JPH1093064A - Solid-state image-sensing element - Google Patents

Solid-state image-sensing element

Info

Publication number
JPH1093064A
JPH1093064A JP8243367A JP24336796A JPH1093064A JP H1093064 A JPH1093064 A JP H1093064A JP 8243367 A JP8243367 A JP 8243367A JP 24336796 A JP24336796 A JP 24336796A JP H1093064 A JPH1093064 A JP H1093064A
Authority
JP
Japan
Prior art keywords
substrate
epitaxial layer
semiconductor substrate
solid
ring
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.)
Granted
Application number
JP8243367A
Other languages
Japanese (ja)
Other versions
JP3584629B2 (en
Inventor
Koichi Harada
耕一 原田
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.)
Sony Corp
Original Assignee
Sony 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 Sony Corp filed Critical Sony Corp
Priority to JP24336796A priority Critical patent/JP3584629B2/en
Publication of JPH1093064A publication Critical patent/JPH1093064A/en
Application granted granted Critical
Publication of JP3584629B2 publication Critical patent/JP3584629B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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

Abstract

PROBLEM TO BE SOLVED: To make the potential differences of both ends of PN junctions zero and to prevent leakage currents from flowing by perfectly depleting the section between a semiconductor substrate and an area above a ring provided in the vicinity of the element by applying a voltage between an epitaxial layer forming an overflow barrier, and the semiconductor substrate and the area. SOLUTION: In the vicinity of the periphery of the peripheral part 4 of the N-type semiconductor region of an element, an N<+> -type region 6 on a ring is formed. When in use, a substrate bias voltage Vsub to be applied to a semiconductor substrate 1 is applied to the N<+> -type region 6. When in use, the section between the substrate 1 and the N<+> -type region 6 on a ring is completely depleted, and voltage difference is not generated in each PN-junction between an overflow barrier 2, composed of an epitaxial layer 2, the substrate 1, and the N-type semiconductor region 4. Consequently, voltage difference is not produced, even if the exposed part to the scribed surface 5 of each PN-junction is rough, and it becomes possible to prevent leakage currents from flowing.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、固体撮像素子、特
にオーバーフローバリアを成し半導体基板及び光電変換
部とは逆導電型のエピタキシャル層を有する縦型オーバ
ーフロードレイン方式の固体撮像素子に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a solid-state imaging device, and more particularly to a vertical overflow drain type solid-state imaging device which forms an overflow barrier and has an epitaxial layer of a conductivity type opposite to that of a semiconductor substrate and a photoelectric conversion portion.

【0002】[0002]

【背景技術】固体撮像素子として、受光部での余剰の電
荷を基板側に排出するようにした、所謂縦型オーバーフ
ロードレイン方式の固体撮像素子が知られており、基板
側への電荷の流れに対しての障壁となるオーバーフロー
バリアは従来においては高エネルギーのイオン注入によ
り基板表面から深いところに形成するようにしていた。
2. Description of the Related Art As a solid-state imaging device, a so-called vertical overflow drain type solid-state imaging device in which excess charge in a light receiving section is discharged to a substrate side is known. Conventionally, the overflow barrier serving as a barrier is formed deep from the substrate surface by high-energy ion implantation.

【0003】しかし、イオン注入によれば、オーバーフ
ローバリアを最大でも5μm程度の深さのところにしか
できず、オーバーフローバリアの形成位置の深さを深く
することに限界がある。
However, according to ion implantation, the overflow barrier can be formed only at a depth of about 5 μm at the maximum, and there is a limit in increasing the depth of the overflow barrier formation position.

【0004】一方、固体撮像素子として可視光のみなら
ず近赤外線に対しても感度を有するものの要求がある
が、そのような固体撮像素子はオーバーフローバリアの
深さをより深くする必要があり、イオン注入による形成
方法によっては必要な深さにすることが不可能乃至困難
である。そこで、エピタキシャル層によりオーバーフロ
ーバリアを形成することにより、バリアの深さを任意の
深さにすることが試みられた。
On the other hand, there is a demand for a solid-state imaging device having sensitivity not only to visible light but also to near-infrared light. In such a solid-state imaging device, it is necessary to make the overflow barrier deeper. It is impossible or difficult to achieve the required depth depending on the formation method by implantation. Therefore, attempts have been made to make the depth of the barrier arbitrary by forming an overflow barrier using an epitaxial layer.

【0005】[0005]

【発明が解決しようとする課題】ところが、そのような
固体撮像素子には、図3に示すように、ウェハをスクラ
イブによりチップ化したときスクライブ面にエピタキシ
ャル層によるPN接合が露出し、半導体基板・接地間で
のリーク電流が生じるという新たな問題が生じた。
However, in such a solid-state imaging device, as shown in FIG. 3, when a wafer is chipped by scribing, a PN junction by an epitaxial layer is exposed on a scribe surface, and the semiconductor substrate and the semiconductor substrate are exposed to light. There is a new problem that a leakage current occurs between the grounds.

【0006】図3において、1はN型半導体基板、2は
エピタキシャル層からなるP型オーバーフローバリア、
3はP+ 型チャンネルストッパ、4はN型半導体領域の
周辺部分、5はスクライブ面であり、基板1とオーバー
フローバリア2との間のPN接合に基板バイアス電圧V
subによるリーク電流が流れる。スクライブ面5は荒
れた面なので、そのリーク電流の大きさは正常な動作を
阻むほど大きい。
In FIG. 3, 1 is an N-type semiconductor substrate, 2 is a P-type overflow barrier made of an epitaxial layer,
Reference numeral 3 denotes a P + type channel stopper, 4 denotes a peripheral portion of an N type semiconductor region, 5 denotes a scribe surface, and a substrate bias voltage V is applied to a PN junction between the substrate 1 and the overflow barrier 2.
A leak current due to the sub flows. Since the scribe surface 5 is a rough surface, the magnitude of the leak current is large enough to prevent normal operation.

【0007】このような問題が生じるのは次の理由によ
る。即ち、従来のようにオーバーフローバリアを、イオ
ン注入により形成した場合には、マスク越しにイオン注
入することによりイオン注入場所を選択し、スクライブ
面にオーバーフローバリアと、基板等とによるPN接合
が露出しないようにすることができるが、エピタキシャ
ル層により形成した場合には、オーバーフローバリアが
全面的に形成されてしまうことになり、該バリアと、基
板等とによるPN接合がスクライブ面に露出することを
避けることは不可能であるからである。
[0007] Such a problem occurs for the following reason. That is, when the overflow barrier is formed by ion implantation as in the related art, the ion implantation site is selected by ion implantation through a mask, and the PN junction between the overflow barrier and the substrate or the like is not exposed on the scribe surface. However, when formed by an epitaxial layer, an overflow barrier is formed over the entire surface, and the PN junction between the barrier and the substrate is prevented from being exposed on the scribe surface. It is impossible.

【0008】そこで、本願発明者はオーバーフローバリ
アを成すエピタキシャル層が(換言すると、エピタキシ
ャル層と基板等との間のPN接合が)スクライブ面に露
出してもリーク電流が流れないようにすべく模索し、オ
ーバーフローバリアのスクライブ面に露出する部分を完
全空乏化することによりそれを成すことができるという
着想を得たうえでさらに考察を重ねて本発明を成すに至
った。
Therefore, the present inventor has sought to prevent leakage current from flowing even when the epitaxial layer forming the overflow barrier (in other words, the PN junction between the epitaxial layer and the substrate or the like) is exposed on the scribe surface. However, the inventors of the present invention obtained the idea that this can be achieved by completely depleting the portion of the overflow barrier that is exposed on the scribed surface.

【0009】即ち、本発明はオーバーフローバリアを成
し半導体基板及び光電変換部とは逆導電型のエピタキシ
ャル層を有する縦型オーバーフロードレイン方式の固体
撮像素子において、オーバーフローバリアを成すエピタ
キシャル層のスクライブ面への露出部におけるリーク電
流をなくすことを目的とする。
That is, the present invention relates to a vertical overflow drain type solid-state imaging device having an overflow barrier and an epitaxial layer of a conductivity type opposite to that of a semiconductor substrate and a photoelectric conversion portion. The purpose of the present invention is to eliminate the leakage current in the exposed part of the above.

【0010】[0010]

【課題を解決するための手段】請求項1の固体撮像素子
は、素子周辺近傍に上記半導体基板および光電変換部と
同じ導電型のリング状領域を形成し、該リング状領域及
び上記半導体基板と、上記オーバーフローバリアを成す
エピタキシャル層との間に、上記半導体基板と上記リン
グ状領域との間を完全空乏化する電圧を印加するように
してなることを特徴とする。
According to a first aspect of the present invention, there is provided a solid-state imaging device, wherein a ring-shaped region having the same conductivity type as that of the semiconductor substrate and the photoelectric conversion portion is formed in the vicinity of the device. A voltage for completely depleting the space between the semiconductor substrate and the ring-shaped region is applied between the epitaxial layer forming the overflow barrier and the epitaxial layer.

【0011】従って、請求項1の固体撮像素子によれ
ば、リング状領域及び半導体基板と、オーバーフローバ
リアを成すエピタキシャル層との間に印加された電圧に
より素子周辺近傍に設けたリング状領域と基板との間が
完全空乏化するので、スクライブ面に露出する、エピタ
キシャル層と半導体基板等との間のPN接合には電位差
の存在しない状態になり、延いてはリーク電流が流れな
い。
Therefore, according to the solid-state imaging device of the first aspect, the ring-shaped region and the substrate provided in the vicinity of the device by the voltage applied between the ring-shaped region and the semiconductor substrate and the epitaxial layer forming the overflow barrier. Is completely depleted, so that there is no potential difference at the PN junction between the epitaxial layer and the semiconductor substrate, etc., which is exposed on the scribe surface, so that no leak current flows.

【0012】[0012]

【発明の実施の形態】以下、本発明を図示実施の形態に
従って詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention will be described in detail with reference to the illustrated embodiments.

【0013】図1(A)、(B)は本発明固体撮像素子
の第1の実施の形態を示すもので、(A)は平面図、
(B)は(A)のB−B′線視拡大断面図であり、図2
は動作時のポテンシャル等高線を示す断面図である。
FIGS. 1A and 1B show a first embodiment of a solid-state imaging device according to the present invention, wherein FIG.
FIG. 2B is an enlarged sectional view taken along line BB ′ of FIG.
FIG. 4 is a cross-sectional view showing potential contours during operation.

【0014】図において、1はN型半導体基板、2はエ
ピタキシャル層からなるP型オーバーフローバリアで、
半導体表面から例えば2〜5μm程度あるいはそれ以上
の深さのところに形成され、厚さは例えば1μm乃至そ
れ以下である。該バリア2の不純物濃度は例えば1015
/cm3 程度である。3はP+ 型チャンネルストッパ、
4はN型半導体領域の周辺部分、5はスクライブ面であ
る。
In the figure, 1 is an N-type semiconductor substrate, 2 is a P-type overflow barrier composed of an epitaxial layer,
It is formed at a depth of, for example, about 2 to 5 μm or more from the semiconductor surface, and has a thickness of, for example, 1 μm to less. The impurity concentration of the barrier 2 is, for example, 10 15
/ Cm 3 . 3 is a P + type channel stopper,
4 is a peripheral portion of the N-type semiconductor region, and 5 is a scribe surface.

【0015】6は素子の上記N型半導体領域の周辺部分
4の表面部において周辺近傍に、具体的には例えば素子
側面(スクライブ面)5から10μm程度内側に寄った
ところに形成されたリング状のN+ 型領域である。この
ように、リング状のN+ 型領域6を有するのが本固体撮
像素子の特徴であり、そして、使用時には、該N+ 型領
域6に、半導体基板1に印加される基板バイアス電圧V
subが印加されるようになっている。それ以外の点で
は図3に示す固体撮像素子と特に異なるところはない。
勿論、オーバーフローバリア2への接地電位(0V)の
付与はチャンネルストッパ3を通じて為される。
Reference numeral 6 denotes a ring formed on the surface of the peripheral portion 4 of the N-type semiconductor region of the element, in the vicinity of the periphery, specifically, for example, at a position inward of the element side surface (scribed surface) 5 by about 10 μm. N + type region. As described above, the solid-state imaging device is characterized by having the ring-shaped N + -type region 6. In use, the substrate bias voltage V applied to the semiconductor substrate 1 is applied to the N + -type region 6.
The sub is applied. In other respects, there is no particular difference from the solid-state imaging device shown in FIG.
Of course, the ground potential (0 V) is applied to the overflow barrier 2 through the channel stopper 3.

【0016】従って、使用時における素子周辺部のポテ
ンシャル等高線は図2に示すようになり[V1=Vsu
b・1/5(例えばVsubが15Vの場合には3V)
の等高線、V2=Vsub・2/5(例えばVsubが
15Vの場合には6V)の等高線、・・・]、リング状
のN+ 型領域6と基板1との間が完全空乏化され、エピ
タキシャル層2からなるオーバーフローバリア2と、基
板1及びN型半導体領域4との間のPN接合には電位差
が生じない。従って、そのPN接合のスクライブ面5へ
の露出部が荒れていてもその間には電位差が生じていな
いのでリーク電流は流れない。
Therefore, the potential contours at the periphery of the device during use are as shown in FIG. 2 [V1 = Vsu
b 1/5 (for example, 3 V when Vsub is 15 V)
, A contour line of V2 = Vsub · 2/5 (for example, 6 V when Vsub is 15 V),...], The space between the ring-shaped N + type region 6 and the substrate 1 is completely depleted, and epitaxial No potential difference occurs at the PN junction between the overflow barrier 2 composed of the layer 2 and the substrate 1 and the N-type semiconductor region 4. Therefore, even if the exposed portion of the PN junction on the scribe surface 5 is rough, no leakage current flows because no potential difference occurs between the exposed portions.

【0017】しかして、本固体撮像素子によれば、オー
バーフローバリア2を選択的形成が不可能なエピタキシ
ャル層により形成することがリーク電流の発生のおそれ
を伴うことなく可能になる。
Thus, according to the present solid-state imaging device, it is possible to form the overflow barrier 2 from an epitaxial layer that cannot be selectively formed without causing a risk of generating a leak current.

【0018】従って、オーバーフローバリア2の深さ、
広がり等不純物濃度の深さ方向のプロファイルの設計の
自由度が顕著に高まり、オーバーフローバリア2を深く
することにより近赤外線に対する感度の高い近赤外線用
固体撮像素子を簡単に実現することができる。
Therefore, the depth of the overflow barrier 2,
The degree of freedom in designing the profile in the depth direction of the impurity concentration such as the spread is remarkably increased, and by making the overflow barrier 2 deep, a solid-state imaging device for near infrared having high sensitivity to near infrared can be easily realized.

【0019】[0019]

【発明の効果】請求項1の固体撮像素子によれば、オー
バーフローバリアを成すエピタキシャル層との間に印加
された電圧により素子周辺近傍に設けたリング状領域と
基板との間が完全空乏化するので、スクライブ面に露出
する、エピタキシャル層と基板等との間のPN接合には
電位差のない状態になり、延いてはリーク電流が流れな
い。
According to the solid-state imaging device of the first aspect, the voltage between the epitaxial layer forming the overflow barrier and the substrate is completely depleted between the ring-shaped region provided in the vicinity of the device and the substrate. Therefore, there is no potential difference at the PN junction between the epitaxial layer and the substrate, etc., which is exposed on the scribe surface, and no leak current flows.

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

【図1】(A)、(B)は本発明固体撮像素子の第1の
実施の形態を示すもので、(A)は平面図、(B)は
(A)のB−B′線視拡大断面図である。
FIGS. 1A and 1B show a first embodiment of a solid-state imaging device according to the present invention, in which FIG. 1A is a plan view, and FIG. 1B is a view taken along line BB ′ of FIG. It is an expanded sectional view.

【図2】使用時における周辺部のポテンシャル等高線を
示す断面図である。
FIG. 2 is a cross-sectional view showing potential contours in a peripheral portion during use.

【図3】背景技術の問題点を示す断面図である。FIG. 3 is a cross-sectional view showing a problem of the background art.

【符号の説明】[Explanation of symbols]

1・・・基板、2・・・オーバーフローバリア、5・・
・スクライブ面、Vsub・・・基板バイアス電圧。
1 ... substrate, 2 ... overflow barrier, 5 ...
-Scribe surface, Vsub ... substrate bias voltage.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 オーバーフローバリアを成し半導体基板
及び光電変換部とは逆導電型のエピタキシャル層を有す
る縦型オーバーフロードレイン方式の固体撮像素子であ
って、 素子周辺近傍に上記半導体基板および光電変換部と同じ
導電型のリング状領域を形成し、 上記リング状領域及び上記半導体基板と、上記オーバー
フローバリアを成すエピタキシャル層との間に、上記半
導体基板と上記リング状領域との間を完全空乏化する電
圧を印加するようにしてなることを特徴とする固体撮像
素子
1. A vertical overflow drain type solid-state imaging device having an epitaxial layer of an opposite conductivity type to a semiconductor substrate and a photoelectric conversion unit, forming an overflow barrier, wherein the semiconductor substrate and the photoelectric conversion unit are provided near the periphery of the device. Forming a ring-shaped region having the same conductivity type as that of the above, and completely depleting the space between the semiconductor substrate and the ring-shaped region between the ring-shaped region and the semiconductor substrate and the epitaxial layer forming the overflow barrier. A solid-state imaging device characterized in that a voltage is applied.
【請求項2】 リング状領域及び半導体基板には基板バ
イアス電位を、上記オーバーフローバリアを成すエピタ
キシャル層にはこれと同じ導電型のチャンネルストッパ
を介して接地電位を与えるようにしてなることを特徴と
する請求項1記載の固体撮像素子
2. The substrate bias potential is applied to the ring-shaped region and the semiconductor substrate, and the ground potential is applied to the epitaxial layer forming the overflow barrier via a channel stopper of the same conductivity type as the epitaxial layer. The solid-state imaging device according to claim 1,
JP24336796A 1996-09-13 1996-09-13 Solid-state imaging device Expired - Fee Related JP3584629B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24336796A JP3584629B2 (en) 1996-09-13 1996-09-13 Solid-state imaging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24336796A JP3584629B2 (en) 1996-09-13 1996-09-13 Solid-state imaging device

Publications (2)

Publication Number Publication Date
JPH1093064A true JPH1093064A (en) 1998-04-10
JP3584629B2 JP3584629B2 (en) 2004-11-04

Family

ID=17102794

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24336796A Expired - Fee Related JP3584629B2 (en) 1996-09-13 1996-09-13 Solid-state imaging device

Country Status (1)

Country Link
JP (1) JP3584629B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006147758A (en) * 2004-11-18 2006-06-08 Sony Corp Solid state imaging device and its manufacturing method
JP2006147757A (en) * 2004-11-18 2006-06-08 Sony Corp Solid state imaging device and its manufacturing method
CN104362164A (en) * 2014-11-21 2015-02-18 北京思比科微电子技术股份有限公司 Back lighting type image sensor structure capable of improving saturation throughput

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006147758A (en) * 2004-11-18 2006-06-08 Sony Corp Solid state imaging device and its manufacturing method
JP2006147757A (en) * 2004-11-18 2006-06-08 Sony Corp Solid state imaging device and its manufacturing method
JP4561328B2 (en) * 2004-11-18 2010-10-13 ソニー株式会社 Solid-state imaging device and manufacturing method thereof
CN104362164A (en) * 2014-11-21 2015-02-18 北京思比科微电子技术股份有限公司 Back lighting type image sensor structure capable of improving saturation throughput

Also Published As

Publication number Publication date
JP3584629B2 (en) 2004-11-04

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