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JPH0673374B2 - Solid-state imaging device - Google Patents
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JPH0673374B2 - Solid-state imaging device - Google Patents

Solid-state imaging device

Info

Publication number
JPH0673374B2
JPH0673374B2 JP61291083A JP29108386A JPH0673374B2 JP H0673374 B2 JPH0673374 B2 JP H0673374B2 JP 61291083 A JP61291083 A JP 61291083A JP 29108386 A JP29108386 A JP 29108386A JP H0673374 B2 JPH0673374 B2 JP H0673374B2
Authority
JP
Japan
Prior art keywords
photosensitive pixel
region
pixel portion
solid
well
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
JP61291083A
Other languages
Japanese (ja)
Other versions
JPS63142856A (en
Inventor
茂則 松本
義光 広島
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 JP61291083A priority Critical patent/JPH0673374B2/en
Publication of JPS63142856A publication Critical patent/JPS63142856A/en
Publication of JPH0673374B2 publication Critical patent/JPH0673374B2/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
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F39/00Integrated devices, or assemblies of multiple devices, comprising at least one element covered by group H10F30/00, e.g. radiation detectors comprising photodiode arrays
    • H10F39/10Integrated devices
    • H10F39/12Image sensors
    • H10F39/15Charge-coupled device [CCD] image sensors
    • H10F39/153Two-dimensional or three-dimensional array CCD image sensors

Landscapes

  • 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 本発明はビデオカメラ等に用いられる固体撮像装置に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a solid-state image pickup device used in a video camera or the like.

従来の技術 第2図は従来のCCDを用いたインターライン転送方式固
体撮蔵装置を示すものである。感光画素部2、垂直CCD
シフトレジスタ3、水平CCDシフトレジスタ4、出力部
5の配置を示している。上記撮像装置1の大部分の領域
は受光領域6となっており、一部の領域は暗時出力成分
生成用のオプティカルブラック領域7(以下、OB領域と
呼ぶ) となっている。第3図は第2図のA−A′に沿った受光
領域6の一部およびOB領域7の一部の断面構造を示す模
式図である。ここで、8はN形シリコン基板,9はPウェ
ル、10は感光画素部となるN形領域、11はCCD転送チャ
ネルとなるN形領域、12は画素分離用のチャンネルスト
ップ部、13は二酸化シリコン膜、14はCCD転送ゲートと
なる多結晶シリコン、15は前記感光画素部となるN形領
域8の上方部を除いて形成された遮光用のアルミニウム
膜、16は表面保護、絶縁のためのリン珪酸ガラス(PS
G)膜である。なおPウェル9は感光画素のN形領域10
の下部の不純物濃度を低くし、過剰電荷をN形基板8へ
オーバーフローさせる構造となっている。
2. Description of the Related Art FIG. 2 shows an interline transfer type solid-state imaging device using a conventional CCD. Photosensitive pixel section 2, vertical CCD
The layout of the shift register 3, the horizontal CCD shift register 4, and the output unit 5 is shown. Most of the area of the image pickup apparatus 1 is a light receiving area 6, and part of the area is an optical black area 7 (hereinafter referred to as an OB area) for generating dark output components. FIG. 3 is a schematic diagram showing a sectional structure of a part of the light receiving region 6 and a part of the OB region 7 along the line AA ′ in FIG. Here, 8 is an N-type silicon substrate, 9 is a P-well, 10 is an N-type region serving as a photosensitive pixel portion, 11 is an N-type region serving as a CCD transfer channel, 12 is a channel stop portion for pixel separation, and 13 is a dioxide. Silicon film, 14 is polycrystalline silicon that serves as a CCD transfer gate, 15 is a light-shielding aluminum film that is formed excluding the upper portion of the N-type region 8 that serves as the photosensitive pixel portion, and 16 is for surface protection and insulation. Phosphosilicate glass (PS
G) Membrane. The P well 9 is an N type region 10 of the photosensitive pixel.
In this structure, the impurity concentration in the lower part of the N-type substrate 8 is lowered to cause excess charges to overflow into the N-type substrate 8.

上記固体撮像装置1において、受光部6に光が入射する
ことによって生成された信号電荷は感光画素部のN形領
域10に蓄積された後、垂直CCDレジスタ3、および水平C
CDレジスタ4を転送され、出力部5より電圧変換され読
み出される。
In the solid-state imaging device 1, the signal charges generated by the light incident on the light receiving unit 6 are accumulated in the N-type region 10 of the photosensitive pixel unit, and then the vertical CCD register 3 and the horizontal C
The data is transferred from the CD register 4, converted from the voltage by the output unit 5, and read.

ここで、光入力を全く遮断したとしても出力成分(暗時
出力成分または暗電流と呼ばれ熱的に生成される一種の
もれ電流である)が観測され、この出力成分は温度上昇
に伴って増加する。このような暗電流が大きくなると信
号処理に必要な、基準黒レベルが変化するという問題が
生じる。そこで温度上昇にともなう暗電流成分の増加分
を差し引くような信号処理が行なわれており、暗電流の
みの増加分を検出するために前記OB領域7が設けられて
いる。このため、OB領域7はアルミニウム膜15が感光画
素部のN形領域10の上部にも形成されている他は受光部
6と同一構造となっている。
Here, even if the light input is completely cut off, an output component (a dark current output component or a kind of leakage current that is thermally generated and called dark current) is observed. Increase. When such a dark current becomes large, there arises a problem that the reference black level necessary for signal processing changes. Therefore, signal processing is performed to subtract the increase in dark current component due to temperature rise, and the OB area 7 is provided to detect the increase in dark current alone. Therefore, the OB region 7 has the same structure as the light receiving unit 6 except that the aluminum film 15 is also formed on the N-type region 10 of the photosensitive pixel portion.

前述したアルミニウム膜15は蒸着後エッチング処理され
て形成されるが、感光画素部となるN形領域10の表面は
各工程でイオン等によるダメージを受け暗電流は著しく
増加する。これはSiO2膜13とN形領域の10の界面に存在
する界面準位密度が増加するためである。これを低減す
るために例えば450℃、窒素が90%、水素が10%の雰囲
気中で30分間程度のアニール処理を施すのが通常であ
る。
The aluminum film 15 described above is formed by etching after vapor deposition, but the surface of the N-type region 10 that becomes the photosensitive pixel portion is damaged by ions or the like in each step, and the dark current remarkably increases. This is because the interface state density existing at the interface between the SiO 2 film 13 and the N-type region 10 increases. In order to reduce this, for example, it is usual to perform annealing treatment for about 30 minutes in an atmosphere of 450 ° C., nitrogen of 90%, and hydrogen of 10%.

発明が解決しようとする問題点 しかしながら、上記アニールを含めて保護絶縁膜成長等
の高温処理をアルミニウム膜15を形成後に行なうため感
光画素の表面にアルミニウム膜15が存在しない受光領域
6と表面にアルミニウム膜15が存在するOB領域7とでは
H2の浸透効果も含めて界面準位密度に差が生じる。した
がって受光領域6の暗電流とOB領域7の暗電流に差が生
じる。このため受光領域の、暗時出力成分のみを検出す
ることをOB領域はその作用がきわめて不完全なものとな
り大きな問題となっていた。
Problems to be Solved by the Invention However, since the high temperature treatment such as the growth of the protective insulating film including the above annealing is performed after the aluminum film 15 is formed, the light receiving region 6 where the aluminum film 15 does not exist on the surface of the photosensitive pixel and the aluminum on the surface. In the OB area 7 where the film 15 exists
There is a difference in the interface state density including the H 2 permeation effect. Therefore, a difference occurs between the dark current of the light receiving area 6 and the dark current of the OB area 7. For this reason, the detection of only the dark output component of the light-receiving region has become a serious problem because the action in the OB region is extremely incomplete.

本発明はこのような問題点を解決するものであり受光領
域とOB領域とで暗電流の差が生じず、受光領域における
暗電流の温度変動に対して正確な補償が可能な固体撮像
装置を実現することを目的とするものである。
The present invention solves such a problem and provides a solid-state imaging device capable of accurately compensating for the temperature fluctuation of the dark current in the light receiving region without causing a difference in dark current between the light receiving region and the OB region. It is intended to be realized.

問題点を解決するための手段 この問題点を解決するために本発明の固体撮像装置は、
OB領域内の感光画素部を形成するウェル領域の接合深さ
および不純物濃度が、受光領域内の感光画素部を形成す
るウェル領域に比べて浅くあるいは低濃度であることを
特徴とするものである。
Means for Solving the Problems In order to solve this problem, the solid-state imaging device of the present invention is
It is characterized in that the junction depth and the impurity concentration of the well region forming the photosensitive pixel portion in the OB region are shallower or lower than those in the well region forming the photosensitive pixel portion in the light receiving region. .

作用 この構成により、受光領域とOB領域の感光画素構造は全
く同一構造となり、暗電流の発生源となるSiとSiO2の界
面準位の状態にも差がなく、上記両領域における暗電流
の差は発生しなくなると同時に、OB領域では入射光によ
り発生した電荷は全く読み出さないため、OB特性として
は完全なものとなる。
Action With this configuration, the photosensitive pixel structure in the light receiving area and the OB area are completely the same structure, there is no difference in the state of the interface state between Si and SiO 2 which is the source of dark current, and the dark current in both areas is At the same time as the difference does not occur, the electric charge generated by the incident light is not read out at all in the OB region, so the OB characteristic is perfect.

実施例 以下、図面を参照して本発明の一実施例を詳細に説明す
る。
Embodiment Hereinafter, an embodiment of the present invention will be described in detail with reference to the drawings.

第1図aは本実施例による固体撮像装置における受光領
域およびOB領域の一部の断面構造を示す模式図である。
第3図の従来構造と比較するとOB領域のPウェル:P(O
B)17の形状が、第3図のPウェル9の場合より感光画
素部となるN形領域10の下部で極めて接合深さを浅くし
た点、およびアルミニウム膜16が受光領域とOB領域とで
全く同一形状である点以外は第3図と同一であるので同
一符号を用いてその詳述を省略する。
FIG. 1A is a schematic view showing a sectional structure of a part of the light receiving region and the OB region in the solid-state imaging device according to the present embodiment.
Compared with the conventional structure shown in FIG. 3, the P well in the OB region: P (O
B) 17 has a shape in which the junction depth is made extremely shallow under the N-type region 10 which is a photosensitive pixel portion as compared with the case of the P well 9 in FIG. 3, and the aluminum film 16 has a light receiving region and an OB region. Since it is the same as FIG. 3 except that it has exactly the same shape, the same reference numerals are used and the detailed description thereof is omitted.

第1図aに示したように、受光領域とOB領域の感光画素
構造をN形領域10の下部のPウェル形状を除き全く同一
形状としている。つまり、アルミニウム膜形成、エッチ
ング、水素による効果も含めて同じ条件で処理されるた
め、SiとSiO2の界面準位密度も全く差は発生しない。こ
のため、暗電流の発生も受光領域、OB領域で全く同じ発
生量、温度依存性を示す。
As shown in FIG. 1A, the photosensitive pixel structures of the light receiving region and the OB region have exactly the same shape except for the P well shape below the N type region 10. That is, since the aluminum film formation, etching, and hydrogen treatment are performed under the same conditions, there is no difference in the interface state density between Si and SiO 2 . Therefore, the generation of dark current also shows exactly the same amount and temperature dependency in the light receiving region and the OB region.

光入射時においては、OB領域で発生した電荷は全てN形
基板8へ掃き出され信号電荷とはならない。第2図bは
そのメカニズムを示すものである。N形基板8に正電位
(Vsub)を印加した状態での感光画素部の電子ポテンシ
ャル分布を示したものである。(図中○印は電子を示
す。)受光領域ではポテンシャルの最大値より表面側で
発生した電子は信号電荷となるが、OB領域ではポテンシ
ャルの最大値はほとんどN形領域10と等しくなるため、
N形基板8に掃き出されてしまう。このため、OB領域
は、光入射の影響を全く受けず、受光領域の暗状態と全
く同じ暗電流を発生する。
At the time of light incidence, all the charges generated in the OB region are swept out to the N-type substrate 8 and do not become signal charges. FIG. 2b shows the mechanism. 6 shows an electron potential distribution of a photosensitive pixel portion in a state where a positive potential (Vsub) is applied to the N-type substrate 8. (The circles in the figure indicate electrons.) In the light-receiving region, the electrons generated on the surface side of the maximum potential value become signal charges, but in the OB region, the maximum potential value is almost equal to the N-type region 10, so
It is swept up on the N-type substrate 8. For this reason, the OB region is not affected by the incidence of light at all, and produces exactly the same dark current as the dark state of the light receiving region.

上記のように、温度変動による受光領域の暗電流の変動
分はOB領域の暗電流により正確に補償が可能となる。
As described above, the dark current variation in the light receiving region due to the temperature variation can be accurately compensated by the dark current in the OB region.

なお、本発明は上記実施例に限られるものではなく、信
号電荷の読み出し方法としてCCD方式以外のものを用い
た場合、感光画素として、MOS容量、アモルファス半導
体、化合物半導体を用いた場合でも全く同様の効果が得
られる。
Note that the present invention is not limited to the above-described embodiment, and when a method other than the CCD method is used as a method for reading out signal charges, the same is true even when a MOS pixel, an amorphous semiconductor, or a compound semiconductor is used as a photosensitive pixel. The effect of is obtained.

発明の効果 以上のように本発明によれば、受光領域の暗電流とOB領
域の暗電流の発生に差が生じないので、温度変化にとも
なう暗電流変化分の正確な補償が可能になり、広い温度
範囲にわたり高画質の固体撮像装置を実現できる。
As described above, according to the present invention, since there is no difference between the dark current in the light receiving region and the dark current in the OB region, it is possible to accurately compensate for the dark current change due to the temperature change. It is possible to realize a high-quality solid-state imaging device over a wide temperature range.

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

第1図aは本発明の一実施例による固体撮像装置の受光
領域およびOB領域の一部の断面構造を示す模式図、第1
図bは第1図aのB−B′,C−C′に沿った電子ポテン
シャル分布を示す図、第2図は従来の固体撮像装置の構
成・配置を示す概略図、第3図は従来の固体撮像装置の
受光領域およびOB領域の一部の断面構造を示す模式図で
ある。 1……固体撮像装置、2……感光画素部、3……垂直CC
Dソフトレジスタ、4……水平CCDシフトレジスタ、5…
…出力部、6……受光領域、7……OB領域、8……N形
シリコン基板、9,17……Pウェル、10……感光画素用N
形領域、11……垂直CCDレジスタ用N形領域、12……チ
ャンネルストッパー用P+領域、13……二酸化シリコン、
14……多結晶シリコン、15……アルミニウム膜、16……
リン珪酸ガラス膜。
FIG. 1a is a schematic view showing a sectional structure of a part of a light receiving region and an OB region of a solid-state imaging device according to an embodiment of the present invention.
FIG. B is a diagram showing the electron potential distribution along BB ′ and CC ′ in FIG. 1a, FIG. 2 is a schematic diagram showing the configuration and arrangement of a conventional solid-state imaging device, and FIG. 3 is a conventional diagram. FIG. 3 is a schematic diagram showing a cross-sectional structure of a part of a light receiving area and an OB area of the solid-state imaging device of FIG. 1 ... Solid-state imaging device, 2 ... Photosensitive pixel part, 3 ... Vertical CC
D soft register, 4 ... Horizontal CCD shift register, 5 ...
… Output section, 6 …… Light receiving area, 7 …… OB area, 8 …… N type silicon substrate, 9,17 …… P well, 10 …… N for photosensitive pixels
Shaped area, 11 …… N-shaped area for vertical CCD register, 12 …… P + area for channel stopper, 13 …… Silicon dioxide,
14 …… Polycrystalline silicon, 15 …… Aluminum film, 16 ……
Phosphosilicate glass film.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】半導体基板と、上記半導体基板の主表面に
設けられ、かつ上記半導体基板と異なる導電形を有する
ウェルと、上記ウェル内にそれぞれ設けられた複数の感
光画素部および上記感光画素部から信号電荷を読み出す
電荷読み出し部と、上記半導体基板上で上記感光画素部
の直上方部を除いて形成された遮光膜とを具備し、上記
複数の感光画素部のうち一部の感光画素部は暗時出力成
分生成用のオプティカルブラック領域に設けられ、残り
の感光画素部は受光用のセンサ領域に設けられ、前記オ
プティカルブラック領域となる感光画素部を形成するウ
ェル領域が受光用感光画素部を形成するウェル領域より
不純物濃度が低く、あるいは接合深さが浅く形成されて
いることを特徴とする固体撮像装置。
1. A semiconductor substrate, a well provided on a main surface of the semiconductor substrate and having a conductivity type different from that of the semiconductor substrate, a plurality of photosensitive pixel portions provided in the well, and the photosensitive pixel portion. And a light-shielding film formed on the semiconductor substrate except a portion directly above the photosensitive pixel portion, and a part of the photosensitive pixel portion among the plurality of photosensitive pixel portions. Is provided in the optical black region for generating the dark output component, the remaining photosensitive pixel portion is provided in the sensor region for receiving light, and the well region forming the photosensitive pixel portion to be the optical black region is the photosensitive pixel portion for receiving light. A solid-state image pickup device having a lower impurity concentration or a shallower junction depth than a well region in which a trench is formed.
JP61291083A 1986-12-05 1986-12-05 Solid-state imaging device Expired - Lifetime JPH0673374B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61291083A JPH0673374B2 (en) 1986-12-05 1986-12-05 Solid-state imaging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61291083A JPH0673374B2 (en) 1986-12-05 1986-12-05 Solid-state imaging device

Publications (2)

Publication Number Publication Date
JPS63142856A JPS63142856A (en) 1988-06-15
JPH0673374B2 true JPH0673374B2 (en) 1994-09-14

Family

ID=17764216

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61291083A Expired - Lifetime JPH0673374B2 (en) 1986-12-05 1986-12-05 Solid-state imaging device

Country Status (1)

Country Link
JP (1) JPH0673374B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6721005B1 (en) * 1998-12-03 2004-04-13 Sony Corporation Solid state image sensor having different structures for effective pixel area and optical black area

Also Published As

Publication number Publication date
JPS63142856A (en) 1988-06-15

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