JPH04141630A - Reflection type liquid crystal electrooptic device - Google Patents

Reflection type liquid crystal electrooptic device

Info

Publication number
JPH04141630A
JPH04141630A JP2265632A JP26563290A JPH04141630A JP H04141630 A JPH04141630 A JP H04141630A JP 2265632 A JP2265632 A JP 2265632A JP 26563290 A JP26563290 A JP 26563290A JP H04141630 A JPH04141630 A JP H04141630A
Authority
JP
Japan
Prior art keywords
liquid crystal
phase plate
crystal layer
reflection
electro
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.)
Granted
Application number
JP2265632A
Other languages
Japanese (ja)
Other versions
JP3067189B2 (en
Inventor
Tomio Sonehara
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)

Abstract

PURPOSE:To eliminate coloration and light quantity loss and to improve threshold characteristics by arranging a polarizing element, a liquid crystal layer, a phase plate, and a reflection body in order as optical elements. CONSTITUTION:This device has basic structure wherein twisted nematic liquid crystal 104 is inserted between a substrate 103 where the reflection body 102 and phase plate 107 are installed and a transparent substrate 101. The the optical element constitution consists of the polarizing element 108, liquid crystal layer 104, phase plate 107, and reflection body 102 in order. Further, a transparent electrode 105 for applying an electric field to the liquid crystal layer is provided and the reflection body 102 formed of a thin film of metal serves as the other electrode. An incident/projection surface, a transparent electrode surface, and a reflecting surface are coated for reflection reduction to suppress unnecessary light beam reflection. Consequently, the degree of freedom of spectrum compensation increases to suppress the coloration and light quantity loss.

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
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a reflective liquid crystal electro-optical device using 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の波長板とシテ使
うもの、USP、4019807、特開昭56−436
81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 reflective liquid crystal electro-optical device using a twisted liquid crystal uses a uniaxial electro-optic medium with a 1/4λ wavelength plate, USP 4019807, JP-A-56-436.
As described in No. 81, the twist angle was 45 degrees, and the linearly polarized incident light was incident at an angle 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, conventional reflective liquid crystal electro-optical devices have a problem in that there is little margin for the thickness of the liquid crystal layer, and display performance tends to be uneven. Furthermore, since the output light is elliptically polarized,
There were also problems with the loss of light intensity and the coloration of the emitted light. Another problem was that the electro-optical characteristics change slowly with respect to voltage, making it unsuitable for multiplex drive. Therefore, it is an object of the present invention to provide a reflective electro-optical device that has a phase plate disposed on a reflective surface, which causes less color change, less light loss, and excellent threshold characteristics.

[課題を解決するための手段] 本発明の反射型液晶電気光学装置は、光学的要素として
、順に偏光素子、液晶層、位相板、反射体の配置をとる
ことを特徴とする。
[Means for Solving the Problems] The reflective liquid crystal electro-optical device of the present invention is characterized in that a polarizing element, a liquid crystal layer, a phase plate, and a reflector are arranged in this order as optical elements.

また、基板の一方が反射体と位相板を有することを特徴
とする。
Further, one of the substrates is characterized in that it has a reflector and a phase plate.

さらに基板の一方は、反射体である電極、該電極上に形
成された位相板を有することを特徴とする。
Furthermore, one of the substrates is characterized by having an electrode that is a reflector and a phase plate formed on the electrode.

また位相板は電気的な絶縁体であることを特徴とする。Further, the phase plate is characterized in that it is an electrical insulator.

以下、実施例により本発明の詳細を示す。Hereinafter, the details of the present invention will be shown by 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。[Example] Example 1 FIG. 1 is a sectional view of a reflective electro-optical device of the present invention.

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がはさまれた基本
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。
The reflective electro-optical device of the present invention has a basic structure in which a twisted nematic liquid crystal 104 is sandwiched between a transparent substrate 101 and a substrate 103 on which a reflector 102 and a phase plate 107 are installed. 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.
becomes. 105 is a transparent electrode for applying an electric field to the liquid crystal layer. A reflector 102 made of a metal thin film also serves as the other electrode. In addition, the entrance and exit surfaces, transparent electrode surfaces,
The reflective surface is coated with anti-reflection coating to suppress unnecessary light reflections.

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/n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 /n and thickness d is 0.5 μm, and the twist angle is 270°. Such conditions can be selected depending on 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Ta205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。
Furthermore, the phase plate of this example is described in "Optics Vol. 19, p. 93".
Ta205 was obliquely deposited on the reflector by the method described in . These specific conditions are shown in Table 1.

第1表 液晶層 ツイストネマティック ツイスト角 、dnd 0.5μm 偏光素子 吸収型直線偏光板 設置角 液晶の入射側夕゛イレクター に対し225°で偏光出射 位相板 蒸着角 nd 厚さ 設置角 Ta2’s  斜め蒸着膜 70’ 0.14μm 2μm 液晶の入射側夕゛イレクター に対し高屈折率方位を180゜ 反射体 アルミ蒸着膜 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
Table 1 Liquid crystal layer twist Nematic Twist angle, dnd 0.5 μm Polarizing element Absorption type linear polarizer installation angle Polarized light output phase plate deposition angle nd Thickness Installation angle Ta2's Oblique Vapor deposited film 70' 0.14 μm 2 μm Reflector aluminum vapor deposited film with high refractive index azimuth 180° with respect to the polarizer on the incident side of the liquid crystal Further, this phase plate can also serve as an alignment film for 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’App1. Phys、
 Letl、 Vol、42. p、492’に記載の
ようにPMMA樹脂をエツチングして作ることができる
This phase plate utilizes the polarization characteristics of a diffraction grating, and the obliquely deposited film has the function of a phase type diffraction grating. Therefore, a diffraction grating with a polarization function can be used in the same way. This is an effect observed in a diffraction grating made with a pitch less than the wavelength, for example 'App1. Phys.
Letl, Vol. 42. It can be made by etching PMMA resin as described in J. P., 492'.

また位相板と液晶層の間に光学的に等方向な層間膜を設
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ド塗
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 deposited layer and the diffraction grating on the alignment 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 insulating properties, it is possible to simultaneously protect the reflective electrode and isolate the liquid crystal and the electrode.

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 conventional ECB mode.
As shown in FIG. 2, it has a steep falling characteristic and can increase the number of multiplex drive lines. 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EC
B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A nd、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 shows the reflection spectrum when the switch is OFF. Traditional EC
Compared to the spectrum 302 of B mode (1/4λ mode), the present invention is also characterized in that it is possible to obtain a reflection spectrum 301 as wide as that even in a twisted state. This is done by designing the arrangement of the optical principal axis of the liquid crystal layer on the phase plate side and the high refractive index orientation of the phase plate, thereby canceling out the phase advance and phase delay due to the wavelength and compensating the reflection spectrum. As described above, according to the present invention, degrees of freedom are added to the phase amount of the phase plate to the And of the liquid crystal layer, the twist angle, and the angle of the polarizing element, making it possible to perform more free spectrum compensation.

実施例2 実施例2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、本実施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0本発明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4
01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。本実施例の詳細を第2表に示す。
Example 2 Example 2 is a case where a phase plate and a reflector are installed on the back side of a transparent substrate. The same thin film type phase plate as in Example 1 may be installed, but in this example, a commercially available film phase plate was bonded to the opposite side of the liquid crystal layer via a transparent substrate using an isotropic adhesive, and then A reflector was glued on top. FIG. 4 is a cross-sectional view thereof.The reflective electro-optical device of the present invention includes a reflector 402,
A transparent substrate 403 and a transparent substrate 4 on which a phase plate 407 is installed
It has a basic structure in which a twisted nematic liquid crystal 404 is sandwiched between 01 and 01. Therefore, the optical element configuration is
The polarizing element 408, the liquid crystal layer 404, the phase plate 407, and the reflector 402 are formed in this order. 405 is a transparent electrode for applying an electric field to the liquid crystal layer, and is installed on the liquid crystal side of the two transparent electrodes. Furthermore, anti-reflection coatings are applied to the input/output surfaces, transparent electrode surfaces, and reflective surfaces to suppress unnecessary light reflections. Details of this example are shown in Table 2.

第2表 液晶層 ツイストネマティック ツイスト角 270’ nd 0.93μm 偏光素子 設置角 吸収型偏光板 液晶の入射側夕゛イレクター に対し225°偏光 位相板 、6nd 設置角 1軸延伸型複屈折フイルム 0.14μm 液晶の入射側夕゛イレクター に対し高屈折率方位を180゜ 反射体 アルミ蒸着型反射フィルム 本実施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実施例3 実施例3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、5
o6は対向透明基板、507はアクティブ素子であるT
PT素子である。なお液晶セルの前方に置がれる偏光素
子として直線偏光板と偏光ビームスプリッタ−を選択で
きる。
Table 2 Liquid Crystal Layer Twisted Nematic Twist Angle 270'nd 0.93μm Polarizing Element Installation Angle Absorption Polarizer 225° with respect to the polarizer on the incident side of the liquid crystal Polarizing phase plate, 6nd Installation angle Uniaxially stretched birefringent film 0. 14 μm High refractive index orientation 180° with respect to the incident side polarizer of the liquid crystal Reflector Aluminum vapor deposited reflective film In this example, it is sufficient to install a phase plate and a reflector on the back side of a conventional liquid crystal electro-optical element, and the manufacturing process Embodiment 3 Embodiment 3 is an example in which the 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. An aluminum vapor-deposited film 503 is a reflector of the active matrix substrate 502, 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, 5
o6 is an opposing transparent substrate, 507 is an active element T
It is a PT element. Note that 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3表 液晶層 Δnd 偏光素子1 設置角 偏光素子2 設置角 位相板 蒸着角 、6nd 厚さ 設置角 反射体 アクナイフ1マトリクス基板 ツイストネマティック 63″′ 0.3μm 吸収型直線偏光板 液晶の入射側夕゛イレクター に対し108°で偏光出射 偏光ビームスプリッタ 液晶の入射側夕゛イレクター に対し108°で偏光出射 Ta2’s  斜め蒸着膜 70゜ 0.14μm 2μm 液晶の入射側夕′イレクター に対し高屈折率方位を153゜ アルミニウム蒸着膜 TPT設置石英ガラス基板 ツイスト角 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榮件を選んだ。
Table 3 Liquid crystal layer Δnd Polarizing element 1 Installation angle Polarizing element 2 Installation angle Phase plate Vapor deposition angle, 6nd Thickness Installation angle Reflector Akknife 1 Matrix substrate Twisted nematic 63''' 0.3 μm Absorption linear polarizer Liquid crystal incident side Polarized light output at 108° with respect to the elector Polarized beam splitter Polarized light output at 108° with respect to the elector Polarized beam splitter Polarized light output at 108° with respect to the elector Obliquely deposited film 70° 0.14 μm 2 μm High refractive index on the input side of the liquid crystal with respect to the elector The orientation is 153°.The twist angle of the quartz glass substrate with aluminum vapor deposited film TPT is installed.Figure 6 shows the electro-optical characteristics at that time.Figure 7 shows the reflection spectrum.Unlike Example 1.2, when driving with an active matrix, Since steep electro-optical characteristics are not required, this example selected a material with gentler electro-optic characteristics and a wider reflection spectrum than in Example 1.

第3表に示すように、偏光素子として偏光ビムスプリッ
ターを用いると、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 a polarizing element, under these conditions, when no voltage is applied, the reflectance is in an extinction state of 0, resulting in a display that is reversed from negative to positive with respect to a 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。
By laminating a reflective film and a phase plate on an active matrix substrate in this way, it was possible to simplify the manufacturing process and obtain a bright display with a wide reflection spectrum.

また従来の1/4^条件であるA nd=0.138μ
mに比べ、厚い液晶層を許容でき、液晶層の厚さ制御が
容易になる。
Also, the conventional 1/4^ condition is A nd = 0.138μ
Compared to M, a thicker liquid crystal layer can be tolerated, and the thickness of the liquid crystal layer can be easily controlled.

本実施例ではTPTを使用したが、M OS F ET
、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 TPT was used in this example, MOS FET
The same effect can be obtained with an active matrix that assists the driving of liquid crystals, such as a two-terminal device.

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 can be applied not only to the above embodiments but also to a wide range of reflective optical elements, light valves, and the like.

[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 in spectral compensation is increased, which has the effect of suppressing color change and loss of light amount. Furthermore, since the electro-optical characteristics are steep, it has the effect of excellent multiplex drive characteristics. Furthermore, since it is inserted between the reflective electrode and the liquid crystal, it has the effect of improving the reliability of the liquid crystal and the electrode. Furthermore, since the phase plate is installed closely inside the substrate, the structure is simple and the phase plate is less likely to be 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。
Furthermore, the type in which the phase plate is installed inside the substrate has the advantage that there is no double image caused by the thickness of the substrate.

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

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区は本発明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 位相板を設置されたアクティブマ ト リ ク 大基板 以 上
FIG. 1 is a sectional view of a reflective electro-optical device of 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 of the present invention when it is OFF. Section 4 is another cross-sectional view of the reflective electro-optical device according to the present invention. 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 shown in FIG. 5. FIG. 7 is a diagram showing the reflection spectrum of the LCD of FIG. 5. 101.401,506...Transparent substrate 102.402
,503...Reflector 103.403...Substrate 104 on which a phase plate is installed.
404,504...Liquid crystal layer 107.407,501...Phase plate 108.408...Active matrix large substrate on which polarizing element phase plate is installed or higher

Claims (1)

【特許請求の範囲】 1)対向する二枚の基板間にツイストしたネマチック液
晶を挟持した反射型液晶電気光学装置において、光学的
要素として、順に偏光素子、液晶層、位相板、反射体の
配置をとることを特徴とする反射型液晶電気光学装置。 2)該基板の一方が反射体と位相板を有することを特徴
とする請求項1記載の反射型液晶電気光学装置。 3)前記基板の一方は、反射体である電極、該電極上に
形成された位相板を有することを特徴とする請求項1記
載の反射型液晶電気光学装置。 4)前記位相板は電気的な絶縁体であることを特徴とす
る請求項1記載の反射型液晶電気光学装置。
[Claims] 1) In a reflective liquid crystal electro-optical device in which a twisted nematic liquid crystal is sandwiched between two opposing substrates, a polarizing element, a liquid crystal layer, a phase plate, and a reflector are arranged in order as optical elements. A reflective liquid crystal electro-optical device characterized by: 2) The reflective liquid crystal electro-optical device according to claim 1, wherein one of the substrates has a reflector and a phase plate. 3) The reflective liquid crystal electro-optical device according to claim 1, wherein one of the substrates has an electrode that is a reflector and a phase plate formed on the electrode. 4) The reflective liquid crystal electro-optical device according to claim 1, wherein the phase plate is an electrical insulator.
JP2265632A 1990-10-03 1990-10-03 Liquid crystal electro-optical device Expired - Fee Related JP3067189B2 (en)

Priority Applications (1)

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

Applications Claiming Priority (1)

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

Publications (2)

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

Family

ID=17419836

Family Applications (1)

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

Country Status (1)

Country Link
JP (1) JP3067189B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0737882A2 (en) * 1995-04-11 1996-10-16 Sony Corporation Reflection type guest-host liquid crystal display
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

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0737882A2 (en) * 1995-04-11 1996-10-16 Sony Corporation Reflection type guest-host liquid crystal display
EP0737882A3 (en) * 1995-04-11 1997-04-23 Sony Corp Reflection type guest-host liquid crystal display
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
KR100254834B1 (en) * 1996-04-30 2000-05-01 가네꼬 히사시 Liquid crystal display apparatus having improved gray scale display characteristics
US6160602A (en) * 1996-04-30 2000-12-12 Nec Corporation TN-mode liquid crystal display apparatus having improved gray scale display characteristics
US6580485B1 (en) 1996-04-30 2003-06-17 Nec Corporation Liquid crystal display apparatus having improved gray scale display characteristics
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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Publication number Publication date
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