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JP2596023B2 - Evaluation method of semiconductor photo detector - Google Patents
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JP2596023B2 - Evaluation method of semiconductor photo detector - Google Patents

Evaluation method of semiconductor photo detector

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Publication number
JP2596023B2
JP2596023B2 JP62306609A JP30660987A JP2596023B2 JP 2596023 B2 JP2596023 B2 JP 2596023B2 JP 62306609 A JP62306609 A JP 62306609A JP 30660987 A JP30660987 A JP 30660987A JP 2596023 B2 JP2596023 B2 JP 2596023B2
Authority
JP
Japan
Prior art keywords
light receiving
receiving element
linearity
bias voltage
semiconductor 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.)
Expired - Lifetime
Application number
JP62306609A
Other languages
Japanese (ja)
Other versions
JPH01146375A (en
Inventor
修三 香川
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.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
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Filing date
Publication date
Application filed by Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP62306609A priority Critical patent/JP2596023B2/en
Publication of JPH01146375A publication Critical patent/JPH01146375A/en
Application granted granted Critical
Publication of JP2596023B2 publication Critical patent/JP2596023B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)
  • Light Receiving Elements (AREA)
  • Testing Of Individual Semiconductor Devices (AREA)

Description

【発明の詳細な説明】 〔概 要〕 半導体受光素子の出力特性の評価方法に関し、 ウエハーまたはチップの状態で出力特性のリニアリテ
イを評価して、製造コストを低減させることを目的と
し、 半導体受光素子の入射光強度に対する光電流の出力特
性と、該素子のP電極N電極間逆バイアス電圧に対する
該素子のキャパシタンス値の関係との相関関係を予め求
めておく工程と、 評価対象である半導体受光素子の前記逆バイアス電圧
の特定の値に対するキャパシタンス値を測定する工程
と、 測定した前記キャパシタンス値を前記相関関係を参照
することにより評価し、該半導体受光素子の前記出力特
性の直線性の良・不良の判定を行なう工程を有すること
を特徴とする。
DETAILED DESCRIPTION OF THE INVENTION [Summary] The present invention relates to a method for evaluating the output characteristics of a semiconductor light-receiving element. The object of the present invention is to evaluate the linearity of the output characteristics in a state of a wafer or a chip and to reduce the manufacturing cost. Determining in advance the correlation between the output characteristic of the photocurrent with respect to the incident light intensity and the relationship between the capacitance value of the element and the reverse bias voltage between the P electrode and the N electrode of the element; Measuring a capacitance value for a specific value of the reverse bias voltage, and evaluating the measured capacitance value by referring to the correlation to determine whether the output characteristic of the semiconductor light receiving element is linear or non-linear. And a step of determining

また、半導体受光素子の入射光強度に対する光電流の
出力特性と、該素子のP電極N電極間逆バイアス電圧に
対する該素子のシリーズ抵抗値の関係との相関関係を予
め求めておく工程と、 評価対象である半導体受光素子の前記逆バイアス電圧
の特定の値に対するシリーズ抵抗値を測定する工程と、 測定した前記シリーズ抵抗値を前記相関関係を参照す
ることにより評価し、該半導体受光素子の前記出力特性
の直線性の良・不良の判定を行なう工程を有することを
特徴とする。
A step of obtaining in advance a correlation between a photocurrent output characteristic with respect to an incident light intensity of the semiconductor light receiving element and a relation of a series resistance value of the element with respect to a reverse bias voltage between a P electrode and an N electrode of the element; Measuring a series resistance value of the target semiconductor light receiving element with respect to a specific value of the reverse bias voltage; and evaluating the measured series resistance value by referring to the correlation to obtain the output of the semiconductor light receiving element. The method is characterized by including a step of determining whether the linearity of characteristics is good or bad.

〔産業上の利用分野〕[Industrial applications]

本発明は半導体受光素子の出力特性の評価方法に関す
る。
The present invention relates to a method for evaluating output characteristics of a semiconductor light receiving element.

最近、光ファイバ通信が実用化され、その光ファイバ
通信に用いられる半導体受光素子(フォトダイオード)
の一層の品質向上・コストダウンが期待されている。
Recently, optical fiber communication has been put to practical use, and a semiconductor light receiving element (photodiode) used for the optical fiber communication has been developed.
Are expected to further improve quality and reduce costs.

〔従来の技術〕[Conventional technology]

シリコン,ゲルマニウムや化合物半導体等からなる種
々の半導体受光素子(フォトダイオード)が使用されて
おり、例えば、1.3μm帯の波長の光に対して受光効率
の良い半導体受光素子としてInGaAs系受光素子が知られ
ている。第4図はそのPIN形InGaAs受光素子の断面図を
示し、図中の1はn−InP基板,2はn−InPバッファ層,3
はn−InGaAs光吸収層,4はn−InPキャップ層,5はp−
受光領域,6はp−電極,7はn−電極で、電極間に逆バイ
アス電圧を印加してp−受光領域5に光が入射すると、
n−InGaAs光吸収層3中に電子と正孔が励起されてpn接
合部に光電流が流れ、その出力が検出される構造であ
る。
Various semiconductor light-receiving elements (photodiodes) made of silicon, germanium, compound semiconductors, etc. are used. For example, an InGaAs-based light-receiving element is known as a semiconductor light-receiving element having high light-receiving efficiency for light in a wavelength of 1.3 μm band. Have been. FIG. 4 is a cross-sectional view of the PIN type InGaAs light receiving element, wherein 1 is an n-InP substrate, 2 is an n-InP buffer layer, 3
Is an n-InGaAs light absorbing layer, 4 is an n-InP cap layer, and 5 is a p-
The light receiving region, 6 is a p-electrode, 7 is an n-electrode, and when light is incident on the p-light receiving region 5 by applying a reverse bias voltage between the electrodes,
The structure is such that electrons and holes are excited in the n-InGaAs light absorbing layer 3, photocurrent flows through the pn junction, and the output is detected.

さて、上記のような受光素子の重要な特性の一つに、
入射した光強度の強弱に応じて比例した光電流の出力が
得られるかどうかの光出力の直線性(リニアリテイ;lin
earity)がある。第5図はその従来のリニアリテイの測
定方法を示す図で、図中の11は受光素子,12は温度制御
器,13は発光素子,14はアッテネータ,15は光ファイバ,16
は出力計である。例えば、受光素子が低温度で使用され
る場合を想定して、温度制御器12の温度を−40℃に設定
し、発光素子13からの光をアッテネータ14を介して光フ
ァイバ15を通して受光素子11に入射させると、発光素子
13からの光エネルギーに対する受光素子11の電流出力が
得られる。なお、一般に、電流出力は光電流とバイアス
電圧の積として電力で表わされる。
Now, one of the important characteristics of the light receiving element as described above,
The linearity of light output (linearity; lin) to determine whether a photocurrent output proportional to the intensity of the incident light is obtained.
earity). FIG. 5 is a diagram showing the conventional linearity measurement method, in which 11 is a light receiving element, 12 is a temperature controller, 13 is a light emitting element, 14 is an attenuator, 15 is an optical fiber, 16
Is an output meter. For example, assuming that the light receiving element is used at a low temperature, the temperature of the temperature controller 12 is set to −40 ° C., and light from the light emitting element 13 is transmitted through the optical fiber 15 via the attenuator 14 to the light receiving element 11. When it is incident on the light emitting element
The current output of the light receiving element 11 with respect to the light energy from 13 is obtained. In general, a current output is represented by electric power as a product of a photocurrent and a bias voltage.

このような発光素子13の光エネルギーをアッテネータ
14で切り換えて受光素子11に入射する光量を変化させ、
入射光パワー(ワット)に対する受光素子11の電流出力
(ワット)をプロットした出力特性を第6図に示してい
る。この第6図において、入射光パワーに比例して電流
出力が増加する場合に、リニアリテイが良いと云うこと
になり、実線で示す曲線Iはリニアリテイの良い受光素
子(良品)、点線で示す曲線IIは低い入射光パワーで直
線性が崩れているからリニアリテイの悪い受光素子(不
良品)である。なお、従来、第6図に示すような曲線を
検出するのは工数がかかるため、通常、曲線上の定めた
3点を測定する方式が採られている。且つ、受光素子11
の温度によってもリニアリティは変化するので、受光素
子11の温度が変動しないように温度制御器12に受光素子
11を収納しているのである。
The light energy of such a light emitting element 13 is attenuated.
Switch with 14 to change the amount of light incident on the light receiving element 11,
FIG. 6 shows output characteristics in which the current output (watt) of the light receiving element 11 is plotted against the incident light power (watt). In FIG. 6, when the current output increases in proportion to the incident light power, it means that the linearity is good. Curve I shown by a solid line is a light receiving element (good product) having good linearity, and curve II shown by a dotted line Is a light receiving element (defective product) with poor linearity because the linearity is broken at low incident light power. Conventionally, since detecting a curve as shown in FIG. 6 requires a lot of man-hour, a method of measuring three specified points on the curve is usually employed. And the light receiving element 11
Since the linearity changes depending on the temperature of the light-receiving element, the temperature controller 12
11 are stored.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

ところで、第5図に示した従来の測定方法は被測定用
の受光素子11がパッケージに組み込んだ完成品であるか
ら、リニアリテイを測定して不良品であると、組立完成
品を廃棄することになり、そうすると組立工数が無駄に
なり、それだけ製造コストがアップすることになる。
By the way, the conventional measuring method shown in FIG. 5 is a completed product in which the light receiving element 11 to be measured is incorporated in a package. If the linearity is measured and the product is defective, the assembled product is discarded. In such a case, the number of assembling steps is wasted, and the manufacturing cost increases accordingly.

従つて、本発明はこのような問題点を解消させ、ウエ
ハーまたはチップの状態でリニアリテイを評価して、製
造コストを低下させることを目的とした評価方法を提案
するものである。
Accordingly, the present invention proposes an evaluation method for solving such a problem and evaluating linearity in a state of a wafer or a chip to reduce manufacturing cost.

〔問題点を解決するための手段〕[Means for solving the problem]

その目的は、半導体受光素子の入射光強度に対する光
電流の出力特性と、該素子のP電極N電極間逆バイアス
電圧に対する該素子のキャパシタンス値の関係との相関
関係を予め求めておく工程と、 評価対象である半導体受光素子の前記逆バイアス電圧
の特定の値に対するキャパシタンス値を測定する工程
と、 測定した前記キャパシタンス値を前記相関関係を参照
することにより評価し、該半導体受光素子の前記出力特
性の直線性の良・不良の判定を行なう工程を有する半導
体受光素子の評価方法によって達成される。
The object is to obtain in advance a correlation between the output characteristic of the photocurrent with respect to the intensity of the incident light of the semiconductor light receiving element and the relationship between the capacitance value of the element and the reverse bias voltage between the P electrode and the N electrode of the element. Measuring a capacitance value of the semiconductor light receiving element to be evaluated with respect to a specific value of the reverse bias voltage; and evaluating the measured capacitance value by referring to the correlation to obtain the output characteristic of the semiconductor light receiving element. This is achieved by a method for evaluating a semiconductor light receiving element having a step of determining whether the linearity is good or bad.

また、その目的は、半導体受光素子の入射光強度に対
する光電流の出力特性と、該素子のP電極N電極間逆バ
イアス電圧に対する該素子のシリーズ抵抗値の関係との
相関関係を予め求めておく工程と、 評価対象である半導体受光素子の前記逆バイアス電圧
の特定の値に対するシリーズ抵抗値を測定する工程と、 測定した前記シリーズ抵抗値を前記相関関係を参照す
ることにより評価し、該半導体受光素子の前記出力特性
の直線性の良・不良の判定を行なう工程を有する半導体
受光素子の評価方法によって達成される。
In addition, the purpose is to obtain in advance the correlation between the output characteristic of the photocurrent with respect to the incident light intensity of the semiconductor light receiving element and the series resistance of the element with respect to the reverse bias voltage between the P electrode and the N electrode of the element. A step of measuring a series resistance value of the semiconductor light receiving element to be evaluated with respect to a specific value of the reverse bias voltage; and evaluating the measured series resistance value by referring to the correlation. This is achieved by a method for evaluating a semiconductor light receiving element, which comprises a step of determining whether the linearity of the output characteristic of the element is good or bad.

〔作 用〕(Operation)

即ち、半導体受光素子の入射光強度に対する光電流の
出力特性をキャパシタンスの逆バイアス電圧依存性から
予め求めておき、この半導体受光素子の逆バイアス電圧
の特定の値に対するキャパシタンスの値を求めることに
より、半導体受光素子の出力特性の直線性を評価するこ
とが可能となり、また、半導体受光素子の入射光強度に
対する光電流の出力特性をシリーズ抵抗の逆バイアス電
圧依存性から予め求めておき、この半導体受光素子の逆
バイアス電圧の特定の値に対するシリーズ抵抗の値を求
めることにより、半導体受光素子の出力特性の直線性を
評価することが可能となります。
That is, the output characteristic of the photocurrent with respect to the incident light intensity of the semiconductor light receiving element is previously obtained from the reverse bias voltage dependency of the capacitance, and the capacitance value for the specific value of the reverse bias voltage of the semiconductor light receiving element is obtained. It is possible to evaluate the linearity of the output characteristics of the semiconductor light receiving element, and to obtain the output characteristics of the photocurrent with respect to the incident light intensity of the semiconductor light receiving element in advance from the dependence of the series resistance on the reverse bias voltage. By determining the value of the series resistance for a specific value of the reverse bias voltage of the device, it is possible to evaluate the linearity of the output characteristics of the semiconductor photo detector.

〔実施例〕〔Example〕

以下、図面を参照して実施例によつて詳細に説明す
る。
Hereinafter, embodiments will be described in detail with reference to the drawings.

第1図は本発明にかかるキャパシタンスのバイアス電
圧依存性、または、シリーズ抵抗のバイアス電圧依存性
の測定方法を示す図で、21はウエハー,22は基板ステー
ジ,23はLCRメータ,24はコンピュータ,25はプロッタであ
る。そうして、ウエハー25内の1つのチップ(素子)の
p−電極にプローバ26を接触させ、そのプローバ26と基
板ステージ22(ウエハー裏面のn−電極に接触してい
る)との間にバイアス電圧を印加する。
FIG. 1 is a diagram showing a method for measuring the bias voltage dependency of the capacitance or the bias voltage dependency of the series resistance according to the present invention, wherein 21 is a wafer, 22 is a substrate stage, 23 is an LCR meter, 24 is a computer, 25 is a plotter. Then, the prober 26 is brought into contact with the p-electrode of one chip (element) in the wafer 25, and a bias is applied between the prober 26 and the substrate stage 22 (which is in contact with the n-electrode on the back surface of the wafer). Apply voltage.

そうして、周波数1MHZ,振幅電圧10mVにて変調した信
号電流を加えて測定したキャパシタンスのバイアス電圧
依存性をコンピュータ24で処理してプロッタ25に記録す
る。第2図(a),(b)はそのキャパシタンスのバイ
アス電圧依存性の測定結果を例示しており、第2図
(a)はリニアリテイの悪い受光素子、第2図(b)は
リニアリテイの良い受光素子の例である。第2図より、
逆バイアス電圧1Vにおけるキャパシタンス(PF)の値を
列記すると、第2図(a)におけるリニアリテイの悪い
受光素子のキャパシタンスは 101.89PF,105.06PF,118.26PF,115.09PF,97.78PF になり、一方の第2図(b)におけるリニアリテイの良
い受光素子のキャパシタンスは 42.15PF,44.12PF,41.74PF,44.62PF,44.66PF となつている。
Then, the bias voltage dependency of the capacitance measured by adding the signal current modulated at the frequency of 1 MHz and the amplitude voltage of 10 mV is processed by the computer 24 and recorded on the plotter 25. 2 (a) and 2 (b) exemplify the measurement results of the dependence of the capacitance on the bias voltage. FIG. 2 (a) shows a light receiving element with poor linearity, and FIG. 2 (b) shows good linearity. It is an example of a light receiving element. From Figure 2,
When the values of the capacitance (PF) at a reverse bias voltage of 1 V are listed, the capacitance of the light receiving element having poor linearity in FIG. In FIG. 2B, the capacitance of the light receiving element having good linearity is 42.15PF, 44.12PF, 41.74PF, 44.62PF, 44.66PF.

従つて、上記の実施例では、1Vの逆バイアス電圧にお
けるキャパシタンスを検出すれば、キャパシタンスの小
さい受光素子がリニアリテイが良く、キャパシタンスの
大きい受光素子がリニアリテイが悪くて、出力特性のリ
ニアリテイ(直線性)を評価することが可能である。な
お、このリニアリテイの量・不良は上記の測定後、組立
完成品について従来の測定方法によつて検出したもので
ある。
Therefore, in the above embodiment, if the capacitance at a reverse bias voltage of 1 V is detected, the light receiving element having a small capacitance has good linearity, the light receiving element having a large capacitance has poor linearity, and the linearity of output characteristics (linearity) It is possible to evaluate It should be noted that the linearity amount / defectiveness is detected by the conventional measuring method for the assembled product after the above-described measurement.

次に、同様の測定条件によつて測定したシリーズ抵抗
のバイアス電圧依存性を説明すると、第3図(a),
(b)はそのシリーズ抵抗のバイアス電圧依存性の測定
結果を示しており、第3図(a)はリニアリテイの良い
受光素子、第3図(b)はリニアリテイの悪い受光素子
の例である。第3図より、その順バイアス電圧(V)に
おけるシリーズ抵抗(Ω)の値を表記すると、リニアリ
テイの良い受光素子の場合は 一方、リニアリテイの悪い受光素子の場合は となつて、明らかに有意差が見られ、シリーズ抵抗の大
きい受光素子はリニアリテイが悪く、シリーズ抵抗の小
さい受光素子はリニアリテイが良い結果となつている。
Next, the bias voltage dependence of the series resistance measured under the same measurement conditions will be described.
3B shows a measurement result of the bias voltage dependence of the series resistance. FIG. 3A shows an example of a light receiving element having good linearity, and FIG. 3B shows an example of a light receiving element having poor linearity. From FIG. 3, when the value of the series resistance (Ω) at the forward bias voltage (V) is described, in the case of a light receiving element having good linearity, On the other hand, in the case of a light receiving element with poor linearity, Therefore, a significant difference is clearly seen, and the light receiving element having a large series resistance has poor linearity, and the light receiving element having a small series resistance has good linearity.

従つて、本発明によれば温度制御器を用いずに常温に
おいて、ウエハーの状態で出力特性のリニアリテイを評
価することができ、そうすれば、リニアリテイの不良品
を組み立てることなく、リニアリテイの良品のみ完成品
に組み立てて、製造コストを低下させることができる。
Therefore, according to the present invention, it is possible to evaluate the linearity of the output characteristics in the state of a wafer at room temperature without using a temperature controller, so that only a non-defective product of linearity can be evaluated without assembling a defective product of linearity. It can be assembled into a finished product to reduce manufacturing costs.

なお、上記はウエハーの状態で評価する実施例である
が、チップに切断した後でも同様に評価できることは云
うまでもない。
Although the above is an example in which the evaluation is performed in the state of the wafer, it goes without saying that the evaluation can be similarly performed even after the wafer is cut into chips.

〔発明の効果〕〔The invention's effect〕

以上の説明から明らかなように、本発明によれば出力
特性のリニアリテイをウエハーまたはチップの状態で評
価でき、製造コストの低減に顕著な効果があるものであ
る。
As is clear from the above description, according to the present invention, the linearity of the output characteristics can be evaluated in the state of a wafer or a chip, which has a remarkable effect in reducing the manufacturing cost.

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

第1図は本発明にかかる測定方法を示す図、 第2図(a),(b)はキャパシタンスのバイアス電圧
依存性を示す図、 第3図(a),(b)はシリーズ抵抗のバイアス電圧依
存性を示す図、 第4図はInGaAs受光素子の断面図、 第5図は従来の測定方法を示す図、 第6図は受光素子の出力特性を示す図である。 図において、 21はウエハー、 22は基板ステージ、 23はLCRメータ、 24はコンピュータ、 25はプロッタ、 26はプローバ を示している。
FIG. 1 is a diagram showing a measuring method according to the present invention, FIGS. 2 (a) and 2 (b) are diagrams showing a bias voltage dependency of capacitance, and FIGS. 3 (a) and 3 (b) are biases of a series resistor. FIG. 4 is a diagram showing voltage dependency, FIG. 4 is a cross-sectional view of an InGaAs light receiving device, FIG. 5 is a diagram showing a conventional measuring method, and FIG. 6 is a diagram showing output characteristics of the light receiving device. In the figure, 21 indicates a wafer, 22 indicates a substrate stage, 23 indicates an LCR meter, 24 indicates a computer, 25 indicates a plotter, and 26 indicates a prober.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】半導体受光素子の入射光強度に対する光電
流の出力特性と、該素子のP電極N電極間逆バイアス電
圧に対する該素子のキャパシタンス値の関係との相関関
係を予め求めておく工程と、 評価対象である半導体受光素子の前記逆バイアス電圧の
特定の値に対するキャパシタンス値を測定する工程と、 測定した前記キャパシタンス値を前記相関関係を参照す
ることにより評価し、該半導体受光素子の前記出力特性
の直線性の良・不良の判定を行なう工程 を有することを特徴とする半導体受光素子の評価方法。
A step of obtaining in advance a correlation between an output characteristic of a photocurrent with respect to an incident light intensity of a semiconductor light receiving element and a relation of a capacitance value of the element with respect to a reverse bias voltage between a P electrode and an N electrode of the element. Measuring a capacitance value of the semiconductor light receiving element to be evaluated with respect to a specific value of the reverse bias voltage; and evaluating the measured capacitance value by referring to the correlation, and outputting the output of the semiconductor light receiving element. A method for evaluating a semiconductor light receiving element, comprising a step of determining whether the linearity of characteristics is good or bad.
【請求項2】半導体受光素子の入射光強度に対する光電
流の出力特性と、該素子のP電極N電極間逆バイアス電
圧に対する該素子のシリーズ抵抗値の関係との相関関係
を予め求めておく工程と、 評価対象である半導体受光素子の前記逆バイアス電圧の
特定の値に対するシリーズ抵抗値を測定する工程と、 測定した前記シリーズ抵抗値を前記相関関係を参照する
ことにより評価し、該半導体受光素子の前記出力特性の
直線性の良・不良の判定を行なう工程 を有することを特徴とする半導体受光素子の評価方法。
2. A method of obtaining a correlation between output characteristics of a photocurrent with respect to an incident light intensity of a semiconductor light receiving element and a series resistance of the element with respect to a reverse bias voltage between a P electrode and an N electrode of the element. Measuring a series resistance value for a specific value of the reverse bias voltage of the semiconductor light receiving element to be evaluated; and evaluating the measured series resistance value by referring to the correlation to evaluate the semiconductor light receiving element. Determining whether the linearity of the output characteristics is good or bad.
JP62306609A 1987-12-02 1987-12-02 Evaluation method of semiconductor photo detector Expired - Lifetime JP2596023B2 (en)

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JP62306609A JP2596023B2 (en) 1987-12-02 1987-12-02 Evaluation method of semiconductor photo detector

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Application Number Priority Date Filing Date Title
JP62306609A JP2596023B2 (en) 1987-12-02 1987-12-02 Evaluation method of semiconductor photo detector

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JPH01146375A JPH01146375A (en) 1989-06-08
JP2596023B2 true JP2596023B2 (en) 1997-04-02

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Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS50126182A (en) * 1974-03-22 1975-10-03
JPS5459890A (en) * 1977-10-20 1979-05-14 Nec Corp Discriminating method of spectral sensitivity characteristics of photo diodes
JPS5754379A (en) * 1980-09-19 1982-03-31 Toshiba Corp Selecting method for light-emitting element

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