JPH0834568B2 - Driving method for solid-state imaging device - Google Patents

Driving method for solid-state imaging device

Info

Publication number
JPH0834568B2
JPH0834568B2 JP63095881A JP9588188A JPH0834568B2 JP H0834568 B2 JPH0834568 B2 JP H0834568B2 JP 63095881 A JP63095881 A JP 63095881A JP 9588188 A JP9588188 A JP 9588188A JP H0834568 B2 JPH0834568 B2 JP H0834568B2
Authority
JP
Japan
Prior art keywords
image pickup
solid
region
pickup unit
photocharges
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 - Fee Related
Application number
JP63095881A
Other languages
Japanese (ja)
Other versions
JPH01268269A (en
Inventor
裕二 北村
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.)
Sanyo Denki Co Ltd
Original Assignee
Sanyo Denki Co Ltd
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 Sanyo Denki Co Ltd filed Critical Sanyo Denki Co Ltd
Priority to JP63095881A priority Critical patent/JPH0834568B2/en
Publication of JPH01268269A publication Critical patent/JPH01268269A/en
Publication of JPH0834568B2 publication Critical patent/JPH0834568B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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

Description

【発明の詳細な説明】 (イ)産業上の利用分野 本発明は、縦型オーバーフロードレイン方式のCCD固
体撮像装置の駆動方法に関する。
TECHNICAL FIELD The present invention relates to a driving method of a vertical overflow drain type CCD solid-state imaging device.

(ロ)従来の技術 第3図は、縦型オーバーフロードレイン方式のCCD固
体撮像装置の断面図である。N型のSi基板(4)の一方
の面には、P−Well領域(1)が形成され、その受光部
分にはN+型の拡散領域(7)が形成される。そして、P
−Well領域(1)上に絶縁膜(2)を介して蓄積ゲート
電極(6)と転送電極(3)とが形成され、光電荷の蓄
積を制御する制御パルスφcと、光電荷を転送する駆動
パルスφtとが夫々印加される。また、Si基板(4)の
他方の面には裏面電極(5)が形成される。このような
縦型オーバーフロードレイン構造のCCD固体撮像装置
は、例えば特開昭59−19480号公報に開示されている。
(B) Prior Art FIG. 3 is a cross-sectional view of a vertical overflow drain type CCD solid-state imaging device. A P-Well region (1) is formed on one surface of the N type Si substrate (4), and an N + type diffusion region (7) is formed in the light receiving portion thereof. And P
-A storage gate electrode (6) and a transfer electrode (3) are formed on the well region (1) through an insulating film (2), and a control pulse φ c for controlling the accumulation of photocharges and the photocharges are transferred. Drive pulses φ t are applied respectively. Further, a back surface electrode (5) is formed on the other surface of the Si substrate (4). A CCD solid-state image pickup device having such a vertical overflow drain structure is disclosed in, for example, Japanese Patent Application Laid-Open No. 59-19480.

CCD固体撮像装置の電荷の蓄積期間は、通常1/60秒に
設定され、斯る状態に於いて静止画を得る場合には、シ
ャッタ速度は1/60秒となる。このシャッタ速度をさらに
速くするためには、電荷の蓄積期間を短くすることが必
要であり、その方法(電子シャッタ)が、例えば日経マ
イクロデバイス1987年10月号P60〜P67に記載されてい
る。この電子シャッタ機能は、撮像部のチャンネルに蓄
積される光電荷を蓄積期間中所望の期間に基板へ掃出さ
せ、残りの期間で電荷をチャンネルに蓄積するように構
成される。例えば、1/60秒の蓄積期間のうち2/3の期間
に電荷をチャンネルから外部に掃出し、残りの1/3の期
間に電荷を蓄積すれば1/180秒のシャッタ速度が得られ
る。第3図に示すような縦型オーバーフロードレイン方
式のCCD固体撮像装置では、裏面電極(5)に印加され
る電圧VSの制御に依って上述の電荷の掃出し動作が行わ
れる。通常、電荷の蓄積時及び転送時には、裏面電極
(5)に一定レベルの電圧VSが印加されているが、この
電圧VSをあるレベル以上にすると、撮像部に発生した光
電荷が全てSi基板(4)に流れ、撮像部には光電荷が蓄
積されなくなる。そこで、所望の期間中裏面電極(5)
に電荷掃出し用のパルスφsが印加されて撮像部に発生
する光電荷が掃出される。
The charge accumulation period of the CCD solid-state image pickup device is usually set to 1/60 second, and when obtaining a still image in such a state, the shutter speed is 1/60 second. In order to further increase the shutter speed, it is necessary to shorten the charge accumulation period, and the method (electronic shutter) is described in, for example, Nikkei Microdevice October 1987 issue P60 to P67. This electronic shutter function is configured to sweep the photocharges accumulated in the channel of the image pickup unit to the substrate for a desired period during the accumulation period and accumulate the charges in the channel for the remaining period. For example, if the charge is swept out of the channel in the 2/3 period of the 1/60 second accumulation period and the charge is accumulated in the remaining 1/3 period, the shutter speed of 1/180 second is obtained. In the vertical overflow drain type CCD solid-state imaging device as shown in FIG. 3, the above-mentioned charge sweeping operation is performed by controlling the voltage V S applied to the back surface electrode (5). Normally, a voltage V S of a constant level is applied to the back surface electrode (5) at the time of storing and transferring charges, but if this voltage V S is set to a certain level or higher, all the photo-charges generated in the imaging unit are Si. It flows to the substrate (4), and photocharges are no longer accumulated in the imaging section. Therefore, the back surface electrode (5) for a desired period
The pulse φ s for sweeping out the electric charges is applied to the photo electric charges to sweep out the photo electric charges generated in the imaging unit.

第4図は、第3図のX−X′線に於けるポテンシャル
分布を示す図であり、Aは電荷の蓄積時、Bは電子シャ
ッタ動作時を示す。蓄積時には、転送電極(3)及びゲ
ート電極(6)に印加する駆動パルスφt及びφcが拡散
領域(7)とP−Well領域(1)間の閾値以下のレベル
で駆動され、裏面電極(5)に一定の電圧VSが印加され
て第3図に波線で示すようにポテンシャル井戸(10)が
形成される。ここで、電圧VSが高くなる(パルスφs
印加される)と、裏面電極(5)近傍のポテンシャルが
さらに深くなり、撮像部に発生する光電荷がSi基板
(4)に流れ易くなる。従って、この電圧VSをある値以
上に設定すれば、撮像部のチャンネルには光電荷が蓄積
されず、掃出し動作が行われる。
FIG. 4 is a diagram showing the potential distribution along the line XX ′ in FIG. 3, where A is the charge accumulation and B is the electronic shutter operation. During storage, the drive pulses φ t and φ c applied to the transfer electrode (3) and the gate electrode (6) are driven at a level below the threshold value between the diffusion region (7) and the P-Well region (1), and the back electrode A constant voltage V S is applied to (5) to form a potential well (10) as shown by the broken line in FIG. Here, when the voltage V S becomes higher (the pulse φ s is applied), the potential in the vicinity of the back surface electrode (5) becomes deeper, and the photocharges generated in the imaging section easily flow to the Si substrate (4). . Therefore, if this voltage V S is set to a certain value or higher, the photocharge is not accumulated in the channel of the image pickup section, and the sweep operation is performed.

(ハ)発明が解決しようとする課題 しかしながら、裏面電極(5)に印加される電圧V
Sは、装置の裏面全体に亘って略均一に印加されるた
め、この電圧VSを高くすると、撮像部以外の領域、例え
ば垂直転送部等に於いてもチャンネルからSi基板(4)
に光電荷が流れ易くなり、素子特性の劣化や、信頼性の
低下を招く虞れがある。
(C) Problems to be Solved by the Invention However, the voltage V applied to the back surface electrode (5) is
Since S is applied substantially uniformly over the entire back surface of the device, if the voltage V S is increased, the Si substrate (4) is also removed from the channel even in a region other than the imaging unit, for example, in the vertical transfer unit.
There is a possibility that photocharges easily flow into the device, resulting in deterioration of device characteristics and deterioration of reliability.

(ニ)課題を解決するための手段 本発明は、上述の問題点を解決するためになされたも
ので、一導電型の半導体基板の一方の面に絶縁膜を介し
て転送電極が形成され、他方の面に逆導電型のオーバー
フロー領域が形成される縦型オーバーフロードレイン方
式のCCDを用いた固体撮像装置の駆動方法に於いて、撮
像部の転送電極にその他の領域の転送電極よりも低レベ
ルの駆動パルスを印加し、撮像部の転送電極の下に発生
する光電荷を上記半導体基板に掃出せしめることを特徴
とする。
(D) Means for Solving the Problems The present invention has been made to solve the above-mentioned problems, and a transfer electrode is formed on one surface of a semiconductor substrate of one conductivity type via an insulating film, In a method of driving a solid-state image pickup device using a vertical overflow drain type CCD in which an overflow region of the opposite conductivity type is formed on the other surface, the transfer electrode of the image pickup unit has a lower level than the transfer electrodes of other regions. Is applied to drive the photocharge generated under the transfer electrode of the image pickup section to the semiconductor substrate.

(ホ)作用 本発明に依れば、撮像部の転送電極にその他の領域の
転送電極より低レベルの駆動パルスを印加することで撮
像部のみの転送電極近傍のポテンシャルを浅くさせ撮像
部の転送電極の下に発生する光電荷のみをオーバーフロ
ー領域に効率良く掃出させることができ、撮像部以外の
領域に於いて裏面電極近傍のポテンシャルが深くなるこ
とがなくなるため、撮像部以外の領域からオーバーフロ
ー領域に光電荷が流れることがなくなる。
(E) Action According to the present invention, by applying a drive pulse of a lower level to the transfer electrodes of the image pickup unit than the transfer electrodes of other regions, the potential near the transfer electrodes of only the image pickup unit is made shallow and the transfer of the image pickup unit is performed. Only the photocharges generated under the electrodes can be swept out to the overflow area efficiently, and the potential near the back surface electrode does not become deeper in the area other than the imaging section, so that the overflow from the area other than the imaging section does not occur. The photocharge does not flow to the area.

(ヘ)実施例 本発明の一実施例を図面に従って説明する。(F) Embodiment An embodiment of the present invention will be described with reference to the drawings.

第1図は、本発明の駆動方法を説明するための装置断
面図である。N+型のSi基板(4)の一方の面にはP−We
ll領域(1)が形成され、さらに絶縁膜(2)を介して
転送電極(3a)〜(3d)が形成される。また、Si基板
(4)の他方の面には裏面電極(5)が形成される。本
発明駆動方法の特徴とするところは、電子シャッタ動作
時に撮像部の転送電極(3a)〜(3d)に印加される駆動
パルスφ1〜φ4を夫々低レベルに固定するところにあ
る。
FIG. 1 is a sectional view of a device for explaining the driving method of the present invention. On one surface of the N + type Si substrate (4), P-We
ll region (1) is formed, and further transfer electrodes (3a) to (3d) are formed via the insulating film (2). Further, a back surface electrode (5) is formed on the other surface of the Si substrate (4). A feature of the driving method of the present invention is that the driving pulses φ 1 to φ 4 applied to the transfer electrodes (3a) to (3d) of the image pickup unit are fixed to low levels during the operation of the electronic shutter.

即ち、電子シャッタ動作時に於いても裏面電極(5)
には電圧VSのみが印加され、転送電極(3a)〜(3d)に
印加される駆動パルスφ1〜φ4がVSと同等或いはVSより
僅かに高いレベルに固定される。駆動パルスφ1〜φ4
VSと同等のレベルに固定されると、Si基板(1)中に形
成されるポテンシャル井戸(10)は、第1図に示すよう
に、深さが極めて浅くなるか、或いはポテンシャル井戸
(10)が形成されず、光電荷が蓄積されなくなる。
That is, even when the electronic shutter is operating, the back surface electrode (5)
Only voltage V S is applied, the drive pulse phi 1 to [phi] 4 is applied to the transfer electrodes (3a) ~ (3d) is secured to a slightly higher level than V S equal to or V S to. Drive pulses φ 1 to φ 4
When fixed at a level equivalent to V S , the potential well (10) formed in the Si substrate (1) becomes extremely shallow as shown in FIG. ) Is not formed and photocharges are not accumulated.

第2図は、第1図のX−X′線断面に於けるポテンシ
ャル分布を示す図で、A′は電荷の蓄積時、B′は電子
シャッタ動作時を示す。蓄積時には、従来と同様に裏面
電極(5)に電圧VSが印加されて駆動パルスφ1〜φ4
固定され、第4図Aと同様のポテンシャルの分布を示
す。ここで、駆動パルスφ1〜φ4を低レベルに固定する
と、絶縁膜(2)近傍のポテンシャルが浅くなり、転送
電極(3a)〜(3d)の下には光電荷が蓄積されにくくな
る。従って、駆動パルスを一定のレベル以下に設定すれ
ば、撮像部の転送電極(3a)〜(3d)の下のP−Well領
域(1)内に発生する光電荷が全てSi基板(4)に掃出
される。
FIG. 2 is a diagram showing a potential distribution in a cross section taken along the line XX 'in FIG. 1, where A'indicates charge accumulation and B'indicates an electronic shutter operation. During storage, the drive pulses conventional voltage V S to the back electrode (5) in the same manner is applied phi 1 to [phi] 4 is fixed, the distribution of the same potential and Figure 4 A. Here, if the drive pulses φ 1 to φ 4 are fixed at a low level, the potential in the vicinity of the insulating film (2) becomes shallow and it becomes difficult for photocharges to be accumulated under the transfer electrodes (3a) to (3d). Therefore, if the drive pulse is set to a certain level or less, all the photocharges generated in the P-Well region (1) under the transfer electrodes (3a) to (3d) of the image pickup unit are transferred to the Si substrate (4). Swept out.

斯る駆動方法では、撮像部のみで光電荷をSi基板
(4)へ流れ易くすることができるため、撮像部以外の
垂直転送部や蓄積部等で光電荷がSi基板(4)へ流れる
のを防止できる。
In such a driving method, the photocharges can easily flow to the Si substrate (4) only by the imaging unit, so that the photocharges flow to the Si substrate (4) at the vertical transfer unit and the storage unit other than the imaging unit. Can be prevented.

(ト)発明の効果 本発明に依れば、電子シャッター動作時に撮像部に発
生する光電荷を効率良くオーバーフロー領域に掃出させ
ることができると共に、撮像部以外の領域からオーバー
フロー領域に光電荷が流れることがなくなり、素子特性
を向上でき信頼性を高めることができる。
(G) Effect of the Invention According to the present invention, it is possible to efficiently sweep out photocharges generated in the image pickup unit during the operation of the electronic shutter to the overflow region, and at the same time, to prevent photocharges from the region other than the image pickup unit in the overflow region. It can be prevented from flowing, the device characteristics can be improved, and the reliability can be improved.

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

第1図は本発明の駆動方法を説明するためのCCD固体撮
像装置の断面図、第2図は第1図のX−X′線断面図に
於けるポテンシャルの分布を示す図、第3図は従来の駆
動方法を説明するためのCCD固体撮像装置の断面図、第
4図は第3図のX−X′線断面に於けるポテンシャルの
分布を示す図である。 (1)…チャンネル領域、(3a)〜(3d)…転送電極、
(4)…Si基板、(5)…裏面電極、(10)…ポテンシ
ャル井戸。
FIG. 1 is a sectional view of a CCD solid-state image pickup device for explaining a driving method of the present invention, FIG. 2 is a diagram showing potential distribution in a sectional view taken along line XX ′ of FIG. 1, and FIG. FIG. 4 is a sectional view of a CCD solid-state imaging device for explaining a conventional driving method, and FIG. 4 is a diagram showing a potential distribution in a section taken along line XX ′ of FIG. (1) ... Channel region, (3a) to (3d) ... Transfer electrode,
(4) ... Si substrate, (5) ... Back electrode, (10) ... Potential well.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】一導電型の半導体基板の一方の面に逆導電
型の拡散領域が形成され、この拡散領域上に絶縁膜を介
して複数の転送電極が形成される縦型オーバーフロード
レイン方式のCCDを用いた固体撮像装置の駆動方法に於
いて、撮像部の転送電極に、撮像部以外の領域の転送電
極よりも低レベルの駆動パルスを印加し、撮像部の転送
電極の下の上記拡散領域内に発生する光電荷を上記半導
体基板に掃出せしめることを特徴とする固体撮像装置の
駆動方法。
1. A vertical overflow drain system in which a diffusion region of opposite conductivity type is formed on one surface of a semiconductor substrate of one conductivity type, and a plurality of transfer electrodes are formed on the diffusion region via an insulating film. In a method of driving a solid-state image pickup device using a CCD, a drive pulse of a lower level than that of a transfer electrode in a region other than the image pickup unit is applied to the transfer electrode of the image pickup unit, and the diffusion under the transfer electrode of the image pickup unit is applied. A method for driving a solid-state imaging device, characterized in that photocharges generated in a region are swept out to the semiconductor substrate.
JP63095881A 1988-04-19 1988-04-19 Driving method for solid-state imaging device Expired - Fee Related JPH0834568B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63095881A JPH0834568B2 (en) 1988-04-19 1988-04-19 Driving method for solid-state imaging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63095881A JPH0834568B2 (en) 1988-04-19 1988-04-19 Driving method for solid-state imaging device

Publications (2)

Publication Number Publication Date
JPH01268269A JPH01268269A (en) 1989-10-25
JPH0834568B2 true JPH0834568B2 (en) 1996-03-29

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Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JPH0834568B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR930008527B1 (en) * 1990-10-13 1993-09-09 금성일렉트론 주식회사 Solid state image of the vccd structure

Also Published As

Publication number Publication date
JPH01268269A (en) 1989-10-25

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