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JPS6342876B2 - - Google Patents
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JPS6342876B2 - - Google Patents

Info

Publication number
JPS6342876B2
JPS6342876B2 JP1345282A JP1345282A JPS6342876B2 JP S6342876 B2 JPS6342876 B2 JP S6342876B2 JP 1345282 A JP1345282 A JP 1345282A JP 1345282 A JP1345282 A JP 1345282A JP S6342876 B2 JPS6342876 B2 JP S6342876B2
Authority
JP
Japan
Prior art keywords
layer
conductivity type
active layer
semiconductor
oscillation
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
JP1345282A
Other languages
Japanese (ja)
Other versions
JPS58131785A (en
Inventor
Masafumi Seki
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
NTT Inc
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp, Nippon Electric Co Ltd filed Critical Nippon Telegraph and Telephone Corp
Priority to JP1345282A priority Critical patent/JPS58131785A/en
Publication of JPS58131785A publication Critical patent/JPS58131785A/en
Publication of JPS6342876B2 publication Critical patent/JPS6342876B2/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
    • H01S5/2277Buried mesa structure ; Striped active layer mesa created by etching double channel planar buried heterostructure [DCPBH] laser

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】 本発明は埋込み型でかつ単一軸モード発振をす
る単一軸モード発振半導体レーザに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a single-axis mode oscillation semiconductor laser which is an embedded type and oscillates in a single-axis mode.

埋込み型半導体レーザは低しきい値発振等の優
れた特性を有しているが、発振軸モードが安定せ
ずまた発振波長の温度変化が大きい欠点があつ
た。この欠点を解決するために、埋込み型半導体
レーザを分布帰還型レーザとする試みが研究され
ている。従来の方法では活性層の上側ないし下側
に活性層中の発振光波長の1/2の整数倍の周期を
もつ周期構造(凹凸)を形成する方法や、活性層
の側面外側に同様の周期構造を形成する方法等が
実施されていた。前者の方法では半導体層の成長
が困難になつたり得られた半導体レーザの長寿命
化が難しいなどの問題点があつた。後者の方法で
は寿命の点で好ましいものの、活性層の側面外側
に適切な周期構造を作ることが種々の点から難し
い上に室温連続発振が困難などの問題点があつ
た。
Although buried semiconductor lasers have excellent characteristics such as low threshold oscillation, they have the disadvantage that the oscillation axis mode is not stable and the oscillation wavelength varies greatly with temperature. In order to solve this drawback, attempts are being made to convert the buried semiconductor laser into a distributed feedback laser. Conventional methods include forming a periodic structure (unevenness) on the upper or lower side of the active layer with a period that is an integral multiple of 1/2 of the oscillation light wavelength in the active layer, or forming a periodic structure (unevenness) on the outside of the side surface of the active layer. Methods for forming structures, etc. were implemented. The former method has problems such as difficulty in growing the semiconductor layer and difficulty in extending the life of the obtained semiconductor laser. Although the latter method is preferable in terms of longevity, it is difficult for various reasons to create an appropriate periodic structure on the outside of the side surfaces of the active layer, and it also has problems such as difficulty in continuous oscillation at room temperature.

本発明の目的は、これらの問題点を解決すべ
く、極めて高効率な埋込み型で単一軸モード発振
が特性を損なうことなく実現される単一軸モード
発振半導体レーザを提供することにある。
SUMMARY OF THE INVENTION In order to solve these problems, an object of the present invention is to provide an extremely highly efficient buried type single-axis mode oscillation semiconductor laser in which single-axis mode oscillation can be realized without deteriorating the characteristics.

本発明によれば、第1導電型半導体基板上に少
なくとも活性層を含む半導体層を成長させた半導
体ウエーハに、活性層より深い2本のエツチング
溝を形成してなるメサストライプの上面のみを除
いて順次積層された第2導電型電流ブロツク層、
第1導電型電流ブロツク層と、メサストライプ及
び第1導電型電流ブロツク層の上の全面にわたり
積層された第2導電型埋込み層とを含む埋込み型
半導体レーザにおいて、メサストライプの側面に
周期が該活性層中の発振光波長の1/2の整数倍の
凹凸周期構造を形成したことを特徴とする単一軸
モード発振半導体レーザが得られる。
According to the present invention, in a semiconductor wafer in which a semiconductor layer including at least an active layer is grown on a semiconductor substrate of a first conductivity type, only the upper surface of a mesa stripe formed by forming two etching grooves deeper than the active layer is removed. a second conductivity type current blocking layer laminated in sequence;
In a buried semiconductor laser including a first conductivity type current blocking layer and a second conductivity type buried layer laminated over the entire surface of the mesa stripe and the first conductivity type current blocking layer, a period is formed on the side surface of the mesa stripe. A single-axis mode oscillation semiconductor laser is obtained, which is characterized by forming a periodic structure of concavities and convexities having an integral multiple of 1/2 of the wavelength of oscillation light in the active layer.

本発明の単一軸モード発振半導体レーザにおい
ては、第1に、活性層を含む半導体ウエーハに2
本の溝を形成してなるメサストライプを埋込んだ
埋込み型半導体レーザの構造を用いているので分
布帰還型にした場合にも高効率な発振が可能であ
るという特長がある。第2に、そのメサストライ
プの側面境界に凹凸の周期構造を形成するので、
半導体レーザの活性層に損傷を与えることが極め
て少なく長寿命化に有利でありまたメサストライ
プ上への半導体の再成長を困難にすることがない
という特長がある。また、周期構造が活性層の側
面境界という発振光電界分布の比較的大きいとこ
ろにあるのでその効果が大きく、周期構造の周期
を2次以上のものにできるので作製が非常に容易
であるという特長がある。なお、活性層を含む半
導体ウエーハに2本の溝を形成してなるメサスト
ライプを埋込んだ埋込み型半導体レーザに関して
は、北村らの特許出願特願昭56−166666号明細書
「埋め込みヘテロ構造体半導体レーザ」を参照さ
れたい。
In the single-axis mode oscillation semiconductor laser of the present invention, firstly, the semiconductor wafer including the active layer has two
Since it uses a buried semiconductor laser structure in which a mesa stripe formed by a book groove is embedded, it has the advantage that highly efficient oscillation is possible even when it is a distributed feedback type. Second, since a periodic structure of concavities and convexities is formed on the side boundaries of the mesa stripes,
It has the advantage that it causes very little damage to the active layer of the semiconductor laser, is advantageous in extending its life, and does not make it difficult to re-grow the semiconductor on the mesa stripe. In addition, since the periodic structure is located at the side boundary of the active layer, where the oscillation optical electric field distribution is relatively large, the effect is large, and the period of the periodic structure can be made quadratic or higher, making it very easy to fabricate. There is. Regarding a buried semiconductor laser in which a mesa stripe formed by forming two grooves in a semiconductor wafer including an active layer is buried, see the patent application specification of patent application No. 166666/1983 by Kitamura et al. Please refer to "Semiconductor Laser".

次に図面を用いて本発明の実施例を説明する。 Next, embodiments of the present invention will be described using the drawings.

第1図は本発明の実施例の単一軸モード発振半
導体レーザ1の斜視図である。これは、(100)面
方位のn−InPウエーハ101上にn−InPバツ
フア層102、発振波長1.5μmのInGaAsP活性
層103、p−InPクラツド層104を順次エピ
タキシヤル成長された半導体ウエーハ1に、<011
>方向に平行に幅5μm、深さ3μmの第1、第2
の溝151,152を、中央の発光再結合するメ
サストライプ150を残しかつそのメサストライ
プ250の側面に周期0.95μmの凹凸周期構造を
形成するようにエツチングして形成し、得られた
エツチング済み半導体ウエーハ2にp−InP電流
ブロツク層105、n−InP電流ブロツク層10
6をメサストライプ150の上面を除いて順次エ
ピタキシヤル成長させ、さらにp−InPの埋込み
層107、p−InGaAsP層108を全面にわた
つて成長させたものである。
FIG. 1 is a perspective view of a single-axis mode oscillation semiconductor laser 1 according to an embodiment of the present invention. This is a semiconductor wafer 1 in which an n-InP buffer layer 102, an InGaAsP active layer 103 with an oscillation wavelength of 1.5 μm, and a p-InP cladding layer 104 are epitaxially grown on an n-InP wafer 101 with a (100) plane orientation. ,<011
> Parallel to the direction with a width of 5 μm and a depth of 3 μm.
The grooves 151 and 152 are etched to leave the central mesa stripe 150 for light emission recombination and to form an uneven periodic structure with a period of 0.95 μm on the sides of the mesa stripe 250, and the resulting etched semiconductor A p-InP current blocking layer 105 and an n-InP current blocking layer 10 are formed on the wafer 2.
6 was epitaxially grown in sequence except for the upper surface of the mesa stripe 150, and then a p-InP buried layer 107 and a p-InGaAsP layer 108 were grown over the entire surface.

第2図、第3図、第4図は本発明の実施例の単
一軸モード発振半導体レーザの作製工程を順次示
すものである。第2図は半導体ウエーハ1の斜視
図、第3図は半導体ウエーハ1の上に形成された
第1、第2の保護膜201,202のパターンを
示す平面図、第4図はエツチング終了後のエツチ
ング済み半導体ウエーハ2の斜視図である。第3
図の第1の保護膜201はHe−Cdレーザの4416
Åの発振光を約53゜の角度で干渉させる二光束干
渉露光法により<011>方向に沿つた周期スト
ライプのフオトレジスト膜である。その周期
0.95μmはメサストライプ中の活性層の発振光波
長の2.5倍に相当し、その発振光に対して5次の
回折格子として機能する。第3図の第2の保護膜
202は第1の保護膜201を形成焼しめ後、フ
オトレジストの塗布及びフオトマスクを用いた露
光により形成された<011>方向の溝間隔約5μm
溝幅約15μmのフオトレジスト膜である。第4図
は、第3図の第1、第2の保護膜201,202
を用いて半導体ウエーハ1をエツチングした後の
エツチング済み半導体ウエーハ2の斜視図であ
る。エツチングにおいては、はじめのうち第1、
第2の保護膜201,202の付いてない四角形
の開口部がエツチングされるが、エツチングが進
むにつれ細い第1の保護膜201の下がサイドエ
ツチングにより大部分取り除かれ、主として第2
の保護膜202の形状で定まる形にエツチングさ
れる。このため、エツチング済み半導体ウエーハ
2のメサストライプ150の形状は、その側面に
第1の保護膜201の周期と同一の周期の凹凸周
期構造をもつたものとなる。その後このエツチン
グ済み半導体ウエーハ2を埋込み成長させること
により、第1図の単一軸モード発振半導体レーザ
10が得られる。
FIGS. 2, 3, and 4 sequentially show the manufacturing process of a single-axis mode oscillation semiconductor laser according to an embodiment of the present invention. FIG. 2 is a perspective view of the semiconductor wafer 1, FIG. 3 is a plan view showing the patterns of the first and second protective films 201 and 202 formed on the semiconductor wafer 1, and FIG. 4 is a diagram showing the pattern after etching is completed. FIG. 2 is a perspective view of an etched semiconductor wafer 2. FIG. Third
The first protective film 201 in the figure is 4416 of He-Cd laser.
This is a photoresist film in the form of periodic stripes along the <011> direction, which is produced by a two-beam interference exposure method in which oscillated light of 3.5 Å interferes with each other at an angle of about 53 degrees. its cycle
0.95 μm corresponds to 2.5 times the oscillation light wavelength of the active layer in the mesa stripe, and functions as a fifth-order diffraction grating for the oscillation light. The second protective film 202 in FIG. 3 is formed by forming and baking the first protective film 201, applying photoresist, and exposing the grooves in the <011> direction using a photomask.
It is a photoresist film with a groove width of approximately 15 μm. FIG. 4 shows the first and second protective films 201 and 202 in FIG.
FIG. 2 is a perspective view of an etched semiconductor wafer 2 after etching the semiconductor wafer 1 using the etching method. In etching, first,
The rectangular opening where the second protective films 201 and 202 are not attached is etched, but as the etching progresses, most of the area under the thin first protective film 201 is removed by side etching, and the second protective film 201 is mainly etched.
It is etched into a shape determined by the shape of the protective film 202. Therefore, the shape of the mesa stripe 150 of the etched semiconductor wafer 2 has a concavo-convex periodic structure having the same period as that of the first protective film 201 on its side surface. Thereafter, the etched semiconductor wafer 2 is embedded and grown to obtain the single-axis mode oscillation semiconductor laser 10 shown in FIG.

本発明の単一軸モード発振半導体レーザにおい
ては、単一軸モード発振をおこさせるための周期
構造を形成するために特に余分なエピタキシヤル
成長が必要とされないという利点がある。また、
周期構造はメサストライプ150の側面境界に直
接に形成されるので、分布帰還の効果が大きく、
そのため周期構造を1次にしなくともよく2次以
上の周期で十分であるので作製が非常に容易であ
るという利点がある。さらに周期構造は活性層1
03の上面あるいは下面にないので寿命を損なう
必配がない等の利点がある。なお、周期構造は一
方の側面のみにあつても良い。
The single-axis mode oscillation semiconductor laser of the present invention has the advantage that no extra epitaxial growth is required to form a periodic structure for causing single-axis mode oscillation. Also,
Since the periodic structure is formed directly on the side boundary of the mesa stripe 150, the effect of distributed feedback is large.
Therefore, the periodic structure does not need to be of primary order, and a period of secondary or higher order is sufficient, so there is an advantage that manufacturing is very easy. Furthermore, the periodic structure is the active layer 1
Since it is not on the upper or lower surface of 03, there are advantages such as there is no need to impair the service life. Note that the periodic structure may be provided only on one side.

本発明の実施例の形態は、以上のべた実施例の
他に種々のものがありうる。InPウエーハ101
はp型のものであつてもよい。なおこの場合成長
半導体層は実施例の導電型と全て逆にすることが
必要である。また、この実施例の結晶構成はInP
及びInGaAsP以外のものであつてもよい。また、
発振波長は1.5μmに限定されることなく他の波長
でもよいことは当然である。
The embodiments of the present invention may have various forms in addition to the embodiments described above. InP wafer 101
may be of p-type. In this case, it is necessary for the grown semiconductor layer to have a conductivity type completely opposite to that of the embodiment. In addition, the crystal structure of this example is InP
And it may be something other than InGaAsP. Also,
It goes without saying that the oscillation wavelength is not limited to 1.5 μm and may be any other wavelength.

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

第1図、第2図、第3図、第4図はそれぞれ、
本発明の一実施例の斜視図、半導体ウエーハの斜
視図、第1、第2エツチング保護膜のパターンを
示す図、エツチング済み半導体ウエーハの斜視図
である。 図において、1……半導体ウエーハ、2……エ
ツチング済み半導体ウエーハ、101……n−
InPウエーハ、102……バツフア層、103…
…活性層、104……クラツド層、105……p
−InP電流ブロツク層、106……n−InP電流
ブロツク層、107……p−InP埋込み層、10
8……オーミツク層、150……メサストライ
プ、151,152……溝である。
Figures 1, 2, 3 and 4 are respectively
FIG. 1 is a perspective view of an embodiment of the present invention, a perspective view of a semiconductor wafer, a view showing patterns of first and second etching protection films, and a perspective view of an etched semiconductor wafer. In the figure, 1... semiconductor wafer, 2... etched semiconductor wafer, 101... n-
InP wafer, 102... Buffer layer, 103...
...active layer, 104...clad layer, 105...p
-InP current blocking layer, 106...n-InP current blocking layer, 107...p-InP buried layer, 10
8... Ohmic layer, 150... Mesa stripe, 151, 152... Groove.

Claims (1)

【特許請求の範囲】[Claims] 1 第1導電型半導体基板上に少くとも活性層を
含む半導体層を成長させた半導体ウエーハに、前
記活性層より深い2本のエツチング溝を形成して
なるメサストライプの上面のみを除いて順次積層
された第2導電型電流ブロツク層、第1導電型電
流ブロツク層と、前記メサスライトライプおよび
第1導電型電流ブロツク層の上の全面にわたり積
層された第2導電型埋込み層とを含む埋込み型半
導体レーザにおいて、前記メサストライプの側面
に周期が前記活性層中の発振光波長の1/2の整数
倍の凹凸周期構造を形成したことを特徴とする単
一軸モード発振半導体レーザ。
1. A semiconductor wafer in which a semiconductor layer including at least an active layer is grown on a semiconductor substrate of a first conductivity type, and the mesa stripes formed by forming two etched grooves deeper than the active layer are sequentially laminated except for the upper surface. a second conductivity type current blocking layer, a first conductivity type current blocking layer, and a second conductivity type buried layer laminated over the entire surface of the mesa light stripe and the first conductivity type current blocking layer. 1. A single-axis mode oscillation semiconductor laser, characterized in that a concavo-convex periodic structure whose period is an integral multiple of 1/2 of the wavelength of oscillation light in the active layer is formed on the side surface of the mesa stripe.
JP1345282A 1982-01-29 1982-01-29 Single axis mode oscillating semiconductor laser Granted JPS58131785A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1345282A JPS58131785A (en) 1982-01-29 1982-01-29 Single axis mode oscillating semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1345282A JPS58131785A (en) 1982-01-29 1982-01-29 Single axis mode oscillating semiconductor laser

Publications (2)

Publication Number Publication Date
JPS58131785A JPS58131785A (en) 1983-08-05
JPS6342876B2 true JPS6342876B2 (en) 1988-08-25

Family

ID=11833528

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1345282A Granted JPS58131785A (en) 1982-01-29 1982-01-29 Single axis mode oscillating semiconductor laser

Country Status (1)

Country Link
JP (1) JPS58131785A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH037582U (en) * 1989-06-10 1991-01-24

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62169388A (en) * 1986-01-21 1987-07-25 Oki Electric Ind Co Ltd Semiconductor laser element
US4870468A (en) * 1986-09-12 1989-09-26 Kabushiki Kaisha Toshiba Semiconductor light-emitting device and method of manufacturing the same
JPH07112094B2 (en) * 1990-03-16 1995-11-29 株式会社東芝 Semiconductor laser device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH037582U (en) * 1989-06-10 1991-01-24

Also Published As

Publication number Publication date
JPS58131785A (en) 1983-08-05

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