JPH03161988A - Semiconductor laser device - Google Patents

Semiconductor laser device

Info

Publication number
JPH03161988A
JPH03161988A JP30168889A JP30168889A JPH03161988A JP H03161988 A JPH03161988 A JP H03161988A JP 30168889 A JP30168889 A JP 30168889A JP 30168889 A JP30168889 A JP 30168889A JP H03161988 A JPH03161988 A JP H03161988A
Authority
JP
Japan
Prior art keywords
layer
gaas
type
interface
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.)
Granted
Application number
JP30168889A
Other languages
Japanese (ja)
Other versions
JP2744093B2 (en
Inventor
Masaharu Honda
正治 本多
Hiroyoshi Hamada
弘喜 浜田
Masayuki Shono
昌幸 庄野
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo Electric 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP30168889A priority Critical patent/JP2744093B2/en
Publication of JPH03161988A publication Critical patent/JPH03161988A/en
Application granted granted Critical
Publication of JP2744093B2 publication Critical patent/JP2744093B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PURPOSE:To prevent P from leaving the crystal surface of A GaInP at the time of re-growth, and improve the interface quality of a constriction layer, by forming an interface protecting layer between the etching surface of a clad layer of a stopper layer and a GaAs current constriction layer. CONSTITUTION:Double hetero junction structure is formed by crystalgrowing the following in order on an n-GaAs substrate 1; an n-GaInP buffer layer 2, an n-AlGaInP clad layer 3, a GaInP active layer 4, a p-AlGaInP clad layer 5, a p-GalnP band gap relieving layer 6, and a p-GaAs contact layer 7. An SiO2 film 13 is formed; by using it as a mask, the layers 7, 6 and a part of the layer 5 are etched; thus a mesa type protrusion 14 is formed. While the SiO2 film 13 is used as a mask as it is, an n-GaIn interface protecting layer 12 and an n-GaAs current constriction layer 8 are grown. The film 13 is eliminated, a p-GaAs contact layer 9 is grown, and a p-side electrode 10 and an n-side electrode 11 are vapor-deposited.

Description

【発明の詳細な説明】 〔産業」一の利用分野〕 本発明は、OaAs系の電流狭窄層を備えたke(k>
 1.n P系可視光半導体レーザ装置に関する。
[Detailed description of the invention] [Field of application in industry] The present invention provides a ke(k>
1. The present invention relates to an nP-based visible light semiconductor laser device.

〔従来の技術〕[Conventional technology]

従来、この種半導体レーザ装置は、例えば特開昭62−
200786号公報(■oIS3/18)ニ示サレテい
るように、MOCVD法(有機金属化学気相成長法)を
用い、n型半導体基板上にAJGa ].n P系のn
型クラッド層,活性層及びp型クラッド層を順次或長さ
せてダプノレヘテロ接合構造を形成すると共に、p型ク
ラッド層をメサ状あるいは構状にエノチングし、これに
n型GaAs電流狭1層を再威長させて構或している。
Conventionally, this type of semiconductor laser device has been disclosed, for example, in Japanese Patent Application Laid-Open No. 1986-
As shown in Publication No. 200786 (■oIS3/18), AJGa ]. n P type n
The type cladding layer, the active layer, and the p-type cladding layer are sequentially elongated to form a double heterojunction structure, and the p-type cladding layer is etched into a mesa shape or structure, and an n-type GaAs current narrow single layer is re-etched on this. It is made to look dignified.

すなわち、第5図は従来の半導体レーザ装置の素子構造
を示してち・り、(1)はn型GaAs基板であり、こ
υ基板(1)上にn型GalnP ハソ7 7層f21
 ,  n型AgGalnP I ランド層(3) ,
 GalnP活性層(41p5A/’GalnP クラ
7ド層(51 , p型Gal.nPバンドギャノプ緩
和層(6)及びp型GaAsコンタクト層(7)を順次
結晶或長させ、活性層(4)とこの両面にそれぞれ接合
シタクラッド層(3) , (51とによりダプノレヘ
テロ接合構造を形成する。
That is, FIG. 5 shows the element structure of a conventional semiconductor laser device. (1) is an n-type GaAs substrate, and on this substrate (1) is formed an n-type GalnP 7 layer f21.
, n-type AgGalnP I land layer (3),
The GalnP active layer (41p5A/'GalnP cladding layer (51), p-type Gal.nP band Ganop relaxation layer (6) and p-type GaAs contact layer (7) are crystallized in sequence, and the active layer (4) and both surfaces thereof A double heterojunction structure is formed by the junction cladding layers (3) and (51), respectively.

尚、緩和層(6)は、クラッドll+51とコンタクト
帝r7)とのバンドギャソプの不連続を緩和するために
設けられている。
Note that the relaxation layer (6) is provided to alleviate the discontinuity of the band gap between the cladding 11+51 and the contact layer 7).

+8+はn型GaAs電流狭窄層であシ、前記コンタク
ト層『7》l緩和層(6)及びクラッド層(5)をメサ
状にエッチングした後,再或長される。
+8+ is an n-type GaAs current confinement layer, which is re-lengthened after etching the contact layer ``7'' l relaxation layer (6) and cladding layer (5) into a mesa shape.

(9)はP型GaAsコンタクト層, noはAu−C
r合金よシなるP側電極、01) (d Au−Sn−
Or合金よりなるn側電極である。
(9) is P-type GaAs contact layer, no is Au-C
r alloy P side electrode, 01) (d Au-Sn-
This is an n-side electrode made of an Or alloy.

ところで、前述した構造においては、電流狭窄層(8)
を再或長する際、エッチングした結晶表面にクラッド層
(5)のAg(ialnP結晶が露出するため、再戒長
に伴なう昇温時に結晶表面よりPが蒸発つ1り離脱し、
結晶表面の損傷を招く不都合がある。
By the way, in the structure described above, the current confinement layer (8)
When re-lengthening, the Ag(ialnP crystal of the cladding layer (5) is exposed on the etched crystal surface, so when the temperature rises due to re-lengthening, P evaporates and leaves the crystal surface.
This has the disadvantage of causing damage to the crystal surface.

このため、前記公報のものでは、昇温時にPHs(ホス
フィン)のガヌを流して昇温に伴々うPの離脱を防止し
、GaAs戒長直前にV族ガスをPHaからA8H8 
(アルシン)(7)ガヌに切換え、(4aの有機金属ガ
スを導入して(4aAsを結晶戊長させる方法を採って
いる。
For this reason, in the above-mentioned publication, a flow of PHs (phosphine) is flowed during temperature rise to prevent the separation of P as the temperature rises, and group V gas is added from PHa to A8H8 immediately before the GaAs precipitate.
(Arsine) (7) A method is adopted in which the organic metal gas of (4a) is introduced to elongate the crystals of (4aAs).

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかし、前述した方法では、再威長に伴なう昇温時のP
の離脱は防止できるものの、V族ガスの切換え時にPの
結晶表面からの離脱が生じ、これに伴なってA7’ (
4a 1nP結晶のエッチング面と或長されたCiaA
sとの界面に欠陥が導入され、素子の寿命等に悪影響を
及ぼす結果となる。
However, in the method described above, P
Although the separation of P can be prevented, when switching the V group gas, P is removed from the crystal surface, and along with this, A7' (
4a Etched surface of 1nP crystal and elongated CiaA
Defects are introduced at the interface with s, resulting in an adverse effect on the life of the element.

本発明は、従来の技術の有するこのような問題点に留意
してなされたものであり、その目的とするところは、C
ia A s系の電流狭窄層を備えたAeGa In 
P系可視光半導体レーザ装置において、再或長時のAI
!Ga In P結晶表面からのPの離脱を防止し、G
aAs系電流狭窄層の界面を良好にすることにある。
The present invention has been made in consideration of such problems of the prior art, and its purpose is to solve
AeGa In with ia As-based current confinement layer
In a P-based visible light semiconductor laser device, AI during re-lengthening
! Preventing the separation of P from the GaInP crystal surface,
The objective is to improve the interface of the aAs-based current confinement layer.

〔課題を解決するための手段〕[Means to solve the problem]

前記目的を達或するために、本発明の半導体レザ装置に
訃いては、第1伝導型クラッド層,活性層及び第2伝導
型クラッド層によりAeGa In P系のダブルへテ
ロ接合構造を形成し、かつ、第2伝導型クラッド層に形
成されるGaAs系の第1伝導型電流狭窄層と第2伝導
型クラッド層會たは該クラッド層のエッチング用ストツ
パ層との間に、電流狭窄層と同じ伝導型を持ち(A4x
Ga+−x)o.51no.5P ( 0,?x(1)
系結晶あるいはGal.nAsP系結晶よりなる界面保
護層を形成したことを特徴とするものである。
In order to achieve the above object, the semiconductor laser device of the present invention includes an AeGaInP-based double heterojunction structure formed by a first conductivity type cladding layer, an active layer, and a second conductivity type cladding layer. , and a current confinement layer is provided between the GaAs-based first conductivity type current confinement layer formed in the second conductivity type cladding layer and the second conductivity type cladding layer or the etching stopper layer of the cladding layer. They have the same conductivity type (A4x
Ga+-x)o. 51 no. 5P (0,?x(1)
system crystal or Gal. It is characterized in that an interface protective layer made of nAsP-based crystal is formed.

〔作用〕[Effect]

前述のように構威された半導体レーザ装置にあっては、
GaAs系第1伝導型電流狭窄層と,第2伝導型クラッ
ド層のエッチング面渣たはこれに予めエッチング用ヌト
ッパ層が形成されている場合にはこのヌトッパ層との間
にPを含む第1伝導型界面保護膜が形成される構造であ
るため、クラツド層のエッチング後,電流狭9層を再或
長ずる際、昇温時に例えばPusのガスを流してクラツ
ド層會たぱストツパ層の結晶表面からのPの離脱を防止
できる上、このガスを流した状態で( Aex GaI
−x)o.s 1no.6P系あるいはGalnAsP
系の界面保護層を形成することができ、従って、電流狭
窄層用GaAsの或長直前にV族ガスをPHaからAs
f{aに切換えても、クラツド層筐たはストツパ層よp
Pが離脱することがなくなり、再或長の界面への欠陥の
導入が防止される。
In the semiconductor laser device configured as described above,
A first conductive layer containing P between the GaAs-based current confinement layer of the first conductivity type and the etched surface residue of the second conductivity type cladding layer or, if a Nutopper layer for etching is formed in advance on this Nutopper layer, is formed. Since the structure is such that a conductive interface protective film is formed, when the current narrowing layer 9 is re-lengthened after etching the cladding layer, for example, Pus gas is flowed while the temperature is raised to increase the crystallization of the cladding layer and the stopper layer. In addition to preventing P from leaving the surface, with this gas flowing (Aex GaI
-x) o. s 1 no. 6P series or GalnAsP
Therefore, just before a certain length of GaAs for the current confinement layer, group V gas is changed from PHa to As.
Even if you switch to f{a, the cladding layer or stopper layer p
P is no longer detached, and defects are prevented from being introduced into the re-elongated interface.

〔実施例〕〔Example〕

本発明の1実施例につき、第1図ないし第4図を用いて
説明する。
One embodiment of the present invention will be explained using FIGS. 1 to 4.

第1図は素子構造を示したものであう、前記第5図で示
した従来のものと異なる点は、p型Al!GalnPク
ラッド層151等のエッチング後に再或長されるn型G
aAs電流狭9層(8)とクラッド層C51等のエッチ
ング面との間にn 型GalnP ((AexGa+−
x)o.51no.5P + x =0)よわなる界面
保護層a2を薄〈形成した点である。
FIG. 1 shows the device structure.The difference from the conventional device shown in FIG. 5 is that p-type Al! n-type G re-lengthened after etching the GalnP cladding layer 151 etc.
An n-type GalnP ((AexGa+-
x)o. 51 no. 5P + x = 0) is formed with a thin interface protective layer a2.

第2図fa)〜fdlはIitI記素子の製造過程を示
したものであり、以下これを用いて製造方法を説明する
FIGS. 2fa) to 2fdl show the manufacturing process of the IitI element, and the manufacturing method will be explained below using this.

同図fa)に示すように、減圧MOCVD法によシ或長
温度720℃で、n型GaAs基板(1)上に、n型G
a I nPハッファ層f21 , n型AgCial
nP クラ7ド層(3) . GalnP活性層(41
.1)型Al!GalnP I ラッド層151,p型
GalnPバンドギャップ緩和層+61及びp型GaA
sコンタクト層f71を順次結晶或長させ、ダブルへテ
ロ接合構造を形成する。
As shown in figure fa), n-type G
a I nP huffer layer f21, n-type AgCial
nP clad 7d layer (3). GalnP active layer (41
.. 1) Type Al! GalnP I rad layer 151, p-type GalnP bandgap relaxation layer +61 and p-type GaA
The s-contact layer f71 is successively crystallized to form a double heterojunction structure.

続いて、同図向に示すように、Si 02膜0を形戒し
、これをマスクにして、GaAs系のコンタクト層(7
)を硫酸系エッチング液を用いてエッチングすると共に
、Ag Ga In P系の緩和層(6)及びp型タラ
ッド層C51をそれぞれHBr (臭化水素)系のエッ
チング液を用いp型クラッド層C51を0.8/lm程
度残るようにしてエッチングし、メサ状凸部04)を形
戒する。
Next, as shown in the same figure, a GaAs-based contact layer (7
) using a sulfuric acid-based etching solution, and etching the AgGaInP-based relaxation layer (6) and the p-type TALLAD layer C51 using an HBr (hydrogen bromide)-based etching solution. Etching is performed so that about 0.8/lm remains to form the mesa-shaped convex portion 04).

次に、同図(clに示すように、S i02膜03をマ
スクにしたFLn型Gal.nP界面保護層02及びn
型C4a A s電流狭窄層(8)をそれぞれ威長温度
650℃で結晶成長する。
Next, as shown in the same figure (cl), the FLn type Gal.nP interface protection layer 02 and n
A type C4a As current confinement layer (8) is grown at a crystal growth temperature of 650°C.

との再或長の際、昇温時にPf{sのガヌを導入し,、
所定或長温度に達した後, PHsガスの導入状態でG
alnP結晶を或長させ、界面保護層αのを形成する。
When re-elongating with Pf{s, Ganu of Pf{s is introduced at the time of temperature rise,
After reaching a predetermined temperature, the G
The AlnP crystal is lengthened to a certain extent to form an interface protective layer α.

更に、V族ガスをPHsからAsHaに切換え、界面保
護層02上にGaAs結晶を戊長させ、電流狭窄層+8
1を形成する。
Furthermore, the V group gas is switched from PHs to AsHa, and the GaAs crystal is elongated on the interface protection layer 02, thereby creating a current confinement layer +8
form 1.

その後、8i02膜的をHF (フッ化水素)系エッチ
ング液を用いて除去し、同図fd)κ示すように、p型
GaASコンタクト層(9)を或長させ、p側電樺帥及
びn側電極(II)をそれぞれ蒸着させて第1図の素子
を完或させる。
Thereafter, the 8i02 film surface was removed using an HF (hydrogen fluoride)-based etching solution, and the p-type GaAS contact layer (9) was lengthened to a certain extent, and the p-side electrode layer and n Side electrodes (II) are respectively deposited to complete the device of FIG.

第3図は、このようにし7て作製された半導体レーザ装
置を、50゜Cに釦いて出力3mWoAPC (オトパ
ワーコントローノレ)動作によシ寿命試験を行った場合
の結果を示したものであり、実線で示す本発明の素子は
、破線で示す従来構造のものに比べ、長寿命化が図れる
ことが明らかである。
Figure 3 shows the results of a life test of the semiconductor laser device fabricated in this manner at 50°C and output 3m WoAPC (Auto Power Controller) operation. It is clear that the device of the present invention shown by the solid line can have a longer lifespan compared to the conventional structure shown by the broken line.

尚、界面保護層qカは薄く形成されているため、熱抵抗
の増加による温度上昇といった問題もほとんどない。
Incidentally, since the interface protective layer q is formed thinly, there is almost no problem of temperature rise due to an increase in thermal resistance.

ところで、Gal.nP結晶は、そのエネノレギギャッ
プが第4図に示すように或長温度に依存するため、Ga
l.nP活性層(41の或長温度とn型(JalnP界
面保護層aカの或長温度とを、例えば実施例のように7
20℃,650℃というように違えることにより、それ
ぞれのエネルギギャップを異ならせ、すなわち界面保護
層0ののエネノレギギャップの方を小さくすることがで
き、従って、この界面保M F (IZが光吸収層とし
て働き、横モード制御型半導体レーザ装置を得ることが
可能になる。
By the way, Gal. Since the energy gap of nP crystal depends on temperature as shown in Figure 4, Ga
l. For example, if a certain long temperature of the nP active layer (41) and a certain long temperature of the n-type (JalnP interface protection layer a) are set to 7 as in the example,
By changing the temperature to 20°C and 650°C, the energy gap can be made different, that is, the energy gap of the interface protective layer 0 can be made smaller. It functions as a light absorption layer, making it possible to obtain a transverse mode control type semiconductor laser device.

尚、前記実施例では、活性層(4)としてGal.nP
を用いたため、界面保護層0ηをn−GalnlFとし
、或長温度を変えて界面保護層αカのエネノレギギャソ
プを活性層(4)のそれより小さくするようにしたが、
活性層(4)を(AeyGa+−y)o.5’no,s
r ( 0≦yく1)で構或し,た場合、界面保護層0
のを(#x 01−gc)0.5 ’no.6 Pで構
或してそのAe組威XをX≦yとすれば、活性層(4)
のエネルギギャップと等しいか小さいエネlレギギャッ
プを有する界面保護層aのを得ることができる。
In the above embodiment, the active layer (4) is made of Gal. nP
was used, the interfacial protective layer 0η was made n-GalnlF, and the long temperature was changed to make the energy gap of the interfacial protective layer α smaller than that of the active layer (4).
The active layer (4) is (AeyGa+-y)o. 5'no,s
If r (0≦y×1), the interface protective layer 0
(#x 01-gc) 0.5' no. If it is composed of 6 P and its Ae group weight X is X≦y, then the active layer (4)
It is possible to obtain an interfacial protective layer a having an energy gap equal to or smaller than the energy gap of a.

又、実施例は、再成長に伴なう昇温時等に訃いてkg 
Ga In P結晶表面からのPの離脱を防止する場合
であるが、GaAs結晶表面及びAe Ga In P
結晶表面それぞれからの■族元素As,I’双方の離脱
を防止する場合には、昇温時にV族ガスとしてAsf{
sとPHBとを同時に導入すると共に、この導入状態で
クラッド層等のエッチング而にGalnAsP系結晶の
界面保護層を或長させればよい。
In addition, in the example, when the temperature rises due to regrowth, etc.
This is a case of preventing the separation of P from the GaInP crystal surface.
In order to prevent the separation of both group Ⅰ elements As and I' from each crystal surface, Asf{
It is sufficient to introduce S and PHB at the same time, and in this introduced state, cladding layers etc. are etched and the interface protective layer of the GalnAsP crystal is lengthened to a certain extent.

更に、P型クラッド層(5}にエッチング停止用のスト
ッパ層(低,J7組或のp型Al!GalnP )を形
戊する場合には、このストソパ層と電流狭窄層との間4 に界面保護層を形成することにより、ストッパ層表面か
らのPの離脱を防止することができる。
Furthermore, when forming a stopper layer (low, J7 group or p-type Al!GalnP) for stopping etching on the P-type cladding layer (5), an interface is formed at 4 between this cladding layer and the current confinement layer. By forming the protective layer, separation of P from the surface of the stopper layer can be prevented.

〔発明の効果〕〔Effect of the invention〕

以上説明し2たように、本発明の半導体レーザ装置によ
ると、クラッド層1たはストッパ層のエッチング表而と
GaAs電流狭窄層との間に界面保護層を形成する構造
であるため、再或長時におけるAeGa In P結晶
表面からのPの離脱を防止することができ、再或長結晶
の界面を良好にし、素子の長寿命化が図れ、信頼性が高
まるものである。
As described above, the semiconductor laser device of the present invention has a structure in which an interface protective layer is formed between the etched surface of the cladding layer 1 or the stopper layer and the GaAs current confinement layer, so that re-orientation is not necessary. It is possible to prevent P from leaving the AeGaInP crystal surface over a long period of time, improve the interface between the long crystals, extend the life of the device, and increase reliability.

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

第1図ないし第4図は本発明による半導体レザ装置の1
実施例を示し、第■図は断面図、第27 fa)〜(d
)はそれぞれ製造過程を示す異なる状態の断面図、第3
図は素子寿命試験結果を示す電流特性図、第4図はGa
lnP結晶におけるエネpギギャソプの或長温度依存性
を示す特性図、第5図は従来例の断面図である。 (3) ・= n if’J AeGalnl’ I 
ラノド胴、(41 =− Gnl.nI’活性層、+5
1−p型AeGalnP クラッド居、it’ll ・
−n型C4*AS電流狭窄層、 0カ ・・n型rJal.nl’界面保護居。
1 to 4 show a semiconductor laser device according to the present invention.
Examples are shown, and Fig. 2 is a cross-sectional view, and Fig.
) are cross-sectional views of different states showing the manufacturing process, respectively.
The figure is a current characteristic diagram showing the element life test results, and Figure 4 is a Ga
FIG. 5 is a characteristic diagram showing the long-term temperature dependence of energy pg in an lnP crystal, and is a cross-sectional view of a conventional example. (3) ・= n if'J AeGalnl' I
Ranod trunk, (41 =- Gnl.nI' active layer, +5
1-p type AeGalnP cladding, it'll ・
-n-type C4*AS current confinement layer, 0ka...n-type rJal. nl' interface protection.

Claims (1)

【特許請求の範囲】 1 第1伝導型クラッド層、活性層及び第2伝導型クラ
ッド層によりダブルヘテロ接合構造を形成し、前記第2
伝導型クラッド層にGaAs系の第1伝導型電流狭窄層
を備えてなるAlGalnP系可視光半導体レーザ装置
において、 前記電流狭窄層と前記第2伝導型クラッド層または該ク
ラッド層のエッチング用ストッパ層との間に、前記電流
狭窄層と同じ伝導型を持ち(Al_xGa_1_−_x
)_0_._5In_0_._5P(0≦x<1)系結
晶あるいはGaInAsP系結晶よりなる界面保護層を
形成したことを特徴とする半導体レーザ装置。
[Scope of Claims] 1. A double heterojunction structure is formed by a first conduction type cladding layer, an active layer, and a second conduction type cladding layer, and the second
In an AlGalnP visible light semiconductor laser device comprising a GaAs-based first conduction type current confinement layer in a conduction type cladding layer, the current confinement layer and the second conductivity type cladding layer or an etching stopper layer for the cladding layer; has the same conductivity type as the current confinement layer (Al_xGa_1_-_x
)_0_. _5In_0_. A semiconductor laser device characterized by forming an interface protective layer made of a _5P (0≦x<1) crystal or a GaInAsP crystal.
JP30168889A 1989-11-20 1989-11-20 Semiconductor laser device Expired - Fee Related JP2744093B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP30168889A JP2744093B2 (en) 1989-11-20 1989-11-20 Semiconductor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP30168889A JP2744093B2 (en) 1989-11-20 1989-11-20 Semiconductor laser device

Publications (2)

Publication Number Publication Date
JPH03161988A true JPH03161988A (en) 1991-07-11
JP2744093B2 JP2744093B2 (en) 1998-04-28

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP30168889A Expired - Fee Related JP2744093B2 (en) 1989-11-20 1989-11-20 Semiconductor laser device

Country Status (1)

Country Link
JP (1) JP2744093B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05110192A (en) * 1991-10-18 1993-04-30 Kubota Corp Semiconductor laser element
US5568501A (en) * 1993-11-01 1996-10-22 Matsushita Electric Industrial Co., Ltd. Semiconductor laser and method for producing the same

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05110192A (en) * 1991-10-18 1993-04-30 Kubota Corp Semiconductor laser element
US5568501A (en) * 1993-11-01 1996-10-22 Matsushita Electric Industrial Co., Ltd. Semiconductor laser and method for producing the same
US5856207A (en) * 1993-11-01 1999-01-05 Matsushita Electric Industrial Co., Ltd. Method for producing a semiconductor laser
US6110756A (en) * 1993-11-01 2000-08-29 Matsushita Electric Industrial Co., Ltd. Method for producing semiconductor laser

Also Published As

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JP2744093B2 (en) 1998-04-28

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