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JPS6149610B2 - - Google Patents
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JPS6149610B2 - - Google Patents

Info

Publication number
JPS6149610B2
JPS6149610B2 JP56055929A JP5592981A JPS6149610B2 JP S6149610 B2 JPS6149610 B2 JP S6149610B2 JP 56055929 A JP56055929 A JP 56055929A JP 5592981 A JP5592981 A JP 5592981A JP S6149610 B2 JPS6149610 B2 JP S6149610B2
Authority
JP
Japan
Prior art keywords
reflecting mirror
infrared
optical system
convex lens
charge transfer
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
Application number
JP56055929A
Other languages
Japanese (ja)
Other versions
JPS57171225A (en
Inventor
Junichiro Yamashita
Riichi Saeki
Toshio Takei
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56055929A priority Critical patent/JPS57171225A/en
Publication of JPS57171225A publication Critical patent/JPS57171225A/en
Publication of JPS6149610B2 publication Critical patent/JPS6149610B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/58Means for changing the camera field of view without moving the camera body, e.g. nutating or panning of optics or image sensors
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/20Cameras or camera modules comprising electronic image sensors; Control thereof for generating image signals from infrared radiation only

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Radiation Pyrometers (AREA)

Description

【発明の詳細な説明】 この発明は、電荷転送素子と複数の赤外線検出
器の組合わせより構成した赤外線用固体撮像装置
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an infrared solid-state imaging device constructed from a combination of a charge transfer element and a plurality of infrared detectors.

多数の赤外線検出器を配列し、この配列と各検
出器において入射赤外光量に応じて発生蓄積した
電荷を転送出力する電荷転送素子を組合わせた
IRCCDは、素子内部に走査機能を持つているこ
と、多くの検出器出力を蓄積した後に出力するた
め信号対雑音比が改善できること等の点から赤外
線撮像装置の受光素子として用いれば装置の小型
軽量化、高性能化を図ることができる。
A large number of infrared detectors are arranged, and this arrangement is combined with a charge transfer element that transfers and outputs the charges generated and accumulated in each detector according to the amount of incident infrared light.
IRCCDs have a scanning function inside the device, and the signal-to-noise ratio can be improved by accumulating a large amount of detector output before outputting it, so if it is used as a light-receiving device in an infrared imaging device, the device will be small and lightweight. It is possible to improve the performance and performance.

第1図は、カタデイオプトリツク受光光学系を
持つ従来のIRCCD赤外線撮像装置の構成を表わ
す図である。入射赤外光1は対物レンズ2を透過
した後、一次反射平面鏡3、二次反射平面鏡4に
よつて順次反射され、IRCCD5上に結像され
る。またIRCCD出力6は、増幅器7によつて増
幅された後に表示器8に供給され、ドライバ9は
IRCCD5を駆動するのに必要な信号を供給す
る。第1図に示したようなカタデイオプトリツク
光学系は、光路が折返されるため、光学系の焦点
距離に比べて光学系の長さを短かくすることがで
き、IRCCDを用いた小型の赤外線撮像装置の光
学系としては有用である。
FIG. 1 is a diagram showing the configuration of a conventional IRCCD infrared imaging device having a catadioptric light receiving optical system. After the incident infrared light 1 passes through the objective lens 2, it is sequentially reflected by the primary reflecting plane mirror 3 and the secondary reflecting plane mirror 4, and is imaged on the IRCCD 5. Further, the IRCCD output 6 is supplied to the display 8 after being amplified by the amplifier 7, and the driver 9 is
Provides the signals necessary to drive IRCCD5. In the catadioptric optical system shown in Figure 1, the optical path is folded back, so the length of the optical system can be shortened compared to the focal length of the optical system. It is useful as an optical system for an infrared imaging device.

ところで面状に検出器を配置したIRCCDにお
いては、各検出器の出力をそれぞれ電荷転送素子
に接続しなければならないために、複数の検出器
列の間に検出器列と交互に線状の電荷転送素子が
配置されることが多い。ところが、電荷転送素子
は入射赤外光を出力電気信号に変換することがで
きないため、結像面上に入射赤外光に対する不感
帯が生ずる。結像面において検出器の面積が占め
る割合は充足率(filling factor)とも呼ばれ、現
在製造されているIRCCDにおいてこの値は大き
いものでも20%程度である。従つてIRCCDの各
検出器が見る瞬時視野の間には大きな隙間が生
じ、撮像対象の形状に関する情報が損なわれるば
かりか小さな目標の場合には見失われる場合も生
ずる。
By the way, in an IRCCD in which detectors are arranged in a planar manner, the output of each detector must be connected to a charge transfer element, so linear charges are transferred between multiple detector rows alternately with the detector rows. Transfer elements are often arranged. However, since the charge transfer element cannot convert incident infrared light into an output electrical signal, a dead zone for incident infrared light is generated on the imaging plane. The ratio of the detector area to the imaging plane is also called the filling factor, and in currently manufactured IRCCDs, this value is around 20% at most. Therefore, there is a large gap between the instantaneous fields of view seen by each detector of the IRCCD, and information regarding the shape of the object to be imaged is not only lost, but also may be lost in the case of a small target.

第2図は、例として円形目標に対してIRCCD
の各検出器が見る瞬時視野を表わした図である。
第2図は充足率が約40%と現在製造されているも
のより大きな値に相当する図であるが、瞬時視野
内の隙間が大きく、目標よりの情報が少なからず
損なわれている。
Figure 2 shows IRCCD for a circular target as an example.
FIG. 3 is a diagram showing the instantaneous field of view seen by each detector.
Figure 2 shows a sufficiency rate of about 40%, which corresponds to a higher value than those currently manufactured, but the gap in the instantaneous field of view is large, and information from the target is lost to some extent.

この発明は、この欠点を除去するために、赤外
線撮像装置の受光光学系の一部を振動鏡としたも
のであり、その内容について以下、図面を用いて
詳細に説明する。
In order to eliminate this drawback, the present invention uses a vibrating mirror as a part of the light receiving optical system of an infrared imaging device, and its contents will be explained in detail below with reference to the drawings.

第3図はこの発明の実施例であり、入射赤外光
1は対物レンズ2を透過した後に一次反射平面鏡
3で反射されるが、従来の装置において二次反射
平面鏡が設けられていた部分に設置されたインタ
レイス鏡10で反射された後にIRCCD5上で結
像される。インタレイス鏡10は鏡駆動モータ1
4によつて、IRCCD5が1フイールド分の入射
赤外光1を受光し、蓄積された電荷を検出器から
電荷転送素子に転送した直後にわずかにその光軸
に対する角度が変化し、IRCCD5の各検出器列
が、一つ前のフイールドで見ていた瞬時視野の間
の瞬時視野を見るように光路を変化させる。
FIG. 3 shows an embodiment of the present invention, in which incident infrared light 1 is reflected by a primary reflecting flat mirror 3 after passing through an objective lens 2. After being reflected by the installed interlace mirror 10, it is imaged on the IRCCD 5. The interlace mirror 10 is driven by a mirror drive motor 1
4, immediately after the IRCCD 5 receives one field of incident infrared light 1 and transfers the accumulated charge from the detector to the charge transfer element, its angle with respect to the optical axis changes slightly, and each IRCCD 5 The optical path is changed so that the detector array sees an instantaneous field of view between the instantaneous fields seen in the previous field.

第4図a,bは、IRCCDの各検出器列が見る
瞬時視野の関係を表わす図である。第4図aは先
に第1図に示した従来の赤外線撮像装置において
見られたようにインタレイス鏡を用いない場合の
図で、各検出器列が見る瞬時視野11は互いに大
きく離れており、検出器が見ない部分がかなりの
割合を占める。第4図bはインタレイス鏡を用い
て2:1インタレイスを行なつた場合の図で、偶
数フイールドにおいて各検出器列が見る瞬時視野
12と奇数フイールドにおいて各検出器列が見る
瞬時視野13は交互に並んでおり、それぞれ視野
の隙間を補い合つている。
FIGS. 4a and 4b are diagrams showing the relationship between the instantaneous fields of view seen by each detector row of the IRCCD. FIG. 4a is a diagram when an interlaced mirror is not used as seen in the conventional infrared imaging device shown in FIG. A large portion of the image is not seen by the detector. Figure 4b shows a case where 2:1 interlacing is performed using an interlacing mirror, and the instantaneous field of view 12 seen by each detector row in even fields and the instantaneous field of view 13 seen by each detector row in odd fields are alternate. They are lined up in a row, each supplementing the gaps in the field of view.

なお、以上はカタデイオプトリツク受光光学系
における一次鏡、二次鏡が平面鏡の場合について
説明したが、この発明は、これら反射鏡が平面鏡
でない場合や対物レンズを用いる代りに一次鏡が
凹面鏡になつた受光光学系を用いる場合に有効で
あることは言うまでもない。
Although the above description has been made on the case where the primary mirror and secondary mirror in the catadioptric light receiving optical system are plane mirrors, this invention is also applicable when these reflecting mirrors are not plane mirrors or when the primary mirror is a concave mirror instead of using an objective lens. Needless to say, this is effective when using a mature light-receiving optical system.

以上のように、この発明に係る赤外線撮像装置
においては、二次鏡を振動させることにより受光
光学系の光路を各フイールド毎に変化させること
によりIRCCDの各検出器列が見る瞬時視野の間
隙を各瞬時視野が補い合うために、視野中に生ず
る撮像にされないマスク領域を低減させることが
できる。また、以上の説明は2:1インタレイス
を行なう場合について説明したが、インタレイス
比は2:1に限らず任意の比率で行なうことが可
能であることは言うまでもない。
As described above, in the infrared imaging device according to the present invention, by changing the optical path of the light receiving optical system for each field by vibrating the secondary mirror, the gap in the instantaneous field of view seen by each detector row of the IRCCD is reduced. Because each instantaneous field of view complements each other, the mask area that occurs in the field of view that is not imaged can be reduced. Furthermore, although the above description has been made regarding the case where 2:1 interlacing is performed, it goes without saying that the interlacing ratio is not limited to 2:1 and can be performed at any desired ratio.

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

第1図はカタデイオプトリツク受光光学系を持
つ従来のIRCCD赤外線撮像装置の構成を表わす
図、第2図は例として円形目標に対してIRCCD
の各検出器が見る瞬時視野を表わした図、第3図
はこの発明の実施例、第4図a,bはIRCCDの
各検出器列が見る瞬時視野の関係を表わす図であ
る。 図中2は対物レンズ、3は一次反射平面鏡、5
はIRCCD、10はインタレイス鏡、14は鏡駆
動モータである。なお、図中同一あるいは相当部
分には同一符号を付して示してある。
Figure 1 shows the configuration of a conventional IRCCD infrared imaging device with a catadioptric light receiving optical system.
FIG. 3 is an embodiment of the present invention, and FIGS. 4a and 4b are diagrams showing the relationship between the instantaneous fields of view seen by each detector row of the IRCCD. In the figure, 2 is an objective lens, 3 is a primary reflection plane mirror, and 5
is an IRCCD, 10 is an interlace mirror, and 14 is a mirror drive motor. It should be noted that the same or corresponding parts in the figures are indicated by the same reference numerals.

Claims (1)

【特許請求の範囲】[Claims] 1 直線上の光軸上に配置されて、凸レンズ、前
記凸レンズ側に反射面を持ち中央部に前記光軸を
中心とした開口を持つ第1の反射鏡、および第1
の反射鏡側に反射面を持ち前記凸レンズと第1の
反射鏡との間に位置する第2の反射鏡とを有し、
入射光が前記凸レンズを透過した後に、第1の反
射鏡、第2の反射鏡で順々に反射されるように構
成された受光光学系と、前記受光光学系結像面に
設けられた面状固体撮像素子上に複数の赤外線検
出器から成る配列と、前記赤外線検出器配列が受
ける赤外線量に応じて発生した電荷を所定のセル
に蓄える電荷転送素子とからなり、前記電荷転送
素子を駆動することにより赤外線像を得る赤外線
撮像装置において、前記各赤外線検出器が見る瞬
時視野の位置をフイールド毎に、各フイールドで
上記赤外線検出器それぞれが見る瞬時視野の隙間
を補い合うように動かすべく上記受光光学系の光
路を傾けるように前記第2の反射鏡を振動させる
駆動装置を設けたことを特徴とする赤外線撮像装
置。
1. A convex lens, a first reflecting mirror having a reflective surface on the convex lens side and having an aperture centered on the optical axis in the center;
a second reflecting mirror having a reflecting surface on the reflecting mirror side and located between the convex lens and the first reflecting mirror;
a light-receiving optical system configured such that the incident light is sequentially reflected by a first reflecting mirror and a second reflecting mirror after passing through the convex lens; and a surface provided on an image-forming surface of the light-receiving optical system. The charge transfer element is composed of an array of a plurality of infrared detectors on a solid-state image sensor, and a charge transfer element that stores charges generated in accordance with the amount of infrared radiation received by the infrared detector array in a predetermined cell, and drives the charge transfer element. In an infrared imaging device that obtains an infrared image by An infrared imaging device comprising a drive device that vibrates the second reflecting mirror so as to tilt an optical path of an optical system.
JP56055929A 1981-04-14 1981-04-14 Infrared image pickup device Granted JPS57171225A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56055929A JPS57171225A (en) 1981-04-14 1981-04-14 Infrared image pickup device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56055929A JPS57171225A (en) 1981-04-14 1981-04-14 Infrared image pickup device

Publications (2)

Publication Number Publication Date
JPS57171225A JPS57171225A (en) 1982-10-21
JPS6149610B2 true JPS6149610B2 (en) 1986-10-30

Family

ID=13012772

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56055929A Granted JPS57171225A (en) 1981-04-14 1981-04-14 Infrared image pickup device

Country Status (1)

Country Link
JP (1) JPS57171225A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59228130A (en) * 1983-06-10 1984-12-21 Matsushita Electric Ind Co Ltd Thermal infrared detection device

Also Published As

Publication number Publication date
JPS57171225A (en) 1982-10-21

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