JPH01283870A - Charge transfer device - Google Patents

Charge transfer device

Info

Publication number
JPH01283870A
JPH01283870A JP11428488A JP11428488A JPH01283870A JP H01283870 A JPH01283870 A JP H01283870A JP 11428488 A JP11428488 A JP 11428488A JP 11428488 A JP11428488 A JP 11428488A JP H01283870 A JPH01283870 A JP H01283870A
Authority
JP
Japan
Prior art keywords
charge transfer
gate electrode
output
region
floating diffusion
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
Application number
JP11428488A
Other languages
Japanese (ja)
Inventor
Hiromasa Yamamoto
山本 裕將
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 JP11428488A priority Critical patent/JPH01283870A/en
Publication of JPH01283870A publication Critical patent/JPH01283870A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To reduce the total capacity of a floating diffused layer and to improve a signal detecting sensitivity by providing a low concentration region in the drain region of an output transistor having a gate electrode connected to the diffused layer. CONSTITUTION:The drain region of an output transistor 7 having a gate electrode 6 connected to a floating diffused layer 4 which receives charge through an output gate 3 from a charge transfer unit containing a plurality of charge transfer electrodes 2-1-2-6... provided through an insulating film on a P-type semiconductor substrate 1 is formed of a low concentration region 10 disposed near the electrode 6 and a high concentration region 11 provided adjacently thereto. In this transistor 7, a channel is formed at the time of source follower operation, and a depleted layer is extended in the drain region. In this case, since the depleted layer is extended toward the region 10, a capacity between the drain region and the gate electrode is reduced. Thus, an output signal voltage having high sensitivity can be obtained.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は電荷転送装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a charge transfer device.

〔従来の技術〕[Conventional technology]

電荷転送装置は、電気信号や入射光等の情報入力を電荷
の形で蓄積ししかもその電荷を多数の電荷転送用電極に
よって順次転送し、電気信号として増幅して取出すこと
ができることから、電荷転送装置を含む半導体装置は撮
像装置やメモリその他信号処理装置等に使用されている
Charge transfer devices accumulate information input such as electrical signals and incident light in the form of charges, and then sequentially transfer the charges using a large number of charge transfer electrodes, amplifying and extracting them as electrical signals. Semiconductor devices including such devices are used in imaging devices, memories, signal processing devices, and the like.

第2図は従来の電荷転送装置の一例の断面模式この従来
例は、第2図に示すように例えばP型半導体基板1の上
に絶縁膜8を介して設けられ、かつ3相のクロック信号
φ1.φ2及びφ3によって駆動される多数の電荷転送
用電極2−1〜2−6と、電荷転送用電極の最終段(2
−6)に近接したP型半導体基板1の上に絶縁膜を介し
て設けられかつ電位V2に固定された出力用ゲート3と
、転送されてきた電荷を電圧に変換するためのN型浮遊
拡散層4をソースとし、電位V1に固定されたN型不純
物層をドレイン、リセットクロック信号φRを印加され
るゲート電極を有するリセットトランジスタ5と、浮遊
拡散層4とゲート電極6を接続することによって内部電
荷を電圧信号として外部へ取り出すための出力トランジ
スタ7とで構成されている。
FIG. 2 is a schematic cross-sectional view of an example of a conventional charge transfer device. This conventional example is provided, for example, on a P-type semiconductor substrate 1 with an insulating film 8 interposed therebetween, as shown in FIG. φ1. A large number of charge transfer electrodes 2-1 to 2-6 driven by φ2 and φ3 and the final stage (2
-6) An output gate 3 provided through an insulating film on a P-type semiconductor substrate 1 in close proximity to the P-type semiconductor substrate 1 and fixed to a potential V2, and an N-type floating diffusion for converting transferred charges into voltage. By connecting the floating diffusion layer 4 and the gate electrode 6, a reset transistor 5 has the layer 4 as the source, the N-type impurity layer fixed at potential V1 as the drain, and the gate electrode to which the reset clock signal φR is applied. It is composed of an output transistor 7 for extracting charges to the outside as a voltage signal.

この従来例の駆動方法はまずリセットトランジスタ5を
オフ状態にして浮遊拡散層4の電位を電源の電位v1に
設定することによりリセットし、しかる後にリセットト
ランジスタ5をオフ状態にする。
In this conventional driving method, reset is performed by first turning off the reset transistor 5 and setting the potential of the floating diffusion layer 4 to the potential v1 of the power supply, and then turning off the reset transistor 5.

次に、3相のクロック信号φ1.φ2及びφ。Next, the three-phase clock signal φ1. φ2 and φ.

によって多数の電荷転送用電極2−1〜2−6を駆動し
て、各々の電荷転送電極下のP型半導体基板1の表面に
ポテンシャル井戸を生じさせ電荷信号を転送、最終段の
電荷転送用電極2−6直下のポテンシャル井戸に第3図
(a)に示すように溜める。
drives a large number of charge transfer electrodes 2-1 to 2-6 to generate potential wells on the surface of the P-type semiconductor substrate 1 under each charge transfer electrode to transfer charge signals, and for charge transfer in the final stage. The potential is stored in the potential well just below the electrode 2-6 as shown in FIG. 3(a).

続いて次のクロックタイミングの時にその電荷を電位V
2を印加した出力用ゲート3の下のP型半導体基板1の
表面を通って浮遊拡散層4へ第3図(b)に示すように
流し込む。
Then, at the next clock timing, the charge is changed to the potential V
It is poured into the floating diffusion layer 4 through the surface of the P-type semiconductor substrate 1 under the output gate 3 to which 2 is applied, as shown in FIG. 3(b).

この場合、転送されてきた電荷量をQとし、浮遊拡散層
4の全容量をCとすると、電荷が流入する前と後の浮遊
拡散層4の電位差△VはΔV=− と表わすことができる。
In this case, if the amount of charge transferred is Q and the total capacitance of the floating diffusion layer 4 is C, the potential difference ΔV between the floating diffusion layer 4 before and after the charge flows can be expressed as ΔV=-. .

従って、この電位差へVを出力トランジスタ7を介して
出力すれば、この従来例の半導体装置内に蓄積された情
報を読取ることができる。
Therefore, by outputting V to this potential difference through the output transistor 7, the information stored in this conventional semiconductor device can be read.

ここで浮遊拡散層部4の全容量Cとは、浮遊拡散層4と
P型半導体基板1との容量、浮遊拡散層4と出力用ゲー
ト3間の容量、浮遊拡散層4とゲート電極(φR)間の
容量、およびゲート電極6のゲート容量の和でほぼ決定
されるものである。
Here, the total capacitance C of the floating diffusion layer section 4 includes the capacitance between the floating diffusion layer 4 and the P-type semiconductor substrate 1, the capacitance between the floating diffusion layer 4 and the output gate 3, and the capacitance between the floating diffusion layer 4 and the gate electrode (φR ) and the sum of the gate capacitance of the gate electrode 6.

上述のゲート容量について出力トランジスタ7の部分を
第4図の断面模式図を用いて具体的に説明する。
Regarding the above-mentioned gate capacitance, the portion of the output transistor 7 will be specifically explained using the schematic cross-sectional view of FIG.

浮遊拡散層4と電気的に接続されたゲート電極6によっ
て作られる出力トランジスタ7は、ソースフォロワのト
ランジスタとして、ゲート電極電位の変化に応じて出力
信号電圧が変化するようにトランジスタの飽和領域が使
われているためゲート電極下のチャンネル部9は第4図
に示すようにゲート電極直下で切れている。このため、
ゲート容量は、V1電圧に固定されたドレインとゲート
電極間の容量および出力信号端子12と結ばれたソース
とゲート電極間の容量およびゲート電極とP型半導体基
板との容量に分けられる。
The output transistor 7 formed by the gate electrode 6 electrically connected to the floating diffusion layer 4 is used as a source follower transistor in which the saturation region of the transistor is used so that the output signal voltage changes according to changes in the gate electrode potential. Because of this, the channel portion 9 under the gate electrode is cut just below the gate electrode, as shown in FIG. For this reason,
The gate capacitance is divided into the capacitance between the drain and the gate electrode fixed at the V1 voltage, the capacitance between the source and the gate electrode connected to the output signal terminal 12, and the capacitance between the gate electrode and the P-type semiconductor substrate.

以上述べた浮遊拡散層の全容量Cによって、出力信号の
値が決定されることになる。すなわち高感度の信号出力
を得るには前述の浮遊拡散層の全容量Cを小さくする必
要がある。またこの浮遊拡散層容量は主に浮遊拡散層の
面積とゲート容量で大部分が決定されることから高感度
化には浮遊拡散層の面積の縮少およびゲート容量の低下
が必要となる。
The value of the output signal is determined by the total capacitance C of the floating diffusion layer described above. That is, in order to obtain a highly sensitive signal output, it is necessary to reduce the total capacitance C of the floating diffusion layer mentioned above. Furthermore, since the floating diffusion layer capacitance is largely determined by the area of the floating diffusion layer and the gate capacitance, it is necessary to reduce the area of the floating diffusion layer and lower the gate capacitance in order to increase sensitivity.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上述した従来の電荷転送装置では、信号電荷に対して高
感度な出力信号電圧を得るには浮遊拡散層の全容量Cを
小さくする必要があるが、浮遊拡散層の面積を縮少させ
るのも限界があり、ゲート容量も出力インピーダンスの
関係からトランジスタのサイズを小さくできないので、
高感度の信号出力ができないという欠点がある。
In the conventional charge transfer device described above, in order to obtain an output signal voltage that is highly sensitive to signal charges, it is necessary to reduce the total capacitance C of the floating diffusion layer, but it is also possible to reduce the area of the floating diffusion layer. There is a limit, and the size of the transistor cannot be reduced due to the gate capacitance and output impedance.
The drawback is that it cannot output highly sensitive signals.

〔課題を解決するための手段〕[Means to solve the problem]

本発明の電荷転送装置は、半導体基板上に絶縁膜を介し
て設けられた複数の電荷転送用電極を含む電荷転送部か
ら出力用ゲートを介して電荷を受取る浮遊拡散層に接続
されたゲート電極を有する出力トランジスタを含む電荷
転送装置において、前記出力トランジスタのドレイン領
域は前記ゲート電極寄りに配置された低濃度領域及びこ
れと隣接して設けられた高濃度領域からなるというもの
である。
The charge transfer device of the present invention has a gate electrode connected to a floating diffusion layer that receives charges via an output gate from a charge transfer section including a plurality of charge transfer electrodes provided on a semiconductor substrate via an insulating film. In the charge transfer device including an output transistor, the drain region of the output transistor is composed of a low concentration region disposed near the gate electrode and a high concentration region adjacent thereto.

〔実施例〕〔Example〕

次に、本発明の実施例について図面を参照して説明する
Next, embodiments of the present invention will be described with reference to the drawings.

第1図は本発明の一実施例の主要部を示す半導体チップ
の断面模式図であり、出力トランジスタ部を示したもの
であり、その他の部分は第2図と同じである。
FIG. 1 is a schematic cross-sectional view of a semiconductor chip showing the main parts of an embodiment of the present invention, showing an output transistor section, and other parts are the same as FIG. 2.

この実施例はP型半導体基板1上に絶縁膜を介して設け
られた複数の電荷転送用電極2−1〜2−6・・・を含
む電荷転送部から出力用ゲート3を介して電荷を受取る
浮遊拡散層4に接続されたゲート電極6を有する出力ト
ランジスタ7を含む電荷転送装置において、出力トラン
ジスタ7のドレイン領域はゲート電極6寄りに配置され
た低濃度領域10及びこれと隣接して設けられた高濃度
領域11からなるというものである。なお、13はソー
ス領域であり、高濃度領域11と同時に形成される。
In this embodiment, charges are transferred through an output gate 3 from a charge transfer section including a plurality of charge transfer electrodes 2-1 to 2-6 provided on a P-type semiconductor substrate 1 via an insulating film. In a charge transfer device including an output transistor 7 having a gate electrode 6 connected to a receiving floating diffusion layer 4, the drain region of the output transistor 7 includes a low concentration region 10 disposed near the gate electrode 6 and a low concentration region 10 disposed adjacent thereto. It consists of a high concentration region 11 with a high concentration. Note that 13 is a source region, which is formed at the same time as the high concentration region 11.

この出力トランジスタにおいて、第4図と同様のチャン
ネルがソースフォロワ動作時に形成され、また、ドレイ
ン領域では空乏層が広がる。この時、低度領域10が設
けられているので、空乏層が低濃度領域10の方向にも
伸びることからトレイン領域とゲート電極間の容量は従
来例に比較して小さくなる。
In this output transistor, a channel similar to that shown in FIG. 4 is formed during source follower operation, and a depletion layer expands in the drain region. At this time, since the low concentration region 10 is provided, the depletion layer also extends in the direction of the low concentration region 10, so that the capacitance between the train region and the gate electrode becomes smaller than in the conventional example.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明は、浮遊拡散層部の全容量を
小さくするため、浮遊拡散層部と接続したゲート電極を
有する出カドランジスのドレイン領域に低濃度領域を設
けることにより、浮遊拡散層部の全容量を小さくして、
信号検出感度を改善できる効果がある。
As explained above, in order to reduce the total capacitance of the floating diffusion layer, the present invention provides a low concentration region in the drain region of the output transistor having the gate electrode connected to the floating diffusion layer. By reducing the total capacity of
This has the effect of improving signal detection sensitivity.

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

第1図は本発明の一実施例の主要部を示す半導体チップ
の断面模式図、第2図は電荷転送装置の断面模式図、第
3図(a)、(b)は電荷転送装置の動作を説明するた
めのポテンシャル推移図、第4図は従来例の主要部を示
す断面模式図である。 1・・・P型半導体基板、2−1〜2−6・・・電荷転
送用電極、3・・・出力用ゲート、4・・・浮遊拡散層
、5・・・リセットトランジスタ、6・・・ゲート電極
、7・・・出力トランジスタ、8・・・絶縁膜、9・・
・チャンネル部、10・・・低濃度領域、11・・・高
濃度領域、12・・・出力信号端子、13・・・ソース
領域。
FIG. 1 is a schematic cross-sectional view of a semiconductor chip showing the main parts of an embodiment of the present invention, FIG. 2 is a schematic cross-sectional view of a charge transfer device, and FIGS. 3(a) and (b) are operations of the charge transfer device. FIG. 4 is a schematic cross-sectional view showing the main parts of a conventional example. DESCRIPTION OF SYMBOLS 1... P-type semiconductor substrate, 2-1 to 2-6... Electrode for charge transfer, 3... Gate for output, 4... Floating diffusion layer, 5... Reset transistor, 6...・Gate electrode, 7... Output transistor, 8... Insulating film, 9...
- Channel portion, 10...Low concentration region, 11...High concentration region, 12...Output signal terminal, 13... Source region.

Claims (1)

【特許請求の範囲】[Claims]  半導体基板上に絶縁膜を介して設けられた複数の電荷
転送用電極を含む電荷転送部から出力用ゲートを介して
電荷を受取る浮遊拡散層に接続されたゲート電極を有す
る出力トランジスタを含む電荷転送装置において、前記
出力トランジスタのドレイン領域は前記ゲート電極寄り
に配置された低濃度領域及びこれと隣接して設けられた
高濃度領域からなることを特徴とする電荷転送装置。
A charge transfer unit including an output transistor having a gate electrode connected to a floating diffusion layer that receives charges via an output gate from a charge transfer unit including a plurality of charge transfer electrodes provided on a semiconductor substrate via an insulating film. A charge transfer device, wherein the drain region of the output transistor comprises a low concentration region disposed near the gate electrode and a high concentration region adjacent thereto.
JP11428488A 1988-05-10 1988-05-10 Charge transfer device Pending JPH01283870A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11428488A JPH01283870A (en) 1988-05-10 1988-05-10 Charge transfer device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11428488A JPH01283870A (en) 1988-05-10 1988-05-10 Charge transfer device

Publications (1)

Publication Number Publication Date
JPH01283870A true JPH01283870A (en) 1989-11-15

Family

ID=14633987

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11428488A Pending JPH01283870A (en) 1988-05-10 1988-05-10 Charge transfer device

Country Status (1)

Country Link
JP (1) JPH01283870A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5357129A (en) * 1992-12-28 1994-10-18 Sharp Kabushiki Kaisha Solid state imaging device having high-sensitivity and low-noise characteristics by reducing electrostatic capacity of interconnection
FR2704095A1 (en) * 1993-04-13 1994-10-21 Samsung Electronics Co Ltd Charge coupled device type image sensor.

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5357129A (en) * 1992-12-28 1994-10-18 Sharp Kabushiki Kaisha Solid state imaging device having high-sensitivity and low-noise characteristics by reducing electrostatic capacity of interconnection
FR2704095A1 (en) * 1993-04-13 1994-10-21 Samsung Electronics Co Ltd Charge coupled device type image sensor.

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