JPH07122722A - Image pickup device - Google Patents

Image pickup device

Info

Publication number
JPH07122722A
JPH07122722A JP5262455A JP26245593A JPH07122722A JP H07122722 A JPH07122722 A JP H07122722A JP 5262455 A JP5262455 A JP 5262455A JP 26245593 A JP26245593 A JP 26245593A JP H07122722 A JPH07122722 A JP H07122722A
Authority
JP
Japan
Prior art keywords
charge
charge transfer
patterns
light receiving
transfer element
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.)
Granted
Application number
JP5262455A
Other languages
Japanese (ja)
Other versions
JP2616672B2 (en
Inventor
Kazuo Konuma
和夫 小沼
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP5262455A priority Critical patent/JP2616672B2/en
Publication of JPH07122722A publication Critical patent/JPH07122722A/en
Application granted granted Critical
Publication of JP2616672B2 publication Critical patent/JP2616672B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Transforming Light Signals Into Electric Signals (AREA)
  • Solid State Image Pick-Up Elements (AREA)

Abstract

PURPOSE:To control the shapes of false patterns by providing adjacent sweeping switches which sweep part of charges of photodetectors to charge transferring elements which are different from the charge transfer elements to which the charges of the photodetectors are transferred. CONSTITUTION:TG1 and TG2 are maintained in opened states at the charge overflowing timing. Overflowing charges flow into the charge transferring element between adjacent false lateral patterns P1 and P3 after passing over the potential across an adjacent sweeping switch and photodetector reading-out switch which is lower than the potential in the charge transfer element in the transferring direction. When ordinary transfer is performed after the above- mentioned series of operations, the lateral false patterns P1, P2, and P3 are generated as oversaturation patterns. The saturation patterns can be changed to such arbitrary patterns as the cross patterns, etc., by adjusting the correlation between the potential obtained when the adjacent sweeping switches and the potential obtained when the charge transfer elements are set in the state of barrier.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は撮像装置に関するもの
である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an image pickup device.

【0002】[0002]

【従来の技術】従来の撮像装置の一例を図4に示す。図
の上から下方向への一次元方向への電荷転送を行なう電
荷結合素子からなる電荷転送素子2と受光素子1および
受光素子から電荷転送素子への信号電荷を転送する読み
出しスイッチ3より構成される単位画素7を二次元アレ
イ状に配してある。前記電荷結合素子は前記読み出しス
イッチが接続する部分3と非接続部分4とを有してい
る。この構造を有するイメージセンサはインターライン
型イメージセンサと呼ばれている。
2. Description of the Related Art FIG. 4 shows an example of a conventional image pickup apparatus. The charge transfer device 2 is composed of a charge-coupled device that transfers charges one-dimensionally from the top to the bottom of the figure, and is composed of a light receiving device 1 and a read switch 3 for transferring signal charges from the light receiving device to the charge transfer device. The unit pixels 7 are arranged in a two-dimensional array. The charge coupled device has a portion 3 to which the read switch is connected and a non-connection portion 4. An image sensor having this structure is called an interline image sensor.

【0003】[0003]

【発明が解決しようとする課題】インターライン型イメ
ージセンサを用いた撮像装置においては、受光素子から
転送される信号電荷量が電荷転送素子の保持電荷限界を
越えないように設定されている。前記限界を越える信号
電荷が受光素子から転送された場合、低いポテンシャル
障壁で分離された隣接する単位画素の信号と混ざってし
まう。図5を用いて具体的に説明する。図5(b)は単
位画素を二次元アレイ状に配して形成したイメージエリ
アを示す。図中に示すように一つの単位画素をQ2と呼
び、その上下方向の単位画素をQ1,Q3と呼ぶ。Q1
〜Q3は同一の電荷転送素子に接続されている。ここ
で、Q2の受光素子から電荷転送素子へ保持電荷限界を
越える電荷量が転送された状況を考える。この状況にお
ける電荷転送素子のポテンシャルの状態を図5(a)に
示す。保持限界を越えた分の電荷はQ1とQ3に混入す
る。即ち、図5(b)に示すように上下方向の線状の偽
パターンが生じてしまう。線状偽パターンの長さは受光
素子から転送される電荷量と保持限界との比に依存す
る。
In an image pickup device using an interline image sensor, the amount of signal charges transferred from the light receiving element is set so as not to exceed the held charge limit of the charge transfer element. When the signal charges exceeding the above limit are transferred from the light receiving element, they are mixed with the signals of the adjacent unit pixels separated by the low potential barrier. This will be specifically described with reference to FIG. FIG. 5B shows an image area formed by arranging unit pixels in a two-dimensional array. As shown in the figure, one unit pixel is called Q2, and the unit pixels in the vertical direction are called Q1 and Q3. Q1
To Q3 are connected to the same charge transfer element. Now, consider a situation in which a charge amount exceeding the held charge limit is transferred from the light receiving element of Q2 to the charge transfer element. The state of the potential of the charge transfer element in this situation is shown in FIG. The charges exceeding the holding limit are mixed in Q1 and Q3. That is, as shown in FIG. 5B, a vertical false pattern is generated. The length of the linear pseudo pattern depends on the ratio between the amount of charge transferred from the light receiving element and the holding limit.

【0004】撮像装置においては、受光素子で発生する
電荷量は外部から照射される光量に依存する。強い照射
光の下では多くの信号電荷が発生する。外部照射光は撮
像装置自身では制御することは出来ない。有害偽パター
ン発生を防ぐために、個々の受光素子にオーバーフロー
ドレインの機能を付加して電荷転送素子の保持限界を越
える発生電荷を捨てる工夫をしたり、リセット電圧を調
整することで受光素子の電荷容量を制限することで電荷
転送素子に保持限界を越えて電荷を転送しないようにし
ている。しかしながら、オーバーフロードレイン機能を
実現するためには横型オーバーフロードレインに於ては
単位画素内の有効受光素子面積減少で感度が低下する問
題を抱えてしまう。また、縦型オーバーフロードレイン
構造では検出器の構造に敏感なため、厳密に制御した製
造工程を必要とする。リセット電圧を調整する場合には
受光素子自身のダイナミックレンジ及び感度特性を劣化
させてしまう。
In the image pickup device, the amount of electric charge generated in the light receiving element depends on the amount of light emitted from the outside. Many signal charges are generated under strong irradiation light. The external irradiation light cannot be controlled by the imaging device itself. In order to prevent the generation of harmful false patterns, the function of overflow drain is added to each light receiving element to discard the generated charge that exceeds the holding limit of the charge transfer element, or the reset voltage is adjusted to adjust the charge capacity of the light receiving element. By limiting the charge, the charge is not transferred to the charge transfer element beyond the holding limit. However, in order to realize the overflow drain function, the lateral overflow drain has a problem that the sensitivity is lowered due to the reduction of the effective light receiving element area in the unit pixel. Further, since the vertical overflow drain structure is sensitive to the structure of the detector, it requires a strictly controlled manufacturing process. When the reset voltage is adjusted, the dynamic range and sensitivity characteristics of the light receiving element itself are deteriorated.

【0005】以上述べたように従来の撮像装置では想定
される最大の発生電荷量が電荷転送素子の保持限界を越
えないようにして有害偽パターンである上下方向の線偽
パターンの発生を防がなければならない問題を抱えてい
た。
As described above, in the conventional image pickup apparatus, the assumed maximum amount of generated charges does not exceed the holding limit of the charge transfer element to prevent the generation of the vertical line false pattern which is a harmful false pattern. I had a problem I had to do.

【0006】[0006]

【課題を解決するための手段】本発明は、一次元方向の
電荷転送を行なう電荷転送素子に隣接して受光素子を配
し、受光素子から電荷転送素子への電荷読み出しを行な
う読み出しスイッチで結んだ単位画素を二次元アレイ状
に配したイメージセンサを用いた撮像装置において、受
光素子の電荷を受光素子の電荷が転送される電荷転送素
子とは異なる隣接した電荷転送素子へ一部掃き出すため
の隣接掃き出しスイッチが具備されていることを特徴と
する撮像装置、及び、上記撮像装置において、前記読み
出しスイッチを介して電荷転送素子に信号電荷転送を開
始した後で、かつ、電荷転送素子での転送動作を開始す
る前に前記隣接掃き出しスイッチを開き、前記電荷転送
素子の保持電荷量を越えた分の電荷を前記読み出しスイ
ッチ、受光素子を介して前記隣接掃き出しスイッチと接
続された電荷転送素子へ転送することを特徴とする撮像
装置である。この構成によって、偽パターンの形状を制
御することが可能となるため、有害であった偽パターン
を用いて電荷の過飽和となっている箇所を検出すること
が可能となり、ひいては電荷の過飽和による電荷転送素
子の機能低下を防ぐことも可能となる。
According to the present invention, a light receiving element is arranged adjacent to a charge transfer element for transferring charges in a one-dimensional direction, and a read switch for reading out charges from the light receiving element to the charge transfer element is connected. In an imaging device using an image sensor in which sub-pixels are arranged in a two-dimensional array, the charge of the light receiving element is partially swept to an adjacent charge transfer element different from the charge transfer element to which the charge of the light receiving element is transferred. An image pickup device comprising an adjacent sweep switch, and in the image pickup device, after starting signal charge transfer to a charge transfer device via the readout switch, and at a charge transfer device. Before the operation is started, the adjacent sweep switch is opened, and the charge exceeding the amount of charge held in the charge transfer element is transferred to the read switch and the light receiving element. An imaging apparatus characterized by to transfer the adjacent sweep the charge transfer device which is connected to the switch. With this configuration, it is possible to control the shape of the false pattern, so that it is possible to detect the location where the charge is oversaturated by using the harmful false pattern, which in turn leads to charge transfer due to charge oversaturation. It is also possible to prevent the functional deterioration of the element.

【0007】[0007]

【実施例】本発明について図面を参照して説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described with reference to the drawings.

【0008】(実施例1)図1は本発明の第1の実施例
の構成図である。単位画素7には図4で示したインター
ライン型イメージセンサの構成に加えて隣接掃き出しス
イッチ6が具備されている。図2を用いてその駆動方法
と動作を示す。図1のV1,V4,TG1,TG3ゲー
ト電極への印加電圧を図2(a)に、そのチャネル電位
を図2(b)に示す。他の電極V3,V2はそれぞれV
1,V4の反転電圧である。また、本実施例1ではイン
ターレース読み出しの例であるがTG2とTG4は図2
(a)で示したフィールド(このフィールドを第1フィ
ールドと呼ぶ)では常にL(低)レベルであり、第2フ
ィールドで図2(a)と同様のパルス波形となる。図2
(a)の、、の各タイミングでのA−A’および
B−B’(図1)のポテンシャル分布を図2(c)にて
実線および破線で示す。説明のために図2(c)はP2
単位画素(図2(d)参照)の受光素子にa(図2
(c)−)の量の電荷が発生、保持されており、P1
およびP3の受光素子の電荷量が0(ゼロ)である状況
を設定した。さらに、この設定では電荷量aが電荷転送
素子の保持限界を越えているとした。のタイミングで
はTG1、TG3ともに閉状態であるため、電荷aはP
2の受光素子内で保持されている。TG1が開になって
からt[秒]後にTG3が開状態となる。この遅延時間
はパルス電圧印加にポテンシャル分布の形成および電荷
の移動が追随できるための待ち時間として設定してあ
る。この遅延時間をおいて隣接掃き出しスイッチ(TG
3)を開状態にすることで必要な電荷量の範囲で歪なく
受光素子の電荷を電荷転送素子へ移動させることを可能
にする。この実施例ではのタイミングにおける電荷量
bはのaと等しい。しかしながら、上記設定によりa
すなわちbの電荷量は電荷転送素子の保持限界を越えて
おり、転送動作中に電荷がポテンシャル井戸からあふれ
る。このあふれるタイミングをとする。図2(a)で
示したように、電荷があふれるタイミングではTG1お
よびTG3が開状態を維持している。このため、図2
(c)ので示したようにあふれた電荷は電荷転送素子
内の転送方向のポテンシャルバリアよりも低い隣接掃き
出しスイッチと受光素子読みだしスイッチのポテンシャ
ル上を通り、隣接するP1、P3の電荷転送素子内に流
れ込む。この一連の動作の後、通常の転送が行われると
図2(d)で示す過飽和パターンとして横偽パターン
(P1,、P2、P3)が発生する。
(Embodiment 1) FIG. 1 is a block diagram of the first embodiment of the present invention. The unit pixel 7 is provided with an adjacent sweep switch 6 in addition to the structure of the interline image sensor shown in FIG. The driving method and operation will be described with reference to FIG. The applied voltage to the V1, V4, TG1, and TG3 gate electrodes in FIG. 1 is shown in FIG. 2 (a), and the channel potential thereof is shown in FIG. 2 (b). The other electrodes V3 and V2 are V
It is an inversion voltage of 1, V4. In the first embodiment, an example of interlaced reading is used, but TG2 and TG4 are shown in FIG.
The field shown in (a) (this field is called the first field) is always at the L (low) level, and the second field has the same pulse waveform as in FIG. 2 (a). Figure 2
The potential distributions of AA ′ and BB ′ (FIG. 1) at the respective timings of and of (a) are shown by a solid line and a broken line in FIG. 2 (c). For the purpose of explanation, FIG. 2 (c) shows P2.
The light receiving element of the unit pixel (see FIG. 2D) is a (see FIG.
(C)-) is generated and held, and P1
And the situation where the charge amount of the light receiving element of P3 is 0 (zero) was set. Further, in this setting, the charge amount a exceeds the holding limit of the charge transfer element. At the timing of, since both TG1 and TG3 are in the closed state, the charge a is P
It is held in the second light receiving element. After t [seconds] after opening TG1, TG3 becomes open. This delay time is set as a waiting time so that the formation of potential distribution and the movement of charges can follow the pulse voltage application. Adjacent sweep switch (TG
By making 3) open, it is possible to move the charge of the light receiving element to the charge transfer element without distortion within the required charge amount range. In this embodiment, the charge amount b at the timing of is equal to a. However, because of the above setting,
That is, the amount of charges in b exceeds the holding limit of the charge transfer element, and charges overflow from the potential well during the transfer operation. Let this overflow timing. As shown in FIG. 2A, TG1 and TG3 maintain the open state at the timing when the charges overflow. For this reason,
As shown in (c), the overflowed charge passes over the potentials of the adjacent sweep switch and the light-receiving element reading switch, which are lower than the potential barrier in the transfer direction in the charge transfer element, and in the adjacent charge transfer elements of P1 and P3. Flow into. When normal transfer is performed after this series of operations, horizontal false patterns (P1, P2, P3) are generated as the oversaturation pattern shown in FIG.

【0009】過飽和パターンは隣接掃き出しスイッチの
開状態のポテンシャルと電荷転送素子のバリア状態のポ
テンシャルとの相対的な関係を調整することで十字パタ
ーン等の任意のパターンにすることができる。対象の中
心位置を検出する場合には十字過飽和パターンで充分に
行える。
The supersaturated pattern can be made into an arbitrary pattern such as a cross pattern by adjusting the relative relationship between the potential of the adjacent sweep switch in the open state and the potential of the charge transfer element in the barrier state. When detecting the center position of the target, the cross supersaturation pattern can be sufficiently used.

【0010】(実施例2)本発明に第2の実施例を図3
に示す。第1の実施例との相違は隣接掃き出しスイッチ
5が接続している部分との印加電圧が異なる点である。
接続部分が異なるために実施例1とは異なる過飽和パタ
ーンが得られる。
(Embodiment 2) A second embodiment of the present invention is shown in FIG.
Shown in. The difference from the first embodiment is that the applied voltage is different from the part to which the adjacent sweep switch 5 is connected.
Since the connecting portion is different, a supersaturation pattern different from that of the first embodiment can be obtained.

【0011】(実施例3)上述した2つの実施例では読
みだしスイッチと隣接掃き出しスイッチとのチャネル電
位特性が同じであったが、異なる特性とすることで、両
者に共通の駆動パルスを印加することも可能である。こ
の例では隣接掃き出しスイッチのチャネル電位特性のピ
ニング電位、ピニング印加電圧がそれぞれ読みだしスイ
ッチの特性と比べて浅く(ピニング電位)、高い(ピニ
ング印加電圧)。このイメージセンサに図2(a)のT
G1と同様の台形状の電圧を印加する。TG1の立ち上
がり部分の傾きを緩くすると各部チャネル電位の時間変
化は図2(a)で示したTG3がTG1よりも遅れて立
ち上がることと等価となる。遅延時間は台形波の立ち上
がり傾きで制御できる。また、V1〜V4の駆動波形を
3値パルスとすることで、電荷転送素子があふれるタイ
ミングを制御することも可能である。
(Embodiment 3) In the above-mentioned two embodiments, the read switch and the adjacent sweep switch have the same channel potential characteristics, but by adopting different characteristics, a common drive pulse is applied to both. It is also possible. In this example, the pinning potential and the pinning applied voltage of the channel potential characteristics of the adjacent sweep switch are shallower (pinning potential) and higher (pinning applied voltage) than the characteristics of the read switch, respectively. This image sensor has a T shown in FIG.
A trapezoidal voltage similar to G1 is applied. When the slope of the rising portion of TG1 is loosened, the time change of the channel potential of each part is equivalent to that of TG3 shown in FIG. 2A, which rises later than TG1. The delay time can be controlled by the rising slope of the trapezoidal wave. Further, by setting the driving waveform of V1 to V4 to be a ternary pulse, it is possible to control the timing when the charge transfer element overflows.

【0012】以上の例では電荷転送素子として電荷結合
素子(CCD)を用いた場合であるが、チャージスイー
プドデバイス(CSD)についても同様に実現できる。
CSDでは飽和レベルの定義が難しいが、電荷転送素子
に多量の電荷が入った場合にCSD内にひろがった電荷
を全て転送方向に流すためには追加転送パルスの増加を
必要とし、転送周波数が高くなる問題が顕著になる。本
発明により追加転送に対する負担が軽減できる。
In the above example, a charge coupled device (CCD) is used as a charge transfer device, but a charge swept device (CSD) can be similarly realized.
It is difficult to define the saturation level in CSD, but when a large amount of charge enters the charge transfer element, it is necessary to increase the number of additional transfer pulses in order to flow all the charge spread in the CSD in the transfer direction, and the transfer frequency is high. The problem becomes significant. The present invention can reduce the burden of additional transfer.

【0013】[0013]

【発明の効果】本発明による撮像装置では電荷転送素子
の転送電荷保持限界を越えた過飽和の電荷が受光素子で
発生した場合に、その過飽和パターンを選定することが
できる。特に、対象物の位置検出を行っている場合には
十字の過飽和パターンにすることで過飽和時にも位置検
出の機能を損なわない。このように、過飽和時でも機能
を損なうことの問題を軽減できるために、受光素子の感
度特性とダイナミックレンジの設定の自由度を増すこと
ができる。
In the image pickup device according to the present invention, when supersaturated charges exceeding the transfer charge holding limit of the charge transfer element are generated in the light receiving element, the supersaturation pattern can be selected. In particular, when the position of the object is being detected, the cross-saturation pattern is used so that the position detection function is not impaired even during oversaturation. As described above, since the problem of loss of function even at the time of oversaturation can be reduced, the degree of freedom in setting the sensitivity characteristics and the dynamic range of the light receiving element can be increased.

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

【図1】本発明の実施例1を示す撮像装置のイメージセ
ンサの構成図である。
FIG. 1 is a configuration diagram of an image sensor of an image pickup apparatus according to a first embodiment of the present invention.

【図2】本発明の実施例1の撮像装置の駆動方法を示す
図である。
FIG. 2 is a diagram showing a driving method of the image pickup apparatus according to the first embodiment of the present invention.

【図3】本発明の第2の実施例を示すイメージセンサの
構成図である。
FIG. 3 is a configuration diagram of an image sensor showing a second embodiment of the present invention.

【図4】従来の撮像装置の一例を示す構成図である。FIG. 4 is a configuration diagram showing an example of a conventional imaging device.

【図5】従来の撮像装置の抱える問題を説明するための
模式図である。
FIG. 5 is a schematic diagram for explaining a problem that a conventional imaging device has.

【符号の説明】[Explanation of symbols]

1 受光素子 2 電荷転送素子 3 電荷転送素子の読みだしスイッチ接続部 4 電荷転送素子の読みだしスイッチ非接続部 5 読みだしスイッチ 6 隣接掃き出しスイッチ 7 単位画素 V1、V2、V3、V4 電荷転送素子の電極名であ
る。
1 Light receiving element 2 Charge transfer element 3 Read switch connection section of charge transfer element 4 Read switch non-connection section of charge transfer element 5 Read switch 6 Adjacent sweep switch 7 Unit pixel V1, V2, V3, V4 Charge transfer element The electrode name.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 一次元方向の電荷転送を行なう電荷転送
素子に隣接して受光素子を配し、受光素子から電荷転送
素子への電荷読み出しを行なう読み出しスイッチで結ん
だ単位画素を二次元アレイ状に配したイメージセンサを
用いた撮像装置において、受光素子の電荷を受光素子の
電荷が転送される電荷転送素子とは異なる隣接した電荷
転送素子へ一部掃き出すための隣接掃き出しスイッチが
具備されていることを特徴とする撮像装置。
1. A two-dimensional array of unit pixels in which a light receiving element is arranged adjacent to a charge transfer element for transferring charges in a one-dimensional direction and connected by a read switch for reading out charges from the light receiving element to the charge transfer element. In an image pickup device using the image sensor arranged in, the adjacent sweep switch for partially sweeping the charge of the light receiving element to an adjacent charge transfer element different from the charge transfer element to which the charge of the light receiving element is transferred is provided. An imaging device characterized by the above.
【請求項2】 読み出しスイッチを介して電荷転送素子
に信号電荷転送を開始した後、かつ電荷転送素子におけ
る転送動作を開始するより前に、隣接掃き出しスイッチ
を開き、前記電荷転送素子の保持電荷量を越えた分の電
荷を前記読み出しスイッチ、受光素子を介して前記隣接
掃き出しスイッチと接続された電荷転送素子へ転送する
ことを特徴とする請求項1記載の撮像装置。
2. The amount of charge held in the charge transfer element is opened by opening the adjacent sweep switch after starting the signal charge transfer to the charge transfer element via the read switch and before starting the transfer operation in the charge transfer element. 2. The image pickup apparatus according to claim 1, wherein the charge exceeding the amount is transferred to the charge transfer element connected to the adjacent sweep switch via the read switch and the light receiving element.
JP5262455A 1993-10-20 1993-10-20 Imaging device Expired - Lifetime JP2616672B2 (en)

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Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5262455A JP2616672B2 (en) 1993-10-20 1993-10-20 Imaging device

Publications (2)

Publication Number Publication Date
JPH07122722A true JPH07122722A (en) 1995-05-12
JP2616672B2 JP2616672B2 (en) 1997-06-04

Family

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Family Applications (1)

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JP5262455A Expired - Lifetime JP2616672B2 (en) 1993-10-20 1993-10-20 Imaging device

Country Status (1)

Country Link
JP (1) JP2616672B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04189081A (en) * 1990-11-22 1992-07-07 Fujitsu Ltd Infrared image pickup device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04189081A (en) * 1990-11-22 1992-07-07 Fujitsu Ltd Infrared image pickup device

Also Published As

Publication number Publication date
JP2616672B2 (en) 1997-06-04

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