JPS5941317B2 - Manufacturing method of semiconductor laser device - Google Patents
Manufacturing method of semiconductor laser deviceInfo
- Publication number
- JPS5941317B2 JPS5941317B2 JP54130387A JP13038779A JPS5941317B2 JP S5941317 B2 JPS5941317 B2 JP S5941317B2 JP 54130387 A JP54130387 A JP 54130387A JP 13038779 A JP13038779 A JP 13038779A JP S5941317 B2 JPS5941317 B2 JP S5941317B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- type
- semiconductor layer
- conductivity type
- laser device
- 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
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
- H01S5/20—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
- H01S5/22—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 ridge or stripe structure
- H01S5/223—Buried stripe structure
- H01S5/2238—Buried stripe structure with a terraced structure
-
- 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
- H01S5/02—Structural details or components not essential to laser action
- H01S5/024—Arrangements for thermal management
- H01S5/02461—Structure or details of the laser chip to manipulate the heat flow, e.g. passive layers in the chip with a low heat conductivity
-
- 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
- H01S5/04—Processes or apparatus for excitation, e.g. pumping, e.g. by electron beams
- H01S5/042—Electrical excitation ; Circuits therefor
- H01S5/0425—Electrodes, e.g. characterised by the structure
- H01S5/04256—Electrodes, e.g. characterised by the structure characterised by the configuration
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Geometry (AREA)
- Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
- Semiconductor Lasers (AREA)
Description
【発明の詳細な説明】
本発明は低しきい値電流を有し、かつしきい値電流の温
度特性の良い半導体レーザ装置の製造法法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing a semiconductor laser device having a low threshold current and good temperature characteristics of the threshold current.
半導体レーザ装置でレーザ発振を生ずるしきい値電流を
小さくすることは極めて望ましく、このため構造はいく
つか知られているが単一モード発振の得られるTJS形
レーザ装置は特に優れたものである。It is extremely desirable to reduce the threshold current that causes laser oscillation in a semiconductor laser device, and for this purpose, several structures are known, but a TJS type laser device that can achieve single mode oscillation is particularly excellent.
第1図は従来のTJSレーザ装置の基本的な構造を示す
斜視図で、図において1はP形砒化ガリウム(GaAs
)基板、2、3、4、5、および6はそれぞれGaAs
基板1の一方の主面上に液相成長法に依つて順次成長さ
れたN形GaAs層、、p形アルミニウム・ガリウム・
砒素(AIGaAs)層、N形AlGaAs層、N形G
aAs活性層、及びN形AlGaAs層である。Figure 1 is a perspective view showing the basic structure of a conventional TJS laser device.
) Substrates 2, 3, 4, 5, and 6 are each GaAs
N-type GaAs layers, p-type aluminum, gallium, and
Arsenic (AIGaAs) layer, N-type AlGaAs layer, N-type G
an aAs active layer and an N-type AlGaAs layer.
7はP形
AlGaAs層、8はこのP形AlGaAs層からGa
As基板1及びエピタキシャル層2〜6にフ P形不純
物を拡散して形成したP形層であり、9は活性層5にP
形不純物を拡散して形成された活性領域である。7 is a P-type AlGaAs layer, and 8 is Ga from this P-type AlGaAs layer.
9 is a P-type layer formed by diffusing P-type impurities into the As substrate 1 and epitaxial layers 2 to 6;
This is an active region formed by diffusing type impurities.
また10及び11はそれぞれN側及びP側電極である。
第2図A−Dはこの従来のTJSレーザ装置の5 製造
方法を示すための、その各階段における断面図であるが
、その大略は第1図についての装置の構成から明らかで
あるので、重複を避けて概説に止める。Further, 10 and 11 are N-side and P-side electrodes, respectively.
2A to 2D are cross-sectional views of each step of this conventional TJS laser device to show the manufacturing method, but since the outline is clear from the device configuration in FIG. Avoid this and stick to the general outline.
まずP形GaAs基板1の上に液相エピタキシヤル法に
依つて層2〜6をエピタキシヤル成長させる(第2図A
)。そしてこの様にして得たウエハ上に窒化シリコン(
Si3N4)膜などのマスク15を形成する(第2図B
)。化学エツチング又はエピキシヤル成長前メルトエツ
チングに依りSi3N4膜15を形成していない部分を
GaAs基板1に達するまでエツチングし溝部16を形
成(第2図C)した後、P形AlGaAs層7を構部1
6にのみ選択的にエピタキシヤル成長する。First, layers 2 to 6 are epitaxially grown on a P-type GaAs substrate 1 by a liquid phase epitaxial method (see Fig. 2A).
). Then, silicon nitride (
A mask 15 such as Si3N4) film is formed (Fig. 2B).
). After etching the portion where the Si3N4 film 15 is not formed until it reaches the GaAs substrate 1 by chemical etching or pre-epitaxial melt etching to form the groove 16 (FIG. 2C), the P-type AlGaAs layer 7 is etched into the structural portion 1.
Epitaxial growth is selectively performed only on 6.
またP形AlGaAs層7を成長させ、その途中にP形
不純物をGaAs基板1及びエピタキシヤル層2〜6に
拡散させ、そこにP形層8を形成する(第2図D)。Further, a P-type AlGaAs layer 7 is grown, and a P-type impurity is diffused into the GaAs substrate 1 and epitaxial layers 2 to 6 during the growth to form a P-type layer 8 there (FIG. 2D).
しかる後、Si3N4膜15を除去し、N側及びP側電
極を形成し、チツプ形状に分割して装置は完了する。と
ころが上記従来の装置ではその製造工程において、上述
の第2図Bに示したように、選択成長工程で選択成長マ
スク15を必要とする。Thereafter, the Si3N4 film 15 is removed, N-side and P-side electrodes are formed, and the device is divided into chip shapes to complete the device. However, in the manufacturing process of the conventional apparatus, as shown in FIG. 2B, the selective growth mask 15 is required in the selective growth process.
そしてこのマスク15は、通常Si3N4膜を使用する
が、Si3N4膜は下地のAlGaAs又はGaAs層
と熱膨張係数が異なるため、エピタキシヤル成長層に応
力がかかる。特にSi3N4膜の付いた部分と付いてな
い部分との境界部には応力が集中し、 二選択成長工程
中にエピタキシヤル層に欠陥を発生させる。この欠陥は
GaAs活性領域9にまで侵入して、レーザダイオード
の寿命を短かくし、しかも逆方向特性を悪くするなどの
問題があつた。また上記従来の装置ではP−N接合がチ
ツブ表面Jに露出しており、そのためN側電極10がチ
ツプ表面に一溝にしか形成できない。そのため組立には
、レーザ発振動作中に発熱する活性領域9をチツプの上
方に位置させる所謂アツプサイドアツプ法にしか組立て
る事ができない。アツプサイドア5ツプ法では活性領域
9で発生する熱の拡散が厚みの厚い基板1を通してされ
ねばならない。このため従来の半導体レーザ装置では、
そのしきい値電流が増加するばかりでなく、発熱に依る
特性劣化が早く生じるなどの問題があつた。さらに、上
記4従来の装置の製造方法では、選択成長を行うために
一度エピタキシヤル成長したウエハを加工する工程を止
むなくされていた。そのため、選択成長用のマスクパタ
ーン15の形成等の取扱い時にエピタキシヤルウエハに
歪が入つたり、汚染して、半導体レーザ装置の特性に悪
影響をもたらす原因となつた。また、選択成長工程で、
一度エピタキシヤル成長したウエハが再度高温雰囲気に
晒されるため、最初にエピタキシヤル成長したウエハの
表面が熱分解したり酸化して半導体レーザ装置の特性に
悪影響をおよぼすなどの問題があつた。この発明は、上
述の様な点に鑑みてなされたものであつて、エビタキシ
ヤル層への応力の発生原因となるSi3N4膜等のマス
クを全く使用せず、またP−N接合がチツプの表面に形
成されず、従つてその全面に電極取付が可能であり、さ
らに一度のエピタキシヤル成長で活性領域まで形成する
ことのできる半導体レーザ装置の製造方法を提供するも
のである。第3図はこの発明に依る半導体レーザ装置の
一例の構造を示す斜視図である。This mask 15 normally uses a Si3N4 film, but since the Si3N4 film has a thermal expansion coefficient different from that of the underlying AlGaAs or GaAs layer, stress is applied to the epitaxially grown layer. In particular, stress is concentrated at the boundary between the portions with and without the Si3N4 film, causing defects in the epitaxial layer during the selective growth process. These defects invaded the GaAs active region 9, shortening the life of the laser diode and causing problems such as deterioration of reverse characteristics. Further, in the conventional device described above, the P-N junction is exposed on the chip surface J, and therefore the N-side electrode 10 can be formed in only one groove on the chip surface. Therefore, assembly can only be carried out by the so-called upside-up method in which the active region 9, which generates heat during laser oscillation, is located above the chip. In the upside-down method, the heat generated in the active region 9 must be diffused through the thick substrate 1. For this reason, in conventional semiconductor laser devices,
There were problems in that not only the threshold current increased, but also characteristics deteriorated quickly due to heat generation. Furthermore, in the above-mentioned four conventional device manufacturing methods, in order to perform selective growth, the process of processing the wafer once epitaxially grown is unavoidable. As a result, the epitaxial wafer may be distorted or contaminated during handling such as forming the mask pattern 15 for selective growth, which may adversely affect the characteristics of the semiconductor laser device. In addition, in the selective growth process,
Since the wafer that has been epitaxially grown is once again exposed to a high-temperature atmosphere, there have been problems such as thermal decomposition or oxidation of the surface of the wafer on which epitaxial growth was first performed, which adversely affects the characteristics of the semiconductor laser device. This invention was made in view of the above-mentioned points, and does not use any mask such as Si3N4 film that causes stress to the epitaxial layer, and also has a P-N junction on the surface of the chip. Therefore, it is possible to attach electrodes to the entire surface of the semiconductor laser device, and to provide a method for manufacturing a semiconductor laser device in which an active region can be formed in one epitaxial growth. FIG. 3 is a perspective view showing the structure of an example of a semiconductor laser device according to the present invention.
12は段差を設けたN形GaAs基板、4はN形AlG
aAs層、5はN形GaAs活性層、6はN形AlGa
As層、3はP形AlGaAs層、2はN形GaAs層
であり、7はP形AlGaAs層、13はP形GaAs
コンタクト層である。12 is an N-type GaAs substrate with a step, 4 is an N-type AlG
aAs layer, 5 is N-type GaAs active layer, 6 is N-type AlGa
As layer, 3 is P-type AlGaAs layer, 2 is N-type GaAs layer, 7 is P-type AlGaAs layer, 13 is P-type GaAs layer.
This is the contact layer.
また8はP形AlGaAs層7からエピタキシヤル層4
,5,6,3及び2にP形不純物を拡散したP形層であ
る。14はGaAs基板12に形成されたP形GaAs
層である。Further, 8 is the epitaxial layer 4 from the P-type AlGaAs layer 7.
, 5, 6, 3, and 2 are P-type layers in which P-type impurities are diffused. 14 is P-type GaAs formed on the GaAs substrate 12.
It is a layer.
9はGaAs活性層5の一部にP形不純物の拡散により
形成された活性領域である。Reference numeral 9 denotes an active region formed in a part of the GaAs active layer 5 by diffusion of P-type impurities.
また10及び11はそれぞれN側及びP側電極である。
ここでP形GaAs層14及びP形AlGaAs層3は
その各両側をN形層ではさんだN−P−N構造を形成し
ており、レーザ動作時には逆バイアスとなり電流が流れ
ず、活性領域9に有効に電流集中する構造になつている
。第4図A−Dはこの発明になる製造方法の一実施例を
説明するための各段階における断面図である。Further, 10 and 11 are N-side and P-side electrodes, respectively.
Here, the P-type GaAs layer 14 and the P-type AlGaAs layer 3 form an N-P-N structure in which each side is sandwiched between N-type layers, and during laser operation, the current is reverse biased and no current flows, causing the active region 9 to It has a structure that effectively concentrates current. FIGS. 4A to 4D are cross-sectional views at each stage for explaining an embodiment of the manufacturing method according to the present invention.
まずN形GaAs基板12の表面に拡散又はエピタキシ
ヤル成長にてP形層14を形成したものに、ホトレジス
ト等のマスクを帯状に形成して化学エツチングに依り溝
16を形成後、レジストマスクを除去して表面を清浄に
する(第4図A)。次に上記溝16を設けた基板全面に
、エピタキシヤル成長を行う。まず、GaAs基板12
を設けた溝に添つてN形AlGaAs層4、N形GaA
s活性層5、N形AlGaAs層6、及びP形AlGa
As層3を設け、次に溝16を埋める様に、N形GaA
s層2をエピタキシヤル成長する(第4図B)。First, a P-type layer 14 is formed on the surface of an N-type GaAs substrate 12 by diffusion or epitaxial growth, a band-shaped mask such as photoresist is formed, a groove 16 is formed by chemical etching, and then the resist mask is removed. to clean the surface (Figure 4A). Next, epitaxial growth is performed on the entire surface of the substrate in which the groove 16 is provided. First, the GaAs substrate 12
N-type AlGaAs layer 4, N-type GaA
s active layer 5, N-type AlGaAs layer 6, and P-type AlGa
An As layer 3 is provided, and then an N-type GaA layer is formed so as to fill the trench 16.
The s-layer 2 is epitaxially grown (FIG. 4B).
ここでGaAs基板12に設けた溝に添つて成長させる
には、成長時の徐冷速度を0.5de9/Mm以上にす
ればよく、上記溝を埋める様に成長させるには、成長時
の徐冷速度を0.3de9/Mm以下にすればよい。こ
の様にしてエピタキシヤル成長したウエハをその表面か
ら各エピタキシヤル層4,5,6,3,2の少なくとも
各一部に達するまでメルトエツチングに衣り除去し(第
4図C)、引き続いてP形AlGaAs層7及びP形G
aAs層13を成長する。なおP形AlGaAs層7の
ドーパントにはZnやCd等P形不純物でかつ結晶中へ
の拡散速度の早いものを使用することに依り、上記P形
AlGaAs層7及びP形GaAsコンタクト層13の
成長中に前記エピタキシヤル層に拡散されP層8が形成
される。(第4図D)。しかる後、P形GaAsコンタ
クト層13及びN形GaAs基板12にそれぞれP側及
びN側電極を付けチツプ状に分離することに依りレーザ
装置が完成する。尚、上記実施例ではGaAs−AjG
aAs系結晶を用いた場合について述べたが、一般に禁
制帯巾の異なる半導体結晶を用いた半導体レーザ装置に
広く適用できる。Here, in order to grow along the grooves provided in the GaAs substrate 12, the slow cooling rate during growth should be set to 0.5 de9/Mm or more, and in order to grow so as to fill the grooves, the slow cooling rate during growth should be The cooling rate may be set to 0.3 de9/Mm or less. The epitaxially grown wafer is removed from its surface by melt etching until at least a portion of each epitaxial layer 4, 5, 6, 3, and 2 is reached (FIG. 4C), and then P-type AlGaAs layer 7 and P-type G
An aAs layer 13 is grown. The growth of the P-type AlGaAs layer 7 and the P-type GaAs contact layer 13 is improved by using a P-type impurity such as Zn or Cd which has a high diffusion rate into the crystal as a dopant for the P-type AlGaAs layer 7. A P layer 8 is formed by diffusing into the epitaxial layer. (Figure 4D). Thereafter, P-side and N-side electrodes are attached to the P-type GaAs contact layer 13 and the N-type GaAs substrate 12, respectively, and separated into chips to complete the laser device. In the above embodiment, GaAs-AjG
Although the case using an aAs-based crystal has been described, the present invention can be widely applied to semiconductor laser devices using semiconductor crystals having different forbidden band widths.
更に各部分の伝導形はこの実施例を逆にしてもよい事は
自明である。またP形GaAs層14及びP形AlGa
As層3は無効電流の流れるのを防止するために形成し
たものであるが、これらの層は10Ω?以上の高比抵抗
層であつても効果は全く同様である。Furthermore, it is obvious that the conduction type of each part may be reversed from this embodiment. In addition, the P-type GaAs layer 14 and the P-type AlGa
The As layer 3 is formed to prevent the flow of reactive current, but the resistance of these layers is 10Ω? Even with the above-mentioned high resistivity layer, the effect is exactly the same.
また上記実施例ではシングルヘテロ接合形TJSレーザ
の構造に限つて述べたが、P形AlGaAs層7をp+
形拡散層とするホモ接合形においても本発明の効果は同
様である。ホモ接合形TJSレーザを製造するには、第
4図Bを形成後、第5図に示すようにエピタキシヤル成
長表面の全面よりp+拡散を行つてp+拡散層17を形
成し、引き続いてドライブに依りP形層を形成すればよ
い。Furthermore, in the above embodiment, the structure of a single heterojunction TJS laser was described, but the P-type AlGaAs layer 7 is
The effects of the present invention are also similar in the case of a homojunction type in which a shape diffusion layer is used. To manufacture a homojunction type TJS laser, after forming the layer shown in FIG. 4B, as shown in FIG. 5, p+ diffusion is performed from the entire surface of the epitaxial growth surface to form a p+ diffusion layer 17. Therefore, a P-type layer may be formed.
また上記実施例では活性領域9をヘキ開端面に垂直に直
線状に形成した場合について述べたが、上記P形GaA
s活性領域9は前述の様に、屈折率の小さいAlGaA
s層4,6,7とN形GaAs層5で囲まれているゐで
強いインデイツクスガイデイング構造となる。そのため
活性領域はガイドの強さに応じて曲率を持たせる事がで
き、これを円形にすればリングレーザとして使用する事
も可能である。以上説明した様に、この発明に係る半導
体レーザ装置及びその製造方法では、エピタキシヤル成
長前に基板に溝を形成して、その溝部を利用して活性領
域を形成するため、Si3N4膜などのマスクを必要と
しないので、Si3N4膜と半導体層との熱膨張係数の
差異による悪影響がさけられる。Further, in the above embodiment, a case was described in which the active region 9 was formed in a straight line perpendicular to the helical end face, but the P-type GaA
As mentioned above, the active region 9 is made of AlGaA with a small refractive index.
Surrounded by the S layers 4, 6, and 7 and the N-type GaAs layer 5, a strong index guiding structure is formed. Therefore, the active region can have a curvature depending on the strength of the guide, and if it is made circular, it can also be used as a ring laser. As explained above, in the semiconductor laser device and its manufacturing method according to the present invention, a groove is formed in the substrate before epitaxial growth and an active region is formed using the groove, so a mask such as a Si3N4 film is used. is not required, so that the adverse effects caused by the difference in thermal expansion coefficient between the Si3N4 film and the semiconductor layer can be avoided.
また、電流を活性領域に効率よく集中させるために、無
効電流の流れやすい部分に逆バイアス層を設けた構造で
ある。また、本発明に依れば、エピタキシヤル成長工程
を一回の成長工程で行えるので、再現性が良くしかも途
中工程での汚染がない。さらに、本構造ではP−N接合
が半導体チツプ表面に出て来ないので、全面に電極が形
成でき、放熱の良いアツプサイドダウンマウント法も可
能となる。以上示した様に本発明に依れば、レーザ発振
時におけるしきい値電流が低く、温度特性が良く、しか
も寿命の長い半導体レーザ装置を製造し得る。Furthermore, in order to efficiently concentrate current in the active region, the structure is such that a reverse bias layer is provided in a portion where reactive current tends to flow. Further, according to the present invention, since the epitaxial growth process can be performed in one growth process, reproducibility is good and there is no contamination during the process. Furthermore, in this structure, since the PN junction does not appear on the surface of the semiconductor chip, electrodes can be formed on the entire surface, and an upside-down mounting method with good heat dissipation is also possible. As described above, according to the present invention, it is possible to manufacture a semiconductor laser device that has a low threshold current during laser oscillation, has good temperature characteristics, and has a long life.
第1図は従来のTJS形半導体レーザ装置の基本的な構
造を示す斜視図、第2図A−Dはこの従来装置の製造方
法を示すためのその各段階における断面図、第3図は本
発明に係る半導体レーザ装置の一例の構造を示す斜視図
、第4図A−Dはこの発明に係る製造方法の一実施例を
説明するためのその各段階における断面図、第5図は本
発明の他の実施例を示す断面図である。
図において、12はN形GaAs基板、16は溝、5は
活性層、4,6はN形AlGaA8層、14,3は無効
電流防止用P形層、7はP形AlGaAs層、8はP形
拡散層、9は活性領域である。Figure 1 is a perspective view showing the basic structure of a conventional TJS type semiconductor laser device, Figures 2A-D are cross-sectional views at each stage showing the manufacturing method of this conventional device, and Figure 3 is the main structure of the conventional TJS type semiconductor laser device. A perspective view showing the structure of an example of a semiconductor laser device according to the invention, FIGS. 4A to 4D are cross-sectional views at each stage for explaining an embodiment of the manufacturing method according to the invention, and FIG. FIG. 3 is a sectional view showing another embodiment of the invention. In the figure, 12 is an N-type GaAs substrate, 16 is a groove, 5 is an active layer, 4 and 6 are 8 N-type AlGaA layers, 14 and 3 are P-type layers for preventing reactive current, 7 is a P-type AlGaAs layer, and 8 is a P-type layer. 9 is an active region.
Claims (1)
差を設け、上記半導体基板の上記主面上に上記段差に沿
つて第1の導電形を有する第1の半導体層と、上記第1
の半導体層より禁制帯巾の狭い第1の導電形の第2の半
導体層と、上記第2の半導体層より禁制帯巾の広い第1
の導電形の第3の半導体層と、上記第2の半導体層より
禁制帯巾の広い第2の導電形を有する半導体または高比
抵抗体からなる第4の層を形成し、上記第4の層の表面
上にその段差を減少するように上記第1の半導体層より
禁制帯巾の狭い第1の導電形を有する第5の半導体層を
形成した後、上記第5の半導体層の表面からエッチング
に依り上記第1乃至第5の層の少なくとも各一部を露出
させ、その露出表面全面から所定深さに第2の導電形決
定不純物を導入して、この表面上に上記第2の半導体層
より禁制帯巾の広い第2の導電形を有する第6の半導体
層と、上記第6の半導体層より禁制帯巾の狭い第2の導
電形を有する第7のコンタクト層を形成して成る半導体
レーザ装置の製造方法。1. A step is provided on a part of one main surface of a semiconductor substrate of a first conductivity type, and a first semiconductor layer of a first conductivity type is formed on the main surface of the semiconductor substrate along the step; 1st above
a second semiconductor layer of a first conductivity type having a narrower forbidden band width than the semiconductor layer; and a first semiconductor layer having a wider forbidden band width than the second semiconductor layer.
a third semiconductor layer having a conductivity type of After forming a fifth semiconductor layer having a first conductivity type with a narrower forbidden band width than the first semiconductor layer so as to reduce the step difference on the surface of the layer, from the surface of the fifth semiconductor layer At least a portion of each of the first to fifth layers is exposed by etching, and a second conductivity type determining impurity is introduced to a predetermined depth from the entire exposed surface, and the second semiconductor layer is formed on this surface. A sixth semiconductor layer having a second conductivity type whose forbidden band width is wider than that of the sixth semiconductor layer, and a seventh contact layer having a second conductivity type whose forbidden band width is narrower than that of the sixth semiconductor layer. A method for manufacturing a semiconductor laser device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54130387A JPS5941317B2 (en) | 1979-10-09 | 1979-10-09 | Manufacturing method of semiconductor laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP54130387A JPS5941317B2 (en) | 1979-10-09 | 1979-10-09 | Manufacturing method of semiconductor laser device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5654086A JPS5654086A (en) | 1981-05-13 |
| JPS5941317B2 true JPS5941317B2 (en) | 1984-10-05 |
Family
ID=15033100
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP54130387A Expired JPS5941317B2 (en) | 1979-10-09 | 1979-10-09 | Manufacturing method of semiconductor laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5941317B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62150308A (en) * | 1985-12-25 | 1987-07-04 | Sumitomo Electric Ind Ltd | Light emitting element with optical fiber |
| JPS62150307A (en) * | 1985-12-25 | 1987-07-04 | Sumitomo Electric Ind Ltd | Photodetector with optical fiber |
-
1979
- 1979-10-09 JP JP54130387A patent/JPS5941317B2/en not_active Expired
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62150308A (en) * | 1985-12-25 | 1987-07-04 | Sumitomo Electric Ind Ltd | Light emitting element with optical fiber |
| JPS62150307A (en) * | 1985-12-25 | 1987-07-04 | Sumitomo Electric Ind Ltd | Photodetector with optical fiber |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5654086A (en) | 1981-05-13 |
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