JPH025577A - Optical semiconductor device - Google Patents

Optical semiconductor device

Info

Publication number
JPH025577A
JPH025577A JP63157177A JP15717788A JPH025577A JP H025577 A JPH025577 A JP H025577A JP 63157177 A JP63157177 A JP 63157177A JP 15717788 A JP15717788 A JP 15717788A JP H025577 A JPH025577 A JP H025577A
Authority
JP
Japan
Prior art keywords
resistance
region
electrodes
light
type
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.)
Pending
Application number
JP63157177A
Other languages
Japanese (ja)
Inventor
Nobuyuki Iwamoto
伸行 岩元
Kazuhiko Yamamoto
一彦 山本
Masayuki Yamaguchi
正之 山口
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electronics 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 Matsushita Electronics Corp filed Critical Matsushita Electronics Corp
Priority to JP63157177A priority Critical patent/JPH025577A/en
Publication of JPH025577A publication Critical patent/JPH025577A/en
Pending legal-status Critical Current

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Landscapes

  • Length Measuring Devices By Optical Means (AREA)
  • Photo Coupler, Interrupter, Optical-To-Optical Conversion Devices (AREA)

Abstract

PURPOSE:To make a photodetecting section high in resistance so as to make a noise current small using the photodetecting section of a simple structure by a method wherein the photodetecting sections are formed in parallel with each other, using two or more low resistance regions which are arranged at a right angle with a direction of a line connected between a pair of electrodes. CONSTITUTION:In the formation of a semiconductor, an n-type high resistor 2 inside is formed of a silicon wafer of resistivity of 1000OMEGA, and low resistance P-type regions 3' are formed on the silicon wafer in such a state that they are 1X10<18>cm<-3> in surface concentration and 10mum in width, and an ion implantation is performed with 1.0X10<12>cm<-2> in dose to form a high resistance region 3 10mum in width. The space between the low resistance regions 3' and the high resistance region 3 is 10mum. In result, a photodetecting region can be made high resistive through a conventional ion implantation technique, where its resistance value, about three times as large as that of a conventional ones, can be realized.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、−次元光点位置検出を行う光半導体装置に関
するものである。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to an optical semiconductor device that detects the position of a -dimensional light spot.

従来の技術 PN接合を有する光半導体装置において、同光半導体装
置の受光面に照射されたスポット光の照射位置を受光面
の両端に設けられた2つの電極からの光電流の差により
、−次元的に位置を検出することができる。
Conventional technology In an optical semiconductor device having a PN junction, the irradiation position of a spot light irradiated on the light receiving surface of the same optical semiconductor device is determined by the difference in photocurrent from two electrodes provided at both ends of the light receiving surface. position can be detected.

この装置は第6図(a)、 (b)の側断面図、平面図
に示すように所定の導電形、たとえばn型の半導体基板
1上にn型高抵抗領域2があり、この表面部分にこれら
と異なる導電形のp要領域3を設けた光半導体装置であ
り、p要領域3のパターン形状が、第6図(b)に示さ
れるように長方形を形成したものであり、その両端部に
アノード電極4,4゛が、基板1の裏面にカソード電極
5が、そして。
As shown in the side sectional view and plan view of FIGS. 6(a) and 6(b), this device has an n-type high resistance region 2 on a semiconductor substrate 1 of a predetermined conductivity type, for example, n-type, and this surface portion This is an optical semiconductor device in which a p-required region 3 of a conductivity type different from these is provided, and the p-required region 3 has a rectangular pattern shape as shown in FIG. Anode electrodes 4, 4' are placed on the bottom surface of the substrate 1, and a cathode electrode 5 is placed on the back side of the substrate 1.

最表部の絶縁保護膜6が、それぞれ形成されている。An insulating protective film 6 at the outermost portion is formed respectively.

発明が解決しようとする課題 実使用上では、スポット光が被写体に当り、その反射光
の一部が光半導体装置の受光面に照射される。このため
、照射光に対する光電流のレベルが小さくS/Nが悪く
なり、実使用上信号を検出するのが容易でなかった。
Problems to be Solved by the Invention In actual use, spot light hits a subject, and a portion of the reflected light is irradiated onto the light-receiving surface of the optical semiconductor device. For this reason, the level of the photocurrent with respect to the irradiated light is small and the S/N ratio is poor, making it difficult to detect signals in actual use.

S/Nを上げるためには雑音電流を小さくしなければな
らない。雑音電流は一般に次式で表されin:雑音電流
、に:ボルッマン定数 T:絶対温度、B:周波数帯域幅 Re(1):インビーダンZpの実数部p で雑音電流を低下させるためには、接合容量を小さくし
、受光面の抵抗を大きくする必要があった。
In order to increase the S/N, the noise current must be reduced. The noise current is generally expressed by the following formula: in: noise current, to: Borckmann's constant T: absolute temperature, B: frequency bandwidth Re(1): real part of impedance Zp In order to reduce the noise current, junction It was necessary to reduce the capacitance and increase the resistance of the light-receiving surface.

受光面の抵抗値は不純物量で決まり、イオン注入を制御
して目的の抵抗値を得ることができろが、イオン注入時
のドーズ量を低くしていく七、抵抗のばらつきが大きく
なり、再現性も得られないという欠点があった。
The resistance value of the light-receiving surface is determined by the amount of impurities, and it is possible to obtain the desired resistance value by controlling ion implantation, but if the dose amount during ion implantation is lowered, the variation in resistance will increase and it will be difficult to reproduce. The downside was that I couldn't get sex either.

本発明は、このような問題を解決しようとするもので、
簡便な構造の受光部を用いて受光部を高抵抗にすること
で雑音電流を小さくすることを目的とする。
The present invention aims to solve such problems,
The purpose is to reduce noise current by using a light receiving part with a simple structure and making the light receiving part high in resistance.

課題を解決するための手段 上記問題点を解決するために、本発明は光半導体装置の
受光部分において、低抵抗の領域を一対の電極間を結ぶ
方向に直交して、複数個を互いに平行に形成し、高抵抗
領域で電極間を接続する。
Means for Solving the Problems In order to solve the above problems, the present invention provides a light-receiving portion of an optical semiconductor device, in which a plurality of low-resistance regions are arranged parallel to each other, perpendicular to the direction connecting a pair of electrodes. and connect the electrodes in the high resistance region.

受光部の抵抗は高抵抗領域に依存ずろためにその面積を
小さ(することにより、不純物の1:・−て量が多くて
も受光部(2つの電極間)の抵抗は太き(なる。高抵抗
領域は、受光部の一部であるが、それと接続して低抵抗
層が受光領域全体に拡がっているために、光半導体装置
として使用が可能となる。
Since the resistance of the light receiving part depends on the high resistance region, by making its area small, the resistance of the light receiving part (between two electrodes) becomes large even if the amount of impurities is large. The high-resistance region is a part of the light-receiving section, but since the low-resistance layer is connected to it and spreads over the entire light-receiving region, it can be used as an optical semiconductor device.

作用 受光領域を一対のアノード電極間に、同電極間を結ぶ方
向と直交して複数個の低抵抗領域を互いに平行して設け
、アノード電極間で上記の複数個の低抵抗領域を高抵抗
領域で互いに接続し、受光面を形成ずろこ七により、不
純物量が従来のままでも容易に受光部高抵抗領域が形成
でき、かつ。
The active light-receiving area is provided between a pair of anode electrodes, and a plurality of low resistance areas are provided in parallel with each other perpendicular to the direction connecting the same electrodes, and the above-mentioned multiple low resistance areas are formed as a high resistance area between the anode electrodes. are connected to each other to form a light-receiving surface.By using the 7 scales, a high-resistance region of the light-receiving portion can be easily formed even if the amount of impurities remains the same as before.

ばらつきの少ない特11が実現でき、雑音電流1.ヘル
を小さくすることが可能である。
Characteristic 11 with little variation can be realized, and noise current 1. It is possible to reduce the amount of heat.

実施例 第1図は本発明の一実施例である光半導体装置を示す平
面図であり、第2図、第3図はそのX方向およびY方向
の各断面図を示す。2は口型半導体領域、3は高抵抗口
型半導体領域、3′は低抵抗口型半導体領域、4.4°
ばアノード電極である。実使用旧、スポットの径は受光
面のY方向に対し、半分程度の円であり、位置変位に対
する分解能も従来とほぼ同程度の特性を示す。
Embodiment FIG. 1 is a plan view showing an optical semiconductor device which is an embodiment of the present invention, and FIGS. 2 and 3 show cross-sectional views thereof in the X direction and the Y direction. 2 is a mouth-type semiconductor region, 3 is a high-resistance mouth-type semiconductor region, 3' is a low-resistance mouth-type semiconductor region, 4.4°
This is the anode electrode. In actual use, the diameter of the spot is about half a circle with respect to the Y direction of the light receiving surface, and the resolution with respect to positional displacement is also approximately the same as that of the conventional method.

この半導体を形成ずろにあたり、内部のn型高抵抗2に
は、1000Ωc!0のシリコンウェーハを用い、この
シリコンウェーハ上に低抵抗P型領域3″を表面濃度I
 X 1018cm−3幅1.0μm、さらにボロンの
ドーズ量1. OX 10” cn+−’でイオン注入
を施し、高抵抗領域3を幅10μrT1形成した1、低
抵抗領域3°と低抵抗領域3′との間隔は10μn1で
ある。この結果、受光部領域を従来のイオン(を人技術
で高抵抗に形成することが出来、従来の抵抗値に対して
約3倍程度のものが実現できた。第4図はイオン注入ド
ーズ量と受光領域の抵抗値との関係図であり、従来例装
置の相関特1−1′ニアと本実施例装置の相関特性8と
を対比して示した。これからもわかるように、低ドーズ
領域においても本実施例の場合、そのバラツキが小さく
なった。
When forming this semiconductor, the internal n-type high resistance 2 has a resistance of 1000Ωc! A low resistance P-type region 3'' is formed on this silicon wafer with a surface concentration of I
X 1018cm-3 width 1.0μm, and boron dose 1. Ion implantation was performed with OX 10"cn+-' to form the high resistance region 3 with a width of 10μrT1, and the spacing between the low resistance region 3° and the low resistance region 3' was 10μn1. As a result, the light receiving area was changed from the conventional one. We were able to form ions (with human technology) to have a high resistance, and were able to achieve a resistance value approximately three times that of the conventional one. Figure 4 shows the relationship between the ion implantation dose and the resistance value of the light receiving area. This is a relational diagram showing a comparison between the correlation characteristic 1-1'near of the conventional device and the correlation characteristic 8 of the present embodiment device.As can be seen from this, even in the low dose region, in the case of the present embodiment, The variation has become smaller.

第5図は他の実施例で、パターンを互い(ご違い状のp
型骨光領域を作成したもので、第1図の例の場合と同様
の結果が得られる。
Figure 5 shows another embodiment, in which the patterns are arranged with each other (different p
A pattern bone light region is created, and the same results as in the example shown in FIG. 1 can be obtained.

発明の効果 以上のように本発明によれば、光半導体装置の受光部を
電極に対して低抵抗領域を平行(−複数個設け、電極に
垂直に高抵抗領域を形成シ2.7ノ一ド電極間を接続す
る二りにより、従来のイオン注入技術でP型領域(2つ
の電極間)の抵抗値のみを大きくし、他の特性は従来と
同程度のものが(1られる。受光領域の抵抗値を容易に
大ぎくできることにより、S/Nが大きくなり、実用的
価値は大なるものである。
Effects of the Invention As described above, according to the present invention, the light-receiving portion of an optical semiconductor device is arranged in parallel to the electrode with a plurality of low-resistance regions formed, and a high-resistance region is formed perpendicular to the electrode. By connecting two electrodes, the resistance value of only the P-type region (between two electrodes) is increased using conventional ion implantation technology, and the other characteristics are the same as conventional ones (1). By being able to easily increase the resistance value, the S/N ratio increases, which is of great practical value.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の実施例である)号1−ダイオードの平
面図、第2図9第3図は同実施例7寸トダイオ・−ドX
方向断面図、Y方向断面図、第4図は高抵抗領域形成時
のイオン注入量と受光領域〈電極間〉抵抗値との関係図
、第5図は本発明の他の実施例を示す平面図、第0図は
受ソこ面に2つの電極を有する従来例フォトダイオード
の断面図および平面図である。 1・・・・・・n型半導体基板、2・・・・・・n型高
抵抗半導体層、3・・・・・・n型高抵抗半導体層、3
゛・・・・・・p型低抵抗半導体層、4,4′・・・・
・・p型電極領域、5・・・・・・n型半導体基板電極
、6・・・・・・絶縁膜、7・・・・・・イオン注入量
と電極間抵抗の従来の関係図、8・・・・・・本発明の
イオン注入量と電極間抵抗との関係図。 代理人の氏名 弁理士 中尾敏男 ほか1名第1図 第40 第6図 第5図 2−71型牟1体1 3’−P  里 b匙i 領域 本−t@傾 城
Figure 1 shows an embodiment of the present invention.) Figure 2 is a plan view of a diode No. 1.
A sectional view in the Y direction, a sectional view in the Y direction, FIG. 4 is a diagram showing the relationship between the ion implantation amount and the resistance value of the light receiving area (between electrodes) when forming a high resistance region, and FIG. 5 is a plane view showing another embodiment of the present invention. FIG. 0 is a sectional view and a plan view of a conventional photodiode having two electrodes on the receiving surface. 1... N-type semiconductor substrate, 2... N-type high resistance semiconductor layer, 3... N-type high resistance semiconductor layer, 3
゛...P-type low resistance semiconductor layer, 4,4'...
... p-type electrode region, 5 ... n-type semiconductor substrate electrode, 6 ... insulating film, 7 ... conventional relationship diagram between ion implantation amount and interelectrode resistance, 8... Relationship diagram between ion implantation amount and interelectrode resistance of the present invention. Name of agent: Patent attorney Toshio Nakao and one other person Figure 1 Figure 40 Figure 6 Figure 5 2-71 type 1 body 1 3'-P Ri b-soui Territory book-t@Kanjo

Claims (1)

【特許請求の範囲】[Claims] 所定導電形の半導体領域上に、同一導電形の高抵抗領域
と逆導電形の低抵抗領域とを一対の電極間に同電極間を
結ぶ方向と直交して複数個設け、前記高抵抗領域間を高
抵抗電極間で互いに接続したことを特徴とする光半導体
装置。
A plurality of high resistance regions of the same conductivity type and low resistance regions of opposite conductivity type are provided on a semiconductor region of a predetermined conductivity type between a pair of electrodes, perpendicular to the direction connecting the same electrodes, and a plurality of high resistance regions of the same conductivity type are provided between the high resistance regions. An optical semiconductor device characterized in that these are connected to each other between high-resistance electrodes.
JP63157177A 1988-06-24 1988-06-24 Optical semiconductor device Pending JPH025577A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63157177A JPH025577A (en) 1988-06-24 1988-06-24 Optical semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63157177A JPH025577A (en) 1988-06-24 1988-06-24 Optical semiconductor device

Publications (1)

Publication Number Publication Date
JPH025577A true JPH025577A (en) 1990-01-10

Family

ID=15643870

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63157177A Pending JPH025577A (en) 1988-06-24 1988-06-24 Optical semiconductor device

Country Status (1)

Country Link
JP (1) JPH025577A (en)

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