JPH0567798A - Photo detector and manufacture of photo detector - Google Patents
Photo detector and manufacture of photo detectorInfo
- Publication number
- JPH0567798A JPH0567798A JP3226025A JP22602591A JPH0567798A JP H0567798 A JPH0567798 A JP H0567798A JP 3226025 A JP3226025 A JP 3226025A JP 22602591 A JP22602591 A JP 22602591A JP H0567798 A JPH0567798 A JP H0567798A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- impurity diffusion
- conductivity type
- receiving element
- light
- 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.)
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- Light Receiving Elements (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、光通信、光記録、光情
報処理等に用いる半導体受光素子、その受光素子の製造
方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor light receiving element used for optical communication, optical recording, optical information processing, etc., and a method for manufacturing the light receiving element.
【0002】[0002]
【従来の技術】従来より、上記のような技術分野におけ
る受光素子としては、半導体のPN接合やショットキー
接合を用いたフォトダイオードが多く用いられる。中で
もPINフォトダイオードは高量子効率、小暗電流、小
動作電圧でかつ高速応答が可能であるため多用されてい
る(「光通信素子工学」米津宏雄著、工学図書株式会社
版参照)。2. Description of the Related Art Conventionally, as a light receiving element in the above technical field, a photodiode using a semiconductor PN junction or a Schottky junction is often used. Among them, PIN photodiodes are widely used because of their high quantum efficiency, small dark current, small operating voltage and high-speed response (see "Optical Communication Device Engineering" written by Hiroo Yonezu, Engineering Book Co., Ltd. edition).
【0003】その構造の一例として、シリコンPINフ
ォトダイオードの縦断面図を図7に示す。このシリコン
PINフォトダイオードは、基板100として第1導電
型のシリコン基板を用いる。基板100は低抵抗層11
0の上に高抵抗層120を形成して構成されている。基
板100の一部の表面付近には、第2導電型の不純物拡
散層120が形成され、受光部を形成している。この基
板100の表面は絶縁膜130で覆われ、不純物拡散層
120は、絶縁膜130の一部を除去した接続部90を
通して電極140と電気的に接続されている。又、基板
100の裏面等に接続して設けられた図示しない電極と
対になって受光素子の2つの端子が構成されている。な
お、図8にシリコンPINフォトダイオードの波長と量
子効率(感度)との関係を示す。As an example of the structure, a vertical sectional view of a silicon PIN photodiode is shown in FIG. In this silicon PIN photodiode, a silicon substrate of the first conductivity type is used as the substrate 100. The substrate 100 is the low resistance layer 11
0 is formed with a high resistance layer 120. A second conductive type impurity diffusion layer 120 is formed near a part of the surface of the substrate 100 to form a light receiving portion. The surface of the substrate 100 is covered with an insulating film 130, and the impurity diffusion layer 120 is electrically connected to the electrode 140 through the connection portion 90 from which a part of the insulating film 130 is removed. Further, two terminals of the light receiving element are formed by pairing with an electrode (not shown) provided by being connected to the back surface of the substrate 100 or the like. Note that FIG. 8 shows the relationship between the wavelength of the silicon PIN photodiode and the quantum efficiency (sensitivity).
【0004】[0004]
【発明が解決しようとする課題】しかしながら、前述の
PINフォトダイオードにおいては、入射した光のう
ち、光電流出力に寄与するのは、主として空乏層108
(破線で示す)内で吸収される光により生じる電子−ホ
ール対である。この空乏層108の上下両側において
も、それぞれの空乏層108端から少数キャリアの拡散
長程度以内で吸収された光により生じた少数キャリア
が、拡散により空乏層108に到達して光電流となり得
るが、拡散の速度が遅いため、高速動作時には有効な光
電流出力とはなり得ない。However, in the PIN photodiode described above, it is mainly the depletion layer 108 that contributes to the photocurrent output of the incident light.
It is an electron-hole pair generated by the light absorbed in (shown by the broken line). On both the upper and lower sides of the depletion layer 108, minority carriers generated by light absorbed within the diffusion length of minority carriers from the end of each depletion layer 108 may reach the depletion layer 108 by diffusion and become a photocurrent. Since the diffusion speed is slow, the effective photocurrent output cannot be achieved at high speed operation.
【0005】一方、最近、種々の青色発光素子や第2高
調波発生素子による緑、青色発光源の開発が盛んであ
り、これを光記録や光情報処理等に用いるためにはその
受光素子が必要となる。このような受光素子に、製造プ
ロセスや製品の安定性、他の電子素子との集積化等の要
求からシリコンを用いようとする場合、次のような問題
がある。On the other hand, recently, development of green and blue light emitting sources by various blue light emitting elements and second harmonic generating elements has been actively made, and in order to use them for optical recording and optical information processing, the light receiving elements are Will be needed. When silicon is used for such a light receiving element due to the requirements of manufacturing process, product stability, integration with other electronic elements, etc., there are the following problems.
【0006】即ち、シリコンの光の吸収長が、波長0.
5μmで1μm程度、波長0.4μmで0.2μm以下
であるため、上述のような関係から従来のフォトダイオ
ード構造では短波長側の感度が著しく低下してしまう。
なぜなら、前述の構造において第2導電型の不純物拡散
層120は、通常の製造プロセスによれば1μm程度の
厚さになるため、光が空乏層108に達する以前に吸収
されてしまうからである。このため、短波長側の感度を
向上させるには、受光部の第2導電型の不純物拡散層1
20をできるだけ薄くする必要がある。That is, the absorption length of light of silicon has a wavelength of 0.
Since it is about 1 μm at 5 μm and 0.2 μm or less at the wavelength of 0.4 μm, the sensitivity on the short wavelength side is remarkably lowered in the conventional photodiode structure due to the above relationship.
This is because, in the above-described structure, the second conductivity type impurity diffusion layer 120 has a thickness of about 1 μm according to a normal manufacturing process, and thus light is absorbed before reaching the depletion layer 108. Therefore, in order to improve the sensitivity on the short wavelength side, the second conductivity type impurity diffusion layer 1 of the light receiving portion is required.
It is necessary to make 20 as thin as possible.
【0007】これに対する1つのアプローチとして特開
平2−20073号に示されている方法がある。この方
法は、n導電型の配向シリコン単結晶内にB+イオンを
注入することにより平坦なpn接合を形成し、その際生
じた比較的低いp型ドーピングを有する上層を、比較的
高いp+型ドーピングを有するより深い個所に存在する
層の領域まで異方性エッチングにより削り取ることによ
り、極めて薄いpn接合を形成する方法である。As an approach to this, there is a method disclosed in Japanese Patent Laid-Open No. 200733. According to this method, a flat pn junction is formed by implanting B + ions into an n-conducting oriented silicon single crystal, and an upper layer having a relatively low p-type doping generated at that time is replaced with a relatively high p +. This is a method of forming an extremely thin pn junction by shaving off a region of a layer existing at a deeper portion having type doping by anisotropic etching.
【0008】しかし、この方法では、B+イオンを3
0keV程度の比較的低加速電圧でイオン注入すること
の問題、B+注入層の深部側への据引き分の厚さが残
存する問題、受光部のシリコン表面をエッチングによ
り削り取ったことによる表面状態(界面状態)の劣化が
表面再結合を増加させ感度を低下させる問題等の問題が
ある。又、N型不純物としてAs+、あるいは、P型不
純物としてBF2+をイオン注入して浅い接合を形成する
技術を利用することも考えられるが、上述のように薄い
拡散層を形成しようとすると、注入イオン量を多くでき
ず、拡散層のシート抵抗を下げることができない。この
問題はイオン注入以外の他の浅い接合の形成方法による
場合でも同様に起こり、受光部のシート抵抗の増大は、
受光素子の動作に悪影響を及ぼす。However, in this method, B + ions are
Problems of ion implantation at a relatively low acceleration voltage of about 0 keV, problems of residual thickness of the B + implantation layer on the deep side, and surface condition caused by etching off the silicon surface of the light receiving part. There is a problem that deterioration of (interface state) increases surface recombination and lowers sensitivity. Further, As + as the N-type impurity, or when it is also conceivable to use a technique of forming a shallow junction by implanting BF 2 + as a P-type impurity, an attempt to form a thin diffusion layer as described above However, the amount of implanted ions cannot be increased, and the sheet resistance of the diffusion layer cannot be reduced. This problem also occurs when using a shallow junction forming method other than ion implantation, and the increase in sheet resistance of the light receiving portion is
It adversely affects the operation of the light receiving element.
【0009】本発明の目的は上記のような問題を解決
し、受光部拡散部分を薄くして、短波長の光も空乏層で
吸収されるような部分を有しながら、全体として受光部
拡散部分の抵抗を低くすることのできる受光素子と、そ
の製造方法を提案することにある。The object of the present invention is to solve the above problems and to thin the light receiving portion diffusion portion so that the light receiving portion diffuses as a whole while having a portion where short wavelength light is also absorbed by the depletion layer. It is to propose a light receiving element that can reduce the resistance of a part and a manufacturing method thereof.
【0010】[0010]
【課題を解決するための手段】請求項1記載の発明は、
第1導電型の基板表面近傍に形成する第2導電型の不純
物拡散層を比較的厚い層と比較的薄い層とが周期的に配
置された構造とされている。請求項2記載の発明の構成
は、上記の周期的な構造の周期が形成される方向をそれ
らの第2導電型不純物拡散層と外部への電極とが接続さ
れる部分に向かう方向に略垂直としたものである。The invention according to claim 1 is
The second conductivity type impurity diffusion layer formed in the vicinity of the surface of the first conductivity type substrate has a structure in which relatively thick layers and relatively thin layers are periodically arranged. According to a second aspect of the present invention, the direction in which the period of the periodic structure is formed is substantially perpendicular to the direction in which the second conductivity type impurity diffusion layer and the electrode to the outside are connected. It is what
【0011】請求項3記載の発明の構成は、前記の第2
導電型不純物拡散層と外部への電極とが接続される部分
においては、前記第2導電型不純物拡散層をその比較的
厚い層としておくものである。請求項4記載の受光素子
の製造方法は、基板表面に形成した第1形状のマスク層
により規定される平面形状で第2導電型の不純物拡散層
の比較的厚い層に対応する部分を形成した後、新たに形
成した第2形状のマスク層により規定される平面形状で
第2導電型の不純物拡散層の比較的薄い層および比較的
厚い層を形成する方法である。According to a third aspect of the invention, there is provided the above-mentioned second aspect.
In the portion where the conductivity type impurity diffusion layer and the electrode to the outside are connected, the second conductivity type impurity diffusion layer is made a relatively thick layer. According to a fourth aspect of the present invention, there is provided a method of manufacturing a light receiving element, wherein a portion corresponding to a relatively thick layer of a second conductivity type impurity diffusion layer is formed in a plane shape defined by a first shape mask layer formed on a surface of a substrate. After that, it is a method of forming a relatively thin layer and a relatively thick layer of the second-conductivity-type impurity diffusion layer having a planar shape defined by the newly formed second-shaped mask layer.
【0012】請求項5記載の受光素子の製造方法は、基
板表面に形成したマスク層により規定される平面形状で
第2導電型の不純物拡散層の比較的厚い層に対応する部
分を形成した後、熱処理を行なうことにより、第2導電
型の不純物拡散層の比較的薄い層および比較的厚い層を
形成する方法である。請求項6記載の受光素子の製造方
法は、基板表面に形成した、第1形状の比較的薄い部分
と第2形状の比較的厚い部分とを有するマスク層を用い
て第2導電型の不純物を拡散することにより、比較的薄
い層および比較積に厚い層を有する第2導電型の不純物
拡散層を形成する方法である。According to a fifth aspect of the present invention, there is provided a method for manufacturing a light receiving element, wherein after forming a portion corresponding to a relatively thick layer of the second-conductivity-type impurity diffusion layer having a planar shape defined by a mask layer formed on the substrate surface. In this method, a relatively thin layer and a relatively thick layer of the second conductivity type impurity diffusion layer are formed by performing heat treatment. According to a sixth aspect of the present invention, there is provided a method of manufacturing a light receiving element, wherein a mask layer having a relatively thin portion having a first shape and a relatively thick portion having a second shape is formed on a surface of a substrate to remove impurities of a second conductivity type. This is a method of forming a second conductivity type impurity diffusion layer having a relatively thin layer and a comparatively thick layer by diffusion.
【0013】[0013]
【作用】請求項1記載の発明によれば、比較的薄い層は
その厚さを所望の受光波長の吸収長よりも薄くすること
により、その部分で光が空乏層まで達してから吸収され
る割合が大となり、発生した電子−ホール対は空乏層内
をドリフトにより高速に移動して、電子はN型領域に、
ホールはP型領域へたどりつく。一方、比較的厚い層は
不純物が多く、深く拡散されているのでその部分の抵抗
を十分に小さくすることができる。したがって上記のよ
うな比較的薄い層と比較的厚い層とを周期的に配置する
ことにより、薄い部分で吸収された短波長の光により発
生したキャリアを近傍の厚い部分の低抵抗部分を介して
伝達できるので、短波長の光にも感度を有し、かつ高速
応答が可能な受光素子が得られる。According to the invention described in claim 1, by making the thickness of the relatively thin layer thinner than the absorption length of a desired light receiving wavelength, light is absorbed at that portion after reaching the depletion layer. The ratio becomes large, and the generated electron-hole pairs move at high speed due to drift in the depletion layer, and the electrons move to the N-type region,
The holes reach the P-type region. On the other hand, the relatively thick layer has a large amount of impurities and is deeply diffused, so that the resistance of that portion can be made sufficiently small. Therefore, by periodically arranging the relatively thin layer and the relatively thick layer as described above, the carriers generated by the light of the short wavelength absorbed in the thin portion are passed through the low resistance portion of the thick portion in the vicinity. Since the light can be transmitted, it is possible to obtain a light receiving element which is sensitive to light having a short wavelength and can respond at high speed.
【0014】請求項2記載の発明によれば、短波長の光
を吸収する比較的薄い層の面積(受光面積)を最大限に
大きくしながら、かつ光電流の外部への取り出しのため
の低抵抗層を成す比較的厚い層の面積を最小限にするこ
とができる。請求項3記載の発明によれば、電極が接続
される部分は低抵抗の半導体層となるため、オーミック
コンタクトが得られ易くなると共に、電極のメタル等と
シリコン等の半導体の合金化によるPN接合の破壊を未
然に防ぐことができる。もちろんこの問題のためには半
導体層と電極のメタル層との間にバリア層を設けること
も有効ではあるが、本構成によれば製造工程の増加がな
く、簡便である。According to the second aspect of the present invention, the area (light receiving area) of the relatively thin layer that absorbs light of a short wavelength is maximized, and at the same time, it is low for extracting the photocurrent to the outside. The area of the relatively thick layer forming the resistive layer can be minimized. According to the third aspect of the invention, since the portion to which the electrode is connected is a low-resistance semiconductor layer, ohmic contact is easily obtained, and a PN junction is formed by alloying the metal of the electrode and a semiconductor such as silicon. You can prevent the destruction of. Of course, for this problem, it is effective to provide a barrier layer between the semiconductor layer and the metal layer of the electrode, but according to this configuration, there is no increase in the number of manufacturing steps and it is simple.
【0015】請求項4記載の発明の方法により、不純物
拡散層の比較的厚い層と比較的薄い層とをそれぞれほぼ
独立した拡散条件により形成できるので、製造条件の幅
が広くなる。請求項5記載の発明の方法により、1形状
のマスクで上記の受光素子を製造できる。又、極めて薄
い不純物拡散層が形成可能である。請求項6記載の発明
の方法により、1度の不純物導入工程により上記の受光
素子が製造できる。According to the method of the fourth aspect of the present invention, since the relatively thick layer and the relatively thin layer of the impurity diffusion layer can be formed under substantially independent diffusion conditions, the range of manufacturing conditions is widened. According to the method of the invention described in claim 5, the above-mentioned light receiving element can be manufactured with a mask having one shape. Also, an extremely thin impurity diffusion layer can be formed. According to the method of the sixth aspect of the present invention, the light receiving element can be manufactured by a single impurity introduction step.
【0016】[0016]
【実施例】以下、本発明の実施例を説明する。図1は、
本発明の第1実施例に係る受光素子の構成を示す縦断面
図である。本実施例の受光素子は、基板10として第1
導電型のシリコン基板を用いる。基板10は低抵抗層1
1の上に高抵抗層12を形成して構成されている。ま
た、第1導電型の半導体基板10の高抵抗層12の表面
付近に第2導電型の不純物拡散層20が形成されてい
る。第2導電型の不純物拡散層20は、その比較的厚い
層21と比較的薄い層22とで形成され、周期的な構造
となっており、それらは受光部を成している。この基板
10の表面は絶縁膜30で覆われ、不純物拡散層20
は、絶縁膜30の一部を除去した接続部を通して電極と
電気的に接続されている。又、基板10の裏面等に接続
して設けられた図示しない電極と対になって受光素子の
2つの端子が構成されている。EXAMPLES Examples of the present invention will be described below. Figure 1
FIG. 3 is a vertical cross-sectional view showing the configuration of the light receiving element according to the first embodiment of the present invention. The light receiving element of this embodiment has the first substrate 10
A conductive silicon substrate is used. Substrate 10 is low resistance layer 1
1 on which a high resistance layer 12 is formed. Further, the second conductivity type impurity diffusion layer 20 is formed in the vicinity of the surface of the high resistance layer 12 of the first conductivity type semiconductor substrate 10. The second conductivity type impurity diffusion layer 20 is formed of a relatively thick layer 21 and a relatively thin layer 22 and has a periodic structure, and they form a light receiving portion. The surface of the substrate 10 is covered with an insulating film 30, and the impurity diffusion layer 20
Are electrically connected to the electrodes through the connection part obtained by removing a part of the insulating film 30. Further, two terminals of the light receiving element are formed by pairing with an electrode (not shown) connected to the back surface of the substrate 10 or the like.
【0017】受光部の周期的な構造は、縞状、格子状、
放射状、同心円状あるいはそれらの組み合せにより任意
に構成できる。又、比較的厚い層21と比較的薄い層2
2とは二値的に区別される必要はなく、その厚さが連続
的に変化したものとして形成しても良い。更にそれら各
々の面積比率は、短波長光に有効な受光面と低抵抗部分
との兼ね合いで任意に設定できる。ただし、比較的薄い
層22の部分に入射し、多くを空乏層内で吸収された電
子又はホール(導電型により異なる)が比較的厚い層2
1の低抵抗の部分により光電流として伝達される、本発
明の原理は変らない。The periodic structure of the light receiving portion is striped, grid-shaped,
Radial, concentric, or a combination thereof can be arbitrarily configured. Also, a relatively thick layer 21 and a relatively thin layer 2
It is not necessary to be binary-differentiated from 2, and the thickness may be continuously changed. Further, the area ratio of each of them can be arbitrarily set in consideration of the light receiving surface effective for short wavelength light and the low resistance portion. However, the electrons or holes (depending on the conductivity type) that are incident on the relatively thin layer 22 and are mostly absorbed in the depletion layer 2 are relatively thick.
The principle of the invention, which is transmitted as photocurrent by the low resistance part of 1, remains unchanged.
【0018】図2は本発明の第2実施例に係る受光素子
の平面図である。同図において、不純物拡散層20は、
絶縁膜30に設けた開孔部33を通し、接続部92の部
分で外部へ引き出されるメタル等の電極40と接続して
いる。そこで比較的厚い層21と比較的薄い層22を縞
状の周期構造とし、その周期の方向を接続部92へ向か
う方向と略垂直にする、即ち各縞状部分を接続部92へ
略向かう方向として比較的薄い層22の面積を確保しつ
つ、比較的厚い層21の接続部92への光電流伝達の効
率を上げている。図2では矩形の受光領域の一辺側で接
続をとる例を示したが、他に例えば円形の受光領域の外
周部で接続を行なうような場合には比較的厚い層21,
比較的薄い層22を放射線状あるいは扇状の周期的な構
造とする等、形態に合せて最適化することができる。FIG. 2 is a plan view of a light receiving element according to the second embodiment of the present invention. In the figure, the impurity diffusion layer 20 is
Through the opening portion 33 provided in the insulating film 30, the connection portion 92 is connected to the electrode 40 such as a metal which is drawn out to the outside. Therefore, the relatively thick layer 21 and the relatively thin layer 22 have a striped periodic structure, and the direction of the period is substantially perpendicular to the direction toward the connecting portion 92, that is, each striped portion is substantially toward the connecting portion 92. As a result, the efficiency of photocurrent transmission to the connection portion 92 of the relatively thick layer 21 is increased while ensuring the area of the relatively thin layer 22. In FIG. 2, an example is shown in which the connection is made on one side of the rectangular light receiving area, but in the case where the connection is made at the outer peripheral portion of the circular light receiving area, for example, a relatively thick layer 21,
The relatively thin layer 22 can be optimized according to the form, such as a radial or fan-shaped periodic structure.
【0019】図3は本発明の第3実施例に係る受光素子
の構成を説明するための図であり、図3(a)がその平
面図、図3(b)がその縦断面図である。この実施例で
は、不純物拡散層20と電極40との接続部93を少な
くとも含む不純物拡散層20の部分が、比較的厚い層2
1となっている。この場合、他の部分の不純物拡散層2
0の構造は任意であるが、それらのうちの比較的厚い層
21の部分が上記の接続部93を含む比較的厚い層21
の部分と接続している方が、光電流の伝達の点で有利で
ある。以上、第1〜第3実施例について、シリコンPI
Nフォトダイオードの例で示したが、他のフォトダイオ
ードでも本発明の構成は有効である。3A and 3B are views for explaining the structure of a light receiving element according to the third embodiment of the present invention. FIG. 3A is its plan view and FIG. 3B is its longitudinal sectional view. .. In this embodiment, the portion of the impurity diffusion layer 20 including at least the connecting portion 93 between the impurity diffusion layer 20 and the electrode 40 is a relatively thick layer 2.
It is 1. In this case, the impurity diffusion layer 2 in the other portion
The structure of 0 is arbitrary, but the portion of the relatively thick layer 21 among them includes the above-mentioned connecting portion 93.
It is more advantageous in connection with the part of (1) to transfer photocurrent. As described above, for the first to third embodiments, the silicon PI
Although the example of the N photodiode is shown, the configuration of the present invention is also effective for other photodiodes.
【0020】次に、以上のような構成の受光素子の製造
方法について述べる。図4は本発明の第4実施例に係る
受光素子の製造方法を説明するための図であり、図4
(a),(b)共に、製造工程の一部を示した縦断面図
である。この実施例の方法は、まず、マスク層81を基
板10表面に形成し、その形状により後の比較的厚い層
21に対応する、第2導電型の不純物拡散層211を形
成する(図4(a))。次に、マスク層81の一部又は
全部を取り除いた後、新たなマスク層82を形成し、こ
れを用いて比較的薄い層22および比較的厚い層21を
形成する(図4(b))。このように深い接合を形成し
た後、浅い接合を形成することで両者を混在させて形成
することができる。Next, a method of manufacturing the light-receiving element having the above structure will be described. FIG. 4 is a diagram for explaining the method of manufacturing the light receiving element according to the fourth embodiment of the present invention.
8A and 8B are vertical sectional views showing a part of the manufacturing process. In the method of this embodiment, first, the mask layer 81 is formed on the surface of the substrate 10, and the second conductivity type impurity diffusion layer 211 corresponding to the later relatively thick layer 21 due to its shape is formed (FIG. 4 ( a)). Next, after removing a part or all of the mask layer 81, a new mask layer 82 is formed and is used to form a relatively thin layer 22 and a relatively thick layer 21 (FIG. 4B). .. After forming the deep junction as described above, the shallow junction is formed, so that both can be formed in a mixed manner.
【0021】上記のような不純物拡散層の形成には、イ
オン注入後のアニール処理や、二段階拡散法あるいはド
ープドポリシリコンからの拡散等の半導体プロセス技術
が利用可能であり、マスク層も拡散方法に合せてレジス
トや酸化膜、窒化膜、アモルファスシリコン膜等を用い
ることができる。このとき誘電体膜を用いた場合、その
一部をフォトダイオードの絶縁膜30として残してもよ
い。又、マスク形状はマスク層の有無に限らず、マスク
層厚の差であってもよい。更に拡散工程において受光部
上の絶縁膜形成を同時に行なってもよい。In order to form the impurity diffusion layer as described above, it is possible to use an annealing process after ion implantation, a two-step diffusion method or a semiconductor process technique such as diffusion from doped polysilicon, and the mask layer is also diffused. Depending on the method, a resist, an oxide film, a nitride film, an amorphous silicon film or the like can be used. At this time, when a dielectric film is used, a part thereof may be left as the insulating film 30 of the photodiode. Further, the mask shape is not limited to the presence or absence of the mask layer, and may be the difference in the mask layer thickness. Further, the insulating film may be formed on the light receiving portion simultaneously in the diffusion process.
【0022】図5は本発明の第5実施例に係る受光素子
の製造方法を説明するための図であり、図5(a),
(b)共に、製造工程の一部を示した縦断面図である。
この実施例の方法は、先ず、前記第4実施例のマスク層
81と同様のマスク層83により第2導電型の不純物拡
散層211と同様の第2導電型の不純物拡散層212を
形成する(図5(a))。次いで不活性あるいは酸化性
のガス中で熱処理を行なう。これにより、第2導電型の
不純物拡散層212の部分からの不純物の拡散を引き続
き行ない、深さ方向と共に横方向への拡散が進み、隣接
する第2導電型の不純物拡散層212の中間の表面付近
で両方からの拡散層が接するまで行なうことにより比較
的厚い層21および比較的薄い層22を形成する(図5
(b))。FIG. 5 is a diagram for explaining a method of manufacturing a light receiving element according to the fifth embodiment of the present invention.
(B) Both are longitudinal sectional views showing a part of the manufacturing process.
In the method of this embodiment, first, a second conductivity type impurity diffusion layer 212 similar to the second conductivity type impurity diffusion layer 211 is formed by using the mask layer 83 similar to the mask layer 81 of the fourth embodiment ( FIG. 5A). Then, heat treatment is performed in an inert or oxidizing gas. As a result, the diffusion of impurities from the portion of the second-conductivity-type impurity diffusion layer 212 is continued, and the diffusion proceeds in the lateral direction along with the depth direction, and the intermediate surface of the adjacent second-conductivity-type impurity diffusion layer 212. A relatively thick layer 21 and a relatively thin layer 22 are formed by performing the process until the diffusion layers from both sides come into contact with each other in the vicinity (FIG.
(B)).
【0023】比較的薄い層22の部分では極めて薄い拡
散層を形成することも可能である。本実施例では、製造
に際してマスクは1形状のみで済む。この場合、あらか
じめ、第2導電型の不純物拡散層212の部分は幅狭に
かつ表面側程高濃度にしておき、その間隔を横方向への
拡散の広がりの2倍程度にしておくとよい。It is also possible to form an extremely thin diffusion layer in the portion of the relatively thin layer 22. In this embodiment, only one mask is required for manufacturing. In this case, it is preferable that the second conductivity type impurity diffusion layer 212 has a narrower width and a higher concentration on the surface side in advance, and the distance between them is about twice the spread of the diffusion in the lateral direction.
【0024】図6は本発明の第6実施例に係る受光素子
の製造方法を説明するための図であり、製造工程の一部
を示した縦断面図である。この実施例の方法は、マスク
層84の膜厚の差を利用して比較的厚い層21および比
較的薄い層22を同時に形成するものである。即ち、マ
スク層84を酸化シリコン膜等で形成し、イオン注入あ
るいは酸化シリコン膜を通した熱拡散により、不純物拡
散層20を形成する。このとき、マスク層84の厚い部
分の下では不純物拡散層20が形成されず、マスク層8
4の薄い部分の下では、比較的薄い層22が形成され、
かつマスク層が無いかあるいは更に薄い部分では比較的
厚い層21が形成されるよう、マスク層84厚差および
拡散条件を選ぶことにより、所望の構造が得られる。マ
スク層84のようなマスクは1つの材質で形成してもよ
いし、厚さの差の部分に応じて酸化膜とレジスト等、2
以上の材質の積層としてもよい。FIG. 6 is a view for explaining a method of manufacturing a light receiving element according to the sixth embodiment of the present invention, and is a vertical sectional view showing a part of the manufacturing process. In the method of this embodiment, the relatively thick layer 21 and the relatively thin layer 22 are simultaneously formed by utilizing the difference in the film thickness of the mask layer 84. That is, the mask layer 84 is formed of a silicon oxide film or the like, and the impurity diffusion layer 20 is formed by ion implantation or thermal diffusion through the silicon oxide film. At this time, the impurity diffusion layer 20 is not formed under the thick portion of the mask layer 84, and the mask layer 8 is formed.
Below the thin portion of 4, a relatively thin layer 22 is formed,
Moreover, a desired structure can be obtained by selecting the mask layer 84 thickness difference and diffusion conditions so that a relatively thick layer 21 is formed in a portion having no mask layer or a thinner layer. The mask such as the mask layer 84 may be formed of one material, or an oxide film and a resist, etc. may be formed depending on the difference in thickness.
It may be a laminate of the above materials.
【0025】[0025]
【発明の効果】請求項1記載の発明の構成により、短波
長の光も比較的薄い不純物拡散層を通り、その下の空乏
層で吸収され、高速移動できるキャリアを発生して光電
流に寄与し、その光電流を比較的厚い不純物拡散層の低
抵抗部分を通して伝達できるので、短波長側の光にも高
感度でかつ高速応答可能な受光素子が得られる。請求項
2記載の発明の構成により上記に加え、短波長光に対す
る感度を有する受光部と、低抵抗部、相方の効率を最適
化した構造の受光素子が得られる。請求項3記載の発明
の構成により上記に加え、受光部からの電極取り出し部
の低抵抗でかつ確実な接触と、信頼性を向上した受光素
子が得られる。According to the first aspect of the present invention, short wavelength light also passes through a relatively thin impurity diffusion layer and is absorbed by the depletion layer below it, generating carriers that can move at high speed and contributing to photocurrent. However, since the photocurrent can be transmitted through the low resistance portion of the relatively thick impurity diffusion layer, it is possible to obtain a light receiving element which is highly sensitive and can respond at high speed to light on the short wavelength side. In addition to the above, the light receiving element having a sensitivity to short-wavelength light, the low resistance portion, and the light receiving element having a structure in which the efficiency of the other side is optimized can be obtained. In addition to the above, the structure of the third aspect of the present invention can provide a light-receiving element having a low resistance and reliable contact of the electrode lead-out portion from the light-receiving portion and improved reliability.
【0026】請求項4記載の発明の方法により、不純物
拡散層の厚い部分と薄い部分とをそれぞれほぼ独立した
拡散条件により形成できるので、製造条件の幅が広く安
定して、受光素子を製造できる。請求項5記載の発明の
方法により、1形状のマスクで上記の受光素子を製造で
きる。又、極めて薄い不純物拡散層が形成可能なのでよ
り短波長側の感度を向上させた受光素子が製造できる。
請求項6記載の発明の方法により、1度の不純物導入工
程により上記の受光素子が製造できるので、量産性が良
い。According to the method of the fourth aspect of the present invention, since the thick portion and the thin portion of the impurity diffusion layer can be formed under substantially independent diffusion conditions, the range of manufacturing conditions can be wide and stable, and the light receiving element can be manufactured. .. According to the method of the invention described in claim 5, the above-mentioned light receiving element can be manufactured with a mask having one shape. Further, since an extremely thin impurity diffusion layer can be formed, a light receiving element with improved sensitivity on the shorter wavelength side can be manufactured.
According to the method of the invention as set forth in claim 6, the light-receiving element can be manufactured by a single impurity introduction step, so that mass productivity is good.
【図1】本発明の第1実施例に係る受光素子の構成を示
す縦断面図である。FIG. 1 is a vertical sectional view showing a configuration of a light receiving element according to a first embodiment of the present invention.
【図2】本発明の第2実施例に係る受光素子の平面図で
ある。FIG. 2 is a plan view of a light receiving element according to a second embodiment of the present invention.
【図3】本発明の第3実施例に係る受光素子の構成を説
明するための図であり、図3(a)がその平面図、図3
(b)がその縦断面図である。3A and 3B are views for explaining the configuration of a light receiving element according to a third embodiment of the present invention, FIG. 3A being a plan view thereof and FIG.
(B) is the longitudinal cross-sectional view.
【図4】本発明の第4実施例の受光素子の製造方法を説
明するための図であり、(a),(b)共に、製造工程
の一部を示した縦断面図である。FIG. 4 is a view for explaining the manufacturing method of the light receiving element of the fourth embodiment of the present invention, and both (a) and (b) are vertical cross-sectional views showing a part of the manufacturing process.
【図5】本発明の第5実施例の受光素子の製造方法を説
明するための図であり、(a),(b)共に、製造工程
の一部を示した縦断面図である。FIG. 5 is a view for explaining the manufacturing method of the light receiving element of the fifth embodiment of the present invention, and both (a) and (b) are vertical sectional views showing a part of the manufacturing process.
【図6】本発明の第6実施例の受光素子の製造方法を説
明するための図であり、製造工程の一部を示した縦断面
図である。FIG. 6 is a view for explaining the method of manufacturing the light receiving element of the sixth embodiment of the present invention, which is a vertical cross-sectional view showing a part of the manufacturing process.
【図7】従来のシリコンPINフォトダイオードの縦断
面図である。FIG. 7 is a vertical sectional view of a conventional silicon PIN photodiode.
【図8】シリコンPINフォトダイオードの波長と量子
効率(感度)との関係を示す図である。FIG. 8 is a diagram showing the relationship between the wavelength and quantum efficiency (sensitivity) of a silicon PIN photodiode.
10 半導体基板 11 低抵抗層 12 高抵抗層 20 不純物拡散層 21 比較的厚い層 22 比較的薄い層 30 絶縁膜 40 電極 81,82,83,84 マスク層 92,93 接続部 10 semiconductor substrate 11 low resistance layer 12 high resistance layer 20 impurity diffusion layer 21 relatively thick layer 22 relatively thin layer 30 insulating film 40 electrode 81, 82, 83, 84 mask layer 92, 93 connection part
Claims (6)
導電型の不純物拡散層を形成して成る受光素子におい
て、前記第2導電型の不純物拡散層が周期的に配置され
た比較的厚い層と比較的薄い層とから形成されているこ
とを特徴とする受光素子。1. A second conductivity type is provided near a surface of a semiconductor substrate of a first conductivity type.
In a light receiving element formed by forming a conductivity type impurity diffusion layer, the second conductivity type impurity diffusion layer is formed of a relatively thick layer and a relatively thin layer which are periodically arranged. Light receiving element.
い層と比較的薄い層とが配置される周期の方向が前記第
2導電型の不純物拡散層と、電極とが電気的に接続され
る部分に向かう方向に略垂直であることを特徴とする請
求項1記載の受光素子。2. The impurity diffusion layer of the second conductivity type is electrically connected to the electrode in a cycle direction in which a relatively thick layer and a relatively thin layer of the second conductivity type impurity diffusion layer are arranged. The light-receiving element according to claim 1, wherein the light-receiving element is substantially perpendicular to the direction toward the connected portion.
なくとも電極に電気的に接続される部分は、比較的厚い
層であることを特徴とする請求項1記載又は請求項2記
載の受光素子。3. The impurity diffusion layer of the second conductivity type, wherein at least a portion electrically connected to the electrode is a relatively thick layer. Light receiving element.
より規定される平面形状で第2導電型の不純物拡散層の
比較的厚い層に対応する部分を形成した後、新たに形成
した第2形状のマスク層により規定される平面形状で第
2導電型の不純物拡散層の比較的薄い層および比較的厚
い層を形成する請求項1記載、請求項2記載、又は請求
項3記載の受光素子の製造方法。4. A portion newly formed after forming a portion corresponding to a relatively thick layer of an impurity diffusion layer of the second conductivity type in a plane shape defined by a mask layer having a first shape formed on the surface of a substrate. The light receiving according to claim 1, 2, or 3, wherein a relatively thin layer and a relatively thick layer of the second-conductivity-type impurity diffusion layer are formed in a planar shape defined by the two-shaped mask layer. Manufacturing method of device.
れる平面形状で第2導電型の不純物拡散層の比較的厚い
層に対応する部分を形成した後、熱処理を行なうことに
より、第2導電型の不純物拡散層の比較的薄い層および
比較的厚い層を形成する、請求項1記載、請求項2記
載、又は請求項3記載の受光素子の製造方法。5. The second conductive material is formed by forming a portion corresponding to a relatively thick layer of the second conductive type impurity diffusion layer in a planar shape defined by the mask layer formed on the surface of the substrate and then performing a heat treatment. The method for manufacturing a light-receiving element according to claim 1, claim 2, or claim 3, wherein a relatively thin layer and a relatively thick layer of the type impurity diffusion layer are formed.
い部分と第2形状の比較的厚い部分とを有するマスク層
を用いて第2導電型の不純物を拡散することにより、比
較的薄い層および比較積に厚い層を有する第2導電型の
不純物拡散層を形成する、請求項1記載、請求項2記
載、又は請求項3記載の受光素子の製造方法。6. A mask layer having a relatively thin portion of the first shape and a relatively thick portion of the second shape formed on the surface of the substrate is used to diffuse impurities of the second conductivity type, thereby relatively The method of manufacturing a light-receiving element according to claim 1, claim 2, or claim 3, wherein a second-conductivity-type impurity diffusion layer having a thin layer and a comparatively thick layer is formed.
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JP03226025A JP3101015B2 (en) | 1991-09-05 | 1991-09-05 | Light receiving element and method of manufacturing light receiving element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP03226025A JP3101015B2 (en) | 1991-09-05 | 1991-09-05 | Light receiving element and method of manufacturing light receiving element |
Publications (2)
Publication Number | Publication Date |
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JPH0567798A true JPH0567798A (en) | 1993-03-19 |
JP3101015B2 JP3101015B2 (en) | 2000-10-23 |
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ID=16838609
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