JPS59141282A - Semiconductor laser device - Google Patents

Semiconductor laser device

Info

Publication number
JPS59141282A
JPS59141282A JP58016593A JP1659383A JPS59141282A JP S59141282 A JPS59141282 A JP S59141282A JP 58016593 A JP58016593 A JP 58016593A JP 1659383 A JP1659383 A JP 1659383A JP S59141282 A JPS59141282 A JP S59141282A
Authority
JP
Japan
Prior art keywords
substrate
active layer
semiconductor laser
axis
plane
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.)
Pending
Application number
JP58016593A
Other languages
Japanese (ja)
Inventor
Takashi Murakami
隆志 村上
Toshio Tanaka
利夫 田中
Shoichi Kakimoto
柿本 昇一
Yutaka Mihashi
三橋 豊
Saburo Takamiya
高宮 三郎
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 Electric Corp
Original Assignee
Mitsubishi Electric 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 Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP58016593A priority Critical patent/JPS59141282A/en
Publication of JPS59141282A publication Critical patent/JPS59141282A/en
Pending 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
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/32Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
    • 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
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/32Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
    • H01S5/3202Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures grown on specifically orientated substrates, or using orientation dependent growth

Landscapes

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

Abstract

PURPOSE:To obtain a laser, characteristics thereof are excellent and reliability thereto is superior, by suppressing a surface morphology with a terraced stepped difference by inclining a main surface only by a specific angle while using a waveguide direction as an axis, growing a thin uniform active layer and preventing the displacement of the direction of emitting beams by controlling the direction of inclination. CONSTITUTION:A main surface is inclined at an angle of 0.2-5 deg. while using the waveguide direction as an axis. For example, a face orientation of a substrate consisting of GaAs is inclined at 1 deg. from a 100 face. Since a thin uniform active layer 13 can be acquired by inclining the substrate, currents injected to the active layer 13 are equalized, and beams emitted by injection currents do not scatter and are emitted uniformly. Since the substrate 11 is inclined in the direction that is turned while using emitting beams as an axis, the direction of emitting beams is the same as conventional type devices through the substrate 11 is inclined, and no trouble is generated even when a laser chip is mounted to a package.

Description

【発明の詳細な説明】 この発明は、半導体レーザ装置に関するものであり、薄
く均一な厚みの活性層を持つ半導体レーザ装置を実現す
るものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a semiconductor laser device, and is intended to realize a semiconductor laser device having an active layer having a thin and uniform thickness.

第1図は通常の電極ストライプ構造を持った半導体し′
−ザを示すもので、1は基板、2はクラッド層、3は活
性層、4はコンタクト層である。そして5はストライプ
電極、6は基板側電極である。
Figure 1 shows a semiconductor with a normal electrode stripe structure.
1 is a substrate, 2 is a cladding layer, 3 is an active layer, and 4 is a contact layer. Further, 5 is a stripe electrode, and 6 is a substrate side electrode.

従来の半導体レーザでは基板1としてはGaAsの(1
00)面を用い、その上へ結晶成長技術を用いて、前記
した2〜4の各層を成長させ、共振面としては導波路方
向と垂直である( o hl)面を用いていた。
In a conventional semiconductor laser, the substrate 1 is made of GaAs (1
The above-mentioned layers 2 to 4 were grown using a crystal growth technique on the 00) plane, and the (o hl) plane perpendicular to the waveguide direction was used as the resonance plane.

すなわち面方位<100)の基板1上にクラッド層2.
活性層3等を液相成長させた後、(011)面に平行に
臂開する。そして、第1図では(011)面および(0
11)面を共振面として利用している。したがって電流
注入により活性層3で発生した元は一組の対向する(0
11)および(o jl )面間を往復しながら光増幅
作用を受け、増幅率がある閾値を越えた時点で(alt
)面より外部ヘレーザ元として出射される。
That is, a cladding layer 2.
After the active layer 3 and the like are grown in a liquid phase, the arms are opened parallel to the (011) plane. In Figure 1, the (011) plane and (0
11) The surface is used as a resonance surface. Therefore, the elements generated in the active layer 3 due to current injection form a pair of opposing (0
11) and (o jl ) undergoes optical amplification while reciprocating between the planes, and when the amplification factor exceeds a certain threshold, (alt
) surface as an external laser source.

(011)面および(oir)面を共振面として利用し
た場合も同様で、この場合はレーザ元は、(011)面
より外部へ出射される。
The same applies to the case where the (011) plane and the (oir) plane are used as resonant planes; in this case, the laser source is emitted to the outside from the (011) plane.

従来の半導体レーザは以上のように基板として、(10
0)面からできるだけ面方位ずれの少ない基板1を用い
ているが、厳密に面方位ずれが全(ない基板を得ること
は不可能である。そのため、このような微小な面方位ず
れがある基板1上に液相成長法によりクラッド層2.活
性層3等を成長させると、成長層表面にテラス等の表面
モフオロジーが現われる。すると膜厚の薄い活性層3は
第2図に示すように厚みが不均一となり、また不純物分
布やA1組成分布も不均一となり、レーザの特性や信頼
性を悪化させるという欠点があった。
Conventional semiconductor lasers use (10
Although we use a substrate 1 with as little deviation from the surface orientation as possible from the 0) plane, it is impossible to obtain a substrate with absolutely no deviation from the surface orientation. When a cladding layer 2, active layer 3, etc. are grown on top of layer 1 by liquid phase growth, a surface morphology such as terraces appears on the surface of the grown layer.Then, active layer 3, which is thin, has a thickness as shown in FIG. becomes non-uniform, and the impurity distribution and A1 composition distribution also become non-uniform, which has the drawback of deteriorating the characteristics and reliability of the laser.

この発明は、上記のような欠点を除去するためになさね
たもので、主面の面方位1に0.2°〜5゜だけ(10
0)面から傾けることによりテラス状の段差を有する表
面モフオロジーをおさえ、薄くて均一な活性層を成長さ
せ、しかも傾げる方向を制御することにより出射光の方
向がずれないようにした半導体レーザな提供することを
目的としている。
This invention was made in order to eliminate the above-mentioned drawbacks, and the main surface has an angle of 0.2° to 5° (10
0) Providing a semiconductor laser that suppresses surface morphology with terrace-like steps by tilting from the surface, grows a thin and uniform active layer, and prevents the direction of emitted light from shifting by controlling the tilting direction. It is intended to.

以下この発明の具体的な一実施例を第3図に基づいて説
明する。
A specific embodiment of the present invention will be described below with reference to FIG.

第3図において、11はGaAa からなる基板で、活
性層を薄く均一に成長させるため基板11の面方位は(
100)面から1°傾げている。ただし傾ける方向は半
導体レーザを製作した場合、主面と共振面とのなす角度
が90°からすねないようK、出射光を軸として回転さ
せる方向である。
In FIG. 3, reference numeral 11 denotes a substrate made of GaAa, and in order to grow the active layer thinly and uniformly, the surface orientation of the substrate 11 is (
100) is tilted 1° from the plane. However, when a semiconductor laser is manufactured, the tilting direction is such that the angle between the main surface and the resonant surface does not deviate from 90 degrees, and the direction is such that the emitted light is rotated as an axis.

12〜14は液相エピタキシャル成長法によって得られ
た層で、12はAlxGap、As (X’; 0.4
5 )のクラッド層、13はAtz Ga+−1Aa 
(x ヘo、 ls )の活性層、14はGa Asの
コンタクト層である。
12 to 14 are layers obtained by liquid phase epitaxial growth, and 12 is AlxGap, As (X'; 0.4
5) cladding layer, 13 is Atz Ga+-1Aa
(x heo, ls) is an active layer, and 14 is a GaAs contact layer.

セして15はストライプ電極、16は基板側電極である
15 is a stripe electrode, and 16 is a substrate side electrode.

動作原理は従来と同じで、活性層13で発生した元が一
組の対向する(oli)、(oTx)面間を往復しなが
ら光増幅作用を受け、増幅率があるしきい値を超えた時
点で(Olj)面よりレーザー元として出射される。と
ころでこの発明では基板を傾けることにより薄く均一な
活性層13を得ることができるので活性層13に注入さ
れる電流は均一になり、注入電流によって発光された光
は散乱もなく均一に発光する。また基板11を傾ける方
向が出射光を軸に回転させる方向なので、出射光の方向
は基板11を傾けたkもがかわらず従来型と同様となり
、レーザチップをパッケージにマワントする場合にも支
障は起きない。
The operating principle is the same as the conventional one; the light generated in the active layer 13 is subjected to optical amplification while reciprocating between a pair of opposing (oli) and (oTx) surfaces, and the amplification factor exceeds a certain threshold. At this point, the light is emitted from the (Olj) plane as a laser source. By the way, in this invention, a thin and uniform active layer 13 can be obtained by tilting the substrate, so that the current injected into the active layer 13 becomes uniform, and the light emitted by the injected current is uniformly emitted without scattering. Furthermore, since the direction in which the substrate 11 is tilted is the direction in which the emitted light is rotated around the axis, the direction of the emitted light remains the same as in the conventional type even when the substrate 11 is tilted, and there is no problem when mounting a laser chip in a package. It doesn't happen.

以上第3図に示す電極ストライプ構造の半導体レーザに
ついて述べてきたが、内部ストライプレーザ、T J 
S (Tranaverae Junction 5t
ripe)レーザ等の他の半導体レーザ構造にも適用が
可能で、薄く均一な活性層をもった半導体レーザな得る
ことができる。
The semiconductor laser with the electrode stripe structure shown in FIG. 3 has been described above, but the internal stripe laser, TJ
S (Tranaverae Junction 5t
It is also possible to apply the present invention to other semiconductor laser structures such as a multilayer (ripe) laser, and it is possible to obtain a semiconductor laser having a thin and uniform active layer.

第4図に内部ストライプレーザに適用した実施例を、第
5図KTJSレーザに適用した実施例を示す。
FIG. 4 shows an embodiment applied to an internal stripe laser, and FIG. 5 shows an embodiment applied to a KTJS laser.

これらの図で、符号11〜14は第3図と同一部分を示
し、11は電極、18は電流1222層、19はZn拡
散によるP+部、20は拡散ドライブによるP部である
In these figures, numerals 11 to 14 indicate the same parts as in FIG. 3, 11 is an electrode, 18 is a current 1222 layer, 19 is a P+ part by Zn diffusion, and 20 is a P part by diffusion drive.

上記二つの実施例も活性層13を薄く均一に成長させる
ために基板11の面方位は(100)面から10傾げた
場合について示しているが、傾ける角度を0.2°〜5
°にした場合でも第3図で説明したのと同様な効果があ
る。
In the above two embodiments, the plane orientation of the substrate 11 is tilted by 10 degrees from the (100) plane in order to grow the active layer 13 thinly and uniformly.
Even when the angle is set to .degree., the same effect as explained in FIG. 3 can be obtained.

以上説明したように、この発明によれば基板結晶の主面
の面方位を、主面から特定の方向へわずかに傾けたので
、レーザ元の出射方向を傾けることなく、活性層が薄く
しかも均一な半導体レーザの製作が可能となり、特性が
良く信頼性の優れた半導体レーザな実現することができ
る。
As explained above, according to the present invention, the plane orientation of the main surface of the substrate crystal is slightly tilted in a specific direction from the main surface, so the active layer can be made thin and uniform without tilting the emission direction of the laser source. This makes it possible to manufacture semiconductor lasers with excellent characteristics and reliability.

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

第1図は従来の半導体レーザの一例を示す構造  ゛斜
視図、第2図は従来の半導体レーザで問題となっていた
成長層厚の不均一性を示す断面図、第3図はこの発明に
よる一実施例の構造斜視図、第4図と第5図はこの発明
を他の半導体レーザ構造に実施した場合の構造断面図を
示す。 図中、11はGaAsからなる基板、12はクラッド層
、13は活性層、14はコンタクト層、15はストライ
プ電極、16は基板側電極である。 代理人  葛 野 信 −(外1名) 第1図 第3図 第4図 第5図 手続補正書(自発) 1.事件の表示   特願昭58−18593号2、発
明の名称   半導体レーザ装置3、補正をする者 事件との関係 特許出願人 住 所    東京都千代田区丸の内二丁目2番3号名
 称  (601)三菱電機株式会社代表者片山仁八部 4、代理人 住 所    東京都千代田区丸の内二丁目2番3号5
、補正の対象 明細書の発明の詳細な説明の欄および図面6、補正の内
容 (1)明細書第2頁13行(7)r(011)Jを、r
<011)Jと補正する。 (2)図面第3図を別紙のように補正する。 以上
Fig. 1 is a perspective view of the structure of an example of a conventional semiconductor laser, Fig. 2 is a cross-sectional view showing the non-uniformity of the growth layer thickness, which has been a problem in conventional semiconductor lasers, and Fig. 3 is a structure according to the present invention. A perspective view of the structure of one embodiment, and FIGS. 4 and 5 show cross-sectional views of the structure when the present invention is applied to other semiconductor laser structures. In the figure, 11 is a substrate made of GaAs, 12 is a cladding layer, 13 is an active layer, 14 is a contact layer, 15 is a stripe electrode, and 16 is a substrate side electrode. Agent Shin Kuzuno - (1 other person) Figure 1 Figure 3 Figure 4 Figure 5 Procedural amendment (voluntary) 1. Indication of case: Japanese Patent Application No. 58-18593 2, Title of invention: Semiconductor laser device 3, Relationship with the person making the amendment: Address of patent applicant: 2-2-3 Marunouchi, Chiyoda-ku, Tokyo Name (601) Mitsubishi Denki Co., Ltd. Representative: Hitoshi Katayama 4, Agent Address: 2-2-3-5 Marunouchi, Chiyoda-ku, Tokyo
, Detailed Description of the Invention column of the specification subject to amendment and Drawing 6, Contents of the amendment (1) Page 2 of the specification, line 13 (7) r(011)J, r
<011) Corrected as J. (2) Amend Figure 3 of the drawing as shown in the attached sheet. that's all

Claims (4)

【特許請求の範囲】[Claims] (1)対向する一対の面を共振面とし、前記一対の面の
うち一万の面の方向を導波方向とする半導体レーザにお
いて、主面が前記導波方向を軸として0.2°〜5°傾
いていることを特徴とする半導体レーザ装置。
(1) In a semiconductor laser in which a pair of opposing surfaces are used as resonant surfaces and the waveguide direction is the direction of 10,000 of the pair of surfaces, the principal surface is 0.2° to 0.2° with respect to the waveguide direction as an axis. A semiconductor laser device characterized by being tilted by 5 degrees.
(2)主面は、(100)面であることを特徴とする特
許請求の範囲第(1)項記載の半導体レーザ装置。
(2) The semiconductor laser device according to claim (1), wherein the main surface is a (100) plane.
(3)主面は、(001)面であることを特徴とする特
許請求の範囲第(1)項記載の半導体レーザ装置。
(3) The semiconductor laser device according to claim (1), wherein the main surface is a (001) plane.
(4)主面は、(010)面であることを特徴とする特
許請求の範囲第(1)項記載の半導体レーザ装置。
(4) The semiconductor laser device according to claim (1), wherein the main surface is a (010) plane.
JP58016593A 1983-02-02 1983-02-02 Semiconductor laser device Pending JPS59141282A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58016593A JPS59141282A (en) 1983-02-02 1983-02-02 Semiconductor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58016593A JPS59141282A (en) 1983-02-02 1983-02-02 Semiconductor laser device

Publications (1)

Publication Number Publication Date
JPS59141282A true JPS59141282A (en) 1984-08-13

Family

ID=11920572

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58016593A Pending JPS59141282A (en) 1983-02-02 1983-02-02 Semiconductor laser device

Country Status (1)

Country Link
JP (1) JPS59141282A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4958355A (en) * 1989-03-29 1990-09-18 Rca Inc. High performance angled stripe superluminescent diode
US5329134A (en) * 1992-01-10 1994-07-12 International Business Machines Corporation Superluminescent diode having a quantum well and cavity length dependent threshold current

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5662386A (en) * 1979-10-29 1981-05-28 Hitachi Ltd Manufacture of semiconductor device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5662386A (en) * 1979-10-29 1981-05-28 Hitachi Ltd Manufacture of semiconductor device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4958355A (en) * 1989-03-29 1990-09-18 Rca Inc. High performance angled stripe superluminescent diode
US5329134A (en) * 1992-01-10 1994-07-12 International Business Machines Corporation Superluminescent diode having a quantum well and cavity length dependent threshold current
US5556795A (en) * 1992-01-10 1996-09-17 International Business Machines Corporation Quantum well superluminescent diode

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