JPS6320395B2 - - Google Patents

Info

Publication number
JPS6320395B2
JPS6320395B2 JP16302181A JP16302181A JPS6320395B2 JP S6320395 B2 JPS6320395 B2 JP S6320395B2 JP 16302181 A JP16302181 A JP 16302181A JP 16302181 A JP16302181 A JP 16302181A JP S6320395 B2 JPS6320395 B2 JP S6320395B2
Authority
JP
Japan
Prior art keywords
layer
striped
protrusions
stripe
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.)
Expired
Application number
JP16302181A
Other languages
Japanese (ja)
Other versions
JPS5864087A (en
Inventor
Mitsunori Sugimoto
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
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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP16302181A priority Critical patent/JPS5864087A/en
Publication of JPS5864087A publication Critical patent/JPS5864087A/en
Publication of JPS6320395B2 publication Critical patent/JPS6320395B2/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

Landscapes

  • Physics & Mathematics (AREA)
  • Geometry (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Optics & Photonics (AREA)
  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 本発明は、半導体レーザに関し特に埋め込み構
造半導体レーザの改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to semiconductor lasers, and more particularly to improvements in 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
る従来の電流狭窄型メサ基板埋め込み構造レーザ
Current Confinement Mesa Substrate Buried
Heterostructure Laser Diode略してCCM−
LD;参考文献、電子通信学会光量子エレクトロ
ニクス研究会資OQE80−117)を示す。CCM−
LDはn・InP基板1上に形成されたストライプ
状突起2上に活性層4a(InGaAsP、λg〜1.3μ
m)、ストライプ状突起2の両側に活性層4b
(InGaAsP、λg〜1.3μm)が途切れて形成され
ているため、活性層4aが屈折率の小さなバツフ
アー層3(n・InP)及び第1クラツド層(p・
Inp)でまわりを囲まれた、いわゆる埋め込み構
造となつている。又、電流阻止層6(n・InP)
がストライプ状突起2上で欠損し、その両側にの
み形成されているため活性層4aに効率良く電流
が集中することができる。
Figure 1 shows a conventional current confinement type mesa substrate buried structure laser, which is a type of buried structure semiconductor laser.
Current Confinement Mesa Substrate Buried
Heterostructure Laser DiodeCCM−
LD: References, Institute of Electronics and Communication Engineers Photon Quantum Electronics Study Group materials OQE80-117) are shown. CCM−
The LD has an active layer 4a (InGaAsP, λg~1.3μ
m), active layers 4b on both sides of the striped projections 2;
(InGaAsP, λg ~ 1.3 μm) is formed with interruptions, so that the active layer 4a includes the buffer layer 3 (n.InP) with a small refractive index and the first cladding layer (p.
It has a so-called embedded structure, surrounded by Inp). Also, current blocking layer 6 (n.InP)
is missing on the striped protrusion 2 and is formed only on both sides thereof, so that current can be efficiently concentrated in the active layer 4a.

このCCM−LDの結果は、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を形成後続けて第1クラ
ツド層5及び電流阻止層6を形成する場合に、活
性層4aがストライプ状突起2上にあるため、そ
の他の領域よりも突き出ており、液相成長用カー
ボン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
点があつた。この様な機械的な損傷を受けた結晶
から製作したCCM−LDは通電時の劣化率が大き
く、寿命が短かつた。
This CCM-LD result is formed using the sliding method, which is a type of liquid phase growth method. In this liquid phase growth, when forming the first cladding layer 5 and the current blocking layer 6 after forming the active layers 4a and 4b, since the active layer 4a is on the striped protrusion 2, it protrudes more than other regions. It has the disadvantage that it easily comes into contact with the carbon boat for liquid phase growth, and as a result, it is susceptible to mechanical damage, resulting in crystal breakage and the generation of dislocations. CCM-LDs made from such mechanically damaged crystals had a high rate of deterioration when energized and had a short lifespan.

本発明の目的ろ、活性層が上述した機械的損傷
を受け難く、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-mentioned mechanical damage and has a long life.

本発明によれば、少なくとも3つの互いに平行
なストライプ状突起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、ストライプ
状突起の少なくとも1つに欠損部を有する電流阻
止層とを具備したことを特徴とする半導体レーザ
が得られる。
According to the present invention, a semiconductor substrate having at least three mutually parallel stripe-like protrusions, an active layer formed on the semiconductor substrate, and a current blocking layer having a defect in at least one of the stripe-like protrusions are provided. A semiconductor laser characterized by the following features is obtained.

以下図面を参照して本発明を詳しく説明する。
第2図は本発明の一実施例の断面図である。図中
11はn・InP基板、12,13,14はストラ
イプ状突起、15は平担部、16はバツフアー層
(n・InP、厚さ〜0.5μm)、17a,b,c,d
は、活性層(InGaAsP、λg〜1.3μm、厚さ〜
0.2μm)、18は第1クラツド層(P・InP、厚さ
0.7μm)、19は電流阻止層(n・InP、厚さ〜
0.7μm)、20は第2クラツド層(p・InP、厚さ
2〜5μm)、21はキヤツプ層(p・InGaAsP、
λg〜1.3μm、厚さ〜1μm)、22はp電極、2
3はn電極である。本実施例の埋め込み構造レー
ザの主たる発光領域は、ストライプ状突起12上
に形成された、活性層17aである。段差のとこ
ろで活性層17が段切れを伴なつて形成されるた
め、活性層17a,17b,17c,17dはそ
れぞれ不連続となる。又、電流阻止層は、活性層
17a上で欠損しているため電流は集中的に、活
性層17aに注入される。ストライプ状突起12
の上辺の幅は約2μm、高さは約3μmストライプ
上突起12と13の間隔およびストライプ状突起
12と14の間隔は5〜20μm、ストライプ状突
起13及び14の上辺の幅は20〜50μm、高さは
約3μm、平担部15の幅は100〜150μmである。
The present invention will be described in detail below with reference to the drawings.
FIG. 2 is a sectional view of one embodiment of the present invention. In the figure, 11 is an n-InP substrate, 12, 13, 14 are striped projections, 15 is a flat part, 16 is a buffer layer (n-InP, thickness ~0.5 μm), 17a, b, c, d
is the active layer (InGaAsP, λg ~ 1.3 μm, thickness ~
0.2μm), 18 is the first cladding layer (P/InP, thickness
0.7 μm), 19 is a current blocking layer (n InP, thickness ~
0.7 μm), 20 is the second cladding layer (p-InP, thickness 2-5 μm), 21 is the cap layer (p-InGaAsP,
λg ~ 1.3 μm, thickness ~ 1 μm), 22 is the p electrode, 2
3 is an n-electrode. The main light emitting region of the buried structure laser of this embodiment is the active layer 17a formed on the striped protrusion 12. Since the active layer 17 is formed with a step break at the step, the active layers 17a, 17b, 17c, and 17d are each discontinuous. Furthermore, since the current blocking layer is missing on the active layer 17a, current is intensively injected into the active layer 17a. Striped projection 12
The width of the upper side is about 2 μm, the height is about 3 μm, the interval between the striped upper protrusions 12 and 13 and the interval between the striped protrusions 12 and 14 is 5 to 20 μm, the width of the upper side of the striped protrusions 13 and 14 is 20 to 50 μm, The height is about 3 μm, and the width of the flat portion 15 is 100 to 150 μm.

さて、従来のCCM−LDは発光領域が他の領域
よりも突き出ていため、結晶成長中に機械的損傷
を受けやすい欠点があつた。しかし本実施例の半
導体レーザでは、活性層17aとその両側の活性
層17b及び17eの3つの活性層領域が平担部
15よりも突き出ているため、主たる発光領域で
ある活性層17aが液相成長用カーボンボートと
の接触により機械的損傷を受ける確率が大幅に減
少した。
Now, in conventional CCM-LDs, the light-emitting region protrudes more than other regions, which has the disadvantage of being susceptible to mechanical damage during crystal growth. However, in the semiconductor laser of this embodiment, since the three active layer regions of the active layer 17a and the active layers 17b and 17e on both sides thereof protrude beyond the flat portion 15, the active layer 17a which is the main light emitting region is in the liquid phase. The probability of mechanical damage due to contact with the growth carbon boat was significantly reduced.

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。まず主面が(100)面である
n・InP基板11上にホトエツチング技術によ
り、3つのストライプ状突起12,13,14を
結晶方位<011>方向に沿つて形成する。次に液
相成長法の一種のスライド法により、バツフアー
層16、活性層17a,b,c,d、第1クラツ
ド層18、電流阻止層19、第2クラツド層2
0、キヤツプ層21を順次連続成長する。このと
き液相成長用溶液の過冷却度を制御することによ
り、バツフアー層15及び第1クラツド層18は
ストライプ状突起12の上部に成長するが、電流
阻止層19はストライプ状突起12上で欠損して
成長する。又、電流阻止層19は、ストライプ状
突起13及び14上には、その幅がストライプ状
突起12よりも広いため成長する。又、
InGaAsPからなる活性層17a,b,c,dは
ストライプ状突起12の側面に成長せず段切れを
伴なつて形成される。この様に得られたレーザ結
晶を厚さ約100μm程度に研摩した後、キヤツプ
層21上にp電極22又n・InP基板11にn電
極23を真空蒸着法にて形成した後、熱処理を行
ない電極をオーミツク接触にする。その後共振器
長200〜300μm程度に切り出して埋め込み構造半
導体レーザが得られる。
The manufacturing method of the buried structure semiconductor laser of this example will be briefly described. First, three stripe-shaped protrusions 12, 13, and 14 are formed along the <011> crystal orientation on an n.InP substrate 11 whose main surface is the (100) plane by photoetching. Next, by a kind of sliding method of liquid phase growth method, the buffer layer 16, the active layers 17a, b, c, d, the first cladding layer 18, the current blocking layer 19, and the second cladding layer 2 are formed.
0, the cap layer 21 is successively grown. At this time, by controlling the degree of supercooling of the liquid phase growth solution, the buffer layer 15 and the first cladding layer 18 grow on the striped projections 12, but the current blocking layer 19 is cut off on the striped projections 12. and grow. Further, the current blocking layer 19 grows on the striped projections 13 and 14 because its width is wider than that of the striped projection 12. or,
The active layers 17a, b, c, and d made of InGaAsP do not grow on the side surfaces of the striped projections 12, but are formed with steps. After polishing the laser crystal thus obtained to a thickness of about 100 μm, a p-electrode 22 is formed on the cap layer 21 and an n-electrode 23 is formed on the n-InP substrate 11 by vacuum evaporation, followed by heat treatment. Make ohmic contact between the electrodes. Thereafter, a buried structure semiconductor laser is obtained by cutting out a cavity with a length of about 200 to 300 μm.

本実施例では、電流阻止層19を結晶成長中に
ストライプ状突起12上で欠損して成長し、電流
通路を形成したが、この方法のみならず電流阻止
層19をストライプ状突起12上にも液相成長で
形成した後、ストライプ状突起12付近だけ選択
的にp型不純物のZnあるいはCd等を拡散あるい
はイオン注入等の方法で導入し、電流阻止層19
の導電型をn型からp型へ反転して電流通路を形
成しても良い。又、本実施例では、ストライプ状
突起が、主発光領域のストライプ状突起12とそ
の両側のストライプ状突起13,14の3つを備
えていたが、これに限らずストライプ状突起1
3,14と同様なものが3つ以上備えていても良
い。
In this embodiment, the current blocking layer 19 is grown by cutting it on the striped projections 12 during crystal growth to form a current path. After forming the current blocking layer 19 by liquid phase growth, a p-type impurity such as Zn or Cd is selectively introduced into the vicinity of the striped protrusions 12 by diffusion or ion implantation.
A current path may be formed by inverting the conductivity type from n type to p type. Further, in this embodiment, the stripe-like protrusions include three stripe-like protrusions, the stripe-like protrusion 12 in the main light emitting region and the stripe-like protrusions 13 and 14 on both sides of the stripe-like protrusion 12, but the stripe-like protrusion 1 is not limited to this.
Three or more items similar to 3 and 14 may be provided.

最後に本発明の有する特徴を要約すれば活性層
が結晶成長中に機械的損傷を受け難く、従つて長
寿命の埋め込み構造半導体レーザを歩留まり良く
得られることにある。
Finally, to summarize the features of the present invention, the active layer is less susceptible to mechanical damage during crystal growth, and therefore a long-life buried structure semiconductor laser can be obtained with a high yield.

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

第1図は電流狭容型メサ基板埋め込み構造レー
ザ(CCM−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造半導体レー
ザの断面図である。 図中、1……n・InP基板、2……ストライプ
状突起、3……バツフアー層、4a,4b……活
性層、5……第1クラツド層、6……電流阻止
層、7……第2クラツド層、8……キヤツプ層、
9……p電極、10……n電極、11……n・
InP基板、12,13,14……ストライプ状突
起、15……平担部、16……バツフアー層、1
7a,17b,17c,17dは活性層、18…
…第1クラツド層、19……電流阻止層、20…
…第2クラツド層、21……キヤツプ層、22…
…p電極、23……n電極、である。
FIG. 1 is a cross-sectional view of a current constriction type mesa substrate embedded laser (CCM-LD). FIG. 2 is a sectional view of a buried structure semiconductor laser according to an embodiment of the present invention. In the figure, 1... n.InP substrate, 2... striped protrusion, 3... buffer layer, 4a, 4b... active layer, 5... first cladding layer, 6... current blocking layer, 7... 2nd cladding layer, 8...cap layer,
9...p electrode, 10...n electrode, 11...n・
InP substrate, 12, 13, 14...stripe-like projections, 15...flat portion, 16...buffer layer, 1
7a, 17b, 17c, 17d are active layers, 18...
...First cladding layer, 19... Current blocking layer, 20...
...Second cladding layer, 21...Cap layer, 22...
. . . p electrode, 23 . . . n electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 互いに平行な第1及び第2のストライプ状突
起と、前記第1及び第2のストライプ状突起の間
にこれら突起と互いに平行で且つ前記第1及び第
2のストライプ状突起の幅よりも狭い幅の第3の
ストライプ状突起とが形成された半導体基板と、
前記第1乃至第3のストライプ状突起上とストラ
イプ状突起の谷との間で途切れて前記半導体基板
上に形成された活性層と、前記活性層をおおうク
ラツド層と、前記クラツド層上に前記第3のスト
ライプ状突起上に形成された前記クラツド層上を
除いて形成した電流阻止層とを有し、前記第3の
ストライプ状突起上の活性層に電流を注入して発
光させることを特徴とする半導体レーザ。
1. first and second striped protrusions parallel to each other, and a space between the first and second striped protrusions that is parallel to these protrusions and narrower than the width of the first and second striped protrusions. a semiconductor substrate on which a third stripe-shaped projection having a width is formed;
an active layer formed on the semiconductor substrate discontinuously between the first to third striped protrusions and valleys of the striped protrusions; a cladding layer covering the active layer; and a cladding layer disposed on the cladding layer. and a current blocking layer formed on the third stripe-shaped protrusion except for the cladding layer, and a current is injected into the active layer on the third stripe-shaped protrusion to cause the active layer to emit light. semiconductor laser.
JP16302181A 1981-10-13 1981-10-13 Semiconductor laser Granted JPS5864087A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16302181A JPS5864087A (en) 1981-10-13 1981-10-13 Semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16302181A JPS5864087A (en) 1981-10-13 1981-10-13 Semiconductor laser

Publications (2)

Publication Number Publication Date
JPS5864087A JPS5864087A (en) 1983-04-16
JPS6320395B2 true JPS6320395B2 (en) 1988-04-27

Family

ID=15765681

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16302181A Granted JPS5864087A (en) 1981-10-13 1981-10-13 Semiconductor laser

Country Status (1)

Country Link
JP (1) JPS5864087A (en)

Also Published As

Publication number Publication date
JPS5864087A (en) 1983-04-16

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