JPS6074475A - Solid state image pickup element - Google Patents
Solid state image pickup elementInfo
- Publication number
- JPS6074475A JPS6074475A JP58181465A JP18146583A JPS6074475A JP S6074475 A JPS6074475 A JP S6074475A JP 58181465 A JP58181465 A JP 58181465A JP 18146583 A JP18146583 A JP 18146583A JP S6074475 A JPS6074475 A JP S6074475A
- Authority
- JP
- Japan
- Prior art keywords
- region
- conductivity type
- transfer
- type
- type semiconductor
- 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.)
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F39/00—Integrated devices, or assemblies of multiple devices, comprising at least one element covered by group H10F30/00, e.g. radiation detectors comprising photodiode arrays
- H10F39/10—Integrated devices
- H10F39/12—Image sensors
- H10F39/15—Charge-coupled device [CCD] image sensors
- H10F39/158—Charge-coupled device [CCD] image sensors having arrangements for blooming suppression
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- Solid State Image Pick-Up Elements (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、電荷転送素子がfllいらノ12、受光によ
り得られる信号電荷が一定の方向に転送さItで、撮像
113力信号が生ぜしめらフ]、るように構i戊埒ノ′
1.左固体撮像素子に関する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention is directed to a charge transfer device that transfers a signal charge obtained by receiving light in a fixed direction and generates an imaging signal. , the structure is like this
1. Regarding the left solid-state image sensor.
背景技術とその問題点
電荷結合素子(チャージ・カップルド・ディバイス、以
下CCDと呼ぶ)舌の11L荷Ilv、送、4・ミ子が
用いられて構成き、t′した固体撮像素子には、大別し
て、フレーム転送型とインク−ライン転送)−りとがあ
り、夫々、その長所を有効に生かすべく使い分けらソ1
ている。BACKGROUND TECHNOLOGY AND PROBLEMS A charge-coupled device (hereinafter referred to as CCD) is constructed using a 11L load Ilv, 4, and 4 mm, and a solid-state image sensor with t' is as follows: Broadly speaking, there are two types: frame transfer type and ink-line transfer type.
ing.
例えば、インターライン転送型CCI)撮像7了の一例
は図面の第1図に示きれる如く、)1重樽体基体上に、
水平列及び垂iば列を形成して配さ才1.た複数の受:
)’e素子部/と受光素子部/の垂i(j 1111心
沿って配てれた複数列のCCDfl¥で形成σ)1.た
垂1i!i ql、<送部氾とを含んで成る受光・垂1
1ゴ転送部3と、この受光・垂直転送部、?に結合きれ
た水平1匠送部夕と、出力部Sと奢備えて構成きれ、受
光・正直転送部3及び水平転送部グによって、受)℃に
より倍号電荷全発生するとともに得られた信号電荷全垂
直方向及び水平方向に転送−4−る活性領域が形成され
る。For example, an example of interline transfer type CCI) imaging 7 is as shown in Figure 1 of the drawings.
1. Arranged to form horizontal rows and vertical rows. Multiple ukes:
) 'e Vertical i of the element part / and the light receiving element part / (formed by multiple rows of CCD fl\ arranged along the j 1111 center σ) 1. Tadare 1i! i ql, <light reception/reduction 1 comprising <transmission section flooding
1 Go transfer section 3 and this light receiving/vertical transfer section, ? It is composed of a horizontal transmitter, an output section S, and a horizontal transmitter connected to the receiver. An active region is formed in which charge is transferred both vertically and horizontally.
斯かる撮像素子による撮像動作が行われる場合にば、垂
)α転送部ス及び水平転送部グに所定の垂直転送、駆動
信号及び水平転送駆動信号が夫々供給されて電荷転送動
作がなされる。その場合、例えば、/フレーム期間内の
受光により各受光素子部/に得らまた信号電荷が、垂直
転送部−に読み出はれ、これが垂直転送部iの電荷転送
動作により、各水平ブランキング期間ごとに順次水平転
送部りへ垂11T転送きれていく。この水平転送部グに
は、信号電荷が受9′6累子部/の/水平列で得らノ1
.る信号電荷ごとに順次転送きれ、これが水平転送部グ
の電荷転送動作により、各水平映像期間に出力部3へ水
平転送きれていき、Ilj力部kから撮像出力信号が得
られるのである。When such an imaging device performs an imaging operation, a predetermined vertical transfer drive signal and horizontal transfer drive signal are supplied to the vertical α transfer unit S and horizontal transfer unit G, respectively, and a charge transfer operation is performed. In that case, for example, the signal charge obtained in each light receiving element section / by light reception within the /frame period is read out to the vertical transfer section -, and this is transferred to each horizontal blanking section by the charge transfer operation of the vertical transfer section i. The vertical 11T transfer to the horizontal transfer section is completed sequentially in each period. In this horizontal transfer section, the signal charge is obtained in the horizontal column of the receiving section 9'6.
.. The horizontal transfer of each signal charge to the output section 3 is completed in each horizontal video period by the charge transfer operation of the horizontal transfer section k, and an imaging output signal is obtained from the Ilj output section k.
上述の撮像素子の受光・垂直転送部3は、より詳細には
、例えば、第λ図Aに示される如く、受光素子部/の各
垂直列と各垂直転送部lとの間に読出ゲート部乙が形成
芒へ、各受光素子部/の周囲には、芒らに、チーヤンネ
ル・7.トソノぐ−7が形成きれている。寸た、チVン
ネル・ストソノ々−7に隣接してオーバーフロー・ドレ
インgが配σノ12、このオーバーフロー・ドレインg
と隣りの垂直転送yt++ 、2との間はチャンネル・
ストッパー9で1区別き汎でいる。芒らに、垂1r■転
送部二」二には、絶縁層イ亡介して、水平方向に延びる
重置転送電極10が垂直方向に順次配列きノ]、ている
。垂直転送部(11i10は第1の電)l夕φ/と第氾
の電極φ−とが父力に配きれて形1戊σれており、01
./の電極φ/及び第1の電極φ2は、夫々、蓄積部電
極φ/。及びφユ。と転送部電極(電位障壁電極)φ/
L及びφytとて構成σ′i1.ている。そして、垂1
に転送部記に於ける]電荷転送動作は、第1の電極φ/
及び第2の電極φaに、例えば、ス相の転送1駆動信号
が夫々供給芒九て、行われ、そのとき、蓄積部′電極φ
/。More specifically, as shown in FIG. B is formed into the awn, and around each light-receiving element part/awn is a chiyannel 7. Tosonog-7 is completely formed. In addition, an overflow drain g is arranged adjacent to the channel 7, and this overflow drain g
There is a channel between yt++ and the adjacent vertical transfer yt++, 2.
Stopper 9 makes one difference. In the vertical transfer section 2, overlapping transfer electrodes 10 extending in the horizontal direction are sequentially arranged in the vertical direction with an insulating layer interposed therebetween. The vertical transfer part (11i10 is the first electrode) φ/ and the electrode φ- of the first electrode are arranged in the father force and have a shape of 1 σ, 01
.. The electrode φ/ and the first electrode φ2 are respectively the storage electrode φ/. and φyu. and transfer section electrode (potential barrier electrode) φ/
L and φyt are configured σ'i1. ing. And then 1
[in the transfer section]] The charge transfer operation is performed using the first electrode φ/
For example, a phase transfer 1 drive signal is supplied to the second electrode φa and the second electrode φa, and at that time, the storage section' electrode φ
/.
及びφ2cの下方に垂直転送部ユに於ける蓄積領域が形
成式、f71、また、転送部電極φ/を及びφ2Lの下
方に垂直転送部スに於ける転送領域(電位障壁領域)が
形成きれるようにきれてお9、転送領域には、隣接する
蓄積領域よシミ位が浅く(低く)なって電イ〜γ障壁ケ
形成するため、例えば、イオン注入領1戊が設けらノ1
.る、あるいは、転送部電極φ/を及Uφ、2を下の絶
縁層の厚さが犬とさ、tする等の処理がなをハ、ている
。第2図13は第ス図Aの■13−II Bの断面を示
し、例えば、P形の半導体基体//の一方の表面側に、
上述の受−)−素−了部/、垂直転送部ノ及びオーバー
フロー・トレインgカN形半導体領域とE7て、寸り、
チャンネル・ストッパー7及び9が不純物濃度が高めら
れたP形用り導体領域として、夫々、−に記各部が形成
てれ、絶縁層72ケ介して垂直転送電極70ケ形成する
第1の市、極φノが配はれている。この例に、垂直転送
7[j、極が読出ゲート電イ浜をも兼ねる」局舎であり
、読出ゲート部乙上にもこの第氾の電極φ) (詳細V
こは、その蓄積¥SIS電極φコ。)が配きれている。The storage region in the vertical transfer section Y is formed below the transfer section electrode φ/ and φ2c, and the transfer region (potential barrier region) in the vertical transfer section S is formed below the transfer section electrode φ/ and φ2L. For example, an ion implantation region 1 is not provided in the transfer region because the stain level is shallower (lower) than in the adjacent storage region and forms an electric charge to γ barrier.
.. Alternatively, the thickness of the insulating layer below the transfer section electrode φ/Uφ may be increased or the thickness of the underlying insulating layer may be increased. FIG. 2 13 shows a cross section of 13-II B in FIG.
The dimensions of the above-mentioned receiving section, the vertical transfer section and the overflow train G, the N-type semiconductor region and E7,
Channel stoppers 7 and 9 are respectively formed as P-type conductor regions with increased impurity concentration, and a first region in which 70 vertical transfer electrodes are formed via 72 insulating layers; Pole φノ is placed. In this example, the vertical transfer 7[j, pole also serves as the readout gate electrode A], and the readout gate part B also has this third electrode φ) (Details V
This is the accumulation\SIS electrode φ. ) are distributed.
従来の斯かる固体撮像素子に於いては、P形の半導体基
体//に形成てれた受光・垂直転送部3と水平転送部グ
とから成る活性領域の周囲に、活性領域を囲み、σらに
は、活性領域の受)Y−・垂111転送部3と11」i
刃部Sとの間に延びる、P形の″1′カ体基体//の不
純物濃度が高めらノ1.てイPtられる17ξ1不純物
濃度ヶ有するP形半導体領域が形成@ ;!1.1低い
電位をとるチャンネル・ストップ領域とてΣノ15、活
性領域り(で発生した電荷(電子)が活性領域内に流入
しないようにされている。活性領域りlて発生した電荷
が活性領(或内に流入すると、ン占竹領l・表内で(1
%ら才1.る信号電荷に混入して転送きれ、出力部Sか
ら取り出される撮像出力信号中にノイズIJk分を生ぜ
しめる虞れがあるからである、。In such a conventional solid-state image sensing device, an active region consisting of a light receiving/vertical transfer section 3 and a horizontal transfer section 3 formed on a P-type semiconductor substrate is surrounded by a σ In addition, the active area receiver) Y-/vertical 111 transfer section 3 and 11''
Since the impurity concentration of the P-type ``1'' body substrate // extending between the blade part S is increased, a P-type semiconductor region having an impurity concentration of 17ξ1 is formed. The channel stop region, which takes a low potential, is designed to prevent charges (electrons) generated in the active region from flowing into the active region. When it flows into a certain area, it becomes (1
%Rasai1. This is because there is a risk that the noise IJk may be mixed with the signal charge transferred and may be transferred, causing noise IJk in the image pickup output signal taken out from the output section S.
しかしながら、」二連の如くに括ゼ1:′IJ11域の
周囲に形成a ′11.るチャンネル・ストップ領域U
、その表面積が比軟重大になるものとはt′l−1その
上1c )゛にが入射すると、入射光はチャンネル・ス
トップ領域から埒らには半導体基体に到達して>’e
’1.lI、変換により電荷を発生し、斯かる電荷は゛
1′導体基体中を拡1)りしていくが、その一部がP形
31′導体基体からl内性領域に不要電荷として入るも
のとなって1〜寸う3、このようLC2活性領域の周囲
のチャンネノ【・・ストツブ領域からの入射光にもとず
く光電変換により発生し、半導体基体から活1ツ1:、
領域に入る不要電荷は、活性領域内を信号電荷に混入し
て転送はれ、その結果、出力部りから取り出される撮像
出力信号中にノイズ成分を生せしめるという不都合を伴
うものとなる。However, a double bracket 1:' is formed around the IJ11 region a'11. Channel stop area U
, the surface area of which becomes relatively important is t'l-1 and 1c) When incident light reaches the semiconductor substrate from the channel stop region and becomes
'1. A charge is generated by the conversion, and this charge spreads through the 1' conductor substrate, but some of it enters the 1 internal region from the P-type 31' conductor substrate as an unnecessary charge. 1 to 3, the channel around the LC2 active region [... is generated by photoelectric conversion based on the incident light from the stop region, and the active region 1 from the semiconductor substrate is generated.
Unnecessary charges entering the region mix with signal charges within the active region and are transferred, resulting in the inconvenience of producing noise components in the imaging output signal taken out from the output section.
発明の目的
斯かる点に鑑み本発明は、半導体基体上に、受光により
信号電荷を発生するとともに得られた信号電荷全所定の
方向に転送する活性領域が、その周囲にチャンネル・ス
トップ領域生伴って形h+iさね、る構成?有し、その
チャンネル・ストップ領域に入射する光にもとずく光電
変換により電荷が発生しても、斯かる電荷が半導体基体
中を拡散して活性領域に不要電荷として入っていくこと
を防−f[−できるようにきれた固体彫像素子を提供す
ることケ目的とする。Purpose of the Invention In view of the above, the present invention provides an active region on a semiconductor substrate, which generates signal charges by receiving light and transfers all the obtained signal charges in a predetermined direction, and a channel stop region is formed around the active region. Te form h + i Sane, Ru composition? Even if charges are generated by photoelectric conversion based on light incident on the channel stop region, such charges are prevented from diffusing in the semiconductor substrate and entering the active region as unnecessary charges. It is an object of the present invention to provide a solid-state statuary element capable of producing f[-.
発明の概要
本発明に係る固体撮像素子は、第1の導電形、例えば、
P形の半導体基体上に、受光によシ信号電荷を発生する
とともに得られた信号電荷を所定の電荷転送方向をもっ
て転送する」:うにされた活性領域が、その周囲に第1
の導電形盆もつ第1及び第2の半導体領域を2重に伴っ
て配置さIl、、第1及び第2の半導体領域の夫々の間
に、第1 J)導電形とは異なる第2の導電形、例えば
、P形の第、?の半導体領域及びこの第3の半導体領域
と同一の導電形をもち、第3の半導体領域」:り不純物
濃度が高い第ダの半導体領域が、夫々、第1及び第認の
半導体領域に沿って配てれて、こttら第1゜第氾、第
、?及び第グの半導体領域がチーへ′ン坏ル・ストップ
領域を形1戊するように構成さノ95、第3及び第グの
半導体領域にfl−j所定の電圧が印加てれろよう(C
なσ)上る。Summary of the Invention A solid-state image sensor according to the present invention has a first conductivity type, for example,
On a P-type semiconductor substrate, a signal charge is generated by light reception and the obtained signal charge is transferred in a predetermined charge transfer direction.
J) A second semiconductor region having a conductivity type different from the first conductivity type is arranged between each of the first and second semiconductor regions. The conductivity type, for example, P type, ? A semiconductor region having the same conductivity type as the third semiconductor region and a third semiconductor region having a high impurity concentration are arranged along the first and third semiconductor regions, respectively. Handed out, these are the 1st, 1st, 1st, ? 95, a predetermined voltage fl-j may be applied to the third and third semiconductor regions (C).
Naσ) Go up.
このようにきれることにより、ン占性領域の周囲に形6
父σ汎るチャンネル・ストップ領域に人9.r −rる
光にもとすく光電変換により電荷が発生しても、発生し
た電荷は、比)1反的旨い電位となる第3の半導体領域
に吸引され、芒らに、より高い電位となる第グの半導体
領域に集めらソ7.ること(Cなり従つて、半導体基体
中を拡散していくことが防市でれて、半導体基体から活
性領域へ流入することがほとんどないものとて)1.る
。By cutting in this way, a shape of 6 is formed around the occupied area.
9. People in the father σ channel stop area. Even if charges are generated by photoelectric conversion in response to r-r light, the generated charges are attracted to the third semiconductor region, which has a higher potential than the ratio of 1, and is transferred to the awn with a higher potential. 7. (Assuming that C diffuses through the semiconductor substrate and almost never flows from the semiconductor substrate into the active region) 1. Ru.
実 施 例
第3図は本発明に係る固体撮像素子の一例ケ示1゛o
この例に於いては、例えばP形の半導体基体−」−に、
受光によシ信号電荷ケ発生するとともに得られた信号電
荷を所定の電荷転送方向孕もって転送するようにきれた
活性類1或ノ0が配置されている。この活性領域、、2
0は、第1図に示’g、aると同様の複数の受光素子部
/及び平面転送部、2を含んで成る受光・垂直転送部3
と、水平転送部ダとで形FJy、a ;n、ており、さ
らに、この活性領域、20の水平転送1lljグの−4
に接して、第1図に示芒71.ると同様の出力部5が配
てれている。そして、活性領域、;20は、その中の各
受光素子部/に於ける受光1(より信号電荷を発生して
、発生きれた言号電荷を垂直転送部氾によって水平転送
部ダへと垂直方向に転送し、芒らに、水平転送部ヶによ
り[1,を接する出力部Sへと水平方向に転送1−る。Embodiment FIG. 3 shows an example of the solid-state image sensor according to the present invention.
In this example, for example, in a P-type semiconductor substrate,
Active groups 1 and 0 are arranged so as to generate signal charges upon reception of light and to transfer the obtained signal charges in a predetermined charge transfer direction. This active region, 2
0 is a light receiving/vertical transfer section 3 comprising a plurality of light receiving element sections/and a plane transfer section 2 similar to those shown in Fig. 1.
, and the horizontal transfer section DA has the form FJy,a;n, and furthermore, this active region has -4
71. is shown in FIG. A similar output section 5 is provided. The active region; 20 generates signal charges at each light-receiving element section in the active region; Then, the horizontal transfer section transfers [1, to the adjacent output section S in the horizontal direction.
斯かる活性領域記0及び1」A刃部にの周囲には、これ
らを隣接包囲する、例えば、■〕形の半導体早2体の不
純物濃度を高めて得られたP形゛」〈導体領域2/が形
成さノ′シ、芒らに、その夕日[111ケP形゛]′導
体領1戒」/との間に所定の間隔を伴って包囲rる、同
様に、P形の半導体基体の不純物#度を高めて得られた
P形半導体領域aaが形成式ノ1.でいる、。Surrounding the active regions 0 and 1''A blade portions, for example, a P-type conductor region obtained by increasing the impurity concentration of a semiconductor diode of type ■゛゛゛〈 which surrounds these active regions adjacently. Similarly, a P-type semiconductor surrounds the awn with a predetermined distance between it and the awn 2/ is formed. The P-type semiconductor region aa obtained by increasing the impurity concentration of the substrate is formed according to the formation formula No. 1. I'm here.
即ち、活性領域、、20及び出力部、S−fil: 、
旨不純物濃度ケ有したiつのP形半導体領域λ/及びβ
−Vこよって氾重に包囲σれているのである1、そして
、P形半導体領域、、2/と、Ilとの間にd、■)形
゛1′1体鎖域22の内縁に隣接して一周する゛I′専
休基体と1″:i異なる導゛ボ、形の半導体領域、この
曜1合には、N形半導体領域、、!3が、比較的太なる
面積をSもって配きれ、孕らに、このN形半導体領域認
3の内縁及びP形半導体領域2/の外縁に隣1’、i
Lで一周する、N形半導体領域、23より不純物濃度が
高めらfl、た高不純物濃度N形半導体領域(以−[・
、N1−形半導体領域という)、24が配でノコ、てい
る。N1−形半導体領域、2/1.は、活性領域スθ及
び13力部kを包囲して一周1゛るとともに、活性領域
20の受光・正面転送部3ど出力部にとで挾1ノ1.た
部分にも延びるものときれている。That is, the active region, , 20 and the output section, S-fil: ,
i P-type semiconductor regions λ/ and β with impurity concentrations
-V is therefore surrounded by flood weight σ, and between the P-type semiconductor region, , 2/ and Il, d, 1'': i is a semiconductor region of a different conductive shape, an N-type semiconductor region,...!3 with a relatively thick area S. 1', i next to the inner edge of this N-type semiconductor region 3 and the outer edge of P-type semiconductor region 2/
An N-type semiconductor region with a higher impurity concentration than 23 and a high impurity concentration N-type semiconductor region (hereinafter referred to as [.
, N1-type semiconductor region), 24 are arranged. N1-type semiconductor region, 2/1. 1. surrounds the active region θ and 13 force part k and goes around the active region 1. It also extends to the lower part and is broken.
第夕図A、 1−j 第、?図ノIll A−IV A
ノ断面を示し、P形の半導体基体//の一方の表面側
に、」二連の活性領域、、20の外縁部に隣接して、−
に二連のP形仝IL導体領域−!/2反4−形半導体領
域氾グ、N形半導体領域23及びP形半導体領域、2.
2が順次形成てれていることがわかる。Evening figure A, 1-jth, ? Figure Ill A-IV A
On one surface side of the P-type semiconductor substrate, adjacent to the outer edge of the double active region, 20, -
Two series of P-shaped IL conductor areas-! /2 anti-4-type semiconductor region flooding, N-type semiconductor region 23 and P-type semiconductor region, 2.
It can be seen that 2 is formed sequentially.
このよう姥配さノ1−たP形半導体領域dl及び、2.
2.N形半導体領域ユ、?及びN十形半導体領j・曳、
2/l:は、全体として、活性領域aθに対するチャン
ネル・ストップ領域を形成してkす、N形崖樽体領域2
3及びN1形半導体領域、、2ケは、動作時には所定の
電I:Eが印加さ:t1.るようにな芒れている。2. The P-type semiconductor region dl arranged in this way;
2. N-type semiconductor region? and N-decade semiconductor region j.
2/l: is an N-shaped barrel region 2 which collectively forms a channel stop region for the active region aθ.
During operation, a predetermined voltage I:E is applied to t1.3 and N1 type semiconductor regions. The awn is shaped like a tree.
このため、動作時に於いては、チャンネル・ストップ領
域を形成する各領域2/、、2.2..1.3及び、2
/l−の電位は、第9図13にて、第ケ図Aに関連させ
、−]:た、縦軸に電位■を下方に行く程大走して示す
如く、活性領域20に接して最内端部に位置するP形半
導体領域、2/及び最外瑞部に位置−「るP形半導体領
域、2.2の電位力稍股も低く、N形半導体領域23の
電f)/はP形半導体領1・ilj、2/及びdlの電
位より高り、KF形半導体領域2t/、の電位し」、さ
らに高くなるものLさノ1.る3、
こノ1.により、P形′″1を導体領域ユ/にj:゛つ
て、ン占性領域、、!0に対するii′lT接的なヂA
・ンネル・ストップ作用がな式ハ2、萱た、jυiかる
チャンネル・ストップ領域ケ形成する各領域、2/、:
l:、1.、)、3及びdヶに光が入射し、人躬元が各
領1戎、!/、!認。Therefore, during operation, each region 2/, 2.2, . .. 1.3 and 2
The potential of /l- is shown in FIG. 9 and 13 in relation to FIG. The potential force of the P-type semiconductor region located at the innermost end, 2/, and the P-type semiconductor region located at the outermost part, 2.2, is also low, and the electric potential f)/ of the N-type semiconductor region 23 is low. is higher than the potential of the P-type semiconductor region 1.ilj, 2/ and dl, and the potential of the KF-type semiconductor region 2t/, which becomes even higher. 3. This 1. Therefore, when P-type ′″1 is placed in the conductor region/j:
・Equation 2, where the channel stop action takes place, are each area forming the channel stop region, 2/:
l:, 1. , ), 3 and d, the light enters each region, and the human body is 1 time in each region,! /,! Approved.
23及び、2夕からさら1(は■)形の半導体基体に3
H11達して元′セ変換により電荷(重任)欠発生せし
めた場合には、斯かる?(i、荷は、比イ19的人なる
表jrii に’iをもって広がる電位が高いN形2F
導体領1或」3しこ効果的に吸引さ))1、さらに、よ
り高い′ff、 Ij、7忙イ)つN1形半導体領域、
2 Z +/im集めらI’して、■〕形の゛l′j、
’7:休基体//中を体散(7ていくことがなく、従っ
て、各領域:、l/、22.、、!3及び271からの
入射−ン“(、によシ発生せしめられた電荷(電子〕が
、P形のAt/。23 and 3 from 2 to 1 (■) shaped semiconductor substrate.
If H11 is reached and charge (duplex) deficiency is generated by the element's conversion, will this happen? (i, the load is an N type 2F with a high potential spreading with 'i'
The conductor region 1 or 3 is effectively attracted) 1), and the higher 'ff, Ij, 7) 1) N1 type semiconductor region,
2 Z +/im gather I', ■] form ゛l'j,
'7: The dormant substrate // does not dissipate (7), therefore, each region: , l/, 22., ! The electric charge (electron) is P-type At/.
導体基体から活性領域、20に不要電子として入ること
が防1Jl−きノコ、ることCでなる。This prevents unnecessary electrons from entering the active region 20 from the conductive substrate.
なお、不発f4Jl]に係る固体撮像素子は、その半導
体及び各部分や半導体領域のj? ?lJ形が上述の例
に1jii%らハ、るものではない。In addition, the solid-state image sensing device related to the unexploded f4Jl is the j? ? The lJ type is not 1jiii% more similar to the above example.
発明の効果
以上の説明力・ら明らかな如く、本発明に係る固体撮像
素子によれば、活性領域の周囲に形成σれたチャンネル
・ストップ領域に光が入射することによシ発生する′m
荷か、半導体基体中足拡散していき活性領域に不要電荷
として入り込むことが防1トキノしるので、チャンネル
・ストソゲ領域への入射光による電荷が信号電荷に9;
1シて影響を及ぼ芒ないようにできることになり、常に
、ノイズ成分の少なる良ψIな撮像l”−1」力信号を
得ることができる。As is clear from the explanatory power that exceeds the effect of the invention, according to the solid-state imaging device according to the present invention, the phenomenon occurs when light enters the channel stop region formed around the active region.
This prevents the charge from diffusing into the semiconductor substrate and entering the active region as unnecessary charge, so that the charge due to the light incident on the channel/transmission region becomes the signal charge.
Therefore, it is possible to always obtain a good imaging l''-1'' force signal with less noise components.
そ(−で、活性領域の周囲に配σ)またチャンネル・ス
トップ領域への入射光による電荷の半導体基体中の拡散
防11−.孕すべく、斯かる電荷を集中せしめるにあた
り、チャンネル・ストップ領域中に、比較的太なる面積
をもって広がる、半導体基体とは異なる導1.TV、形
をもつ半導体領域と、それに隣接する、半導体基体とは
異なる導電1形をもつ、冒3イ・鈍物濃度の半導体領域
とが配式7’Lるので、チャンネル・ストップ領域への
入射光による電荷がこれら゛1′導体領域に極めて効果
的に吸引及び集中ぜし7め[゛っ)17、半導体基体中
の拡散防1Fが僅実ilこなσハ、る1、It also prevents the diffusion of charges in the semiconductor substrate due to light incident on the channel stop region 11-. In order to concentrate such charges, a conductor 1. which is different from the semiconductor body and which extends over a relatively large area in the channel stop region is used. Since the semiconductor region having the shape of the TV and the adjacent semiconductor region having the conductivity type 1 which is different from that of the semiconductor body and having the concentration of the 3I/object, have the structure 7'L, Charges caused by incident light are very effectively attracted and concentrated in these 1' conductor regions.
第1図はインクルライン転送型CC1つイ1(Fi像木
了の一例全示す槻略構I&1ツ]、第d図Aに第1図に
ろ−くσ′I″l、る撮像素子の1<1〜分を示す部分
拡大図、」、4図13(1第1図AのIf B−If
B ItC於ける断面図、第31ツ1に本発明νこ係る
固体撮像素子の−f+1.l ’r示す11!’J略構
らy図、第グ図Aは第3図のIV A−1〜jΔに於り
イ)断面図、第グじ113は第3図に水式29.る例の
!ml、’I l’+の弱、明に供さノしる図である。
図中、3(」受う℃・重i!″T転送部、11.(弓水
平11す、送部、汐は1/1力部、//はP形の4半〕
、り体フ1(体、ソθ何l占性領域5.2/及び2.2
はP形、′1′1体鎖1・題1.;;362N形半導体
領域1.2りはN形−′4LH,v、体領域である3゜
代理人 弁理士 神原1気昭、′、。Figure 1 shows an image sensor with an incl line transfer type CC (1 & 1 schematic structure showing all examples of Fi images), Figure dA shows an image sensor with σ'I''l as shown in Figure 1. 1<1 ~ minute enlarged partial view, 4 Figure 13 (1 If B-If of Figure 1 A)
B Cross-sectional view at ItC, -f+1. l'r show 11! 'J schematic diagram y, Figure A is a cross-sectional view of IV A-1 to jΔ in Figure 3, and Figure 113 is a water type 29. For example! ml, 'I l' + weak, clear diagram. In the figure, 3 ("receiving ° C / weight i!" T transfer part, 11. (bow horizontal 11, sending part, tide is 1/1 force part, // is 4 and a half of P type)]
, body f1 (body, so θ what l occupied area 5.2/and 2.2
is P-form, '1' 1-body chain 1・Problem 1. ;;362N-type semiconductor region 1.2 is the N-type-'4LH,v, body region 3゜Representative Patent attorney 1 Keiaki Kanbara,'.
Claims (1)
発生するとともに得らitた信号電荷を所定の電荷転送
方向をもって転送するようにを′I]、た活性領域が、
その周囲に第1の導電形孕もつ第1及び第一の半導体領
域を2重に伴って配置きれ、上記第1及び第一の半導体
領域の夫々の間に、第1の導電形とは異なる第一の導電
形をもつ第3の半導体領域及び該第3の半導体領域よシ
ネ鈍物濃度が高い第一の導電形をもつ第グの半導体領域
が、夫々、」二記第1及び第一の半導体領域に沿って配
ざノ1.て、上記第1.第a、第3及び第グの半導体領
域によりチャンネル・ストップ領域が形成さt″L、上
記第3及び第グの半導体領域には所定の電圧が印加てれ
るようにな式7″1.た固体撮像素子。An active region is formed on the semiconductor substrate of the first conductivity type to generate signal charges by receiving light and to transfer the obtained signal charges in a predetermined charge transfer direction.
First and first semiconductor regions having a first conductivity type are arranged in a double manner around the first conductivity type, and between each of the first and first semiconductor regions, a conductivity type different from the first conductivity type is arranged. A third semiconductor region having a first conductivity type and a third semiconductor region having a first conductivity type having a higher concentration of cine obtuse than the third semiconductor region, respectively. 1. 1. above. A channel stop region is formed by the a-th, third and g-th semiconductor regions t''L, and a predetermined voltage is applied to the third and g-th semiconductor regions according to formula 7''1. solid-state image sensor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58181465A JPS6074475A (en) | 1983-09-29 | 1983-09-29 | Solid state image pickup element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58181465A JPS6074475A (en) | 1983-09-29 | 1983-09-29 | Solid state image pickup element |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6074475A true JPS6074475A (en) | 1985-04-26 |
| JPH0527271B2 JPH0527271B2 (en) | 1993-04-20 |
Family
ID=16101226
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58181465A Granted JPS6074475A (en) | 1983-09-29 | 1983-09-29 | Solid state image pickup element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6074475A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62156858A (en) * | 1985-12-28 | 1987-07-11 | Matsushita Electronics Corp | solid-state imaging device |
| JPS63110668A (en) * | 1986-10-28 | 1988-05-16 | Toshiba Corp | Solid-state image sensing device |
| JP2007173390A (en) * | 2005-12-20 | 2007-07-05 | Fujifilm Corp | CCD type solid-state imaging device |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5632776A (en) * | 1979-08-23 | 1981-04-02 | Sanyo Electric Co Ltd | Ccd image sensor |
| JPS574162A (en) * | 1980-06-10 | 1982-01-09 | Sony Corp | Manufacture of charge transfer device |
| JPS5726971A (en) * | 1980-07-24 | 1982-02-13 | Sanyo Electric Co Ltd | Solidstate image sensor |
-
1983
- 1983-09-29 JP JP58181465A patent/JPS6074475A/en active Granted
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5632776A (en) * | 1979-08-23 | 1981-04-02 | Sanyo Electric Co Ltd | Ccd image sensor |
| JPS574162A (en) * | 1980-06-10 | 1982-01-09 | Sony Corp | Manufacture of charge transfer device |
| JPS5726971A (en) * | 1980-07-24 | 1982-02-13 | Sanyo Electric Co Ltd | Solidstate image sensor |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62156858A (en) * | 1985-12-28 | 1987-07-11 | Matsushita Electronics Corp | solid-state imaging device |
| JPS63110668A (en) * | 1986-10-28 | 1988-05-16 | Toshiba Corp | Solid-state image sensing device |
| JP2007173390A (en) * | 2005-12-20 | 2007-07-05 | Fujifilm Corp | CCD type solid-state imaging device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0527271B2 (en) | 1993-04-20 |
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