JPH0727161B2 - Display device in the finder - Google Patents

Display device in the finder

Info

Publication number
JPH0727161B2
JPH0727161B2 JP60173791A JP17379185A JPH0727161B2 JP H0727161 B2 JPH0727161 B2 JP H0727161B2 JP 60173791 A JP60173791 A JP 60173791A JP 17379185 A JP17379185 A JP 17379185A JP H0727161 B2 JPH0727161 B2 JP H0727161B2
Authority
JP
Japan
Prior art keywords
grating
display device
optically anisotropic
electric field
liquid crystal
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
JP60173791A
Other languages
Japanese (ja)
Other versions
JPS6234142A (en
Inventor
肇 坂田
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.)
Canon Inc
Original Assignee
Canon 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 Canon Inc filed Critical Canon Inc
Priority to JP60173791A priority Critical patent/JPH0727161B2/en
Priority to DE19863627113 priority patent/DE3627113A1/en
Priority to GB8619323A priority patent/GB2180946B/en
Publication of JPS6234142A publication Critical patent/JPS6234142A/en
Priority to US08/092,569 priority patent/US5299037A/en
Publication of JPH0727161B2 publication Critical patent/JPH0727161B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Liquid Crystal (AREA)
  • Indication In Cameras, And Counting Of Exposures (AREA)
  • Diffracting Gratings Or Hologram Optical Elements (AREA)

Description

【発明の詳細な説明】 (1)技術分野 本発明は、表示装置、特にカメラやビデオ等の撮影装置
に於るファインダー内に、撮影時の各種情報を表示する
表示装置に関する。
Description: TECHNICAL FIELD The present invention relates to a display device, and more particularly to a display device for displaying various information at the time of shooting in a viewfinder of a shooting device such as a camera or a video.

(2)従来技術 従来、カメラやビデオ等の撮影装置に於るフアインダー
内に、所定の撮影情報を表示する場合、撮影視野枠の外
側に配置されたLEDや液晶を用いていた。しかしなが
ら、この様な機構では、露出状態の不適切を警告する表
示を見落とす可能性があり、更に、撮影視野内の合焦領
域や露出適正領域等を表示する事は不可能であった。
(2) Conventional Technology Conventionally, when displaying predetermined photographing information in a finder of a photographing device such as a camera or a video, an LED or a liquid crystal arranged outside the photographing field frame has been used. However, with such a mechanism, there is a possibility of overlooking the display that warns of an inappropriate exposure state, and it is impossible to display a focus area, an appropriate exposure area, and the like within the field of view.

上記の如き欠点を鑑みて、液晶デイスプレイ等を視野と
重ねて表示を行なうなどの提案が本件出願人などから出
されている。例えば、特開昭52−110626ではTN(ツイス
ト・ネマチック)液晶デイスプレイを利用している。し
かし、この種のデイスプレイでは通常偏光板を使用する
為、光利用効率が最大で50%程度しか得られなかった。
又、特開昭58−62626はGH(ゲスト・ホスト)型液晶デ
イスプレイを利用したもので、偏光板は不要であるもの
の色素分子による光吸収が常時存在する為に光利用効率
が低下していた。
In view of the above-mentioned drawbacks, the applicant of the present application has proposed that the liquid crystal display or the like is overlapped with the field of view for display. For example, in JP-A-52-110626, a TN (twisted nematic) liquid crystal display is used. However, in this type of display, since a polarizing plate is usually used, the maximum light utilization efficiency was about 50%.
Further, JP-A-58-62626 uses a GH (guest-host) type liquid crystal display, and although a polarizing plate is unnecessary, light absorption efficiency by dye molecules is always present, resulting in a decrease in light utilization efficiency. .

従って、従来の方式ではフアインダーに於る撮影視野内
表示装置の有用性が高いにもかかわらず、フアインダー
内の明るさが十分に取れないという欠点を有していた。
Therefore, the conventional method has a drawback in that the brightness in the finder cannot be sufficiently obtained although the display device in the field of view in the finder is highly useful.

(3)発明の概要 本発明の目的は、上記従来の欠点を除去し、フアインダ
ー光路中のほぼ全光束を覆う位置に配置する事が可能
で、且つ常時フアインダー内の明るさを保持したまま
で、任意の場所に鮮明な表示が出来るフアインダー内表
示装置を提供する事にある。
(3) Outline of the Invention An object of the present invention is to eliminate the above-mentioned conventional drawbacks and to arrange the light beam at a position that covers almost all the light flux in the finder optical path, while maintaining the brightness inside the finder all the time. , It is to provide a display device in the finder that can display a clear image in any place.

上記目的を達成する為に、本発明に係るフアインダー内
表示装置はカメラのフアインダー内に撮影情報、パター
ン等の表示を行なうフアインダー内表示装置に於て、 前記ファインダー内の被写体光の光路にほぼ垂直な平面
に沿って第1と第2の光学的異方性物質を交互に配した
グレーティングと、前記第1と第2の光学的異方性物質
の光学軸方向が互いにほぼ一致することにより前記被写
体光が前記グレーティングを素通りする第1の状態と前
記第1と第2の光学的異方性物質の光学軸方向が前記平
面に平行で且つ互いに異なることにより前記被写体光が
前記グレーティングで回折する第2の状態とを生じさせ
るために前記光学的異方性物質の光学軸方向を制御する
手段とを有することを特徴とする。
In order to achieve the above object, a display device in a finder according to the present invention is a display device in a finder that displays shooting information, a pattern, etc. in a finder of a camera, and is substantially perpendicular to an optical path of a subject light in the viewfinder. A grating in which first and second optically anisotropic substances are alternately arranged along a flat plane, and the optical axis directions of the first and second optically anisotropic substances substantially coincide with each other. The subject light is diffracted by the grating because the subject light passes through the grating in a first state and the optical axis directions of the first and second optically anisotropic substances are parallel to the plane and different from each other. Means for controlling the optical axis direction of the optically anisotropic substance to generate the second state.

前記光学的異方性物質は電界,磁界,熱,圧力,光等に
よりその光学軸を変化させる事が出来る物質、もしくは
屈折率を変化せしめる事が出来る物質であって、例え
ば、液晶や電気光学結晶、即ち、PLZT,LiNbO3,LiTa
O3,TiO2,PMMA,CCl4,KDP,ADP,ZnO,BaTiO3,Bi12SiO20
Ba2NaNb5O15,MnBi,EuO,CS2,Gd2(MoO4)3,Bi4Ti3O12,Cu
Cl,GaAs,ZnTe,As2Se3,Se,AsGeSeS,DKDP,MNA,mNA,UREA,
フオトレジスト,ネマチツク液晶、コレステリツク液
晶,スメクチツク液晶,強誘電液晶等が挙げられる。特
に液晶は安価で、且つ制御法が容易である為に好適な材
料である。
The optically anisotropic substance is a substance whose optical axis can be changed by an electric field, a magnetic field, heat, pressure, light, or the like, or a substance whose refractive index can be changed. Crystal, ie PLZT, LiNbO 3 , LiTa
O 3 , TiO 2 , PMMA, CCl 4 , KDP, ADP, ZnO, BaTiO 3 , Bi 12 SiO 20 ,
Ba 2 NaNb 5 O 15 ,, MnBi, EuO, CS 2 , Gd 2 (MoO 4 ) 3 , Bi 4 Ti 3 O 12 ,, Cu
Cl, GaAs, ZnTe, As 2 Se 3 , Se, AsGeSeS, DKDP, MNA, mNA, UREA,
Photoresist, nematic liquid crystal, cholesteric liquid crystal, smectic liquid crystal, ferroelectric liquid crystal and the like can be mentioned. In particular, liquid crystals are suitable materials because they are inexpensive and easy to control.

又、本表示装置は被写体光の透過,遮断(回折)による
モノクロパターンの表示の他、カラーフイルター等を用
いたカラー表示、グレーテイングの分光透過率特性を利
用したカラー表示等を行なう事も出来る。
In addition to displaying a monochrome pattern by transmitting and blocking (diffracting) the subject light, this display device can also perform color display using a color filter or the like, color display using the spectral transmittance characteristic of grating, etc. .

更に上述のグレーテイングを作成する方法としては、レ
ジストを用いる方法フオトリソグラフイーとドライエツ
チングによる方法、熱硬化性樹脂あるいは紫外線硬化性
樹脂等を用いたレプリカ法、ルーリングエンジンを用い
た切削法あるいはエンボス法等の各種方法が挙げられ
る。
Further, as a method for creating the above-mentioned grating, a method using a resist, a method by photolithography and dry etching, a replica method using a thermosetting resin or an ultraviolet curable resin, a cutting method using a ruling engine or embossing is used. There are various methods such as the method.

以下、図面を用いて本表示装置に関して詳述する。Hereinafter, the display device will be described in detail with reference to the drawings.

(4)実施例 第1図は本発明に係るフアンダー内表示装置に用いる表
示素子の基本構成例を示し動作原理の説明図も兼ねる。
ここで、1及び2は光学的異方性物質、3は透明電極、
4は透明光学部材、5は入射光、6,6′は入射光5に於
る任意の互いに直交する偏光成分を示す。
(4) Example FIG. 1 shows an example of the basic constitution of a display element used in the display device in a fan according to the present invention and also serves as an explanatory view of the operating principle.
Here, 1 and 2 are optically anisotropic substances, 3 is a transparent electrode,
Reference numeral 4 denotes a transparent optical member, 5 denotes incident light, and 6 and 6 ′ denote arbitrary orthogonal polarization components in the incident light 5.

ここで示される素子は異方性物質1と異方性物質2の界
面で三角波状のグレーテイングを形成し、各々の光学軸
は図の矢印方向(グレーテイングの溝方向及び配列方
向)を向いており互いに直交している。該グレーテイン
グを成す層が、透明電極3を形成した2枚の透明光学部
材4により挟まれて素子を形成している。
The device shown here forms a triangular wave-shaped grating at the interface between the anisotropic substance 1 and the anisotropic substance 2, and the respective optical axes are oriented in the arrow directions (groove direction and arrangement direction of the grating) in the figure. And are orthogonal to each other. The layer forming the grating is sandwiched by the two transparent optical members 4 on which the transparent electrodes 3 are formed to form an element.

一般に、ランダムな偏光特性を有する光は、第1図に示
す如くその成分を直交する2つの偏光成分6,6′に分け
る事が出来る。図の表示素子を電界駆動する場合、対向
する透明電極3間に電界が印加されていない静的状態に
於て、入射光5の偏光成分6の偏光方向は異方性物質1
の光学軸方向と一致しており、偏光成分6は異方性物質
1の異常屈折率neを感じる。又、異方性物質2の光学軸
方向とは直交する為、偏光成分6は異方性物質2の常屈
折率no′を感じる。更に同様の原理に基づいて、入射光
5の偏光成分6′は異方性物質1及び2に対して各々常
屈折率no及び異常屈折率ne′を感じる。従って、偏光成
分6及び6′に対して各々屈折率ne,no′及びno,neから
成る位相型のグレーテイングが存在する事になる。次
に、対向する透明電極3間に電界を印加した状態では、
異方性物質1及び2の光学軸方向は電界量に従って変化
し、同時に入射光5の偏光成分6及び6′が各々感じる
屈折率も変化してグレーテイングの変調度が変わる事に
なる。この時、偏光成分6及び6′が各々感じる異方性
物質1及び2の屈折率が等しくなる様に制御する事によ
り、入射光5に対してグレーテイングが存在しない事に
なり、入射光5は異方性物質1及び2から成るグレーテ
イングを素通りする。
In general, light having random polarization characteristics can be divided into two polarization components 6, 6'that are orthogonal to each other as shown in FIG. When the display device shown in the figure is driven by an electric field, the polarization direction of the polarization component 6 of the incident light 5 is anisotropic when the electric field is not applied between the transparent electrodes 3 facing each other.
Coincides with the optical axis direction of, and the polarization component 6 feels the extraordinary refractive index n e of the anisotropic substance 1. Also, since the orthogonal to the optical axis direction of the anisotropic material 2, the polarization component 6 feel ordinary refractive index n o 'of the anisotropic material 2. Further, based on the same principle, the polarization component 6 of the incident light 5 'each ordinary refractive index n o and the extraordinary refractive index n e with respect to anisotropic materials 1 and 2' feel. Therefore, there exists a phase type grating having refractive indexes n e , n o ′ and n o , n e for the polarization components 6 and 6 ′, respectively. Next, in a state where an electric field is applied between the transparent electrodes 3 facing each other,
The optical axis directions of the anisotropic substances 1 and 2 change according to the amount of electric field, and at the same time, the refractive indexes felt by the polarization components 6 and 6'of the incident light 5 also change, and the modulation degree of the grating changes. At this time, by controlling so that the refractive indices of the anisotropic substances 1 and 2 sensed by the polarization components 6 and 6'are equal, there is no grating for the incident light 5, and the incident light 5 Passes through a grating consisting of anisotropic substances 1 and 2.

例えば、異方性物質1及び2に同じ正誘電性ネマチツク
液晶を用いる場合(no=no′,ne=ne′)、電界印加に
より該液晶は電界方向に配向される。液晶の配向方向と
光学軸は一致しており、この為に透明電極3に対してほ
ぼ垂直に配向された液晶に対し、入射光5の偏光成分6
及び6′は共に該液晶の常屈折率noを感じて該液晶から
成るグレーデイングを透過する。又、電界を印加しない
静的状態では、液晶は矢印の方向に配向されており、入
射光5の偏光成分6及び6′は共に屈折率neとnoから成
るグレーテイングを感じる。ここで入射光5の波長を
λ,液晶か成る異方性物質1及び2の屈折率差をΔn、
液晶等の厚さ(グレーデイングの高さ)をTとすれば、
該液晶で形成されたグレーデイングで回折される零次透
過回折光の回折効率ηは次の1式で表わす事が出来
る。
For example, when the same positive dielectric nematic liquid crystal is used for the anisotropic substances 1 and 2 (n o = n o ′, n e = n e ′), the liquid crystal is aligned in the direction of the electric field by applying an electric field. The alignment direction of the liquid crystal and the optical axis coincide with each other. Therefore, the polarization component 6 of the incident light 5 with respect to the liquid crystal aligned substantially perpendicular to the transparent electrode 3
Both 6 and 6'perceive the ordinary index of refraction n o of the liquid crystal and transmit the grading composed of the liquid crystal. Further, in the static state where no electric field is applied, the liquid crystal is oriented in the direction of the arrow, and the polarization components 6 and 6'of the incident light 5 both feel a grating consisting of the refractive indices n e and n o . Here, the wavelength of the incident light 5 is λ, the refractive index difference between the anisotropic substances 1 and 2 made of liquid crystal is Δn,
If the thickness of the liquid crystal (grading height) is T,
The diffraction efficiency η o of the zero-order transmitted diffracted light diffracted by the grading formed by the liquid crystal can be expressed by the following formula 1.

但し、Δnmax=|ne−no|,Δnmin=0であり、Δn・T
=mλ(m=1,2,3,……)を満足する場合ηo=0とな
る。つまり入射光5の偏光成分6,6′は共にグレーテイ
ングで回折され、零次方向への出射光は存在しない。
又、Δn=0即ち異方性物質1及び2の屈折率が偏光成
分6,6′に対して共に等しい場合、前述の様に入射光5
はグレーテイングを素通りして全て零次透過光となる。
尚、透明電極3間に印加する電界量に従いΔnは変化す
る為、電界量を制御する事により上式の回折効率η
可変となる。
However, Δn max = | n e −n o |, Δn min = 0, and Δn · T
= Mλ (m = 1,2,3, ...) Is satisfied, ηo = 0. That is, the polarization components 6 and 6'of the incident light 5 are both diffracted by the grating, and the emitted light in the zero-order direction does not exist.
Further, when Δn = 0, that is, when the refractive indices of the anisotropic substances 1 and 2 are equal to the polarization components 6 and 6 ′, the incident light 5 as described above is used.
Passes through the grating and becomes zero-order transmitted light.
Since Δn changes according to the amount of electric field applied between the transparent electrodes 3, the diffraction efficiency η o in the above equation is variable by controlling the amount of electric field.

以上の説明から解る様に、自然光の如きランダムな偏光
特性を有する光であっても、その互いに直交する偏光成
分に対して個々に透過制御を行なう事により、光利用効
率を低下させる事なく変調出来る。
As can be seen from the above description, even light having random polarization characteristics such as natural light can be modulated without decreasing the light utilization efficiency by individually controlling the transmission of the polarization components orthogonal to each other. I can.

第2図は上記表示素子に於る他のグレーテイング形状例
を示し、第2図(A)は矩形状、第2図(B)は正弦波
状グレーテイングを有する素子で、図中の符号は全て第
1図と同じ部材を指す。
FIG. 2 shows another example of the grating shape in the above display element. FIG. 2 (A) is a rectangular element, and FIG. 2 (B) is an element having a sinusoidal grating. All refer to the same members as in FIG.

第2図に示す様なグレーテイング形状を含む如何なる形
状であっても本発明は達成し得るが、グレーテイング形
状が異なる場合、(1)式で示した様な回折効率の式が
異なってくる。例えば、矩形状グレーテイングでは次の
(2)式で零次透過光の回折効率を表わす。
The present invention can be achieved with any shape including the grating shape as shown in FIG. 2. However, when the grating shape is different, the formula of the diffraction efficiency as shown in the formula (1) is different. . For example, in the rectangular grating, the diffraction efficiency of zero-order transmitted light is expressed by the following equation (2).

次に、グレーテイングの形状による分光特性の違いを例
を挙げて示す。
Next, the difference in the spectral characteristics depending on the shape of the grating will be shown as an example.

第3図は三角波状,矩形状のグレーテイングを用いた場
合の本素子に於る零次透過光の可視波長域400〜700nmで
の分光透過率特性を示している。ここで縦軸は透過率η
、横軸は波長λで、図中7,7′は各々光透過時の三角
形状,矩形状グレーテイングの特性を、8,8′は各々光
遮断時の三角波状,矩形状グレーテイングの特性を示し
ている。図の様に矩形状グレーテイングは波長選択性が
強く、三角波状グレーテイングは波長選択性が殆ど無
い。
FIG. 3 shows the spectral transmittance characteristics of the zero-order transmitted light in the visible wavelength range of 400 to 700 nm in this device when triangular wave-shaped and rectangular-shaped gratings are used. Here, the vertical axis is the transmittance η
o , the horizontal axis is the wavelength λ, 7 and 7'in the figure show the characteristics of the triangular and rectangular gratings when transmitting light, and 8 and 8'the triangular wave and rectangular gratings when the light is blocked. It shows the characteristics. As shown in the figure, the rectangular grating has strong wavelength selectivity and the triangular wave grating has almost no wavelength selectivity.

従って、グレーテイング形状は製作の容易性、撮影装置
の使用目的、表示装置周辺のシステム、仕様等を考慮し
て選択される。
Therefore, the grating shape is selected in consideration of the ease of manufacture, the purpose of use of the photographing device, the system around the display device, specifications and the like.

以下、第1図に示した表示素子を用いた表示装置の作成
法の一例を示す。
Hereinafter, an example of a method of manufacturing a display device using the display element shown in FIG. 1 will be shown.

第4図は第1図の表示素子の作成過程を示し、9は波状
透明スペーサ、10はグレーテイングの溝方向に配向した
液晶、10′はグレーテイングの配列方向に配向した液
晶、11はSiOであり、第1図と同じ部材には同番号を符
してある。ここでは異方性物質として正誘電性ネマチツ
ク液晶を用いている。
FIG. 4 shows a process of manufacturing the display device of FIG. 1, 9 is a wavy transparent spacer, 10 is a liquid crystal aligned in the groove direction of the grating, 10 'is a liquid crystal aligned in the array direction of the grating, and 11 is SiO. The same members as those in FIG. 1 are designated by the same reference numerals. Here, a positive dielectric nematic liquid crystal is used as the anisotropic substance.

コーニング7059ガラス基板4(コーニング社製、37×26
×1mm3)の両面を研磨して透明平面を形成し、基板4
の全面にITO膜を1000Åの厚さに成膜して透明電極3を
作成した。次に透明電極3にSiO11を斜方蒸着して配向
処理を行ない、液晶が第4図(A)の矢印の如く配向す
る様にした。又、上記ガラス基板と同種のガラス基板4
に第4図(C)に示す様なパターン透明電極3をITO膜
を様いて形成した後、該透明電極3にSiOを斜方蒸着し
て配向処理を行ない、液晶が第4図(C)の矢印の如く
配向する様にした。一方、第4図(B)に示す様な波状
透明スペーサ9を圧述加工により形成した。尚、この波
状透明スペーサ9に於る波の山と谷の高さTは2.3μm
である。続いで、波状透明スペーサ9を挟む形で上記2
枚のガラス基板4を透明電極3が相対するよう向かい合
せ、正誘電性ネマチツク液晶10,10′を間隙部に充填し
た後封着して第4図(D)に示す表示装置を作成した。
Corning 7059 Glass Substrate 4 (Corning, 37 × 26
X 1 mm 3 ) both sides are polished to form a transparent flat surface, and the substrate 4
An ITO film having a thickness of 1000 Å was formed on the entire surface of to prepare a transparent electrode 3. Next, SiO11 was obliquely vapor-deposited on the transparent electrode 3 for orientation treatment so that the liquid crystal was oriented as shown by the arrow in FIG. 4 (A). Further, a glass substrate 4 of the same kind as the above glass substrate
After forming the patterned transparent electrode 3 as shown in FIG. 4 (C) on the ITO film, SiO is obliquely vapor-deposited on the transparent electrode 3 for alignment treatment, and the liquid crystal is changed to FIG. 4 (C). The orientation is as indicated by the arrow. On the other hand, a wavy transparent spacer 9 as shown in FIG. 4 (B) was formed by pressure processing. The height T of the peaks and valleys of the waves in this wavy transparent spacer 9 is 2.3 μm.
Is. Subsequently, the above-mentioned 2
The glass substrates 4 were opposed to each other with the transparent electrodes 3 facing each other, and the positive dielectric nematic liquid crystals 10 and 10 'were filled in the gaps and then sealed to complete the display device shown in FIG. 4 (D).

第5図は本発明に係るフアインダー内表示装置の一例を
示す図で、12は上記表示装置、13はフレネルレンズ付ピ
ント板、14はコンデンサレンズ、15はペンタプリズム、
16は接眼レンズ、17は反射鏡を示す。
FIG. 5 is a view showing an example of the display device in the finder according to the present invention, in which 12 is the display device, 13 is a focusing plate with a Fresnel lens, 14 is a condenser lens, 15 is a pentaprism,
Reference numeral 16 is an eyepiece lens, and 17 is a reflecting mirror.

反射鏡17によりフアインダー内に導かれた被写体光は、
表示装置12、フレネルレンズ兼ピント板13、コンデンサ
ーレンズ14を介し、ペンタプリズム15により正立像とな
り接眼レンズ16を通して撮影者の目に入る。ここで、表
示装置12に於て、両電極間に矩形波交流電界を印加して
いる期間は、フアインダー内の視野全体が光透過状態と
なっており、接眼レンズ16を通して被写体像を鮮明に見
る事は出来る。一方、露出不足警告や合焦状態等の警告
を表示する場合、露出や合焦等の検出装置からの信号に
従ってパターン化され警告表示部分の電界を0とし、該
表示部分を光遮断状態として表示を行なう事が出来る。
The subject light guided into the finder by the reflecting mirror 17 is
The pentaprism 15 forms an erect image through the display device 12, the Fresnel lens / focus plate 13 and the condenser lens 14, and enters the eye of the photographer through the eyepiece lens 16. Here, in the display device 12, while the rectangular wave AC electric field is being applied between both electrodes, the entire visual field in the finder is in a light transmitting state, and the subject image can be clearly seen through the eyepiece lens 16. Things can be done. On the other hand, in the case of displaying an underexposure warning or a warning such as an in-focus state, the electric field of the warning display portion is patterned to 0 according to a signal from a detection device such as exposure or focus, and the display portion is displayed as a light-blocking state. Can be done.

その一例を第6図に示す。図中18は中央部に45°の傾斜
面の半透明鏡を有する透明光学部材で撮影レンズを通っ
た光の一部を露出検出用もしくは合焦検出用受光素子21
に送る作用を持つ。22は受光素子21の出力を受けて分析
する露出量検出回路もしくは合焦検出回路で、又23は検
出回路22からの検出信号を受けてこれを電圧発生回路
で、この回路の出力が本表示装置12に印加される。
An example thereof is shown in FIG. In the figure, reference numeral 18 denotes a transparent optical member having a semi-transparent mirror having an inclined surface of 45 ° in the central portion, and a part of light passing through the photographing lens is used as a light receiving element 21 for exposure detection or focus detection.
To send to. 22 is an exposure amount detection circuit or a focus detection circuit that receives and analyzes the output of the light receiving element 21, and 23 is a voltage generation circuit that receives the detection signal from the detection circuit 22 and the output of this circuit is the main display. Applied to the device 12.

表示の例を第7図に示す。図中(a)は露出量アンダー
警告、(b)は露出量オーバー警告、(c)は適正露出
表示、(d)は前ピン状態、(e)は後ピン状態、
(f)は合焦を表わしている。以上のように、撮影視野
枠内表示が、高いコントラストで像の明るさは損なわず
に出来、且つ表示を行なわない場合は被写体像の観察に
対する影響が全くない。
An example of the display is shown in FIG. In the figure, (a) is an underexposure warning, (b) is an overexposure warning, (c) is a proper exposure display, (d) is a front focus state, (e) is a rear focus state,
(F) represents focusing. As described above, the display in the photographing field frame can be performed with a high contrast without impairing the brightness of the image, and when the display is not performed, there is no influence on the observation of the subject image.

上記実施例では、表示装置12をコンデンサレンズ14とピ
ント板13の間に配しているが、フアインダー内に於るシ
ステム構成によっては接眼レンズ16は近傍等に配しても
良い事は明らかである。又、本表示装置はグレーテイン
グによる回折現像を利用している為、フレアー光となる
回折光を除去する手段、例えばフアイバプレート等を本
表示装置の光束出射側に設ける等の対策を施すのも有効
である。
In the above embodiment, the display device 12 is arranged between the condenser lens 14 and the focusing plate 13, but it is clear that the eyepiece 16 may be arranged in the vicinity depending on the system configuration in the finder. is there. Further, since this display device uses diffraction development by grating, it is also possible to take measures such as a means for removing diffracted light that becomes flare light, such as providing a fiber plate or the like on the light exit side of the display device. It is valid.

第8図は本表示装置に於る別の構成例の作成過程を示
し、第9図は第8図に示す表示装置の駆動法の説明図で
ある。ここで、24は強誘電性液晶、25及び25′は櫛状電
極を示し、前記実施例と同じ部材には同番号を付す。以
下、作成過程を詳述する。
FIG. 8 shows a manufacturing process of another constitutional example in the present display device, and FIG. 9 is an explanatory diagram of a driving method of the display device shown in FIG. Here, 24 is a ferroelectric liquid crystal, and 25 and 25 'are comb-like electrodes, and the same members as those in the above-mentioned embodiment are designated by the same reference numerals. The creation process will be described in detail below.

前記実施例同様、コーニング7059ガラス基板4(37×26
×1mm3)を2枚用意した。1枚は全面に第8図(A)
に示す如くITO透明電極3を厚さ1000Åで形成し、他の
1枚は第8図(B)に示す如くパターン部のみ櫛状にIT
O透明電極25,25′を厚さ1000Åで形成した。尚、この櫛
状電極25,25′は第8図(C)に示す様交互に設けられ
ている。更に上記2枚のガラス基板4にPVC(ポリビニ
ルカルバゾール)膜を形成した後、ラビング処理を施し
て櫛状電極25,25′に沿う方向へ液晶の配向軸を揃わせ
た。続いて、第8図(C)に示す如く、上記2枚のガラ
ス基板4をスペーサを介して両電極面3,25,25′が相対
する様に貼り合わせ、間隙部に強誘電性液晶MORA−8を
充填した後シールした。
As in the previous embodiment, Corning 7059 glass substrate 4 (37 × 26
Two pieces of × 1 mm 3 ) were prepared. One sheet is shown in Fig. 8 (A)
The ITO transparent electrode 3 is formed with a thickness of 1000 Å as shown in Fig. 4, and the other one is formed by comb-shaped IT only in the pattern part as shown in Fig. 8 (B).
O transparent electrodes 25, 25 'were formed with a thickness of 1000Å. The comb-shaped electrodes 25, 25 'are provided alternately as shown in FIG. 8 (C). Further, a PVC (polyvinylcarbazole) film was formed on the two glass substrates 4 and then subjected to rubbing treatment to align the liquid crystal alignment axes in the direction along the comb-shaped electrodes 25, 25 '. Then, as shown in FIG. 8 (C), the two glass substrates 4 are bonded to each other so that the electrode surfaces 3, 25, 25 'face each other via a spacer, and the ferroelectric liquid crystal MORA is provided in the gap. After filling with -8, it was sealed.

次に、上記方法で作成した表示装置の駆動方法も第9図
を用いて説明する。
Next, a method of driving the display device created by the above method will be described with reference to FIG.

最初に表示を行なわない場合、透明電極3及び櫛状電極
25,25′共に電圧を印加しない。従って強誘電性液晶を2
4の光学軸は第9図(A)の如く初期状態のまま一方向
に揃い、屈折率の異方性は面内で一様な状態となってグ
レーテイングは形成されず、入射光は素通りする。一
方、表示を行なう場合、表示パターンを形成する櫛状電
極25,25′に正負が逆で絶対値の等しい電圧、例えば±5
Vを透明電極3との間に印加する。この時、強誘電性液
晶24の光学軸は第9図(B)の如く交互に傾き、表示パ
ターン部のみ入射光に対してグレーテイングが形成され
る事になる。従って、前記(2)式を満足する様に液晶
層の厚さTと屈折率差Δn′と入射光の波長λとの関係
を調整しておけば、表示パターン部を通過する被写体光
は遮断される。従って、撮影視野枠内表示が、像全体の
明るさは保持したままで高いコントラストの表示が出来
る。
When the display is not performed first, the transparent electrode 3 and the comb-shaped electrode
No voltage is applied to both 25 and 25 '. Therefore, the ferroelectric liquid crystal
The optical axis of 4 is aligned in one direction in the initial state as shown in FIG. 9 (A), the anisotropy of the refractive index is uniform in the plane, no grating is formed, and the incident light passes through. To do. On the other hand, in the case of displaying, a voltage with opposite positive and negative absolute values, for example ± 5, is applied to the comb-shaped electrodes 25, 25 'forming the display pattern.
V is applied across the transparent electrode 3. At this time, the optical axis of the ferroelectric liquid crystal 24 is alternately tilted as shown in FIG. 9 (B), and only the display pattern portion is formed with a grating for the incident light. Therefore, if the relationship between the thickness T of the liquid crystal layer, the refractive index difference Δn ′, and the wavelength λ of the incident light is adjusted so as to satisfy the equation (2), the subject light passing through the display pattern portion is blocked. To be done. Therefore, the display within the field of view frame can be displayed with high contrast while maintaining the brightness of the entire image.

尚、上述の強誘電性液晶はメモリ機能を持たせないもの
であるが、メモリ性を有する液晶であれば初期配向状態
を一様とした後、25もしくは25′のいずれかのみの電極
に加える電界の符号を切換えるだけで上述の機能は果さ
れる。
The above-mentioned ferroelectric liquid crystal does not have a memory function, but if the liquid crystal has a memory property, it is added to the electrode of either 25 or 25 'after making the initial alignment state uniform. The function described above is achieved only by switching the sign of the electric field.

上記の2つの実施例に於る表示装置は、予め表示すべき
パターンを装置内に作成して設けているが、本フアイン
ダー内表示装置はマトリツクス駆動をする事も当然可能
であり、カメラの各種検出装置と組み合せてマトリツク
ス駆動を行えば、合焦領域表示や露出適性領域表示等も
可能であり、種々の表示形態を得る事が出来る。
The display devices in the above two embodiments are provided with patterns to be displayed in advance in the device, but it is naturally possible to drive the matrix display device in the finder, and various types of cameras can be used. If matrix driving is performed in combination with a detection device, focusing area display, exposure appropriate area display, and the like are possible, and various display forms can be obtained.

更に上記実施例では光学的な異方性物質として液晶を適
用した一例を示したが、異方性物質は液晶に限られるも
のではなく、電気光学結晶等の電気光学効果、熱光学効
果、磁気光学効果を有する種々の異方性物質を適用出来
る。
Further, in the above-mentioned embodiment, an example in which liquid crystal is applied as an optically anisotropic substance is shown, but the anisotropic substance is not limited to liquid crystal, and electro-optical effect such as electro-optical crystal, thermo-optical effect, magnetic effect, etc. Various anisotropic substances having an optical effect can be applied.

(5)発明の効果 以上説明した様に、本発明に係るフアインダー内表示装
置は偏光特性が無い為に偏光板が不要であり、通常の状
態に於て被写体光を高透過率で通過させ、撮影情報等を
表示する際は高コントラストで表示が可能な装置であ
る。従って、フアインダー内視野枠内外をとわず全面に
わたり警告パターンの表示や領域の表示等を、視野の構
成、明るさと保持したままで行なう事が出来る装置とな
る。
(5) Effects of the Invention As described above, the display device in the finder according to the present invention does not need a polarizing plate because it does not have a polarization characteristic, and allows the subject light to pass with a high transmittance in a normal state. This is a device capable of displaying with high contrast when displaying shooting information and the like. Therefore, the device is capable of displaying the warning pattern, the region, and the like on the entire surface regardless of the inside and the outside of the field frame within the finder while maintaining the field structure and brightness.

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

第1図は本発明に係るフアインダー内表示装置に用いる
表示素子の基本構成例を示す図。 第2図は表示素子の別のグレーテイング形状例を示す
図。 第3図は三角波状及び矩形状のグレーテイングに於る可
視波長域の分光透過率特性を示す図で、光透過時と光遮
断時に関して示している。 第4図は第1図に示す表示素子を用いた表示装置の作成
過程を示す図。 第5図は本発明に係るフアインダー内表示装置の一例を
示す図。 第6図は露出量もしくは合焦検出装置と、本表示装置と
を組合せた一例を示す図。 第7図は本表示装置による表示パターン例を示す図。 第8図は本表示装置に於る別の構成例の作成過程を示す
図。 第9図は第8図に示す表示装置の駆動法を示す説明図。 1,2……光学的異方性物質 3……透明電極 4……透明光学部材(基板) 5……入射光 6,6′……入射光に於る互いに直交する偏光成分 7……光透過時の三角波状グレーテイングの分光透過率
特性 7′……光透過時の矩形状グレーテイングの分光透過率
特性 8……光遮断時の三角波状グレーテイングの分光透過率
特性 8′……光遮断時の矩形状グレーテイングに分光透過率
特性 9……波状透明スペーサ 10,10′……液晶 11……SiO 12……表示装置 13……ピント板 14……コンデンサレンズ 15……ペンタプリズム 16……接眼レンズ 17……反射鏡 18……中央に45°の傾斜面の半透明鏡を有する透明光学
部材 19……レンズ 20……鏡 21……検出用受光素子 22……検出用回路 23……電圧発生回路 24……強誘電性液晶 25,25′……櫛状電極
FIG. 1 is a diagram showing a basic configuration example of a display element used in a display device in a finder according to the present invention. FIG. 2 is a diagram showing another example of the grating shape of the display element. FIG. 3 is a diagram showing the spectral transmittance characteristics in the visible wavelength region in the case of triangular wave-shaped and rectangular gratings, which are shown when light is transmitted and when light is blocked. FIG. 4 is a diagram showing a manufacturing process of a display device using the display element shown in FIG. 1. FIG. 5 is a diagram showing an example of a display device in a finder according to the present invention. FIG. 6 is a diagram showing an example in which an exposure amount or focus detection device and this display device are combined. FIG. 7 is a diagram showing an example of a display pattern by this display device. FIG. 8 is a diagram showing a production process of another configuration example of the display device. FIG. 9 is an explanatory diagram showing a driving method of the display device shown in FIG. 1,2 ...... Optically anisotropic substance 3 ...... Transparent electrode 4 ...... Transparent optical member (substrate) 5 ...... Incident light 6,6 '…… Polarizing components in incident light orthogonal to each other 7 ...... Light Spectral transmittance characteristic of triangular wave grating when transmitting 7 '... Spectral transmittance characteristic of rectangular grating when transmitting light 8 ...... Spectral transmittance characteristic of triangular wave grating when blocking light 8' ... Light Spectral transmittance characteristics in rectangular grating when cut off 9 Wavy transparent spacer 10,10 '…… Liquid crystal 11 …… SiO 12 …… Display device 13 …… Focus plate 14 …… Condenser lens 15 …… Penta prism 16 ...... Eyepiece 17 ...... Reflecting mirror 18 ...... Transparent optical member having a semi-transparent mirror with a 45 ° inclined surface in the center 19 …… Lens 20 …… Mirror 21 …… Detecting light receiving element 22 …… Detecting circuit 23 ...... Voltage generator 24 …… Ferroelectric liquid crystal 25,25 '…… Comb shaped electrode

フロントページの続き (51)Int.Cl.6 識別記号 庁内整理番号 FI 技術表示箇所 G02F 1/141 Continuation of front page (51) Int.Cl. 6 Identification code Office reference number FI technical display location G02F 1/141

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】カメラのファインダー内に撮影情報、パタ
ーン等の表示を行なうファインダー内表示装置におい
て、前記ファインダー内の被写体光の光路にほぼ垂直な
平面に沿って第1と第2の光学的異方性物質を交互に配
したグレーティングと、前記第1と第2の光学的異方性
物質の光学軸方向が互いにほぼ一致することにより前記
被写体光が前記グレーティングを素通りする第1の状態
と前記第1と第2の光学的異方性物質の光学軸方向が前
記平面に平行で且つ互いに異なることにより前記被写体
光が前記グレーティングで回折する第2の状態とを生じ
させるために前記光学的異方性物質の光学軸方向を制御
する手段とを有することを特徴とするファインダー内表
示装置。
1. A viewfinder display device for displaying shooting information, patterns, etc. in a viewfinder of a camera, wherein first and second optical differences are provided along a plane substantially perpendicular to an optical path of subject light in the viewfinder. The first state and the first state in which the subject light passes directly through the grating due to the optical axes of the first and second optically anisotropic substances being substantially aligned with each other The optical difference between the optical axes of the first and second optically anisotropic substances is parallel to the plane and different from each other so that a second state in which the subject light is diffracted by the grating is generated. And a means for controlling the optical axis direction of the isotropic substance.
【請求項2】前記第1と第2の光学的異方性物質は各々
ネマチック液晶より成り、前記制御手段は前記第1と第
2の光学的異方性物質に電界を印加する手段を備え、前
記グレーティングの所定部分における前記第1と第2の
光学的異方性物質の光学軸方向は、前記電界を印加しな
い状態で前記平面に平行で且つ互いに直交しており、前
記電界の印加により双方とも前記電界の方向と一致する
ことを特徴とする特許請求の範囲第(1)記載のファイ
ンダー内表示装置。
2. The first and second optically anisotropic substances each comprise a nematic liquid crystal, and the control means comprises means for applying an electric field to the first and second optically anisotropic substances. The optical axis directions of the first and second optically anisotropic substances in a predetermined portion of the grating are parallel to the plane and orthogonal to each other when the electric field is not applied, and The display device in the finder according to claim (1), characterized in that both of them coincide with the direction of the electric field.
【請求項3】前記第1と第2の光学的異方性物質は各々
強誘電性液晶より成り、前記制御手段は前記第1と第2
の光学的異方性物質に電界を印加する手段を備え、前記
グレーティングの所定部分における前記第1と第2の光
学的異方性物質の光学軸方向は、前記電界を印加しない
状態で前記平面に平行で且つ互いに一致しており、前記
電界の印加により前記平面に平行で且つ互いに直交する
方向に向くことを特徴とする特許請求の範囲第(1)記
載のファインダー内表示装置。
3. The first and second optically anisotropic substances are each made of a ferroelectric liquid crystal, and the control means comprises the first and second
Means for applying an electric field to the optically anisotropic substance, and the optical axis directions of the first and second optically anisotropic substances in a predetermined portion of the grating are the planes when the electric field is not applied. The display device in a finder according to claim (1), characterized in that they are parallel to each other and coincide with each other, and are oriented in a direction parallel to the plane and orthogonal to each other by applying the electric field.
JP60173791A 1985-08-07 1985-08-07 Display device in the finder Expired - Fee Related JPH0727161B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP60173791A JPH0727161B2 (en) 1985-08-07 1985-08-07 Display device in the finder
DE19863627113 DE3627113A1 (en) 1985-08-07 1986-08-06 DISPLAY DEVICE IN A VIEWFINDER
GB8619323A GB2180946B (en) 1985-08-07 1986-08-07 Display device in viewfinder
US08/092,569 US5299037A (en) 1985-08-07 1993-07-16 Diffraction grating type liquid crystal display device in viewfinder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60173791A JPH0727161B2 (en) 1985-08-07 1985-08-07 Display device in the finder

Publications (2)

Publication Number Publication Date
JPS6234142A JPS6234142A (en) 1987-02-14
JPH0727161B2 true JPH0727161B2 (en) 1995-03-29

Family

ID=15967218

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60173791A Expired - Fee Related JPH0727161B2 (en) 1985-08-07 1985-08-07 Display device in the finder

Country Status (1)

Country Link
JP (1) JPH0727161B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6433520A (en) * 1987-07-29 1989-02-03 Canon Kk Liquid crystal optical modulator
JP2570314B2 (en) * 1987-09-01 1997-01-08 キヤノン株式会社 Viewfinder optical system
JPH0281037A (en) * 1988-09-17 1990-03-22 Olympus Optical Co Ltd Optical system of finder

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3843231A (en) 1971-04-22 1974-10-22 Commissariat Energie Atomique Liquid crystal diffraction grating
US4294529A (en) 1978-09-07 1981-10-13 Canon Kabushiki Kaisha Camera

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3843231A (en) 1971-04-22 1974-10-22 Commissariat Energie Atomique Liquid crystal diffraction grating
US4294529A (en) 1978-09-07 1981-10-13 Canon Kabushiki Kaisha Camera

Also Published As

Publication number Publication date
JPS6234142A (en) 1987-02-14

Similar Documents

Publication Publication Date Title
US5299037A (en) Diffraction grating type liquid crystal display device in viewfinder
US5013141A (en) Liquid crystal light modulation device
US4878742A (en) Liquid crystal optical modulator
US4856869A (en) Display element and observation apparatus having the same
US6295145B1 (en) Switchable holographic device
JP4586630B2 (en) Diffraction type display device and display device in viewfinder of camera
KR100425641B1 (en) Polarizing element and image projection device
US20070041684A1 (en) Switchable viewfinder display
GB2071864A (en) Liquid crystal display/record cell
JP4242862B2 (en) Optical property variable optical element and display device including optical property variable optical element
US4822146A (en) Optical modulation element
JPH09243806A (en) Optical characteristic variable optical element
JPH0727161B2 (en) Display device in the finder
JP4194381B2 (en) Optical deflection device
JPH0664269B2 (en) Display device in the finder
JP3717016B2 (en) Reflective liquid crystal display device using hologram
JPH1090730A (en) Optical element, its drive method and display device
JP3156303B2 (en) Manufacturing method of liquid crystal phase diffraction grating
JPH083584B2 (en) Liquid crystal optical shutter
JP2517589B2 (en) Light modulation element
GB2180946A (en) Display device in viewfinder
JP2588541B2 (en) Projection color display device
JPH0652351B2 (en) Light modulator
GB2219099A (en) Tunable Fabry-Perot filter
JP3235163B2 (en) Liquid crystal display device and liquid crystal projector with liquid crystal display device

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees