JP2777432B2 - Manufacturing method of semiconductor laser - Google Patents

Manufacturing method of semiconductor laser

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Publication number
JP2777432B2
JP2777432B2 JP29833289A JP29833289A JP2777432B2 JP 2777432 B2 JP2777432 B2 JP 2777432B2 JP 29833289 A JP29833289 A JP 29833289A JP 29833289 A JP29833289 A JP 29833289A JP 2777432 B2 JP2777432 B2 JP 2777432B2
Authority
JP
Japan
Prior art keywords
semiconductor laser
layer
buffer layer
manufacturing
growth
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
JP29833289A
Other languages
Japanese (ja)
Other versions
JPH03159185A (en
Inventor
弘喜 浜田
昌幸 庄野
正治 本多
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.)
Sanyo Denki Co Ltd
Original Assignee
Sanyo Denki Co Ltd
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Publication date
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Priority to JP29833289A priority Critical patent/JP2777432B2/en
Publication of JPH03159185A publication Critical patent/JPH03159185A/en
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Publication of JP2777432B2 publication Critical patent/JP2777432B2/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】 (イ) 産業上の利用分野 本発明は可視光を発振可能なAlGaInP系の半導体レー
ザの製造方法に関する。
The present invention relates to a method for manufacturing an AlGaInP-based semiconductor laser capable of oscillating visible light.

(ロ) 従来の技術 従来、可視光を発振可能な半導体レーザとして、例え
ば特開昭62−200786号公報に開示されている如く、AlGa
InP系の半導体レーザが提案されている。斯る半導体レ
ーザでは活性層にGaInPを用いて、670〜680nmのレーザ
光が得られている。
(B) Conventional technology Conventionally, as a semiconductor laser capable of oscillating visible light, for example, as disclosed in JP-A-62-200786, AlGa
InP-based semiconductor lasers have been proposed. In such a semiconductor laser, laser light of 670 to 680 nm is obtained by using GaInP for the active layer.

近年、半導体レーザにおいては短波長化が望まれてお
り、上記AlGaInP系の半導体レーザを短波長化する方法
として、活性層にAlを添加する、活性層を超格子構
造とする、活性層のGa/(Ga+In)比例を増やす、等
の方法が考えられている。
In recent years, it has been desired to shorten the wavelength of a semiconductor laser. As a method for shortening the wavelength of the AlGaInP-based semiconductor laser, Al is added to the active layer, the active layer has a superlattice structure, and the Ga of the active layer is A method of increasing the ratio of / (Ga + In) has been considered.

(ハ) 発明が解決しようとする課題 しかし乍ら、の方法においてはAl組成比の増加とと
もに発振しきい値が上昇し、連続動作が困難となり、
及びの方法においては、膜質の良い結晶成長が困難で
あり、特性の再現性や装置の信頼性が乏しいなどの問題
があった。
(C) Problems to be Solved by the Invention However, in the above method, the oscillation threshold value increases with an increase in the Al composition ratio, making continuous operation difficult.
In the methods (1) and (2), it is difficult to grow a crystal having good film quality, and there is a problem that reproducibility of characteristics and reliability of the device are poor.

したがって、本発明はAlGaInP系の半導体レーザを短
波長化するとともに、再現性良く製造可能な半導体レー
ザの製造方法を提供するものである。
Accordingly, the present invention is to provide a method for manufacturing a semiconductor laser that can shorten the wavelength of an AlGaInP-based semiconductor laser and that can be manufactured with good reproducibility.

(ニ) 課題を解決するための手段 本発明は、GaAsの基板上にGaxIn1-xPからなるバッフ
ァ層を積層し、該バッファ層上に(AlzGa1-zyIn1-yP
(0≦z≦1,y>0.5)からなる発振層を積層する半導体
レーザの製造方法であって、上記課題を解決するため、
上記バッファ層を、そのGaの組成比xを徐々に増加させ
ると同時に、その結晶成長温度を徐々に上昇させて形成
することを特徴とする。
(D) Means for Solving the Problems According to the present invention, a buffer layer made of Ga x In 1-x P is laminated on a GaAs substrate, and (Al z Ga 1-z ) y In 1 is formed on the buffer layer. -y P
A method of manufacturing a semiconductor laser in which an oscillation layer composed of (0 ≦ z ≦ 1, y> 0.5) is stacked.
The buffer layer is formed by gradually increasing the composition ratio x of Ga and simultaneously increasing the crystal growth temperature.

(ホ) 作用 本発明方法によれば、GaAs基板上にGaxIn1-xPからな
るバッファ層を積層する際に、このバッファ層を、その
Gaの組成比xを0.5から徐々に増加させると同時にその
成長温度を徐々に上昇させることによって、バッファ層
の格子定数が徐々に小さくなり、且つバッファ層表面に
生じる格子欠陥が減少する。
(E) Function According to the method of the present invention, when a buffer layer made of Ga x In 1-x P is laminated on a GaAs substrate, this buffer layer is
By gradually increasing the composition ratio x of Ga from 0.5 and simultaneously increasing the growth temperature, the lattice constant of the buffer layer gradually decreases and the lattice defects generated on the buffer layer surface decrease.

(ヘ) 実施例 第1図はAlGaInP系半導体レーザの製造工程を示し、
以下図を参照して本発明方法の一実施例を説明する。
(F) Example FIG. 1 shows a manufacturing process of an AlGaInP semiconductor laser.
An embodiment of the method of the present invention will be described below with reference to the drawings.

第1図(a)は第1の工程を示し、先ずn型のGaAsか
らなる基板(1)を準備し、この一主面(1a)上に周知
のMOCVD法を用い、成長圧力を70Torrとして、n型のGax
In1-xPからなるバッファ層(2)を積層する。
FIG. 1 (a) shows a first step, in which a substrate (1) made of n-type GaAs is first prepared, and a growth pressure is set to 70 Torr on this one main surface (1a) using a well-known MOCVD method. , N-type Ga x
A buffer layer (2) made of In 1-x P is laminated.

斯るバッファ層(2)は、成長開始時のGa組成比x
を、GaAsの格子整合する値、例えば0.5程度、より好適
には0.51とし、成長温度を630℃として5〜10分成長を
行い、続いて、V/III供給比を一定に保ちつつGa組成比
xを徐々に0.58まで増加させると同時に成長温度を徐々
に680℃まで上昇させながら成長を行う。
Such a buffer layer (2) has a Ga composition ratio x at the start of growth.
Is a value matching the lattice of GaAs, for example, about 0.5, more preferably 0.51, and the growth temperature is 630 ° C., and the growth is performed for 5 to 10 minutes, and then the Ga composition ratio is maintained while the V / III supply ratio is kept constant. The growth is performed while gradually increasing x to 0.58 and gradually increasing the growth temperature to 680 ° C.

第1図(b)は第2の工程を示し、表面の組成がGa
0.58In0.42Pであるバッファ層(2)上に、n型の(Al
0.7Ga0.30.58In0.42Pからなるn型クラッド層
(3)、アンドープのGa0.58In0.42Pからなる活性層
(4)、p型の(Al0.7Ga0.30.58In0.42Pからなるキ
ャップ層(6)をこの順に積層する。これらの層の成長
温度は、いずれも680℃で一定である。
FIG. 1 (b) shows the second step, in which the surface composition is Ga
On the buffer layer (2) of 0.58 In 0.42 P, an n-type (Al
0.7 Ga 0.3 ) 0.58 In 0.42 P n-type cladding layer (3), undoped Ga 0.58 In 0.42 P active layer (4), p-type (Al 0.7 Ga 0.3 ) 0.58 In 0.42 P cap layer (6) is laminated in this order. The growth temperature of each of these layers is constant at 680 ° C.

第1図(c)は第3の工程を示し、周知のフォトリソ
技術を用いてキャップ層(6)及びp型クラッド(5)
をエッチング除去し、紙面垂直方向に延在するストライ
プ状のリッジ(7)を形成する。ここでは、リッジ
(7)頂部の幅を5μmとし、共振器長を250μmとし
た。また、キャップ層(6)及びp型クラッド層(5)
の除去にはエッチャントとして臭化水素酸が用いられ
る。
FIG. 1 (c) shows a third step, in which a cap layer (6) and a p-type clad (5) are formed using a well-known photolithography technique.
Is removed by etching to form a stripe-shaped ridge (7) extending in the direction perpendicular to the paper surface. Here, the width of the top of the ridge (7) was 5 μm, and the cavity length was 250 μm. The cap layer (6) and the p-type clad layer (5)
Hydrobromic acid is used as an etchant for the removal.

第1図(d)は第4の工程を示し、キャップ層(6)
上及び露出したp型クラッド層(5)上にスパッタ法を
用いてSiO2膜(8)を被着し、リフトオフ法を用いてリ
ッジ(7)頂部、即ちキャップ層(6)上のSiO2
(8)を除去する。
FIG. 1D shows a fourth step, in which a cap layer (6) is formed.
P-type cladding layer and the upper and exposed (5) sputtering deposited a SiO 2 film (8) by using the on ridge (7) by lift-off top, or cap layer (6) on the SiO 2 The film (8) is removed.

第1図(e)は第5の工程を示し、基板(1)の他主
面(1b)上にCr、Sn、Auこの順に蒸着したn型電極
(9)、キャップ層(6)上及びSiO2膜(8)上にCr、
Auをこの順に蒸着したp型電極(10)を形成する。
FIG. 1 (e) shows a fifth step, in which Cr, Sn and Au are deposited on the other main surface (1b) of the substrate (1) in this order, on the n-type electrode (9), on the cap layer (6) and Cr on the SiO 2 film (8)
Au is deposited in this order to form a p-type electrode (10).

斯る方法により形成した半導体レーザの電流−光出力
特性及び出力2mWにおける発振スペクトル特性を測定し
た。その結果を第2図及び第3図に示す。また測定条件
はいずれも室温のパルス動作時のものである。
The current-light output characteristics and the oscillation spectrum characteristics at an output of 2 mW of the semiconductor laser formed by such a method were measured. The results are shown in FIGS. 2 and 3. The measurement conditions are all those at the time of pulse operation at room temperature.

これらの特性図から明らかな如く、本実施例方法を用
いて作成した装置では第2図に示される様に、発振しき
い値電流が90mA程度で光出力が4mWまで直線的な特性が
得られ、また第3図に示される様に634nmのレーザ発振
波長が得られた。
As is clear from these characteristic diagrams, in the device prepared by using the method of the present embodiment, as shown in FIG. 2, a linear characteristic can be obtained up to an oscillation threshold current of about 90 mA and an optical output up to 4 mW. As shown in FIG. 3, a laser oscillation wavelength of 634 nm was obtained.

ここで比較のため、各層の成長温度を630℃で一定と
し、本実施例と同様な装置を作製した。尚、他の成長条
件は本実施例方法と同じである。斯る比較装置からは、
650.4nmのレーザ発振波長が得られた。
Here, for comparison, an apparatus similar to that of the present example was manufactured with the growth temperature of each layer kept constant at 630 ° C. The other growth conditions are the same as in the method of this embodiment. From such a comparison device,
A laser oscillation wavelength of 650.4 nm was obtained.

これより、活性層(4)の組成が同じであっても本発
明方法を用いればより短波長化が図れることがわかる。
これは、AlGaInP計半導体レーザでは、成長温度によっ
てバンドギャップの大きさが変化するためであると考え
られる(日経エレクトロニクス,1987年8月10日号,No.4
27,p.136)。
This shows that even if the composition of the active layer (4) is the same, the wavelength can be further shortened by using the method of the present invention.
This is considered to be due to the fact that the band gap changes in the AlGaInP meter semiconductor laser depending on the growth temperature (Nikkei Electronics, August 10, 1987, No. 4).
27, p.136).

次に、各層の成長温度を680℃で一定とした以外は本
実施例方法と同じ条件で比較装置を作製した。しかし乍
ら斯る比較装置ではレーザ発振は生じなかった。これは
成長温度680℃ではGaAs基板(1)上に単結晶のGaInP系
バッファ層(2)が成長せず、多結晶化したためであ
る。また、バッファ層(2)を630℃で成長し、n型ク
ラッド層(3)の成長を始める前に、温度を680℃まで
上昇させると、通常温度上昇に数分の時間がかかるた
め、下地層であるバッファ層(2)表面から蒸気圧の高
いPが蒸発してしまい、この上に結晶性の良い膜を成長
させることは困難となる。勿論活性層(4)の成長直前
に成長温度を上昇させる場合でも同様の減少が起こり、
活性層(4)の結晶性は悪くなる。
Next, a comparative device was manufactured under the same conditions as in the method of this example except that the growth temperature of each layer was fixed at 680 ° C. However, no laser oscillation occurred in such a comparison device. This is because the single-crystal GaInP-based buffer layer (2) did not grow on the GaAs substrate (1) at the growth temperature of 680 ° C. and was polycrystalline. If the temperature of the buffer layer (2) is increased to 680 ° C. before the growth of the buffer layer (2) at 630 ° C. and the growth of the n-type cladding layer (3) is started, it usually takes several minutes to increase the temperature. P having a high vapor pressure evaporates from the surface of the buffer layer (2), which is the formation layer, and it becomes difficult to grow a film having good crystallinity on this. Of course, a similar decrease occurs when the growth temperature is increased immediately before the growth of the active layer (4).
The crystallinity of the active layer (4) deteriorates.

(ト) 発明の効果 本発明方法によれば、GaAs基板にGaxIn1-xPからなる
バッファ層を、そのGa組成比xを徐々に増加させると同
時に、その結晶成長温度を徐々に上昇させて形成し、こ
の上に(AlzGa1-zyIn1-yP(0≦z≦1,y>0.5)から
なる発振層を形成することによって、短波長化された半
導体レーザが再現性良く製造できる。
(G) Effects of the Invention According to the method of the present invention, a buffer layer made of Ga x In 1-x P is formed on a GaAs substrate by gradually increasing its Ga composition ratio x and gradually increasing its crystal growth temperature. A semiconductor laser with a shorter wavelength is formed by forming an oscillation layer of (Al z Ga 1-z ) y In 1-y P (0 ≦ z ≦ 1, y> 0.5). Can be manufactured with good reproducibility.

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

第1図(a)乃至(e)は本発明方法の一実施例を説明
するための工程別断面図、第2図及び第3図は夫々本実
施例方法を用いて作製された半導体レーザの電流−光出
力特性図及び発振スペクトル特性図である。
1 (a) to 1 (e) are cross-sectional views for explaining steps of an embodiment of the method of the present invention, and FIGS. 2 and 3 are views of a semiconductor laser manufactured using the method of the embodiment. It is a current-light output characteristic diagram and an oscillation spectrum characteristic diagram.

フロントページの続き (56)参考文献 特開 昭63−42114(JP,A) 特開 平1−251684(JP,A) 特開 昭63−177487(JP,A) 特開 昭61−166186(JP,A) 特開 平3−104183(JP,A) (58)調査した分野(Int.Cl.6,DB名) H01S 3/18Continuation of front page (56) References JP-A-63-42114 (JP, A) JP-A-1-251684 (JP, A) JP-A-63-177487 (JP, A) JP-A-61-166186 (JP) , A) JP-A-3-104183 (JP, A) (58) Fields investigated (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基板上にGaxIn1-xPからなるバッファ
層を積層し、該バッファ層上に(AlzGa1-zyIn1-yP
(0≦z≦1,y>0.5)からなる発振層を積層する半導体
レーザの製造方法において、上記バッファ層を、そのGa
の組成比xを徐々に増加させると同時に、その結晶成長
温度を徐々に上昇させて形成することを特徴とする半導
体レーザの製造方法。
1. A buffer layer comprising Ga x In 1-x P is laminated on a GaAs substrate, and (Al z Ga 1-z ) y In 1-y P is formed on the buffer layer.
In the method for manufacturing a semiconductor laser in which an oscillation layer composed of (0 ≦ z ≦ 1, y> 0.5) is laminated, the buffer layer is
Characterized by gradually increasing the composition ratio x and simultaneously increasing the crystal growth temperature thereof.
JP29833289A 1989-11-16 1989-11-16 Manufacturing method of semiconductor laser Expired - Fee Related JP2777432B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29833289A JP2777432B2 (en) 1989-11-16 1989-11-16 Manufacturing method of semiconductor laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29833289A JP2777432B2 (en) 1989-11-16 1989-11-16 Manufacturing method of semiconductor laser

Publications (2)

Publication Number Publication Date
JPH03159185A JPH03159185A (en) 1991-07-09
JP2777432B2 true JP2777432B2 (en) 1998-07-16

Family

ID=17858294

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29833289A Expired - Fee Related JP2777432B2 (en) 1989-11-16 1989-11-16 Manufacturing method of semiconductor laser

Country Status (1)

Country Link
JP (1) JP2777432B2 (en)

Also Published As

Publication number Publication date
JPH03159185A (en) 1991-07-09

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