JPH0458610B2 - - Google Patents
Info
- Publication number
- JPH0458610B2 JPH0458610B2 JP61194617A JP19461786A JPH0458610B2 JP H0458610 B2 JPH0458610 B2 JP H0458610B2 JP 61194617 A JP61194617 A JP 61194617A JP 19461786 A JP19461786 A JP 19461786A JP H0458610 B2 JPH0458610 B2 JP H0458610B2
- Authority
- JP
- Japan
- Prior art keywords
- liquid crystal
- display
- cholesteric
- state
- light
- 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
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/01—Devices 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
- G02F1/13—Devices 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
- G02F1/137—Devices 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 characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering
- G02F1/13731—Devices 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 characterised by the electro-optical or magneto-optical effect, e.g. field-induced phase transition, orientation effect, guest-host interaction or dynamic scattering based on a field-induced phase transition
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/01—Devices 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
- G02F1/13—Devices 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
- G02F1/1313—Devices 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 specially adapted for a particular application
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/01—Devices 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
- G02F1/13—Devices 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
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL 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
- G02F1/00—Devices 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
- G02F1/01—Devices 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
- G02F1/13—Devices 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
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1347—Arrangement of liquid crystal layers or cells in which the final condition of one light beam is achieved by the addition of the effects of two or more layers or cells
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B21/00—Projectors or projection-type viewers; Accessories therefor
- G03B21/132—Overhead projectors, i.e. capable of projecting hand-writing or drawing during action
Landscapes
- Physics & Mathematics (AREA)
- Nonlinear Science (AREA)
- General Physics & Mathematics (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- Optics & Photonics (AREA)
- Liquid Crystal (AREA)
- Mathematical Physics (AREA)
- Liquid Crystal Display Device Control (AREA)
Description
【発明の詳細な説明】
〔概要〕
液晶セルの光波長選択性を利用して選択波長の
異なるセルを積層し、これに白色光を投写し、通
過光を集光レンズで集光してスクリーンに投写す
るカラー表示装置を提供する。[Detailed Description of the Invention] [Summary] Using the light wavelength selectivity of liquid crystal cells, cells with different selected wavelengths are stacked, white light is projected onto this, and the passing light is focused by a condensing lens to form a screen. The present invention provides a color display device for projecting images onto the screen.
本発明は螺旋構造をとるコレステリツク液晶の
波長選択性を利用する投写形カラー表示装置に関
する。
The present invention relates to a projection type color display device that utilizes the wavelength selectivity of a cholesteric liquid crystal having a helical structure.
今まで、液晶表示法として捩れネマテイツク効
果(Twisted Nematic Effect)を用いたTN表
示が一般に行われているが、偏光板を必要とする
ため投写表示を行うには、光損失が大きく、明る
い表示が得られにくい。 Until now, TN display using the twisted nematic effect has been commonly used as a liquid crystal display method, but since it requires a polarizing plate, projection display has a large optical loss and requires a bright display. Hard to obtain.
コレステリツク−ネマテイツク相転移型液晶を
用いるカラー表示装置は知られているが、これら
は投写型ではなく、直視型表示装置である(特開
昭59−116614、特開昭59−116680、特開昭52−
133781、特開昭61−32801、特開昭60−29091、特
開昭59−18925、特開昭57−124712、特開昭57−
111514、F.J.Kahn”ELECTRIC−FIELD−
INDUCED COLOR CHANGES AND PITCH
DILATION IN CHOLESTERIC LIQUID
CRYSTALS” PHYSICAL
REVIEWLETTERS Vol.24、No.5、1970、p209
−212)。更に、これらのカラー表示装置の着色原
理は本発明による多色カラー表示装置の着色原理
と異なる。又、特開昭57−201218はネマテイツク
液晶とコレステリツク液晶を主成分とする液晶層
が2層積層された液晶表示装置を示す。液晶分子
の螺旋軸が壁面に垂直配向するグランジユアン組
織を利用し電圧V4以上に印加して透明状態hと
した後、電圧を徐々に減少させた光散乱状態iを
経て第1記憶状態jとするか、電愛を急激に減少
させ透明状態g(第2記憶状態)とする。印加電
圧をoffした状態で、光散乱状態で(フオーカル
コニツク)−透明状態(グランジユアン)とで表
示する表示装置でありコントラスト比の改善であ
り、本発明の同一駆動電圧(Vd)でホメオトロ
ピツクとフオーカルコニツクとの双安定状態をと
る相移転型液晶を用いるものと異なる。又、カラ
ー表示に関し何ら述べない。 Color display devices using cholesteric-nematic phase change liquid crystals are known, but these are not projection type display devices but direct view type display devices (Japanese Patent Application Laid-open No. 59-116614, JP-A No. 59-116680, JP-A No. 59-116680, 52−
133781, JP-A-61-32801, JP-A-60-29091, JP-A-59-18925, JP-A-57-124712, JP-A-57-
111514, FJKahn”ELECTRIC−FIELD−
INDUCED COLOR CHANGES AND PITCH
DILATION IN CHOLESTERIC LIQUID
CRYSTALS” PHYSICAL
REVIEWLETTERS Vol.24, No.5, 1970, p209
−212). Furthermore, the coloring principle of these color display devices is different from the coloring principle of the multicolor color display device according to the invention. Further, Japanese Patent Application Laid-Open No. 57-201218 discloses a liquid crystal display device in which two liquid crystal layers each containing a nematic liquid crystal and a cholesteric liquid crystal as main components are laminated. Utilizing the Grange Yuan structure in which the helical axes of liquid crystal molecules are aligned perpendicular to the wall surface, a voltage of V4 or more is applied to obtain a transparent state h, and then the voltage is gradually reduced to a light scattering state i and then to a first memory state j. Alternatively, the electric power is rapidly reduced to a transparent state g (second memory state). This is a display device that displays a light scattering state (focalconic) and a transparent state (grunge) when the applied voltage is turned off, and improves the contrast ratio. This differs from those using phase-transition liquid crystals that take a bistable state between Also, nothing is said about color display.
一方ネマテイツク−コレステリツク相転移型液
晶表示は偏光板を用いないために明るく、見やす
い時を得ることができ、また単純マトリツクす構
成で大容量表示ができると云う特徴がある。 On the other hand, the nematic-cholesteric phase change type liquid crystal display is characterized in that it is bright and easy to view because it does not use a polarizing plate, and that it can display a large capacity with a simple matrix structure.
第3図は相転移型液晶を用いた投写型デイスプ
レイの表示原理を示すもので、横軸には印加電圧
を、縦軸には散乱することなく液相層を通過した
光量比(非散乱透過率)を示している。 Figure 3 shows the display principle of a projection display using a phase change liquid crystal. percentage).
すなわち、印加電圧が低い場合は液晶は螺旋状
態の分子配列をとるコレステリツク相をとり、光
は散乱されて投写用の集光レンズ18の外に散つ
てしまうため、スクリーン上では暗部となる。 That is, when the applied voltage is low, the liquid crystal assumes a cholesteric phase in which the molecules are arranged in a helical state, and the light is scattered and scattered outside the projection condensing lens 18, resulting in a dark area on the screen.
また、電圧が高い状態では液晶は電界の方向に
分子が配列したネマテイツク相となり、光は散乱
されずにレンズに入射するため、スクリーン上で
は明部となる。 Furthermore, when the voltage is high, the liquid crystal becomes a nematic phase in which molecules are aligned in the direction of the electric field, and light enters the lens without being scattered, resulting in a bright area on the screen.
このようにネマテイツク液晶にコレステリツク
液晶を混合した液晶組成物は電圧が掛からない状
態ではコレステリツク相を示しているが、電界の
増加によりネマテイツク相に変化し、一方、電界
を減じてゆくとネマテイツク相からコレステリツ
ク相に相転移が起こり、この際の相変化が印加電
圧に対してヒステリシスカーブを描くことが知ら
れている。 In this way, a liquid crystal composition in which cholesteric liquid crystal is mixed with nematic liquid crystal exhibits a cholesteric phase when no voltage is applied, but as the electric field increases, it changes to the nematic phase, and on the other hand, as the electric field decreases, it changes from the nematic phase to the cholesteric phase. It is known that a phase transition occurs in the cholesteric phase, and the phase change at this time draws a hysteresis curve with respect to the applied voltage.
このことは、同一の駆動電圧で光学的に異なる
双安定状態をとり得ることを示し、このメモリ効
果を利用して大容量表示が行われている。 This shows that optically different bistable states can be achieved with the same driving voltage, and this memory effect is used to perform large-capacity displays.
〔A.Mochizuki etc.“New Nematic−
Cholesteric LCD Using Hysteresis Behavior”
(ネマテイツク−コレステリツク液晶のヒステリ
シス特性を用いた表示方法)Proceedings of the
Society for Information Display(SID)26、No.
4、p243−248、1985]
本発明はかゝるネマテイツク−コレステリツク
相転移液晶を用いた投写型カラー表示に関するも
のである。 [A.Mochizuki etc. “New Nematic−
Cholesteric LCD Using Hysteresis Behavior”
(Display method using hysteresis characteristics of nematic-cholesteric liquid crystal) Proceedings of the
Society for Information Display (SID) 26, No.
4, p. 243-248, 1985] The present invention relates to a projection type color display using such a nematic-cholesteric phase change liquid crystal.
今まで、投写型のカラー表示法として、次の二
つの方法が知られているが、何れも実用化される
に到つていない。
Until now, the following two methods have been known as projection-type color display methods, but neither has yet been put into practical use.
RGB(Red−Green−Blue)フイルタを使う
方法。 How to use an RGB (Red-Green-Blue) filter.
それぞれ別の液相層を透過した光を光学系に
よつてスクリーン上で混合して投写する方法。 A method in which light that passes through different liquid phase layers is mixed and projected onto a screen using an optical system.
ここで、の方法はスクリーンに投写すると、
投写光量が白黒画像の場合の1/3以下になると云
う問題がある。 Here, the method is to project on the screen,
There is a problem in that the amount of projected light is less than 1/3 of that for black and white images.
すなわち、投写型デイスプレイを会議や公衆へ
の表示に用いる場合、暗闇で使用することは希で
あり、そのため投写光量が少ないと投写像が外部
光で隠れてしまうことによる。 That is, when a projection display is used for a meeting or for displaying to the public, it is rarely used in the dark, and therefore, if the amount of projected light is small, the projected image will be hidden by external light.
また、の方法は装置が大形化してしまい、高
価についてしまうと云う問題がある。 Further, the method (2) has the problem that the apparatus becomes large and expensive.
以上記したように液晶を使用した投写型のカラ
ー表示には性能的および価格的な問題がある。
As described above, projection-type color displays using liquid crystals have performance and cost problems.
そこで、大容量表示が可能な相転移型液晶表示
法を用い、明るく、解像度が高く、且つコンパク
トの投写型液晶表示装置を実現することが課題で
ある。 Therefore, it is an issue to realize a bright, high-resolution, and compact projection-type liquid crystal display device using a phase-transition liquid crystal display method that allows large-capacity display.
上記の目的は正の誘電率異方性を有するコレス
テリツク−ネマテイツク相転移型液晶の複数の層
を有する液晶パネルと、該液晶パネルに白色光を
はぼ垂直入射させ、該液晶パネル中の画素毎にホ
メオトロピツク状態とフオーカルコニツク状態を
選択することにより形成されたイメージをスクリ
ーン上に形成する光学系とを有し、上記相転移型
液晶は同一電圧でホメオトロピツクとフオーカル
コニツクとの双安定状態をとる相転移型液晶であ
り、上記複数の液晶層が液晶層の厚さ及び/又は
液晶材料の屈折率異方性を各々異なるように設定
することでフオーカルコニツク状態における透過
率の波長依存性が各々異なるように設定されてい
る投写型カラー表示装置により達成される。
The above purpose is to provide a liquid crystal panel having multiple layers of cholesteric-nematic phase change liquid crystal having positive dielectric constant anisotropy, to make white light almost perpendicularly incident on the liquid crystal panel, and to The phase change type liquid crystal has an optical system that forms an image on a screen by selecting a homeotropic state and a focal conic state. It is a phase change type liquid crystal in which the plurality of liquid crystal layers have different thicknesses and/or refractive index anisotropy of the liquid crystal material, so that the wavelength dependence of the transmittance in the focal conic state can be improved. This is achieved by projection type color display devices each having different settings.
本発明の投写型カラー表示装置において、コレ
ステリツク−ネマテイツク相転移型液晶はフオー
カルコニツク(コレステリツク)及びホメオトロ
ピツク(ネマテイツク)組織をとる。フオーカル
コニツク組織において液晶分子は螺旋軸が液晶パ
ネルに平行に配列される。フオーカルコニツク状
態の液晶分子の螺旋軸に垂直に入射する光は波長
選択性を有する散乱が生ずる。光がコレステリツ
ク相の液晶分子の螺旋軸に垂直に入射する時、波
長選択性を有する散乱が生ずる現象は本発明以前
知られていない。本発明の方法では、透過光の波
長或いは色相又は表示された色は僅かに入射角度
に依存するのみであり、セル厚さに顕著に依存す
る。これに対し、光がコレステリツク液晶分子の
螺旋軸に平行に入射した時、波長選択性を有する
反射が生ずることが公知である(前記、F.J.
Kahn)。又、特開昭59−116614、特開昭52−
133781では、コレステリツク液晶層はカラーフイ
ルターとして用いられる、しかし、コレステリツ
ク液晶層はグランジユアン組織であり、液晶分子
の螺旋軸は液晶パネル又は基板に垂直に配列す
る。これら公知の波長選択性を有する散乱では、
散乱光の波長はセル長さに依存せず、ラセンピツ
チと入射角度に依存する。 In the projection type color display device of the present invention, the cholesteric-nematic phase transition liquid crystal has focalonic (cholesteric) and homeotropic (nematic) structures. In the focal conic structure, the helical axes of liquid crystal molecules are aligned parallel to the liquid crystal panel. Light incident perpendicularly to the helical axis of the liquid crystal molecules in the focal conic state undergoes scattering with wavelength selectivity. Prior to the present invention, there was no known phenomenon in which wavelength-selective scattering occurs when light is incident perpendicularly to the helical axis of liquid crystal molecules in the cholesteric phase. In the method of the invention, the wavelength or hue of the transmitted light or the displayed color depends only slightly on the angle of incidence and significantly on the cell thickness. On the other hand, it is known that when light is incident parallel to the helical axis of cholesteric liquid crystal molecules, reflection with wavelength selectivity occurs (see above, FJ
Kahn). Also, JP-A-59-116614, JP-A-52-
In 133781, the cholesteric liquid crystal layer is used as a color filter, but the cholesteric liquid crystal layer has a grunge texture, and the helical axes of the liquid crystal molecules are aligned perpendicular to the liquid crystal panel or substrate. In these known wavelength-selective scattering methods,
The wavelength of the scattered light does not depend on the cell length, but on the helical pitch and incidence angle.
本発明はコレステリツク−ネマテイツク相転移
型液晶の光散乱を研究した結果なされたものであ
る。
The present invention was made as a result of research into light scattering of cholesteric-nematic phase transition type liquid crystals.
すなわち、発明者等は双安定状態におけるコレ
ステリツク相での光散乱は螺旋構造に由来するも
のであり、螺旋ピツチに対応した屈折率変調によ
つて光が回折されている点に着目した。 That is, the inventors focused on the fact that light scattering in the cholesteric phase in a bistable state originates from the helical structure, and that light is diffracted by refractive index modulation corresponding to the helical pitch.
すなわち、液晶分子は細長い構造をとり、屈折
率の異方性をもつているために液晶分子が基板に
垂直に配列している所と、、水平に配列している
所とでは屈折率が異なる。 In other words, liquid crystal molecules have an elongated structure and have anisotropy in refractive index, so the refractive index is different between where the liquid crystal molecules are aligned perpendicular to the substrate and where they are aligned horizontally. .
そのために螺旋ピツチに対応した屈折率変調が
存在し体積位相形の回折格子が形成されている。
回折効率ηはブラツグ角入射におけるH.
Kogelnicの式(THE BELLSYSTEM
TECHNICAL JOURNAL、Vol.48、No.9、
p2909−2947、1969)で表される。 Therefore, there is refractive index modulation corresponding to the helical pitch, and a volume phase type diffraction grating is formed.
The diffraction efficiency η is H at Bragg angle incidence.
Kogelnic's formula (THE BELLSYSTEM)
TECHNICAL JOURNAL, Vol.48, No.9,
p2909-2947, 1969).
ηnax=Sin2(πδnd/2λcosθ)
式で、δnは屈折率変調幅で、熱揺らぎなどの
擾乱のために液晶の屈折率異方性Δnよりも小さ
い値となる。λは波長、dは回折格子の厚さで、
ここではコレステリツク相の厚さに対応してい
る。また、θはブラツグ角でコレステリツク液晶
(フオーカルコニツク)の場合、cosθ≒1である。
なお、コレステリツク相においては螺旋ピツチに
はある程度のばらつきがあり、また螺旋軸の方向
は面内でランダムなため、光は幅の広い同心円状
に散乱される。 η nax = Sin 2 (πδnd/2λcosθ) In the formula, δn is the refractive index modulation width, which has a value smaller than the refractive index anisotropy Δn of the liquid crystal due to disturbances such as thermal fluctuation. λ is the wavelength, d is the thickness of the diffraction grating,
Here it corresponds to the thickness of the cholesteric phase. Further, θ is the Bragg angle, and in the case of a cholesteric liquid crystal (focal conic), cos θ≈1.
In the cholesteric phase, there is some variation in the helical pitch and the direction of the helical axis is random within the plane, so light is scattered in wide concentric circles.
これから、ηnaxはセル厚の増加に伴つて周期的
に変動することが判る。 From this, it can be seen that η nax fluctuates periodically as the cell thickness increases.
第1図は第3図に示したように広いヒステリシ
ス幅をもつ相転移型液晶についてセル厚と非散乱
透過率Ψnioとの関係を示すもので、光源としてア
ルゴン(Ar)レーザー1(波長476nm)とヘリ
ウム−ネオン(He−Ne)レーザ2(波長633n
m)を用いて測定した結果を示している。 Figure 1 shows the relationship between the cell thickness and the non-scattering transmittance Ψ nio for a phase change type liquid crystal with a wide hysteresis width as shown in Figure 3. ) and helium-neon (He-Ne) laser 2 (wavelength 633n)
The results of measurements using m) are shown.
ここで、Ψnioは第3図に示すヒステリシスルー
プにおいて最良の動作条件である駆動電圧vdを
印加したときのネマテイツク状態3の非散乱透過
光量に対するコレステリツク状態4の透過光量の
比である。 Here, Ψnio is the ratio of the amount of transmitted light in the cholesteric state 4 to the amount of unscattered transmitted light in the nematic state 3 when the driving voltage vd, which is the best operating condition, is applied in the hysteresis loop shown in FIG.
第1図からΨnioはセル厚が増すに従つて周期的
に変動し、また測定波長が短いと周期も短くなる
ことが判る。 From FIG. 1, it can be seen that Ψ nio changes periodically as the cell thickness increases, and that the shorter the measurement wavelength, the shorter the period.
同図から青色の表示を行うにはセル厚を7μm
とするのがよく、また赤色の表示を行うにはセル
厚を3μmとするのがよいことが判る。 From the same figure, to display blue color, the cell thickness should be 7 μm.
It can be seen that it is best to set the cell thickness to 3 μm in order to display a red color.
すなわちセル厚が7μmの場合は、He−Neレー
ザ光2は散乱される割合が多く非散乱透過率
(ψnio)が低い、一方Arレーザ光1は散乱される
割合が少なく非散乱透過率(ψnio)が高いので
He−Neレーザ光2の非散乱透過率及びArレー
ザ光1の非散乱透過率に応じた透過光となり、結
果として青色の光がスクリーンに投写される。 In other words, when the cell thickness is 7 μm, the He-Ne laser beam 2 has a high scattering rate and a low unscattered transmittance (ψ nio ), while the Ar laser beam 1 has a low scattering rate and a low unscattered transmittance (ψ nio ). ψ nio ) is high, so
The transmitted light corresponds to the non-scattered transmittance of the He--Ne laser beam 2 and the non-scattered transmittance of the Ar laser beam 1, and as a result, blue light is projected onto the screen.
また、3μmの場合はArレーザ光1は散乱され
る割合が多く非散乱透過率(ψnio)が低い、一方
He−Neレーザ光2は散乱される割合が少なく非
散乱透過率(ψnio)が高いのでHe−Neレーザ光
2の非散乱透過率及びArレーザ光1の非散乱透
過率に応じた透過光となり、結果として赤色の光
が投写されて赤色の表示が得られる。 In addition, in the case of 3 μm, the Ar laser beam 1 has a high scattering rate and the non-scattered transmittance (ψ nio ) is low;
Since the He-Ne laser beam 2 has a low scattering rate and a high non-scattered transmittance (ψ nio ), the transmitted light depends on the unscattered transmittance of the He-Ne laser beam 2 and the non-scattered transmittance of the Ar laser beam 1. As a result, red light is projected and a red display is obtained.
なお、より鮮やかな発色を得るには二色性色素
を併用するのは補助的手段として有効である。 Note that in order to obtain more vivid coloring, it is effective to use dichroic dyes as an auxiliary means.
本発明はこのようにコレステリツク−ネマテイ
ツク相転移型液晶を用いた液晶セルは第1図に示
すように波長選択性をもつことから、第4図に示
すように複数の液晶セルを重ね合わせ、これに光
を投写してカラー表示を行うものである。 Since a liquid crystal cell using a cholesteric-nematic phase transition type liquid crystal has wavelength selectivity as shown in FIG. It displays color by projecting light onto the screen.
第4図は二個の液晶セルを重ね合わせた例で、
両面に透明電極5を設けた第1のガラス基板6に
対向させて透明電極7を設けた第2のガラス基板
8,9を設け、セパレータ10により一定の間隔
を保つて液晶11を封入した構造をしている。 Figure 4 is an example of two liquid crystal cells stacked on top of each other.
A structure in which a first glass substrate 6 with transparent electrodes 5 provided on both sides is provided with second glass substrates 8 and 9 provided with transparent electrodes 7 on both sides, and liquid crystal 11 is sealed with a separator 10 at a constant distance. doing.
ここで、二個の液晶セルの厚さを、それぞれ表
示色に対応した光の波長に対して非散乱透過率が
高くなるように設定し、白色光に対して減色混合
によつて表示を行う。 Here, the thickness of the two liquid crystal cells is set so that the non-scattering transmittance is high for the wavelength of light corresponding to the display color, and display is performed by subtractive color mixing for white light. .
すなわち、二つの層ともネマテイツク相のとき
は白色表示となり、片方だけコレステリツク相の
ときは、そのセル厚の条件に対応した色となり、
両方ともコレステリツク相のときは二つの色の減
色混合色を呈することになる。 In other words, when both layers are in the nematic phase, the display is white, and when only one layer is in the cholesteric phase, the color corresponds to the cell thickness condition.
When both are in the cholesteric phase, they exhibit a subtractive mixture of the two colors.
第2図は本発明に使用した投写型表示装置の断
面図を示すもので、光源13よりの光は第1のフ
レネルレンズ14により平行光とした後、紫外線
カツトフイルタ15を通して液晶パネル16にほ
ぼ垂直に入射し、透過光は第2のフレネルレンズ
17でレズ18に集光され、ミラー19で反射さ
れて、スクリーン20に投影される。
FIG. 2 shows a cross-sectional view of the projection display device used in the present invention, in which the light from the light source 13 is made into parallel light by the first Fresnel lens 14, and then passes through the ultraviolet cut filter 15 and hits the liquid crystal panel 16 almost perpendicularly. The transmitted light is focused on a lens 18 by a second Fresnel lens 17, reflected by a mirror 19, and projected onto a screen 20.
ここで液晶パネル16は本実施例の場合、二個
の液晶セルで構成してあるが、この液晶の組成は
ネマテイツク液晶としてエタン系、ビシクロヘキ
サン系およびエステル系を主成分とする混合液晶
を87重量%、コレステリツク液晶として不斉炭素
を二個有するカイラルネマテイツク液晶を13重量
%を用い、これを等方相転移温度以上で混合して
相転移形液晶を作つた。 In this embodiment, the liquid crystal panel 16 is composed of two liquid crystal cells, and the composition of this liquid crystal is a mixed liquid crystal containing ethane, bicyclohexane, and ester as main components as a nematic liquid crystal. Chiral nematic liquid crystal having two asymmetric carbon atoms was used in an amount of 13% by weight as a cholesteric liquid crystal, and this was mixed above the isotropic phase transition temperature to produce a phase transition type liquid crystal.
この液晶をセル厚の異なる液晶セルに注入し、
セル厚と非散乱透過率との関係をHe−Neレーザ
(633nm)とArレーザ(476nm)を用いて測定
し、第1図の結果を得た。 This liquid crystal is injected into liquid crystal cells with different cell thicknesses,
The relationship between cell thickness and non-scattered transmittance was measured using a He-Ne laser (633 nm) and an Ar laser (476 nm), and the results shown in FIG. 1 were obtained.
この結果から青表示用のセルの厚さは7.0μm
に、また赤表示用のセルの厚さとして3.0μmを選
び、それぞれ80×120ドツトの表示パネルを形成
した。 From this result, the thickness of the cell for blue display is 7.0 μm.
In addition, 3.0 μm was selected as the thickness of the cells for red display, and display panels of 80×120 dots were formed for each cell.
これらの表示パネルに上記の相転移型液晶を注
入し、封止したが、その際に青表示用の液晶セル
には青の二色性色素を、また赤表示用液晶セルに
は赤の二色性色素を1重量%づつ添加した。 These display panels were injected with the above phase change type liquid crystal and sealed. At that time, a blue dichroic dye was added to the liquid crystal cell for blue display, and a red dichroic dye was added to the liquid crystal cell for red display. Color pigments were added in 1% by weight portions.
このように二層の液晶セルからなる表示パネル
16を第2図に示すように表示装置にセツトし、
また光源は650Wのハロゲンランプを用いた。 The display panel 16 consisting of two layers of liquid crystal cells is set in the display device as shown in FIG.
A 650W halogen lamp was used as the light source.
そして、青のカラー表示をする場合は赤表示用
の液晶セルはネマテイツク相として透明状態とし
ておき、青表示用の液晶セルに画像を形成して行
う。 In the case of blue color display, the liquid crystal cell for red display is kept in a transparent state as a nematic phase, and an image is formed on the liquid crystal cell for blue display.
また赤のカラー表示をする場合は同様に青表示
用の液晶セルは透明状態としておき、赤表示用の
液晶セルを表示させる。 Similarly, when displaying red color, the liquid crystal cell for blue display is kept in a transparent state, and the liquid crystal cell for red display is displayed.
また黒(現実にはやや紫)の表示を行うには両
方のセルを同時に表示させればよい。 Also, to display black (actually a little purple), both cells should be displayed at the same time.
このようにすることにより青、赤、黒、白(背
景部)の四色表示を行うことができた。 By doing this, it was possible to display four colors: blue, red, black, and white (background area).
なお、液晶セルを積層構成することにより、一
層の場合に較べて光損失が大きいように思われる
が、液晶セルがネマテイツク相をとる場合はセル
厚が薄いこともあり、透過率は良く、光吸収な影
響は無視することができる。 It should be noted that the layered structure of the liquid crystal cell seems to cause greater optical loss than the case of a single layer, but when the liquid crystal cell takes a nematic phase, the cell thickness is thin, so the transmittance is good and the light loss is large. Absorptive effects can be ignored.
以上記したようにコレステリツク−ネマテイツ
ク相転移型液晶セルを波長選択性をもたせて形成
し、これを重ね合わせて形成すると複数のカラー
表示を行うことができる。
As described above, by forming cholesteric-nematic phase change liquid crystal cells with wavelength selectivity and stacking them, a plurality of color displays can be performed.
なお、会議用や公衆表示用としては注意をひく
べき部分にのみ色付けを行うので、通常は二層構
成で足りるが、三層構成にすれば更に多くのカラ
ー表示を行うことができる。 Note that for conferences and public displays, only the parts that should attract attention are colored, so a two-layer structure is usually sufficient, but a three-layer structure allows for even more color display.
正の誘電率異方性及び同一電圧でコレステリツ
ク相(フオーカルコニツク状態)とネマテイツク
相(ホメオトロピツク状態)との双安定状態をと
ることができ電圧に対する相転移履歴を有するコ
レステリツク−ネマテイツク相転移型液晶を用い
る投写型の表示装置により、速いスイツチング、
明るく、大容量情報デイスプレイを可能にする利
点を有する。 A cholesteric-nematic phase transition type liquid crystal with positive dielectric anisotropy and a bistable state of a cholesteric phase (focalconic state) and a nematic phase (homeotropic state) at the same voltage, and a phase transition history with respect to voltage. A projection type display device that uses
It has the advantage of enabling bright, large-capacity information displays.
第1図は非散乱透過率(ψnio)とセル厚との関
係図、第2図は本発明に使用した投写型表示装置
の断面図、第3図は相転移型液晶について非散乱
透過率と印加電圧との関係図、第4図は本発明に
使用した液晶パネルの断面図。である。
図において、3はネマテイツク状態、4はコレ
ステリツク状態、11は液晶、13は光源、16
は液晶パネル、20はスクリーン、である。
Figure 1 is a diagram of the relationship between non-scattered transmittance (ψ nio ) and cell thickness, Figure 2 is a cross-sectional view of the projection display device used in the present invention, and Figure 3 is the non-scattered transmittance of phase change type liquid crystal. FIG. 4 is a cross-sectional view of the liquid crystal panel used in the present invention. It is. In the figure, 3 is a nematic state, 4 is a cholesteric state, 11 is a liquid crystal, 13 is a light source, and 16 is a cholesteric state.
is a liquid crystal panel, and 20 is a screen.
Claims (1)
ネマテイツク相転移型液晶の複数の層を有する液
晶パネルと、 該液晶パネルに白色光をほぼ垂直入射させ、該
液晶パネル中の画素毎にホメオトロピツク状態と
フオーカルコニツク状態を選択することにより形
成されたイメージをスクリーン上に形成する光学
系とを有し、 上記相転移型液晶は同一電圧でホメオトロピツ
クとフオーカルコニツクとの双安定状態をとる相
転移型液晶であり、 上記複数の液晶層が液晶層の厚さ及び/又は液
晶材料の屈折率異方性を各々異なるように設定す
ることでフオーカルコニツク状態における透過率
の波長依存性が各々異なるように設定されている
ことを特徴とする投写型カラー表示装置。[Claims] 1. Cholesteric material with positive dielectric anisotropy
A liquid crystal panel having multiple layers of nematic phase change type liquid crystal, and a liquid crystal panel formed by making white light almost perpendicularly incident on the liquid crystal panel and selecting a homeotropic state or a focal conic state for each pixel in the liquid crystal panel. The above-mentioned phase change type liquid crystal is a phase change type liquid crystal that takes a homeotropic and focal conic bistable state at the same voltage, and the above-mentioned plurality of liquid crystal layers are liquid crystal layers. A projection type characterized in that the wavelength dependence of transmittance in a focal conic state is set to be different by setting the thickness of the liquid crystal material and/or the refractive index anisotropy of the liquid crystal material to be different. Color display device.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61194617A JPS6349736A (en) | 1986-08-20 | 1986-08-20 | Projection type color display method |
| CA000544780A CA1278080C (en) | 1986-08-20 | 1987-08-18 | Projection-type multi-color liquid crystal display device |
| US07/086,803 US4832461A (en) | 1986-08-20 | 1987-08-19 | Projection-type multi-color liquid crystal display device |
| EP87307321A EP0259058B1 (en) | 1986-08-20 | 1987-08-19 | Projection-type multi-colour liquid crystal display device |
| DE3789081T DE3789081T2 (en) | 1986-08-20 | 1987-08-19 | Projection color liquid crystal display device. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61194617A JPS6349736A (en) | 1986-08-20 | 1986-08-20 | Projection type color display method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6349736A JPS6349736A (en) | 1988-03-02 |
| JPH0458610B2 true JPH0458610B2 (en) | 1992-09-18 |
Family
ID=16327511
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61194617A Granted JPS6349736A (en) | 1986-08-20 | 1986-08-20 | Projection type color display method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6349736A (en) |
Families Citing this family (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5189503A (en) * | 1988-03-04 | 1993-02-23 | Kabushiki Kaisha Toshiba | High dielectric capacitor having low current leakage |
| US5089810A (en) * | 1990-04-09 | 1992-02-18 | Computer Accessories Corporation | Stacked display panel construction and method of making same |
| US4966441A (en) * | 1989-03-28 | 1990-10-30 | In Focus Systems, Inc. | Hybrid color display system |
| US5050965A (en) * | 1989-09-01 | 1991-09-24 | In Focus Systems, Inc. | Color display using supertwisted nematic liquid crystal material |
| JP2951339B2 (en) * | 1989-10-27 | 1999-09-20 | 富士通株式会社 | Terminal member for fixed optical attenuator and fixed optical attenuator using the same |
| JPH03206425A (en) * | 1990-01-08 | 1991-09-09 | Fujitsu Ltd | Projection type liquid crystal display element |
| JP4033148B2 (en) | 2004-03-03 | 2008-01-16 | ソニー株式会社 | Lens barrel and imaging device |
| JP5560962B2 (en) * | 2010-06-30 | 2014-07-30 | ソニー株式会社 | Liquid crystal display |
-
1986
- 1986-08-20 JP JP61194617A patent/JPS6349736A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6349736A (en) | 1988-03-02 |
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