JPH0329193B2 - - Google Patents
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- Publication number
- JPH0329193B2 JPH0329193B2 JP59182081A JP18208184A JPH0329193B2 JP H0329193 B2 JPH0329193 B2 JP H0329193B2 JP 59182081 A JP59182081 A JP 59182081A JP 18208184 A JP18208184 A JP 18208184A JP H0329193 B2 JPH0329193 B2 JP H0329193B2
- Authority
- JP
- Japan
- Prior art keywords
- photodiode
- semiconductor device
- region
- optical semiconductor
- 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.)
- Expired - Lifetime
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Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F30/00—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
- H10F30/20—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors
- H10F30/21—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation
- H10F30/24—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only two potential barriers, e.g. bipolar phototransistors
- H10F30/245—Bipolar phototransistors
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- Light Receiving Elements (AREA)
Description
【発明の詳細な説明】
〈技術分野〉
本発明は半導体装置を用いて波長検知を行なう
光半導体装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION Technical Field The present invention relates to an optical semiconductor device that performs wavelength detection using a semiconductor device.
〈従来技術〉
従来、半導体装置を用いた光検知を行なう光半
導体装置として本発明者等によつて次のような装
置が開発されている。即ち半導体基板の厚さ方向
における光吸収の度合が照射光の波長に依存する
性質を利用し、半導体基板内部に深さを相違させ
て少なくとも2個のPN接合部を形成し、各PN
接合部での光電流出力比を照射光の波長と対応さ
せるものである。第2図は本発明者等によつて開
発された光半導体装置1の断面図で、例えばP型
シリコン基板2にN型導電性を示すエピタキシヤ
ル層3が設けられ、更に該N型エピタキシヤル層
3中に比較的浅くP+拡散が旋こされてP型領域
4が設けられ、P型基板2とN型エピタキシヤル
層3との間で深く位置する第1のPN接合5が形
成され、N型エピタキシヤル層3とP+領域4と
の間で浅く位置する第2のPN接合6が形成され
ている。従来のホトトランジスタにおいては、上
記第2のPN接合に相当するベース・エミツタ間
のPN接合は直ちに光電変換に寄与する処がない
ため半導体領域の極めて限られた領域に設けられ
ていたが、上記開発された光半導体装置1におい
ては第2のPN接合6からも光電流が取り出され
るため、N型エピタキシヤル領域3内の比較的広
い範囲に第2のPN接合6が生じるように拡散領
域のパターンが設計されている。<Prior Art> Conventionally, the following devices have been developed by the present inventors as optical semiconductor devices that perform light detection using semiconductor devices. That is, by utilizing the property that the degree of light absorption in the thickness direction of a semiconductor substrate depends on the wavelength of irradiated light, at least two PN junctions are formed at different depths inside the semiconductor substrate, and each PN junction is
The photocurrent output ratio at the junction is made to correspond to the wavelength of the irradiated light. FIG. 2 is a cross-sectional view of an optical semiconductor device 1 developed by the present inventors, in which, for example, an epitaxial layer 3 exhibiting N-type conductivity is provided on a P-type silicon substrate 2; A relatively shallow P + diffusion is swirled into the layer 3 to provide a P-type region 4 and a first PN junction 5 located deep between the P-type substrate 2 and the N-type epitaxial layer 3 is formed. , a second PN junction 6 located shallowly between the N-type epitaxial layer 3 and the P + region 4 is formed. In conventional phototransistors, the base-emitter PN junction, which corresponds to the second PN junction, is provided in a very limited area of the semiconductor region because it does not immediately contribute to photoelectric conversion. In the developed optical semiconductor device 1, since photocurrent is also taken out from the second PN junction 6, the diffusion region is designed so that the second PN junction 6 is generated in a relatively wide range within the N-type epitaxial region 3. The pattern is designed.
7はN型はピタキシヤル層3を貫通して設けら
れたP+アイソレーシヨン領域である。上記P型
基板2、N型エピタキシヤル領域3及びP+領域
4には夫々オーミツクコンタクトがとられた電極
8,9,10が設けられ、少なくともP+領域4
を被う半導体層上に反射防止膜等の透光性絶縁膜
11(例えばSiO2膜)が被着されている。 Reference numeral 7 denotes a P + isolation region provided through the N-type pitaxial layer 3 . Electrodes 8, 9, and 10 are provided in ohmic contact with the P type substrate 2, the N type epitaxial region 3, and the P + region 4, respectively .
A translucent insulating film 11 (for example, SiO 2 film) such as an antireflection film is deposited on the semiconductor layer covering the semiconductor layer.
第3図は上記光半導体装置1の等価回路図で、
P型基板2とN型エピタキシヤル領域3で第1の
ホトダイオードPD1が形成され、N型エピタキシ
ヤル領域3とP+領域4とで第2のホトダイオー
ドPD2が形成される。 FIG. 3 is an equivalent circuit diagram of the optical semiconductor device 1,
The P-type substrate 2 and the N-type epitaxial region 3 form a first photodiode PD 1 , and the N-type epitaxial region 3 and the P + region 4 form a second photodiode PD 2 .
第4図は上記構造の光半導体装置1における分
光感度特性を示す図で、曲線Aは深いPN接合を
もつ第1のホトダイオードPD1から、曲線Bは浅
いPN接合をもつ第2のホトダイオードPD2から
得られた照射光の波長(λmμ)と感度との関係
を夫々示し、第1のホトダイオードPD1では長波
長成分が吸収され、第2のホトダイオードPD2で
は短波長成分が吸収されている。 FIG. 4 is a diagram showing the spectral sensitivity characteristics of the optical semiconductor device 1 having the above structure, where curve A is from the first photodiode PD 1 having a deep PN junction, and curve B is from the second photodiode PD 2 having a shallow PN junction. The relationship between the wavelength (λmμ) of the irradiated light and the sensitivity obtained from the above is shown, with the first photodiode PD 1 absorbing the long wavelength component, and the second photodiode PD 2 absorbing the short wavelength component.
第5図は上記光半導体装置1を用いてなる波長
検知回路で、第1ホトダイオードPD1及び第2ホ
トダイオードPD2の光出力電流IPD1,IPD2が夫々導
出されて入力インピーダンスの高い演算増幅回路
のOP1及ぼOP2に入力される。該演算増幅回路
OP1及びOP2にはいずれもフイードバツク路に対
数圧縮特性を備えた対数圧縮ダイオードD1,D2
が接続され、入力されたホトダイオードPD1,
PD2の光出力電流が対数圧縮されて出力される。
両演算増幅回路OP1,OP2から導出された出力信
号VOP1,VOP2は続いて夫々抵抗R1或いは抵抗R2
を介してオペアンプOP3の端子或いは端子に
入力される。ここでオペアンプOP3に接続された
抵抗R1,R2,R3,R4を各抵抗値が予めR1=R2,
R3=R4の関係になるように設計するとにより、
オペアンプ出力として上記VOP1とVOP2を減算した
値に比例するVoutは両ホトダイオードPD1,PD2
の光出力電流IPD1,IPD2の比を対数圧縮した値
ogIPD1/IPD2に比例した値として得られる。 FIG. 5 shows a wavelength detection circuit using the optical semiconductor device 1 described above, in which the optical output currents I PD1 and I PD2 of the first photodiode PD 1 and the second photodiode PD 2 are derived, respectively, into an operational amplifier circuit with high input impedance. OP 1 and OP 2 are entered. The operational amplifier circuit
OP 1 and OP 2 both have logarithmic compression diodes D 1 and D 2 with logarithmic compression characteristics in their feedback paths.
is connected and input photodiode PD 1 ,
The optical output current of PD 2 is logarithmically compressed and output.
The output signals V OP1 and V OP2 derived from both operational amplifier circuits OP 1 and OP 2 are then connected to a resistor R 1 or a resistor R 2 respectively.
It is input to the terminal or terminals of operational amplifier OP3 via. Here, the resistance values of the resistors R 1 , R 2 , R 3 , and R 4 connected to the operational amplifier OP 3 are set in advance as R 1 = R 2 ,
By designing to have the relationship R 3 = R 4 ,
Vout, which is proportional to the value obtained by subtracting the above V OP1 and V OP2 as the operational amplifier output, is the output of both photodiodes PD 1 and PD 2.
The value obtained by logarithmically compressing the ratio of the optical output current I PD1 and I PD2 of
Obtained as a value proportional to ogI PD1 /I PD2 .
第6図の実線データは上記波長検知回路出力
Voutと照射光の波長(λmμ)との関係を示す図
で、ほぼ直線関係が得られ、照射光の波長に応じ
た値の出力信号を得ることができることがわか
る。従つて光半導体装置の分光感度特性が予め決
定されれば、光出力比と波長の関係は一義的に決
定され、波長が不明な光が光半導体装置に照射さ
れた場合に、波長検知回路の出力によつて波長を
測定することができる。 The solid line data in Figure 6 is the output of the wavelength detection circuit above.
This is a diagram showing the relationship between Vout and the wavelength (λmμ) of the irradiation light, and it can be seen that a nearly linear relationship is obtained, and an output signal having a value corresponding to the wavelength of the irradiation light can be obtained. Therefore, if the spectral sensitivity characteristics of the optical semiconductor device are determined in advance, the relationship between the optical output ratio and the wavelength is uniquely determined, and when the optical semiconductor device is irradiated with light of unknown wavelength, the wavelength detection circuit The wavelength can be measured by the output.
しかし、上記実線のデータは照射光が光半導体
装置1の中央部に入射した時のデータであつて、
照射光が光半導体装置1の周辺部や側面部に入射
した場合、特性は上記実線のデータからずれ、破
線で示すようになる。つまり照射光の入射する位
置により光電流比が異なるのである。 However, the data indicated by the solid line above is data when the irradiation light enters the central part of the optical semiconductor device 1, and
When the irradiation light is incident on the periphery or side surface of the optical semiconductor device 1, the characteristics deviate from the solid line data and become as shown by the broken line. In other words, the photocurrent ratio differs depending on the position where the irradiation light is incident.
さて、光半導体装置1をハーメチツクシールで
シールし表面にレンズ付キヤツプを設けた場合、
照射光は光半導体装置1の中央部分に集まるので
比較的問題が少ない。しかし光半導体装置1を樹
脂モールドした場合は照射光は中央部のみならず
周辺部或いは側面部からも入射する度合が大きく
なり、この様な場合は照射光の入射位置によつて
光電流比が異なる為信頼性の高い波長検出が難し
くなる。 Now, when the optical semiconductor device 1 is sealed with a hermetic seal and a cap with a lens is provided on the surface,
Since the irradiation light is concentrated at the center of the optical semiconductor device 1, there are relatively few problems. However, if the optical semiconductor device 1 is molded with resin, the irradiation light will be incident not only from the center but also from the periphery or side surfaces, and in such a case, the photocurrent ratio will depend on the incident position of the irradiation light. The difference makes reliable wavelength detection difficult.
〈目的〉
本発明は以上の従来点に鑑みなされたものであ
り照射光が中央部のみならず周辺部或いは側面部
から入射しても信頼性の高い波長検知を行なうこ
とのできる光半導体装置を提供することをその目
的とする。<Purpose> The present invention has been made in view of the above-mentioned conventional points, and provides an optical semiconductor device that can perform highly reliable wavelength detection even when irradiation light is incident not only from the center but also from the periphery or side surfaces. Its purpose is to provide.
〈実施例〉
以下本発明に係る光半導体装置の一実施例につ
いて図面を用いて詳細に説明する。<Example> An example of the optical semiconductor device according to the present invention will be described in detail below with reference to the drawings.
第1図は本発明に係る光半導体装置の一実施例
の側断面図である。光半導体装置1の基板として
P型シリコン基板2が用いられ、該P型シリコン
基板2にN型導電性を示すエピタキシヤル層3が
設けられ、更に該N型エピタキシヤル層3中に比
較的浅くP+拡散が旋こされてP型領域4が設け
られる。この構造によればP型基板2とN型エピ
タキシヤル層3との間で深く位置する第1のPN
接合5が形成され、N型エピタキシヤル層3と
P+領域4との間で浅く位置する第2のPN接合6
が形成されている。7はN型エピタキシヤル層3
を貫通して設けられたP+アイソレーシヨン領域
である。上記P型基板2、N型エピタキシヤル領
域3及びP+領域4には夫々オーミツクコンタク
トがとられた電極8,9,10が設けられ、少な
くともP+領域4を被う半導体層上に反射防止膜
等の透光性絶縁膜11(例えばSiO2膜)が被着
されている。更に上記電極9は上記透光性絶縁膜
11上においてP型領域4の周辺部、P型領域4
の周辺のN型エピタキシヤル領域3部、P+アイ
ソレーシヨン領域7を被うように延出して被着さ
れる。そして、P+アイソレーシヨン領域7及び
さらにその外側の領域にわたる位置に第3のホト
ダイオード12が形成される。該第3のホトダイ
オード12は短絡状態に保たれる。即ちチツプ周
辺部においてN型エピタキシヤル層13とP+ア
イソレーシヨン領域7及びP型領域2よりなる第
3のホトダイオード12が形成され、更にP+拡
散によるP型領域14及びN+拡散によるN型領
域15が形成されアルミニウム電極16によつて
両者が短絡(短絡部では一箇所でよい)されてい
る。尚、上記P型領域14及びN型領域15はP
型領域4及びN型領域17と同時に形成すれば効
率的である。上記第3のホトダイオード12の有
効受光領域は第1図の1点鎖線(A),(B)の外
側である。即ち第2のPN接合6によるホトダイ
オードと上記第3のホトダイオード12との有効
受光領域の境界線が上記1点鎖線(A),(B)で
ある。以上の第1図の構造によれば光半導体装置
1の周辺部や側面部に入射した光によつて発生し
た少数キヤリアは第3のホトダイオード12によ
つて多く吸収される。この構造の場合周辺部或い
は側面部からの入射光による少数キヤリアの拡散
長を考慮する必要が無く、有効受光領域の境界線
(1点鎖線(A)(B))の外側の寸法を小さくで
きるので装置全体の大きさを小型化できるという
利点を有する。 次に第7図に第1図を更に改良
した構造の実施例の側断面図を示す。同図におい
て、18はリンガラス、ポリイミド系樹脂等から
なる層間絶縁物であり、該層間絶縁物を介してア
ルミニウム膜19を被覆し、該アルミニウム膜1
9によつて電極9,16の隙間部分を遮光してい
る。上記アルミニウム膜19を設けることにより
電極配線の自由度を増加せしめることができる。 FIG. 1 is a side sectional view of an embodiment of an optical semiconductor device according to the present invention. A P-type silicon substrate 2 is used as a substrate of the optical semiconductor device 1, an epitaxial layer 3 exhibiting N-type conductivity is provided on the P-type silicon substrate 2, and a relatively shallow layer 3 is provided in the N-type epitaxial layer 3. P + diffusion is swirled to provide a P type region 4 . According to this structure, the first PN located deep between the P-type substrate 2 and the N-type epitaxial layer 3
A junction 5 is formed between the N-type epitaxial layer 3 and
Second PN junction 6 located shallowly between P + region 4
is formed. 7 is an N-type epitaxial layer 3
This is a P + isolation region provided through the . The P type substrate 2, the N type epitaxial region 3 , and the P + region 4 are provided with electrodes 8, 9, and 10, respectively, which are in ohmic contact. A light-transmitting insulating film 11 (for example, SiO 2 film) such as a prevention film is deposited. Further, the electrode 9 is located on the periphery of the P-type region 4 on the transparent insulating film 11 .
It extends and is deposited so as to cover the N type epitaxial region 3 and the P + isolation region 7 around the periphery. A third photodiode 12 is formed at a position covering the P + isolation region 7 and an area further outside thereof. The third photodiode 12 is kept short-circuited. That is, a third photodiode 12 consisting of an N-type epitaxial layer 13, a P + isolation region 7, and a P-type region 2 is formed in the peripheral area of the chip, and a P-type region 14 by P + diffusion and an N-type region 14 by N + diffusion are formed. A mold region 15 is formed, and both are short-circuited by an aluminum electrode 16 (one short-circuit portion is sufficient). Note that the P type region 14 and the N type region 15 are P type regions 14 and N type regions 15.
It is efficient to form the type region 4 and the N-type region 17 at the same time. The effective light-receiving area of the third photodiode 12 is outside the dashed-dotted lines (A) and (B) in FIG. That is, the boundaries of the effective light receiving area between the photodiode formed by the second PN junction 6 and the third photodiode 12 are the dashed-dotted lines (A) and (B). According to the structure shown in FIG. 1 described above, a large amount of minority carriers generated by light incident on the periphery or side surface of the optical semiconductor device 1 is absorbed by the third photodiode 12. In this structure, there is no need to consider the diffusion length of minority carriers due to incident light from the periphery or side, and the dimensions outside the boundary line (dotted chain lines (A) and (B)) of the effective light receiving area can be reduced. This has the advantage that the overall size of the device can be reduced. Next, FIG. 7 shows a side sectional view of an embodiment of a structure that is a further improvement of FIG. 1. In the figure, 18 is an interlayer insulating material made of phosphor glass, polyimide resin, etc., which covers the aluminum film 19 through the interlayer insulating material.
9 shields the gap between the electrodes 9 and 16 from light. By providing the aluminum film 19, the degree of freedom in electrode wiring can be increased.
〈効果〉
以上の本発明によれば光半導体装置を小型化
し、かつ周辺部或いは側面部から入射した光の悪
影響を防止して正確な光出力比と波長の関係が得
られる光半導体装置を提供できる。<Effects> According to the present invention, it is possible to provide an optical semiconductor device that is miniaturized, prevents the adverse effects of light incident from the peripheral portion or side portion, and obtains an accurate relationship between optical output ratio and wavelength. can.
第1図は本発明に係る光半導体装置の一実施例
の側断面図、第2図は従来の光半導体装置の側断
面図、第3図は等価回路図、第4図は分光感度特
性のグラフ図、第5図は波長検知回路の回路図、
第6図は波長検知回路出力と照射光の波長の関係
を示すグラフ図、第7図は本発明に係る光半導体
装置の他の実施例の側断面図を示す。図中、1…
…光半導体装置、2……基板、3……N型エピタ
キシヤル層、4……P型領域、5……第1のPN
接合、6……第2のPN接合、7……P+アイソレ
ーシヨン領域、8,9,10……電極、11……
透光性絶縁膜、12……第3のホトダイオード、
13……N型エピタキシヤル層、14……P型領
域、15……N型領域、16……アルミニウム電
極、17……N型領域、18……層間絶縁物、1
9……アルミニウム膜。
FIG. 1 is a side sectional view of an embodiment of an optical semiconductor device according to the present invention, FIG. 2 is a side sectional view of a conventional optical semiconductor device, FIG. 3 is an equivalent circuit diagram, and FIG. 4 is a diagram of spectral sensitivity characteristics. Graph diagram, Figure 5 is a circuit diagram of the wavelength detection circuit,
FIG. 6 is a graph showing the relationship between the wavelength detection circuit output and the wavelength of irradiated light, and FIG. 7 is a side sectional view of another embodiment of the optical semiconductor device according to the present invention. In the figure, 1...
... Optical semiconductor device, 2 ... Substrate, 3 ... N type epitaxial layer, 4 ... P type region, 5 ... First PN
Junction, 6... Second PN junction, 7... P + isolation region, 8, 9, 10... Electrode, 11...
Transparent insulating film, 12... third photodiode,
13... N-type epitaxial layer, 14... P-type region, 15... N-type region, 16... aluminum electrode, 17... N-type region, 18... interlayer insulator, 1
9...Aluminum film.
Claims (1)
2つのPN接合により第1のホトダイオード及び
第2のホトダイオードが形成され、光が照射され
た状態で上記第1のホトダイオードと第2のホト
ダイオードの各PN接合に生じた光電流を夫々導
出する電極が設けられた光半導体装置において、
上記各PN接合部の周辺に設けられたアイソレー
シヨン領域及びさらにその外側の領域にわたる位
置に、短絡状態に保持された第3のホトダイオー
ドを形成したことを特徴とする光半導体装置。1 A first photodiode and a second photodiode are formed by two PN junctions having different depths in the thickness direction of the semiconductor substrate, and the first photodiode and the second photodiode are connected to each other when irradiated with light. In an optical semiconductor device provided with electrodes for respectively deriving photocurrents generated in each PN junction,
An optical semiconductor device characterized in that a third photodiode maintained in a short-circuited state is formed at a position covering an isolation region provided around each of the PN junctions and a region further outside the isolation region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59182081A JPS6158280A (en) | 1984-08-29 | 1984-08-29 | Optical semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59182081A JPS6158280A (en) | 1984-08-29 | 1984-08-29 | Optical semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6158280A JPS6158280A (en) | 1986-03-25 |
| JPH0329193B2 true JPH0329193B2 (en) | 1991-04-23 |
Family
ID=16112018
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59182081A Granted JPS6158280A (en) | 1984-08-29 | 1984-08-29 | Optical semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6158280A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS51138185A (en) * | 1975-05-26 | 1976-11-29 | Oki Electric Ind Co Ltd | Semi-conductor device |
| JPS55150280A (en) * | 1979-05-11 | 1980-11-22 | Sharp Corp | Device for correcting light semiconductor device |
-
1984
- 1984-08-29 JP JP59182081A patent/JPS6158280A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6158280A (en) | 1986-03-25 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EXPY | Cancellation because of completion of term |