JPS5871682A - Semiconductor light emitting device - Google Patents
Semiconductor light emitting deviceInfo
- Publication number
- JPS5871682A JPS5871682A JP56169759A JP16975981A JPS5871682A JP S5871682 A JPS5871682 A JP S5871682A JP 56169759 A JP56169759 A JP 56169759A JP 16975981 A JP16975981 A JP 16975981A JP S5871682 A JPS5871682 A JP S5871682A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- type
- transistor
- semiconductor
- laser
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/06—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
- H01S5/062—Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes
- H01S5/06203—Transistor-type lasers
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S5/00—Semiconductor lasers
- H01S5/20—Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
- H01S5/24—Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a grooved structure, e.g. V-grooved, crescent active layer in groove, VSIS laser
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Solid State Image Pick-Up Elements (AREA)
- Photo Coupler, Interrupter, Optical-To-Optical Conversion Devices (AREA)
Abstract
Description
【発明の詳細な説明】 本発明は半導体発光装置に関する。[Detailed description of the invention] The present invention relates to a semiconductor light emitting device.
近年、半導体レーザと他の能動素子9例えばFET等を
組み合わせたり、或りは、半導体レーザに発光装置以外
の新たな機能を持たせて複合装置を構成する試みがなさ
れている。In recent years, attempts have been made to construct a composite device by combining a semiconductor laser with another active element 9 such as an FET, or by giving a semiconductor laser a new function other than a light emitting device.
第1図に於いてはplFin形ガリウム・ヒ素(GaA
s)基板、2は口形ガリウム・アルミニウム・ヒ素(G
aAIAs)り2ラド層e 3 FiGaAIAs
活性層t4Fip形GaAlAs クラッド層、5Fi
p形GaAs層。In Figure 1, plFin type gallium arsenide (GaA
s) Substrate, 2 is a mouth-shaped gallium aluminum arsenic (G
aAIAs) 2 Rad layers e 3 FiGaAIAs
Active layer t4Fip type GaAlAs cladding layer, 5Fi
p-type GaAs layer.
6はp形GaAl人S高抵抗層、7はn形Ga As
PET動作層*sFs亜鉛(Zn)を拡散して形成した
p形ストライプ生成用領斌、9は二酸化シリコン(8i
0宜)絶縁層、1GはPETソース電極、11FiF’
ETゲート電極、12はFETドレイン電極、13はn
側電極をそれぞれ示す。6 is a p-type GaAl layer with high resistance, 7 is an n-type GaAs layer
PET active layer
0) Insulating layer, 1G is PET source electrode, 11FiF'
ET gate electrode, 12 is FET drain electrode, 13 is n
The side electrodes are shown respectively.
従来、レーザ(第1図装置左側)と駆動素子、ζこでは
FET(第1図装置左側)金一体化するために、高抵抗
層6とFET動作層7の二つの層を余分に設ける必要が
あった。Conventionally, in order to integrate the laser (on the left side of the apparatus in Figure 1) and the drive element, here the FET (on the left side of the apparatus in Figure 1), it was necessary to provide two extra layers: a high resistance layer 6 and an FET operating layer 7. was there.
本発明の目的は、半導体レーザの半導体層の構造を利用
して2wI半導体層の一部から構成される駆動素子を設
けることにより、半導体レーザとその駆動素子を同一基
板に形成し、従来、駆動素子形成の為に必要な余分な半
導体層を取り除いた半導体発光装置を提供するにある。It is an object of the present invention to utilize the structure of the semiconductor layer of a semiconductor laser to provide a driving element composed of a part of a 2wI semiconductor layer, thereby forming a semiconductor laser and its driving element on the same substrate. It is an object of the present invention to provide a semiconductor light emitting device in which unnecessary semiconductor layers necessary for element formation are removed.
本発明は、レーザ発振を起こす活性層と、該活性層より
大きい禁制帯幅を有し、且つ該活性層を挾んだ第1及び
第2のクラッド層とストライプ形状の電流路を画定する
p −n−p形石しくFin−p−n形構造の半導体層
とを基板上に有するストライブ形ダブルへテロ構造の半
導体レーザ装置と、該半導体レーザが設けられた前記基
板上に前記p−n−p形若しく形石n−p−n形構造の
半導体層を有するトランジスタ或いはフォトトランジス
タとを設けたものである。The present invention provides an active layer that causes laser oscillation, a p-cladding layer that has a larger forbidden band width than the active layer, and that defines a stripe-shaped current path with first and second cladding layers that sandwich the active layer. - a semiconductor laser device having a stripe type double hetero structure having a semiconductor layer having a Fin-p-n type structure on a substrate; A transistor or a phototransistor having a semiconductor layer having an n-p type or an amorphous n-p-n type structure is provided.
半導体レーザに設けられているp−n−p形石しくはn
−p−n形構造の半導体層は、動作時p−n逆バイアス
がかかる為、該半導体層には電流が流れず、電流阻止領
域としての役目を果し、半導体レーザの電流路を画定す
る為に設けられていた。そこで9本発明ではとのp−n
−p形石しくはn−p−n形構造の半導体層を利用して
半導体レーザの駆動素子となるトランジスタ或いはフォ
トトランジスタを形成しようというものである。A p-n-p type stone provided in a semiconductor laser, or n
- A semiconductor layer with a p-n type structure is subjected to a p-n reverse bias during operation, so no current flows through the semiconductor layer, which serves as a current blocking region and defines the current path of the semiconductor laser. It was set up for the purpose. Therefore, in the present invention, the p-n
- The idea is to form a transistor or a phototransistor which becomes a driving element of a semiconductor laser by using a semiconductor layer having a p-type structure or an n-pn-type structure.
以下1本発明の一実施例を用いて本発明を説明すること
にする。第2図は本発明の一実施例の半導体発光装置の
断面図である。The present invention will be explained below using one embodiment of the present invention. FIG. 2 is a sectional view of a semiconductor light emitting device according to an embodiment of the present invention.
第2図の半導体装置の製造工程を簡単に説明することに
する。n形インジウム・リン(InP)基板14上に不
純物が1017〜10 ”cm−”ドーグされた厚さ2
〜3Pr11のn形InP層15.不純物が10 ”〜
10 ” an−3ドープされた厚さ1.5 )o>
OF形InP層16を順次液相成長させ死後、n形In
P層15に達する深さのV字型の溝を形成する。次に、
#V字型の溝内に不純物が1.17〜10cm ドー
プされたn形InPグラッド層17.P形着しく Ld
n形インジウム・ガリウム・ヒ素・リン(InGaA
sP)活性層18を順次液相成長させると。The manufacturing process of the semiconductor device shown in FIG. 2 will be briefly explained. An n-type indium phosphide (InP) substrate 14 is doped with impurities to a thickness of 10 cm to 10 cm.
~3Pr11 n-type InP layer 15. Impurities are 10”~
10” an-3 doped thickness 1.5)o>
The OF-type InP layer 16 is successively liquid-phase grown, and after death, the n-type InP layer 16 is
A V-shaped groove with a depth reaching the P layer 15 is formed. next,
#N-type InP grading layer doped with 1.17 to 10 cm of impurity in the V-shaped groove 17. P-shaped Ld
n-type indium gallium arsenic phosphorus (InGaA
sP) The active layer 18 is sequentially grown in liquid phase.
該7字型の牌が形成されていないP形1nP層16上に
厚さ0.3Pmのn形InP層19.厚さ0.05 P
wmのInGaAsP層20が形成される。この時溝内
の活性層は中央部で0.15prag度になる。P形1
nPをInGaAsP層20表面から1〜15P+mの
厚さに液相成長させ2表面が平担なP形InPクラッド
層21を形成し、更に厚さ0.5P01のP形InGa
AsP層22を液酸成長させる。半導体レーザとトラン
ジスタを電気的に分離する為に層形InP層15に達す
る深さまでエツチングし1分離の為の溝を形成する。ト
ランジスタun形InP層15とP形InP層16とn
形InPHII19のn −p−n形の構造のInP半
導体層を利用して形成されるので、トランジスタを形成
すべき領域には、n形InP層19の一部を除いてn形
InP層19.P杉苔しくけn形のInGaAsP層2
0.p形InP層21.P形InGaAsP層22をエ
ツチングによって除去する。−半導体レーザが形成され
たP形InGaAsP層22上にレーザのP側電極兼ト
ランジスタのエミッタ又はコレクタ電極23.トランジ
スタ形成領域のn形InP層19上にレーザのn1lK
極兼トランジスタのコレクタ又はエミッタ電極24.該
トランジスタ形成領域のP形InP層16の一部にベー
ス電極25をそれぞれ形成する。An n-type InP layer 19 with a thickness of 0.3 Pm is formed on the P-type 1nP layer 16 on which the 7-shaped tiles are not formed. Thickness 0.05P
A wm InGaAsP layer 20 is formed. At this time, the active layer in the groove has a degree of 0.15 prag at the center. P type 1
A P-type InP cladding layer 21 with a flat surface is formed by liquid phase growth of nP to a thickness of 1 to 15P+m from the surface of the InGaAsP layer 20, and then a P-type InGa with a thickness of 0.5P01 is formed.
The AsP layer 22 is grown using liquid acid. In order to electrically isolate the semiconductor laser and the transistor, etching is performed to a depth that reaches the layered InP layer 15 to form a trench for one isolation. Transistor un type InP layer 15, p type InP layer 16 and n
Since it is formed using an InP semiconductor layer having an n-p-n structure of type InPHII 19, a region where a transistor is to be formed has an n-type InP layer 19. N-type InGaAsP layer 2
0. p-type InP layer 21. The P-type InGaAsP layer 22 is removed by etching. - On the P-type InGaAsP layer 22 on which the semiconductor laser is formed, there is a P-side electrode of the laser and an emitter or collector electrode 23 of the transistor. Laser n1lK is applied on the n-type InP layer 19 in the transistor formation region.
Collector or emitter electrode of the transistor which also serves as a pole 24. A base electrode 25 is formed on a portion of the P-type InP layer 16 in the transistor formation region.
尚、半導体レーザの電流路は7字型の溝の外に形成され
たP形InP層16とn形InP層19のp−n逆バイ
アスによって電流が阻止され、7字型の溝内のみを電流
が流れる。Note that the current path of the semiconductor laser is blocked by the p-n reverse bias of the P-type InP layer 16 and the n-type InP layer 19 formed outside the figure-7 groove, and the current flows only inside the figure-7 groove. Current flows.
このレーザではv n p n構造の半導体質をト
ランジスタとして用いてベース電極24の電位を変化さ
せる事により、レーザに変調をかけることができる。ま
な、ベース即ちトランジスタ形成領域のP形1nP層1
6に光26を照射することにより、n−p−n形構造の
半導体層をフォトトランジスタとして用いることができ
。In this laser, the laser can be modulated by using a semiconductor material with a v n p n structure as a transistor and changing the potential of the base electrode 24 . Mainly, the P-type 1nP layer 1 in the base, that is, the transistor formation region.
By irradiating light 26 to 6, the semiconductor layer having an npn type structure can be used as a phototransistor.
k
一つのチップで、受は取った数41Wの光を数mWのレ
ーザ光に増幅して送り出すことができ、光中継器として
用いる事ができる。この時、このフォトトランジスタが
受光することのできる光の波長はベースを形成する半導
体層の禁制帯@に相当する波長よりも短波点の光である
。従って2本実施例ではn−P−n形構造の半導体層が
InPで形成されているので、 InPの波長より短波
長の光1例えばガリウム・アルミニウム・ヒ素(()a
ALAs)の光音受光することができる。また目的に応
じてベースのInPiIaGaAsPとしてバンドギツ
プを小さくして受光できる光の波長範囲を広くすること
ができる。k With one chip, the receiver can amplify the light of several 41 W into a laser beam of several mW and send it out, and it can be used as an optical repeater. At this time, the wavelength of light that can be received by this phototransistor is shorter than the wavelength corresponding to the forbidden band of the semiconductor layer forming the base. Therefore, in this embodiment, since the semiconductor layer with the n-P-n type structure is formed of InP, light with a wavelength shorter than that of InP (1), such as gallium, aluminum, arsenic (()a
It is possible to receive photo-sounds of ALAs). Furthermore, depending on the purpose, the band gap can be reduced by using InPiIaGaAsP as the base to widen the wavelength range of light that can be received.
n −p−n若しくFip−n−pがトランジスタとし
て有効に働く為にはベースに相当する層が少数キャリア
の拡散長より薄いことが必要であるが、これはベースの
厚さを1.5Pm以下にする事により充分実現される。In order for n-p-n or Fip-n-p to function effectively as a transistor, it is necessary that the layer corresponding to the base be thinner than the diffusion length of minority carriers. This can be sufficiently achieved by setting the temperature to 5 Pm or less.
本発明の一実施例によれば、半導体レーザの電流路を画
定する為に設けられたn形InPJi15とP形InP
層16とn形InP層19のn −p−n形半導体層を
利用第3図は第2図の半導体レーザと異った構造を有す
る場合の本発明の一実施例の半導体装置断面図である。According to one embodiment of the present invention, an n-type InPJi 15 and a p-type InP provided to define a current path of a semiconductor laser
FIG. 3 is a cross-sectional view of a semiconductor device according to an embodiment of the present invention, which uses n-p-n type semiconductor layers of layer 16 and n-type InP layer 19. be.
第3図に於いて、37はn形InP基板、28はn形り
InPfラッド層、29はn形InGaAsP活性層、
30り
はP形InP Ifラッド層、31はn形InGaAs
P層、32はP形InP層、33はP形InGaAsP
層、34はP側電極、35はn側電極、36#iペース
電極をそれぞれ示している。In FIG. 3, 37 is an n-type InP substrate, 28 is an n-type InPf rad layer, 29 is an n-type InGaAsP active layer,
30 is P-type InP If rad layer, 31 is n-type InGaAs
P layer, 32 is P type InP layer, 33 is P type InGaAsP
34 indicates a P-side electrode, 35 indicates an N-side electrode, and 36#i pace electrode.
夕
このレーザでは電流路はP形InPjjラッド層30と
n形I n GaAs P層31のp−n逆バイアスに
よって電流が阻止され、n形InGaAiP層31が形
成されていない領域に電流は絞られ、該領域が電流路と
なる。また、トランジスタはこの電流路を画定する為の
半導体層、即ちn形InGaAsP活性層29とP形I
nPクラッド層30とn形InGaAs P層31のn
−p−n形の構造の半導体層を利用して前述の実施例と
同様にトランジスタ或いはフォトトランジスタを形成す
る。尚、この装置でtjn−p−n形の半導体層の中に
活性層29が含まれているので、不純物濃度をトランジ
スタに合わせて自由に選択することはできない。In this laser, the current path is blocked by the p-n reverse bias of the P-type InPjj rad layer 30 and the n-type InGaAs P layer 31, and the current is narrowed to the region where the n-type InGaAiP layer 31 is not formed. , the region becomes a current path. The transistor also has semiconductor layers for defining this current path, that is, an n-type InGaAsP active layer 29 and a p-type I
nP cladding layer 30 and n-type InGaAs P layer 31
A transistor or a phototransistor is formed using a semiconductor layer having a -pn type structure in the same manner as in the previous embodiment. In this device, since the active layer 29 is included in the tjn-pn type semiconductor layer, the impurity concentration cannot be freely selected depending on the transistor.
本発明によれば、半導体レーザを構成するn−p−it
形形石くtfp−n−p形半導体層の構造を利用して同
一基板にトランジスタ或いはフォトトランジスタを形成
することができる。従って、トランジスタ或いはフォト
トランジスタを形成する為に余分に半導体層を形成する
必要はない。According to the present invention, n-p-it constituting a semiconductor laser
A transistor or a phototransistor can be formed on the same substrate by utilizing the structure of the TFP-NP type semiconductor layer. Therefore, there is no need to form an extra semiconductor layer to form a transistor or phototransistor.
【図面の簡単な説明】
の半導体発光装置の断面図、第3図は第2図の半導体レ
ーザと異った構造を有する場合の本発明の一実施例の装
置の断面図である。
6 高抵抗層
7 F’BT動作層
15.1G 、形InP層BRIEF DESCRIPTION OF THE DRAWINGS FIG. 3 is a cross-sectional view of a device according to an embodiment of the present invention having a structure different from that of the semiconductor laser shown in FIG. 2. 6 High resistance layer 7 F'BT operation layer 15.1G, InP layer
Claims (1)
帯幅を有し、且つ該活性層を挾んだ第1及び第2のクラ
ッド層と、ストライプ形状の電流路を画定するp−n−
p形、7しくはn−p−n形構造の半導体層とを基板上
に有するストライプ形ダブルへテロ構造の半導体レーザ
装置と皺半導体レーザが設けられた前記基板上に帥記p
−n−p形若しくはn −p−n形構造の半導体層を有
するトランジスタ或いはフォトトランジスタとを設けた
ことを特徴とする半導体発光装置。an active layer that causes radar oscillation; first and second cladding layers that have a larger forbidden band width than the active layer and sandwich the active layer; and a p-n- layer that defines a stripe-shaped current path.
A striped double heterostructure semiconductor laser device having a p-type, 7- or n-p-n structure semiconductor layer on the substrate and a wrinkled semiconductor laser are provided on the substrate.
- A semiconductor light-emitting device comprising a transistor or a phototransistor having a semiconductor layer having an n-p type or n-p-n type structure.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56169759A JPS5871682A (en) | 1981-10-23 | 1981-10-23 | Semiconductor light emitting device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP56169759A JPS5871682A (en) | 1981-10-23 | 1981-10-23 | Semiconductor light emitting device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5871682A true JPS5871682A (en) | 1983-04-28 |
Family
ID=15892318
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP56169759A Pending JPS5871682A (en) | 1981-10-23 | 1981-10-23 | Semiconductor light emitting device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5871682A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58164255U (en) * | 1982-04-28 | 1983-11-01 | オムロン株式会社 | Light emitting light receiving element |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51139789A (en) * | 1975-05-29 | 1976-12-02 | Fujitsu Ltd | Photo-electric conversion semiconductor device |
-
1981
- 1981-10-23 JP JP56169759A patent/JPS5871682A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS51139789A (en) * | 1975-05-29 | 1976-12-02 | Fujitsu Ltd | Photo-electric conversion semiconductor device |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS58164255U (en) * | 1982-04-28 | 1983-11-01 | オムロン株式会社 | Light emitting light receiving element |
JPS6320128Y2 (en) * | 1982-04-28 | 1988-06-03 |
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