JPH04237182A - Manufacture of distorted quantum well laser - Google Patents
Manufacture of distorted quantum well laserInfo
- Publication number
- JPH04237182A JPH04237182A JP580891A JP580891A JPH04237182A JP H04237182 A JPH04237182 A JP H04237182A JP 580891 A JP580891 A JP 580891A JP 580891 A JP580891 A JP 580891A JP H04237182 A JPH04237182 A JP H04237182A
- Authority
- JP
- Japan
- Prior art keywords
- quantum well
- layer
- strained quantum
- active layer
- gaas
- 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.)
- Withdrawn
Links
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 18
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims abstract description 24
- 239000000758 substrate Substances 0.000 claims abstract description 17
- 238000000034 method Methods 0.000 claims abstract description 14
- 238000009792 diffusion process Methods 0.000 claims abstract description 5
- 238000005253 cladding Methods 0.000 claims description 9
- 230000003287 optical effect Effects 0.000 claims description 7
- 239000002994 raw material Substances 0.000 claims description 4
- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 abstract description 11
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 abstract description 9
- 230000010355 oscillation Effects 0.000 abstract description 6
- 239000013078 crystal Substances 0.000 abstract description 3
- 239000004065 semiconductor Substances 0.000 description 6
- 238000001312 dry etching Methods 0.000 description 3
- 238000003486 chemical etching Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 229910052733 gallium Inorganic materials 0.000 description 2
- 230000001678 irradiating effect Effects 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 1
- 238000003776 cleavage reaction Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 150000001875 compounds Chemical class 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 229910052738 indium Inorganic materials 0.000 description 1
- 230000010365 information processing Effects 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000001459 lithography Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000005693 optoelectronics Effects 0.000 description 1
- 230000007017 scission Effects 0.000 description 1
- 238000000772 tip-enhanced Raman spectroscopy Methods 0.000 description 1
Landscapes
- Semiconductor Lasers (AREA)
Abstract
Description
【0001】0001
【産業上の利用分野】本発明は、化合物半導体の光・電
子デバイスの高性能化に大きく寄与する歪み量子井戸レ
ーザの製造方法に関するものである。即ち、2種類のバ
ンドギャップの違う半導体から構成され、エネルギーギ
ャップが大きい半導体によって他方の半導体が包み込ま
れ、活性層となる量子井戸が基板と格子定数が異なり歪
むことを特徴とした歪み量子井戸レーザの製造方法に関
するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for manufacturing a strained quantum well laser, which greatly contributes to improving the performance of compound semiconductor opto-electronic devices. In other words, it is a strained quantum well laser that is composed of two types of semiconductors with different band gaps, in which the other semiconductor is surrounded by the semiconductor with a large energy gap, and the quantum well serving as the active layer has a different lattice constant from the substrate and is distorted. The present invention relates to a manufacturing method.
【0002】0002
【従来の技術】従来、このような分野の技術としては、
例えば
A.Lasson,S.Forouhar,J.Cod
y and R.J.Lang:「980nmで発
振する高信頼性狭ストライプ・プッシュドモーフィック
・単一量子井戸レーザの高出力動作」(High−Po
wer Operation of Highl
y Reliable Narrow Stri
pePseudomorphic Single
Quantum WellLasers Emit
ting at 980 nm)IEEE P
HOTONICS TECHNOLOGY LET
TERS VOL.2,No.5,MAY,1990
年 P.307−309に記載されるものがあった。[Prior Art] Conventionally, technologies in this field include:
For example, A. Lasson, S. Forouhar, J. Cod
y and R. J. Lang: "High-power operation of a highly reliable narrow stripe pushed morphic single quantum well laser oscillating at 980 nm" (High-Po
Were Operation of High
y Reliable Narrow Stri
pePseudomorphic Single
Quantum Well Lasers Emit
ting at 980 nm) IEEE P
HOTONICS TECHNOLOGY LET
TERS VOL. 2, No. 5, MAY, 1990
Year P. There was one described in 307-309.
【0003】図3はかかる従来の分子線エピタキシャル
成長InGaAs/GaAs/AlGaAs GRI
N−SCH SQWの組成プロファイル及び層厚を示
す図、図4はかかる歪み量子井戸レーザの断面図である
。
これらの図に示すように、この種の歪み量子井戸レーザ
の製造方法としては、分子線エピタキシャル成長によっ
て、n−GaAs基板1上にn−AlGaAsクラッド
層2、AlGaAs GRIN−SCH(Grate
d IndexSeparate Confine
ment Heterostracture)+In
GaAs SQW(Single Quantum
Well)層3、p−AlGaAsクラッド層4、
p−GaAsコンタクト層5を積層した後、3μm程度
のストライプの領域を残し、屈折率導波機構を形成する
ため、活性層近傍までドライエッチングあるいは化学エ
ッチングでp−GaAsコンタクト層5、p−AlGa
Asクラッド層4の大部分を除去し、リッジ構造を形成
し、その後、絶縁膜6を用い電流狭窄を行っていた。FIG. 3 shows such conventional molecular beam epitaxial growth InGaAs/GaAs/AlGaAs GRI.
FIG. 4, which is a diagram showing the composition profile and layer thickness of N-SCH SQW, is a cross-sectional view of such a strained quantum well laser. As shown in these figures, the method for manufacturing this type of strained quantum well laser is to form an n-AlGaAs cladding layer 2 and an AlGaAs GRIN-SCH (Grate) on an n-GaAs substrate 1 by molecular beam epitaxial growth.
dIndexSeparate Confine
ment Heterostructure)+In
GaAs SQW (Single Quantum
Well) layer 3, p-AlGaAs cladding layer 4,
After laminating the p-GaAs contact layer 5, the p-GaAs contact layer 5 and the p-AlGa are deposited by dry etching or chemical etching to the vicinity of the active layer, leaving a stripe region of about 3 μm and forming a refractive index waveguide mechanism.
Most of the As cladding layer 4 was removed to form a ridge structure, and then an insulating film 6 was used to perform current confinement.
【0004】0004
【発明が解決しようとする課題】しかしながら、上記の
歪み量子井戸レーザの製造方法では、基本横モード発振
させるためのリッジ構造を、精度良く作製するのが化学
エッチングでは困難であり、ドライエッチングでは、活
性層に損傷が入るという欠点があった。また、基板と格
子整合しないInGaAsを全面に成長しているので、
高出力発振時にストレスに起因する欠陥が生じ、レーザ
素子が劣化するという欠点があった。[Problems to be Solved by the Invention] However, in the above-mentioned method for manufacturing a strained quantum well laser, it is difficult to precisely produce the ridge structure for fundamental transverse mode oscillation by chemical etching, and by dry etching, There was a drawback that the active layer was damaged. In addition, since InGaAs, which is not lattice matched to the substrate, is grown on the entire surface,
There is a drawback that defects occur due to stress during high-output oscillation, and the laser element deteriorates.
【0005】本発明は、以上に述べたリッジ構造をエッ
チングによって作製する時の問題点とストレスが基板全
面にかかるという問題点を除去し、特性が向上し、信頼
性の高い歪み量子井戸レーザの製造方法を提供すること
を目的としている。The present invention eliminates the above-mentioned problems when fabricating a ridge structure by etching and stress applied to the entire surface of the substrate, and creates a strained quantum well laser with improved characteristics and high reliability. The purpose is to provide a manufacturing method.
【0006】[0006]
【課題を解決するための手段】本発明によれば、上記目
的を達成するために、基板上に分子線エピタキシャル成
長によりクラッド層及び光導波層が形成される基板部を
形成する工程と、該基板部上方にストライプ状のマスク
をセットする工程と、分子線エピタキシャル成長法を用
いて活性層となる歪み量子井戸を成長中の原子の拡散を
制御し、歪み量子井戸活性層を埋め込む埋め込み層を形
成する工程とを施すようにしたものである。[Means for Solving the Problems] According to the present invention, in order to achieve the above object, a step of forming a substrate portion on which a cladding layer and an optical waveguide layer are formed by molecular beam epitaxial growth on a substrate; A step in which a striped mask is set above the active layer and a molecular beam epitaxial growth method is used to control the diffusion of atoms during growth of the strained quantum well that will become the active layer, forming a buried layer that buries the strained quantum well active layer. The process is as follows.
【0007】また、前記歪み量子井戸活性層を埋め込む
工程は、微小領域に歪み量子井戸活性層を成長させ、I
II ,V族原料を交互及び同時に供給することによっ
て行う。更に、前記歪み量子井戸活性層は、InGaA
sからなり、前記埋め込み層はGaAsからなる。[0007] Furthermore, the step of embedding the strained quantum well active layer involves growing the strained quantum well active layer in a minute region,
This is done by feeding Group II and V raw materials alternately and simultaneously. Furthermore, the strained quantum well active layer is made of InGaA
The buried layer is made of GaAs.
【0008】[0008]
【作用】本発明によれば、上記したように、分子線エピ
タキシャル成長により、ストライプ状のマスクを用いて
、微小領域に歪み量子井戸活性層を成長させ、III
,V族原料を交互及び同時に供給し、活性層を埋め込む
。
従って、結晶成長によって電流狭窄機構と屈折率導波機
構を持つ歪み量子井戸レーザ構造が形成できるので、レ
ーザ素子作製時間を大幅に短縮できる。[Operation] According to the present invention, as described above, a strained quantum well active layer is grown in a minute region by molecular beam epitaxial growth using a striped mask, and
, V group raw materials are supplied alternately and simultaneously to embed the active layer. Therefore, since a strained quantum well laser structure having a current confinement mechanism and a refractive index waveguide mechanism can be formed by crystal growth, the time for manufacturing a laser device can be significantly shortened.
【0009】また、このように、作製ストライプ領域だ
けに形成された歪み量子井戸を活性層とする半導体レー
ザを作製することにより、発振閾値電流の低減と温度依
存性の低減、発光線幅の低減、変調周波数の増大および
信頼性の高いレーザを得ることができる。Furthermore, by manufacturing a semiconductor laser in which the active layer is a strained quantum well formed only in the fabrication stripe region, it is possible to reduce the oscillation threshold current, temperature dependence, and emission line width. , it is possible to obtain an increased modulation frequency and a highly reliable laser.
【0010】0010
【実施例】以下、本発明の実施例を図面を用いて詳細に
説明する。図1は本発明の実施例を示す歪み量子井戸レ
ーザの製造工程断面図である。まず、図1(a)に示す
ように、分子線エピタキシャル成長により、n−GaA
s(001)基板11上に、n−AlGaAsクラッド
層12(約1μm)、GaAs光導波層13(約20n
m)を積層する。つまり、基板部を形成する。Embodiments Hereinafter, embodiments of the present invention will be explained in detail with reference to the drawings. FIG. 1 is a sectional view showing the manufacturing process of a strained quantum well laser according to an embodiment of the present invention. First, as shown in Figure 1(a), n-GaA
On the s(001) substrate 11, an n-AlGaAs cladding layer 12 (approximately 1 μm) and a GaAs optical waveguide layer 13 (approximately 20 nm) are formed.
m) is laminated. In other words, a substrate portion is formed.
【0011】次に、図1(b)に示すように、幅3μm
程度のストライプ状のマスク14をかぶせる。そこで、
図2に示すように、数秒間シャッタを閉め、全原料供給
を停止し、Gaのシャッタを開き(t1 )1原子層程
度のGaビームを照射後、シャッタを閉じ、数秒間Ga
原子の表面拡散を促進する。次に、Asのシャッタを開
き(t2 )、これに引き続き、Inのシャッタを開き
(t3 )、1原子層以下のInビームを照射後に、I
nシャッタを閉じてから、Asのシャッタを閉じ、In
原子の表面拡散を抑制する。数秒間の後にGaシャッタ
を開け(t4 )、1原子層程度のGaを照射すること
を繰り返し、InGaAs量子井戸活性層15とGaA
s埋め込み層16を同時にストライプ領域に形成する。
Inビームの供給量は、1原子層以下で、発振波長と閾
値電流が最小になるようにする。InGaAs量子井戸
活性層15の厚みもこの条件によって決まる。更に、G
aAs光導波層17(約20nm)もGaとAsビーム
の1原子層程度の交互供給の成長手法で形成する。Next, as shown in FIG. 1(b), the width is 3 μm.
Cover with a striped mask 14 of about 100 mL. Therefore,
As shown in Figure 2, the shutter is closed for a few seconds, all raw material supply is stopped, and the Ga shutter is opened (t1). After irradiating a Ga beam of approximately one atomic layer, the shutter is closed and the Ga beam is
Facilitates surface diffusion of atoms. Next, the As shutter is opened (t2), followed by the In shutter (t3), and after irradiating the In beam of one atomic layer or less, the I
Close the n shutter, then close the As shutter, and then
Suppresses surface diffusion of atoms. After a few seconds, the Ga shutter is opened (t4) and irradiation with about one atomic layer of Ga is repeated until the InGaAs quantum well active layer 15 and the GaA
An s-buried layer 16 is simultaneously formed in the stripe region. The amount of In beam supplied is set to be one atomic layer or less so that the oscillation wavelength and threshold current are minimized. The thickness of the InGaAs quantum well active layer 15 is also determined by this condition. Furthermore, G
The aAs optical waveguide layer 17 (about 20 nm) is also formed by a growth method in which Ga and As beams are alternately supplied in layers of about one atomic layer.
【0012】次いで、通常の成長法で、p−AlGaA
sクラッド層18(約1μm)、p−GaAsコンタク
ト層19(約0.5μm)をストライプ領域に形成する
。マスク14上には、InGaAs多結晶23、GaA
s多結晶24、AlGaAs多結晶25、GaAs多結
晶26が積層される。次いで、図1(c)に示すように
、絶縁膜20を形成し、通常のリソグラフィ技術を用い
て、p−GaAsコンタクト層19上の絶縁膜を取り除
き、p側電極21を形成する。次に、裏面にn側電極2
2を形成し、ドライエッチングあるいはへき開によって
、レーザ端面を形成する。[0012] Next, p-AlGaA is grown using a normal growth method.
An s-cladding layer 18 (approximately 1 μm) and a p-GaAs contact layer 19 (approximately 0.5 μm) are formed in the stripe region. On the mask 14, InGaAs polycrystal 23, GaA
S polycrystal 24, AlGaAs polycrystal 25, and GaAs polycrystal 26 are stacked. Next, as shown in FIG. 1C, an insulating film 20 is formed, and the insulating film on the p-GaAs contact layer 19 is removed using a normal lithography technique to form a p-side electrode 21. Next, the n-side electrode 2 is placed on the back side.
2 is formed, and a laser end face is formed by dry etching or cleavage.
【0013】上記した実施例では、n−GaAs基板上
での成長について説明を行ったが、不純物の選択によっ
て、p−GaAs基板上でもかまわない。更に、GaS
b基板上へのInGaSb量子井戸レーザ、GaP基板
上へのGaInP量子井戸レーザの形成等についても応
用できる。なお、本発明は上記実施例に限定されるもの
ではなく、本発明の趣旨に基づいて種々の変形が可能で
あり、これらを本発明の範囲から排除するものではない
。In the above embodiments, growth on an n-GaAs substrate was explained, but growth on a p-GaAs substrate may be used depending on the selection of impurities. Furthermore, GaS
It can also be applied to the formation of an InGaSb quantum well laser on a b substrate, a GaInP quantum well laser on a GaP substrate, etc. Note that the present invention is not limited to the above-mentioned embodiments, and various modifications can be made based on the spirit of the present invention, and these are not excluded from the scope of the present invention.
【0014】[0014]
【発明の効果】以上詳細に説明したように、本発明によ
れば、結晶成長によって電流狭窄機構と屈折率導波機構
を持つ歪み量子井戸レーザ構造を形成できるので、レー
ザ素子作製時間を大幅に短縮できる。また、このように
、作製ストライプ領域だけに形成された歪み量子井戸を
活性層とする半導体レーザを作製することにより、発振
閾値電流の低減と温度依存性の低減、発光線幅の低減、
変調周波数の増大および信頼性の高いレーザを得るこき
ができる。そして、本発明は、超高速の光情報処理及び
通信等の広い分野に適用することができる。[Effects of the Invention] As explained in detail above, according to the present invention, a strained quantum well laser structure having a current confinement mechanism and a refractive index waveguide mechanism can be formed by crystal growth, so that the manufacturing time of a laser device can be significantly reduced. Can be shortened. In addition, by manufacturing a semiconductor laser in which the active layer is a strained quantum well formed only in the fabricated stripe region, it is possible to reduce the oscillation threshold current, reduce temperature dependence, and reduce the emission line width.
It is possible to increase the modulation frequency and obtain a highly reliable laser. The present invention can be applied to a wide range of fields such as ultra-high speed optical information processing and communication.
【図1】本発明の実施例を示す歪み量子井戸レーザの製
造工程断面図である。FIG. 1 is a cross-sectional view showing the manufacturing process of a strained quantum well laser according to an embodiment of the present invention.
【図2】本発明の歪み量子井戸作製時のGa,In,A
sシャッタの開閉フローチャートである。[Figure 2] Ga, In, A during fabrication of strained quantum wells of the present invention
5 is a flowchart for opening and closing the s-shutter.
【図3】従来の分子線エピタキシャル成長InGaAs
/GaAs/AlGaAs GRIN−SCH S
QWの組成プロファイル及び層厚を示す図である。[Figure 3] Conventional molecular beam epitaxial growth InGaAs
/GaAs/AlGaAs GRIN-SCH S
It is a figure which shows the composition profile and layer thickness of QW.
【図4】従来の歪み量子井戸レーザの断面図である。FIG. 4 is a cross-sectional view of a conventional strained quantum well laser.
11 n−GaAs(001)基板12
n−AlGaAsクラッド層13 GaAs光導
波層
14 マスク
15 InGaAs量子井戸活性層16
GaAs埋め込み層
17 GaAs光導波層
18 p−AlGaAsクラッド層19
p−GaAsコンタクト層20 絶縁膜
21 p側電極
22 n側電極
23 InGaAs多結晶
24 GaAs多結晶
25 AlGaAs多結晶
26 GaAs多結晶11 n-GaAs (001) substrate 12
n-AlGaAs cladding layer 13 GaAs optical waveguide layer 14 mask 15 InGaAs quantum well active layer 16
GaAs buried layer 17 GaAs optical waveguide layer 18 p-AlGaAs cladding layer 19
p-GaAs contact layer 20 insulating film 21 p-side electrode 22 n-side electrode 23 InGaAs polycrystal 24 GaAs polycrystal 25 AlGaAs polycrystal 26 GaAs polycrystal
Claims (3)
によりクラッド層及び光導波層が形成される基板部を形
成する工程と、 (b)該基板部上方にストライプ状のマスクをセットす
る工程と、 (c)分子線エピタキシャル成長法を用いて活性層とな
る歪み量子井戸を成長中の原子の拡散を制御し、歪み量
子井戸活性層を埋め込む埋め込み層を形成する工程とを
施すことを特徴とする歪み量子井戸レーザの製造方法。1. (a) forming a substrate portion on which a cladding layer and an optical waveguide layer are formed by molecular beam epitaxial growth, and (b) setting a striped mask above the substrate portion. (c) controlling the diffusion of atoms during growth of the strained quantum well that will become the active layer using a molecular beam epitaxial growth method to form a buried layer that buries the strained quantum well active layer. A method for manufacturing strained quantum well lasers.
程は、微小領域に歪み量子井戸活性層を成長させ、II
I ,V族原料を交互及び同時に供給することを特徴と
する請求項1記載の歪み量子井戸レーザの製造方法。2. In the step of embedding the strained quantum well active layer, the strained quantum well active layer is grown in a micro region, and
2. The method of manufacturing a strained quantum well laser according to claim 1, wherein the I and V group raw materials are supplied alternately and simultaneously.
sからなり、前記埋め込み層はGaAsからなる請求項
1記載の歪み量子井戸レーザの製造方法。3. The strained quantum well active layer is made of InGaA.
2. The method of manufacturing a strained quantum well laser according to claim 1, wherein the buried layer is made of GaAs.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP580891A JPH04237182A (en) | 1991-01-22 | 1991-01-22 | Manufacture of distorted quantum well laser |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP580891A JPH04237182A (en) | 1991-01-22 | 1991-01-22 | Manufacture of distorted quantum well laser |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04237182A true JPH04237182A (en) | 1992-08-25 |
Family
ID=11621387
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP580891A Withdrawn JPH04237182A (en) | 1991-01-22 | 1991-01-22 | Manufacture of distorted quantum well laser |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04237182A (en) |
-
1991
- 1991-01-22 JP JP580891A patent/JPH04237182A/en not_active Withdrawn
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