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JP2781182B2 - Compound semiconductor laser device having a waveguide - Google Patents
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JP2781182B2 - Compound semiconductor laser device having a waveguide - Google Patents

Compound semiconductor laser device having a waveguide

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Publication number
JP2781182B2
JP2781182B2 JP63203527A JP20352788A JP2781182B2 JP 2781182 B2 JP2781182 B2 JP 2781182B2 JP 63203527 A JP63203527 A JP 63203527A JP 20352788 A JP20352788 A JP 20352788A JP 2781182 B2 JP2781182 B2 JP 2781182B2
Authority
JP
Japan
Prior art keywords
laser device
semiconductor laser
compound semiconductor
active layer
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 - Fee Related
Application number
JP63203527A
Other languages
Japanese (ja)
Other versions
JPH0252480A (en
Inventor
尚範 加藤
秀樹 後藤
謙司 下山
哲 長尾
優一 井上
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.)
Mitsubishi Chemical Corp
Original Assignee
Mitsubishi Chemical 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 Mitsubishi Chemical Corp filed Critical Mitsubishi Chemical Corp
Priority to JP63203527A priority Critical patent/JP2781182B2/en
Publication of JPH0252480A publication Critical patent/JPH0252480A/en
Application granted granted Critical
Publication of JP2781182B2 publication Critical patent/JP2781182B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は高出力、高速であると共に、信頼性の高い新
規な導波路を有する化合物半導体レーザー装置に関する
ものである。
Description: BACKGROUND OF THE INVENTION The present invention relates to a compound semiconductor laser device having a novel waveguide with high output, high speed, and high reliability.

〔従来の技術〕[Conventional technology]

従来の縦型電流路型半導体レーザーにおいて、共振器
の両端から内部へ向かう一部分にレーザー発振光を吸収
しない導波路を設けた化合物半導体レーザーが試みら
れ、出力向上に効果があったことが報告されている(19
87,第48回応用物理学会学術講演会講演予稿集p739,18a
−ZR−8)。本装置は縦型のNAH(Non Absorbing Mirro
r)−LOC(Large Optical Cavity)レーザーと呼ばれ、
ミラーの自己吸収破壊を起こしにくくなっている。
In a conventional vertical current path type semiconductor laser, a compound semiconductor laser in which a waveguide that does not absorb laser oscillation light is provided in a part of the cavity that goes from both ends to the inside was tried, and it was reported that the output was improved. (19
87, Proceedings of the 48th Annual Meeting of the Japan Society of Applied Physics p739,18a
-ZR-8). This device is a vertical NAH (Non Absorbing Mirro
r)-called LOC (Large Optical Cavity) laser,
It is less likely to cause self-absorption destruction of the mirror.

〔発明が解決すべき課題〕[Problems to be solved by the invention]

しかしながら、上記の縦型電流路型半導体レーザー装
置においては、構造が複雑であり、かつ縦型であるため
に基板が導電性を有し、集積化を行うことが困難であっ
た。
However, in the above-described vertical current path type semiconductor laser device, the structure is complicated and the substrate is conductive because of the vertical type, and it is difficult to integrate the substrate.

本発明は上記問題点を解決するためのもので、他の素
子との集積化が容易であると共に、大出力が得られ、高
速動作が可能な化合物半導体レーザー装置を提供するこ
とを目的とする。
SUMMARY OF THE INVENTION The present invention has been made to solve the above problems, and has as its object to provide a compound semiconductor laser device which can be easily integrated with other elements, has a large output, and can operate at high speed. .

〔課題を解決するための手段〕[Means for solving the problem]

本発明の導波路を有する化合物半導体レーザー装置
は、他素子との集積化が容易な横接合埋込型(TJ−BH)
とし、レーザーの活性層と接するところの一部にあらか
じめ活性層の屈折率よりも小さな屈折率を有し、かつレ
ーザー発振光を吸収しない物質(非吸収体)を埋め込ん
で導波路を形成する共に、電流注入層を別々に埋む込
み、前記非吸収体で共振器の端面を形成するように構成
したことを特徴とする。
The compound semiconductor laser device having the waveguide according to the present invention is a lateral junction buried type (TJ-BH) which can be easily integrated with other elements.
And forming a waveguide by embedding a substance (a non-absorber) having a refractive index smaller than that of the active layer and not absorbing laser oscillation light in advance in a portion in contact with the active layer of the laser. The present invention is characterized in that the current injection layers are separately embedded and the non-absorber forms the end face of the resonator.

〔作用〕[Action]

本発明は横接合埋込ヘテロ構造レーザーにおいて、共
振器の両端から内部に向かう部分にレーザー光を吸収し
ない導波路を設けたので、この非吸収体が端面劣化の発
生を防止し、そのため大電流を注入することが可能とな
り、高出力を得ることができると共に、横接合型である
ので基板を半絶縁性で構成することができ、その結果集
積化が容易となり、また電極間容量を大幅に減らし、高
速動作を行わせることが可能となる。
According to the present invention, in a lateral junction buried heterostructure laser, a waveguide that does not absorb laser light is provided in a portion extending from both ends of the resonator toward the inside. Can be implanted, high output can be obtained, and since the lateral junction type is used, the substrate can be configured with semi-insulating properties. As a result, integration becomes easy, and the capacitance between electrodes is greatly reduced. Thus, high-speed operation can be performed.

〔実施例〕〔Example〕

以下、実施例を図面を参照して説明する。 Hereinafter, embodiments will be described with reference to the drawings.

第1図は本発明の化合物半導体レーザー装置の製造工
程の一実施例を示す図である。
FIG. 1 is a view showing one embodiment of a manufacturing process of the compound semiconductor laser device of the present invention.

まず、第1図(イ)に示すように、半絶縁性GaAs:Cr
基板1上にアンドープAl0.42Ga0.58As層2を2μm、ア
ンドープGaAs活性層3を0.2μm、アンドープAl0.42Ga
0.58As層4を0.5μm、それぞれエピタキャル成長させ
る。このエピタキシャル基板上にSiNxを形成し、次いで
第1図(ロ)に示すようにフォトリソグラフィー、及び
エッチングによって図の<10>方向に平行に深さ0.
8μmのストライプ溝5,6を形成する。次いでSiNxをマス
クとしてMOCVD法によりストライプ溝5,6にアンドープAl
0.42Ga0.58As層7,8を0.8μm成長させる(第1図
(ハ))。アンドープAl0.42Ga0.58As層7,8は、アンド
ープGaAs活性層3よりも誘電率、従って屈折率が小さ
く、かつバンドギャップが大きいのでレーザー発振光を
吸収しない。次いで、SiNxをエッチングで落とし、選択
成長用マスクとしてWNxを形成する。フォトリソグラフ
ィー、およびエッチングにより<110>方向に対して平
行に深さ0.8μmのストライプ溝9を形成し(第1図
(ニ))、更にSiNxを0.8μm形成する。次に<10
>方向に平行で、かつ先に形成したストライプ7,8間の
間隔よりも狭いストライプ溝を形成し、その後MOCVD法
により、この窓にn−Al0.35Ga0.65As層10を選択成長さ
せてSiNxをエッチングにより除去する(第1図
(ホ))。p−Al0.35Ga0.65As層11も同様にして埋め込
みを行い(第1図(へ))、先の<10>方向に平行
に埋め込んだ層の内部(第1図(ヘ)のC1,C2の位置)
に劈開を入れ、共振器端面を形成する(第1図
(ト))。
First, as shown in FIG. 1 (a), semi-insulating GaAs: Cr
An undoped Al 0.42 Ga 0.58 As layer 2 of 2 μm, an undoped GaAs active layer 3 of 0.2 μm, an undoped Al 0.42 Ga
The 0.58 As layer 4 is grown 0.5 μm thick by epitaxy. SiNx is formed on this epitaxial substrate, and then, as shown in FIG. 1 (b), photolithography and etching are performed to a depth of 0.1 in parallel with the <10> direction of the figure.
8 μm stripe grooves 5 and 6 are formed. Then, undoped Al was added to stripe grooves 5, 6 by MOCVD using SiNx as a mask.
The 0.42 Ga 0.58 As layers 7, 8 are grown to 0.8 μm (FIG. 1 (c)). The undoped Al 0.42 Ga 0.58 As layers 7 and 8 do not absorb laser oscillation light because the undoped GaAs active layer 3 has a smaller dielectric constant, and thus a lower refractive index, and a larger band gap. Next, SiNx is removed by etching, and WNx is formed as a selective growth mask. A stripe groove 9 having a depth of 0.8 μm is formed in parallel with the <110> direction by photolithography and etching (FIG. 1 (d)), and then 0.8 μm of SiNx is formed. Then <10
> A stripe groove parallel to the direction and narrower than the interval between the previously formed stripes 7 and 8 is formed, and then an n-Al 0.35 Ga 0.65 As layer 10 is selectively grown on this window by MOCVD to obtain SiNx. Is removed by etching (FIG. 1E). The p-Al 0.35 Ga 0.65 As layer 11 is similarly buried (FIG. 1 (F)), and the inside of the layer buried parallel to the <10> direction (C 1 , FIG. 1 (F)). C 2 position)
Are cleaved to form cavity end faces (FIG. 1 (g)).

そしてクラッド層10,11上に電極を形成し、横方向に
電流注入を行って発振を行わせたとき、アンドープ層7,
8は活性層3よりも屈折率が小さいので導波路として機
能すると共に、バンドギャップが大きいのでレーザー発
振光を吸収せず、端面の劣化を防止する層として機能す
る。
Then, when an electrode is formed on the cladding layers 10 and 11 and current is injected in the lateral direction to oscillate, the undoped layers 7 and
8 has a smaller refractive index than the active layer 3 and thus functions as a waveguide, and has a large band gap so that it does not absorb laser oscillation light and functions as a layer for preventing deterioration of the end face.

なお、発光面のみでなく、装置表面を活性層の屈折率
よりも小さな単一種もくしは複数種の材料で覆うように
すれば、レーザー発振光の漏れを防止し、発振効率を向
上させることができる。
In addition, if the device surface is covered not only with the light emitting surface but also with a single type or a plurality of types of materials smaller than the refractive index of the active layer, it is possible to prevent leakage of laser oscillation light and improve oscillation efficiency. Can be.

また上記実施例においては、クラッド層10,11がアン
ドープ層7,8にまで達していないために活性層3が露出
することになるが、これは後のパッシベーションにより
酸化防止膜を形成して活性層の酸化を防止するようにす
ればよく、またクラッド層10,11をアンドープ層7,8まで
延ばし、キャリア層が露出しないようにしてもよい。
In the above embodiment, the active layer 3 is exposed because the cladding layers 10 and 11 do not reach the undoped layers 7 and 8. This is because the active layer 3 is formed by the passivation to form an antioxidant film. The layers may be prevented from being oxidized, and the cladding layers 10 and 11 may be extended to the undoped layers 7 and 8 so that the carrier layer is not exposed.

さらに、バンドギャップの大きい方の材料、すなわち
バリアー層にn型またはp型あるいはその両方の不純物
をドーピングして単数または複数の単一量子井戸構造、
あるいは多重量子井戸構造を形成することにより活性層
へのキャリアの注入効率を向上させ、出力を増大させる
ようにしてもよい。
Further, a material having a larger band gap, that is, a barrier layer is doped with n-type or p-type or both impurities to form a single quantum well structure or a plurality of single quantum well structures,
Alternatively, the efficiency of carrier injection into the active layer may be improved by forming a multiple quantum well structure to increase the output.

〔発明の効果〕〔The invention's effect〕

以上のように本発明によれば、横接合埋込ヘテロ構造
レーザー装置において縦型のNAM(Non Absorbing Mirro
r)−LOC(Large Optical Cavity)レーザーの場合と同
様に非吸収反射ミラーをレーザー共振器の端面に設ける
ことができ、ミラーが光を吸収して自己破壊を起こすこ
とを防止し、大出力を得ることができる。
As described above, according to the present invention, in a lateral junction buried heterostructure laser device, a vertical NAM (Non Absorbing Mirro
r) As in the case of -LOC (Large Optical Cavity) laser, a non-absorbing reflection mirror can be provided at the end face of the laser resonator, preventing the mirror from absorbing light and causing self-destruction, and providing a large output. Obtainable.

また、横接合レーザーのため半絶縁性基板を用いるこ
とができるので、他の素子との集積が容易となり、また
縦型に比して電流注入する面積を大幅に小さくできるの
で電極間容量を減らすことができ、高速動作を行うこと
が可能となる。
In addition, since a semi-insulating substrate can be used for the lateral junction laser, integration with other elements is easy, and the area for current injection can be significantly reduced as compared with the vertical type, thereby reducing the capacitance between electrodes. And high-speed operation can be performed.

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

第1図は本発明の化合物半導体レーザー装置の製造工程
の一実施例を示す図である。 1…半絶縁性GaAs:Cr基板、2…アンドープAl0.42Ga
0.58As層、3…アンドープGaAs活性層3、4…アンドー
プAl0.42Ga0.58As層、5、6…ストライプ溝、7,8…ア
ンドープAl0.42Ga0.58As層、9…ストライプ溝、10…n
−Al0.35Ga0.65As層、11…p−Al0.35Ga0.65As層。
FIG. 1 is a view showing one embodiment of a manufacturing process of the compound semiconductor laser device of the present invention. 1 ... Semi-insulating GaAs: Cr substrate, 2 ... Undoped Al 0.42 Ga
0.58 As layer, 3 undoped GaAs active layer 3, 4 undoped Al 0.42 Ga 0.58 As layer, 5, 6 stripe groove, 7,8 undoped Al 0.42 Ga 0.58 As layer, 9 stripe groove, 10 n
-Al 0.35 Ga 0.65 As layer, 11 ... p-Al 0.35 Ga 0.65 As layer.

フロントページの続き (72)発明者 長尾 哲 茨城県牛久市東猯穴町1000番地 三菱化 成株式会社総合研究所内 (72)発明者 井上 優一 茨城県牛久市東猯穴町1000番地 三菱化 成株式会社総合研究所内 (56)参考文献 特開 昭60−198883(JP,A) 特開 昭59−13387(JP,A) 特開 昭62−214687(JP,A) (58)調査した分野(Int.Cl.6,DB名) H01S 3/18Continued on the front page (72) Inventor Satoshi Nagao 1000 Higashikanamachi, Ushiku City, Ibaraki Prefecture Inside Mitsubishi Chemical Research Institute (72) Inventor Yuichi Inoue 1000 Higashikianamachi, Ushiku City, Ibaraki Prefecture Mitsubishi Chemical Corporation (56) References JP-A-60-198883 (JP, A) JP-A-59-13387 (JP, A) JP-A-62-214687 (JP, A) (58) Fields investigated (Int. . 6, DB name) H01S 3/18

Claims (7)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】横接合埋込ヘテロ構造レーザー装置におい
て、共振器の両端から内部へ向かう領域に活性層端面と
略同一幅で活性層端面を覆うように、レーザー発振光を
吸収しない導波路を設けたことを特徴とする化合物半導
体レーザー装置。
In a lateral junction buried heterostructure laser device, a waveguide that does not absorb laser oscillation light is provided in a region extending from both ends of the resonator to the inside so as to cover the active layer end surface with substantially the same width as the active layer end surface. A compound semiconductor laser device characterized by being provided.
【請求項2】活性層が単数もしくは複数の単一量子井戸
構造よりなる請求項1記載の化合物半導体レーザー装
置。
2. The compound semiconductor laser device according to claim 1, wherein the active layer has one or more single quantum well structures.
【請求項3】活性層が多重量子井戸構造よりなる請求項
1記載の化合物半導体レーザー装置。
3. The compound semiconductor laser device according to claim 1, wherein the active layer has a multiple quantum well structure.
【請求項4】活性層はバリア層に一方の導電型不純物が
選択的にドープされた単数もしくは複数の単一量子井戸
構造よりなる請求項1記載の化合物半導体レーザー装
置。
4. The compound semiconductor laser device according to claim 1, wherein the active layer has a single quantum well structure or a single quantum well structure in which a barrier layer is selectively doped with one conductivity type impurity.
【請求項5】活性層はバリア層に一方の導電型の不純物
が選択的にドープされた多重量子井戸構造よりなる請求
項1記載の化合物半導体レーザー装置。
5. The compound semiconductor laser device according to claim 1, wherein the active layer has a multiple quantum well structure in which a barrier layer is selectively doped with an impurity of one conductivity type.
【請求項6】活性層はバリア層に両方の導電型の不純物
が交互に選択的にドープされた多重量子井戸構造よりな
る請求項1記載の化合物半導体レーザー装置。
6. The compound semiconductor laser device according to claim 1, wherein the active layer has a multiple quantum well structure in which a barrier layer is selectively doped with impurities of both conductivity types alternately.
【請求項7】発光面および装置表面は活性層の屈折率よ
りも小さな単一種もしくは複数種の材料が覆われている
請求項1〜6のうちいずれか1項記載の化合物半導体レ
ーザー装置。
7. The compound semiconductor laser device according to claim 1, wherein the light-emitting surface and the device surface are covered with a single material or a plurality of materials smaller than the refractive index of the active layer.
JP63203527A 1988-08-16 1988-08-16 Compound semiconductor laser device having a waveguide Expired - Fee Related JP2781182B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63203527A JP2781182B2 (en) 1988-08-16 1988-08-16 Compound semiconductor laser device having a waveguide

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63203527A JP2781182B2 (en) 1988-08-16 1988-08-16 Compound semiconductor laser device having a waveguide

Publications (2)

Publication Number Publication Date
JPH0252480A JPH0252480A (en) 1990-02-22
JP2781182B2 true JP2781182B2 (en) 1998-07-30

Family

ID=16475630

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63203527A Expired - Fee Related JP2781182B2 (en) 1988-08-16 1988-08-16 Compound semiconductor laser device having a waveguide

Country Status (1)

Country Link
JP (1) JP2781182B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0828553B2 (en) * 1989-03-10 1996-03-21 三菱電機株式会社 Semiconductor laser

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5913387A (en) * 1982-07-14 1984-01-24 Omron Tateisi Electronics Co Semiconductor laser
JPS60198883A (en) * 1984-03-23 1985-10-08 Nec Corp Semiconductor laser
JPS61236182A (en) * 1985-04-12 1986-10-21 Hitachi Ltd semiconductor laser equipment
JPS62214687A (en) * 1986-03-14 1987-09-21 Fujitsu Ltd Structure of semiconductor laser

Also Published As

Publication number Publication date
JPH0252480A (en) 1990-02-22

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