JPH024220A - Liquid crystal device - Google Patents

Liquid crystal device

Info

Publication number
JPH024220A
JPH024220A JP63152914A JP15291488A JPH024220A JP H024220 A JPH024220 A JP H024220A JP 63152914 A JP63152914 A JP 63152914A JP 15291488 A JP15291488 A JP 15291488A JP H024220 A JPH024220 A JP H024220A
Authority
JP
Japan
Prior art keywords
liquid crystal
light
refractive index
polarized light
crystal device
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
JP63152914A
Other languages
Japanese (ja)
Inventor
Mitsuyoshi Hara
光義 原
Takayoshi Hanami
孝義 葉波
Kokichi Ito
伊藤 耕吉
Koji Iwasa
浩二 岩佐
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.)
Seiko Instruments Inc
Original Assignee
Seiko Instruments Inc
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 Seiko Instruments Inc filed Critical Seiko Instruments Inc
Priority to JP63152914A priority Critical patent/JPH024220A/en
Publication of JPH024220A publication Critical patent/JPH024220A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F1/00Devices 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
    • G02F1/01Devices 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 
    • G02F1/13Devices 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
    • G02F1/133Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
    • G02F1/1333Constructional arrangements; Manufacturing methods
    • G02F1/1335Structural association of cells with optical devices, e.g. polarisers or reflectors
    • G02F1/13363Birefringent elements, e.g. for optical compensation
    • GPHYSICS
    • G02OPTICS
    • G02FOPTICAL 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
    • G02F2413/00Indexing 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
    • G02F2413/01Number of plates being 1

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  • Physics & Mathematics (AREA)
  • Nonlinear Science (AREA)
  • Mathematical Physics (AREA)
  • Chemical & Material Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Liquid Crystal (AREA)

Abstract

PURPOSE:To obtain a sufficient contrast ratio and a light shielding property by providing a layer having an anisotropy of a refractive index with one layer or more on the inside of a pair of polarizing plates. CONSTITUTION:A light beam from a light source passes through a polarizer 62 is made into linearly polarized light, and also, elliptically polarized light by a refractive index anisotropy of a liquid crystal in a liquid crystal panel 63. Since such a refractive index anisotropy is different in accordance with wavelength, the elliptically polarized light which comes out is different in degree, therefore, a phase correcting plate 64 is placed so that each wavelength light returns to roughly linearly polarized light. When an analyzer of 65 is installed in the direction vertical to this polarization direction, it comes to scarcely allow a light beam to pass through and goes to black. When a voltage is applied to the liquid crystal panel 63, since the balance for compensating the elliptically polarized light is broken, the light beam which cannot be compensated leaks from the analyzer, and the display is executed thereby. In such a way, the light shielding property of a dark state ascends, the contrast ratio can be increased, and a liquid crystal device having a high picture quality is obtained.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は、コンピュータ一端末、画像表示装置、シャ
ッターのようなシステムに使用される液晶を用いた電気
光学装置、特に強誘電性液晶を用いた液晶装置において
1表示特性を改善した液晶装置に関するものである。
[Detailed Description of the Invention] [Field of Industrial Application] This invention relates to electro-optical devices using liquid crystals used in systems such as computer terminals, image display devices, and shutters, particularly electro-optical devices using ferroelectric liquid crystals. This invention relates to a liquid crystal device with improved display characteristics.

[発明の概要] この発明は液晶装置に関し、詳しくは一対の平行基板と
、前記一対の平行基板の面に対して垂直な複数の層を形
成している分子の配列を持つ強誘電性液晶とを有し、か
つ前記平行基板の外側に一対の偏光板をそなえた液晶装
置において、屈折率の異方性を持った層が前記一対の偏
光板の内側に1層以上あることにより、液晶表示装置の
透過スペクトルを可視光域においてニュートラルにし、
背景色を白色に、表示色を黒色に近づけることにより画
質の向上を狙ったものである。
[Summary of the Invention] The present invention relates to a liquid crystal device, and more specifically, a ferroelectric liquid crystal device having a pair of parallel substrates and an arrangement of molecules forming a plurality of layers perpendicular to the planes of the pair of parallel substrates. and a pair of polarizing plates on the outside of the parallel substrates, the liquid crystal display is The transmission spectrum of the device is made neutral in the visible light range,
The aim is to improve image quality by making the background color closer to white and the display color closer to black.

[従来の技術] 強誘電性液晶分子の屈折率異方性を利用して偏光素子と
の組合せにより透過光線を制御する型の表示装置がC1
arkおよびLagerwallにより提案されている
(特開昭56−107218号公報、米国特許4367
924号明細書等)。この強誘電性液晶は、一般に特定
の温度域において、カイラルスメクチックC相(SmC
ゞ)を有し、この状態において、印加される電界に対し
て2つの光学的安定状態をとり、かつ電界の印加されな
いときはその状態を保持する性質(双安定性)を有し、
表示装置としての広い利用が期待されている。
[Prior Art] C1 is a type of display device that uses the refractive index anisotropy of ferroelectric liquid crystal molecules to control transmitted light in combination with a polarizing element.
ark and Lagerwall (Japanese Unexamined Patent Publication No. 107218/1983, U.S. Patent No. 4367).
924 specification, etc.). This ferroelectric liquid crystal generally has a chiral smectic C phase (SmC) in a specific temperature range.
), and in this state, it has two optically stable states in response to an applied electric field, and has the property (bistability) of maintaining that state when no electric field is applied,
It is expected that it will be widely used as a display device.

ところで強誘電性液晶の配向方法としては、ラビング処
理や斜方蒸着処理などによる一軸配向処理を用いる方法
が知られている。
By the way, as a method for aligning ferroelectric liquid crystal, a method using a uniaxial alignment process such as a rubbing process or an oblique evaporation process is known.

しかし前述した配向制御膜をC1a rkらによって発
表された双安定性を示す非螺旋構造の強誘電性液晶に対
する配向制御に適用した場合には、下達のような課題を
有していた。
However, when the above-mentioned alignment control film was applied to control the alignment of a ferroelectric liquid crystal with a non-helical structure exhibiting bistability published by C1a rk et al., the following problems were encountered.

[発明が解決しようとする課題] 第5図に従来の液晶装置の断面図を示す。51a。[Problem to be solved by the invention] FIG. 5 shows a cross-sectional view of a conventional liquid crystal device. 51a.

sibは透明基板、52a、52bは透明導電膜、53
a。
sib is a transparent substrate, 52a, 52b are transparent conductive films, 53
a.

53bは一軸配向膜、54は液晶分子層、55はチルト
角、58は光源、59aは偏光子、59bは検光子、5
A、5Bはシーリング剤である。
53b is a uniaxial alignment film, 54 is a liquid crystal molecular layer, 55 is a tilt angle, 58 is a light source, 59a is a polarizer, 59b is an analyzer, 5
A and 5B are sealants.

ここで従来の配向制御膜によって配向させて得られた非
螺旋構造の強誘電性液晶でのチルト角が小さいため液晶
分子は透明基板に対して平行に並ばず、液晶分子層は「
くの字」になる。
Here, since the tilt angle of the ferroelectric liquid crystal with a non-helical structure obtained by alignment using a conventional alignment control film is small, the liquid crystal molecules are not aligned parallel to the transparent substrate, and the liquid crystal molecule layer is
It becomes "kunoji".

そのため第5図中51a、51bの偏光板の透過軸方向
をコントラスト比が最大になるように設置しても、十分
なコントラスト比と遮光性が得られず、視認性を低下さ
せていた。
Therefore, even if the transmission axes of the polarizing plates 51a and 51b in FIG. 5 are set so that the contrast ratio is maximized, a sufficient contrast ratio and light shielding property cannot be obtained, resulting in a decrease in visibility.

[課題を解決するための手段] 上記問題を解決するためにこの発明は一対の平行基板と
、その平行基板の面に対して垂直な複数のJt’Jを形
成している分子の配列を持つ強誘電性液晶とを有し、か
つ平行基板の外側に一対の偏光板をそなえた液晶装置に
おいて、屈折率の異方性を持った層が一対の偏光板の内
側に1層以上ある様に決められていることを特徴とする
ものである。
[Means for Solving the Problems] In order to solve the above problems, the present invention has a pair of parallel substrates and an arrangement of molecules forming a plurality of Jt'J perpendicular to the plane of the parallel substrates. In a liquid crystal device that has a ferroelectric liquid crystal and a pair of polarizing plates on the outside of parallel substrates, there is one or more layers with anisotropy of refractive index on the inside of the pair of polarizing plates. It is characterized by being determined.

[作用] 第6図は位相補正板を持つ液晶装置の動作原理にもとず
く作用を説明する図で、61は光源、62は偏光子、6
3は液晶駆動電圧が印加される液晶パネル、64は位相
補償板、65は検光子である。偏光子と検光子の透過軸
方向はコントラスト比が最大になるように決められてい
る。
[Function] FIG. 6 is a diagram explaining the function based on the operating principle of a liquid crystal device having a phase correction plate, in which 61 is a light source, 62 is a polarizer, and 6
3 is a liquid crystal panel to which a liquid crystal driving voltage is applied, 64 is a phase compensation plate, and 65 is an analyzer. The directions of the transmission axes of the polarizer and analyzer are determined to maximize the contrast ratio.

光源からの光は62の偏光子を通り直線偏光しさらに6
3の液晶パネル内の液晶の屈折率異方性により楕円偏光
になる。この屈折率異方性が波長により異なるため出て
くる楕円偏光の度合いが異なるが、64のように位相補
正板を置き、各波長光ともほぼ直線偏光に戻るようにす
る。この偏光方向に対し直角方向に65の一検光子を設
置すればほとんど光は通さなくなり、黒色になる。
The light from the light source passes through 62 polarizers and becomes linearly polarized.
It becomes elliptically polarized light due to the refractive index anisotropy of the liquid crystal in the liquid crystal panel No. 3. Since this refractive index anisotropy differs depending on the wavelength, the degree of elliptically polarized light that emerges differs, but a phase correction plate 64 is placed so that each wavelength of light returns to approximately linearly polarized light. If one analyzer 65 is installed in a direction perpendicular to this polarization direction, almost no light will pass through, resulting in a black color.

63の液晶パネルに電圧が印加されると楕円偏光補償の
バランスがくずれるため補償できない光が検光子からも
れ、これにより表示を行なう。
When a voltage is applied to the liquid crystal panel 63, the balance of elliptical polarization compensation is disrupted, so that light that cannot be compensated leaks from the analyzer, thereby producing a display.

[実施例] 以下に本発明の詳細を図示した実施例に基づいて説明す
る。
[Examples] The details of the present invention will be described below based on illustrated examples.

第1図は本発明に係る液晶装置で1図中性号11a、l
lbは液晶分子を挟持するためのガラス、プラスチック
等の透明基板で、表面に透明電極層12a、12bと、
さらに印刷、ディッピング、蒸着等によって、ポリイミ
ド、テフロン等の薄膜を形成し配向処理をした一軸性配
向膜層13a、 13bが設けられている。基板11a
とllbはその配向膜層どおしを対向させ、強誘電性液
晶分子14が一軸配向状態をとるようになっている。透
明電極層12a、12bには液晶駆動電圧が印加される
。17は位相補償板で屈折率の異方性を有する層を1層
以上積層している。18は光源、19aは偏光子、19
bは検光子である。LA、1Bは液晶分子を封入するた
めのシーリングである。
Figure 1 shows a liquid crystal device according to the present invention.
lb is a transparent substrate made of glass, plastic, etc. for sandwiching liquid crystal molecules, and has transparent electrode layers 12a and 12b on the surface,
Furthermore, uniaxial alignment film layers 13a and 13b are provided in which thin films of polyimide, Teflon, or the like are formed by printing, dipping, vapor deposition, etc., and then subjected to alignment treatment. Substrate 11a
and llb have their alignment film layers facing each other, so that the ferroelectric liquid crystal molecules 14 are uniaxially aligned. A liquid crystal driving voltage is applied to the transparent electrode layers 12a and 12b. Reference numeral 17 denotes a phase compensator, which has one or more laminated layers having anisotropy in refractive index. 18 is a light source, 19a is a polarizer, 19
b is an analyzer. LA and 1B are sealings for sealing liquid crystal molecules.

ここで本発明になる液晶装置の具体的実施例と測定結果
を説明する。
Here, specific examples and measurement results of the liquid crystal device according to the present invention will be described.

第2図は第1図で示した液晶装置における光学軸方向を
示した図であり、21は上偏光板透過軸方向、22は下
偏光板透過軸方向、23は屈折率の異方性を有する層に
おける屈折率の最大方向、24は強誘電性液晶の液晶分
子層方向である。25は下偏光板透過軸方向から液晶分
子層方向までの角度(以下[I]と略す)、26は下偏
光板透過軸方向から屈折率の異方性を有する層における
屈折率の最大方向までの角度(以下[D]と略す)、2
7は下偏光板透過軸方向から上偏光板透過軸方向までの
角度(以下[H]と略す)である。
FIG. 2 is a diagram showing the optical axis directions in the liquid crystal device shown in FIG. The maximum direction of refractive index in the layer 24 is the direction of the liquid crystal molecule layer of the ferroelectric liquid crystal. 25 is the angle from the lower polarizing plate transmission axis direction to the liquid crystal molecule layer direction (hereinafter abbreviated as [I]), 26 is the angle from the lower polarizing plate transmission axis direction to the maximum direction of refractive index in the layer having refractive index anisotropy angle (hereinafter abbreviated as [D]), 2
7 is an angle (hereinafter abbreviated as [H]) from the lower polarizing plate transmission axis direction to the upper polarizing plate transmission axis direction.

測定には屈折率の異方性を有する層としてポリカーボネ
イト系の一軸延伸フィルムを使用した。
In the measurement, a polycarbonate uniaxially stretched film was used as a layer having refractive index anisotropy.

角度の方向は時計回りを「十Jとした。The direction of the angle is ``10 J'' clockwise.

強誘電性液晶はピリミジン系の組成物を使用した。透明
基板に対し法線方向の液晶層の厚み(d)と強誘電性液
晶組成物の屈折率異方性(Δn)の積はΔn X d 
=0.25μmである。
A pyrimidine-based composition was used for the ferroelectric liquid crystal. The product of the thickness (d) of the liquid crystal layer in the normal direction to the transparent substrate and the refractive index anisotropy (Δn) of the ferroelectric liquid crystal composition is Δn X d
=0.25 μm.

また位相補正板の一軸延伸フィルムのリタデーションは
0.14μInである。
Further, the retardation of the uniaxially stretched film of the phase correction plate is 0.14 μIn.

(実施例1) ここでは背景が暗状態の場合、すなわちネガ・モードの
例を示す。
(Embodiment 1) Here, an example will be shown where the background is in a dark state, that is, in negative mode.

[I]=90’、[D]=O’、[H] = 35@で
ある。
[I] = 90', [D] = O', [H] = 35@.

第3図は本発明による液晶装置の電圧印加時の透過スペ
クトルで、1/400デユーティ−の駆動波形印加時で
ある。31は明状態の電圧が印加−されている時、32
は暗状態の電圧が印加されている時のスペクトルである
FIG. 3 shows the transmission spectrum of the liquid crystal device according to the present invention when a voltage is applied, and when a driving waveform of 1/400 duty is applied. 31 is 32 when the bright state voltage is applied.
is the spectrum when a dark state voltage is applied.

また第4図は従来の強誘電性液晶装置の透過スペクトル
である。上・下偏光板の透過軸方向は、第3図に示した
実施例と明状態の電圧が印加されている時のスペクトル
がほぼ一致するように設置した。41は明状態の電圧が
印加されている時、42は暗状態の電圧が印加されてい
る時のスペクトルである。
Furthermore, FIG. 4 shows the transmission spectrum of a conventional ferroelectric liquid crystal device. The transmission axes of the upper and lower polarizing plates were arranged so that the spectra of the embodiment shown in FIG. 3 and when a voltage in the bright state was applied were approximately the same. 41 is a spectrum when a bright state voltage is applied, and 42 is a spectrum when a dark state voltage is applied.

第3図、第4図の暗状態の電圧が印加されている場合の
透過率(550nm)は表1のようになる。
Table 1 shows the transmittance (550 nm) when the dark state voltage shown in FIGS. 3 and 4 is applied.

表1から明らかなように550nmにおける遮光性は、
従来の液晶装置と比較して上昇していることが解る。
As is clear from Table 1, the light shielding property at 550 nm is
It can be seen that this has increased compared to conventional liquid crystal devices.

(実施例2) ここでは背景が明状態の場合、すなわちポジ・モードの
例を示す。
(Embodiment 2) Here, an example will be shown where the background is in a bright state, that is, in positive mode.

[I]=35° [D] 、110@[H] =100
0である。
[I] = 35° [D] , 110@[H] = 100
It is 0.

この場合(実施例1)と同様の効果があった。The same effect as in this case (Example 1) was obtained.

実施例では第1図に示したように、液晶装置の背面に光
源を配置した状態で測定しているが、光源の代わりに反
射板を使用すれば、反射型の液晶表示装置として使用す
ることができる。
In the example, measurements were taken with a light source placed on the back of the liquid crystal device as shown in Figure 1, but if a reflector is used in place of the light source, it can be used as a reflective liquid crystal display device. I can do it.

(実施例1)、(実施例2)では角度を固定した場合の
結果を示したが、角度[I]、[D]、[H]をそれぞ
れ−30″〜+30’ずらしても同様の効果が得られる
(Example 1) and (Example 2) show the results when the angle is fixed, but the same effect can be obtained by shifting the angles [I], [D], and [H] by -30'' to +30', respectively. is obtained.

また液晶パネル、延伸フィルムのΔndを固定した場合
の結果を示したが、Δndを−0,1〜+0.1(μm
)変化させても、液晶パネルと延伸フィルムのΔndを
最適の値になるよう変化させれば同様の効果が得られる
In addition, the results are shown when the Δnd of the liquid crystal panel and stretched film is fixed, but the Δnd is -0.1 to +0.1 (μm
), the same effect can be obtained by changing Δnd between the liquid crystal panel and the stretched film to an optimal value.

実施例では強誘電性液晶としてピリミジン系の組成物を
使用したが他の系でも液晶パネルと延伸フィルムのΔn
d、光学軸方向を最適の値になるよう変化させれば同様
の効果が得られる。
In the examples, a pyrimidine-based composition was used as the ferroelectric liquid crystal, but other systems may also be used to improve the Δn of the liquid crystal panel and stretched film.
d. A similar effect can be obtained by changing the optical axis direction to an optimum value.

(実施例3) 前記実施例と同じ液晶装置の構成で、材質の異なる屈折
率異方性を有する層について効果を調べた。その結果、 セロハン、サクサンセルロース、ポリエチレン、ポリプ
ロピレン、ポリ塩化ビニル、ポリ塩化ビニリデン、ポリ
スチレン、ポリビニルアルコール、ポリエチレンテレフ
タレート、ナイロン、塩酸ゴム、ポリテトラフルオロエ
チレン、ポリイミドのフィルムにおいてもフィルムのΔ
ndが前記実施例と同一であれば同様の効果が得られた
(Example 3) Using the same liquid crystal device configuration as in the above example, the effects of layers having different refractive index anisotropy made of different materials were investigated. As a result, the film's ∆
Similar effects were obtained when nd was the same as in the previous example.

[発明の効果] 以上説明したように本発明によれば、一対の平行基板と
、その平行基板の面に対して垂直な複数の層を形成して
いる分子の配列を持つ強誘電性液晶とを有し、かつ下行
基板の外側に一対の偏光板をそなえた液晶装置において
、屈折率の異方性を持った層が一対の偏光板の内側に1
層以上あることにより、暗状態の遮光性が上昇し、コン
トラスト比を増加させることが可能となり、高画質の液
晶装置が得られる。
[Effects of the Invention] As explained above, according to the present invention, a ferroelectric liquid crystal having a pair of parallel substrates and an arrangement of molecules forming a plurality of layers perpendicular to the planes of the parallel substrates. In a liquid crystal device, a layer with anisotropy of refractive index is provided on the inside of the pair of polarizing plates.
By having more than one layer, the light-shielding property in the dark state is improved, the contrast ratio can be increased, and a liquid crystal device with high image quality can be obtained.

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

第1図は本発明の実施例の液晶装置の構成図、第2図は
本発明の実施例の液晶装置における光学軸方向を示す図
、第3図は本発明の実施例の液晶装置の透過スペクトル
図、第4図は従来の液晶装置の透過スペクトル図、第5
図は従来の液晶装置の構成図、第6図は液晶補正板を有
する液晶装置の動作原理を説明する図である。 11a 、 llb ・・・・・・・・透明基板12a
 、 12b ・・・・・・・・透明電極層13a 、
 13b ・・・・・・・・配向膜14・・・・・・・
・・・・・液晶分子17・・・・・・・・・・・・屈折
率の異方性を有する層 18・・・・・・・・・・・・光源 19a ・・・・・・・・・・・偏光子19b ・・・
・・・・・・・・検光子IA、 IB・・・・・・・・
・・液晶分子を封入するためのシーリング 出願人 セイコー電子工業株式会社
FIG. 1 is a configuration diagram of a liquid crystal device according to an embodiment of the present invention, FIG. 2 is a diagram showing the optical axis direction in a liquid crystal device according to an embodiment of the present invention, and FIG. 3 is a diagram showing transmission of the liquid crystal device according to an embodiment of the present invention. Spectrum diagram, Figure 4 is a transmission spectrum diagram of a conventional liquid crystal device, Figure 5 is a transmission spectrum diagram of a conventional liquid crystal device.
This figure is a block diagram of a conventional liquid crystal device, and FIG. 6 is a diagram illustrating the operating principle of a liquid crystal device having a liquid crystal correction plate. 11a, llb...Transparent substrate 12a
, 12b......Transparent electrode layer 13a,
13b...Alignment film 14...
......Liquid crystal molecules 17......Layer 18 having anisotropy of refractive index...Light source 19a... ...Polarizer 19b ...
......Analyzer IA, IB...
...Sealing for encapsulating liquid crystal molecules Applicant: Seiko Electronics Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] 一対の平行基板と、前記一対の平行基板の面に対して垂
直な複数の層を形成している分子の配列を持つ強誘電性
液晶とを有し、かつ前記平行基板の外側に一対の偏光板
をそなえた液晶装置において、屈折率の異方性を持った
層が前記一対の偏光板の内側に1層以上あることを特徴
とする液晶装置。
a pair of parallel substrates, and a ferroelectric liquid crystal having a molecular arrangement forming a plurality of layers perpendicular to the planes of the pair of parallel substrates, and a pair of polarized light beams arranged outside the parallel substrates. 1. A liquid crystal device comprising a plate, the liquid crystal device comprising one or more layers having anisotropy of refractive index inside the pair of polarizing plates.
JP63152914A 1988-06-21 1988-06-21 Liquid crystal device Pending JPH024220A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63152914A JPH024220A (en) 1988-06-21 1988-06-21 Liquid crystal device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63152914A JPH024220A (en) 1988-06-21 1988-06-21 Liquid crystal device

Publications (1)

Publication Number Publication Date
JPH024220A true JPH024220A (en) 1990-01-09

Family

ID=15550906

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63152914A Pending JPH024220A (en) 1988-06-21 1988-06-21 Liquid crystal device

Country Status (1)

Country Link
JP (1) JPH024220A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0432818A (en) * 1990-05-30 1992-02-04 Hitachi Ltd Liquid crystal display device
JPH04186224A (en) * 1990-11-21 1992-07-03 Canon Inc optical modulation element

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61290420A (en) * 1985-06-18 1986-12-20 Alps Electric Co Ltd Liquid crystal display element
JPS62148925A (en) * 1985-12-23 1987-07-02 Seiko Epson Corp liquid crystal optical modulator
JPH01183625A (en) * 1988-01-18 1989-07-21 Matsushita Electric Ind Co Ltd Liquid crystal display device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61290420A (en) * 1985-06-18 1986-12-20 Alps Electric Co Ltd Liquid crystal display element
JPS62148925A (en) * 1985-12-23 1987-07-02 Seiko Epson Corp liquid crystal optical modulator
JPH01183625A (en) * 1988-01-18 1989-07-21 Matsushita Electric Ind Co Ltd Liquid crystal display device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0432818A (en) * 1990-05-30 1992-02-04 Hitachi Ltd Liquid crystal display device
JPH04186224A (en) * 1990-11-21 1992-07-03 Canon Inc optical modulation element

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