JPH0541559A - Semiconductor laser - Google Patents

Semiconductor laser

Info

Publication number
JPH0541559A
JPH0541559A JP19631891A JP19631891A JPH0541559A JP H0541559 A JPH0541559 A JP H0541559A JP 19631891 A JP19631891 A JP 19631891A JP 19631891 A JP19631891 A JP 19631891A JP H0541559 A JPH0541559 A JP H0541559A
Authority
JP
Japan
Prior art keywords
semiconductor laser
layer
inp
current block
current
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
JP19631891A
Other languages
Japanese (ja)
Inventor
Hirohito Yamada
博仁 山田
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP19631891A priority Critical patent/JPH0541559A/en
Publication of JPH0541559A publication Critical patent/JPH0541559A/en
Pending legal-status Critical Current

Links

Landscapes

  • Semiconductor Lasers (AREA)

Abstract

PURPOSE:To realize a semiconductor laser which has excellent temperature characteristics with a low threshold value by controlling an inductive current of a semiconductor laser. CONSTITUTION:A semiconductor laser of InGaAsP/InP group comprises a current block layer structure having a distorted superlattice structure 15 alternately forming InxGa1-xAs layer where the composition x of In is larger than 0.53 and InP layer on the entire region or a part of the pn junction interface where a clad layer 16 on the substrate side is in contact with the part other than an active layer 14.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は電流ブロック層構造を有
する半導体レーザに関し、特に加入者光伝送に用いるホ
スタイル仕様の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 current blocking layer structure, and more particularly to a semiconductor laser of a hostile type used for subscriber optical transmission.

【0002】[0002]

【従来の技術】従来構造のpnpnサイリスタ型電流ブ
ロック層を有する半導体レーザにおいては、電流ブロッ
ク層と活性層との隙間を流れるリーク電流が問題とな
り、しきい値の上昇や高温特性の劣化を招いていた。こ
れはブロック層と活性層との隙間を流れるリーク電流に
対しては、基板側クラッド層との界面が順方向にバイア
スされるホモ接合になるため、この部分に拡散電位以上
の電圧が加われば容易に電流が流れてしまう。従ってこ
の部分の電気的抵抗を大きくしなければこれらの特性改
善は望めない。
2. Description of the Related Art In a semiconductor laser having a pnpn thyristor type current blocking layer having a conventional structure, a leak current flowing through a gap between the current blocking layer and the active layer poses a problem, leading to an increase in threshold value and deterioration of high temperature characteristics. Was there. This is a homojunction in which the interface with the substrate-side cladding layer is biased in the forward direction with respect to the leakage current flowing through the gap between the block layer and the active layer, so if a voltage above the diffusion potential is applied to this portion. Electric current easily flows. Therefore, these characteristics cannot be improved unless the electric resistance of this portion is increased.

【0003】[0003]

【発明が解決しようとする課題】本発明の目的はこの様
な従来型の電流ブロック構造の欠点を除去せしめて、低
しきい値でかつ高温特性に優れた半導体レーザを実現す
ることにある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate such drawbacks of the conventional current block structure and realize a semiconductor laser having a low threshold value and excellent high temperature characteristics.

【0004】[0004]

【課題を解決するための手段】本発明の半導体レーザは
電流ブロック構造を有する半導体レーザであって、基板
側クラッド層と活性層以外の部分が接するpn接合界面
の全部あるいは一部に圧縮歪の歪超格子構造を有する電
流ブロック構造を備えることを特徴としている。
The semiconductor laser of the present invention is a semiconductor laser having a current block structure, and a compressive strain is applied to all or part of the pn junction interface where the substrate-side cladding layer and the portion other than the active layer are in contact with each other. It is characterized by having a current block structure having a strained superlattice structure.

【0005】電流ブロック構造を有するInGaAsP
/InP系半導体レーザにおいて、基板側クラッド層と
活性層以外の部分が接するpn接合界面の全部あるいは
一部分に、Inの組成xが0.53よりも大きいInx
Ga1 - x AsとInPを交互に積層させた歪超格子構
造を有する電流ブロック層構造によって上記の課題を解
決できる。
InGaAsP having a current block structure
/ In InP-based semiconductor laser, the whole or part of the pn junction interface where the portions other than the substrate-side cladding layer and the active layer in contact with the composition x of In is larger than 0.53 In x
The above problems can be solved by a current block layer structure having a strained superlattice structure in which Ga 1 -x As and InP are alternately laminated.

【0006】また、電流ブロック構造を有するAlGa
As/GaAs系半導体レーザにおいては、基板側クラ
ッド層と活性層以外の部分が接するpn接合界面の全部
あるいは一部分に、InGaAsとAlGaAsを交互
に積層させた歪超格子構造を有する電流ブロック層の構
造によって上記の課題を解決できる。
AlGa having a current block structure
In an As / GaAs semiconductor laser, a structure of a current block layer having a strained superlattice structure in which InGaAs and AlGaAs are alternately laminated on all or part of a pn junction interface where the substrate-side cladding layer and a portion other than the active layer are in contact with each other. The above problems can be solved by the above.

【0007】[0007]

【作用】本発明の原理を材料をInP/InGaAsP
系レーザを例にして説明する。
The principle of the present invention is that the material is InP / InGaAsP.
A system laser will be described as an example.

【0008】Inの組成xが0.53よりも大きなIn
x Ga1- x AsとInPとを交互に積層させたInx
Ga1 - x As/InP歪超格子(この場合圧縮歪)で
は、バンド不連続(特に価電子帯不連続)が大きくな
り、キャリア注入が起こりにくくなることが最近分かっ
てきた。これは、In0 . 5 3 Ga0 . 4 7As/In
Pヘテロ接合では価電子帯のエネルギー不連続が約30
0meVあるが、Inの組成を大きくしていくと、In
As/InPヘテロ接合において最高520meVのエ
ネルギー不連続の値が得られる。この様に大きなエネル
ギー不連続があるとキャリヤ(この場合はホール)の注
入が妨げられ、電気的には大きな抵抗となる。
In having a composition x of In larger than 0.53
x Ga 1-x As and has a InP are stacked alternately In x
It has recently been found that in a Ga 1 -x As / InP strained superlattice (compressive strain in this case), band discontinuity (particularly valence band discontinuity) becomes large and carrier injection hardly occurs. This, In 0. 5 3 Ga 0 . 4 7 As / In
In the P heterojunction, the energy discontinuity in the valence band is about 30.
Although there is 0 meV, as the composition of In is increased, In
Values of energy discontinuity of up to 520 meV are obtained in As / InP heterojunctions. Such a large energy discontinuity hinders the injection of carriers (holes in this case), resulting in a large electrical resistance.

【0009】図2は本発明の原理を説明するための図
で、この様子を模式的に示したものである。図2(a)
の従来構造の場合InPのホモ接合に拡散電位を越える
順方向電圧が加わると、電子およびホールがpn接合を
越えて注入され、電流が流れる。ところが図2(b)の
本発明の構造では中間に歪Inx Ga1 - x As/In
P歪超格子が入るので、Inx Ga1 - x As/InP
ヘテロ界面でキャリヤの流れがある程度防げられる。従
って従来構造に比べて電気抵抗が大きくなり、リーク電
流を低減することが可能となる。
FIG. 2 is a diagram for explaining the principle of the present invention, and schematically shows this state. Figure 2 (a)
In the conventional structure, when a forward voltage exceeding the diffusion potential is applied to the InP homojunction, electrons and holes are injected over the pn junction, and a current flows. However, in the structure of the present invention shown in FIG. 2B, strain In x Ga 1 -x As / In
Since a P-strained superlattice is included, In x Ga 1 -x As / InP
The flow of carriers can be prevented to some extent at the hetero interface. Therefore, the electric resistance becomes larger than that of the conventional structure, and the leak current can be reduced.

【0010】AlGaAs/GaAs系や他の材料にお
いても原理は同じである。
The principle is the same for the AlGaAs / GaAs system and other materials.

【0011】[0011]

【実施例】次に本発明について図面を参照して説明す
る。図1は本発明の一実施例のInGaAsP/InP
系半導体レーザの断面を示す図である。歪超格子構造の
部分を部分拡大した図もあわせて示した。この素子の作
製に当たっては、まずn−InP基板上に約1μm厚の
n−InPクラッド層16,0.15μm厚のn−In
0 . 7 6 Ga0 . 2 4 As0 . 5 5 P0 . 4 5 活性層1
4,約1μm厚のp−InPクラッド層12を順次結晶
成長し、DHウエハを作製する。次にSiO2 マスクを
用いて幅1.5μm,高さ1.5μmのリッジ状に加工
し、MOVPE法により30オングストローム(A)厚
のIn0 . 8 Ga0 . 2 As17,100A厚のInP
18を交互に5層成長し歪超格子層15を形成した後、
引き続いて0.8μm厚のp−InP12,0.7μm
厚のn−InP13を順次成長する。フッ酸によりSi
O2 マスクを除去した後、この上に1μm厚のp−In
P12,0.5μm厚のp+ −InGaAs11を成長
する。最後に基板を約150μmの厚さまで研磨した
後、p側およびn側に電極を形成する。このようにして
作製した本発明の電流ブロック構造を有する半導体レー
ザを、共振器長300μmのサイズに切り出し、シリコ
ン・ヒートシンク上にマウントした後電流−光出力特性
を評価した。
The present invention will be described below with reference to the drawings. FIG. 1 shows an InGaAsP / InP according to an embodiment of the present invention.
It is a figure which shows the cross section of a semiconductor laser. A partially enlarged view of the strained superlattice structure is also shown. In manufacturing this element, first, an n-InP clad layer 16 having a thickness of about 1 μm and an n-In layer having a thickness of 0.15 μm were formed on an n-InP substrate.
0. 7 6 Ga 0. 2 4 As 0. 5 5 P 0. 4 5 active layer 1
4, p-InP clad layer 12 having a thickness of about 1 μm is sequentially crystal-grown to produce a DH wafer. Then SiO 2 width 1.5 [mu] m using a mask, processed into a ridge-like height 1.5 [mu] m, an In 0 of 30 angstroms (A) thick by MOVPE. 8 Ga 0. 2 As17,100A thick InP
After alternately growing 5 layers of 18 to form the strained superlattice layer 15,
Subsequently, 0.8 μm thick p-InP12, 0.7 μm
The thick n-InP 13 is grown sequentially. Si with hydrofluoric acid
After removing the O 2 mask, a 1 μm thick p-In layer is formed on the O 2 mask.
P12, 0.5 μm thick p + -InGaAs11 is grown. Finally, after polishing the substrate to a thickness of about 150 μm, electrodes are formed on the p-side and the n-side. The semiconductor laser having the current block structure of the present invention thus manufactured was cut into a size having a cavity length of 300 μm, mounted on a silicon heat sink, and evaluated for current-optical output characteristics.

【0012】試作した素子は1.3μm帯で発振し、8
5℃,5mWでの電流値は平均40mA,最小35mA
と良好で、従来構造のベストな値を上回る結果が得られ
ている。また最大光出力は両端面へき開で150mW、
片端面に高反射コーティングを施すことにより300m
Wが得られており、従来構造に比べて改善されている。
The prototype device oscillates in the 1.3 μm band,
Current value at 5 ° C, 5mW is 40mA on average, 35mA minimum
The result is excellent and exceeds the best value of the conventional structure. Also, the maximum light output is 150 mW when cleaved on both ends,
300m by applying a highly reflective coating on one end surface
W is obtained, which is an improvement over the conventional structure.

【0013】図3は本発明の半導体レーザの第2の実施
例を説明するための図であり、図1とは異なる構造の半
導体レーザを示した。InP半導体基板上にn−InP
クラッド層36、n−In0 . 8 Ga0 . 2 As/In
P歪超格子層35、p−InP32、n−InP33を
順次結晶成長する。フォトリソグラフィ法によりマスク
を形成し、エッチングによりストライプ状のV字型また
は逆台形の溝を形成する。マスクを除去したあと、その
溝の中にn−InP、n−InGaAsP活性層34、
p−InPを順次形成し、さらにP−InGaAsコン
タクト層31を成長し、図3の半導体構造が得られる。
この素子においても従来より優れた低しきい値かつ高温
特性が得られた。
FIG. 3 is a view for explaining a second embodiment of the semiconductor laser of the present invention, and shows a semiconductor laser having a structure different from that of FIG. N-InP on InP semiconductor substrate
Cladding layer 36, n-In 0. 8 Ga 0. 2 As / In
The P-strained superlattice layer 35, p-InP32, and n-InP33 are sequentially crystal-grown. A mask is formed by photolithography, and stripe-shaped V-shaped or inverted trapezoidal grooves are formed by etching. After removing the mask, the n-InP, n-InGaAsP active layer 34,
By sequentially forming p-InP and growing the P-InGaAs contact layer 31, the semiconductor structure shown in FIG. 3 is obtained.
Also in this device, excellent low threshold and high temperature characteristics were obtained.

【0014】本発明は他の構造の半導体レーザにも応用
できる。また電流ブロック構造の超格子構造は他の材料
でもよい。例えばInGaAsP/InP系の半導体レ
ーザでは歪超格子構造の井戸層としてInGaAsの他
InAs,InSb、InGaSbおよびこれらの混晶
を用いることができる。バリア層としてはAlP、Ga
P,AlAs,GaAs,AlSb,InPおよびこれ
らの混晶を用いることができる。
The present invention can be applied to semiconductor lasers having other structures. Further, other materials may be used for the superlattice structure of the current block structure. For example, in an InGaAsP / InP-based semiconductor laser, InAs, InSb, InGaSb, or a mixed crystal of these can be used as the well layer of the strained superlattice structure in addition to InGaAs. AlP, Ga as the barrier layer
P, AlAs, GaAs, AlSb, InP and mixed crystals thereof can be used.

【0015】AlGaAs/GaAs系のレーザではI
nGaAs/AlGaAs歪超格子構造を用いることが
できる。他にも井戸層としてInAs,GaAs,In
Sb,GaSb及びそれらの混晶用いることができる。
バリア層としてAlP,GaP,AlAs及びそれらの
混晶を用いることができる。
In the AlGaAs / GaAs laser, I
An nGaAs / AlGaAs strained superlattice structure can be used. In addition, InAs, GaAs, In as well layers
Sb, GaSb and mixed crystals thereof can be used.
AlP, GaP, AlAs and mixed crystals thereof can be used as the barrier layer.

【0016】その他AlGaInP/GaAs、GaI
nP/GaAs系等III−V族材料の半導体レーザに
適用することができる。
Others AlGaInP / GaAs, GaI
It can be applied to a semiconductor laser of III-V group material such as nP / GaAs system.

【0017】[0017]

【発明の効果】本発明の電流ブロック構造を有する半導
体レーザは、低しきい値、高温特性に優れており、1.
3μm帯加入者用のホスタイル仕様としてばかりでな
く、リーク電流が抑制されているので高出力動作も可能
であり、1.48μm帯ファイバー・アンプ励起用ある
いは1.55μm帯OTDR用の高出力の半導体レーザ
にも応用できる。また、幹線系用のDFBレーザや半導
体光変調器等に用いても良い結果が期待できる。
The semiconductor laser having the current block structure of the present invention is excellent in low threshold and high temperature characteristics.
Not only as a hostile specification for 3 μm band subscribers, but also high output operation is possible because the leak current is suppressed. High output for 1.48 μm band fiber amplifier excitation or 1.55 μm band OTDR It can also be applied to semiconductor lasers. Also, good results can be expected when used in a DFB laser for a main line system, a semiconductor optical modulator, or the like.

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

【図1】本発明の第1の実施例の半導体レーザを説明す
るための図である。
FIG. 1 is a diagram for explaining a semiconductor laser according to a first embodiment of the present invention.

【図2】本発明の原理を説明するための図である。FIG. 2 is a diagram for explaining the principle of the present invention.

【図3】本発明の第2の実施例の半導体レーザを説明す
るための図である。
FIG. 3 is a diagram for explaining a semiconductor laser according to a second embodiment of the present invention.

【符号の説明】[Explanation of symbols]

11、31 p+ −InGaAs 12、32 p−InP 13、33 n−InP 14、34 n−InGaAsP活性層 15、35 n−InGaAs/InP歪超格子層 16、36 n−InP 17 n−In0 . 8 Ga0 . 2 As 18 n−InP11, 31 p + -InGaAs 12, 32 p-InP 13, 33 n-InP 14, 34 n-InGaAsP active layer 15, 35 n-InGaAs / InP strained superlattice layer 16, 36 n-InP 17 n-In 0 . 8 Ga 0. 2 As 18 n-InP

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 電流ブロック構造を有する半導体レーザ
であって、基板側クラッド層と活性層以外の部分が接す
るpn接合界面の全部あるいは一部に圧縮歪の歪超格子
構造を有する電流ブロック構造を備えることを特徴とす
る半導体レーザ。
1. A semiconductor laser having a current block structure, wherein a current block structure having a strained superlattice structure of compressive strain is formed on all or part of a pn junction interface where the substrate-side cladding layer and a portion other than the active layer are in contact with each other. A semiconductor laser comprising.
【請求項2】 電流ブロック構造を有するInGaAs
P/InP系半導体レーザにおいて、基板側クラッド層
と活性層以外の部分が接するpn接合界面の全部あるい
は一部分に、Inの組成xが0.53よりも大きいIn
x Ga1 - x AsとInPを交互に積層させた歪超格子
構造を有する電流ブロック層を備えることを特徴とする
半導体レーザ。
2. InGaAs having a current block structure
In a P / InP-based semiconductor laser, the In composition x is larger than 0.53 in all or part of the pn junction interface where the substrate-side cladding layer and the portion other than the active layer are in contact with each other.
A semiconductor laser comprising a current blocking layer having a strained superlattice structure in which x Ga 1 -x As and InP are alternately laminated.
【請求項3】 電流ブロック構造を有するAlGaAs
/GaAs系半導体レーザにおいて、基板側クラッド層
と活性層以外の部分が接するpn接合界面の全部あるい
は一部分に、InGaAsとAlGaAsを交互に積層
させた歪超格子構造を有する電流ブロック層を備えるこ
とを特徴とする半導体レーザ。
3. AlGaAs having a current block structure
In a / GaAs semiconductor laser, a current blocking layer having a strained superlattice structure in which InGaAs and AlGaAs are alternately laminated is provided at all or a part of a pn junction interface where the substrate-side cladding layer and a portion other than the active layer are in contact with each other. Characteristic semiconductor laser.
JP19631891A 1991-08-06 1991-08-06 Semiconductor laser Pending JPH0541559A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19631891A JPH0541559A (en) 1991-08-06 1991-08-06 Semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19631891A JPH0541559A (en) 1991-08-06 1991-08-06 Semiconductor laser

Publications (1)

Publication Number Publication Date
JPH0541559A true JPH0541559A (en) 1993-02-19

Family

ID=16355825

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19631891A Pending JPH0541559A (en) 1991-08-06 1991-08-06 Semiconductor laser

Country Status (1)

Country Link
JP (1) JPH0541559A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01302791A (en) * 1988-02-02 1989-12-06 Nec Corp Buried structure semiconductor laser
JPH03174792A (en) * 1989-09-04 1991-07-29 Hitachi Ltd Semiconductor laser device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01302791A (en) * 1988-02-02 1989-12-06 Nec Corp Buried structure semiconductor laser
JPH03174792A (en) * 1989-09-04 1991-07-29 Hitachi Ltd Semiconductor laser device

Similar Documents

Publication Publication Date Title
US20090203161A1 (en) Semiconductor laser diode with a ridge structure buried by a current blocking layer made of un-doped semiconductor grown at a low temperature and method for producing the same
US5847415A (en) Light emitting device having current blocking structure
JP4057802B2 (en) Semiconductor optical device
JPH0732285B2 (en) Semiconductor laser device
JP3024611B2 (en) Semiconductor laser and method of manufacturing the same
JP2882335B2 (en) Optical semiconductor device and method for manufacturing the same
JPH05102600A (en) Semiconductor laser
JPS6243357B2 (en)
JP2697615B2 (en) Multiple quantum well semiconductor laser
KR20010020581A (en) A laser diode of the type having a buried heterostructure
JP2812273B2 (en) Semiconductor laser
JP3488137B2 (en) Optical semiconductor device and method of manufacturing the same
US20040136427A1 (en) Semiconductor optical device
JP3241002B2 (en) Manufacturing method of semiconductor laser
US7924896B2 (en) Optical semiconductor device
JP2550714B2 (en) High-resistance semiconductor layer embedded semiconductor laser
JP3403915B2 (en) Semiconductor laser
JP2550729B2 (en) Semiconductor laser
JP2002026455A (en) Semiconductor optical element and method of manufacturing the same
JPH03133189A (en) Highly resistive semiconductor layer buried type semiconductor laser
JP2793464B2 (en) Semiconductor laser
JP2004111743A (en) Semiconductor optical device
JP2743769B2 (en) Semiconductor laser and manufacturing method thereof
JP2001345518A (en) Semiconductor laser element
JP3638305B2 (en) Quantum well crystal, semiconductor laser and manufacturing method thereof

Legal Events

Date Code Title Description
A02 Decision of refusal

Free format text: JAPANESE INTERMEDIATE CODE: A02

Effective date: 19980609