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JPS641072B2 - - Google Patents
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JPS641072B2 - - Google Patents

Info

Publication number
JPS641072B2
JPS641072B2 JP72282A JP72282A JPS641072B2 JP S641072 B2 JPS641072 B2 JP S641072B2 JP 72282 A JP72282 A JP 72282A JP 72282 A JP72282 A JP 72282A JP S641072 B2 JPS641072 B2 JP S641072B2
Authority
JP
Japan
Prior art keywords
layer
semiconductor
current blocking
buried
mesa stripe
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
Application number
JP72282A
Other languages
Japanese (ja)
Other versions
JPS58118184A (en
Inventor
Mitsuhiro Kitamura
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.)
NEC Corp
Original Assignee
Nippon 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP72282A priority Critical patent/JPS58118184A/en
Publication of JPS58118184A publication Critical patent/JPS58118184A/en
Publication of JPS641072B2 publication Critical patent/JPS641072B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure 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
    • H01S5/22Structure 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
    • H01S5/227Buried mesa structure ; Striped active layer
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure 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
    • H01S5/2054Methods of obtaining the confinement
    • H01S5/2059Methods of obtaining the confinement by means of particular conductivity zones, e.g. obtained by particle bombardment or diffusion
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure 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
    • H01S5/22Structure 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
    • H01S5/227Buried mesa structure ; Striped active layer
    • H01S5/2275Buried mesa structure ; Striped active layer mesa created by etching
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure 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
    • H01S5/22Structure 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
    • H01S5/227Buried mesa structure ; Striped active layer
    • H01S5/2275Buried mesa structure ; Striped active layer mesa created by etching
    • H01S5/2277Buried mesa structure ; Striped active layer mesa created by etching double channel planar buried heterostructure [DCPBH] laser

Landscapes

  • Physics & Mathematics (AREA)
  • Geometry (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 本発明は活性層の周囲をよりエネルギーギヤツ
プが大きく屈折率の小さな半導体材料で埋め込ん
だ埋め込みヘテロ構造半導体レーザに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a buried heterostructure semiconductor laser in which an active layer is surrounded by a semiconductor material having a larger energy gap and a lower refractive index.

埋め込みヘテロ構造半導体レーザ(BH−LD)
は低い発振しきい値電流、安定化された発振横モ
ード、高温動作可能などの優れた特性を有してい
るため、光フアイバ通信用光源として注目を集め
ている。本願の発明者らは特願昭56−166666号明
細書に示した様に、2本のほぼ平行な溝にはさま
れて形成された発光再結合する活性層を含むメサ
ストライプ以外で確実に電流ブロツク層が形成で
き、したがつて温度特性に優れ、種々の基板処理
過程でのダメージを受けることが少なく製造歩留
りの向上したIn1-xGaxAsyP1-yBH−LDを発明し
た。しかしながらこの構造のBH−LDでは発光
再結合する活性層を含むメサストライプをはさん
でいる溝の幅が小さい場合、その部分においては
電流ブロツク層の成長速度が大きく、p−InP電
流ブロツク層、n−InP電流ブロツク層の積層に
際し、特にn−InP電流ブロツク層がメサストラ
イプ上部で連続して成長してしまうことがあり、
歩留りの低下を招いていた。またそれを防ぐため
に溝の幅を大きくすると、溝部分での電流ブロツ
ク層のブレークダウン耐圧が十分とれなくなるた
めに、BH−LDのもれ電流が大きくなり、特性
にもバラツキを生ずることがあつた。
Buried heterostructure semiconductor laser (BH-LD)
Because it has excellent properties such as a low oscillation threshold current, a stabilized oscillation transverse mode, and the ability to operate at high temperatures, it is attracting attention as a light source for optical fiber communications. As shown in Japanese Patent Application No. 56-166666, the inventors of the present application have reliably developed a method other than a mesa stripe that includes an active layer that recombines light and is sandwiched between two substantially parallel grooves. Invented an In 1-x Ga x As y P 1-y BH-LD that can form a current blocking layer, has excellent temperature characteristics, is less susceptible to damage during various substrate processing processes, and has improved manufacturing yields. did. However, in a BH-LD with this structure, if the width of the groove between the mesa stripes containing the active layer that undergoes luminescent recombination is small, the growth rate of the current blocking layer is high in that part, and the p-InP current blocking layer, When laminating the n-InP current blocking layer, the n-InP current blocking layer may grow continuously on the top of the mesa stripe.
This resulted in a decrease in yield. In addition, if the width of the groove is increased to prevent this, the breakdown voltage of the current blocking layer in the groove part cannot be maintained sufficiently, which may increase the leakage current of the BH-LD and cause variations in characteristics. Ta.

本発明の目的は上記の欠点を除去し、電流ブロ
ツク層のブレークダウン耐圧が高く、結晶成長の
再現性がよく、製造歩留りの大幅に向上したBH
−LDを提供することにある。
The purpose of the present invention is to eliminate the above-mentioned drawbacks, and to provide a BH that has a high breakdown voltage of the current blocking layer, good reproducibility of crystal growth, and significantly improved manufacturing yield.
- To provide LD.

本発明によれば、第1導電型半導体基板上に少
くとも活性層、第2導電型半導体クラツド層む半
導体多層膜を成長させた多層膜構造半導体ウエフ
アを、活性層よりも深くメサエツチングしてメサ
ストライプを形成した後埋め込み成長してなる埋
め込みヘテロ構造半導体レーザにおいて、発光再
結合する活性層を含むメサストライプが2つの溝
によつてはさまれてなり、2つの溝の底面部に第
2導電型半導体領域が形成され、メサストライプ
の上面のみを除いて第1導電型半導体電流ブロツ
ク層が形成され、さらに第1導電型半導体電流ブ
ロツク層よりもエネルギーギヤツプの小さな半導
体層、全面にわたつて第2導電型埋め込み層が順
次積層されてなることを特徴とする埋め込みヘテ
ロ構造半導体レーザが得られる。
According to the present invention, a multilayer structure semiconductor wafer in which a semiconductor multilayer film including at least an active layer and a second conductivity type semiconductor clad layer is grown on a first conductivity type semiconductor substrate is mesa-etched to a depth deeper than the active layer. In a buried heterostructure semiconductor laser that is formed by forming a stripe and then growing the mesa stripe, a mesa stripe containing an active layer that recombines light is sandwiched between two grooves, and a second conductive layer is formed at the bottom of the two grooves. A first conductivity type semiconductor current blocking layer is formed except for only the upper surface of the mesa stripe, and a semiconductor layer having a smaller energy gap than the first conductivity type semiconductor current blocking layer is formed over the entire surface. As a result, a buried heterostructure semiconductor laser characterized in that buried layers of the second conductivity type are sequentially laminated is obtained.

以下実施例を示す図面を用いて本発明を説明す
る。
The present invention will be explained below using drawings showing examples.

第1図は実施例であるBH−LDの断面図であ
る。このようなBH−LDを得るには、まず
(100)n−InP基板101上にn−InPバツフア
層102、発光波長1.3μmに対応するノンドープ
In0.72Ga0.28As0.61P0.39活性層103、p−InPク
ラツド層104を順次積層した多層膜構造ウエフ
アに<011>方向に平行に2本の溝152,15
3およびそれらによつてはさまれたメサストライ
プ151を形成する。溝152,153の幅は
10μm、メサストライプ151は幅2μmとする。
次に溝のエツチングマスクとして用いたSiO2
を残したままZn拡散領域105を形成する。こ
のZn拡散領域105の形成に際しては、まずp
−InPクラツド層を選択エツチングによつて取り
去つた後、Zn拡散し、拡散した後にIn0.72Ga0.28
As0.61P0.39活性層を選択エツチングすると続く埋
め込み成長においてメルトのぬれがよく、結晶成
長の再現性がよい。このようにして得られた多層
膜構造半導体ウエフアに埋め込み成長を行ない、
n−InP電流ブロツク層106をメサストライプ
上面を除いて、続いて発光波長1.3μmに対応する
p−In0.72Ga0.28As0.61P0.39層107、p−InP埋
め込み層108、発光波長1.1μmに対応するp−
In0.85Ga0.15As0.33P0.67電極層109を積層させて
目的のBH−LDを得る。なお、この際p−In0.72
Ga0.28As0.61P0.39層107はメサストライプ15
1の上面をおおつてもかまわない。またn型であ
つてもよいが、この場合にはメサストライプ15
1の上面をおおつてしまつてはいけない。この
In1-xGaxAsyP1-y/InP BH−LDにおいてはメサ
ストライプ151をはさんでいる2本の平行な溝
152,153が10μmとやや広めの幅をもつて
いるため、溝のエツチング後の埋め込み成長に際
して電流ブロツク層がメサストライプ151をお
おつてしまうということが少なく、結晶成長の再
現性が向上した。また従来例においては2本の溝
の幅を広くすると、その部分でのp−n−p−n
構造のブレークダウン耐圧が十分高くとれないの
で、特性上のバラツキを生ずることがあつたが、
n−InP電流ブロツク層106の上にp−In0.72
Ga0.28As0.61P0.39層107を積層させることによ
り、エピタキシヤル成長層側から形成されている
p−n−pトランジスタの電流利得を小さくする
ことができるので、この部分でもブレークダウン
耐圧を十分高くすることができ、特性もよい。
FIG. 1 is a sectional view of a BH-LD according to an embodiment. To obtain such a BH-LD, first, an n-InP buffer layer 102 is formed on a (100) n-InP substrate 101, and a non-doped layer corresponding to an emission wavelength of 1.3 μm is formed on the (100) n-InP substrate 101.
In 0.72 Ga 0.28 As 0.61 P 0.39 Two grooves 152 and 15 are formed in parallel to the <011> direction in a multilayer structure wafer in which an active layer 103 and a p-InP cladding layer 104 are sequentially laminated.
3 and mesa stripes 151 sandwiched between them. The width of the grooves 152 and 153 is
The width of the mesa stripe 151 is 2 μm.
Next, a Zn diffusion region 105 is formed while leaving the SiO 2 film used as an etching mask for the trench. When forming this Zn diffusion region 105, first
- After removing the InP cladding layer by selective etching, Zn is diffused, and after the diffusion In 0.72 Ga 0.28
As 0.61 P 0.39 Selective etching of the active layer results in good melt wetting during the subsequent buried growth, and good crystal growth reproducibility. Embedded growth is performed on the multilayer structure semiconductor wafer obtained in this way,
The n-InP current blocking layer 106 is removed from the top surface of the mesa stripe, followed by the p-In 0.72 Ga 0.28 As 0.61 P 0.39 layer 107, which corresponds to the emission wavelength of 1.3 μm, and the p-InP buried layer 108, which corresponds to the emission wavelength of 1.1 μm. p-
In 0.85 Ga 0.15 As 0.33 P 0.67 electrode layer 109 is laminated to obtain the desired BH-LD. In addition, at this time p-In 0.72
Ga 0.28 As 0.61 P 0.39 Layer 107 is mesa stripe 15
It does not matter if the top surface of 1 is covered. It may also be n-type, but in this case, the mesa stripe 15
Do not cover the top of 1. this
In 1-x Ga x As y P 1-y /InP In BH-LD, the two parallel grooves 152 and 153 sandwiching the mesa stripe 151 have a slightly wider width of 10 μm, so the groove During buried growth after etching, the current blocking layer rarely covers the mesa stripe 151, and the reproducibility of crystal growth is improved. In addition, in the conventional example, when the width of the two grooves is widened, the p-n-p-n
Because the breakdown voltage of the structure was not high enough, variations in characteristics sometimes occurred.
p-In 0.72 on top of n-InP current blocking layer 106
By stacking the Ga 0.28 As 0.61 P 0.39 layer 107, the current gain of the p-n-p transistor formed from the epitaxial growth layer side can be reduced, so the breakdown voltage can be made sufficiently high in this area as well. It can be used and has good characteristics.

本発明の実施例においては、メサストライプ1
51の両側の溝部分の電流ブロツク層構造として
n−InP/p−InP/n−InP/p−In0.72Ga0.28
As0.61P0.39/p−InPという層構造を適用してい
るので、この溝部分においてもp−n−p−n電
流ブロツク構造のブレークダウン耐圧が十分高く
とれる。したがつてメサストライプ151をはさ
んでいる2本の平行な溝152,153を幅広く
とることができ、埋め込み成長において電流ブロ
ツク層がメサストライプをおおつてしまうという
ことが少なくなり、結晶成長の再現性も向上し
た。
In an embodiment of the invention, mesa stripe 1
The current blocking layer structure of the groove portions on both sides of 51 is n-InP/p-InP/n-InP/p-In 0.72 Ga 0.28
Since the layer structure As 0.61 P 0.39 /p-InP is applied, the breakdown voltage of the p-n-p-n current blocking structure can be maintained sufficiently high even in this groove portion. Therefore, the two parallel grooves 152 and 153 sandwiching the mesa stripe 151 can be made wider, which reduces the possibility that the current blocking layer covers the mesa stripe during buried growth, making it easier to reproduce crystal growth. Sexuality also improved.

なお実施例においてはIn1-xGaxAsyP1-yを活性
層とし、InP基板を用いた1μm波長帯のBH−LD
を示したが、この材料系に限ることなく、他の半
導体材料にも適用可能である。また半導体層の導
電型もpとnとをすべてとりかえたものでも差し
つかえない。
In the example, a BH-LD in the 1 μm wavelength band using an InP substrate with In 1-x Ga x As y P 1-y as the active layer was used.
However, the present invention is not limited to this material system, and can be applied to other semiconductor materials. Furthermore, the conductivity type of the semiconductor layer may be such that all p and n conductivity types are changed.

本発明の特徴は発光再結合する活性層を含むメ
サストライプの両側の溝の電流ブロツク層構造に
いて、第1導電型電流ブロツク層と、第2導電型
埋め込み層の間に、それらよりもエネルギーギヤ
ツプの小さな半導体層を積層させたことである。
これによつて溝の部分の電流ブロツク層構造のブ
レークダウン耐圧も十分高くとれるので、溝の幅
を広くすることができ、したがつて埋め込み成長
の際、電流ブロツク層がメサストライプをおおつ
てしまうことが少なくなり、結晶成長の再現性も
向上した。
The feature of the present invention lies in the current blocking layer structure of the grooves on both sides of the mesa stripe containing the active layer that emits and recombines. This is because semiconductor layers with small gaps are stacked.
This allows the breakdown voltage of the current blocking layer structure in the trench to be sufficiently high, making it possible to widen the trench, thereby preventing the current blocking layer from covering the mesa stripe during buried growth. This also improved the reproducibility of crystal growth.

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

第1図は実施例であるIn1-xGaxAsyP1-y/InP
BH−LDの断面図である。 図中101……n−InP基板、102……n−
InPバツフア層、103……In0.72Ga0.28As0.61
P0.39活性層、104……p−InPクラツド層、1
05……Zn拡散領域、106……n−InP電流ブ
ロツク層、107……p−In0.72Ga0.28As0.61P0.39
層、108……p−InP埋め込み層、109……
p−In0.85Ga0.15As0.33P0.67電極層、110……p
形オーミツク性電極、111……n形オーミツク
性電極である。
Figure 1 shows an example of In 1-x Ga x As y P 1-y /InP
It is a sectional view of BH-LD. In the figure, 101... n-InP substrate, 102... n-
InP buffer layer, 103...In 0.72 Ga 0.28 As 0.61
P 0.39 active layer, 104...p-InP clad layer, 1
05...Zn diffusion region, 106...n-InP current blocking layer, 107...p-In 0.72 Ga 0.28 As 0.61 P 0.39
Layer, 108... p-InP buried layer, 109...
p-In 0.85 Ga 0.15 As 0.33 P 0.67 Electrode layer, 110...p
111 is an n-type ohmic electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 第1導電型半導体基板上に少くとも活性層、
第2導電型半導体クラツド層を含む半導体多層膜
を成長させた多層膜構造半導体ウエフアを、前記
活性層よりも深くメサエツチングしてメサストラ
イプを形成した後埋め込み成長してなる埋め込み
ヘテロ構造半導体レーザにおいて、発光再結合す
る前記活性層を含む前記メサストライプが2つの
溝によつてはさまれてなり、前記2つの溝の底面
部に第2導電型半導体領域が形成され、前記メサ
ストライプの上面のみを除いて第1導電型半導体
電流ブロツク層が形成され、さらに前記第1導電
型半導体電流ブロツク層よりもエネルギーギヤツ
プの小さな半導体層、全面にわたつて第2導電型
埋め込み層が順次積層されてなることを特徴とす
る埋め込みヘテロ構造半導体レーザ。
1 At least an active layer on the first conductivity type semiconductor substrate,
In a buried heterostructure semiconductor laser, a multilayer structure semiconductor wafer on which a semiconductor multilayer film including a semiconductor cladding layer of a second conductivity type is grown is mesa-etched deeper than the active layer to form a mesa stripe, and then buried and grown. The mesa stripe including the active layer that undergoes luminescent recombination is sandwiched between two grooves, and a second conductivity type semiconductor region is formed at the bottom of the two grooves, and only the upper surface of the mesa stripe is sandwiched between two grooves. A semiconductor current blocking layer of a first conductive type is formed except for the semiconductor current blocking layer of the first conductive type, and a buried layer of a second conductive type is sequentially laminated over the entire surface of the semiconductor layer having a smaller energy gap than the semiconductor current blocking layer of the first conductive type. A buried heterostructure semiconductor laser characterized by:
JP72282A 1982-01-06 1982-01-06 Buried hetero structural semiconductor laser Granted JPS58118184A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP72282A JPS58118184A (en) 1982-01-06 1982-01-06 Buried hetero structural semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP72282A JPS58118184A (en) 1982-01-06 1982-01-06 Buried hetero structural semiconductor laser

Publications (2)

Publication Number Publication Date
JPS58118184A JPS58118184A (en) 1983-07-14
JPS641072B2 true JPS641072B2 (en) 1989-01-10

Family

ID=11481634

Family Applications (1)

Application Number Title Priority Date Filing Date
JP72282A Granted JPS58118184A (en) 1982-01-06 1982-01-06 Buried hetero structural semiconductor laser

Country Status (1)

Country Link
JP (1) JPS58118184A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60223183A (en) * 1984-04-19 1985-11-07 Matsushita Electric Ind Co Ltd Manufacture of semiconductor laser device
FR2587852B1 (en) * 1985-09-24 1989-04-07 Chaminant Guy METHOD FOR PRODUCING A LASER WITH A SEMICONDUCTOR WITH A TUBE BURIED WITH OR WITHOUT A DIFFRACTION NETWORK AND LASER OBTAINED BY THIS PROCESS
JP2815049B2 (en) * 1989-05-30 1998-10-27 株式会社前田鉄工所 Steam boiler with juxtaposed soot blower

Also Published As

Publication number Publication date
JPS58118184A (en) 1983-07-14

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