JPS58113729A - One-dimensional detector - Google Patents
One-dimensional detectorInfo
- Publication number
- JPS58113729A JPS58113729A JP56214919A JP21491981A JPS58113729A JP S58113729 A JPS58113729 A JP S58113729A JP 56214919 A JP56214919 A JP 56214919A JP 21491981 A JP21491981 A JP 21491981A JP S58113729 A JPS58113729 A JP S58113729A
- Authority
- JP
- Japan
- Prior art keywords
- dimensional
- face
- image sensor
- array side
- optical fiber
- 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
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N23/00—Cameras or camera modules comprising electronic image sensors; Control thereof
- H04N23/50—Constructional details
- H04N23/54—Mounting of pick-up tubes, electronic image sensors, deviation or focusing coils
Landscapes
- Engineering & Computer Science (AREA)
- Multimedia (AREA)
- Signal Processing (AREA)
- Radiation Pyrometers (AREA)
Abstract
Description
【発明の詳細な説明】
発明の技術分野
本発明はたとえば海洋１ｍ測衛鳳や地球資＃Ｉ探食衛星
（二搭載される可視近赤外放射針等（；用いられる一次
元検出器に関する０
発明の妖術的背景とその間細点
可視近赤外放射針の定食方式≦二は、大別して第ＩＷＪ
ｉ二不す確械走食万式と第２因（：示す電子走査方式の
ニガ式が知られている・ｌ［！ＩＶＣおいて、ｊは機械
的６二回転駆動される定食鏡、２は光学系、３は近赤外
検出用の一次元検出器。DETAILED DESCRIPTION OF THE INVENTION Technical Field of the Invention The present invention relates to, for example, a 1-meter oceanographic surveying satellite, a global satellite #I exploration satellite (visible and near-infrared radiation needles mounted on two The magical background of the invention and the set meal method of the fine point visible near infrared radiation needle ≦2 are broadly classified into No. IWJ
The Niga type of electronic scanning system is known as the i2-infinite mechanical scanning system and the second factor (:).l[!In IVC, j is a set mirror that is mechanically driven 62 times, and 2 3 is an optical system, and 3 is a one-dimensional detector for near-infrared detection.
４は地球表面の観測または探査饋域である・秦２図にお
いて、５は電荷結合素子ＣＣＤを用いたラインセンナよ
りなる一次元検出器、６は光学系、Ｌは地球表面王道＝
おける観測または探査−城の輻（走査幅）である・第２
図の電子走査方式では、衛星の進行方向ｒ ｃ直角な方
向を走査するものであり、衛星の進行Ｃ：伴って新しい
ラインを走査すること幅＝よって二次元イメージを得る
ことができる・この場合、ラインセンサのＣＣＤ素子数
を真、最小地上分解能をｄとすると。4 is the observation or exploration area of the earth's surface. In the Hata 2 diagram, 5 is a one-dimensional detector consisting of a line sensor using a charge-coupled device CCD, 6 is an optical system, and L is the earth's surface road =
Observation or exploration at - Castle convergence (scanning width) - Second
In the electronic scanning method shown in the figure, scanning is performed in a direction perpendicular to the satellite's traveling direction r c, and the satellite's traveling direction C: Accompanied by scanning a new line Width = Therefore, a two-dimensional image can be obtained - In this case , the number of CCD elements of the line sensor is true, and the minimum ground resolution is d.
１個のラインセンナを用いた場合には次式が成り立つ・
１、 ｍ Ｂ ｄ
たとえは最小地上分解能ｄｍ３０ｍ、ｃｃＤ索子数ｎ冨
２０４８とすると、走査幅りは約６１．４−となる。ｔ
ころで衛星のミツシコン要求からは走査幅りが広いほど
運用上有利であり、また最小地上分解能ｄは小さいほど
精度の高い情暢が得られる。このような要求からライン
七ンψのＣＣＤＣＤ素子数人きいほど前ましいが、テバ
イスの製作上多くの困難がある。なお少ない素子数のラ
インセンナを用いて走査幅を増す方法として、第３因Ｃ
ニホす如くラインセンナ９゜９を千鳥配置にする方法が
考えられるが、各ラインセンｆ９．９のＣＣＤの視線方
向を個別に副！１する必要があり、また各ラインセンナ
９゜９それぞれ６二別々の周辺回路を必要とする欠点か
ある・
＠萌の目的
従来のラインｃ ｅ ｔ＋センサでは実現困婦であった
大容量−１ｇ（たとえば致方から数十万画素）を有する
ことが＝’Ｉ能な一次元検出１１！を提供するものであ
る・
発明のｍｓ
すなわち本発明は、二へ元ＣＣＤイメージセンナの受光
部に対して、−次元・二次元配列側！ｌＩｖ？′Ｔなう
オプチカルファイバ束の二次元配列側端ｒｋＵを接合し
たものであり、上記オプチカルファイバ束の一次元配列
側端由が大容量−素の一次元受光面となる・
発明の実施例
以下内面を参照して本発明の一実施例を詳細に説明する
・第４因において、ｉｏは二次元ＣＣＤイメージセンナ
、１１はオプチカルファイバ束である・このオプチカル
ファイバー１１は。When one line sensor is used, the following formula holds true: 1, m B d For example, if the minimum ground resolution dm is 30 m and the number n of CCD cables is 2048, the scanning width will be approximately 61.4-. t
However, from the satellite's Mitsushicon requirements, the wider the scanning width, the more advantageous it is for operation, and the smaller the minimum ground resolution d, the more accurate the accuracy can be obtained. Due to these requirements, it is desirable to have several CCDCD devices with seven lines ψ, but there are many difficulties in manufacturing the device. Furthermore, as a method of increasing the scanning width using a line sensor with a small number of elements, the third factor C
It is conceivable to arrange the line sensors 9°9 in a staggered arrangement, as in Japan, but it would be better to set the viewing direction of the CCD of each line sensor f9.9 separately! It also has the disadvantage of requiring 62 separate peripheral circuits for each line sensor 9°9.@Moe's purpose Large capacity -1g, which was difficult to achieve with conventional line cet+ sensors. One-dimensional detection (for example, hundreds of thousands of pixels) is possible! ms of the invention In other words, the present invention provides a -dimensional/two-dimensional array side! lIv? The two-dimensionally arrayed side ends rkU of the optical fiber bundle 'T' are joined, and the one-dimensionally arrayed side end of the optical fiber bundle becomes a large-capacity element one-dimensional light-receiving surface. An embodiment of the present invention will be described in detail with reference to the inner surface.In the fourth factor, io is a two-dimensional CCD image sensor, and 11 is an optical fiber bundle.This optical fiber 11 is.
−次元画素を二次元画素に変換するためのものであり、
二次元配列側の端面は前記イメージセンナ１０の受光部
１１に接合さ゛れており、−次元配列側の端面は受光面
ＩＭとなっている・ここで説明の便宜上、ｉｌｓ図にＸ
、Ｙ方向とも３画素のＣＣＤよりなる二次元ＣＣＤイメ
ージセンナを用いて９嵩曇の一次元検出器を実現する原
理囚を示す・ここで１４はオプチカルファイバ束、ｉｌ
は二次元側端（１，ｔｉは一次元側地面である・
上記構成によれは、二次元ＣＯＤイメージセンナ１０と
して現在実用化されているたとえば４００Ｘ４００素子
程度のものを用いれば、１ｇ子数が１６万の一次元検出
器を実現できる・これは、ラインＣＣＤセンチの素子数
としては現在２０４８票子のものが実用レベルのものと
しては最大であることＣ：鑑みれば、非常な大容量
−である・
なお弗４因に示す二次元ＣＣＤイメージセンｆｉｌｌと
しては、特定の方式４：＠定するものではなく、良く知
られているフレームトランスファ方式、インターライン
方式、テヤージインジエクＶ−！Ｉン方式勢いずれ感＝
も適用可能である・まだオプチカルファイバ束１１の一
次元から二次元への変換配列≦；関しても、特定の配列
Ｃ：限定するものではなく、二次元ＣＣＵイメージセン
ｆｌｕの信号処理上最も有利な配列を選択することがで
きる−
発明の効果
上述したよ５５二本発明Ｃ二よれば、従来のＣＣＤライ
ンセンナでは冥埃困雌であった敵方から数十万−集の一
次元検出１１な容ｉζ：・蝿供でき、このような−次元
検出器をたとえばリモートセンシング用の可視近赤外放
射釘等１：４用することによ啼゛て、′、高分解能、広
い走査幅を持った装置を構成できる。It is for converting -dimensional pixels into two-dimensional pixels,
The end surface on the two-dimensional array side is joined to the light receiving section 11 of the image sensor 10, and the end surface on the -dimensional array side is the light receiving surface IM.
, shows the principle of realizing a one-dimensional detector with nine clouds using a two-dimensional CCD image sensor consisting of a three-pixel CCD in both the Y direction.Here, 14 is an optical fiber bundle, il
is the two-dimensional side edge (1, ti is the one-dimensional side ground). According to the above configuration, if a 400×400 element, which is currently in practical use as a two-dimensional COD image sensor 10, is used, the number of particles per gram is A one-dimensional detector of 160,000 can be realized. This means that the number of elements in a line CCD centimeter is currently 2,048, which is the largest at a practical level. C: Considering this, it has a very large capacity.
- It should be noted that the two-dimensional CCD image sensor fill shown in the 4th factor is not limited to a specific method 4, but the well-known frame transfer method, interline method, and thermal image sensor V- ! I feel like the in-method is at a loss =
Also applicable is the one-dimensional to two-dimensional conversion array of the optical fiber bundle 11≦; in this regard, the specific array C: is not limited to the most advantageous for signal processing of the two-dimensional CCU image sensor flu. Effects of the Invention As mentioned above, according to the present invention C2, one-dimensional detection of hundreds of thousands of samples from the enemy, which was difficult with the conventional CCD line sensor. By using such a -dimensional detector such as a visible near-infrared emitting nail for remote sensing at a ratio of 1:4, it is possible to obtain high resolution and wide scanning width. You can configure your own devices.
第１因は機械走査方式の放射針のｊ［理を示す図、第２
図は電子走査方式の放射針の原理を示すＩＩＶ、 １３
３図はＣＣＤラインセンナ（二より一次元画素数を増す
ための従来の方法を説明するためのＩｋ、１１４図は本
発明（：係る一次元検出器の一実施例を示す構成説明Ｉ
Ｎ、＊５ｅｌ！ａは第４図のオプチカルファイバ束の省
略な構成例を示す肉である・
１０・・・二次元ＣＣＵイメージセンサ、Ｉｌ−・・オ
プチカルファイバ束、ＩＩ−・・受光部、ＪＪ−・・−
次元受光面・
出−人代理人 弁理士 鈴江武 彦
第１１Ｉ１
１
嬉３１！１
１１１１４＋＠
１
ｊ
ｆＩｓ５５１１The first factor is the mechanical scanning radiation needle j [Figure showing the principle, second
Figure IIV shows the principle of an electronic scanning radiation needle, 13
3 is a CCD line sensor (Ik for explaining the conventional method for increasing the number of one-dimensional pixels from two), and FIG.
N, *5el! 10. Two-dimensional CCU image sensor, Il-. Optical fiber bundle, II-. Light receiving section, JJ--.
Dimensional light-receiving surface / Patent attorney Takehiko Suzue No. 11I1 1 Joy 31! 1 11114+@ 1 j fIs5511
Claims (1)
、−次元・二次元相互変換を行なうオプチカルファイバ
束の二次元配列側端面を接合させ、このファイバ末の一
次元配列側端面を一次元検出器としたことを特徴とする
一次元検出器・The end face on the two-dimensional array side of the optical fiber bundle that performs -dimensional and two-dimensional conversion is joined to the light receiving part C2 of the two-dimensional charge-coupled confectionery image sensor, and the end face on the one-dimensional array side of this fiber end is detected in one dimension. One-dimensional detector/
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56214919A JPS58113729A (en) | 1981-12-26 | 1981-12-26 | One-dimensional detector |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56214919A JPS58113729A (en) | 1981-12-26 | 1981-12-26 | One-dimensional detector |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS58113729A true JPS58113729A (en) | 1983-07-06 |
Family
ID=16663745
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56214919A Pending JPS58113729A (en) | 1981-12-26 | 1981-12-26 | One-dimensional detector |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS58113729A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0735611A (en) * | 1993-07-23 | 1995-02-07 | Nec Corp | Infrared camera |
| EP0694771A1 (en) * | 1994-06-29 | 1996-01-31 | BFI ENTSORGUNGSTECHNOLOGIE GmbH | An optical monitoring apparatus |
| JP2004518948A (en) * | 2000-08-10 | 2004-06-24 | レイセオン・カンパニー | Multicolor Stirling sensor system |
| EP1931133A1 (en) * | 2006-12-07 | 2008-06-11 | Sick Ag | Method and device for optical acquisition of a structure |
-
1981
- 1981-12-26 JP JP56214919A patent/JPS58113729A/en active Pending
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0735611A (en) * | 1993-07-23 | 1995-02-07 | Nec Corp | Infrared camera |
| EP0694771A1 (en) * | 1994-06-29 | 1996-01-31 | BFI ENTSORGUNGSTECHNOLOGIE GmbH | An optical monitoring apparatus |
| US5668367A (en) * | 1994-06-29 | 1997-09-16 | Bfi Entsorgungstechnologie Gmbh | Optical space monitoring apparatus comprising light guiding fibers transmitting light through the space to be monitored |
| USRE36094E (en) * | 1994-06-29 | 1999-02-16 | Bfi Entsorgungstechnologie Gmbh | Optical space monitoring apparatus comprising light guiding fibers transmitting light through the space to be monitored |
| JP2004518948A (en) * | 2000-08-10 | 2004-06-24 | レイセオン・カンパニー | Multicolor Stirling sensor system |
| EP1931133A1 (en) * | 2006-12-07 | 2008-06-11 | Sick Ag | Method and device for optical acquisition of a structure |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| WO2016199594A1 (en) | Solid-state imaging device and electronic device | |
| US5416324A (en) | Optical imaging device with integrated polarizer | |
| US20140198183A1 (en) | Sensing pixel and image sensor including same | |
| US7491937B2 (en) | Two-wavelength image sensor picking up both visible and infrared images | |
| CN105991978B (en) | The method of imaging sensor and generation depth data with depth detection pixel | |
| JP2018064086A5 (en) | ||
| JP2003007994A (en) | Solid-state image pickup element, stereoscopic camera apparatus, and range finder | |
| US20100044822A1 (en) | Luminous radiation colour photosensitive structure | |
| US5119181A (en) | Color array for use in fabricating full width arrays | |
| JP2008268112A (en) | Sensor | |
| KR100783335B1 (en) | Measuring method of incident light and sensor having spectroscopic mechanism employing it | |
| US4596930A (en) | Arrangement for multispectal imaging of objects, preferably targets | |
| CN106899790A (en) | Camera head and camera | |
| KR20110121531A (en) | Solid-state imaging element and imaging device | |
| JPS58113729A (en) | One-dimensional detector | |
| US9509930B2 (en) | Device comprising a set of electromagnetic radiation sensitive detectors and arrangement of a set of such devices | |
| EP0250456A1 (en) | Method and apparatus for scanning thermal images. | |
| JP3949360B2 (en) | Color image sensor | |
| JP2011205085A (en) | Imaging device | |
| JPH0222973A (en) | Solid-state image pickup device | |
| JP3640515B2 (en) | Distance detector | |
| JP6245942B2 (en) | Image sensor | |
| JPS63193678A (en) | Solid-state area image pickup device | |
| JPH0572470A (en) | Phase difference detection type focus detection device | |
| EP0066020B1 (en) | Infrared energy detector system utilizing a charge transfer device sensor |