JPH0243788A - Multi-wavelength integrated semiconductor laser device and its manufacturing method - Google Patents

Multi-wavelength integrated semiconductor laser device and its manufacturing method

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Publication number
JPH0243788A
JPH0243788A JP19338088A JP19338088A JPH0243788A JP H0243788 A JPH0243788 A JP H0243788A JP 19338088 A JP19338088 A JP 19338088A JP 19338088 A JP19338088 A JP 19338088A JP H0243788 A JPH0243788 A JP H0243788A
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JP
Japan
Prior art keywords
active layers
active layer
layers
layer
manufacturing
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
Application number
JP19338088A
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Japanese (ja)
Inventor
Yoshinobu Sekiguchi
芳信 関口
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.)
Canon Inc
Original Assignee
Canon Inc
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Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP19338088A priority Critical patent/JPH0243788A/en
Publication of JPH0243788A publication Critical patent/JPH0243788A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a laser device whose active layers are uniform in the laser characteristic and which is long in a life span without imposing any restriction on the material and the composition of the active layers by a method wherein two or more kinds of active layers, which oscillate light rays different from each other, are laminated, and impurity is diffused to the place near the active layers. CONSTITUTION:Two or more kinds of active layers 41-43, which oscillate light rays whose wavelengths are different from each other, are laminated, and then impurity is diffused so as to reach to the active layers 41-43 or the position near them for the formation of carrier injection regions 103, 203 and 303 to enable the layers 41-43 to be driven independently from each other. For instance, an n-type GaAs buffer layer 6 and an n-type first clad layer 5 are formed on an n-type GaAs substrate 7, and n<->-type barrier layers 34, 33, 32 and 31 and the n<->-type or undoped active layers 43, 42 and 41 whose oscillating light rays are different from each other in wavelength, are alternately formed in succession thereon. Next, Be is injected in stripes to form the p<+> regions 303, 202 and 103 corresponding to the active layers 43, 42 and 41 respectively. Then, a high resistance second clad layer 2 and a high resistance cap layer 1 are formed, and Zn is diffused in stripes to form the p<+> regions 302, 202 and 102.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、異なる波長の光を発振する複数種の活性層を
有し、各活性層が独立駆動可能な多波長集積半導体レー
ザ装置およびその製造方法に関する。
Detailed Description of the Invention [Field of Industrial Application] The present invention relates to a multi-wavelength integrated semiconductor laser device that has a plurality of types of active layers that oscillate light of different wavelengths, and each active layer can be driven independently, and its Regarding the manufacturing method.

〔従来の技術] 従来より、多波長集積半導体レーザ装置は例えば光通信
などに利用されており、その製造方法としては、例えば
下記■および■などの方法が知られている。
[Prior Art] Conventionally, multi-wavelength integrated semiconductor laser devices have been used, for example, in optical communications, and methods such as the following (1) and (2) are known as methods for manufacturing the same.

■、下地層の表面形状に応じて異なる組成の層が形成で
きる三元以上の化合物を用いて、異なる組成の活性層を
所望の位置に形成する製造方法(特開昭59−1654
87号公報など)。第4図は、このような製造方法によ
り得られるレーザ装置を示す模式的断面図であり、基板
401の上の所定位置に組成の異なる各活性層60a、
 60bが形成され、それら活性層を独立駆動するため
の各電極70a、70bが形成されている。
(1) A manufacturing method for forming active layers with different compositions at desired positions using ternary or higher compounds that can form layers with different compositions depending on the surface shape of the base layer (Japanese Patent Laid-Open No. 59-1654
Publication No. 87, etc.). FIG. 4 is a schematic cross-sectional view showing a laser device obtained by such a manufacturing method, in which active layers 60a having different compositions are placed at predetermined positions on a substrate 401,
60b is formed, and electrodes 70a and 70b for independently driving these active layers are formed.

■、1回目の成膜を行ない、その後活性層に達する所望
のエツチングを行ない、その後2回目の成膜を行なうこ
とにより製造する方法(特開昭57−152183号公
報など)。第5図は、このような製造方法により得られ
るレーザ装置を示す模式的断面図であり、基板401の
上の所定位置にリッジ型等形状の発振波長の異なる各活
性1層80a、 80b、 80cが形成され、それら
活性層を独立駆動するための各電極90a、 90b、
 90cが形成されている。
(2) A manufacturing method in which a first film is formed, then a desired etching is performed to reach the active layer, and then a second film is formed (Japanese Unexamined Patent Publication No. 152183/1983, etc.). FIG. 5 is a schematic cross-sectional view showing a laser device obtained by such a manufacturing method, in which active single layers 80a, 80b, and 80c each having a ridge-like shape and having different oscillation wavelengths are formed at predetermined positions on a substrate 401. are formed, and each electrode 90a, 90b is used to independently drive the active layer.
90c is formed.

[発明が解決しようとする課題] 前記製造方法■においては、活性層の形成に下地形状依
存性を有する化合物しか用いることができず、活性層の
材料および組成に制限があり、波長の制御に限界が有る
。更には、下地層の形状が各活性層によって異なるので
、各活性層の断面形状も当然具なり、それ故に非点収差
、しきい値電流などのレーザ特性が各活性層によって異
なるという欠点が有る。
[Problems to be Solved by the Invention] In the above manufacturing method (1), only a compound that is dependent on the shape of the base can be used to form the active layer, there are restrictions on the material and composition of the active layer, and it is difficult to control the wavelength. There are limits. Furthermore, since the shape of the underlying layer differs depending on each active layer, the cross-sectional shape of each active layer also naturally changes, and therefore there is a drawback that laser characteristics such as astigmatism and threshold current differ depending on each active layer. .

前記製造方法■においては、活性層に達するエツチング
が必須の工程なので活性層が直接大気やエツチング液に
接触し、活性層の酸化や加工ダメージが生じることがあ
り、またその後2回目の成膜に伴う欠陥の導入が生じる
ことあり、それ故にレーザ特性が各活性層によって異な
る場合があり、またレーザの寿命が短くなる場合がある
In the above manufacturing method (2), since etching to reach the active layer is an essential step, the active layer may come into direct contact with the atmosphere or the etching solution, which may cause oxidation or processing damage to the active layer. The introduction of concomitant defects may occur and therefore the laser properties may differ from each active layer and the lifetime of the laser may be shortened.

本発明は、これらの課題を解決するためになされたもの
であり、その目的は、活性層の材料および組成に特別な
制限がなく、各活性層レーザ特性が均一であり、レーザ
の寿命が短くならないような多波長集積半導体レーザの
製造方法を提供することにある。
The present invention has been made to solve these problems, and its purpose is to have no special restrictions on the material and composition of the active layer, to make the laser characteristics of each active layer uniform, and to shorten the laser life. It is an object of the present invention to provide a method for manufacturing a multi-wavelength integrated semiconductor laser that does not require the following steps.

[課題を解決するための手段] 本発明は、 (イ)異なる波長の光を発振する複数種の活性層を積層
する過程と、 (ロ)該複数種の活性層に達する位置または近傍の位置
まで不純物を拡散することにより、該活性層を独立駆動
するためのキャリア注入領域を形成する過程とを含むこ
とを特徴とする多波長集積半導体レーザ装置の製造方法
およびその方法により製造された多波長集積半導体レー
ザ装置である。
[Means for Solving the Problems] The present invention includes (a) a process of laminating a plurality of types of active layers that oscillate light of different wavelengths, and (b) a position at or near a position reaching the plurality of types of active layers. A method for manufacturing a multi-wavelength integrated semiconductor laser device, comprising the step of forming a carrier injection region for independently driving the active layer by diffusing impurities up to It is an integrated semiconductor laser device.

本発明の方法においては、不純物の拡散によってキャリ
ア注入領域を形成するので、例えば第2図に示すように
各活性層を適当な層を介して積層状に形成したプレーナ
ー状態で独立駆動可能である。したがって、第4図に示
したような活性層の組成を同一層内で部分的に変化させ
る必要がなく、第5図に示したようなリッジ型にエツチ
ングする必要もない。それ故に、活性層の材料および組
成に特別な制限がなく、各活性層レーザ特性が均一であ
り、レーザの寿命劣化が生じにくい。
In the method of the present invention, since the carrier injection region is formed by diffusion of impurities, each active layer can be independently driven in a planar state formed in a stacked manner with appropriate layers interposed therebetween, as shown in FIG. 2, for example. . Therefore, there is no need to partially change the composition of the active layer within the same layer as shown in FIG. 4, and there is no need to etch the active layer into a ridge shape as shown in FIG. Therefore, there are no special restrictions on the material and composition of the active layer, the laser characteristics of each active layer are uniform, and the life of the laser is less likely to deteriorate.

以下、本発明の製造方法を、工程に沿って詳細に説明す
る。
Hereinafter, the manufacturing method of the present invention will be explained in detail along the steps.

(イ)まず、異なる波長の光を発振する複数種の活性層
を積層状に形成する。
(a) First, multiple types of active layers that oscillate light of different wavelengths are formed in a stacked manner.

例えば、活性層形成の際の材料、組成、層厚などを適当
に制御することにより、異なる波長の光を発振する複数
種の活性層を形成することができる。その材料、組成、
層厚なとは、所望とする発振波長に応じて適宜決定すれ
ばよく、本発明においては特に限定されるものではない
For example, by appropriately controlling the material, composition, layer thickness, etc. when forming the active layer, it is possible to form a plurality of types of active layers that emit light of different wavelengths. its materials, composition,
The layer thickness may be appropriately determined depending on the desired oscillation wavelength, and is not particularly limited in the present invention.

その複数種の活性層は、例えば第2図などに示すように
適当な層(障壁層等)を介して積層状に形成するとよい
。本発明においては、この積層状に形成した活性層はそ
のまま独立駆動可能となるので、前述の第5図に示した
ような活性層のエツチングに起因する問題は生じない。
The plurality of active layers may be formed in a laminated manner with appropriate layers (barrier layers, etc.) interposed therebetween, as shown in FIG. 2, for example. In the present invention, the laminated active layer can be driven independently as it is, so that the problem caused by the etching of the active layer as shown in FIG. 5 described above does not occur.

また、本発明においては、各活性層を各々積層状に形成
するので、前述の第4図に示したような下地形状による
組成の制御をする必要は特になく、それ故に活性層の材
料および組成に制限がなく、各活性層の断面を均一にで
きる。
Furthermore, in the present invention, since each active layer is formed in a laminated manner, there is no particular need to control the composition by the underlying shape as shown in FIG. There is no limit to the cross section of each active layer, and the cross section of each active layer can be made uniform.

(ロ)次いで、その複数種の活性層に達する位置または
近傍の位置まで不純物を拡散することにより、該活性層
を独立駆動するためのキャリア注入領域を形成する。
(b) Next, by diffusing impurities to a position reaching or near the plurality of types of active layers, a carrier injection region for independently driving the active layers is formed.

不純物の種類は、各活性層にキャリアの注入を行なうこ
とのできる領域を形成可能な不純物であれば特に限定さ
れず、被拡散部分を構成する材料の種類などに応じて適
宜決定すればよい。例えばAlGaAs系半導体の場合
には、Be%Zn、 Ge、 S、 Siなどを用いる
ことができる。
The type of impurity is not particularly limited as long as it can form a region into which carriers can be injected into each active layer, and may be appropriately determined depending on the type of material constituting the diffused portion. For example, in the case of an AlGaAs-based semiconductor, Be%Zn, Ge, S, Si, etc. can be used.

不純物の拡散は、集束イオンビーム注入法により加速電
圧を変えて、対応する活性層に達する位置または近傍の
位置まで行なう。その近傍の位置は、不純物拡散領域か
ら活性層へとキャリアが良好に注入されるような位置で
あればよい。また、不純物の拡散は、各活性層に対す゛
る拡散領域が接することのないよう、すなわち各活性層
が各々独立駆動可能となるよう行なう。
The impurity is diffused by focused ion beam implantation by changing the acceleration voltage until it reaches the corresponding active layer or a position near it. The position in the vicinity may be any position that allows carriers to be well injected from the impurity diffusion region to the active layer. Further, the impurity diffusion is performed so that the diffusion regions for each active layer do not touch each other, that is, each active layer can be driven independently.

以上のようにして複数種の活性層と、キャリア注入領域
を形成した後、所望の工程を経て多波長集積半導体レー
ザ装置を完成できる。
After forming a plurality of types of active layers and carrier injection regions as described above, a multi-wavelength integrated semiconductor laser device can be completed through desired steps.

所望の工程とは、クラッド層やキャップ層などを形成し
、それらの層に対して再度不純物を拡散する工程である
The desired process is a process of forming a cladding layer, a cap layer, etc., and diffusing impurities into these layers again.

例えば本発明の好ましい一態様として、下記のようなA
lGaAs系半導体レーザの製造方法を挙げることがで
きる。
For example, as a preferred embodiment of the present invention, the following A
A method for manufacturing an lGaAs-based semiconductor laser can be mentioned.

(イ)適当なブレーナー基板上に複数の活性層と障壁層
を、ブレーナ状面に形成する。
(a) Forming a plurality of active layers and barrier layers on a suitable brainer substrate in a brainer-like surface.

(ロ)そのブレーナ状面の所望の位置に、Be等を活性
層に達する位置または近傍の位置まで拡散することによ
り、該活性層を独立駆動するためのキャリア注入領域(
a)を形成する。
(B) A carrier injection region (
Form a).

(ハ)キャリア注入領域(a)形成後のブレーナ状面の
上にクラッド層やキャップ層などを形成する。
(c) A cladding layer, a cap layer, etc. are formed on the brainer-like surface after the carrier injection region (a) is formed.

(ニ)そのクラッド層やキャップ層の所望の位置に、Z
n等をキャリア注入領域(a)に達する位置まで拡散し
てキャリア注入領域(b)を形成する。
(d) At the desired position of the cladding layer and cap layer, Z
A carrier injection region (b) is formed by diffusing n, etc. to a position reaching the carrier injection region (a).

(ホ)キャリア注入領域(b)に対応する位置に独立電
極を形成する。
(e) An independent electrode is formed at a position corresponding to the carrier injection region (b).

以上のような態様の製造方法により、良好なAlGaA
s系多波長集積半導体レーザ装置を得ることができる。
By the manufacturing method of the above aspects, good AlGaA
An s-based multi-wavelength integrated semiconductor laser device can be obtained.

このような二回の不純物拡散を行なうことが、制御性の
良い拡散が行なえ、且つ製造工程を簡略化できるという
理由で実用的である。
Performing the impurity diffusion twice as described above is practical because it allows for well-controlled diffusion and simplifies the manufacturing process.

また上述の態様において、クラット層やキャップ層の形
成および二度目の不純物拡散は、ブレーナ状の面に対し
て行なえるので、良好な結晶成長および不純物拡散が容
易にできる。それに対して、先に述べた従来の方法■に
おいては、エツチング後の面は凹凸状なので、結晶の異
常成長や不純物の偏析などの問題が生じる場合が有る。
Further, in the above-described embodiment, the formation of the crat layer and the cap layer and the second diffusion of impurities can be performed on the Brenna-shaped surface, so that good crystal growth and impurity diffusion can be easily achieved. On the other hand, in the above-mentioned conventional method (2), since the surface after etching is uneven, problems such as abnormal growth of crystals and segregation of impurities may occur.

以上の説明したような本発明の製造方法により得られる
多波長集積半導体レーザ装置は、例えば光通信などの分
野に有用である。
The multi-wavelength integrated semiconductor laser device obtained by the manufacturing method of the present invention as described above is useful in fields such as optical communications, for example.

また、本発明の製造方法により得られる多波長集積半導
体レーザ装置の構成は、以上の製造方法の説明にて明ら
かなように、異なる波長の光を発振する複数種の活性層
および必要な場合には所望の障壁層を有し、且つ該活性
層を独立駆動するためのキャリア注入領域を有し、その
キャリア注入領域は該複数種の活性層に達する位置また
は近傍の位置まで不純物を拡散することにより形成され
たものであることを特徴とする装置である。
Furthermore, as is clear from the above description of the manufacturing method, the configuration of the multi-wavelength integrated semiconductor laser device obtained by the manufacturing method of the present invention includes multiple types of active layers that oscillate light of different wavelengths and, if necessary, has a desired barrier layer and a carrier injection region for independently driving the active layer, and the carrier injection region diffuses impurities to a position reaching or near the plurality of active layers. This device is characterized in that it is formed by.

[実施例] 以下、実施例により、本発明の詳細な説明する。[Example] Hereinafter, the present invention will be explained in detail with reference to Examples.

実施例1 まず、第1図に示すように、n型GaAs基板7上に、
n型GaAs緩衝層6、n型第1クラッド層5を形成し
、その上にn−型障壁層34.33.32.31と、発
振波長の異なるn−型またはundope活性層43.
42.41とを順次交互に形成した。
Example 1 First, as shown in FIG. 1, on an n-type GaAs substrate 7,
An n-type GaAs buffer layer 6 and an n-type first cladding layer 5 are formed, on which are formed an n-type barrier layer 34, 33, 32, 31, and an n-type or undoped active layer 43.33 having a different oscillation wavelength.
42 and 41 were formed sequentially and alternately.

次いで、集束イオンビーム注入により、加速電圧を各々
40kV、60kV、80kVとして、Beを幅2 p
mのストライプ状にdose量lXl0”程度注入し、
それぞれの活性層に対応したp1領域303.203.
103を形成した。
Next, by focused ion beam implantation, the Be was implanted into a width of 2 p with acceleration voltages of 40 kV, 60 kV, and 80 kV, respectively.
Inject a dose of about 1X10'' in stripes of m,
p1 regions 303.203.corresponding to each active layer.
103 was formed.

次いで、第2図に示すように、高抵抗第2クラツドN2
、高抵抗キャップ層lを形成した。その後、5iJ4膜
をマスクとして拡散用窓を形成し、ZnAsと同時に石
英アンプル内に封入し、znをBe注入領域303.2
03.103に達するまで幅4pmのストライプ状に熱
拡散し、それぞれに対応するp+領域302.202.
102を形成した。次いで、n型共通電極401および
p型独立電極301.201.101を形成し、襞間に
よりファブリベロー共振器を形成した。
Next, as shown in FIG. 2, the high resistance second clad N2
, a high resistance cap layer l was formed. Thereafter, a diffusion window was formed using the 5iJ4 film as a mask, and the Zn was sealed in a quartz ampoule at the same time as the ZnAs in the Be implanted region 303.2.
The heat is diffused in stripes with a width of 4 pm until reaching 03.103, and the corresponding p+ regions 302.202.
102 was formed. Next, an n-type common electrode 401 and p-type independent electrodes 301, 201, and 101 were formed, and a Fabry bellows resonator was formed between the folds.

以上のようにして作製した多波長集積半導体レーザ装置
において、電極101と電極401との間に順方向電圧
を印加すると、電子は第1クラッド層5から複数の活性
層43.42.41に注入されるが、電子の拡散長に比
べて、活性層43.42.41までの距離は十分短いの
で、電子は各活性層にほぼ均等に注入される。一方、正
孔は、Be注入領域から活性層43.42.41の積M
方向へ注入されるが、正孔の拡散長は短いので、Be注
入領域に最も近い活性層41に正孔の大部分が注入され
る。したがって、電子と正孔の再結合は活性層41内で
生じ、活性層41に対応した波長の光(λ1)が発生す
る。同様に、電極201.401問および電極301.
401間に順方向電圧を印加することにより、活性層4
2.43からそれぞれに対応した波長の光(λ2、λ3
)が発生する。
In the multi-wavelength integrated semiconductor laser device manufactured as described above, when a forward voltage is applied between the electrode 101 and the electrode 401, electrons are injected from the first cladding layer 5 into the plurality of active layers 43, 42, 41. However, since the distance to the active layers 43, 42, 41 is sufficiently short compared to the electron diffusion length, electrons are injected into each active layer almost equally. On the other hand, holes flow from the Be injection region to the active layer 43, 42, 41 by the product M
However, since the diffusion length of the holes is short, most of the holes are injected into the active layer 41 closest to the Be injection region. Therefore, recombination of electrons and holes occurs within the active layer 41, and light (λ1) of a wavelength corresponding to the active layer 41 is generated. Similarly, electrode 201.401 and electrode 301.
By applying a forward voltage between 401 and 401, the active layer 4
From 2.43, the light of the corresponding wavelength (λ2, λ3
) occurs.

なお、本実施例においては、各層の形成は、分子線エピ
タキシー法(MBE法)により行ない、その厚み等は、
表−1に示すようにした。
In this example, each layer was formed by the molecular beam epitaxy method (MBE method), and the thickness etc.
The procedure was as shown in Table-1.

表−1 上記構成で得られる波長は、活性層43.42.41に
対応してそれぞれλ3=約880nm 、λ、=約86
0nm 、λ3=約840nmであった。
Table 1 The wavelengths obtained with the above configuration are λ3=approximately 880 nm and λ=approximately 86 nm corresponding to the active layers 43, 42, and 41, respectively.
0 nm, and λ3=about 840 nm.

なお、本実施例においては、活性層のGaとA1の組成
を変えて多波長を得たが、活性層の厚さの違いによる量
子準位の違いを利用したものであってもよい。
In this example, multiple wavelengths were obtained by changing the compositions of Ga and A1 in the active layer, but it is also possible to utilize differences in quantum levels due to differences in the thickness of the active layer.

また、本実施例においては、分子線エピタキシー法(層
形成用)と集束イオンビーム注入法(不純物拡散用)を
用いているので、画法の装置を結合すれば、2回目の成
膜までは真空内で行なうことが可能である。
In addition, in this example, the molecular beam epitaxy method (for layer formation) and the focused ion beam implantation method (for impurity diffusion) are used, so if the imaging equipment is connected, up to the second film formation. It is possible to carry out in a vacuum.

実施例2 実施例1におけるBe拡散工程の後に、第3図に示すよ
うに、ホウ素またはガリウムを全ての活性層を分断する
深さにまで注入することにより、高抵抗領域を501.
502を形成した以外は実施例1と同様にして多波長集
積半導体レーザ装置を作製した。
Example 2 After the Be diffusion step in Example 1, as shown in FIG. 3, a high resistance region is formed by implanting boron or gallium to a depth that divides all the active layers.
A multi-wavelength integrated semiconductor laser device was manufactured in the same manner as in Example 1 except that 502 was formed.

本実施例によれば、個々のレーザ間の電気的分離が改善
され、特に、電気的リークによろいクロストークを低減
することが可能である。
According to this embodiment, electrical isolation between individual lasers is improved, and in particular, it is possible to reduce crosstalk caused by electrical leakage.

[発明の効果] 以上説明したように、本発明の製造方法においては、不
純物の拡散によってキャリア注入領域を形成するので、
活性層を積層状に形成した状態のままで独立駆動可能で
あり、それ故に活性層の材料および組成に特別な制限が
なく、各活性層レーザ特性が均一であり、レーザの寿命
が短くならないような多波長集積半導体レーザ装置が得
られる。
[Effects of the Invention] As explained above, in the manufacturing method of the present invention, since the carrier injection region is formed by diffusion of impurities,
The active layer can be driven independently while remaining in a laminated state, so there are no special restrictions on the material and composition of the active layer, and the laser characteristics of each active layer are uniform, so that the laser life is not shortened. A multi-wavelength integrated semiconductor laser device can be obtained.

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

第1図および第2図は実施例1の方法の過程を示す模式
的断面図、第3図は実施例2の方法の過程を示す模式的
断面図、第4図および第5図は従来の方法により得られ
る多波長集積半導体レーザ装置を例示する模式的断面図
である。 l・・・高抵抗キャップ層 2・・・高抵抗クラッド層
31〜34・・・n型障壁層  41〜43・・・活性
層5・・・n型クラッド層  6・・・p型緩衝層7・
・・n型基板 lol、 201.301・・・p型独立電極102、
202.302・・・Zn拡散領域(キャリア注入領域
)103.203,303 ・Be散領領域キャリア注
入領域)401・・・n型共通電極
1 and 2 are schematic sectional views showing the process of the method of Example 1, FIG. 3 is a schematic sectional view showing the process of the method of Example 2, and FIGS. 4 and 5 are schematic sectional views showing the process of the method of Example 2. FIG. 2 is a schematic cross-sectional view illustrating a multi-wavelength integrated semiconductor laser device obtained by the method. l... High resistance cap layer 2... High resistance cladding layer 31-34... N-type barrier layer 41-43... Active layer 5... N-type cladding layer 6... P-type buffer layer 7.
...N-type substrate lol, 201.301...P-type independent electrode 102,
202.302... Zn diffusion region (carrier injection region) 103.203, 303 ・Be diffusion region carrier injection region) 401... n-type common electrode

Claims (1)

【特許請求の範囲】 1)(イ)異なる波長の光を発振する複数種の活性層を
積層する過程と、 (ロ)該複数種の活性層に達する位置または近傍の位置
まで不純物を拡散することにより、該活性層を独立駆動
するためのキャリア注入領域を形成する過程とを含むこ
とを特徴とする多波長集積半導体レーザ装置の製造方法
。 2)請求項1記載の製造方法により作製された多波長集
積半導体レーザ装置。
[Claims] 1) (a) A process of laminating multiple types of active layers that oscillate light of different wavelengths, and (b) Diffusing impurities to a position reaching or near the multiple types of active layers. A method for manufacturing a multi-wavelength integrated semiconductor laser device, comprising the step of forming a carrier injection region for independently driving the active layer. 2) A multi-wavelength integrated semiconductor laser device manufactured by the manufacturing method according to claim 1.
JP19338088A 1988-08-04 1988-08-04 Multi-wavelength integrated semiconductor laser device and its manufacturing method Pending JPH0243788A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19338088A JPH0243788A (en) 1988-08-04 1988-08-04 Multi-wavelength integrated semiconductor laser device and its manufacturing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19338088A JPH0243788A (en) 1988-08-04 1988-08-04 Multi-wavelength integrated semiconductor laser device and its manufacturing method

Publications (1)

Publication Number Publication Date
JPH0243788A true JPH0243788A (en) 1990-02-14

Family

ID=16306961

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19338088A Pending JPH0243788A (en) 1988-08-04 1988-08-04 Multi-wavelength integrated semiconductor laser device and its manufacturing method

Country Status (1)

Country Link
JP (1) JPH0243788A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5708674A (en) * 1995-01-03 1998-01-13 Xerox Corporation Semiconductor laser or array formed by layer intermixing
JP2008135793A (en) * 2008-02-28 2008-06-12 Oki Electric Ind Co Ltd Semiconductor light-emitting apparatus and led array

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5708674A (en) * 1995-01-03 1998-01-13 Xerox Corporation Semiconductor laser or array formed by layer intermixing
US5843802A (en) * 1995-01-03 1998-12-01 Xerox Corporation Semiconductor laser formed by layer intermixing
JP2008135793A (en) * 2008-02-28 2008-06-12 Oki Electric Ind Co Ltd Semiconductor light-emitting apparatus and led array

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