JPH084183B2 - Semiconductor laser - Google Patents
Semiconductor laserInfo
- Publication number
- JPH084183B2 JPH084183B2 JP24259487A JP24259487A JPH084183B2 JP H084183 B2 JPH084183 B2 JP H084183B2 JP 24259487 A JP24259487 A JP 24259487A JP 24259487 A JP24259487 A JP 24259487A JP H084183 B2 JPH084183 B2 JP H084183B2
- Authority
- JP
- Japan
- Prior art keywords
- superlattice
- layers
- layer
- semiconductor laser
- quantum well
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/30—Structure or shape of the active region; Materials used for the active region
- H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
- H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
- H01S5/34313—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y20/00—Nanooptics, e.g. quantum optics or photonic crystals
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/30—Structure or shape of the active region; Materials used for the active region
- H01S5/34—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
- H01S5/343—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
- H01S5/34313—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs
- H01S5/3432—Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer having only As as V-compound, e.g. AlGaAs, InGaAs the whole junction comprising only (AI)GaAs
Landscapes
- Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Engineering & Computer Science (AREA)
- Nanotechnology (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Life Sciences & Earth Sciences (AREA)
- Biophysics (AREA)
- Crystallography & Structural Chemistry (AREA)
- Semiconductor Lasers (AREA)
Description
【発明の詳細な説明】 発明の要約 半導体レーザの活性層を障壁層と井戸層とが交互に積
層されてなる多重量子井戸構造とし,さらにこの多重量
子井戸の障壁層および井戸層を超格子構造とした。これ
により温度特性のよい短波長でかつ低しきい値の半導体
レーザの実現が期待できる。The active layer of a semiconductor laser has a multi-quantum well structure in which barrier layers and well layers are alternately laminated, and the barrier layers and well layers of the multi-quantum well are superlattice structures. And As a result, it can be expected that a semiconductor laser with good temperature characteristics, a short wavelength and a low threshold is realized.
発明の背景 技術分野 この発明は,量子井戸を活性層とする半導体レーザに
関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor laser having a quantum well as an active layer.
従来技術とその問題点 量子井戸を活性層とする従来の量子井戸レーザには特
開昭62−98690号公開に記載のものがある。これは,GaAs
とAlxGa1-xAsの各薄膜層を1層が3分子層以下となる厚
さに設定して,交互に積層した超格子量子井戸を活性層
とする半導体レーザである。超格子量子井戸を用いると
面内均一性のすぐれた活性層が得られ,高性能で低しき
い値の短波長半導体レーザが得られる。Prior art and its problems A conventional quantum well laser using a quantum well as an active layer is disclosed in Japanese Patent Laid-Open No. 62-98690. This is GaAs
This is a semiconductor laser in which each thin film layer of Al x Ga 1-x As and Al x Ga 1-x As is set to have a thickness of 3 molecular layers or less, and superlattice quantum wells alternately stacked are used as active layers. The use of superlattice quantum wells provides an active layer with excellent in-plane uniformity, and provides high-performance, low-threshold short-wavelength semiconductor lasers.
しかしながら,上記の超格子量子井戸レーザにおいて
は活性層が薄いために温度特性が悪いという問題点があ
る。However, the above-mentioned superlattice quantum well laser has a problem that the temperature characteristics are poor because the active layer is thin.
発明の概要 発明の目的 この発明は,低しきい値,短波長という上記超格子量
子井戸レーザの特徴を活かし,かつ温度特性の改善され
た半導体レーザを提供することを目的とする。SUMMARY OF THE INVENTION It is an object of the present invention to provide a semiconductor laser which utilizes the characteristics of the above superlattice quantum well laser such as low threshold and short wavelength and has improved temperature characteristics.
発明の構成と効果 この発明による半導体レーザは超格子障壁層と超格子
井戸層とが交互に積層されてなる多重超格子量子井戸構
造によって活性層を構成したことを特徴とする。Structure and Effect of the Invention A semiconductor laser according to the present invention is characterized in that an active layer is composed of a multiple superlattice quantum well structure in which superlattice barrier layers and superlattice well layers are alternately laminated.
上記超格子障壁層および超格子井戸層はともに,1層が
5分子層以下の組成の異なる2種類の薄層,たとえばGa
As層とAlGaAs層とを交互に積層することにより構成され
る。Both the superlattice barrier layer and the superlattice well layer are composed of two types of thin layers each having a composition of 5 molecular layers or less, such as Ga.
It is configured by alternately stacking As layers and AlGaAs layers.
多重量子井戸構造は発振波長が比較的長いが温度特性
が良いという特徴をもつ。そこでこの発明においては,
超格子構造を温度特性に優れた多重量子井戸構造に適用
し,超格子量子井戸層と超格子障壁層とが交互に積層さ
れてなる多重超格子量子井戸構造によって活性層を構成
した。優れた面内平坦性を保ちながら結晶成長を行なう
ことができるので,超格子構造の特徴である低しきい値
化と短波長性を損うことなく、温度特性が向上するとい
う効果が期待できる。The multi-quantum well structure has a characteristic that the oscillation wavelength is relatively long but the temperature characteristic is good. So, in this invention,
The superlattice structure was applied to a multiple quantum well structure with excellent temperature characteristics, and the active layer was composed of a multiple superlattice quantum well structure in which superlattice quantum well layers and superlattice barrier layers were alternately stacked. Since crystal growth can be performed while maintaining excellent in-plane flatness, it is expected that the temperature characteristics will be improved without lowering the threshold and the short wavelength characteristic of the superlattice structure. .
実施例の説明 第1図はこの発明の実施例を示すもので,AlGaAs系半
導体レーザの断面模式図である。第2図は多重超格子量
子井戸活性層の近傍におけるAl平均混晶分布を示してい
る。Description of Embodiments FIG. 1 shows an embodiment of the present invention and is a schematic sectional view of an AlGaAs semiconductor laser. FIG. 2 shows the Al average mixed crystal distribution in the vicinity of the multiple superlattice quantum well active layer.
n−GaAs基板(キャリア濃度Si=1018cm-3)1上にn
−GaAsバッファ層(Si=1018cm-3,厚さ0.5μm)2,n−A
l0.7Ga0.3Asクラッド層(Si=1018cm-3,厚さ1.5μm)
3,ノンドープAlxGa1-xAsGRIN(granded−index)層(厚
さ0.2μm)4,ノンドープAl0.1Ga0.9As/Al0.3Ga0.7As多
重超格子量子井戸構造の活性層(合計の厚さ約720Å)
5,ノンドープAlxGa1-xAsGRIN層(厚さ0.2μm)6,p−Al
0.7Ga0.3Asクラッド層(Be=1018cm-3,厚さ1.5μm)7,
p−GaAsキャップ層(Be=1018cm-3,厚さ0.5μm)8をM
BE法により連続的に成長させることにより半導体レーザ
が作製される。多重超格子量子井戸活性層5は,第1図
に拡大して示されているように,超格子障壁層21と超格
子井戸層22とが交互に積層されてなる。この実施例では
超格子障壁層21が4層,超格子井戸層22が5層設けられ
ている。n on an n-GaAs substrate (carrier concentration Si = 10 18 cm −3 ) 1
−GaAs buffer layer (Si = 10 18 cm −3 , thickness 0.5 μm) 2, n−A
l 0.7 Ga 0.3 As clad layer (Si = 10 18 cm -3 , thickness 1.5 μm)
3, non-doped Al x Ga 1-x As GRIN (granded-index) layer (thickness 0.2 μm) 4, non-doped Al 0.1 Ga 0.9 As / Al 0.3 Ga 0.7 As active layer with multiple superlattice quantum well structure (total thickness About 720Å)
5, undoped Al x Ga 1-x As GRIN layer (thickness 0.2 μm) 6, p-Al
0.7 Ga 0.3 As clad layer (Be = 10 18 cm -3 , thickness 1.5 μm) 7,
p-GaAs cap layer (Be = 10 18 cm -3 , thickness 0.5 μm) 8
A semiconductor laser is manufactured by continuously growing by the BE method. The multiple superlattice quantum well active layer 5 is formed by alternately superposing superlattice barrier layers 21 and superlattice well layers 22, as shown in an enlarged view in FIG. In this embodiment, four superlattice barrier layers 21 and five superlattice well layers 22 are provided.
超格子障壁層21は,そのAl混晶分布が第2図に拡大さ
れて示されているように、Al0.4Ga0.6As層(厚さ9Åが
3層)31aとGaAs層(厚さ3Åが2層)が交互に積層さ
れてなり,合計の厚さが33Åとなっている。超格子井戸
層22は,GaAs層(厚さ9Åが10層)32aとAl0.4Ga0.6As層
(厚さ3Åが9層)32bが交互に積層されてなり,合計
の厚さが117Åとなっている。The superlattice barrier layer 21 has an Al 0.4 Ga 0.6 As layer (three layers with a thickness of 9Å) 31a and a GaAs layer (thickness 3Å with a thickness of 3Å) as shown in FIG. 2 layers) are laminated alternately, and the total thickness is 33Å. The superlattice well layer 22 is composed of GaAs layers (10 layers having a thickness of 9Å) 32a and Al 0.4 Ga 0.6 As layers (9 layers having a thickness of 3Å) 32b alternately laminated, and the total thickness is 117Å. ing.
第1図はこの発明の実施例の半導体レーザの断面模式
図,第2図は第1図の半導体レーザにおけるAl平均混晶
分布を示すグラフである。 5……多重超格子量子井戸活性層, 21……超格子障壁層, 22……超格子井戸層, 31a,32b……Al0.4Ga0.6As層, 31b,32a……GaAs層。FIG. 1 is a schematic sectional view of a semiconductor laser according to an embodiment of the present invention, and FIG. 2 is a graph showing an Al average mixed crystal distribution in the semiconductor laser of FIG. 5 ... Multiple superlattice quantum well active layer, 21 ... Superlattice barrier layer, 22 ... Superlattice well layer, 31a, 32b ... Al 0.4 Ga 0.6 As layer, 31b, 32a ... GaAs layer.
Claims (2)
層されてなる多重超格子量子井戸構造によって活性層が
構成されている半導体レーザ。1. A semiconductor laser having an active layer having a multiple superlattice quantum well structure in which superlattice barrier layers and superlattice well layers are alternately laminated.
に,1層が5分子層以下のGaAs層とAlGaAs層とを交互に積
層することにより構成されている,特許請求の範囲第
(1)項に記載の半導体レーザ。2. The superlattice barrier layer and the superlattice well layer are both constituted by alternately laminating GaAs layers and AlGaAs layers each having 5 or less molecular layers. ) The semiconductor laser according to the paragraph.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24259487A JPH084183B2 (en) | 1987-09-29 | 1987-09-29 | Semiconductor laser |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24259487A JPH084183B2 (en) | 1987-09-29 | 1987-09-29 | Semiconductor laser |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6486584A JPS6486584A (en) | 1989-03-31 |
| JPH084183B2 true JPH084183B2 (en) | 1996-01-17 |
Family
ID=17091370
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP24259487A Expired - Lifetime JPH084183B2 (en) | 1987-09-29 | 1987-09-29 | Semiconductor laser |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH084183B2 (en) |
-
1987
- 1987-09-29 JP JP24259487A patent/JPH084183B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6486584A (en) | 1989-03-31 |
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