JPS5864084A - Semiconductor laser - Google Patents

Semiconductor laser

Info

Publication number
JPS5864084A
JPS5864084A JP16301881A JP16301881A JPS5864084A JP S5864084 A JPS5864084 A JP S5864084A JP 16301881 A JP16301881 A JP 16301881A JP 16301881 A JP16301881 A JP 16301881A JP S5864084 A JPS5864084 A JP S5864084A
Authority
JP
Japan
Prior art keywords
layer
projection
active
current blocking
active 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.)
Granted
Application number
JP16301881A
Other languages
Japanese (ja)
Other versions
JPS622717B2 (en
Inventor
Mitsunori Sugimoto
杉本 満則
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
Nippon Electric Co Ltd
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, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP16301881A priority Critical patent/JPS5864084A/en
Publication of JPS5864084A publication Critical patent/JPS5864084A/en
Publication of JPS622717B2 publication Critical patent/JPS622717B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
    • H01S5/22Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a ridge or stripe structure
    • H01S5/227Buried mesa structure ; Striped active layer
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES 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
    • H01S5/00Semiconductor lasers
    • H01S5/20Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers
    • H01S5/22Structure or shape of the semiconductor body to guide the optical wave ; Confining structures perpendicular to the optical axis, e.g. index or gain guiding, stripe geometry, broad area lasers, gain tailoring, transverse or lateral reflectors, special cladding structures, MQW barrier reflection layers having a ridge or stripe structure
    • H01S5/227Buried mesa structure ; Striped active layer
    • H01S5/2275Buried mesa structure ; Striped active layer mesa created by etching

Abstract

PURPOSE:To allow a semiconductor laser to be hardly affected by mechanical damage and to have long lifetime by providing a semiconductor substrate having two parallel grooves, an active layer formed on the substrate and a current blocking layer having a defect at the projection between the two grooves in the improvement of the buried type laser and having a main light emitting region of part of the active layer formed on the projection. CONSTITUTION:Two parallel grooves 12 are formed on an n-IP substrate 11 having a main surface in (100) plane along crystal azimuth (011). A buffer layer 15, active layers 16a, 16b, 16c, the first clad layer 17, a current blocking layer 18, the second clad layer 19 and a cap layer 20 are sequentially grown by a liquid growing method. The layer 18 is grown with defect on the projection 12 by selecting the suitable growing condition. The layer 16 made of InGaAsP is formed with stepwise disconnection. Since the current blocking layer is made defective on the layer 16a, the current is concentrically injected to the layer 16a. In addition, the layer 16a is formed substantially in the same height as the other most part of the layer 16c, the projection is hardly subjected to the mechanical damage.

Description

【発明の詳細な説明】 本発明は、半導体レーザ、特に埋め込み構造半導体レー
ザの改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in semiconductor lasers, particularly buried structure semiconductor lasers.

第1図に埋め込み構造半導体レーザの一種である、従来
の電流狭窄製メサ基板埋め込み構造レーザ(Curre
nt Confcnement jdesa−5ubs
tvateBuried Heterc−8truct
uve Lamer Diode略してCCM−LD)
の断面を示す。CCM−LDは電子通偽学会光量子エレ
クトロニクス研究会資料0QE80−117で示される
ようにn、 Inpn板基板l上成された突起部2上に
活性層(InG、aAiP。
Figure 1 shows a conventional current confinement mesa substrate buried structure laser (Curre), which is a type of buried structure semiconductor laser.
nt Confcnement jdesa-5ubs
tvateBuried Heterc-8truct
uve Lamer Diode (abbreviated as CCM-LD)
A cross section of is shown. The CCM-LD has an active layer (InG, aAiP) formed on a protrusion 2 formed on an Inpn plate substrate l, as shown in Material 0QE80-117 of the Photon Quantum Electronics Study Group of the Japan Society of Electronic Communications.

λg〜1.3μm)4a、突起部2の両側に活性層(I
 n Ga A s P *λg〜1.3,1m )4
 bが途切れて形成されている丸め、活性層4aが屈折
率の小さなバッフ7一層(n−InP)3及び第1クラ
ッド層(p−InP) 5でまわシを囲まれたいわゆる
埋め込み構造となっている。又、電流阻止層(H−(n
P)6が央起112上で欠損し、七つ両−にのみ形成さ
れているため、活性層4aに効率良く電流が集中する事
が出来る。このCCM−LDの結晶は、液相成長法の一
種であるスライド法で形成される。この液相成長におい
て活性層4a及び4bを形成した後、第1クラッド層5
、電流阻止層6を形成する場合に、活性層4aが、突起
部2上にあるため、その他の領域よりも突き出ており、
液相成長用ボートに接触しやすくこのため機械的損傷を
受けて、結晶の破損、転位の発生を招きやすい欠点があ
った。
λg ~ 1.3 μm) 4a, active layers (I
n Ga As P *λg~1.3,1m)4
The active layer 4a has a so-called buried structure in which the active layer 4a is surrounded by a buffer layer 7 (n-InP) 3 and a first cladding layer (p-InP) 5 having a small refractive index. ing. In addition, a current blocking layer (H-(n
Since P) 6 is missing on the central origin 112 and is formed only on both sides, current can be efficiently concentrated in the active layer 4a. This CCM-LD crystal is formed by a sliding method, which is a type of liquid phase growth method. After forming the active layers 4a and 4b in this liquid phase growth, the first cladding layer 5
, when forming the current blocking layer 6, since the active layer 4a is on the protrusion 2, it protrudes from other regions,
It has the disadvantage that it easily comes into contact with the liquid-phase growth boat and is therefore susceptible to mechanical damage, resulting in crystal breakage and dislocation generation.

この様な機械的な損傷を受けた結晶から製作し九〇〇M
−LDは、通電時の劣化率が大きく、寿命が短かい欠点
を有していた。
Made from crystals that have undergone such mechanical damage, it costs 900M.
-LDs had the drawbacks of high deterioration rate when energized and short lifespan.

本発明の目的は、活性層が上述した橡な機械的損傷を受
は難く、長寿命の半導体レーザを提供することにある。
An object of the present invention is to provide a semiconductor laser whose active layer is less susceptible to the above-described mechanical damage and has a long life.

本発明によれば互いに千行碌2つの溝を有する半導体基
板と、この半導体基板上に形成された活性層と、上記2
つの溝の間の突起部に欠損部を有する電流阻止層を具備
し、突起部上に形成された活性層の一領域を主たる発光
領域としたことを特徴とした半導体レーザが得られる。
According to the present invention, there is provided a semiconductor substrate having two grooves each having a thousand rows, an active layer formed on the semiconductor substrate, and the above two grooves.
There is obtained a semiconductor laser characterized in that the protrusion between the two grooves is provided with a current blocking layer having a defect, and a region of the active layer formed on the protrusion is used as a main light emitting region.

以下図面を参照して本発明の詳細な説明する。The present invention will be described in detail below with reference to the drawings.

第2図は、本発明の一実施例の断面図である。FIG. 2 is a cross-sectional view of one embodiment of the present invention.

図中11は、互いに平行な$13が形成されたn−In
P基板、15はバッファ一層(n−InP、Jlす〜0
.5μm)、16L 16b、16Cは活性層(InG
mAsP、λg〜1.3μm、犀さ〜0.2μm)、1
7は第1クラット層(p−InP、犀さ〜0.7μm)
 1 Bは電流阻止層(n−Inp、厚さ〜0.7μm
)、19は第2クラット層(p−InP、厚さ2〜5μ
m)、20はキャップ層(pI n G a A s 
P 、λg〜1.3 μm +厚さ〜1.am)、21
はPt極、22はn電極である。
In the figure, 11 is an n-In in which $13 parallel to each other is formed.
P substrate, 15 is a buffer single layer (n-InP, Jl~0
.. 5 μm), 16L 16b, 16C are active layers (InG
mAsP, λg ~ 1.3 μm, rhinoceros size ~ 0.2 μm), 1
7 is the first crat layer (p-InP, thickness ~0.7 μm)
1 B is a current blocking layer (n-Inp, thickness ~0.7 μm
), 19 is the second crat layer (p-InP, thickness 2-5μ
m), 20 is a cap layer (pI n Ga As
P, λg ~ 1.3 μm + thickness ~ 1. am), 21
is a Pt electrode, and 22 is an n electrode.

本実施例の埋め込み構造レーザの、主たる活性領域は、
突起部12上に形成された活性層16aである段差のと
ころで段切れを伴なって活性層が形成されるため溝13
の底部に形成された活性層16bは活性層16a及び活
性層16Cとは不連続となる。又、電流阻止層は、活性
層16a上で欠損している丸め電流線集中的に活性層1
6aに注入される。突起部12の上辺の輪は約2μm1
溝13の幅は5〜10μm深さは約3μmで、平担部1
4の幅は100〜150μmである。
The main active region of the buried structure laser of this example is:
Since the active layer is formed with a step break at the step of the active layer 16a formed on the protrusion 12, the groove 13
The active layer 16b formed at the bottom of the active layer 16b is discontinuous with the active layer 16a and the active layer 16C. Further, the current blocking layer concentrates the rounded current lines missing on the active layer 16a.
6a. The ring on the upper side of the protrusion 12 is approximately 2 μm1
The groove 13 has a width of 5 to 10 μm and a depth of about 3 μm, and the flat portion 1
4 has a width of 100 to 150 μm.

さて、第2図において、主たる活性領域である活性層1
6.11は、平担部14上にある活性層16Cよpも突
き出ていないことがわかる。すなわち、活性層16aは
突起部12上に形成されているが、平担部14上の活性
層16Cと同じ高さに位置しておシ突き出てはいない。
Now, in FIG. 2, active layer 1 which is the main active region
6.11 shows that even the active layer 16C on the flat portion 14 does not protrude. That is, although the active layer 16a is formed on the protruding portion 12, it is located at the same height as the active layer 16C on the flat portion 14 and does not protrude.

このことから、本実施例の埋め込み構造半導体レーザの
結晶を、液相成長法のm−のスライド法にて形成する場
合に、活性層16aは他の大部分の活性層16Cと同じ
高さにある丸め、従来の様に突起部がボートに接触して
機械的損傷を受けることは、t3とんどなくなった。
From this, when the crystal of the buried structure semiconductor laser of this example is formed by the m- slide method of liquid phase growth, the active layer 16a is at the same height as most of the other active layers 16C. In some cases, the mechanical damage caused by the protrusion contacting the boat, which was the case in the past, has almost completely disappeared.

本実施例の埋め込み構造半導体レーザの製作法を簡単に
述べるII tず主面が(100)面であるn−InP
基板11上にホトエツチング技術により、互いに平行な
2つの溝12を結晶方位<011>方向に沿って形成す
る。次に液相成長法の一種のスライド法によシ、バッフ
ァ一層15、活性層16a。
Briefly describe the manufacturing method of the buried structure semiconductor laser of this example II. n-InP whose main surface is the (100) plane
Two mutually parallel grooves 12 are formed along the <011> crystal orientation on the substrate 11 by photoetching. Next, a buffer layer 15 and an active layer 16a are formed by a sliding method, which is a type of liquid phase growth method.

16b、i6c第1クラッド層17、電流阻止層18第
2クラッド層19、キャップ層20を順次連続成長する
。このと亀、過当な成長条件を選ぶことによシ、バッフ
ァ一層15及び#、lクラッド層17は突起部12上に
成長するがt流阻止層18i!突起部12上で欠損して
成長する。又、InGaAsPからなる活性層は突起部
側面に成長せず段切れを伴なって形成される。、この様
にして得られたしiザ結晶を厚さ約100μm@[に研
摩した後、キャップ層20上にPi極21又、n−In
P&板11上にn電極22を真空蒸着法にて形成した抜
熱処理を行ない電極をオーミック接触にする。その後共
振器長200〜39ppm程駄に切シ出して埋め込み構
造半導体レーザが完成する。
16b, i6c first cladding layer 17, current blocking layer 18, second cladding layer 19, and cap layer 20 are successively grown. In this case, by selecting excessive growth conditions, the buffer layer 15 and #, l cladding layer 17 grow on the protrusion 12, but the t-flow blocking layer 18i! It grows on the protrusion 12 in a defective manner. Further, the active layer made of InGaAsP does not grow on the side surface of the protrusion, but is formed with steps. After polishing the thus obtained iza crystal to a thickness of approximately 100 μm, a Pi electrode 21 and an n-In
An n-electrode 22 is formed on the P& plate 11 by vacuum evaporation, and heat removal treatment is performed to bring the electrode into ohmic contact. Thereafter, a cavity length of about 200 to 39 ppm is cut out to complete a buried structure semiconductor laser.

本実施例では、InP/InGaAsPの材料を用いた
が、本発明は他の材料、例えtd GaAs /GaA
lAs勢にも同様に適用できる。
In this example, InP/InGaAsP materials were used, but the present invention is also applicable to other materials, such as td GaAs/GaA
The same can be applied to the lAs group.

最後に本発明の有する%命を要約jれば、活性層が機械
的な損傷を結晶成長プロセス中に受は離〈従がって長寿
命の埋め込み楊造牛導体し−サを歩留tシ良く得られ不
ことにある。
Finally, to summarize the life expectancy of the present invention, the active layer does not suffer from mechanical damage during the crystal growth process, thus making it a long-life buried conductor and reducing the yield rate. It's unfortunate that it doesn't work well.

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

第1図は電流狭窄型メサ基板埋め込み構造レーザ(CC
M−LD’)の断面図である。 第2図は本発明の一実施例に係わる埋め込み構遣手導体
レーザの断面図である。 図中、1・・・・・・n、InP基板、2・・・・・・
突起部、3・・・バッファ一層4a及び4b・・・・・
・活性層、5・・・・・・第1クラッド層、6・・・・
・・電流阻止層、7・・・・・・第2クラッド層、8・
・・・・・キャップ層、9・曲・P電極、lO・・・・
・・n電極、11・・・・・・n−InP基板、12・
・・・・・突起部、13・・・・・・互いに平行な2つ
の溝、14・・・・・・平坦部、15・・・・・・はバ
ッファ一層、16!I、 16bl16C・・・・・・
活性層、17・・・・・・第゛1クラッド層、18・・
・・・・電流阻止層、19・・・・・・第2クラッド層
、20・・・・・・キャップ層、21・・・・・・p電
極、22・・・・・・n電極である。 4η /(/ 草l 図
Figure 1 shows a current confinement mesa substrate buried structure laser (CC
M-LD'). FIG. 2 is a sectional view of a buried conductor laser according to an embodiment of the present invention. In the figure, 1...n, InP substrate, 2...
Projections, 3...Buffer layer 4a and 4b...
・Active layer, 5... First cladding layer, 6...
...Current blocking layer, 7...Second cladding layer, 8.
...Cap layer, 9, curved, P electrode, lO...
...n electrode, 11...n-InP substrate, 12.
... Protrusion, 13 ... Two mutually parallel grooves, 14 ... Flat portion, 15 ... is a buffer layer, 16! I, 16bl16C...
Active layer, 17... First cladding layer, 18...
... Current blocking layer, 19 ... Second cladding layer, 20 ... Cap layer, 21 ... P electrode, 22 ... N electrode be. 4η /(/ grass l figure

Claims (2)

【特許請求の範囲】[Claims] (1)  互いに平行な2つの溝を有する半導体基板と
、骸半導体基板上に形成された活性層と、前記2つの溝
の間の突起部に欠損部を有する電流阻止層とを具備し、
前記突起部上に形成され九活性層の一領域を生える発光
領域としたことを特徴とする半導体ν−ザ。
(1) A semiconductor substrate having two grooves parallel to each other, an active layer formed on the skeleton semiconductor substrate, and a current blocking layer having a defect in a protrusion between the two grooves,
A semiconductor v-zer characterized in that a region of the nine active layers formed on the protrusion is a growing light emitting region.
(2)前記活性層が突起部の側面おいて欠損しているこ
とを特徴とする特許請求の範1181項記載の半導体レ
ーザ。
(2) The semiconductor laser according to claim 1181, characterized in that the active layer has a defect on the side surface of the protrusion.
JP16301881A 1981-10-13 1981-10-13 Semiconductor laser Granted JPS5864084A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16301881A JPS5864084A (en) 1981-10-13 1981-10-13 Semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16301881A JPS5864084A (en) 1981-10-13 1981-10-13 Semiconductor laser

Publications (2)

Publication Number Publication Date
JPS5864084A true JPS5864084A (en) 1983-04-16
JPS622717B2 JPS622717B2 (en) 1987-01-21

Family

ID=15765623

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16301881A Granted JPS5864084A (en) 1981-10-13 1981-10-13 Semiconductor laser

Country Status (1)

Country Link
JP (1) JPS5864084A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63215090A (en) * 1987-03-04 1988-09-07 Matsushita Electric Ind Co Ltd Semiconductor laser
EP0373637A2 (en) * 1988-12-15 1990-06-20 Magyar Tudomanyos Akademia Müszaki Fizikai Kutato Intezete InP/GalnAsP double heterostructure laser diode with buried active layer, and method for its production

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63215090A (en) * 1987-03-04 1988-09-07 Matsushita Electric Ind Co Ltd Semiconductor laser
EP0373637A2 (en) * 1988-12-15 1990-06-20 Magyar Tudomanyos Akademia Müszaki Fizikai Kutato Intezete InP/GalnAsP double heterostructure laser diode with buried active layer, and method for its production
JPH03136289A (en) * 1988-12-15 1991-06-11 Magyar Tudomanyos Akad Mueszaki Fiz Kutato Intezet Double heterostructure diode and its manufacture

Also Published As

Publication number Publication date
JPS622717B2 (en) 1987-01-21

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