Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH079982B2 - Charge transfer device - Google Patents
[go: Go Back, main page]

JPH079982B2 - Charge transfer device - Google Patents

Charge transfer device

Info

Publication number
JPH079982B2
JPH079982B2 JP60024858A JP2485885A JPH079982B2 JP H079982 B2 JPH079982 B2 JP H079982B2 JP 60024858 A JP60024858 A JP 60024858A JP 2485885 A JP2485885 A JP 2485885A JP H079982 B2 JPH079982 B2 JP H079982B2
Authority
JP
Japan
Prior art keywords
gate
region
regions
charge transfer
electrode
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 - Lifetime
Application number
JP60024858A
Other languages
Japanese (ja)
Other versions
JPS61184876A (en
Inventor
博司 大石
Original Assignee
松下電子工業株式会社
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 松下電子工業株式会社 filed Critical 松下電子工業株式会社
Priority to JP60024858A priority Critical patent/JPH079982B2/en
Publication of JPS61184876A publication Critical patent/JPS61184876A/en
Publication of JPH079982B2 publication Critical patent/JPH079982B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D44/00Charge transfer devices
    • H10D44/40Charge-coupled devices [CCD]
    • H10D44/45Charge-coupled devices [CCD] having field effect produced by insulated gate electrodes 
    • H10D44/462Buried-channel CCD

Landscapes

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

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、優れた高速動作特性を得ることができる電荷
転送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 a charge transfer device capable of obtaining excellent high speed operation characteristics.

従来の技術 従来の電荷転送装置は、第2図Aに示すような構造が代
表的なものである。この構造では、2層の多結晶シリコ
ンゲート1,2下に埋め込みチャンネルの領域7,10が形成
されている。また、埋め込みチャンネルの不純物濃度は
領域7の方が同10よりも大きくなっている。従って、多
結晶シリコンゲート1は信号電荷の蓄積ゲート、多結晶
シリコンゲート2は転送のためのバリヤゲートとなって
いる。なお、図中、8はシリコン基板、11はゲート酸化
膜である。
2. Description of the Related Art A conventional charge transfer device has a typical structure as shown in FIG. 2A. In this structure, buried channel regions 7 and 10 are formed below the two layers of polycrystalline silicon gates 1 and 2. Further, the impurity concentration of the buried channel is higher in the region 7 than in the region 10. Therefore, the polycrystalline silicon gate 1 serves as a signal charge storage gate, and the polycrystalline silicon gate 2 serves as a transfer gate. In the figure, 8 is a silicon substrate and 11 is a gate oxide film.

この従来構造の場合の電荷転送の説明を、第2図B,Cの
ポテンシャルモデル図により行う。第2図B,第2図C、
はゲート下のポテンシャルの状態を示すもので、寸法・
位置は第2図Aと対応している。第2図Bは、電極3に
印加されるパルスφ1がハイレベル(以下、“H")、電
極4に印加されるパルスφ2がロウレベル(以下、
“L")の場合を示すもので、電極3の多結晶シリコンゲ
ート1の第1ゲート下に信号電荷9が蓄積されている。
第2図Cにおいては、パルスが次のタイミングになり、
電極3のパルスφ1が“L",電極4のパルスφ2が“H"と
なり、ポテンシャルの状態から信号電荷9が図面におい
て右側の電極4に転送されているのがわかる。
The charge transfer in the case of this conventional structure will be described with reference to the potential model diagrams of FIGS. 2B and 2C. 2B, 2C,
Indicates the state of the potential under the gate.
The position corresponds to FIG. 2A. In FIG. 2B, the pulse φ 1 applied to the electrode 3 is at a high level (hereinafter “H”), and the pulse φ 2 applied to the electrode 4 is at a low level (hereinafter, “H”).
In the case of "L", the signal charge 9 is accumulated under the first gate of the polycrystalline silicon gate 1 of the electrode 3.
In FIG. 2C, the pulse becomes the next timing,
The pulse φ 1 of the electrode 3 becomes “L”, the pulse φ 2 of the electrode 4 becomes “H”, and it can be seen from the potential state that the signal charge 9 is transferred to the electrode 4 on the right side in the drawing.

このように、第2図は2層多結晶シリコンゲート、埋め
込みチャンネル部が蓄積部とバリヤ部とに別かれた構造
を持つ従来の電荷転送部を示し、2相の逆位相のパルス
により駆動される。(参考文献:電荷転送デバイス(近
代科学社)武石喜幸,香山普訳PP22〜27) 発明が解決しようとする問題点 近年、一次元固体撮像素子を複数個配列し、被写体ある
いは紙面原稿と同じサイズにした密着型のイメージセン
サの開発が行われている。この場合、従来のレンズを使
用したタイプの一次元固体撮像素子に比べ、一画素のサ
イズが大きくなり、それに伴い電荷転送部の一段当りの
ゲート長も大きくなる。そのため、フリンジングフィー
ルド効果が小さくなり転送効率が下がることになり、特
に高速動作時においてイメージセンサとしての機能が低
下する。
As described above, FIG. 2 shows a conventional charge transfer portion having a structure in which a buried layer portion is divided into a storage portion and a barrier portion, which is driven by two-phase antiphase pulses. It (Reference: Charge Transfer Device (Modern Science Co., Ltd.) Yoshiyuki Takeishi, Hiroshi Kayama PP22-27) Problems to be Solved by the Invention In recent years, a plurality of one-dimensional solid-state image pickup devices are arrayed to have the same size as a subject or a document on paper. A contact image sensor has been developed. In this case, the size of one pixel is larger than that of a conventional one-dimensional solid-state imaging device using a lens, and accordingly, the gate length per stage of the charge transfer unit is also large. Therefore, the fringing field effect is reduced and the transfer efficiency is lowered, and the function as the image sensor is deteriorated especially at high speed operation.

問題点を解決するための手段 本発明は上記問題点に鑑み、埋め込みチャンネル部が、
基板と反対の導電形を有し、互いに濃度の異なる3つの
領域からなり、前記領域が直列に配置され、さらに最も
濃度の高い領域の上部には第1のゲート電極が形成さ
れ、他の2つの領域の上部には第2のゲート電極が形成
され、前記濃度の異なる他の2つの領域のなかで濃度の
高い方の領域は、前記第1のゲート電極下の最も濃度の
高い領域に近接しており、第1のゲート電極と第2のゲ
ート電極は共通接続されてクロックパルス印加電極に接
続されるものである。
Means for Solving the Problems In view of the above problems, the present invention provides an embedded channel unit,
The region has three opposite conductivity types to the substrate and has different concentrations, the regions are arranged in series, and the first gate electrode is formed on the highest concentration region, and the other two regions are formed. A second gate electrode is formed on one of the two regions, and the region having the higher concentration of the other two regions having different concentrations is adjacent to the region having the highest concentration under the first gate electrode. Therefore, the first gate electrode and the second gate electrode are commonly connected and connected to the clock pulse applying electrode.

作用 この発明により、高転送効率の密着型イメージセンサが
実現できる。
Action According to the present invention, a contact image sensor with high transfer efficiency can be realized.

実施例 本発明による電荷転送部の断面図を第1図Aに、電荷転
送のポテンシャルプロファイルを第1図B,Cに示す。第
1図Aでは、従来例の構造と同じく2層の多結晶シリコ
ンゲート、埋め込みチャンネル部を持つが、第2のゲー
ト長が第1の倍となっている点と埋め込みチャンネル部
が互いに濃度の異なる3つの領域に分かれる点が従来構
造と異なる。第1図Aでは、1が第1のゲートの多結晶
シリコンゲート、2が第2のゲートの多結晶シリコンゲ
ート、5,6,7は埋め込みチャンネル領域で不純物の濃度
は7,6,5の順に大きくなっている。また、埋め込みチャ
ンネル領域5,6の各領域は第2のゲートである多結晶シ
リコンゲート2下に形成され、領域7は従来通り第1の
ゲートの多結晶シリコンゲート下1に形成されている。
なお、埋め込みチャンネル領域5,6,7の各領域は同一寸
法であり、従って第2ゲート長は第1ゲート長の倍にな
っている。8はシリコン基板、11はゲート酸化膜であ
る。電極3と電極4を合わせた領域が電荷転送の一段に
相当する。
EXAMPLE FIG. 1A shows a sectional view of a charge transfer portion according to the present invention, and FIGS. 1B and 1C show potential profiles of charge transfer. In FIG. 1A, the structure has a two-layer polycrystalline silicon gate and a buried channel portion as in the structure of the conventional example, but the second gate length is the first times and the buried channel portion has a concentration different from each other. It is different from the conventional structure in that it is divided into three different regions. In FIG. 1A, 1 is a polycrystal silicon gate of the first gate, 2 is a polycrystal silicon gate of the second gate, 5, 6, and 7 are buried channel regions, and the impurity concentration is 7, 6, 5 It is getting bigger in order. Each of the buried channel regions 5 and 6 is formed under the polycrystalline silicon gate 2 which is the second gate, and the region 7 is formed under the polycrystalline silicon gate 1 of the first gate as in the conventional case.
The buried channel regions 5, 6, and 7 have the same size, and therefore the second gate length is twice the first gate length. Reference numeral 8 is a silicon substrate, and 11 is a gate oxide film. The region where the electrodes 3 and 4 are combined corresponds to one stage of charge transfer.

本発明による構造の電荷転送部での電荷転送を、第1図
B,Cにより説明する。従来例と同様に2相のクロックパ
ルスφ1,φ2で駆動され、第1図Bでは、電極3に印加
されるパルスφ1が“H"電極4に印加されるパルスφ2
“L"である時のポテンシャルプロファイルを示し、電極
3下の埋め込みチャンネル領域6,7に信号電荷9が蓄積
されている。次のタイミングでのポテンシャルプロファ
イルを第1図Cでは示しており、電極3にはパルスφ1
が“L",電極4にはパルスφ2が“H"で印加されている。
第1図Cでは信号電荷9が、電極4下の埋め込みチャン
ネル領域6,7に蓄積されており、図面上、右側に電荷が
転送されている。従来例のポテンシャルプロファイルに
比べ、ゲート領域が細分化された分、ポテンシャルも細
分化され、転送がスムーズに行われる。通常、転送速度
はゲート長の2乗に反比例するとされており、本発明の
構造によりゲート領域を細分化することにより、高い転
送効率が得られ、高速動作時に有利なものとなる。
The charge transfer in the charge transfer portion having the structure according to the present invention is shown in FIG.
This will be explained using B and C. It is driven by two-phase clock pulses φ 1 and φ 2 as in the conventional example. In FIG. 1B, the pulse φ 1 applied to the electrode 3 is “H” and the pulse φ 2 applied to the electrode 4 is “L”. , The signal profile 9 is stored in the buried channel regions 6 and 7 below the electrode 3. The potential profile at the next timing is shown in FIG. 1C, and the pulse φ 1 is applied to the electrode 3.
Is “L”, and the pulse φ 2 is applied to the electrode 4 at “H”.
In FIG. 1C, the signal charge 9 is accumulated in the buried channel regions 6 and 7 below the electrode 4, and the charge is transferred to the right side in the drawing. Compared with the potential profile of the conventional example, the potential is also subdivided by the amount of subdivision of the gate region, and the transfer is performed smoothly. Generally, the transfer rate is said to be inversely proportional to the square of the gate length. By subdividing the gate region by the structure of the present invention, high transfer efficiency can be obtained, which is advantageous at high speed operation.

本発明の実施例は第1図Aに示した通り、埋め込みチャ
ンネル部を互いに濃度の異なる3つの領域に分け、2層
の多結晶シリコンゲート構造を持つ電荷転送部により構
成される。製造方法としては、第2のゲートの多結晶シ
リコンゲート2の形成直前に、埋め込みチャンネル領域
5,6に同一種、同一ドーズ量のイオン注入を2回実施
し、しかも、フォトレジスト膜をパターニングすること
により、1回した注入されない埋め込みチャンネル領域
5と2回とも注入される埋め込みチャンネル領域6とに
分け、濃度差を設ける。また、それぞれの領域の寸法
も、フォトレジスト膜のパターニングにより決定され
る。それ以外の製造方法は、従来例の構造と全く変りな
い方法で実施できる。
As shown in FIG. 1A, the embodiment of the present invention divides the buried channel portion into three regions having different concentrations, and is composed of a charge transfer portion having a two-layer polycrystalline silicon gate structure. As a manufacturing method, a buried channel region is formed immediately before the formation of the polycrystalline silicon gate 2 of the second gate.
By implanting ions 5 and 6 with the same species and the same dose twice, and by patterning the photoresist film, the buried channel region 5 that is not implanted once and the buried channel region 6 that is implanted twice are formed. And the difference in concentration is provided. Further, the size of each region is also determined by patterning the photoresist film. The other manufacturing method can be carried out by a method which is completely the same as the conventional structure.

発明の効果 本発明は、1ゲート長の寸法が大きくなる密着型の一次
元の固体撮像素子において、ゲート領域を細分化によ
り、高い転送効率を得、特に高速動作時に、効果は大な
るものとなる。
EFFECTS OF THE INVENTION The present invention provides a contact type one-dimensional solid-state imaging device in which the size of one gate length is large, and by subdividing the gate region, high transfer efficiency is obtained, and the effect is particularly great at high speed operation. Become.

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

第1図は本発明の一実施例における電荷転送装置の構造
断面図とポテンシャルモデル図、第2図は従来例の電荷
転送装置の構造とポテンシャルモデル図である。 1……多結晶シリコンゲート、2……多結晶シリコンゲ
ート、3,4……クロックパルスが印加される電極、5,6,
7,10……埋め込みチャンネル領域、8……シリコン基
板、9……信号電荷、11……ゲート酸化膜。
FIG. 1 is a structural sectional view and a potential model diagram of a charge transfer device according to an embodiment of the present invention, and FIG. 2 is a structure and a potential model diagram of a conventional charge transfer device. 1 ... Polycrystalline silicon gate, 2 ... Polycrystalline silicon gate, 3,4 ... Electrodes to which clock pulse is applied, 5,6,
7, 10 ... buried channel region, 8 ... silicon substrate, 9 ... signal charge, 11 ... gate oxide film.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】一導電形の半導体基板表面に、基板と反対
の導電形を有し、互いに濃度の異なる3つの領域からな
り、前記領域が直列に配置され、さらに最も濃度の高い
領域の上部には第1のゲート電極が形成され、他の2つ
の領域の上部には第2のゲート電極が形成され、前記濃
度の異なる他の2つの領域のなかで濃度の高い方の領域
は、前記第1のゲート電極下の最も濃度の高い領域に近
接しており、第1のゲート電極と第2のゲート電極は共
通接続されてクロックパルス印加電極に接続されている
構造の電荷転送装置。
1. A semiconductor substrate of one conductivity type, which comprises three regions having conductivity types opposite to those of the substrate and having different concentrations, said regions being arranged in series, and the uppermost region having the highest concentration. Has a first gate electrode formed thereon, a second gate electrode is formed on the other two regions, and the region having the higher concentration of the other two regions having different concentrations is A charge transfer device having a structure in which a first gate electrode and a second gate electrode are commonly connected to a clock pulse applying electrode, being close to a region having the highest concentration under the first gate electrode.
JP60024858A 1985-02-12 1985-02-12 Charge transfer device Expired - Lifetime JPH079982B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60024858A JPH079982B2 (en) 1985-02-12 1985-02-12 Charge transfer device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60024858A JPH079982B2 (en) 1985-02-12 1985-02-12 Charge transfer device

Publications (2)

Publication Number Publication Date
JPS61184876A JPS61184876A (en) 1986-08-18
JPH079982B2 true JPH079982B2 (en) 1995-02-01

Family

ID=12149912

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60024858A Expired - Lifetime JPH079982B2 (en) 1985-02-12 1985-02-12 Charge transfer device

Country Status (1)

Country Link
JP (1) JPH079982B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0404306A3 (en) * 1989-06-19 1991-07-17 Tektronix Inc. Trench structured charge-coupled device
JP2768312B2 (en) * 1995-06-02 1998-06-25 日本電気株式会社 Charge transfer device, driving method and manufacturing method thereof
JP4846139B2 (en) * 2001-08-22 2011-12-28 株式会社東芝 Hydraulic machine

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS575361A (en) * 1980-06-11 1982-01-12 Toshiba Corp Charge transfer device
JPS59115556A (en) * 1982-12-22 1984-07-04 Toshiba Corp Charge transfer type shift register
JPS61179574A (en) * 1985-02-04 1986-08-12 Mitsubishi Electric Corp Charge coupled device

Also Published As

Publication number Publication date
JPS61184876A (en) 1986-08-18

Similar Documents

Publication Publication Date Title
JPS62237761A (en) charge coupled device
JPH08181300A (en) Imaging device
JPH0458702B2 (en)
US5385860A (en) Charge transfer device
JPH079982B2 (en) Charge transfer device
JPH07161970A (en) Solid-state imaging device
JP2671597B2 (en) Solid-state image sensor, manufacturing method and driving method of solid-state image sensor
JPH0682693B2 (en) Charge transfer device
JPH07114278B2 (en) Method for manufacturing charge transfer device
JP2936153B2 (en) Method for manufacturing solid-state imaging device
JP2909158B2 (en) Charge coupled device
JP3301176B2 (en) Charge transfer device
JP2919697B2 (en) Method for manufacturing solid-state imaging device
JP2870046B2 (en) Charge-coupled device
JP3020537B2 (en) Charge-coupled device
JP2888266B2 (en) Charge transfer device
JP2713975B2 (en) Solid-state imaging device and method of manufacturing the same
JP2747328B2 (en) Charge transfer element
JPH11266003A (en) Semiconductor device and manufacturing method thereof
JPH0231858B2 (en)
JP3467918B2 (en) Method for manufacturing solid-state imaging device and solid-state imaging device
JP2867469B2 (en) Charge transfer device and method of manufacturing the same
JP2892547B2 (en) Charge-coupled device
JPH01300561A (en) Charge-coupled device
JPH0322755B2 (en)

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term