JPH03107931A - Oscillation isolator for image pickup optical system - Google Patents
Oscillation isolator for image pickup optical systemInfo
- Publication number
- JPH03107931A JPH03107931A JP1247689A JP24768989A JPH03107931A JP H03107931 A JPH03107931 A JP H03107931A JP 1247689 A JP1247689 A JP 1247689A JP 24768989 A JP24768989 A JP 24768989A JP H03107931 A JPH03107931 A JP H03107931A
- Authority
- JP
- Japan
- Prior art keywords
- refractive index
- liquid crystal
- optical system
- wedge
- image pickup
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 230000003287 optical effect Effects 0.000 title claims abstract description 69
- 230000010355 oscillation Effects 0.000 title abstract 2
- 238000003384 imaging method Methods 0.000 claims description 13
- 239000004973 liquid crystal related substance Substances 0.000 abstract description 31
- 238000006073 displacement reaction Methods 0.000 abstract description 12
- 239000011521 glass Substances 0.000 abstract description 10
- 238000001514 detection method Methods 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 230000000087 stabilizing effect Effects 0.000 description 3
- 230000006866 deterioration Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000006641 stabilisation Effects 0.000 description 2
- 238000011105 stabilization Methods 0.000 description 2
- 230000002542 deteriorative effect Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000005357 flat glass Substances 0.000 description 1
- 239000013307 optical fiber Substances 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 238000007789 sealing Methods 0.000 description 1
- 239000012780 transparent material Substances 0.000 description 1
Landscapes
- Optical Elements Other Than Lenses (AREA)
- Adjustment Of Camera Lenses (AREA)
Abstract
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、カメラ等の撮像光学系の防振装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to an image stabilizing device for an imaging optical system such as a camera.
カメラ等の撮像光学系、特に望遠レンズでは、手ブレ等
の振動による画質の劣化が大きな問題となっている。現
在、様々な防振装置が考えられているが、例えば特開昭
62−153816号公報に記載の如く、2枚の透明板
の間に容易に変形可能な透明材を封入し、手ブレなどの
振動に応じて2枚の透明板を傾動させることによって光
路を曲げて像位置の変動を防止する可変頂角プリズム等
を用いたものがある。BACKGROUND ART In imaging optical systems such as cameras, especially telephoto lenses, deterioration of image quality due to vibrations such as camera shake is a major problem. Currently, various vibration isolating devices are being considered. For example, as described in JP-A-62-153816, an easily deformable transparent material is enclosed between two transparent plates to prevent vibrations such as camera shake. Some use a variable apex prism, etc., which bends the optical path by tilting two transparent plates depending on the situation, thereby preventing fluctuations in the image position.
しかし、上記従来例は、機械的な駆動装置を必要とする
ため、機構が複雑になるという欠点があった。However, the above-mentioned conventional example requires a mechanical drive device, which has the disadvantage that the mechanism is complicated.
本発明は、上記問題点に鑑み、機構が簡単でありながら
、手ブレ等による像位置の変動を補正し得る撮像光学系
の防振装置を提供することを目的としている。SUMMARY OF THE INVENTION In view of the above-mentioned problems, it is an object of the present invention to provide an image stabilizing device for an imaging optical system, which has a simple mechanism and is capable of correcting fluctuations in image position due to camera shake and the like.
〔課題を解決するための手段及び作用〕本発明による撮
像光学系の防振装置は、撮像光学系中に少なくとも一つ
の光軸に対して傾いた面を有する屈折率可変光学素子を
配置し゛、前記撮像光学系の振動に応じて電気的に前記
屈折率可変光学素子の屈折率を変化させることにより該
振動によって生ずる像位置の変動を補正するようにして
成ることにより、機械的な駆動装置を用いずに補正を行
い得るようにしたものである。[Means and effects for solving the problems] A vibration isolating device for an imaging optical system according to the present invention includes a variable refractive index optical element having at least one surface tilted with respect to the optical axis arranged in the imaging optical system, By electrically changing the refractive index of the variable refractive index optical element in accordance with the vibrations of the imaging optical system to correct fluctuations in the image position caused by the vibrations, the mechanical drive device can be corrected. This makes it possible to perform correction without using it.
即ち、本発明による防振装置は、撮像光学系中に1枚又
は複数枚の楔形プリズム又は斜めに傾けた平行平板から
成る屈折率可変光学素子を配置することによって光路を
曲げ、手ブレ等による像位置の変動を補正するようにな
っている。楔形プリズムは、第1図(A)に示した如く
、入射光線に対して射出光線に偏角θを与えるが、この
偏角θは頂角α、プリズムの屈折率nによって変化する
。That is, the image stabilization device according to the present invention bends the optical path by arranging a variable refractive index optical element consisting of one or more wedge-shaped prisms or obliquely tilted parallel flat plates in the imaging optical system, thereby preventing vibration caused by camera shake or the like. It is designed to compensate for fluctuations in image position. As shown in FIG. 1(A), the wedge-shaped prism gives an angle of deviation θ to the emitted ray with respect to the incident ray, and this angle of deviation θ changes depending on the apex angle α and the refractive index n of the prism.
又、第1図(B)に示した如く、斜めに傾けた平行平板
に対して水平に入射した光線はδだけ変位して水平に射
出するが、この変位量δは平行平板の厚さtと、屈折率
nによって変化する。本発明による防振装置では、楔形
プリズム又は平行平板の屈折率nを光学系の変位に応じ
て変化させることによって光路の偏角θ又は変位δをコ
ントロールし、手ブレによる像位置の変動を防止するよ
うになっている。Furthermore, as shown in Figure 1(B), a ray of light that is horizontally incident on an obliquely inclined parallel plate is displaced by δ and exits horizontally, but this displacement δ is equal to the thickness t of the parallel plate. and changes depending on the refractive index n. In the image stabilization device according to the present invention, the deflection angle θ or displacement δ of the optical path is controlled by changing the refractive index n of the wedge prism or parallel plate according to the displacement of the optical system, thereby preventing fluctuations in the image position due to camera shake. It is supposed to be done.
〔実施例〕
以下、図示した実施例に基づき本発明の詳細な説明する
。[Example] Hereinafter, the present invention will be described in detail based on the illustrated example.
第2図は第1実施例の要部を示しており、これは図示し
ない撮像光学系中に、頂角の等しい楔形液晶プリズムl
と屈折率一定のガラスから成る楔形プリズム2とを互い
に上下逆に組み合わせて成る屈折率可変光学素子3が配
置されている。尚、楔形液晶プリズム1は楔形のセル内
に液晶を封入して成るものであって、電源Eによる印加
電圧のON−〇FF又は印加電圧の大きさを変えること
によって屈折率を変化させることが可能である。FIG. 2 shows the main part of the first embodiment, which includes a wedge-shaped liquid crystal prism l with an equal apex angle in an imaging optical system (not shown).
A variable refractive index optical element 3 is disposed in which a wedge-shaped prism 2 made of glass with a constant refractive index is combined upside down. The wedge-shaped liquid crystal prism 1 is formed by sealing a liquid crystal inside a wedge-shaped cell, and the refractive index can be changed by turning on/off the applied voltage by the power source E or by changing the magnitude of the applied voltage. It is possible.
本実施例は上述の如く構成されているから、光学系の変
位のない状態では液晶の屈折率をガラスの屈折率と等し
くしておけば、屈折率可変光学素子3は平行平板ガラス
となり、光路を曲げることはないが、光学系の変位に応
じて液晶の屈折率を変化させれば、第2図に示した如く
光路を曲げることができ、その偏角をコントロールする
ことができる。従って、振動により生じた光学系の変位
により像位置の変動が生じても直ちに該変動を補正する
ことができる。Since this embodiment is configured as described above, if the refractive index of the liquid crystal is made equal to the refractive index of glass in a state where the optical system is not displaced, the variable refractive index optical element 3 becomes a parallel flat glass, and the optical path However, by changing the refractive index of the liquid crystal according to the displacement of the optical system, the optical path can be bent as shown in FIG. 2, and the angle of deviation can be controlled. Therefore, even if the image position fluctuates due to the displacement of the optical system caused by vibration, the fluctuation can be immediately corrected.
かくして、手ブレ等の振動による画質の劣化が防止でき
るが、本実施例は機械的駆動装置を用いずに補正を行い
得るので、機構が極めて簡単になる。In this way, deterioration in image quality due to vibrations such as camera shake can be prevented, but since this embodiment can perform correction without using a mechanical drive device, the mechanism is extremely simple.
第3図は第2実施例の要部を示しており、これは複数枚
の楔形液晶プリズム11〜16とガラスから成る楔形プ
リズム2とを組み合わせて成る屈折率可変光学素子3を
有している。従って、各楔形液晶プリズム11〜1.の
屈折率を夫々独立に変化させれば、更に細かく光路の偏
角をコントロールすることができる。FIG. 3 shows the main part of the second embodiment, which has a variable refractive index optical element 3 formed by combining a plurality of wedge-shaped liquid crystal prisms 11 to 16 and a wedge-shaped prism 2 made of glass. . Therefore, each wedge-shaped liquid crystal prism 11-1. By changing the refractive index of each independently, the polarization angle of the optical path can be controlled more precisely.
第4図は第3実施例の要部を示しており、これは液晶平
行平板4を頂角が等しく且つ上下が逆の二枚のガラスか
ら成る楔形プリズム2..2.の間に斜めに挾み込んで
成る屈折率可変光学素子3を有している。従って、光学
系の変位のない状態では液晶の屈折率をガラスの屈折率
と等しくしておけば光路の変位は0であるが、光学系の
変位に応じて液晶の屈折率を変化させれば、光路を変位
させることができ、その変位量をコントロールすること
ができる。FIG. 4 shows the main part of the third embodiment, in which a liquid crystal parallel plate 4 is replaced by a wedge-shaped prism 2 made of two glass sheets with equal apex angles and opposite sides. .. 2. A variable refractive index optical element 3 is provided obliquely between the two. Therefore, in a state where there is no displacement of the optical system, if the refractive index of the liquid crystal is made equal to the refractive index of the glass, the displacement of the optical path is 0, but if the refractive index of the liquid crystal is changed according to the displacement of the optical system, then the displacement of the optical path is 0. , the optical path can be displaced, and the amount of displacement can be controlled.
第5図は第4実施例の要部を示しており、これは第3実
施例の二枚の楔形プリズム2..2.の間に複数枚の液
晶平行平板41〜4.を挟み込んで成る屈折率可変光学
素子3を有している。従って、各液晶平行平板41〜4
.の屈折率を夫々独立に変化させれば、更に細かく光路
の変位量をコントロールすることができる。FIG. 5 shows the main part of the fourth embodiment, which consists of two wedge-shaped prisms 2 and 3 of the third embodiment. .. 2. Between them, a plurality of liquid crystal parallel flat plates 41 to 4. It has a variable refractive index optical element 3 formed by sandwiching a variable refractive index optical element 3. Therefore, each liquid crystal parallel plate 41 to 4
.. By changing the refractive index of each independently, the amount of displacement of the optical path can be controlled more precisely.
そして、上記各実施例において屈折率可変光学素子3を
光軸を中心に回転させることにより、光軸に対称にあら
ゆる方向に光路を曲げる或は変位させることが可能であ
るが、同じ楔形液晶プリズム又は液晶平行平板を異なる
方向に幾つか重ねて用いれば、機械的に動かすことな(
、全方向に光路を曲げる或は変位させることが可能であ
る。In each of the above embodiments, by rotating the variable refractive index optical element 3 around the optical axis, it is possible to bend or displace the optical path in any direction symmetrically with respect to the optical axis, but the same wedge-shaped liquid crystal prism Alternatively, if you stack several liquid crystal parallel plates in different directions, you can use them without having to move them mechanically (
, it is possible to bend or displace the optical path in all directions.
第6図はその一例である第5実施例の要部を示しており
、第6図(A)及び(B)は夫々その側面図及び平面図
である。これは4枚の同一の楔形液晶プリズム1.〜1
.をガラスから成る平行平板41〜4cを夫々介して互
いに逆(1′、とIb、lcと1.)及び直角(1,、
lbとICjl、)に重ねて成゛る屈折率可変光学素子
3を有している。FIG. 6 shows a main part of a fifth embodiment, which is an example thereof, and FIGS. 6(A) and 6(B) are a side view and a plan view thereof, respectively. This consists of four identical wedge-shaped liquid crystal prisms 1. ~1
.. are arranged opposite to each other (1', Ib, lc and 1.) and at right angles (1,,
It has a variable refractive index optical element 3 which is superimposed on the optical fibers lb and ICjl.
本実施例は上述の如く構成されているから、楔形液晶プ
リズム1..1eの屈折率をガラスよりも大きくし且つ
楔形液晶プリズムlb、laの屈折率をガラスと等しく
すると、光路は実線図示の如く曲げられ、楔形液晶プリ
ズム1..1cの屈折率をガラスと等しくし且つ楔形液
晶プリズムlb、laの屈折率をガラスよりも大きくす
ると、光路は点線図示の如(曲げられる。かくして、機
械的に動かすことなく光路を全方向に曲げることが可能
である。Since this embodiment is constructed as described above, the wedge-shaped liquid crystal prism 1. .. When the refractive index of the wedge-shaped liquid crystal prisms 1e is made larger than that of glass and the refractive index of the wedge-shaped liquid crystal prisms lb and la is made equal to that of glass, the optical path is bent as shown by the solid line, and the wedge-shaped liquid crystal prisms 1. .. If we make the refractive index of 1c equal to that of glass and the refractive index of wedge-shaped liquid crystal prisms lb and la larger than that of glass, the optical path will be bent as shown by the dotted line.Thus, the optical path will be bent in all directions without mechanical movement. Is possible.
尚、図示されていないが、同一の複数の楔形液晶プリズ
ムの代わりに同一の複数の液晶平行平板を用いて第5実
施例と同様な組合せにすれば、機械的に動かすことなく
光路を全方向に変位させることが可能である。Although not shown in the drawings, if a plurality of parallel liquid crystal plates are used instead of the same plurality of wedge-shaped liquid crystal prisms to create a combination similar to that of the fifth embodiment, the optical path can be spread in all directions without mechanical movement. It is possible to displace the
第7図は第5実施例の全体の構成を示しており、5は撮
影レンズ、9は像面であって、それらの間に第6図に示
した屈折率可変光学素子3が配置されている。そして、
屈折率可変光学素子3の各楔形液晶プリズム11〜l、
は夫々電圧印加用の電源6.〜64に接続され、これら
の電源61〜64は振動検知センサ7からの振動検知信
号に応じて制御回路8により制御されるようになってい
る。従って、センサ7で検知した振動に応じて制御回路
8及び電源61〜64により像の変動を補正する方向に
光路を曲げるように4つの楔形液晶プリズム1.〜14
に電圧がかけられ、振動による画質の劣化が防止される
。FIG. 7 shows the overall configuration of the fifth embodiment, in which 5 is a photographing lens, 9 is an image plane, and the variable refractive index optical element 3 shown in FIG. 6 is arranged between them. There is. and,
Each of the wedge-shaped liquid crystal prisms 11 to 1 of the variable refractive index optical element 3,
are the power supplies for voltage application 6. - 64, and these power supplies 61-64 are controlled by a control circuit 8 in response to a vibration detection signal from a vibration detection sensor 7. Therefore, the four wedge-shaped liquid crystal prisms 1. ~14
voltage is applied to prevent image quality from deteriorating due to vibration.
尚、第1乃至第4実施例も第7図のように構成すること
が可能であり、手ブレ等の振動によって像面9上で像が
δだけずれた場合、第1及び第2実施例では、屈折率可
変光学素子3の最終面から像面9までの距離をXとする
と、射出角のずれを補正する方向にXε=δとなる角度
εだけ光路を曲げるように液晶の屈折率を変えてやれば
良く、第3及び第4実施例では、ずれを補正する方向に
光路をδだけ変位させるように液晶の屈折率を変えてや
れば良い。Note that the first to fourth embodiments can also be configured as shown in FIG. 7, and if the image is shifted by δ on the image plane 9 due to vibrations such as camera shake, Now, assuming that the distance from the final surface of the variable refractive index optical element 3 to the image plane 9 is X, the refractive index of the liquid crystal is adjusted so that the optical path is bent by an angle ε such that Xε=δ in the direction that corrects the deviation of the exit angle. In the third and fourth embodiments, it is sufficient to change the refractive index of the liquid crystal so as to displace the optical path by δ in the direction of correcting the deviation.
上述の如く、本発明による撮像光学系の防振装置は、機
構が簡単でありながら手ブレ等による像位置の変動を補
正し得るという実用上重要な利点を有している。As described above, the image stabilizing device for an imaging optical system according to the present invention has a simple mechanism and has the important practical advantage of being able to correct fluctuations in image position due to camera shake and the like.
第1図は本発明による撮像光学系の防振装置の屈折率可
変光学素子の基本原理を示す概念図、第2図乃至第5図
は夫々第1乃至第4実施例の要部を示す図、第6図(A
)及び(B)は夫々第5実施例の要部の側面図及び平面
図、第7図は第5実施例の全体の構成を示す図である。
1.1.〜1..t、〜1.・・・・楔形液晶プリズム
、2,2..22・・・・楔形プリズム、3・・・・屈
折率可変光学素子、4,41〜4.・・・・液晶平行平
板、4a〜4o・・・・平行平板、5・・・・撮影レン
ズ、61〜6.・・・・電源、7・・・・振動検知セン
サ、8・・・・制御回路、9・・・・像面。
第1図
第2図
第6図
Q
b
C
第4図
1
第5図
第7図FIG. 1 is a conceptual diagram showing the basic principle of a variable refractive index optical element of a vibration isolator for an imaging optical system according to the present invention, and FIGS. 2 to 5 are diagrams showing main parts of the first to fourth embodiments, respectively. , Figure 6 (A
) and (B) are a side view and a plan view of essential parts of the fifth embodiment, respectively, and FIG. 7 is a diagram showing the overall configuration of the fifth embodiment. 1.1. ~1. .. t, ~1. ...Wedge-shaped liquid crystal prism, 2,2. .. 22... Wedge-shaped prism, 3... Variable refractive index optical element, 4, 41-4. ...Liquid crystal parallel plate, 4a-4o...Parallel plate, 5...Photographing lens, 61-6. ...Power source, 7...Vibration detection sensor, 8...Control circuit, 9...Image plane. Figure 1 Figure 2 Figure 6 Q b C Figure 4 Figure 1 Figure 5 Figure 7
Claims (1)
面を有する屈折率可変光学素子を配置し、前記撮像光学
系の振動に応じて電気的に前記屈折率可変光学素子の屈
折率を変化させることにより該振動によって生ずる像位
置の変動を補正するようにして成る撮像光学系の防振装
置。A variable refractive index optical element having at least one surface tilted with respect to an optical axis is disposed in an imaging optical system, and the refractive index of the variable refractive index optical element is electrically changed according to vibrations of the imaging optical system. A vibration isolating device for an imaging optical system, which corrects fluctuations in image position caused by the vibration.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1247689A JPH03107931A (en) | 1989-09-22 | 1989-09-22 | Oscillation isolator for image pickup optical system |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1247689A JPH03107931A (en) | 1989-09-22 | 1989-09-22 | Oscillation isolator for image pickup optical system |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03107931A true JPH03107931A (en) | 1991-05-08 |
Family
ID=17167181
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1247689A Pending JPH03107931A (en) | 1989-09-22 | 1989-09-22 | Oscillation isolator for image pickup optical system |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03107931A (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0589651A1 (en) * | 1992-09-25 | 1994-03-30 | Xerox Corporation | Device and apparatus for scan line skew correction in an electrostatographic machine |
| EP0589654A1 (en) * | 1992-09-25 | 1994-03-30 | Xerox Corporation | Device and apparatus for scan line process direction control in a multicolor electrostatographic machine |
| EP0589700A1 (en) * | 1992-09-25 | 1994-03-30 | Xerox Corporation | Device and apparatus for high speed tracking in a raster output scanner |
| JP2006018325A (en) * | 2005-09-12 | 2006-01-19 | Olympus Corp | Variable optical characteristic optical element, and display device equipped with variable optical characteristic optical element |
| EP1918926A3 (en) * | 2006-11-06 | 2008-06-11 | Funai Electric Co., Ltd. | Optical pickup apparatus |
-
1989
- 1989-09-22 JP JP1247689A patent/JPH03107931A/en active Pending
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0589651A1 (en) * | 1992-09-25 | 1994-03-30 | Xerox Corporation | Device and apparatus for scan line skew correction in an electrostatographic machine |
| EP0589654A1 (en) * | 1992-09-25 | 1994-03-30 | Xerox Corporation | Device and apparatus for scan line process direction control in a multicolor electrostatographic machine |
| EP0589700A1 (en) * | 1992-09-25 | 1994-03-30 | Xerox Corporation | Device and apparatus for high speed tracking in a raster output scanner |
| JP2006018325A (en) * | 2005-09-12 | 2006-01-19 | Olympus Corp | Variable optical characteristic optical element, and display device equipped with variable optical characteristic optical element |
| EP1918926A3 (en) * | 2006-11-06 | 2008-06-11 | Funai Electric Co., Ltd. | Optical pickup apparatus |
| US7764587B2 (en) | 2006-11-06 | 2010-07-27 | Funai Electric Co., Ltd. | Optical pickup apparatus |
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