JP2868545B2 - Solid-state imaging device - Google Patents
Solid-state imaging deviceInfo
- Publication number
- JP2868545B2 JP2868545B2 JP1252650A JP25265089A JP2868545B2 JP 2868545 B2 JP2868545 B2 JP 2868545B2 JP 1252650 A JP1252650 A JP 1252650A JP 25265089 A JP25265089 A JP 25265089A JP 2868545 B2 JP2868545 B2 JP 2868545B2
- Authority
- JP
- Japan
- Prior art keywords
- solid
- state imaging
- type
- imaging device
- concentration
- 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
Links
- 238000003384 imaging method Methods 0.000 title claims description 18
- 239000000758 substrate Substances 0.000 claims description 45
- 239000004065 semiconductor Substances 0.000 claims description 24
- 238000009792 diffusion process Methods 0.000 claims description 13
- 239000012535 impurity Substances 0.000 description 20
- 238000000034 method Methods 0.000 description 12
- 238000005468 ion implantation Methods 0.000 description 6
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 229910052760 oxygen Inorganic materials 0.000 description 4
- 239000001301 oxygen Substances 0.000 description 4
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 3
- 229910052799 carbon Inorganic materials 0.000 description 3
- 230000007423 decrease Effects 0.000 description 3
- 238000005247 gettering Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 238000000206 photolithography Methods 0.000 description 1
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 1
- 229920005591 polysilicon Polymers 0.000 description 1
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〕 この発明は、CMD(Charge Modulation Device)受光
素子及び周辺回路を構成するCMOSFETとを備えた固体撮
像装置に関する。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a solid-state imaging device including a CMD (Charge Modulation Device) light-receiving element and a CMOSFET constituting a peripheral circuit.
従来、MIS型受光・蓄積部を有する受光素子からなる
固体撮像装置は種々のものが知られているが、その中、
MIS型受光・蓄積部を有し且つ内部増幅機能を有する受
光素子を用いた固体撮像装置がある。その一例として本
件発明者が提案したCMD受光素子を用いた固体撮像装置
があり、特開昭61−84059号、及び1986年に開催されたI
nternational Electron Device Meeting(IEDM)の予稿
集の第353〜356頁の“A NEW MOS IMAGE SENSOR OPERATI
NG IN A NON−DESTRUCTIVE READOUT MODE"という題名の
論文で、その内容について開示がなされている。Conventionally, various types of solid-state imaging devices including a light receiving element having a MIS type light receiving / accumulating unit are known.
There is a solid-state imaging device using a light receiving element having an MIS type light receiving / accumulating unit and having an internal amplification function. As an example, there is a solid-state imaging device using a CMD light receiving element proposed by the present inventor, which is disclosed in JP-A-61-84059, and
“A NEW MOS IMAGE SENSOR OPERATI” on pages 353 to 356 of the proceedings of the nternational Electron Device Meeting (IEDM)
NG IN A NON-DESTRUCTIVE READOUT MODE ", the contents of which are disclosed.
第3図は、かかるCMD受光素子を用いた固体撮像装置
における単位画素の概略断面構造を示す図である。図に
おいて、101はp-基板、102はn-チャネル層、103はn+ソ
ース拡散層、104はn+ドレイン拡散層、105はゲート絶縁
膜、106はゲートポリシリコン電極、107はソース電極、
108はドレイン電極である。FIG. 3 is a diagram showing a schematic cross-sectional structure of a unit pixel in a solid-state imaging device using such a CMD light receiving element. In the figure, 101 is a p - substrate, 102 is an n - channel layer, 103 is an n + source diffusion layer, 104 is an n + drain diffusion layer, 105 is a gate insulating film, 106 is a gate polysilicon electrode, 107 is a source electrode,
108 is a drain electrode.
次に、このような構成のCMD受光素子の受光動作につ
いて説明する。まず光109がゲート電極106の上部より入
射すると、入射光109はゲート電極106,ゲート絶縁膜105
を通ってn-チャネル層102に入り、そこで正孔−電子対
を発生させる。そのうちの光発生正孔が、逆バイアスが
印加されているゲート電極106のゲート絶縁膜105−n-チ
ャネル層102の界面に蓄積され、その結果、表面電位が
上昇する。それより、ソース拡散層103とドレイン拡散
層104間に存在する電子に対する電子障壁が低下し、n-
チャネル層102中を電子電流が流れる。この電流を読み
取ることにより増幅された光信号が得られるようになっ
ている。Next, the light receiving operation of the CMD light receiving element having such a configuration will be described. First, when light 109 enters from above the gate electrode 106, the incident light 109 enters the gate electrode 106 and the gate insulating film 105.
Through the n - channel layer 102 where a hole-electron pair is generated. Of these, the photogenerated holes are accumulated at the interface between the gate insulating film 105-n and the channel layer 102 of the gate electrode 106 to which a reverse bias is applied, and as a result, the surface potential increases. As a result, the electron barrier for electrons existing between the source diffusion layer 103 and the drain diffusion layer 104 decreases, and n −
An electron current flows through the channel layer 102. By reading this current, an amplified optical signal can be obtained.
ところで、従来のCMD受光素子を用いた固体撮像装置
においては、CMD受光素子のバックゲート電極は、不純
物濃度が1E13〜1E16cm-3のp-型基板をそのまま使用し、
その上に不純物濃度が1E13〜1E14cm-3、厚さが3〜10μ
mのn-エピタキシャル層を形成している。すなわち第4
図(A),(B)に示すように一様な基板濃度Csubのp
型基板上に、高抵抗n-型エピタキシャル層を厚さx1に形
成している。By the way, in a conventional solid-state imaging device using a CMD light receiving element, the back gate electrode of the CMD light receiving element uses a p - type substrate having an impurity concentration of 1E13 to 1E16 cm -3 as it is,
The impurity concentration is 1E13-1E14cm -3 and the thickness is 3-10μ
An n - epitaxial layer of m is formed. That is, the fourth
As shown in FIGS. 9A and 9B, the uniform substrate concentration C sub
On the mold substrate, a high resistance the n - -type epitaxial layer to a thickness x 1.
このような基板とエピタキシャル層を用いて作成した
CMD受光素子を用いた固体撮像装置の欠点としては、所
望の基板濃度のウエハーを得るのに2〜3ヶ月の長期間
を要する点、ゲッタリングに重要となる格子間酸素濃
度,炭素濃度,及びボロン濃度を全て所望の値に入れる
のが困難となる点、基板引き上げの際の成長縞等による
不純物濃度むらが、CMD受光素子を用いたイメージセン
サにおいては出力不均一を引き起こし固定パターンノイ
ズ(FPN)になる点、及び酸素が原因となるサーマルド
ナーの発生による基板不純物濃度の変化がFPNの原因と
なり、熱工程に制限が加わる点などが挙げられ、歩留り
の低下をきたす原因となっていた。Made using such a substrate and epitaxial layer
Disadvantages of the solid-state imaging device using the CMD light-receiving element are that it takes a long time of two to three months to obtain a wafer with a desired substrate concentration, interstitial oxygen concentration, carbon concentration, which are important for gettering, and The point that it is difficult to set all the boron concentration to the desired value, and the impurity concentration unevenness due to the growth stripes when pulling up the substrate causes non-uniform output in the image sensor using the CMD light receiving element, and the fixed pattern noise (FPN) ), And changes in the substrate impurity concentration due to the generation of thermal donors caused by oxygen, which cause the FPN to be restricted and limit the thermal process.
本発明は、従来のCMD受光素子を用いた固体撮像装置
における上記問題点を解消するためになされたもので、
n-エピタキシャル層を所望の不純物濃度をもつ拡散層上
に形成でき、FPNが少なく歩留りの向上した固体撮像装
置を提供することを目的とする。The present invention has been made in order to solve the above-described problems in a solid-state imaging device using a conventional CMD light receiving element,
An object of the present invention is to provide a solid-state imaging device in which an n - epitaxial layer can be formed on a diffusion layer having a desired impurity concentration, which has a small FPN and an improved yield.
上記問題点を解決するため、本発明の固体撮像装置
は、半導体基板部の表面にソース領域及びドレイン領域
を形成すると共に、該ソース領域及びドレイン領域の間
に絶縁膜を介してゲート電極を配置し、前記基板部表面
と平行にソース・ドレイン電流が流れるように構成した
CMD受光素子及びCMOSFETを備えた固体撮像装置であっ
て、前記半導体基板部は、第1導電型の半導体基板と、
該基板の表面上に形成した第1導電型の第1のエピタキ
シャル層と、前記第1のエピタキシャル層の表面上に形
成した第2導電型の2のエピタキシャル層とで構成され
ていることを特徴とする。In order to solve the above problems, a solid-state imaging device according to the present invention has a source region and a drain region formed on a surface of a semiconductor substrate portion, and a gate electrode is disposed between the source region and the drain region via an insulating film. And the source / drain current flows in parallel with the surface of the substrate.
A solid-state imaging device including a CMD light receiving element and a CMOSFET, wherein the semiconductor substrate unit includes a semiconductor substrate of a first conductivity type;
A first conductive type first epitaxial layer formed on the surface of the substrate; and a second conductive type two epitaxial layer formed on the surface of the first epitaxial layer. And
このように半導体基板部を構成することによりチャネ
ル領域となる第2型半導体層下の基板部の不純物濃度
を、第1型半導体層若しくは半導体拡散層により、容易
にデバイス動作を最適な値にすることが可能となる。ま
た、第1型基板濃度は原理的には任意の不純物濃度でよ
いので、ゲッタリング工程に重要となる酸素濃度,炭素
濃度等の濃度の合わせ込みが極めて容易となる。By configuring the semiconductor substrate portion in this way, the impurity concentration of the substrate portion below the second type semiconductor layer which becomes the channel region can be easily adjusted to an optimum value by the first type semiconductor layer or the semiconductor diffusion layer. It becomes possible. In addition, since the first-type substrate concentration may be an arbitrary impurity concentration in principle, it is extremely easy to adjust the concentrations such as the oxygen concentration and the carbon concentration, which are important in the gettering step.
また、不純物濃度が高精度で制御可能なイオン注入
法、エピタキシャル法等により基板不純物濃度を制御す
るため不純物濃度むらによるFPNの増大や歩留りの低下
を有効に防止することができる。In addition, since the substrate impurity concentration is controlled by an ion implantation method, an epitaxial method, or the like in which the impurity concentration can be controlled with high accuracy, it is possible to effectively prevent an increase in FPN and a decrease in yield due to uneven impurity concentration.
以下、この発明に係わる固体撮像装置における実施例
を図面を参照して説明する。なお、説明においては、第
1型基板に設けた第2型エピタキシャル層上の半導体領
域や電極等は上記の従来のCMDと同様であるのでその説
明は省く。Hereinafter, embodiments of a solid-state imaging device according to the present invention will be described with reference to the drawings. In the description, the semiconductor regions, electrodes, and the like on the second type epitaxial layer provided on the first type substrate are the same as those of the above-described conventional CMD, and thus description thereof is omitted.
第1図(A),(B)はこの発明の第1実施例の半導
体基板部及び不純物濃度分布を示す図である。FIGS. 1A and 1B are views showing a semiconductor substrate portion and an impurity concentration distribution according to a first embodiment of the present invention.
第1図(A),(B)において半導体基板の濃度
Csub′をもつP型半導体基板11を用い、そしてn-型エピ
タキシャル層13を積層する前に、P型基板表面に従来の
半導体基板の濃度Csubとほぼ等しい濃度、例えば1E13〜
1E16cm-3となるP型エピタキシャル層12の厚さ(x2−
x1)に形成する。そしてP型エピタキシャル層12の表面
に従来のものと同様にn-型エピタキシャル層13を厚さx1
で形成して半導体基板部を構成するものである。なお、
図示していないが、N−MOSFETを形成するPウエル拡散
層下には、P型エピタキシャル層12を形成した後、n-型
埋込層がイオン注入法等を用いて形成されている。また
本実施例においては、P型半導体基板11の濃度Csub′は
原理的には任意の濃度でよい。1A and 1B, the concentration of the semiconductor substrate is shown.
Before using the P-type semiconductor substrate 11 having C sub 'and laminating the n − -type epitaxial layer 13, the P-type substrate surface has a concentration substantially equal to the concentration C sub of the conventional semiconductor substrate, for example, 1E13E.
The thickness of the P-type epitaxial layer 12 to be 1E16 cm -3 (x 2 −
x 1 ). An n − -type epitaxial layer 13 having a thickness of x 1 is formed on the surface of the P-type epitaxial layer 12 in the same manner as the conventional one.
To form a semiconductor substrate portion. In addition,
Although not shown, an n - type buried layer is formed under a P-well diffusion layer forming an N-MOSFET after forming a P-type epitaxial layer 12 by using an ion implantation method or the like. Further, in this embodiment, the concentration C sub 'of the P-type semiconductor substrate 11 may be an arbitrary concentration in principle.
この実施例によれば、半導体チップ内の速度分布ばら
つきが約1%以下である。エピタキシャル法により実効
基板濃度が決まるため、基板濃度ばらつきに起因する固
定パターンノイズが従来例に比べ大幅に減少させること
ができる。According to this embodiment, the speed distribution variation in the semiconductor chip is about 1% or less. Since the effective substrate concentration is determined by the epitaxial method, the fixed pattern noise caused by the substrate concentration variation can be significantly reduced as compared with the conventional example.
次に、この発明の第2実施例について説明する。第2
図(A),(B)は半導体基板部及び不純物濃度分布を
示す図である。第2図(A),(B)において、任意の
濃度をもつP型基板11、上に従来の半導体基板の濃度C
subより低い濃度Csub′をもつP型エピタキシャル層12
を(x2−x1)=約10〜20μmの厚さで形成する。そして
n-型エピタキシャル層13を積層する前にP型エピタキシ
ャル層12表面にピーク濃度がほぼCsubとなるP型拡散層
14を形成する。そしてこのP型拡散層14の表面に従来の
ものと同様にn-型エピタキシャル層13を厚さx1で形成し
て半導体基板部を構成するものである。Next, a second embodiment of the present invention will be described. Second
FIGS. 7A and 7B are diagrams showing a semiconductor substrate portion and an impurity concentration distribution. 2 (A) and 2 (B), a P-type substrate 11 having an arbitrary concentration and a conventional semiconductor substrate having a concentration C
P-type epitaxial layer 12 having a low concentration C sub 'from sub
Is formed with a thickness of (x 2 −x 1 ) = about 10 to 20 μm. And
P-type diffusion layer having a peak concentration of approximately C sub on the surface of P-type epitaxial layer 12 before stacking n - type epitaxial layer 13
Form 14. Then, an n − -type epitaxial layer 13 is formed on the surface of the P-type diffusion layer 14 with a thickness of x1, similarly to the conventional one , to form a semiconductor substrate portion.
この実施例においては、Csub′はP型導電型が保たれ
る範囲において出来るだけ低い濃度であることが望まし
い。In this embodiment, it is desirable that C sub 'be as low as possible in the range where the P-type conductivity is maintained.
また、P型拡散層14はイオン注入法等を用いて形成さ
れる。更に、このP型拡散層14はウエハー全面或いはフ
ォトリソグラフィー法を用いて、上記P型ウエル以外の
部分に形成する方法等によって達成される。Further, the P-type diffusion layer 14 is formed by using an ion implantation method or the like. Further, the P-type diffusion layer 14 is achieved by a method of forming the entire surface of the wafer or a portion other than the P-type well by using a photolithography method.
この実施例によれば、半導体チップ内の濃度分布ばら
つきが1%以下であるイオン注入法により実効基板濃度
が決まるため基板濃度ばらつきに起因する固定パターン
ノイズが従来例に比べて大幅に減少する。また上記第1
実施例と比べてイオン注入法により実効基板濃度が決ま
るため基板濃度の値の制御が容易になる。According to this embodiment, since the effective substrate concentration is determined by the ion implantation method in which the concentration distribution variation in the semiconductor chip is 1% or less, the fixed pattern noise caused by the substrate concentration variation is significantly reduced as compared with the conventional example. In addition, the first
Since the effective substrate concentration is determined by the ion implantation method as compared with the embodiment, the value of the substrate concentration can be easily controlled.
なお、上記各実施例においては、nチャネルCMDを用
いたもので説明したが、不純物のタイプを変えることで
PチャネルCMDに用いたものも勿論適用可能である。In each of the embodiments described above, an n-channel CMD is used. However, it is needless to say that an n-channel CMD can be used by changing an impurity type.
以上実施例に基づいて説明したように、本発明によれ
ば、チャネル領域となるn-半導体層下のP型不純物濃度
を、イオン注入法のドーズ量或いはエピタキシャル法の
n型不純物ガス流量を調整する等によって容易にデバイ
ス動作に最適な値にすることができ、開発・試作期間の
大幅な短縮ができる。また、基板濃度は原理的にはP型
であれば任意の不純物濃度でよいのでゲッタリング工程
に重要となる酸素、炭素濃度等の濃度の合わせ込みが容
易になる。また、上記実施例で示したように基板の不純
物濃度むらによるFPNの増大に起因する歩留りの低下を
防止することができる等の効果が得られる。As described above with reference to the embodiments, according to the present invention, the P-type impurity concentration under the n − semiconductor layer serving as the channel region is adjusted by adjusting the dose amount of the ion implantation method or the n-type impurity gas flow rate of the epitaxial method. By doing so, the value can be easily optimized for the device operation, and the development / prototype period can be significantly reduced. In addition, since the substrate concentration can be any impurity concentration in principle as long as it is a P-type, it is easy to adjust the concentrations such as oxygen and carbon concentrations which are important in the gettering step. Further, as shown in the above embodiment, effects such as a decrease in yield due to an increase in FPN due to uneven impurity concentration of the substrate can be obtained.
第1図(A),(B)は、本発明に係る固体撮像装置の
第1実施例の基板部の基本構成及び不純物濃度分布を説
明するための図、第2図(A),(B)は該装置の第2
実施例の基板部の基本構成及び不純物濃度分布を説明す
るための図、第3図は、従来のCMD受光素子を用いた固
体撮像装置の一例を示す断面図、第4図(A),(B)
は、従来のCMD受光素子の基板部の構成及び不純物濃度
分布を示す図である。 図において、11はP型基板、12はP型エピタキシャル
層、13はn-型エピタキシャル層、14はP型拡散層を示
す。FIGS. 1A and 1B are diagrams for explaining the basic structure and impurity concentration distribution of a substrate portion of a first embodiment of a solid-state imaging device according to the present invention, and FIGS. 2A and 2B. ) Is the second of the device
FIG. 3 is a view for explaining a basic configuration and an impurity concentration distribution of a substrate portion of the embodiment, FIG. 3 is a cross-sectional view showing an example of a solid-state imaging device using a conventional CMD light receiving element, and FIGS. B)
FIG. 2 is a diagram showing a configuration of a substrate portion and an impurity concentration distribution of a conventional CMD light receiving element. In the figure, 11 indicates a P-type substrate, 12 indicates a P-type epitaxial layer, 13 indicates an n − -type epitaxial layer, and 14 indicates a P-type diffusion layer.
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H01L 27/14 - 27/148 H04N 5/335 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 6 , DB name) H01L 27/14-27/148 H04N 5/335
Claims (2)
イン領域を形成すると共に、該ソース領域及びドレイン
領域の間に絶縁膜を介してゲート電極を配置し、前記基
板部表面と平行にソース・ドレイン電流が流れるように
構成したCMD受光素子及びCMOSFETを備えた固体撮像装置
であって、前記半導体基板部は、第1導電型の半導体基
板と、該基板の表面上に形成した第1導電型の第1のエ
ピタキシャル層と、前記第1のエピタキシャル層の表面
上に形成した第2導電型の2のエピタキシャル層とで構
成されていることを特徴とする固体撮像装置。A source region and a drain region are formed on a surface of the semiconductor substrate portion, and a gate electrode is disposed between the source region and the drain region via an insulating film; A solid-state imaging device including a CMD light receiving element and a CMOSFET configured to allow a drain current to flow, wherein the semiconductor substrate portion includes a semiconductor substrate of a first conductivity type and a first conductivity type formed on a surface of the substrate. A solid-state imaging device, comprising: a first epitaxial layer of (i), and two epitaxial layers of the second conductivity type formed on the surface of the first epitaxial layer.
部に、第1導電型の第1の半導体拡散層が形成されてい
ることを特徴とする請求項第1項記載の固体撮像装置。2. The solid-state imaging device according to claim 1, wherein a first conductive type first semiconductor diffusion layer is formed on at least a part of said first epitaxial layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1252650A JP2868545B2 (en) | 1989-09-28 | 1989-09-28 | Solid-state imaging device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1252650A JP2868545B2 (en) | 1989-09-28 | 1989-09-28 | Solid-state imaging device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH03114260A JPH03114260A (en) | 1991-05-15 |
| JP2868545B2 true JP2868545B2 (en) | 1999-03-10 |
Family
ID=17240307
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1252650A Expired - Fee Related JP2868545B2 (en) | 1989-09-28 | 1989-09-28 | Solid-state imaging device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2868545B2 (en) |
-
1989
- 1989-09-28 JP JP1252650A patent/JP2868545B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH03114260A (en) | 1991-05-15 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |