JP2741292B2 - Surface emitting semiconductor laser - Google Patents
Surface emitting semiconductor laserInfo
- Publication number
- JP2741292B2 JP2741292B2 JP29481491A JP29481491A JP2741292B2 JP 2741292 B2 JP2741292 B2 JP 2741292B2 JP 29481491 A JP29481491 A JP 29481491A JP 29481491 A JP29481491 A JP 29481491A JP 2741292 B2 JP2741292 B2 JP 2741292B2
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- emitting semiconductor
- linearly polarized
- semiconductor
- semiconductor laser
- 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
Links
Landscapes
- Semiconductor Lasers (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、面発光半導体レーザの
改良に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a surface emitting semiconductor laser.
【0002】[0002]
【従来の技術】一般に、基板に対して垂直方向の共振器
を有する、即ち、基板に垂直な方向に向けて発光する面
発光半導体レーザは、偏波方向の制御が困難である。例
えば、平成3年春季第38回応用物理学関係連合講演会
講演予稿集p.1011、31a−D−3にあるよう
に、基板の結晶方位に対し、3つのタイプの偏波特性が
得られることが示されており、主な原因として埋め込み
形状の非対称性が上げられているが、偏波方向を制御で
きる程度に埋め込み形状を制御することは困難である。2. Description of the Related Art In general, a surface emitting semiconductor laser having a resonator perpendicular to a substrate, that is, emitting light in a direction perpendicular to the substrate, has difficulty in controlling the polarization direction. For example, in the 38th Spring Meeting of 1991 Applied Physics Related Lectures, p. As shown in 1011, 31a-D-3, it has been shown that three types of polarization characteristics can be obtained with respect to the crystal orientation of the substrate, and the main cause is that the asymmetry of the buried shape is increased. However, it is difficult to control the embedded shape to the extent that the polarization direction can be controlled.
【0003】[0003]
【発明が解決しようとする課題】上述のように、従来の
垂直方向の共振器を有する面発光半導体レーザは、偏波
方向の制御が困難であるという問題点がある。本発明
は、偏波方向の制御を可能とした垂直方向の共振器を有
する面発光半導体レーザを提供することを目的とする。As described above, the conventional surface emitting semiconductor laser having a vertical resonator has a problem that it is difficult to control the polarization direction. An object of the present invention is to provide a surface emitting semiconductor laser having a vertical resonator capable of controlling the polarization direction.
【0004】[0004]
【課題を解決するための手段】本発明によれば、基板に
対して垂直方向の共振器を有する面発光半導体レーザに
おいて、前記基板は(110)方向の面を有する半導体
基板であり、該半導体基板上に閃亜鉛鉱型結晶構造の半
導体による(110)方向の多重量子井戸よりなり、前
記基板面内の直線偏光の向きに対して屈折率が異なる半
導体多層反射鏡を形成したことを特徴とする面発光半導
体レーザが得られる。また、本発明によれば、基板上に
第1導電型クラッド層、活性層、第2導電型クラッド層
が順に形成され、該第2導電型クラッド層の除去部分に
電流狭搾層を形成し、前記基板に対して垂直方向の共振
器を有する電流狭搾構造の面発光半導体レーザにおい
て、前記基板は(110)方向の面を有する半導体基板
であり、該半導体基板上に閃亜鉛鉱型結晶構造の半導体
による(110)方向の多重量子井戸よりなり、且つ前
記基板面内の直線偏光の向きに対して屈折率が異なる半
導体多層反射鏡を形成したことを特徴とする面発光半導
体レーザが得られる。さらに、本発明によれば、[1be
r 10]方向に直線偏光した光に対してレーザ発振する
ことを特徴とする面発光半導体レーザが得られる。さら
にまた、本発明によれば、[001]方向に直線偏光し
た光に対してレーザ発振することを特徴とする面発光半
導体レーザが得られる。According to the present invention, in a surface emitting semiconductor laser having a resonator perpendicular to a substrate, the substrate is a semiconductor substrate having a surface in a (110) direction. A semiconductor multi-layer reflecting mirror is formed on a substrate, comprising a multiple quantum well in the (110) direction of a semiconductor having a zinc blende type crystal structure and having a different refractive index with respect to the direction of linearly polarized light in the plane of the substrate. Is obtained. Further, according to the present invention, a first conductivity type clad layer, an active layer, and a second conductivity type clad layer are sequentially formed on a substrate, and a current constriction layer is formed in a removed portion of the second conductivity type clad layer. In a surface emitting semiconductor laser having a current constriction structure having a resonator perpendicular to the substrate, the substrate is a semiconductor substrate having a plane in a (110) direction, and a zinc-blende crystal is provided on the semiconductor substrate. A surface emitting semiconductor laser characterized by forming a semiconductor multilayer reflecting mirror comprising a multiple quantum well in the (110) direction by a semiconductor having a structure and having a different refractive index with respect to the direction of linearly polarized light in the plane of the substrate. Can be Further, according to the present invention, [1be
A surface-emitting semiconductor laser characterized in that it oscillates with respect to light linearly polarized in the [r 10] direction. Furthermore, according to the present invention, a surface emitting semiconductor laser characterized in that laser light is emitted for light linearly polarized in the [001] direction.
【0005】[0005]
【作用】(001)方向及び(111)方向を除く所定
方向の量子井戸層は、垂直方向に進む直線偏光に対する
光学遷移の振動子強度が異方的になる。即ち、量子井戸
が形成された活性層では、ある特定の方向に直線偏光し
た光に対して利得が大きく、この方向に直線偏光した光
のみがレーザ発振する。また、量子井戸が形成された半
導体多層膜反射鏡では、直線偏光の向き(基板面内方
向)によって屈折率が異なり、ある特定の方向に直線偏
光した光に対してのみ共振条件を満足するので、この方
向に直線偏光した光のみがレーザ発振する。In the quantum well layer in a predetermined direction except for the (001) direction and the (111) direction, the oscillator intensity of the optical transition with respect to the linearly polarized light traveling in the vertical direction becomes anisotropic. That is, in the active layer in which the quantum well is formed, the gain is large for light linearly polarized in a specific direction, and only the light linearly polarized in this direction oscillates. Moreover, in a semiconductor multilayer film reflecting mirror in which a quantum well is formed, the refractive index varies depending on the direction of linearly polarized light (in-plane direction of the substrate), and the resonance condition is satisfied only for light linearly polarized in a specific direction. Only laser light linearly polarized in this direction oscillates.
【0006】[0006]
【実施例】以下、図面を参照して本発明の実施例を説明
する。図1に本発明の第1実施例を示す。まず、有機金
属気相エピタキシ法により、n型GaAs(110)基
板11上に次の各層を成長させた。成長させた層は下か
ら順に、Al0.2 Ga0.8 As/AlAs(25ペア)
n型半導体多層膜12、Al0.35Ga0.65As n型
クラッド層13(0.5μm)、GaAs/Al0.35G
a0.65As多重量子井戸p型活性層14(1.0μ
m)、Al0.35Ga0.65As p型クラッド層15
(0.5μm)、及びAl0.2 Ga0.8 As p型キャ
ップ層16(0.5μm)である。ここで、活性層14
は、膜厚5nmのAl組成35%のAlGaAs層と、
膜厚5nmのGaAs層とからなる(110)方向の多
重量子井戸である。次に、キャップ層16の表面中央部
に直径7μmのSiO2 マスクを形成し、反応性イオン
エッチングにより活性層14を露出させない程度にp型
クラッド層15をエッチングした。その次に、エッチン
グしたとことに、電流狭搾層として、n型GaAs層1
7を0.7μm、p型GaAs層を0.3μm、選択成
長させた。上述のように本実施例の面発行半導体レーザ
は、(110)方向の多重量子井戸が形成されている。
この(110)方向の多重量子井戸では、[1ber 1
0]方向に直線偏光した光に対する光学遷移の振動子強
度は、[001]方向に直線偏光した光に対する光学遷
移の振動子強度と比較して約1.2倍になる。従って、
この面発光半導体レーザでは、[1ber 10]方向に直
線偏光した光のみがレーザ発振した。なお、[1ber 1
0]は、以下の化1のとおりである。Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 shows a first embodiment of the present invention. First, the following layers were grown on an n-type GaAs (110) substrate 11 by metal organic vapor phase epitaxy. The grown layers are Al 0.2 Ga 0.8 As / AlAs (25 pairs) in order from the bottom.
n-type semiconductor multilayer film 12, Al 0.35 Ga 0.65 As n-type cladding layer 13 (0.5 μm), GaAs / Al 0.35 G
a 0.65 As multiple quantum well p-type active layer 14 (1.0 μm
m), Al 0.35 Ga 0.65 As p-type cladding layer 15
(0.5 μm), and Al 0.2 Ga 0.8 Asp type cap layer 16 (0.5 μm). Here, the active layer 14
Is an AlGaAs layer having a thickness of 5 nm and an Al composition of 35%;
This is a multiple quantum well in the (110) direction composed of a GaAs layer having a thickness of 5 nm. Next, an SiO 2 mask having a diameter of 7 μm was formed at the center of the surface of the cap layer 16, and the p-type cladding layer 15 was etched by reactive ion etching so that the active layer 14 was not exposed. Then, after the etching, the n-type GaAs layer 1 was used as a current constricting layer.
7 was grown selectively at 0.7 μm, and the p-type GaAs layer was grown at 0.3 μm. As described above, the surface emitting semiconductor laser of this embodiment has a multiple quantum well in the (110) direction.
In this multiple quantum well in the (110) direction, [1ber 1
The oscillator strength of the optical transition for the light linearly polarized in the [0] direction is about 1.2 times as large as the oscillator strength of the optical transition for the light linearly polarized in the [001] direction. Therefore,
In this surface emitting semiconductor laser, only light linearly polarized in the [1ber 10] direction oscillated. Note that [1ber 1
0] is as shown in the following chemical formula 1.
【0007】[0007]
【化1】 [1ber 10]=[10][1ber 10] = [10]
【0008】次に本発明の第2の実施例について説明す
る。本実施例は第1の実施例と同様の構成であるが、A
l0.2 Ga0.8 As/AlAs(25ペア) n型半導
体多層膜12のAl0.2 Ga0.8 As膜に代えて、Al
0.1 Ga0.9 As/Al0.35Ga0.65As多重量子井戸
を成長させた。即ち、半導体多層膜反射鏡に(110)
方向の量子井戸を形成した。また、GaAs/Al0.35
Ga0.65As多重量子井戸 p型活性層14に代えて、
p型Al0.1 Ga0.9 Asを成長させた。上記のよう
に、第2の実施例では半導体多層膜反射鏡に、(11
0)方向の量子井戸が形成されており、この(110)
方向の量子井戸では、基板面内の直線偏光の向きに対し
て屈折率が異なる。この結果、ある特定の方向(基板面
内方向)に直線偏光した光に対して共振条件が満足さ
れ、その方向に直線偏光した光のみがレーザ発振する。
上記特定方向は半導体多層膜の膜厚で決定され、本実施
例では[1ber 10]方向に直線偏光した光に対してレ
ーザ発振する膜厚とした。以上述べたように、第1の実
施例、第2の実施例ともに偏光方向を制御することがで
きる。なお、上記実施例では、AlGaAs系面発光半
導体レーザについて述べたが、活性層または半導体多層
膜反射鏡の一部が閃亜鉛鉱型結晶構造の半導体からなる
半導体レーザであれば、AlGaInP系及びGaIn
AsP系等のIII −V族並びにII−IV族系面発光半導体
レーザであっても本発明を適用することができる。ま
た、上記実施例では、成長面側から光を出射する面発光
半導体レーザについて述べたが、基板側から光を出射す
る面発光半導体についても同様に適用することができ
る。さらに、上記実施例では半導体多層膜反射鏡が基板
側に設けられているが、表面側に設けられていても良
い。さらにまた、上記実施例では電流狭搾構造の面発光
半導体レーザについて説明したが、基板と垂直方向の共
振器を有する面発光半導体レーザであれば、埋め込み構
造などの面発光半導体レーザであってもよい。また、第
2の実施例では、[1ber 10]方向に直線偏光したレ
ーザ光を発振させる例について述べたが、半導体多層膜
の膜厚や組成を変えることにより、[001]方向に直
線偏光させるようにすることができる。Next, a second embodiment of the present invention will be described. This embodiment has the same configuration as that of the first embodiment.
l 0.2 Ga 0.8 As / AlAs (25 pairs) Instead of the Al 0.2 Ga 0.8 As film of the n-type semiconductor multilayer film 12, Al
A 0.1 Ga 0.9 As / Al 0.35 Ga 0.65 As multiple quantum well was grown. That is, (110)
Directional quantum wells were formed. Also, GaAs / Al 0.35
Ga 0.65 As Multiple Quantum Well Instead of the p-type active layer 14,
A p-type Al 0.1 Ga 0.9 As was grown. As described above, in the second embodiment, (11)
A quantum well in the 0) direction is formed.
In the quantum well in the direction, the refractive index differs with respect to the direction of linearly polarized light in the plane of the substrate. As a result, the resonance condition is satisfied for light linearly polarized in a specific direction (in-plane direction of the substrate), and only light linearly polarized in that direction oscillates.
The specific direction is determined by the film thickness of the semiconductor multilayer film. In this embodiment, the film thickness is such that the laser beam oscillates with respect to the light linearly polarized in the [1ber 10] direction. As described above, the polarization direction can be controlled in both the first embodiment and the second embodiment. In the above embodiment, an AlGaAs surface emitting semiconductor laser has been described. However, if a part of the active layer or the semiconductor multilayer film reflecting mirror is a semiconductor having a zinc blende type crystal structure, an AlGaInP type and a GaIn
The present invention can be applied to surface emitting semiconductor lasers of the III-V group and the II-IV group such as AsP. Further, in the above embodiment, the surface emitting semiconductor laser that emits light from the growth surface side has been described, but the present invention can be similarly applied to a surface emitting semiconductor that emits light from the substrate side. Further, in the above embodiment, the semiconductor multilayer film reflecting mirror is provided on the substrate side, but may be provided on the surface side. Furthermore, in the above-described embodiment, the surface-emitting semiconductor laser having the current constriction structure has been described. However, any surface-emitting semiconductor laser having a resonator perpendicular to the substrate may be used, even if the surface-emitting semiconductor laser has an embedded structure. Good. Further, in the second embodiment, the example in which the laser light linearly polarized in the [1ber 10] direction is oscillated has been described. However, by changing the thickness and composition of the semiconductor multilayer film, the laser light is linearly polarized in the [001] direction. You can do so.
【0009】[0009]
【発明の効果】本発明によれば、活性層中、あるいは多
層膜反射鏡中に量子井戸を形成することにより偏波方向
が制御されたレーザー光を出射する面発光半導体レーザ
が得られる。According to the present invention, a surface emitting semiconductor laser that emits laser light whose polarization direction is controlled can be obtained by forming a quantum well in an active layer or a multilayer reflector.
【図1】本発明の第1の実施例の構造を示す図である。FIG. 1 is a diagram showing a structure of a first embodiment of the present invention.
11 n型GaAs(110)基板 12 Al0.2 Ga0.8 As/AlAs n型半導体
多層膜 13 Al0.35Ga0.65As n型クラッド層 14 GaAs/Al0.35Ga0.65As多重量子井戸
p型活性層 15 Al0.35Ga0.65As p型クラッド層 16 Al0.2 Ga0.8 As p型キャップ層 17 n型GaAs層 18 p型GaAs層Reference Signs List 11 n-type GaAs (110) substrate 12 Al 0.2 Ga 0.8 As / AlAs n-type semiconductor multilayer film 13 Al 0.35 Ga 0.65 As n-type clad layer 14 GaAs / Al 0.35 Ga 0.65 As multiple quantum well p-type active layer 15 Al 0.35 Ga 0.65 As p-type cladding layer 16 Al 0.2 Ga 0.8 As p-type cap layer 17 n-type GaAs layer 18 p-type GaAs layer
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平5−55704(JP,A) 伊賀健一、小山二三夫著 「面発光レ ーザ」 オーム社 (1990) 平成3年秋季応物学会予稿集 第3分 冊 11p−ZM−5 平成3年春季応物学会予稿集 第3分 冊 31a−D−3 日本物理学会年会講演予稿集 46 〜 2! (1991) P.143 28p−C− 14 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-5-55704 (JP, A) Kenichi Iga, Fumio Koyama “Surface emitting laser” Ohmsha (1990) 3 volumes 11p-ZM-5 Spring 1991 Proceedings of the Japan Society of Applied Physics 3rd Volume 31a-D-3 Proceedings of the Annual Meeting of the Physical Society of Japan 46-2! (1991) P.A. 143 28p-C-14
Claims (4)
面発光半導体レーザにおいて、前記基板は(110)方
向の面を有する半導体基板であり、該半導体基板上に閃
亜鉛鉱型結晶構造の半導体による(110)方向の多重
量子井戸よりなり、前記基板面内の直線偏光の向きに対
して屈折率が異なる半導体多層反射鏡を形成したことを
特徴とする面発光半導体レーザ。1. A surface emitting semiconductor laser having a resonator perpendicular to a substrate, wherein the substrate is a semiconductor substrate having a surface in a (110) direction, and a zinc blende type crystal structure is formed on the semiconductor substrate. A surface emitting semiconductor laser comprising a semiconductor multilayer reflector formed of a semiconductor having multiple quantum wells in the (110) direction and having a different refractive index with respect to the direction of linearly polarized light in the plane of the substrate.
層、第2導電型クラッド層が順に形成され、該第2導電
型クラッド層の除去部分に電流狭搾層を形成し、前記基
板に対して垂直方向の共振器を有する電流狭搾構造の面
発光半導体レーザにおいて、前記基板は(110)方向
の面を有する半導体基板であり、該半導体基板上に閃亜
鉛鉱型結晶構造の半導体による(110)方向の多重量
子井戸よりなり、且つ前記基板面内の直線偏光の向きに
対して屈折率が異なる半導体多層反射鏡を形成したこと
を特徴とする面発光半導体レーザ。A first conductive type clad layer, an active layer, and a second conductive type clad layer are sequentially formed on the substrate, and a current constriction layer is formed in a portion where the second conductive type clad layer is removed. In a surface-emitting semiconductor laser having a current constriction structure having a resonator perpendicular to a semiconductor substrate, the substrate is a semiconductor substrate having a surface in a (110) direction, and a semiconductor having a zinc blende type crystal structure is formed on the semiconductor substrate. A multi-quantum well in the (110) direction according to (1) and a semiconductor multilayer reflector having a different refractive index with respect to the direction of linearly polarized light in the plane of the substrate.
対してレーザ発振することを特徴とする請求項1又は2
記載の面発光半導体レーザ。3. A laser oscillation for light linearly polarized in the [1ber 10] direction.
The surface emitting semiconductor laser as described in the above.
てレーザ発振することを特徴とする請求項1又は2記載
の面発光半導体レーザ。4. The surface emitting semiconductor laser according to claim 1, wherein laser oscillation is performed for light linearly polarized in the [001] direction.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29481491A JP2741292B2 (en) | 1991-10-16 | 1991-10-16 | Surface emitting semiconductor laser |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP29481491A JP2741292B2 (en) | 1991-10-16 | 1991-10-16 | Surface emitting semiconductor laser |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05110198A JPH05110198A (en) | 1993-04-30 |
JP2741292B2 true JP2741292B2 (en) | 1998-04-15 |
Family
ID=17812601
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP29481491A Expired - Fee Related JP2741292B2 (en) | 1991-10-16 | 1991-10-16 | Surface emitting semiconductor laser |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2741292B2 (en) |
-
1991
- 1991-10-16 JP JP29481491A patent/JP2741292B2/en not_active Expired - Fee Related
Non-Patent Citations (4)
Title |
---|
伊賀健一、小山二三夫著 「面発光レーザ」 オーム社 (1990) |
平成3年春季応物学会予稿集 第3分冊 31a−D−3 |
平成3年秋季応物学会予稿集 第3分冊 11p−ZM−5 |
日本物理学会年会講演予稿集 46 〜2! (1991) P.143 28p−C−14 |
Also Published As
Publication number | Publication date |
---|---|
JPH05110198A (en) | 1993-04-30 |
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