JPH04237183A - Distorted quantum well laser - Google Patents
Distorted quantum well laserInfo
- Publication number
- JPH04237183A JPH04237183A JP580991A JP580991A JPH04237183A JP H04237183 A JPH04237183 A JP H04237183A JP 580991 A JP580991 A JP 580991A JP 580991 A JP580991 A JP 580991A JP H04237183 A JPH04237183 A JP H04237183A
- Authority
- JP
- Japan
- Prior art keywords
- quantum well
- active layer
- substrate
- laser
- layer
- 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- Withdrawn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
- 239000000758 substrate Substances 0.000 claims abstract description 21
- 229910001218 Gallium arsenide Inorganic materials 0.000 abstract description 15
- 238000004519 manufacturing process Methods 0.000 abstract description 9
- 239000004065 semiconductor Substances 0.000 abstract description 8
- 238000000034 method Methods 0.000 abstract description 6
- 230000010355 oscillation Effects 0.000 abstract description 6
- 238000005253 cladding Methods 0.000 description 8
- 230000003287 optical effect Effects 0.000 description 7
- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 description 5
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 description 3
- 238000001312 dry etching Methods 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 238000001459 lithography Methods 0.000 description 3
- 238000003486 chemical etching Methods 0.000 description 2
- 238000005530 etching Methods 0.000 description 2
- 229910005542 GaSb Inorganic materials 0.000 description 1
- 230000015572 biosynthetic process Effects 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
- 230000006866 deterioration Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 230000010365 information processing Effects 0.000 description 1
- 238000010030 laminating 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
- 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。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. Concerning 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 that serves as the active layer has a different lattice constant from the substrate and is distorted. It is.
【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2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3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. 2 shows such conventional molecular beam epitaxial growth InGaAs/GaAs/AlGaAs GRI.
FIG. 3, 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、上記し
た従来の歪み量子井戸レーザの製造方法では、基板と格
子整合しないInGaAsを全面に成長しており、発振
波長を長くする時、転位を発生させないで成長できる限
界に近い厚みの活性層を必要とするので、製造プロセス
中や高出力発振時にストレスに起因する欠陥が生じ易く
、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 conventional strained quantum well laser manufacturing method described above, InGaAs, which is not lattice-matched to the substrate, is grown on the entire surface, and when the oscillation wavelength is lengthened, it is difficult to generate dislocations. Since it requires an active layer with a thickness close to the growth limit, it has the disadvantage that defects due to stress are likely to occur during the manufacturing process or during high-output oscillation, and the laser device deteriorates.
【0005】本発明は、以上に述べた活性層の全面にか
かったストレスが素子を劣化させるという問題点を除去
し、特性の向上を図り、信頼性の高い歪み量子井戸レー
ザを提供することを目的としている。The present invention aims to eliminate the above-mentioned problem that stress applied to the entire surface of the active layer deteriorates the device, improve the characteristics, and provide a highly reliable strained quantum well laser. The purpose is
【0006】[0006]
【課題を解決するための手段】本発明は、上記目的を達
成するために、歪み量子井戸レーザにおいて、逆メサ構
造の段差付き基板と、該段差付き基板上に分子線エピタ
キシャル成長法により形成される活性層とを具備し、前
記基板の段差により活性層のつながりを断ち、発光領域
近傍の活性層にかかるストレスの許容度を大きくするよ
うにしたものである。[Means for Solving the Problems] In order to achieve the above object, the present invention provides a strained quantum well laser that includes a stepped substrate having an inverted mesa structure and a structure formed on the stepped substrate by molecular beam epitaxial growth. The active layer is separated from the active layer by the step of the substrate, thereby increasing the tolerance of stress applied to the active layer near the light emitting region.
【0007】[0007]
【作用】本発明は、上記したように、分子線エピタキシ
ャル成長装置を用いて、逆メサの段差付き基板上に半導
体レーザ構造を形成し、段差により活性層のつながりを
断ち、発振領域近傍にかかるストレスの許容度を増大さ
せることができる。従って、従来のように、活性層の全
面にかかるストレスにより、素子を劣化させることはな
くなり、信頼性の高い歪み量子井戸レーザを得ることが
できる。[Operation] As described above, the present invention uses a molecular beam epitaxial growth apparatus to form a semiconductor laser structure on a substrate with an inverted mesa step, and the step breaks the connection between the active layers and causes stress in the vicinity of the oscillation region. Tolerance can be increased. Therefore, unlike in the prior art, stress applied to the entire surface of the active layer does not cause deterioration of the device, and a highly reliable strained quantum well laser can be obtained.
【0008】[0008]
【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、通常のリソ
グラフィ技術と化学エッチングにより、<011>方向
に、幅10μm程度のストライプに逆メサの段差付きn
−GaAs(100)基板11上に、n−GaAsバッ
ファ層12(0.5μm程度)、n−AlX Ga1−
X Asクラッド層13(約1μm)、AlY Ga1
−Y As光導波層14(約100nm)、InV G
a1−V As量子井戸活性層15、AlY Ga1−
Y As光導波層16(約100nm)、p−AlX
Ga1−X Asクラッド層17(約1μm)、p−G
aAsコンタクト層18(約0.5μm)を積層する。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 FIG. 1(a), by molecular beam epitaxial growth, ordinary lithography technology and chemical etching, a stripe with a width of about 10 μm is formed in the <011> direction with an inverted mesa step.
- On a GaAs (100) substrate 11, an n-GaAs buffer layer 12 (about 0.5 μm), an n-AlX Ga1-
X As cladding layer 13 (approximately 1 μm), AlY Ga1
-Y As optical waveguide layer 14 (about 100 nm), InV G
a1-V As quantum well active layer 15, AlY Ga1-
YAs optical waveguide layer 16 (about 100 nm), p-AlX
Ga1-X As cladding layer 17 (approximately 1 μm), p-G
An aAs contact layer 18 (approximately 0.5 μm) is laminated.
【0009】設定された発振波長で、閾値電流を最小に
するという条件で、InV Ga1−V As量子井戸
活性層15の厚みと組成が決まる。AlY Ga1−Y
As光導波層14、16の組成は、活性層でY〜0.
2程度とし、AlX Ga1−X Asクラッド層でY
=Xとなるように直線的に変化させる。次に、図1(b
)に示すように、通常のリソグラフィ技術とドライエッ
チング技術を用いて逆メサの上の中央部に約3μm程度
の幅のストライプを<011>方向に形成し、ストライ
プ領域以外の領域をエッチングし、リッジ構造を形成す
る。このエッチング深さは、AlY Ga1−Y As
光導波層14に到達せず、かつ、屈折率導波機構が作り
付けられるようにする。絶縁膜19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1
8上の絶縁膜を取り除き、p側電極20を形成する。次
に、裏面にn側電極21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。The thickness and composition of the InV Ga1-V As quantum well active layer 15 are determined on the condition that the threshold current is minimized at the set oscillation wavelength. AlYGa1-Y
The composition of the As optical waveguide layers 14 and 16 is Y~0.
2, and Y in the AlX Ga1-X As cladding layer.
=X. Next, Figure 1(b
), a stripe with a width of about 3 μm is formed in the <011> direction at the center of the inverted mesa using normal lithography and dry etching techniques, and the area other than the stripe area is etched. Forms a ridge structure. This etching depth is AlYGa1-YAs
The optical waveguide layer 14 is not reached and a refractive index waveguide mechanism is built. An insulating film 19 is formed, and a p-GaAs contact layer 1 is formed using a normal lithography technique.
The insulating film on 8 is removed, and p-side electrode 20 is formed. Next, an n-side electrode 21 is formed on the back surface, and a laser end face is formed by dry etching or cleaving.
【0010】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基板上でも構わない。また、逆メサ上
以外のエピタキシャル成長領域もエッチングにより、取
り除いてもよい。更に、GaSb基板上へのInGaS
b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。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, the epitaxial growth regions other than those on the inverted mesa may also be removed by etching. Furthermore, InGaS on GaSb substrate
It can also be applied to the formation of b-quantum well lasers, GaInP quantum well lasers on GaP substrates, etc.
【0011】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。It should be noted that the present invention is not limited to the above 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.
【0012】0012
【発明の効果】本発明によれば、逆メサ構造の段差付き
基板上に活性層を成長させることによって、段差により
活性層のつながりを断ち、製造工程及びレーザ発振時に
生じるストレスに対して許容度の大きい歪み量子井戸を
活性層とする半導体レーザを作製することにより、信頼
性の高い歪み量子井戸半導体レーザを得ることができる
。そして、本発明は、超高速な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 According to the present invention, by growing an active layer on a substrate with steps having an inverted mesa structure, the connection between the active layers is severed by the steps, and the tolerance to stress generated during the manufacturing process and laser oscillation is improved. A highly reliable strained quantum well semiconductor laser can be obtained by manufacturing a semiconductor laser having a strained quantum well as an active layer with a large strained quantum well. 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】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 2] 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3】従来の歪み量子井戸レーザの断面図である。FIG. 3 is a cross-sectional view of a conventional strained quantum well laser.
11 逆メサの段差付きn−GaAs(100)
基板12 n−GaAsバッファ層
13 n−AlX Ga1−X Asクラッド層
14 AlY Ga1−Y As光導波層15
InV Ga1−V As量子井戸活性層16
AlY Ga1−Y As光導波層17
p−AlX Ga1−X Asクラッド層18
p−GaAsコンタクト層19 絶縁膜
20 p側電極
21 n側電極11 Inverted mesa stepped n-GaAs (100)
Substrate 12 n-GaAs buffer layer 13 n-AlX Ga1-X As cladding layer 14 AlY Ga1-Y As optical waveguide layer 15
InV Ga1-V As quantum well active layer 16
AlY Ga1-Y As optical waveguide layer 17
p-AlX Ga1-X As cladding layer 18
p-GaAs contact layer 19 insulating film 20 p-side electrode 21 n-side electrode
Claims (1)
)該段差付き基板上に分子線エピタキシャル成長法によ
り形成される活性層とを具備し、 (c)前記基板の段差により活性層のつながりを断ち、
発光領域近傍の活性層にかかるストレスの許容度を大き
くすることを特徴とする歪み量子井戸レーザ。Claim 1: (a) A substrate with steps having an inverted mesa structure; (b)
) an active layer formed by molecular beam epitaxial growth on the stepped substrate; (c) the active layer is disconnected by the stepped substrate;
A strained quantum well laser characterized by increasing the tolerance of stress applied to the active layer near the light emitting region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP580991A JPH04237183A (en) | 1991-01-22 | 1991-01-22 | Distorted quantum well laser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP580991A JPH04237183A (en) | 1991-01-22 | 1991-01-22 | Distorted quantum well laser |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04237183A true JPH04237183A (en) | 1992-08-25 |
Family
ID=11621413
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP580991A Withdrawn JPH04237183A (en) | 1991-01-22 | 1991-01-22 | Distorted quantum well laser |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04237183A (en) |
-
1991
- 1991-01-22 JP JP580991A patent/JPH04237183A/en not_active Withdrawn
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JPH07235732A (en) | Semiconductor laser | |
| US5757835A (en) | Semiconductor laser device | |
| JP2558744B2 (en) | Semiconductor laser device and manufacturing method thereof | |
| JPH08307013A (en) | Semiconductor laser device and manufacturing method thereof | |
| JP2914430B2 (en) | Method for manufacturing semiconductor laser device | |
| JP2960926B2 (en) | Manufacturing method of laser diode | |
| JPS62200786A (en) | Semiconductor laser device and manufacture thereof | |
| JPH05267797A (en) | Light-emitting semiconductor diode | |
| JP2990009B2 (en) | Semiconductor laser and method of manufacturing semiconductor laser | |
| JPH04237183A (en) | Distorted quantum well laser | |
| JP2865160B2 (en) | Manufacturing method of semiconductor laser | |
| JP3022351B2 (en) | Optical semiconductor device and method of manufacturing the same | |
| JPH10209562A (en) | Manufacture of semiconductor laser element | |
| JP3410959B2 (en) | Semiconductor laser device and method of manufacturing the same | |
| JPH11126945A (en) | Manufacture of strained semiconductor crystal and manufacture of semiconductor laser using it | |
| JPH09275239A (en) | Semiconductor laser device | |
| JPH11284276A (en) | Semiconductor laser device and its manufacture | |
| JP3030932B2 (en) | Manufacturing method of semiconductor fine structure | |
| JPH0766992B2 (en) | AlGaInP semiconductor laser and manufacturing method thereof | |
| JPH07176830A (en) | Method for manufacturing semiconductor light emitting device | |
| JPH06112586A (en) | Semiconductor laser diode | |
| JPH08204277A (en) | Semiconductor laser | |
| JPH04280491A (en) | Refractive index waveguide type distortion quantum well laser | |
| JPH06260720A (en) | Semiconductor laser | |
| JPH0936476A (en) | Semiconductor laser |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| A300 | Application deemed to be withdrawn because no request for examination was validly filed |
Free format text: JAPANESE INTERMEDIATE CODE: A300 Effective date: 19980514 |