JPH046113B2 - - Google Patents

Info

Publication number
JPH046113B2
JPH046113B2 JP58040342A JP4034283A JPH046113B2 JP H046113 B2 JPH046113 B2 JP H046113B2 JP 58040342 A JP58040342 A JP 58040342A JP 4034283 A JP4034283 A JP 4034283A JP H046113 B2 JPH046113 B2 JP H046113B2
Authority
JP
Japan
Prior art keywords
layer
stripe
semiconductor laser
oscillation
groove
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
Application number
JP58040342A
Other languages
Japanese (ja)
Other versions
JPS59165487A (en
Inventor
Saburo Yamamoto
Hiroshi Hayashi
Shinji Kaneiwa
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.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP4034283A priority Critical patent/JPS59165487A/en
Publication of JPS59165487A publication Critical patent/JPS59165487A/en
Publication of JPH046113B2 publication Critical patent/JPH046113B2/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
    • H01S5/40Arrangement of two or more semiconductor lasers, not provided for in groups H01S5/02 - H01S5/30
    • H01S5/4025Array arrangements, e.g. constituted by discrete laser diodes or laser bar
    • H01S5/4031Edge-emitting structures
    • 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
    • H01S5/223Buried stripe structure
    • H01S5/2232Buried stripe structure with inner confining structure between the active layer and the lower electrode
    • 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
    • H01S5/40Arrangement of two or more semiconductor lasers, not provided for in groups H01S5/02 - H01S5/30
    • H01S5/4025Array arrangements, e.g. constituted by discrete laser diodes or laser bar
    • H01S5/4087Array arrangements, e.g. constituted by discrete laser diodes or laser bar emitting more than one wavelength

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)
  • Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)

Description

【発明の詳細な説明】 〈技術分野〉 本発明は異なつた波長で発振する複数の半導体
レーザ動作部を同一素子内に配列形成した半導体
レーザアレイ素子の製造方法に関するものであ
る。
DETAILED DESCRIPTION OF THE INVENTION <Technical Field> The present invention relates to a method of manufacturing a semiconductor laser array element in which a plurality of semiconductor laser operating parts emitting oscillations at different wavelengths are arranged in the same element.

〈従来技術〉 複数のレーザ発振動作部を同一基板上に形成し
た半導体レーザアレイ素子についてはすでに知ら
れているが、これは同一波長でレーザ発振する動
作部を具設したものである。一方、半導体レーザ
素子を例えば光フアイバー通信の光源として使用
する場合には、発振波長の異なる複数のレーザ光
を1本のフアイバーに結合させて伝送すればその
情報量を波長の数に比例して多く設定することが
でき大容量の光通信が可能となる。これは一般に
波長多重通信と称されているものであり、光フア
イバー通信の重要な開発課題である。複数の波長
のレーザ光を1本のフアイバーに結合させるため
には波長の異なる複数の半導体レーザ素子をフア
イバーの片端に配置して光結合させることが必要
であり、位置精度等に困難な制御性を要求され
る。半導体レーザ素子単体で波長の異なるレーザ
光を出力できるようにすれば、この点での問題は
大幅に緩和される。
<Prior Art> Semiconductor laser array elements in which a plurality of laser oscillation operating units are formed on the same substrate are already known, and this device is provided with operating units that oscillate lasers at the same wavelength. On the other hand, when using a semiconductor laser element as a light source for optical fiber communication, for example, if multiple laser beams with different oscillation wavelengths are coupled to a single fiber and transmitted, the amount of information will be increased in proportion to the number of wavelengths. Many settings can be made, enabling large-capacity optical communication. This is generally referred to as wavelength division multiplexing communication, and is an important development issue for optical fiber communication. In order to couple laser beams of multiple wavelengths into one fiber, it is necessary to place multiple semiconductor laser elements with different wavelengths at one end of the fiber and optically couple them, which makes controllability difficult due to positional accuracy etc. is required. If a single semiconductor laser element could output laser beams with different wavelengths, this problem would be greatly alleviated.

このような要求に対応したものとして、例えば
特開昭57−139983に示されるようにストライプ状
凸部の幅に応じた禁制帯幅の活性層を得ることに
より多波長を得るようにした半導体レーザアレー
が提案されている。
In order to meet these demands, for example, a semiconductor laser array has been proposed in which multiple wavelengths can be obtained by obtaining an active layer with a forbidden band width corresponding to the width of a striped convex portion, as shown in Japanese Patent Laid-Open No. 57-139983. is proposed.

しかし、この従来提案されているレーザアレー
構造を実際に製造するに際して、混晶組成の融液
の過冷却度を制御して作製する必要であり、また
各クラツド層の混晶比が異なつたものとなりダブ
ルヘテロ接合レーザの特性を充分に発揮すること
が困難であつた。
However, when actually manufacturing this conventionally proposed laser array structure, it is necessary to control the degree of supercooling of the melt with a mixed crystal composition, and the mixed crystal ratio of each cladding layer is different. It has been difficult to fully utilize the characteristics of double heterojunction lasers.

〈発明の目的〉 基板上に三元又は四元系の混晶半導体を液相エ
ピタキシヤル成長させた場合、その成長速度によ
つて成長層の組成比が変化し、結果的にエネルギ
ーバンドギヤツプが異なることが見い出された。
(Appliep Physics Letters42〔5〕P.406)即ち、
異なる成長速度によつて作製された活性層を有す
る半導体レーザ素子はそれぞれ異なる発振波長を
有することになる。本発明はこの点を利用し、比
較的簡単な構造で素子単体に発振波長の異なる複
数のレーザ発振動作部を具設した新規有用な半導
体レーザアレイ素子の製造方法を提供することを
目的とするものである。
<Purpose of the invention> When a ternary or quaternary mixed crystal semiconductor is liquid-phase epitaxially grown on a substrate, the composition ratio of the growth layer changes depending on the growth rate, resulting in an energy band gear. It was found that the two types were different.
(Appliep Letter Physics 42 [5] P.406) That is,
Semiconductor laser devices having active layers manufactured with different growth rates will have different oscillation wavelengths. Taking advantage of this point, the present invention aims to provide a method for manufacturing a new and useful semiconductor laser array element, which has a relatively simple structure and has a plurality of laser oscillation operating parts with different oscillation wavelengths in a single element. It is something.

本発明の他の目的は波長多重通信に最適のレー
ザ光源の製造方法を提供することである。
Another object of the present invention is to provide a method of manufacturing a laser light source that is optimal for wavelength division multiplexing communications.

〈実施例〉 第1図は本発明の1実施例により製造された半
導体レーザアレイ素子の構成斜視図である。本実
施例はp型基板上にn型の電流阻止層を堆積して
V字溝をエツチング加工した内部ストライプ構造
半導体レーザ素子(Appl.Phys.Lett.vol.40,
1March1982,P.312)を基本とする。
<Example> FIG. 1 is a perspective view of the structure of a semiconductor laser array device manufactured according to an example of the present invention. This example is a semiconductor laser device with an internal stripe structure (Appl.Phys.Lett.vol.40,
1March1982, P.312).

P型GaAs基板1上に0.6μmの厚さのn−GaAs
電流阻止層2を液相エピタキシヤル成長した後、
幅w1,w2(w1>w2)を有するストライプ溝3,
4を周知のホトリソグラフイ技術により形成す
る。ストライプ溝3,4の内方は電流阻止層2が
除去され、この部分が電流通路となる。再度液相
エピタキシヤル成長法でp−Ga1-yAlyAsクラツ
ド層5、Ga1-xAlxAs活性層6(0<x<y<
1)、n−Ga1-yAlyAsクラツド層7、n−GaAs
キヤツプ層8を順次積層することによりダブルヘ
テロ接合型のレーザ動作用多層結晶層が形成され
る。次に基板1の裏面をラツピングしてウエハー
の厚さを約120μmとした後、Au−Znのp側電極
9を形成し、一方、キヤツプ層8の上面にはAu
−Ge−Niのn側電極10を形成する。ストライ
プ溝3,4単位でレーザ動作用多層結晶を分割す
るため、n側電極10表面より分離溝11をスト
ライプ溝3,4と平行に核設し、その深さが
GaAs基板1に達する迄この多層結晶をエツチン
グ加工する。以上により、第1図に示す如くスト
ライプ幅の異なるストライプ溝3,4の直上に対
応する活性層6の領域でそれぞれレーザ発振動作
部が形成された半導体レーザアレイ素子が得られ
る。ストライプ幅がw1のストライプ溝3直上の
活性層6は下方に湾曲された厚い動作部となり、
これに対してストライプ幅がw2のストライプ溝
4直上の活性層6は平坦な動作部を構成してい
る。即ち、ストライプ幅がw1>w2であることよ
り、ストライプ溝3,4の上に成長されるクラツ
ド層5は上面が幅w1の部分は凹状となり幅w2
部分は平坦化される。従つてクラツド層5上に堆
積される活性層6はストライプ幅w1の部分が他
より成長速度の速いエピタキシヤル成長層で下方
に湾曲した層の厚い動作部を構成することとな
り、一方ストライプ幅w2の部分はこれより成長
速度の遅いエピタキシヤル成長層で平坦な動作部
を構成することとなる。前述した如く、同一成長
融液よりエピタキシヤル成長させた場合、成長速
度によつて得られる成長層の組成比が異なる。従
つて、湾曲されたレーザ発振動作部と平坦なレー
ザ発振動作部では、Ga1-xAlxAsの混晶化の相違
に基くエネルギーバンドギヤツプの差に起因して
異なる発振波長のレーザ光が出力されることとな
る。
0.6μm thick n-GaAs on P-type GaAs substrate 1
After growing the current blocking layer 2 by liquid phase epitaxial growth,
a striped groove 3 having widths w 1 , w 2 (w 1 >w 2 );
4 is formed by a well-known photolithography technique. The current blocking layer 2 is removed inside the striped grooves 3 and 4, and this portion becomes a current path. A p-Ga 1-y AlyAs cladding layer 5, a Ga 1-x AlxAs active layer 6 (0<x<y<
1), n-Ga 1-y AlyAs cladding layer 7, n-GaAs
By sequentially stacking the cap layers 8, a double heterojunction type multilayer crystal layer for laser operation is formed. Next, after lapping the back surface of the substrate 1 to make the wafer thickness approximately 120 μm, a p-side electrode 9 of Au-Zn is formed, while an Au-Zn p-side electrode 9 is formed on the upper surface of the cap layer 8.
- Form an n-side electrode 10 of Ge-Ni. In order to divide the multilayer crystal for laser operation into units of stripe grooves 3 and 4, separation grooves 11 are formed from the surface of the n-side electrode 10 in parallel to the stripe grooves 3 and 4, and the depth thereof is
This multilayer crystal is etched until the GaAs substrate 1 is reached. Through the above steps, a semiconductor laser array element is obtained in which laser oscillation operating portions are formed in regions of the active layer 6 directly above the stripe grooves 3 and 4 having different stripe widths, as shown in FIG. The active layer 6 directly above the stripe groove 3 with a stripe width of w 1 becomes a thick active part that is curved downward.
On the other hand, the active layer 6 directly above the stripe groove 4 having a stripe width of w 2 constitutes a flat operating section. That is, since the stripe width is w 1 > w 2 , the upper surface of the cladding layer 5 grown on the stripe grooves 3 and 4 is concave in the width w 1 portion and flattened in the width w 2 portion. . Therefore, in the active layer 6 deposited on the cladding layer 5, the part of the stripe width w1 is an epitaxially grown layer whose growth rate is faster than the other part, and constitutes a thick active part of the layer curved downward. The portion w 2 is an epitaxially grown layer whose growth rate is slower than this and constitutes a flat operating section. As described above, when epitaxial growth is performed from the same growth melt, the composition ratio of the resulting grown layer differs depending on the growth rate. Therefore, in the curved laser oscillation area and the flat laser oscillation area, laser beams with different oscillation wavelengths are emitted due to the difference in energy band gap based on the difference in the mixed crystallization of Ga 1-x AlxAs. It will be output.

ストライプ幅w1=8μm、w2=4μm、ストライ
プ溝3,4相互の間隔を20μmとし、活性層6の
Al混晶比x=0.08、クラツド層5,7のAl混晶
比y=0.3に設定すると、ストライプ溝3直上の
活性層6は湾曲し、他の部分は平坦化された活性
層6が得られる。また活性層6の厚さは湾曲部で
最大0.2μm、平坦部で0.06μmとなるようにエピタ
キシヤル成長条件を設定する。これによつて活性
層6のストライプ溝3,4直上領域に対応する湾
曲した発振動作部では830nm、平坦な発振動作部
では810nmの波長を有するレーザ出力光が得られ
る。尚、発振閾値電流は湾曲した発振動作部で
25mA、平坦な発振動作部で35mAであつた。
The stripe width w 1 = 8 μm, w 2 = 4 μm, the distance between the stripe grooves 3 and 4 is 20 μm, and the active layer 6 is
When the Al mixed crystal ratio x = 0.08 and the Al mixed crystal ratio y of the cladding layers 5 and 7 are set to 0.3, the active layer 6 directly above the stripe groove 3 is curved, and the other parts are flattened. It will be done. Further, the epitaxial growth conditions are set so that the thickness of the active layer 6 is at most 0.2 μm in the curved portion and 0.06 μm in the flat portion. As a result, laser output light having a wavelength of 830 nm is obtained in the curved oscillation active portion corresponding to the area directly above the striped grooves 3 and 4 of the active layer 6, and 810 nm in the flat oscillation active portion. Note that the oscillation threshold current is determined by the curved oscillation operating part.
It was 25mA, and 35mA in the flat oscillation area.

次に、ストライプ幅w1=6μm、w2=3μm、ス
トライプ溝3,4相互の間隔を20μmとし、活性
層6のAl混晶比x=0.15、クラツド層5,7の
Al混晶比y=0.5に設定する。また活性層6は湾
曲部で0.15μm、平坦部で0.04μmとする。これに
よつて湾曲した発振動作部では785nmの波長を有
するレーザ出力光が得られる。この場合の発振閾
値電流は湾曲した発振動作部で30mA、平坦な発
振動作部で45mAであつた。
Next, the stripe width w 1 = 6 μm, w 2 = 3 μm, the interval between the stripe grooves 3 and 4 is 20 μm, the Al mixed crystal ratio of the active layer 6 is x = 0.15, and the cladding layers 5 and 7 are
Set Al mixed crystal ratio y=0.5. The active layer 6 has a thickness of 0.15 μm at the curved portion and 0.04 μm at the flat portion. As a result, a laser output light having a wavelength of 785 nm can be obtained in the curved oscillation operating section. In this case, the oscillation threshold current was 30 mA in the curved oscillation area and 45 mA in the flat oscillation area.

第2図は本発明の他の実施例により製造された
半導体レーザアレイ素子の構成斜視図である。本
実施例は幅の異なる3種類のストライプ溝を刻設
し、それぞれの溝上に成長速度が相異する3つの
レーザ発振動作部を形成したものである。図中第
1図と同一符号は同一内容を示す。
FIG. 2 is a perspective view of a semiconductor laser array device manufactured according to another embodiment of the present invention. In this embodiment, three types of stripe grooves having different widths are carved, and three laser oscillation operating parts having different growth rates are formed on each groove. In the figure, the same reference numerals as in FIG. 1 indicate the same contents.

P型GaAs基板1上にn−GaAs電流阻止層2
が液相エピタキシヤル成長され、幅w1,w2,w3
(w1>w2>w3)を有する3本のストライプ溝1
2,13,14が形成されている。この上に第1
図同様レーザ動作用多層結晶が積層されかつスト
ライプ溝間の中央で分離溝11,11′によりス
トライプ溝12,13,14毎に3分割されてい
る。活性層6は各ストライプ幅w1で大きく湾曲
し、ストライプ幅w2で小さく湾曲し、ストライ
プ幅w3では平坦化されている。従つて、この半
導体レーザアレイ素子では3つのレーザ発振動作
部からそれぞれ波長の異なる3本のレーザ出力光
が得られる。
N-GaAs current blocking layer 2 on P-type GaAs substrate 1
are grown by liquid phase epitaxial growth, with widths w 1 , w 2 , w 3
Three stripe grooves 1 with (w 1 > w 2 > w 3 )
2, 13, and 14 are formed. On top of this the first
As shown in the figure, multilayer crystals for laser operation are stacked and divided into three stripe grooves 12, 13, and 14 by separation grooves 11 and 11' at the center between the stripe grooves. The active layer 6 is largely curved at each stripe width w1 , slightly curved at each stripe width w2 , and flattened at each stripe width w3 . Therefore, in this semiconductor laser array element, three laser output lights having different wavelengths are obtained from the three laser oscillation operating parts.

上記実施例はGaAlAs系半導体レーザアレイ素
子について説明したが、本発明はこれに限定され
るものではなく、GaAsP,GaInP,InGaAsPそ
の他の三元系又は四元系化合物半導体を用いるこ
ともできる。また、レーザ発振動作部は4個以上
形成することも可能であり、発振波長差は5〜
40nm程度に適宜設定することができる。
Although the above embodiment describes a GaAlAs-based semiconductor laser array element, the present invention is not limited thereto, and ternary or quaternary compound semiconductors such as GaAsP, GaInP, InGaAsP, and others may also be used. It is also possible to form four or more laser oscillation operating parts, and the difference in oscillation wavelength is 5 to 5.
It can be set appropriately to about 40 nm.

〈発明の効果〉 以上詳説した如く、本発明によれば素子単体に
発振波長の異なる複数個のレーザ発振動作部が形
成された半導体レーザアレイ素子を得ることがで
きる。またその構造はストライプ幅の差を利用し
て成長速度の異なる活性層領域を形成するもので
あり、比較的簡単な構造で波長多重通信に最適の
レーザ光源が確立される。
<Effects of the Invention> As described in detail above, according to the present invention, it is possible to obtain a semiconductor laser array element in which a plurality of laser oscillation operating parts having different oscillation wavelengths are formed in a single element. In addition, the structure utilizes the difference in stripe width to form active layer regions with different growth rates, and a laser light source optimal for wavelength division multiplexing communication is established with a relatively simple structure.

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

第1図は本発明の1実施例により製造された半
導体レーザアレイ素子の構成斜視図である。第2
図は本発明の他の実施例により製造された半導体
レーザアレイ素子の構成斜視図である。 1……基板、2……電流阻止層、3,4,1
2,13,14……ストライプ溝、5……P型ク
ラツド層、6……活性層、7……n型クラツド
層、8……キヤツプ層、9……P側電極、10…
…n側電極、11,11′……分離溝。
FIG. 1 is a perspective view of a semiconductor laser array device manufactured according to an embodiment of the present invention. Second
The figure is a perspective view of a semiconductor laser array device manufactured according to another embodiment of the present invention. 1...Substrate, 2...Current blocking layer, 3, 4, 1
2, 13, 14... Stripe groove, 5... P-type cladding layer, 6... Active layer, 7... N-type cladding layer, 8... Cap layer, 9... P-side electrode, 10...
...N-side electrode, 11, 11'...separation groove.

Claims (1)

【特許請求の範囲】 1 GaAs基板上に逆導電型のGaAs電流阻止層
をエピタキシヤル成長する工程と、 少なくとも幅w1,w2(w1>w2)を有するスト
ライプ溝を形成して、上記電流阻止層の一部をス
トライプ状に除去する工程と、 Ga1-yAlyAsクラツド層、Ga1-xAlxAs活性層
(0<x<y<1)、Ga1-yAlyAsクラツド層及び
GaAsキヤツプ層を順次液相エピタキシヤル成長
法により積層形成する工程と、 前記ストライプ溝単位で該ストライプ溝に略平
行に分離溝を上記GaAs基板に達するまで形成す
る工程 とを含み 上記各ストライプ溝上にそれぞれAl混晶比の
異なる活性層を形成してなることを特徴とする半
導体レーザアレイ素子の製造方法。
[Claims] 1. A step of epitaxially growing a GaAs current blocking layer of the opposite conductivity type on a GaAs substrate, and forming a striped groove having at least widths w 1 and w 2 (w 1 >w 2 ), A step of removing a part of the current blocking layer in a stripe shape, a Ga 1-y Al y As cladding layer, a Ga 1-x Al x As active layer (0<x<y<1), a Ga 1-y Al y As cladding layer, a Ga 1-y Al y As clad layer, a Ga 1-y Al y As clad layer and
A step of sequentially forming a GaAs cap layer by a liquid phase epitaxial growth method, and a step of forming a separation groove in each stripe groove in a manner substantially parallel to the stripe groove until reaching the GaAs substrate. A method for manufacturing a semiconductor laser array element, comprising forming active layers each having a different Al mixed crystal ratio.
JP4034283A 1983-03-09 1983-03-09 Semiconductor laser array element Granted JPS59165487A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4034283A JPS59165487A (en) 1983-03-09 1983-03-09 Semiconductor laser array element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4034283A JPS59165487A (en) 1983-03-09 1983-03-09 Semiconductor laser array element

Publications (2)

Publication Number Publication Date
JPS59165487A JPS59165487A (en) 1984-09-18
JPH046113B2 true JPH046113B2 (en) 1992-02-04

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JP4034283A Granted JPS59165487A (en) 1983-03-09 1983-03-09 Semiconductor laser array element

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Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61287289A (en) * 1985-06-14 1986-12-17 Sharp Corp Semiconductor laser device for light memory
IT1237120B (en) * 1989-11-03 1993-05-18 Lonati Srl PROCEDURE FOR THE IMPLEMENTATION OF DRAWINGS ON SOCKS WITH CIRCULAR DOUBLE CYLINDER MACHINES AND DEVICE FOR ITS IMPLEMENTATION
CA2091302A1 (en) * 1992-03-11 1993-09-12 Ichiro Yoshida Semiconductor laser and process for fabricating the same

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57139983A (en) * 1981-02-24 1982-08-30 Nec Corp Buried double heterojunction laser element

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JPS59165487A (en) 1984-09-18

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