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JP2922010B2 - Semiconductor laser device - Google Patents
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JP2922010B2 - Semiconductor laser device - Google Patents

Semiconductor laser device

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Publication number
JP2922010B2
JP2922010B2 JP9051091A JP9051091A JP2922010B2 JP 2922010 B2 JP2922010 B2 JP 2922010B2 JP 9051091 A JP9051091 A JP 9051091A JP 9051091 A JP9051091 A JP 9051091A JP 2922010 B2 JP2922010 B2 JP 2922010B2
Authority
JP
Japan
Prior art keywords
layer
semiconductor
semiconductor layer
laser device
type
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
JP9051091A
Other languages
Japanese (ja)
Other versions
JPH04322482A (en
Inventor
浩樹 内藤
裕一 清水
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP9051091A priority Critical patent/JP2922010B2/en
Priority to US07/871,913 priority patent/US5297158A/en
Publication of JPH04322482A publication Critical patent/JPH04322482A/en
Application granted granted Critical
Publication of JP2922010B2 publication Critical patent/JP2922010B2/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】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明はコンパクトディスク、プ
リンタ等の光源として用いる低い動作電流値の半導体レ
ーザ装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor laser device having a low operating current value used as a light source for a compact disk, a printer or the like.

【0002】[0002]

【従来の技術】以下に従来の半導体レーザ装置について
説明する。図4は従来の半導体レーザ装置の断面図であ
る。n型のガリウムヒ素(GaAs)基板21の上にn
型GaAsバッファ層が形成されており、その上にn型
のガリウムアルミヒ素(GaAlAs)クラッド層2
3、GaAlAs活性層24、リッジ25aを有するp
型のGaAlAsクラッド層25があり、電流狭窄のた
めにリッジ25a以外の部分にはn型のGaAs電流ブ
ロック層26が形成されている。なお27はp型のGa
As保護層、28はp型のGaAsコンタクト層であ
る。この構造において、p型のGaAsコンタクト層2
8から注入される電流は、リッジ25a内に有効に閉じ
込められ、リッジ25aの下部のGaAlAs活性層2
4でレ−ザ発振が生じる。横モードはGaAlAs活性
層24より禁制帯幅が小さいn型のGaAs電流ブロッ
ク層26が、リッジ25a以外の部分でレ−ザ光を吸収
することにより制御され、レーザ光もリッジ25a内に
閉じ込められている。すなわち、GaAsの屈折率はG
aAlAsよりも高いが、リッジ25aの外のレ−ザ光
は吸収されるので、レーザ光はリッジ25a内に閉じ込
められる。一般に、リッジ25aの幅を5μm程度にす
ることで、コンパクトディスクやプリンタなどに使われ
る単一モ−ドのレ−ザ光が得られる。
2. Description of the Related Art A conventional semiconductor laser device will be described below. FIG. 4 is a sectional view of a conventional semiconductor laser device. On an n-type gallium arsenide (GaAs) substrate 21, n
Type GaAs buffer layer is formed, and an n-type gallium aluminum arsenide (GaAlAs) cladding layer 2 is formed thereon.
3, p having GaAlAs active layer 24 and ridge 25a
There is a GaAlAs cladding layer 25 of an n-type, and an n-type GaAs current blocking layer 26 is formed in a portion other than the ridge 25a for current confinement. 27 is a p-type Ga
The As protective layer 28 is a p-type GaAs contact layer. In this structure, the p-type GaAs contact layer 2
8 is effectively confined in the ridge 25a and the GaAlAs active layer 2 below the ridge 25a.
At 4, laser oscillation occurs. The lateral mode is controlled by the n-type GaAs current blocking layer 26 having a smaller forbidden band width than the GaAlAs active layer 24 absorbing laser light in portions other than the ridge 25a, and the laser light is also confined in the ridge 25a. ing. That is, the refractive index of GaAs is G
Although higher than aAlAs, the laser light outside the ridge 25a is absorbed, so that the laser light is confined in the ridge 25a. Generally, by setting the width of the ridge 25a to about 5 μm, a single mode laser beam used for a compact disk, a printer, or the like can be obtained.

【0003】[0003]

【発明が解決しようとする課題】近年、光ピックアップ
の小型化に伴い、より動作電流が低く発熱が少ないレー
ザが要望されている。しかしながら上記の従来の構成で
は、n型のGaAs電流ブロック層の光の吸収による導
波路の損失によりレーザのしきい値および効率が制限さ
れるという課題を有していた。
In recent years, with the miniaturization of optical pickups, there has been a demand for a laser having a lower operating current and less heat generation. However, the above-described conventional configuration has a problem that the threshold and efficiency of the laser are limited by the loss of the waveguide due to the absorption of light in the n-type GaAs current blocking layer.

【0004】本発明は上記従来の課題を解決するもの
で、動作電流の低い半導体レーザ装置を提供することを
目的とする。
An object of the present invention is to solve the above conventional problems and to provide a semiconductor laser device having a low operating current.

【0005】[0005]

【課題を解決するための手段】この目的を達成するため
に本発明の半導体レーザ装置は、GaAsの半導体基板
の上に、活性層となるGaAsまたはGaAlAsから
なる第1の半導体層を挟んで、第1の半導体層よりも禁
制帯幅が大きく、互いに異なる導電型のGaAlAsか
らなる第2、第3の半導体層が形成されており、前記第
2の半導体層の一部にリッジが形成されており、前記リ
ッジ形状以外の領域に前記第2の半導体層よりAlAs
混晶比が略0.05大きく、かつ前記第2の半導体層と
は異なる導電型のGaAlAsからなる第4の半導体層
が形成された構成を有している。
In order to achieve this object, a semiconductor laser device according to the present invention comprises a GaAs semiconductor substrate with a first semiconductor layer of GaAs or GaAlAs serving as an active layer interposed therebetween. the first larger forbidden band width than the semiconductor layer, a second of different conductivity type GaAlAs each other, is formed a third semiconductor layer, said Li Tsu di part of the second semiconductor layer is formed In the region other than the ridge shape, AlAs is deposited from the second semiconductor layer.
The fourth embodiment has a structure in which a fourth semiconductor layer made of GaAlAs having a mixed crystal ratio of about 0.05 and a conductivity type different from that of the second semiconductor layer is formed.

【0006】[0006]

【作用】この構成によって、第4の半導体層で注入電流
はリッジ内に狭窄され、レーザ発振がリッジの下部の活
性層で生じる。ここで、第4の半導体層の屈折率が第2
の半導体層よりも小さいので、レ−ザ光はリッジの下部
に閉じ込められ、単一横モードが得られる。従来の半導
体レーザ装置のように、電流ブロック層の吸収によるレ
ーザ光の閉じ込めではないので、導波路の損失は大幅に
低減できる。すなわち、レ−ザ発振のしきい値は低く、
効率が高くなるので、大幅に動作電流値を低減できる。
With this configuration, the injection current is confined in the ridge in the fourth semiconductor layer, and laser oscillation occurs in the active layer below the ridge. Here, the refractive index of the fourth semiconductor layer is the second
Laser light is confined below the ridge, and a single transverse mode is obtained. Unlike the conventional semiconductor laser device, the laser beam is not confined by the absorption of the current blocking layer, so that the loss of the waveguide can be greatly reduced. That is, the threshold value of laser oscillation is low,
Since the efficiency is increased, the operating current value can be significantly reduced.

【0007】[0007]

【実施例】以下本発明の一実施例について、図面を参照
しながら説明する。図1は本発明の一実施例における半
導体レーザ装置の断面図である。n型のGaAs基板1
の上にn型のGaAsバッファ層2が形成されており、
その上にn型のGa0.5Al0.5Asクラッド層3、Ga
0.9Al0.1As活性層4、リッジ5aを有するp型のG
0.5Al0.5Asクラッド層5が形成されており、電流
狭窄のためにリッジ5a以外の領域にはn型のGa0.45
Al0.55As層6が形成されている。なお7はp型のG
aAs保護層、8はp型のGaAsコンタクト層であ
る。この構造において、p型のGaAsコンタクト層8
から注入される電流は、リッジ5a内に有効に閉じ込め
られ、リッジ5aの下部のGa0.9Al0.1As活性層3
でレ−ザ発振が生じる。横モードのレーザ光は、n型の
Ga0.45Al0.55As層6の屈折率がp型のGa0.5
0.5Asクラッド層5よりも小さいので、リッジ5a
の下部に閉じ込められる。この場合、横方向のレーザ光
の閉じ込めは吸収ではなく、材料の屈折率の差によるも
のなので、導波路の損失は小さく、動作電流値の小さい
半導体レ−ザ装置が得られる。
An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a sectional view of a semiconductor laser device according to one embodiment of the present invention. n-type GaAs substrate 1
An n-type GaAs buffer layer 2 is formed on
An n-type Ga 0.5 Al 0.5 As clad layer 3 and Ga
P-type G having 0.9 Al 0.1 As active layer 4 and ridge 5a
An a 0.5 Al 0.5 As cladding layer 5 is formed, and an n-type Ga 0.45
An Al 0.55 As layer 6 is formed. 7 is a p-type G
The aAs protection layer 8 is a p-type GaAs contact layer. In this structure, the p-type GaAs contact layer 8
Is effectively confined in the ridge 5a, and the Ga 0.9 Al 0.1 As active layer 3 below the ridge 5a.
Causes laser oscillation. The transverse mode laser beam is obtained by converting the refractive index of the n-type Ga 0.45 Al 0.55 As layer 6 to the p-type Ga 0.5 A.
l 0.5 As clad layer 5 is smaller than
Trapped at the bottom of In this case, the confinement of the laser light in the lateral direction is not due to the absorption but to the difference in the refractive index of the material, so that a semiconductor laser device having a small waveguide loss and a small operating current value can be obtained.

【0008】図2は本発明の一実施例における半導体レ
ーザ装置の製造工程図である。図2(a)に示すよう
に、n型のGaAs基板1の上に、MOCVD成長法に
より、n型のGaAsバッファ層2、n型のGa0.5
0.5Asクラッド層3、Ga0.9Al0.1As活性層
4、p型のGa0.5Al0.5Asクラッド層5、p型のG
aAs保護層7を形成する。次に図2(b)に示すよう
に、ストライプ状に窒化膜9を形成し、この窒化膜9を
マスクとしてエッチングを行い、リッジ5aを形成す
る。次に図2(c)に示すように、減圧MOCVD法に
より、n型のGa0. 45Al0.55As層6を選択的に成長
させる。次に図2(d)に示すように、窒化膜9を除去
し、p型のGaAsコンタクト層8を成長させる。なお
本実施例ではGaAlAs系の材料を用いたが、他の化
合物半導体材料を用いてもよい。
FIG. 2 is a manufacturing process diagram of a semiconductor laser device according to one embodiment of the present invention. As shown in FIG. 2A, an n-type GaAs buffer layer 2 and an n-type Ga 0.5 A are formed on an n-type GaAs substrate 1 by MOCVD growth.
l 0.5 As clad layer 3, Ga 0.9 Al 0.1 As active layer 4, p-type Ga 0.5 Al 0.5 As clad layer 5, p-type G
An aAs protective layer 7 is formed. Next, as shown in FIG. 2B, a nitride film 9 is formed in a stripe shape, and etching is performed using the nitride film 9 as a mask to form a ridge 5a. Next, as shown in FIG. 2 (c), the pressure MOCVD method, selectively growing a Ga 0. 45 Al 0.55 As layer 6 of n-type. Next, as shown in FIG. 2D, the nitride film 9 is removed, and a p-type GaAs contact layer 8 is grown. In this embodiment, a GaAlAs-based material is used, but another compound semiconductor material may be used.

【0009】図3は本発明の一実施例における半導体レ
−ザ装置の電流−光出力特性図である。比較のために従
来の半導体レーザ装置の特性も併せて示した。図3に示
すように、本実施例の半導体レーザ装置では光の損失が
小さいため、しきい値が低く、効率が高くなり、動作電
流値が小さくなっている。具体的には、室温で3mWの
レーザ光を放出させるための動作電流値を従来の50m
Aから30mAに低減できた。
FIG. 3 is a current-light output characteristic diagram of a semiconductor laser device according to one embodiment of the present invention. The characteristics of the conventional semiconductor laser device are also shown for comparison. As shown in FIG. 3, in the semiconductor laser device of this embodiment, since the loss of light is small, the threshold value is low, the efficiency is high, and the operating current value is small. Specifically, the operating current value for emitting a laser beam of 3 mW at room temperature is reduced to 50 m of the conventional value.
A could be reduced to 30 mA.

【0010】[0010]

【発明の効果】以上のように本発明は、GaAsの半導
体基板の上に、活性層となるGaAsまたはGaAlA
sからなる第1の半導体層を挟んで、第1の半導体層よ
りも禁制帯幅が大きく、互いに異なる導電型のGaAl
Asからなる第2、第3の半導体層が形成されており、
前記第2の半導体層の一部にリッジが形成されており、
前記リッジ形状以外の領域に前記第2の半導体層よりA
lAs混晶比が略0.05大きく、かつ前記第2の半導
体層とは異なる導電型のGaAlAsからなる第4の半
導体層が形成された構成とすることにより、動作電流値
が従来と比べて大幅に低い優れた半導体レーザ装置を実
現できるものである。このような半導体レーザ装置は、
光ピックアップの小型化を要求されているコンパクトデ
ィスクやプリンタ用の光源に使用して、効果を発揮する
ものである。
As described above, the present invention provides a semiconductor device of GaAs.
GaAs or GaAlA to be an active layer on a substrate
s with the first semiconductor layer of s interposed therebetween.
GaAl with different forbidden band width and different conductivity types
Second and third semiconductor layers made of As are formed;
A ridge is formed in a part of the second semiconductor layer;
In the region other than the ridge shape, A
The ratio of As mixed crystal is approximately 0.05 large and the second semiconductor
By adopting a structure in which the fourth semiconductor layer made of GaAlAs having a conductivity type different from that of the body layer is formed, an excellent semiconductor laser device having an operation current value significantly lower than that of a conventional semiconductor laser device can be realized. Such a semiconductor laser device,
It is effective when used as a light source for compact discs and printers, for which miniaturization of optical pickups is required.

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

【図1】本発明の一実施例における半導体レーザ装置の
断面図
FIG. 1 is a sectional view of a semiconductor laser device according to an embodiment of the present invention.

【図2】本発明の一実施例における半導体レーザ装置の
製造工程図
FIG. 2 is a manufacturing process diagram of a semiconductor laser device according to an embodiment of the present invention.

【図3】本発明の一実施例における半導体レ−ザ装置の
電流−光出力特性図
FIG. 3 is a current-light output characteristic diagram of a semiconductor laser device according to an embodiment of the present invention.

【図4】従来の半導体レーザ装置の断面図FIG. 4 is a cross-sectional view of a conventional semiconductor laser device.

【符号の説明】[Explanation of symbols]

1 n型のGaAs基板(半導体基板) 3 n型のGa0.5Al0.5Asクラッド層(第3の半導
体層) 4 Ga0.9Al0.1As活性層(第1の半導体層) 5 p型のGa0.5Al0.5Asクラッド層(第2の半導
体層) 5a リッジ 6 n型のGa0.45Al0.55As層(第4の半導体層)
1 n-type GaAs substrate (semiconductor substrate) 3 n-type Ga 0.5 Al 0.5 As clad layer (third semiconductor layer) 4 Ga 0.9 Al 0.1 As active layer (first semiconductor layer) 5 p-type Ga 0.5 Al 0.5 As clad layer (second semiconductor layer) 5a Ridge 6 n-type Ga 0.45 Al 0.55 As layer (fourth semiconductor layer)

───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H01S 3/18 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 6 , DB name) H01S 3/18

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 GaAsの半導体基板の上に、活性層と
なるGaAsまたはGaAlAsからなる第1の半導体
層を挟んで、前記第1の半導体層よりも禁制帯幅が大き
く、互いに異なる導電型のGaAlAsからなる第2、
第3の半導体層が形成されており、前記第2の半導体層
の一部にリッジが形成されており、前記リッジ形状以外
の領域に前記第2の半導体層よりAlAs混晶比が略
0.05大きく、かつ前記第2の半導体層とは異なる導
電型のGaAlAsからなる第4の半導体層が形成され
ている半導体レーザ装置。
1. A semiconductor device comprising a GaAs semiconductor substrate having a first semiconductor layer made of GaAs or GaAlAs serving as an active layer interposed therebetween, having a larger forbidden band width than that of the first semiconductor layer and having different conductivity types. A second made of GaAlAs,
The third semiconductor layer is formed, the part of the second semiconductor layer and Li Tsu di is formed, AlAs mixed crystal ratio than the second semiconductor layer in a region other than the ridge is substantially
A semiconductor laser device having a fourth semiconductor layer made of GaAlAs, which is 0.05 larger and has a conductivity type different from that of the second semiconductor layer.
JP9051091A 1991-04-22 1991-04-22 Semiconductor laser device Expired - Fee Related JP2922010B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP9051091A JP2922010B2 (en) 1991-04-22 1991-04-22 Semiconductor laser device
US07/871,913 US5297158A (en) 1991-04-22 1992-04-21 Semiconductor laser device including a gallium-aluminum arsenic compound

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9051091A JP2922010B2 (en) 1991-04-22 1991-04-22 Semiconductor laser device

Publications (2)

Publication Number Publication Date
JPH04322482A JPH04322482A (en) 1992-11-12
JP2922010B2 true JP2922010B2 (en) 1999-07-19

Family

ID=14000473

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9051091A Expired - Fee Related JP2922010B2 (en) 1991-04-22 1991-04-22 Semiconductor laser device

Country Status (1)

Country Link
JP (1) JP2922010B2 (en)

Also Published As

Publication number Publication date
JPH04322482A (en) 1992-11-12

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