JP3067189B2 - Liquid crystal electro-optical device - Google Patents

Liquid crystal electro-optical device

Info

Publication number
JP3067189B2
JP3067189B2 JP2265632A JP26563290A JP3067189B2 JP 3067189 B2 JP3067189 B2 JP 3067189B2 JP 2265632 A JP2265632 A JP 2265632A JP 26563290 A JP26563290 A JP 26563290A JP 3067189 B2 JP3067189 B2 JP 3067189B2
Authority
JP
Japan
Prior art keywords
liquid crystal
electro
phase plate
optical device
reflection
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 - Fee Related
Application number
JP2265632A
Other languages
Japanese (ja)
Other versions
JPH04141630A (en
Inventor
富雄 曽根原
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 Epson Corp
Original Assignee
Seiko Epson Corp
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 Epson Corp filed Critical Seiko Epson Corp
Priority to JP2265632A priority Critical patent/JP3067189B2/en
Publication of JPH04141630A publication Critical patent/JPH04141630A/en
Application granted granted Critical
Publication of JP3067189B2 publication Critical patent/JP3067189B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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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
    • G02F1/13356Structural association of cells with optical devices, e.g. polarisers or reflectors characterised by the placement of the optical elements
    • G02F1/133565Structural association of cells with optical devices, e.g. polarisers or reflectors characterised by the placement of the optical elements inside the LC elements, i.e. between the cell substrates
    • 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
    • G02F2203/00Function characteristic
    • G02F2203/02Function characteristic reflective

Landscapes

  • Liquid Crystal (AREA)

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は液晶を用いた反射型液晶電気光学装置に関す
る。
Description: TECHNICAL FIELD The present invention relates to a reflective liquid crystal electro-optical device using a liquid crystal.

[従来の技術] 従来のツイストした液晶を用いた反射型液晶電気光学
装置は一軸性の電気光学媒体を1/4λの波長板として使
うもの、USP.4019807、特開昭56−43681に記載のように
ツイスト角を45度とし、かつ直線偏光した入射光は分子
軸に対し傾けて入射するものであった。
[Prior Art] A conventional reflection type liquid crystal electro-optical device using a twisted liquid crystal uses a uniaxial electro-optical medium as a 1 / 4λ wave plate, as described in US Pat. No. 4019807 and JP-A-56-43681. As described above, the incident light having a twist angle of 45 degrees and being linearly polarized was incident with an inclination with respect to the molecular axis.

[発明が解決しようとする課題] しかし、従来の反射型液晶電気光学装置には液晶層の
厚みに対し余裕が少なく、表示性能にむらが生じ易いと
いう課題があった。更に出力光が楕円偏光であるため
に、光量の損失や、出射光に色がつく課題もあった。ま
た電圧に対する電気光学特性の変化が緩やかで、マルチ
プレックス駆動に適さないという課題があった。そこで
本発明では、反射面の上に位相板を設置することによっ
て色づき、光量損失が少なく、閾値特性に優れた反射型
電気光学装置を提供することを目的とするものである。
[Problems to be Solved by the Invention] However, the conventional reflection type liquid crystal electro-optical device has a problem that the margin of the thickness of the liquid crystal layer is small and the display performance tends to be uneven. Further, since the output light is elliptically polarized light, there are also problems such as loss of light quantity and coloring of the emitted light. Further, there is a problem that the change of the electro-optical characteristics with respect to the voltage is gradual and is not suitable for multiplex driving. In view of the above, an object of the present invention is to provide a reflection type electro-optical device which is colored by installing a phase plate on a reflection surface, has a small light amount loss, and has excellent threshold characteristics.

[課題を解決するための手段] 本発明の液晶電気光学装置は、対向する一対の基板間
に液晶を挟持してなる液晶電気光学装置において、前記
一対の基板の一方の基板の液晶側に前記反射体と前記位
相板が形成されてなり、前記他方の基板側のみに偏光手
段が配置されてなることを特徴とする。
[Means for Solving the Problems] In a liquid crystal electro-optical device according to the present invention, in which a liquid crystal is sandwiched between a pair of opposed substrates, the liquid crystal side of one of the pair of substrates is provided on a liquid crystal side. A reflector and the phase plate are formed, and a polarizing means is arranged only on the other substrate side.

以下、実施例により本発明の詳細を示す。 Hereinafter, the present invention will be described in detail with reference to examples.

[実施例] 実施例1 第1図は本発明の反射型電気光学装置の断面図であ
る。本発明の反射型電気光学装置は、反射体102、位相
板107を設置された基板103と透明基板101との間にツイ
ストしたネマチック液晶104がはさまれた基体構造を持
つ。従って、光学的な要素構成は、順に偏光素子108、
液晶層104、位相板107、反射体102となる。105は電界を
液晶層に印加するための透明電極である。もう一方の電
極は金属薄膜で形成された反射体102が兼ねている。さ
らに入出射面、透明電極面、反射面には減反射コーティ
ングが施され、不要な光線反射を抑制している。
Example Example 1 FIG. 1 is a sectional view of a reflection type electro-optical device according to the present invention. The reflective electro-optical device of the present invention has a base structure in which a twisted nematic liquid crystal 104 is sandwiched between a transparent substrate 101 and a substrate 103 provided with a reflector 102 and a phase plate 107. Therefore, the optical element configuration is, in order, the polarizing element 108,
The liquid crystal layer 104, the phase plate 107, and the reflector 102 are formed. 105 is a transparent electrode for applying an electric field to the liquid crystal layer. The other electrode also serves as a reflector 102 formed of a metal thin film. Further, an anti-reflection coating is applied to the incident / exit surface, the transparent electrode surface, and the reflection surface to suppress unnecessary light reflection.

液晶の条件としていくつかの好適な条件のなかで、こ
こではΔnと厚さdの積Δndを0.5μm、ツイスト角270
゜を選んでいる。このような条件は用いる位相板の性
能、必要な閾値特性によって選択することができる。
Among several suitable conditions for the liquid crystal, the product Δnd of Δn and the thickness d is 0.5 μm and the twist angle is 270.
゜ is selected. Such conditions can be selected according to the performance of the phase plate used and the required threshold characteristics.

また本実施例の位相板は、“光学第19巻、p.93"に記
載の方法によりTa2O5を反射体の上に斜め蒸着したもの
である。これら具体的な条件を第1表に示す。
The phase plate of this example is obtained by obliquely depositing Ta 2 O 5 on a reflector by the method described in “Optics, Vol. 19, p. 93”. Table 1 shows these specific conditions.

さらにこの位相板は液晶の配向膜を兼ねることができ
る。
Further, this phase plate can also serve as an alignment film of the liquid crystal.

この位相板は回折格子の偏光特性を利用したものであ
り、斜め蒸着膜が位相型回折格子の機能を有している。
従って偏光機能を持つ回折格子を同じように用いること
ができる。これは波長以下のピッチで作った回折格子で
観察される効果であり、例えば“Appl.Phys.Lett.,Vol.
42,p.492"に記載のようにPMMA樹脂をエッチングして作
ることができる。
This phase plate utilizes the polarization characteristics of the diffraction grating, and the obliquely deposited film has the function of a phase type diffraction grating.
Therefore, a diffraction grating having a polarizing function can be used in the same manner. This is an effect observed in a diffraction grating made with a pitch equal to or less than the wavelength, for example, “Appl. Phys. Lett., Vol.
42, p.492 ", by etching a PMMA resin.

また位相板と液晶層の間に光学的に等方的な層間膜を
設置してもよい。これは蒸着層や回折格子による液晶の
配向への影響を軽減すると共に、表面の平坦化を行なう
ことができる。本実施例ではポリイミドをスピンコート
塗布し、配向層及び保護層とした。
Further, an optically isotropic interlayer film may be provided between the phase plate and the liquid crystal layer. This can reduce the influence of the vapor deposition layer and the diffraction grating on the orientation of the liquid crystal, and can also flatten the surface. In this example, polyimide was spin-coated to form an alignment layer and a protective layer.

また絶縁特性を有する位相板を用いることによって反
射電極の保護、液晶と電極のアイソレーションを同時に
行なうこともできる。
Further, by using a phase plate having an insulating property, protection of the reflective electrode and isolation of the liquid crystal and the electrode can be performed simultaneously.

本装置の電気光学特性は従来のECBモードと異なり、
第2図に示すように急峻な立ち下り特性を有し、マルチ
プレックス駆動ライン数を増やすことができる。これは
STN液晶表示体と同じようなツイスト液晶の弾性による
効果である。
The electro-optical characteristics of this device are different from the conventional ECB mode.
As shown in FIG. 2, it has a sharp falling characteristic, and the number of multiplex drive lines can be increased. this is
This is an effect due to the elasticity of the twisted liquid crystal similar to the STN liquid crystal display.

第3図はOFF時の反射スペクトルである。従来のECBモ
ード(1/4λモード)のスペクトル302に比べ、本発明は
ツイストした状態であっても遜色ない広い反射スペクト
ル301を得ることができることも特徴である。これは位
相板側の液晶層の光学主軸と位相板の高屈折率方位の配
置を設計することによって波長による進相、遅相を相殺
し、反射スペクトルを補償するものである。このように
本発明によって液晶層のΔnd、ツイスト角、偏光素子の
角度に、位相板の位相量の自由度が加わり、より自由な
スペクトル補償が可能となった。
FIG. 3 is a reflection spectrum at the time of OFF. Compared with the conventional ECB mode (1 / 4λ mode) spectrum 302, the present invention is also characterized in that a broad reflection spectrum 301 comparable to that of a twisted state can be obtained. This is to cancel out the leading and lagging phases due to the wavelength by compensating the reflection spectrum by designing the arrangement of the optical axis of the liquid crystal layer on the phase plate side and the high refractive index direction of the phase plate. As described above, according to the present invention, the degree of freedom of the phase amount of the phase plate is added to the Δnd of the liquid crystal layer, the twist angle, and the angle of the polarizing element, so that more free spectrum compensation is possible.

参考例 参考例は位相板、反射体を透明基板の裏側に設置した
場合である。実施例1と同じ薄膜型の位相板を設置して
もよいが、本参考例では市販のフィルム位相板を透明基
板を介して液晶層の反対側に等方性接着剤で接着し、さ
らにその上に反射体を接着した。第4図はその断面図で
ある。本参考例の反射型電気光学装置は、反射体402、
位相板407を設置された透明基板403と透明基板401との
間にツイストしたネマチック液晶404がはさまれた基本
構造を持つ。従って、光学的な要素構成は、順に偏光素
子408、液晶層404、位相板407、反射体402となる。405
は電界を液晶層に印加するための透明電極であり、2枚
の透明電極の液晶側に設置されている。さらに入出射
面、透明電極面、反射面には減反射コーティングが施さ
れ、不要な光線反射を抑制している。本参考例の詳細を
第2表に示す。
Reference Example A reference example is a case where a phase plate and a reflector are installed on the back side of a transparent substrate. Although the same thin-film phase plate as in Example 1 may be installed, in this reference example, a commercially available film phase plate is bonded to the opposite side of the liquid crystal layer via a transparent substrate with an isotropic adhesive, and furthermore, The reflector was glued on top. FIG. 4 is a sectional view thereof. The reflective electro-optical device of the present reference example includes a reflector 402,
It has a basic structure in which a twisted nematic liquid crystal 404 is sandwiched between a transparent substrate 403 provided with a phase plate 407 and a transparent substrate 401. Therefore, the optical element configuration is, in order, the polarizing element 408, the liquid crystal layer 404, the phase plate 407, and the reflector 402. 405
Is a transparent electrode for applying an electric field to the liquid crystal layer, and is provided on the liquid crystal side of the two transparent electrodes. Further, an anti-reflection coating is applied to the incident / exit surface, the transparent electrode surface, and the reflection surface to suppress unnecessary light reflection. Table 2 shows details of this reference example.

本参考例では従来の液晶電気光学素子に位相板と反射
体を裏側に設置すれば済み、製造工程を変えなくても本
発明の優れた効果を得ることができる。
In this reference example, the phase plate and the reflector need only be installed on the back side of the conventional liquid crystal electro-optical element, and the excellent effects of the present invention can be obtained without changing the manufacturing process.

実施例2 実施例2は本発明をアクティブマトリクス型LCDに応
用した例である。第5図は本発明のアクティブマトリク
ス型LCDの断面図である。アクティブマトリクス基板502
の反射体であるアルミニウム蒸着膜503、その上に薄膜
位相板501が実施例1と同様に蒸着されている。したが
って、光学的な構成は実施例1とまったく同じである。
504は液晶層、505は透明対向電極、506は対向透明基
板、507はアクティブ素子であるTFT素子である。なお液
晶セルの前方に置かれる偏光素子として直線偏光板と偏
光ビ−ムスプリッタ−を選択できる。
Embodiment 2 Embodiment 2 is an example in which the present invention is applied to an active matrix type LCD. FIG. 5 is a sectional view of an active matrix type LCD of the present invention. Active matrix substrate 502
An aluminum vapor-deposited film 503 serving as a reflector, and a thin-film phase plate 501 is vapor-deposited thereon in the same manner as in the first embodiment. Therefore, the optical configuration is exactly the same as in the first embodiment.
504 is a liquid crystal layer, 505 is a transparent counter electrode, 506 is a counter transparent substrate, and 507 is a TFT element as an active element. In addition, a linear polarizing plate and a polarizing beam splitter can be selected as the polarizing element placed in front of the liquid crystal cell.

詳細なパラメーターを第3表に示す。 Detailed parameters are shown in Table 3.

第6図はそのときの電気光学特性。第7図は反射スペ
クトルである。実施例1、2と異なり、アクティブマト
リクスで駆動する場合には急峻な電気光学特性を必要と
しないので、本実施例では実施例1と比べてなだらかな
電気光学特性で、反射スペクトルが広い条件を選んだ。
FIG. 6 shows the electro-optical characteristics at that time. FIG. 7 is a reflection spectrum. Unlike the first and second embodiments, when driving with an active matrix, a steep electro-optical characteristic is not required. Therefore, in the present embodiment, a condition in which the electro-optical characteristic is gentler than that of the first embodiment and the reflection spectrum is wide is used. I chose.

第3表に示すように、偏光素子として偏光ビ−ムスプ
リッタ−を用いると、本条件では電圧がかからないとき
反射率が0の消光状態となり、直線偏光板に対し、ネガ
ポジが反転した表示となる。
As shown in Table 3, when a polarizing beam splitter is used as the polarizing element, the extinction state is 0 when no voltage is applied under this condition, and the display is in a state where the negative / positive is inverted with respect to the linear polarizing plate. .

このようにアクティブマトリクスの基板上に反射膜、
位相板を積層することによって、製造工程の簡単化、広
い反射スペクトルによる明るい表示を得ることができ
た。
Thus, a reflective film on the substrate of the active matrix,
By laminating the phase plates, it was possible to simplify the manufacturing process and obtain a bright display with a wide reflection spectrum.

また従来の1/4λ条件であるΔnd=0.138μmに比べ、
厚い液晶厚を許容でき、液晶層の厚さ制御が容易にな
る。
Also, compared to the conventional 1 / 4λ condition, Δnd = 0.138 μm,
A large liquid crystal thickness can be tolerated, and the thickness control of the liquid crystal layer becomes easy.

本実施例ではTFTを使用したが、MOSFET、2端子素子
など液晶の駆動を補助するアクティブマトリクスであれ
ば同じ効果を得ることができる。
Although a TFT is used in this embodiment, the same effect can be obtained with an active matrix such as a MOSFET or a two-terminal element that assists the driving of the liquid crystal.

以上実施例を述べたが、本発明は以上の実施例のみな
らず、広く反射型の光学素子、ライトバルブなどに応用
が可能である。
Although the embodiments have been described above, the present invention is widely applicable not only to the above embodiments but also to a wide range of reflection-type optical elements and light valves.

[発明の効果] 以上述べたように本発明によれば、スペクトル補償の
自由度が増し、これによって色づき、光量損失を抑えら
れるという効果を有する。また電気光学特性が急峻なた
めマルチプレックス駆動特性に優れるという効果を有す
る。さらに反射電極と液晶との間に入るため液晶、電極
の信頼性を向上させる効果がある。また基板の内側に位
相板を密着して設置するため、構成が簡単で位相板の損
傷が少ない利点を持つ。
[Effects of the Invention] As described above, according to the present invention, the degree of freedom of spectrum compensation is increased, thereby providing an effect of coloring and suppressing loss of light quantity. In addition, the steep electro-optical characteristics have an effect of excellent multiplex driving characteristics. Furthermore, since the liquid crystal enters between the reflective electrode and the liquid crystal, there is an effect of improving the reliability of the liquid crystal and the electrode. Further, since the phase plate is closely mounted on the inside of the substrate, there is an advantage that the configuration is simple and the phase plate is less damaged.

また基板の内側に位相板を設置するタイプは、基板厚
によって生じる2重像がない利点がある。
The type in which the phase plate is installed inside the substrate has an advantage that there is no double image caused by the thickness of the substrate.

【図面の簡単な説明】[Brief description of the drawings]

第1図は本発明の反射型電気光学装置の断面図である。 第2図は本発明の反射型電気光学装置の電気光学特性図
である。 第3図は本発明の反射型電気光学装置のOFF時の反射ス
ペクトルである。 第4図は参考例による反射型電気光学装置のもう一つの
断面図である。 第5図は本発明のアクティブマトリクス型LCDの断面図
である。 第6図は第5図のLCDの電気光学特性図である。 第7図は第5図のLCDの反射スペクトル を表す図である。 101,401,506……透明基板 102,402,503……反射体 103,403……位相板を設置された基板 104,404,504……液晶層 107,407,501……位相板 108,408……偏光素子 502……位相板を設置されたアクティブマトリクス基板
FIG. 1 is a sectional view of a reflective electro-optical device according to the present invention. FIG. 2 is an electro-optical characteristic diagram of the reflective electro-optical device of the present invention. FIG. 3 is a reflection spectrum of the reflection-type electro-optical device according to the present invention at the time of OFF. FIG. 4 is another sectional view of the reflection type electro-optical device according to the reference example. FIG. 5 is a sectional view of an active matrix type LCD of the present invention. FIG. 6 is an electro-optical characteristic diagram of the LCD of FIG. FIG. 7 is a diagram showing a reflection spectrum of the LCD of FIG. 101, 401, 506 Transparent substrate 102, 402, 503 Reflector 103, 403 Substrate provided with phase plate 104, 404, 504 Liquid crystal layer 107, 407, 501 Phase plate 108, 408 Polarizing element 502 Active matrix substrate provided with phase plate

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】対向する一対の基板間に液晶を挟持してな
る液晶電気光学装置において、前記一対の基板の一方の
基板の液晶側に前記反射体と前記位相板が形成されてな
り、前記他方の基板側のみに偏光手段が配置されてなる
ことを特徴とする液晶電気光学装置。
1. A liquid crystal electro-optical device comprising a pair of substrates facing each other, wherein a liquid crystal is sandwiched between a pair of substrates facing each other, wherein the reflector and the phase plate are formed on a liquid crystal side of one of the pair of substrates. A liquid crystal electro-optical device comprising a polarizing means arranged only on the other substrate side.
JP2265632A 1990-10-03 1990-10-03 Liquid crystal electro-optical device Expired - Fee Related JP3067189B2 (en)

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JP2265632A JP3067189B2 (en) 1990-10-03 1990-10-03 Liquid crystal electro-optical device

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Application Number Priority Date Filing Date Title
JP2265632A JP3067189B2 (en) 1990-10-03 1990-10-03 Liquid crystal electro-optical device

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JPH04141630A JPH04141630A (en) 1992-05-15
JP3067189B2 true JP3067189B2 (en) 2000-07-17

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Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08286214A (en) * 1995-04-11 1996-11-01 Sony Corp Reflection type guest-host liquid crystal display device
US6008875A (en) 1996-04-30 1999-12-28 Nec Corporation TN-mode liquid crystal display wherein a leveling layer is formed on the surface of an uneven electrode
US6091477A (en) * 1997-03-25 2000-07-18 The Hong Kong University Of Science & Technology Single polarized LCD consisting of particular twist angle and thickness-birefringence product

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