver chloride in a transparent flat plate such as acrylic resin or optical glass, It may be composed of a flat convex lens array, a laminate of a convex lens array and a concave lens array, or a laminate of a plurality of convex lens arrays and concave lens arrays. On the back side of the light introducing means 2, a surface illumination means 4 can be provided as required. This surface illumination means 4
Are a light guide plate 41 such as an acrylic resin flat plate, a linear light source 42 such as a cold cathode tube provided on a side surface of the light guide plate 41, and a surface light diffusion sheet 43 provided on the light guide plate 41 as necessary. Or a back reflection sheet 44 or a cylindrical reflection sheet (not shown) covering the linear light source. Here, the surface light diffusion sheet 43
Can also be used as the light introducing means 2. As shown in FIG. 2, the light diffusing means 3 has the same rectangular plane shape as the liquid crystal cell 1 and has a predetermined range,
For example, a polymer having a special structure that is set so as to diffuse incident light in an angle range from about 50 degrees above to about 20 degrees below the normal (φ = 0 degree) with a diffusion degree corresponding to the incident angle. Consists of a thin film. And this light diffusion means 3
As shown in FIG. 4, the haze ratio (the larger the numerical value, the higher the degree of light diffusion) indicating the ratio of the scattered light transmittance to the total light transmittance when the light incident angle is changed is set as shown in FIG. That is, the haze ratio in the angle range where the incident angle (the angle between the normal and the incident light) is from lower 90 degrees to lower 20 degrees is set to a minimum of almost 0%, and the incident light is transmitted without being diffused and is transparent. The haze ratio is set to approximately 80% of the maximum in an angle range where the incident angle is from about 10 degrees to about 30 degrees, and most of the incident light is diffused to exhibit an opaque state. The light diffusion means 3
In the opaque state, it has the same degree of light transmittance as the transparent state and diffuses most of the transmitted light to give a bright ground glass appearance. Further, the angle of incidence between the angle region where the haze ratio is the smallest and the angle region where the haze ratio is the largest is about 20 degrees below and about 10 degrees above (at least 20 degrees).
The haze ratio is set so as to gradually increase monotonically from the minimum value to the maximum value while changing monotonically, and the haze ratio in the angle region where the incident angle is from about 30 degrees to about 50 degrees. The rate is set so as to gradually decrease monotonically from the maximum value to the minimum value. The polymer thin film constituting the light diffusing means 3 can be an acrylic resin molded product having, for example, a blind phase structure inside. When the internal structure of this molded article is observed with an optical microscope, a phase of a certain length is formed although it is cut in a folded shape in the surface observation, and about 50 μm from the film surface in the longitudinal section.
A phase structure having shades of light and shade is formed from a depth of m. The interval of such a phase structure is about 2 μm at the upper part of the film, and 3 to 4 μm at a depth of about 300 μm from the irradiation surface.
The distance gradually increases along the depth direction, but these may be set in accordance with the desired light diffusion direction and light diffusion degree. Also, by changing the direction of the phase structure to change the inclination of the phase structure with respect to the light irradiation surface, it is possible to freely set the appearance angle of the opaque state, and to pass the ultraviolet light intensity during resin molding or under ultraviolet light. By controlling the speed at which the light is diffused, the haze ratio according to the incident angle can be set freely, so that the haze ratio according to the incident angle range and the incident angle of the light to be diffused can be set as necessary. it can. Furthermore, there is a large difference in the composition distribution between the phase structures. For example, the refractive index is as large as 1.55 in one phase, 1.51 in the other phase, and 0.4 as the refractive index difference between the phases. Could be set to. These values can be formed so as to show the same value at any position in the depth direction of the film. The above-mentioned light scattering having a viewing angle dependence generated in the polymer thin film can be controlled largely due to the refractive index difference between the phase structures. If a polymer thin film constituting the light diffusing means 3 is to be obtained as a commercial product, an optical control film (product name "Lumisty") manufactured by Sumitomo Chemical Co., Ltd. It is preferable to specify the characteristics and use them. The light diffusing means 3 is attached to the surface of the liquid crystal cell 1 using an adhesive. At this time, the light diffusing means 3 is positioned so as to correspond to a predetermined viewing angle dependent direction of the liquid crystal cell 1. Is performed. Causes of the viewing angle dependence include, for example, those caused by twisting of liquid crystal molecules (helix direction and helix start position of liquid crystal molecules determined by rubbing direction) and birefringence anisotropy of liquid crystal (light passing direction). Due to the difference in retardation of the polarizing plate), the characteristics due to the characteristics of the polarizing plate (such as the selectivity of the light vibration direction),
It is caused by the directivity of the light source that irradiates the liquid crystal with light.
One or a combination thereof is conceivable, and the positioning corresponding to the viewing angle dependent direction is performed in consideration of these. In the present embodiment, for example, a case where the viewing angle is improved so that the observer looks from the lower side to the upper side of the liquid crystal cell 1 is illustrated, and as shown in FIG. 3, the range of the line of sight (shown by oblique lines) in which the object looks opaque due to the presence of the light diffusing means 3 is about 50 degrees from the upper 50 degrees to the lower 20 degrees with respect to the normal passing through the viewpoint. The light diffusing means 3 is positioned and adhered to the liquid crystal cell 1 so as to fall within the range. In particular, the light diffusing means 3 is positioned such that light traveling from the liquid crystal cell 1 in the viewing angle direction (observer side direction) to be improved is diffused by the light diffusing means 3 (mainly the haze ratio maximum angle area). Then, it is attached to the liquid crystal cell 1. Here, since the light diffusing means 3 is formed of a thin film, the thickness of the display device can be reduced, and the light diffusing means 3 can be easily attached to the liquid crystal cell 1 using an adhesive or the like. Simplification can be achieved. Thus, the light diffusing means 3 is connected to the liquid crystal cell 1
As a result, as shown in FIG. 3, when the viewpoint of viewing the fixed position of the liquid crystal cell 1 via the light diffusing means 3 was moved from the upper side to the lower side of the liquid crystal cell 1 and the liquid crystal cell 1 was observed, When the angle between the normal and the normal line is in the range of about 90 degrees to 20 degrees, the light coming out of the liquid crystal cell 1
When the haze ratio of the liquid crystal cell 1 falls within the minimum incident angle region, and the angle between the line of sight and the normal line is in the range of about 20 degrees to about 10 degrees, the haze rate of the light diffusing unit 3 is reduced. When the light enters the gradually increasing incident angle region and the angle between the line of sight and the normal line is in the range of about 10 degrees to about 30 degrees, the light coming out of the liquid crystal cell 1 has the maximum haze ratio of the light diffusing means 3. When the angle between the line of sight and the normal line is in the range of about 30 degrees to about 50 degrees below the incident angle range, the light coming out of the liquid crystal cell 1 is incident angle at which the haze ratio of the light diffusing unit 3 is gradually reduced. Enter the area. Therefore, there is a region where the haze ratio gradually changes before and after the incident angle region where the haze ratio of the light diffusing unit 3 is the largest, and the region has at least two regions.
Since the haze ratio extends to an angle region of 0 degrees, the haze ratio can be prevented from sharply changing between a maximum (opaque state) angle region and a minimum (transparent state) angle region, thereby maintaining image continuity. Good display quality can be maintained. still,
As a result of attaching the light diffusing means 3, the incident angle of the light incident on the light diffusing means 3 from the liquid crystal cell 1 is from upper 10 to upper 30
Most of the light in the order of degrees and a part of the light in the angle region in the vicinity thereof are selectively diffused, so that the light coming out of the liquid crystal cell 1 can be averaged and output, and the brightness and contrast can be reduced as a whole. It is possible to increase the brightness and contrast of the peripheral portion by flattening. Here, since the haze ratio is the maximum or the maximum angle region deviates from the normal direction (generally, the brightness and contrast are the highest), it is possible to prevent the brightness and contrast from decreasing in the normal direction. In the above-described embodiment, the case of improving the viewing angle in the downward direction (when the display surface is viewed from the lower side of the normal line with the line of sight disposed above) is described as an example. In order to improve the viewing angle in the case where the line of sight is arranged from the upper side to the lower side of the normal line), the light diffusing unit 3 may be attached upside down to the liquid crystal cell 1. However, in order to improve the viewing angle in the right or left direction, the light diffusing means 3 may be rotated 90 degrees left and right and attached to the liquid crystal cell 1, but the good viewing direction is set to the lower side. In this embodiment, the viewing angle could not be improved as much as in the vertical direction. The liquid crystal cell to which the light diffusing means is attached is not limited to the STN type, but may be a TFT type or MIM type. According to the present invention, since light diffusing means for selectively diffusing light incident within a predetermined angle range from light emitted from a liquid crystal cell is provided, twisting of liquid crystal molecules, The light in the desired direction can be selected and diffused by the light diffusion means, out of the light coming out of the liquid crystal under the influence of the birefringence anisotropy of the liquid crystal, the characteristics of the polarizing plate, the directivity of the light source, etc. , The viewing angle dependency can be reduced. Further, the light diffusing means forms an angle region in which the haze ratio gradually changes according to the incident angle between the angle region where the haze ratio according to the incident angle is the minimum and the maximum angle region. There is no sharp change in the haze ratio, and it is possible to gradually change from an opaque state to a transparent state, or vice versa, from a transparent state to an opaque state, thereby maintaining the display continuity of the liquid crystal cell and preventing the display quality from deteriorating. Can be. Further, the light diffusing means arranges the angle region where the scattered light transmittance is maximum on the viewer side of the liquid crystal cell in correspondence with the predetermined viewing angle dependent direction of the liquid crystal cell. The good visual field range can be expanded by the light diffusing means.

【図面の簡単な説明】 【図1】本発明実施例の液晶表示装置の要部断面図であ
る。 【図2】本発明実施例の液晶セルと光拡散手段の配置を
示す斜視図である。 【図3】本発明実施例の光拡散手段の機能を説明するた
めの説明図である。 【図4】本発明の実施例にかかる光拡散手段の光学特性
図である。 【符号の説明】 1 液晶セル 2 光導入手段 3 光拡散手段 4 面照明手段
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a sectional view of a main part of a liquid crystal display device according to an embodiment of the present invention. FIG. 2 is a perspective view showing an arrangement of a liquid crystal cell and light diffusing means according to an embodiment of the present invention. FIG. 3 is an explanatory diagram for explaining a function of a light diffusing unit according to the embodiment of the present invention. FIG. 4 is an optical characteristic diagram of the light diffusing means according to the example of the present invention. [Description of Signs] 1 Liquid crystal cell 2 Light introducing means 3 Light diffusing means 4 Surface lighting means

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平4−234017(JP,A) 特開 昭60−202464(JP,A) 特開 昭64−40905(JP,A) 特開 昭60−140322(JP,A) 特開 平7−64069(JP,A) 特開 平7−209637(JP,A) 特開 平8−171087(JP,A) (58)調査した分野(Int.Cl.7,DB名) G02F 1/1335 G02F 1/13357 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-4-234017 (JP, A) JP-A-60-202464 (JP, A) JP-A-64-40905 (JP, A) JP-A-60-204 140322 (JP, A) JP-A-7-64069 (JP, A) JP-A-7-209637 (JP, A) JP-A-8-171087 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G02F 1/1335 G02F 1/13357

Claims (1)

(57)【特許請求の範囲】 【請求項1】 所定の液晶層を有する液晶セルと、該液
晶セルの液晶層に光を導く光導入手段と、前記液晶セル
から出てきた光の内、所定の角度範囲で入射する光を選
択的に拡散する光拡散手段とを具備し、前記光拡散手段
は、入射角度に応じたヘイズ率(全光線透過率に対する
散乱光線透過率の割合)が最小の角度領域と最大の角度
領域の間に、入射角度に応じてヘイズ率が徐々に変化す
る角度領域を形成し、前記光拡散手段を介して前記液晶
セルの固定位置を見る視点を液晶セルの上側から下側に
移動させたときに、視線と法線の成す角度が上20度か
ら下10度程度の範囲において前記液晶セルから出てく
る光が前記光拡散手段のヘイズ率が徐々に増加する入射
角度領域に入り、上10度から下30度程度の範囲にお
いて前記液晶セルから出てくる光が前記光拡散手段のヘ
イズ率が最大の入射角度領域に入り、下30度から下5
0度程度の範囲において前記液晶セルから出てくる光が
前記光拡散手段のヘイズ率が徐々に減少する入射角度領
域に入ることを特徴とする液晶表示装置。
(57) Claims 1. A liquid crystal cell having a predetermined liquid crystal layer, light introducing means for guiding light to the liquid crystal layer of the liquid crystal cell, and light out of the liquid crystal cell, Light diffusing means for selectively diffusing light incident in a predetermined angle range, wherein the light diffusing means has a minimum haze ratio (ratio of scattered light transmittance to total light transmittance) according to the incident angle. An angle region where the haze ratio gradually changes according to the incident angle is formed between the angle region and the maximum angle region of the liquid crystal.
View the fixed position of the cell from the top to the bottom of the liquid crystal cell
When moving, the angle between the line of sight and the normal is 20 degrees
Exits the liquid crystal cell within a range of about 10 degrees below
Light that the haze ratio of the light diffusing means gradually increases
Enter the angle range, and from the upper 10 degrees to the lower 30 degrees
Light coming out of the liquid crystal cell
The noise rate falls within the maximum incident angle range, from lower 30 degrees to lower 5 degrees.
The light coming out of the liquid crystal cell in a range of about 0 degrees
Incident angle region where the haze ratio of the light diffusing means gradually decreases
A liquid crystal display device characterized by entering a region .
JP01454695A 1995-01-31 1995-01-31 Liquid crystal display Expired - Lifetime JP3363640B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP01454695A JP3363640B2 (en) 1995-01-31 1995-01-31 Liquid crystal display

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP01454695A JP3363640B2 (en) 1995-01-31 1995-01-31 Liquid crystal display

Publications (2)

Publication Number Publication Date
JPH08201794A JPH08201794A (en) 1996-08-09
JP3363640B2 true JP3363640B2 (en) 2003-01-08

Family

ID=11864160

Family Applications (1)

Application Number Title Priority Date Filing Date
JP01454695A Expired - Lifetime JP3363640B2 (en) 1995-01-31 1995-01-31 Liquid crystal display

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Country Link
JP (1) JP3363640B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005099484A (en) * 2003-09-25 2005-04-14 Toshiba Matsushita Display Technology Co Ltd Liquid crystal display
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