JPS5963776A - Semiconductor device for detecting incident position - Google Patents

Semiconductor device for detecting incident position

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Publication number
JPS5963776A
JPS5963776A JP57173657A JP17365782A JPS5963776A JP S5963776 A JPS5963776 A JP S5963776A JP 57173657 A JP57173657 A JP 57173657A JP 17365782 A JP17365782 A JP 17365782A JP S5963776 A JPS5963776 A JP S5963776A
Authority
JP
Japan
Prior art keywords
layer
electrodes
semiconductor device
detecting
incident position
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
JP57173657A
Other languages
Japanese (ja)
Inventor
Seiji Yamaguchi
誠二 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.)
Hamamatsu TV Co Ltd
Original Assignee
Hamamatsu TV Co Ltd
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 Hamamatsu TV Co Ltd filed Critical Hamamatsu TV Co Ltd
Priority to JP57173657A priority Critical patent/JPS5963776A/en
Publication of JPS5963776A publication Critical patent/JPS5963776A/en
Pending legal-status Critical Current

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  • Measurement Of Optical Distance (AREA)
  • Photo Coupler, Interrupter, Optical-To-Optical Conversion Devices (AREA)

Abstract

PURPOSE:To improve the sensitivity of positional detection by previously making the resistance value of the central section of the other conduction type semiconductor layer opposite to a pair of electrodes for detecting positions higher than sections in the vicinity of each electrode in the device in which the other conduction type semiconductor layer is formed on the surface of one conduction type semiconductor substeate, the electrodes are formed opposed to the other conduction type layer and the positions of particle beams projected to the surface are obtained by outputs from the electrodes. CONSTITUTION:The P type layer 3, which is thin at a central section 3a and is thick in peripheral sections 3b and 3c surrounding the section 3a, is diffused and formed to the surface of the N type semiconductor substrate 1, a light-receiving surface thereof is formed to a rectangular shape. The thickness of the central section 3a is thinned up to approximately 0.2mum while impurity concentration is also brought to 10<17>/cm<3> and resistance is brought to approximately 100kOMEGA, and the thickness of the peripheral sections 3b and 3c is brought to 1.0mum, and concentration is also brought to approximately 10<20>/cm<3> and resistance is lowered up to 100OMEGA. The positional signal electrodes 4 and 5 are formed to the layers 3b and 3c along the short sides of the resistance layer 3, and an electrode 2 is also formed to the back of the substrate 1. Accordingly, the positional resolving power of the central section of the surface is improved without shortening the full length.

Description

【発明の詳細な説明】 本発明は一導電形の半導体基板の表面に他の導電形の半
導体層を形成し、前記他の導電形の半導体層上に対向す
る一対の位置検出用の電極を形成し、表面に入射した粒
子線の位置を前記電極の出力から演算して求める入射位
置検出用半導体装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention comprises forming a semiconductor layer of another conductivity type on the surface of a semiconductor substrate of one conductivity type, and forming a pair of opposing position detection electrodes on the semiconductor layer of the other conductivity type. The present invention relates to a semiconductor device for detecting an incident position in which the position of a particle beam formed and incident on a surface is calculated from the output of the electrode.

まず第1図を参照して入射位置検出用半導体装置の基本
的な構成を説明する。
First, the basic configuration of a semiconductor device for detecting an incident position will be explained with reference to FIG.

第1図(八)は入射位置検出用半導体装置の平面図、同
図(B)は断面図であって、厚さ方向を誇張して示しで
ある。この入射位置検出用半導体装置は、N形の半導体
基板lの表面にP形の半導体層による抵抗層3を形成し
てこの抵抗層の両端に一対の位置信号電極4,5を設け
て構成されている。
FIG. 1(8) is a plan view of the semiconductor device for detecting the incident position, and FIG. 1(B) is a cross-sectional view, in which the thickness direction is exaggerated. This semiconductor device for detecting an incident position is constructed by forming a resistance layer 3 made of a P-type semiconductor layer on the surface of an N-type semiconductor substrate l, and providing a pair of position signal electrodes 4 and 5 at both ends of this resistance layer. ing.

この抵抗層3に光や何重粒子が入射するとキャリートか
発生させられて前記一対の電極4,5から電4%が流入
する。この電荷は入射位置の関数として与えられるので
、前記電極に流れる電流から光等の入射位置を知ること
ができる。
When light or particles enter the resistive layer 3, carry particles are generated, and 4% of the charge flows from the pair of electrodes 4 and 5. Since this charge is given as a function of the incident position, the incident position of light, etc. can be determined from the current flowing through the electrode.

次に前記装置の位置分解能について説明する。Next, the positional resolution of the device will be explained.

第2図は粒子線等の入射位置と電極4から流入する電流
の関係を示すグラフである。
FIG. 2 is a graph showing the relationship between the incident position of a particle beam or the like and the current flowing from the electrode 4.

第1図に示すように電極4と入射点Pの距離をXとし、
x=Qのときの電流をIAOとすると、任意の距離Xに
粒子線が入射したときに電極4から流入する電流I^は
次の式で与えられる。
As shown in FIG. 1, the distance between the electrode 4 and the incident point P is X,
If the current when x=Q is IAO, the current I^ flowing from the electrode 4 when the particle beam is incident at an arbitrary distance X is given by the following equation.

l ^ −IAO・ ’(1−−x)  /しただし:
12は受光面の全長 この装置の位置検出感度は入射光の位置の変化に対する
出力信号の変化として次のように定義する。
l ^ -IAO・'(1--x) / Shidashi:
12 is the total length of the light receiving surface.The position detection sensitivity of this device is defined as the change in the output signal with respect to the change in the position of the incident light as follows.

位置検出感度−一ΔIへ/Δx−TAO/L前記入射位
置検出用半導体装置をレーザ光や光スポットの正確な位
置合わせをするときに、前記位置検出感度を大きくして
欲しいという強い要請がある。
Position Detection Sensitivity - To ΔI/Δx-TAO/L There is a strong demand for increasing the position detection sensitivity when accurately aligning the laser beam or light spot with the semiconductor device for detecting the incident position. .

前記位置検出感度を大きくするためにば、全長りを小さ
くすれば良いのであるが全長りを小さくすると受光範囲
が小さくなり測定できる範囲を犠牲にすることになる。
In order to increase the position detection sensitivity, the overall length can be reduced, but if the overall length is reduced, the light receiving range becomes smaller and the measurable range is sacrificed.

したがって、全長りを小さくすることでは良い解決が得
られない。
Therefore, reducing the total length does not provide a good solution.

本発明の目的は受光面積を小さくすることなく前述の要
請を満足することができる入射位置検出用半導体装置を
提供することにある。
An object of the present invention is to provide a semiconductor device for detecting an incident position that can satisfy the above requirements without reducing the light receiving area.

前記目的を達成するために本発明による入射位置検出用
半導体装置は、−導電形の半導体基板の表面に他の導電
形の半導体層を形成し、前記他の導電形の半導体層上に
対向する一対の位置検出用の電極を形成し、表面に入射
した粒子線の位置を前記電極の出力から演算して求める
入射位置検出用半導体装置において、前記他の導電形の
半導体層の中央部を前記各電極近傍よりも高い抵抗層で
形成することにより、中央部の位置検出感度を周辺部の
位置検出感度よりも大きく構成されている。
In order to achieve the above object, a semiconductor device for detecting an incident position according to the present invention includes: - forming a semiconductor layer of another conductivity type on the surface of a semiconductor substrate of conductivity type, and opposing the semiconductor layer of the other conductivity type; In the semiconductor device for detecting the incident position in which a pair of position detecting electrodes are formed and the position of the particle beam incident on the surface is calculated from the output of the electrodes, the central part of the semiconductor layer of the other conductivity type is By forming the layer with a higher resistance than the layer near each electrode, the position detection sensitivity at the center is made larger than the position detection sensitivity at the periphery.

前記t1η成によれば本発明の目的は完全に達成できる
According to the above t1η configuration, the object of the present invention can be completely achieved.

以下、し1面等を参照して本発明をさらに詳しく説明す
る。
Hereinafter, the present invention will be explained in more detail with reference to the first page and the like.

第3図は本発明による入射位置検出用半導体装置の実施
例を示す図であって、同図(A)は平面図、同図(13
)は断面図である第1図と同様に厚さ方向を拡大して示
しである。
FIG. 3 is a diagram showing an embodiment of a semiconductor device for detecting an incident position according to the present invention, in which FIG. 3(A) is a plan view and FIG.
) is an enlarged view in the thickness direction, similar to FIG. 1 which is a cross-sectional view.

受光面1 mmX 2Hを確保できる短冊形を形成でき
るN形導電性の基板1を用意する。
An N-type conductive substrate 1 that can be formed into a rectangular shape that can secure a light-receiving surface of 1 mm x 2 H is prepared.

表面抵抗層3の3a部は不純物濃度が10”/clに達
するま−11;ロンを注入して、P形専電性の比較的高
い抵抗の層を形成する。
In the portion 3a of the surface resistance layer 3, ions are implanted until the impurity concentration reaches 10''/cl to form a P-type exclusive layer with relatively high resistance.

3a部の1)層の厚さは0.2μIn、3a部のPHの
抵抗は100にΩである。
The thickness of the layer 1) in the section 3a is 0.2 μIn, and the resistance of the PH in the section 3a is 100Ω.

表面抵抗層3の周辺部3b、3c部は不純物濃度が10
 ” / clに達するまでボロンを拡散して、P形導
電性の比較的低い抵抗の層を形成する。
The impurity concentration in the peripheral parts 3b and 3c of the surface resistance layer 3 is 10.
”/cl to form a relatively low resistance layer of P-type conductivity.

この周辺部のP屑の厚さは1.0μm、抵抗は各々10
0Ωである。
The thickness of the P scraps in this peripheral area is 1.0 μm, and the resistance is 10
It is 0Ω.

前記抵抗@3の短辺に沿って位置信号電極4.5を形成
し、底部に電極2を接続する。
A position signal electrode 4.5 is formed along the short side of the resistor @3, and the electrode 2 is connected to the bottom.

第4図に前記実施例装置における粒子線等の入射位置と
電極から流入する電流の関係を示しである。
FIG. 4 shows the relationship between the incident position of a particle beam and the like and the current flowing from the electrode in the apparatus of the embodiment.

第4図から周辺部より中央部の位置分解能−一ΔI^/
ΔXが大きくなっていることが、容易に理解できる。
From Fig. 4, the positional resolution of the center part compared to the peripheral part -1ΔI^/
It can be easily understood that ΔX is large.

前記構成の装置の位置分解能を実測した結果について説
明する。
The results of actually measuring the positional resolution of the device with the above configuration will be explained.

この装置の雑音電流の自乗平均(l d ) rmsを
求めておく。電極2を流れる電流が1.5μAになる光
スポットで前記入射位置検出用半導体装置の表面抵抗層
3を照射して光スポットと表面抵抗層3の相対位置を第
3図において、左右方向に変化さセる。そして電極4を
流れる電流の変化ΔIが前記雑音電流の自乗平均(Id
)’rmsに達するに要する光スポットで前記入射位置
検出用半導体装置の相対移動量を測定する。
The root mean square (ld) rms of the noise current of this device is determined in advance. The surface resistance layer 3 of the semiconductor device for detecting the incident position is irradiated with a light spot whose current flowing through the electrode 2 is 1.5 μA, and the relative position of the light spot and the surface resistance layer 3 is changed in the horizontal direction in FIG. Saseru. Then, the change ΔI in the current flowing through the electrode 4 is the root mean square of the noise current (Id
)'rms.The relative movement amount of the semiconductor device for detecting the incident position is measured using the light spot required to reach rms.

前記相対移動量は中央部3aでは0.2μmでこれば全
長の1/10000に相当する。
The amount of relative movement is 0.2 μm in the central portion 3a, which corresponds to 1/10000 of the total length.

周辺部3b、3cでは200μrnでこれば全長の1/
10に相当する。
For the peripheral parts 3b and 3c, 200 μrn is 1/1 of the total length.
It corresponds to 10.

従来の同種の入射位置検出用半導体装置、(表面の抵抗
層が120 KΩの全面均一な抵抗を有するもの)にお
いて同じ測定をしたところ、前記相対移動量は0.4μ
mでこれば全長の115000に相当する。
When the same measurement was performed on a conventional semiconductor device for detecting the incident position of the same type (the surface resistance layer has a uniform resistance of 120 KΩ), the relative movement amount was 0.4μ.
m, which corresponds to the total length of 115,000.

ずなわら、本発明による装置では表面の中央部の位置分
解能を全長を短くすることな〈従来の相当装置より大き
くすることができるという効果が得られる。
However, the device according to the present invention has the advantage that the positional resolution at the center of the surface can be made greater than that of the conventional equivalent device without shortening the overall length.

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

第1図(八)は従来の入射位置検出用半導体装置の平面
図、同図(、B)は断面図であって、厚さ方向をI広大
して示しである。 第2図は前記装置で、粒子線等の入射位置と電極から流
入する電流の関係を示すグラフである。 第3図は本発明による入射位置検出用半導体装置の実施
例を示す図であって、同図(Δ)は平面図、同図(B)
は断面図であって厚さ方向を拡大して示しである。 第4図は前記実施例装置で、粒子線等の入射位置と電極
から流入する電流の関係を示すグラフである。 1・・・半導体基板 2・・・電極 3・・・表面抵抗層 3a・・・表面抵抗層の中央部 3b、3c・・・表面抵抗層の周辺部 4.5・・・・位置信号電極 特許出願人 浜松テレビ株式会社 代理人 弁理士  井 ノ ロ  壽 第1図 22図 □□9−χ 才3図 才4図 □           χ
FIG. 1(8) is a plan view of a conventional semiconductor device for detecting an incident position, and FIG. 1(B) is a cross-sectional view, with the thickness direction enlarged. FIG. 2 is a graph showing the relationship between the incident position of the particle beam and the current flowing from the electrode in the device. FIG. 3 is a diagram showing an embodiment of the semiconductor device for detecting an incident position according to the present invention, in which (Δ) is a plan view and FIG. 3 (B) is a plan view.
is a sectional view showing an enlarged view in the thickness direction. FIG. 4 is a graph showing the relationship between the incident position of a particle beam or the like and the current flowing from the electrode in the apparatus of the embodiment. 1...Semiconductor substrate 2...Electrode 3...Surface resistance layer 3a...Central part 3b, 3c of surface resistance layer...Peripheral part of surface resistance layer 4.5...Position signal electrode Patent Applicant Hamamatsu Television Co., Ltd. Agent Patent Attorney Hisashi Inoro Figure 1 Figure 22 □□9-χ Figure 3 Figure 4 Figure □ χ

Claims (1)

【特許請求の範囲】 (1,1−導電形の半導体基板の表面に他の導電形の半
導体層を形成し、前記他の導電形の半導体層上に対向す
る一対の位置検出用の電極を形成し、表面に入射した粒
子線の位置を前記電極の出力から演算して求める入射位
置検出用半導体装置において、前記他の導電形の半導体
層の中央部を前記各電極近傍よりも’+Pliい抵抗層
で形成することにより、中央部の位置分解能を周辺部の
位置分解能よりも大きく構成したことを特徴とする入射
位置検出用半導体装造:。 (2)前記1i*9体基板の表面は矩形であっζ、前記
一対の位i6検出用の電極ば短辺に沿って形成され前記
中央部に形成された高い抵抗層部分は、前記矩形の長辺
と前記電極にそれぞれ平行な辺で囲まれる四辺形内に形
成されている特許請求の範囲第1項記載の入射位置検出
用半導体装置。 (3)  前記−導電形の半導体基板はN形シリコンで
あり表面の抵抗層はP形抵抗層であり、周辺をボロンの
拡散により、中央部をボロンのイオン注入により形成し
た特許請求の範囲第1項記載の入射位置検出用半導体装
置。
[Claims] (A semiconductor layer of another conductivity type is formed on the surface of a semiconductor substrate of 1,1-conductivity type, and a pair of position detection electrodes facing each other is provided on the semiconductor layer of the other conductivity type. In the semiconductor device for detecting the incident position in which the position of a particle beam formed and incident on the surface is calculated from the output of the electrode, the central part of the semiconductor layer of the other conductivity type is set to be '+Pli higher than the vicinity of each of the electrodes. A semiconductor device for detecting an incident position, characterized in that the positional resolution of the central part is larger than that of the peripheral part by forming a resistive layer. (2) The surface of the 1i*9 body substrate is The high resistance layer portion formed along the short sides of the pair of position i6 detection electrodes and formed in the central portion is surrounded by the long sides of the rectangle and sides parallel to the electrodes, respectively. A semiconductor device for detecting an incident position according to claim 1, which is formed in a quadrilateral formed in a rectangular shape. (3) The - conductivity type semiconductor substrate is N-type silicon, and the surface resistance layer is a P-type resistance layer. 2. A semiconductor device for detecting an incident position according to claim 1, wherein the peripheral portion is formed by boron diffusion and the central portion is formed by boron ion implantation.
JP57173657A 1982-10-01 1982-10-01 Semiconductor device for detecting incident position Pending JPS5963776A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57173657A JPS5963776A (en) 1982-10-01 1982-10-01 Semiconductor device for detecting incident position

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57173657A JPS5963776A (en) 1982-10-01 1982-10-01 Semiconductor device for detecting incident position

Publications (1)

Publication Number Publication Date
JPS5963776A true JPS5963776A (en) 1984-04-11

Family

ID=15964672

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57173657A Pending JPS5963776A (en) 1982-10-01 1982-10-01 Semiconductor device for detecting incident position

Country Status (1)

Country Link
JP (1) JPS5963776A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62203347A (en) * 1986-03-04 1987-09-08 Hamamatsu Photonics Kk Semiconductor position detector

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62203347A (en) * 1986-03-04 1987-09-08 Hamamatsu Photonics Kk Semiconductor position detector

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