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JPH0138390B2 - - Google Patents
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JPH0138390B2 - - Google Patents

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Publication number
JPH0138390B2
JPH0138390B2 JP7667885A JP7667885A JPH0138390B2 JP H0138390 B2 JPH0138390 B2 JP H0138390B2 JP 7667885 A JP7667885 A JP 7667885A JP 7667885 A JP7667885 A JP 7667885A JP H0138390 B2 JPH0138390 B2 JP H0138390B2
Authority
JP
Japan
Prior art keywords
layer
type
optical waveguide
current confinement
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
Application number
JP7667885A
Other languages
Japanese (ja)
Other versions
JPS61236185A (en
Inventor
Toshiaki Fukunaga
Hisao Nakajima
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP7667885A priority Critical patent/JPS61236185A/en
Publication of JPS61236185A publication Critical patent/JPS61236185A/en
Publication of JPH0138390B2 publication Critical patent/JPH0138390B2/ja
Granted legal-status Critical Current

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  • Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
  • Semiconductor Lasers (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野) この発明は、AlGaAs系材料を用いた横モード
制御半導体レーザ素子の製造法に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention relates to a method for manufacturing a transverse mode control semiconductor laser device using an AlGaAs - based material.

(従来の技術) 従来の横モード制御半導体レーザ素子の一例
は、第4図に示すようにn型GaAs基板1上にn
型AlzGa1-zAsクラツド層2、p型AlwGa1-wAs活
性層3、p型AlxGa1-xAs光導波層4、n型GaAs
電流狭窄層5、p型AlyGa1-yAsクラツド層6、
p型GaAsコンタクト層7を積層して構成される。
(Prior Art) An example of a conventional transverse mode control semiconductor laser device is as shown in FIG .
type Al z Ga 1-z As cladding layer 2, p-type Al w G a1-w As active layer 3, p-type Al x G a1-x As optical waveguide layer 4, n-type Ga A s
Current confinement layer 5, p-type Al y G a1-y As cladding layer 6,
It is constructed by stacking p-type GaAs contact layers 7.

(発明が解決しようとする問題点) 以上の横モード制御半導体レーザ素子を有機金
属気相エピタキシヤル(OMVPE)成長法により
製造する場合にはn型GaAs基板1上にn型Alz
Ga1-zAsクラツド層2、p型AlwGa1-wAs活性層
3、p型AlxGa1-xAs光導電波層4、n型GaAs
流狭窄層5を積層し、次に電流狭窄層5を選択的
にエツチングしてp型AlxGa1-xAs光導波層4を
露出させた後、電流狭窄層5及びエツチングによ
り露出した光導電波層4上にp型AlyGa1-yAsク
ラツド層6、p型GaAsコンタクト層7を積層す
る方法が採用されている。
(Problems to be Solved by the Invention) When manufacturing the above-mentioned transverse mode control semiconductor laser device by the organic metal vapor phase epitaxial (OMVPE) growth method, n-type Al z is grown on the n-type Ga A s substrate 1.
A Ga 1-z As cladding layer 2, a p-type Al w Ga 1-w As active layer 3, a p-type Al x Ga 1-x As photoconductive wave layer 4, and an n-type Ga As current confinement layer 5 are laminated, Next, the current confinement layer 5 is selectively etched to expose the p-type Al x Ga 1-x As optical waveguide layer 4, and then the p-type Al A method is adopted in which a y Ga 1-y As cladding layer 6 and a p-type Ga As contact layer 7 are laminated.

即ち、所謂2回のOMVPE成長による製造法が
採用されているが、この場合光導波層4をエツチ
ングにより部分的に大気中に晒らした後、この上
にp型AlyGa1-yAsクラツド層6を積層するため、
光導波層4とクラツド層6との界面に酸化により
高抵抗な部分が出来易いという欠点がある。
That is, a manufacturing method using so-called two-time OMVPE growth is adopted, but in this case, after the optical waveguide layer 4 is partially exposed to the atmosphere by etching, p-type Al y Ga 1-y As is deposited thereon. In order to laminate the cladding layer 6,
A drawback is that a high resistance portion is easily formed at the interface between the optical waveguide layer 4 and the cladding layer 6 due to oxidation.

また第4図に示すような横モード制御半導体レ
ーザ素子を分子線エピタキシヤル(MBE)成長
法により製造する場合にはp型AlxGa1-xAs光導
波層4上にGaAs層の薄膜を形成してからn型Ga
As電流狭窄層5を積層し、その後上記GaAsの薄
膜を残して電流狭窄層5をエツチングして、次の
成長時に高温にしてAs圧下でGaAsの薄膜を蒸発
させてp型AlyGa1-yAsクラツド層6を積層する
方法が採用されている。
In addition , when manufacturing a transverse mode control semiconductor laser device as shown in FIG. After forming a thin film of n-type Ga
The A s current confinement layer 5 is laminated, and then the current confinement layer 5 is etched , leaving the above Ga s thin film, and during the next growth, the Ga s thin film is evaporated at a high temperature under As pressure. A method of laminating a p-type Al y Ga 1-y As cladding layer 6 is adopted.

この方法は2回のエピタキシヤル成長により横
モード制御半導体レーザ素子を製造することにお
いては上記OMVPE成長法と変わりがないが、光
導電波層4は次の成長時までGaAs薄膜で被覆さ
れているため、光導電波層4とクラツド層6との
界面に高低抗な部分が残ることは少ない。
This method is the same as the OMVPE growth method described above in that a transverse mode control semiconductor laser device is manufactured by two epitaxial growth steps, but the photoconductive wave layer 4 is covered with a GaAs thin film until the next growth. Therefore, it is rare for a high-low resistance portion to remain at the interface between the photoconductive wave layer 4 and the cladding layer 6.

しかし、この方法では、GaAsの薄膜を高温
(750℃)短時間(〜10分)で蒸発させるので、基
板温度の精密な温度コントロール及びこの薄膜の
厚み制御が必要となる。また、下地のAlxGa1-x
Asのxが0.4よりも大きい時には、下地の酸化に
よる高抵抗層ができるという欠点が生じるので、
発振波長の短波長化(740nm以下)が困難とな
る。
However, in this method, the thin film of Ga As is evaporated at high temperature (750° C.) in a short time (~10 minutes), so precise temperature control of the substrate temperature and control of the thickness of the thin film are required. In addition, the underlying Al x Ga 1-x
When x of As is larger than 0.4, there is a disadvantage that a high resistance layer is formed due to oxidation of the base.
It becomes difficult to shorten the oscillation wavelength (740 nm or less).

この発明の目的は、AlGaAs系材料を用い、2
回のエピタキシヤル成長により例えば横モード制
御内部ストライプ半導体レーザ素子を製造するに
際して生ずる以上のような問題点を解決すること
にある。
The purpose of this invention is to use AlG a As based material,
The object of the present invention is to solve the above-mentioned problems that occur when manufacturing, for example, a transverse mode controlled internal stripe semiconductor laser device by epitaxial growth.

(問題点を解決するための手段) この目的のために、この発明では以上のように
内部に光導波層、電流狭窄層、クラツド層の積層
を有するAlGaAs系材料を用いた半導体レーザに
おいて、上記光導波層上に被覆層を形成して該被
覆層上に電流狭窄層を成長させ、更に該電流狭窄
層を選択的にエツチングし、次にエツチング部分
の被覆層を通常の成長温度で蒸発させてからクラ
ツド層を成長させるようにして上記半導体レーザ
を製造する方法を提案するものである。
(Means for Solving the Problems) For this purpose, the present invention provides a semiconductor laser using an AlG a As material, which has an optical waveguide layer, a current confinement layer, and a clad layer stacked therein as described above. In this step, a coating layer is formed on the optical waveguide layer, a current confinement layer is grown on the coating layer, the current confinement layer is selectively etched, and then the etched portion of the coating layer is heated to a normal growth temperature. The present invention proposes a method for manufacturing the above-mentioned semiconductor laser by evaporating the cladding layer and then growing the cladding layer.

ここで、被覆層に適する物質としてはGaAs
成長できる最低温度(450℃)以上で光導波層上
に約100Å程度の厚みの被覆層を成長させること
ができ、且つ通常の成長温度(約650℃)で蒸発
させることができることが好ましく、具体的には
InAs、InP、InSb等のIn系化合物の1種又は2種
以上を使用する。
Here, the material suitable for the coating layer is one that can grow a coating layer with a thickness of about 100 Å on the optical waveguide layer at a temperature higher than the lowest temperature at which GaAs can grow (450°C), and at a normal growth temperature. It is preferable that it can be evaporated at (approximately 650℃), specifically
One or more In-based compounds such as InAs, InP, and InSb are used.

(発明の効果) 以上要するに、この発明によれば光導波層上に
形成した被覆層を残して電流狭窄層をエツチング
し、次にエツチング部分の被覆層を通常の成長温
度で蒸発させてからクラツド層を成長させるた
め、光導波層を次のクラツド層成長までの間大気
中に晒らさないで済み、したがつて光導波層とク
ラツド層との界面に高抵抗部分が生成することが
ない。
(Effects of the Invention) In summary, according to the present invention, the current confinement layer is etched leaving the coating layer formed on the optical waveguide layer, and then the coating layer in the etched portion is evaporated at a normal growth temperature. Since the optical waveguide layer is grown, the optical waveguide layer is not exposed to the atmosphere until the next cladding layer grows, and therefore a high resistance part is not generated at the interface between the optical waveguide layer and the cladding layer. .

また、被覆層は通常の成長温度で蒸発させてか
らクラツド層を成長させているため、高温によつ
て活性層の量子井戸構造が破壊されることなく、
したがつてこの発明により得られる半導体レーザ
素子は低動作電流、高出力までの横基本モード発
振でき、しかも雑音特性が良好であるため、デイ
ジタルオーデイオデイスク、光デイスクメモリ、
レーザービームプリンター等の光源として最適で
ある。
In addition, since the cladding layer is grown after the coating layer is evaporated at a normal growth temperature, the quantum well structure of the active layer is not destroyed by high temperatures.
Therefore, the semiconductor laser device obtained by the present invention can oscillate in the transverse fundamental mode with low operating current and high output, and has good noise characteristics, so it can be used in digital audio disks, optical disk memories,
Ideal as a light source for laser beam printers, etc.

(実施例) 以下、この発明を図示の実施例に基いて説明す
る。
(Example) The present invention will be explained below based on the illustrated example.

実施例 1 第1図は、この発明の製造工程の一例を示すも
ので、n型GaAs基板1の(001)面の上には、第
1図aに示すようにMBE或いはOMVPE成長法
等によつてn型GaAsバツフア層8、n型Alx
Ga1-xAs/GaAs多重量子井戸バツフア層9、n
型AlxGa1-xAsクラツド層10、p型AlyGa1-yAs
活性層11、p型AlzGa1-xAs光導波層12、被
覆層13、n型GaAs電流狭窄層14を積層する。
Embodiment 1 FIG. 1 shows an example of the manufacturing process of the present invention. On the (001) plane of an n -type GaAs substrate 1, MBE or OMVPE is grown as shown in FIG. 1a. The n-type G a A s buffer layer 8 and the n-type Al x
Ga 1-x As/G a A s multiple quantum well buffer layer 9, n
type Al x Ga 1-x As cladding layer 10, p-type Al y Ga 1-y As
An active layer 11, a p-type Al z Ga 1-x As optical waveguide layer 12 , a coating layer 13 , and an n-type Ga As current confinement layer 14 are laminated.

なお、Alの組成は用途によつて異なるが、x
>z>yのように定める。
Note that the composition of Al varies depending on the application, but x
>z>y.

多重量子井戸バツフア層9はOMVPE成長法で
は省略してもよく、活性層11はアンドープの多
重量子井戸(MQW)、単一量子井戸(SQW)い
ずれでもよい。
The multiple quantum well buffer layer 9 may be omitted in the OMVPE growth method, and the active layer 11 may be either an undoped multiple quantum well (MQW) or a single quantum well (SQW).

被覆層13はInAsを用いて光導波層12上に
温度450℃程度で約100Å成長させて形成する。
The covering layer 13 is formed by growing InAs on the optical waveguide layer 12 to a thickness of about 100 Å at a temperature of about 450°C.

またn型GaAs電流狭窄層14は、発振光によ
つて励起される少数キヤリアの拡散を防ぐため
に、キヤリア濃度を3×1018cm-3以上、厚みを約
1μmとするとともに、横モード制御のためにp
型AlzGa1-zAs光導波層12の厚みを薄くして
(例えば0.3μm程度)、電流狭窄層14による横方
向の有効屈折率を減少させるようにしてある。
In addition, the n-type Ga As current confinement layer 14 has a carrier concentration of 3×10 18 cm -3 or more and a thickness of approximately
1μm and p for transverse mode control.
The thickness of the Al z Ga 1-z As optical waveguide layer 12 is made thin (for example, about 0.3 μm) to reduce the effective refractive index in the lateral direction due to the current confinement layer 14 .

なお、被覆層13上にエツチングストツプ層と
してGe、Si等を薄く積層してもよい。
Note that Ge, Si, etc. may be thinly laminated on the covering layer 13 as an etching stop layer.

次に、第1図bに示すように電流狭窄層14の
(110)方向に選択エツチングにより溝15を形成
する。
Next, as shown in FIG. 1B, grooves 15 are formed in the current confinement layer 14 in the (110) direction by selective etching.

なお溝15はその幅を横モード制御に必要な広
さ(〜3μm)とし、被覆層13を露出させる。
Note that the width of the groove 15 is set to a width (~3 μm) necessary for transverse mode control, and the coating layer 13 is exposed.

最後に第1図cに示すように、成長前にAs圧
を加えながら温度600℃で被覆層13を蒸発させ
てからp型AlxGa1-xAsクラツド層16、p型Ga
Asコンタクト層17を成長させ、次にp側電極
18、n側電極19を蒸着によつて形成する。
Finally, as shown in FIG. 1c, before growth, the coating layer 13 is evaporated at a temperature of 600°C while applying As pressure, and then the p-type Al x Ga 1-x As cladding layer 16 and the p-type Ga
A s contact layer 17 is grown, and then a p-side electrode 18 and an n-side electrode 19 are formed by vapor deposition.

このようにして製造された半導体レーザ素子は
p側電極18を接地してn側電極19に負電圧を
加えることによつて電流はn型GaAs電流狭窄層
14によつて狭窄され、活性層11に注入され
る。溝15の直下で発振した光はn型GaAs電流
狭窄層14に吸収され、接合面に平行方向に屈折
率差がつき、高出力までの横基本モード発振が確
保できる。
In the semiconductor laser device manufactured in this way, by grounding the p-side electrode 18 and applying a negative voltage to the n-side electrode 19, the current is constricted by the n-type GaAs current confinement layer 14. is implanted into the active layer 11. The light oscillated directly under the groove 15 is absorbed by the n-type GaAs current confinement layer 14, and a refractive index difference is created in the direction parallel to the junction surface, thereby ensuring transverse fundamental mode oscillation up to high output.

実施例 2 第2図は、この発明により製造された他の半導
体レーザ素子を示すもので、n型GaAs基板1の
(001)面上にMBE或いはOMVPE成長法等によ
つてn型GaAsバツフア層8、n型AlxGa1-xAs/
GaAs多重量子井戸バツフア層9、n型AlxGa1-x
Asクラツド層10、n型光導波層12a(厚み
0.3μm)、アンドープ単一量子井戸或いはアンド
ープ多重量子井戸活性層11a、p型光導波層1
2b(厚み0.3μm)、被覆層13(厚み〜100Å)、
n型GaAs電流狭窄層14を積層する。
Example 2 FIG. 2 shows another semiconductor laser device manufactured according to the present invention. G a A s buffer layer 8, n-type Al x Ga 1-x As/
G a A s multiple quantum well buffer layer 9, n-type Al x Ga 1-x
As cladding layer 10, n-type optical waveguide layer 12a (thickness
0.3 μm), undoped single quantum well or undoped multiple quantum well active layer 11a, p-type optical waveguide layer 1
2b (thickness 0.3 μm), coating layer 13 (thickness ~ 100 Å),
An n-type GaAs current confinement layer 14 is laminated.

この場合、n型乃至p型光導波層12a,12
bは第3図に示すように光及び電流の閉じ込みを
良好に行なわせるために、Alの組成を活性層1
1aに向けて徐々に減少させる構造としてある。
In this case, the n-type to p-type optical waveguide layers 12a, 12
b, as shown in Figure 3, the composition of Al is changed to the active layer 1 in order to achieve good confinement of light and current.
It has a structure in which it gradually decreases toward 1a.

なお、n型乃至p型光導波層12a,12bに
おける最低のAl組成x、及び活性層11aにお
ける多重量子井戸の数、バリヤーのAl組成や厚
み、井戸の厚み及びAlの組成等は用途によつて
最低の閾値電流で発振するように設定してある。
また被覆層13は実施例1と同様にIn化合物を使
用して形成する。
Note that the lowest Al composition x in the n-type to p-type optical waveguide layers 12a and 12b, the number of multiple quantum wells in the active layer 11a, the Al composition and thickness of the barrier, the thickness of the wells, the composition of Al, etc. depend on the application. It is set to oscillate at the lowest threshold current.
Further, the covering layer 13 is formed using an In compound as in Example 1.

次にn型GaAs電流狭窄層14に選択エツチン
グによつて溝15を形成し、被覆層13を露出さ
せる。最後に成長前にAs圧を加えながら温度650
℃で被覆層13を蒸発させてからp型AlxGa1-x
Asクラツド層16、p型GaAsコンタクト層17
を成長させ、次にp側電極18、n側電極19を
蒸着によつて形成する。
Next, a groove 15 is formed in the n-type GaAs current confinement layer 14 by selective etching, and the covering layer 13 is exposed. Finally, before growth, the temperature was raised to 650 while applying As pressure.
After evaporating the coating layer 13 at ℃, p-type Al x Ga 1-x
As clad layer 16, p-type Ga As contact layer 17
is grown, and then a p-side electrode 18 and an n-side electrode 19 are formed by vapor deposition.

このようにして製造された半導体レーザ素子は
実施例1と同様にして動作させることができる。
The semiconductor laser device manufactured in this way can be operated in the same manner as in the first embodiment.

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

第1図は、この発明の製造工程の一例を示すも
ので、第1図aは第1回目のエピタキシヤル成長
工程を示す図、第1図bは電流狭窄層に選択エツ
チングにより溝を作成する工程を示す図、第1図
cは第2回目のエピタキシヤル成長と電極付けの
工程を示す図、第2図はこの発明により製造され
た他の半導体レーザ素子の斜視図、第3図は同上
の半導体レーザ素子の内層におけるAl含有量の
関係を示す図、第4図は従来の方法により製造さ
れた半導体レーザ素子の一例を示す斜視図であ
る。 図中、12,12a,12bは光導波層、13
は被覆層、14は電流狭窄層、15は溝、16は
クラツド層。
Fig. 1 shows an example of the manufacturing process of the present invention, Fig. 1a shows the first epitaxial growth step, and Fig. 1b shows grooves being created in the current confinement layer by selective etching. Figure 1c is a diagram showing the second epitaxial growth and electrode attachment process, Figure 2 is a perspective view of another semiconductor laser device manufactured according to the present invention, and Figure 3 is the same as above. FIG. 4 is a perspective view showing an example of a semiconductor laser device manufactured by a conventional method. In the figure, 12, 12a, 12b are optical waveguide layers, 13
14 is a current confinement layer, 15 is a groove, and 16 is a cladding layer.

Claims (1)

【特許請求の範囲】 1 内部に光導波層、電流狭窄層、クラツド層の
積層を有するAlGaAs系材料を用いた半導体レー
ザの製造法において、 上記光導電波層上に被覆層を形成して該被覆層
上に電流狭窄層を成長させ、更に該電流狭窄層を
選択的にエツチングし、次にエツチング部分の被
覆層を通常の成長温度で蒸発させてからクラツド
層を成長させるようにしたことを特徴とする半導
体レーザの製造法。
[Scope of Claims] 1. A method for manufacturing a semiconductor laser using an AlGaAs - based material having a laminated layer of an optical waveguide layer, a current confinement layer, and a cladding layer therein, comprising: forming a coating layer on the optical waveguide layer; A current confinement layer is grown on the coating layer, the current confinement layer is selectively etched, and the coating layer in the etched portion is evaporated at a normal growth temperature before the cladding layer is grown. A method for manufacturing a semiconductor laser characterized by the following.
JP7667885A 1985-04-12 1985-04-12 Preparation of semiconductor laser element Granted JPS61236185A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7667885A JPS61236185A (en) 1985-04-12 1985-04-12 Preparation of semiconductor laser element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7667885A JPS61236185A (en) 1985-04-12 1985-04-12 Preparation of semiconductor laser element

Publications (2)

Publication Number Publication Date
JPS61236185A JPS61236185A (en) 1986-10-21
JPH0138390B2 true JPH0138390B2 (en) 1989-08-14

Family

ID=13612088

Family Applications (1)

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JP7667885A Granted JPS61236185A (en) 1985-04-12 1985-04-12 Preparation of semiconductor laser element

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Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5146295A (en) * 1988-03-29 1992-09-08 Omron Tateisi Electronic Co. Semiconductor light emitting device having a superlattice buffer layer
JP2910251B2 (en) * 1990-12-28 1999-06-23 日本電気株式会社 Semiconductor laser
JPH04245417A (en) * 1991-01-31 1992-09-02 Sharp Corp Formation method of compound semiconductor layer

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