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JPH0522677B2 - - Google Patents
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JPH0522677B2 - - Google Patents

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Publication number
JPH0522677B2
JPH0522677B2 JP20794484A JP20794484A JPH0522677B2 JP H0522677 B2 JPH0522677 B2 JP H0522677B2 JP 20794484 A JP20794484 A JP 20794484A JP 20794484 A JP20794484 A JP 20794484A JP H0522677 B2 JPH0522677 B2 JP H0522677B2
Authority
JP
Japan
Prior art keywords
type
solution
layer
gaalas
type layer
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 - Lifetime
Application number
JP20794484A
Other languages
Japanese (ja)
Other versions
JPS6186500A (en
Inventor
Susumu Doi
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.)
Resonac Holdings Corp
Original Assignee
Showa Denko KK
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 Showa Denko KK filed Critical Showa Denko KK
Priority to JP59207944A priority Critical patent/JPS6186500A/en
Publication of JPS6186500A publication Critical patent/JPS6186500A/en
Publication of JPH0522677B2 publication Critical patent/JPH0522677B2/ja
Granted legal-status Critical Current

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Classifications

    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/10Inorganic compounds or compositions
    • C30B29/40AIIIBV compounds wherein A is B, Al, Ga, In or Tl and B is N, P, As, Sb or Bi
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B19/00Liquid-phase epitaxial-layer growth
    • C30B19/06Reaction chambers; Boats for supporting the melt; Substrate holders
    • C30B19/063Sliding boat system

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Crystals, And After-Treatments Of Crystals (AREA)
  • Liquid Deposition Of Substances Of Which Semiconductor Devices Are Composed (AREA)
  • Led Devices (AREA)

Description

【発明の詳細な説明】 本発明は液相エピタキシヤル成長による
GaAlAs発光素子の製造方法の改良に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention is based on liquid phase epitaxial growth.
This invention relates to improvements in the manufacturing method of GaAlAs light emitting devices.

近年、光通信用あるいは屋外での表示用などと
して高効率の発光素子の需要が強くなつている。
高効率発光素子の半導体材料としては、GaAlAs
系の特性が最も優れていることが知られている。
Ga1-xAlxAs混晶は組成x=0からx=0.4付近ま
で直接遷移型のバンド構造を有し、6500Å〜9000
Åの間で高効率の発光を得ることができる。
Ga1-xAlxAs混晶の場合バンドギヤツプ(Eg単位
eV)と組成(x)の関係は近似的に次の関係式で表
わされることが知られている。
In recent years, there has been a strong demand for highly efficient light emitting elements for use in optical communications or outdoor displays.
GaAlAs is a semiconductor material for high-efficiency light emitting devices.
It is known that the system has the best characteristics.
The Ga 1-x Al x As mixed crystal has a direct transition type band structure from the composition x = 0 to around x = 0.4, and has a band structure of 6500 Å to 9000 Å.
Highly efficient light emission can be obtained between .
In the case of Ga 1-x Al x As mixed crystal, the band gap (in Eg
It is known that the relationship between eV) and composition (x) is approximately expressed by the following relational expression.

Eg(x)=1.424+1.247x (0<x<0.45) 一般に、GaAlAs発光素子はP型GaAs基板上
に液相エピタキシヤル成長により発光波長に対応
したバンドギヤツプE1 gを持つP型Ga1-xAlxAs層
及びこの波長に対して透明となるようなバンドギ
ヤツプE2 g(E2 g>E1 g)の広いn型Ga1-yAlyAs層を
y>xなる関係のもとに順次成長させた構造とな
つている。
Eg (x) = 1.424 + 1.247x ( 0 < x Al x As layer and an n-type Ga 1-y Al y As layer with a wide band gap E 2 g (E 2 g > E 1 g ) that is transparent to this wavelength under the relationship y>x. It has a structure in which it grows sequentially.

発光はP型GaAlAs層で起きる為、発光波長は
P型層の組成(x)に依存する。
Since light emission occurs in the P-type GaAlAs layer, the emission wavelength depends on the composition (x) of the P-type layer.

発光波長6600Åの典型的な赤色発光素子では組
成x=0.35のP型層及び組成y=0.6〜0.8のN型
層より構成されている。
A typical red light-emitting element with an emission wavelength of 6600 Å is composed of a P-type layer with a composition x=0.35 and an N-type layer with a composition y=0.6 to 0.8.

従来技術では第1図のようなP型成長溶液4及
びN型成長溶液5の2つの溶液で構成された横型
スライドボートを用い、P型層、N型層を徐冷法
または温度差法により順次成長する方式がとられ
ている。この方式の欠点は、P型層を成長させた
後、基板結晶が一旦成長溶液から切り離されるこ
と、および基板結晶をスライドすることによるキ
ズの発生などによりP−N界面付近に種々の欠陥
が導入され、特性劣化及びバラツキが問題となる
ことである。一方、リン化ガリウム(GaP)緑色
発光素子の場合にもN層及びP層を各々別個の溶
液から成長させる方式よりも、1つの溶液からN
層及びP層を連続して成長させる所謂不純物補償
法による発光素子の方が発光特性が優れているこ
とが知られている。
In the conventional technology, a horizontal slide boat composed of two solutions, a P-type growth solution 4 and an N-type growth solution 5, as shown in FIG. A method has been adopted to do so. The disadvantages of this method are that after growing the P-type layer, the substrate crystal is once separated from the growth solution, and that various defects are introduced near the P-N interface due to scratches caused by sliding the substrate crystal. However, deterioration and variation in characteristics become a problem. On the other hand, in the case of gallium phosphide (GaP) green light emitting devices, N layer and P layer are grown from one solution rather than growing from separate solutions.
It is known that a light-emitting element based on the so-called impurity compensation method in which the P layer and the P layer are continuously grown has superior light emission characteristics.

第1の発明は上記事実に鑑みなされたもので、
亜鉛(Zn)とテルル(Te)を同時に添加したP
型成長溶液からP型層を成長させた後、溶液中の
Znを減圧処理により除去し、さらにアルミニウ
ムを追加した後N型層を同一溶液から連続して成
長させ、P−N界面付近に種々の欠陥が導入され
ることを防ぐことにより安定した特性を持つ
GaAlAs層発光素子の製造方法を提供するもので
ある。
The first invention was made in view of the above facts,
P with simultaneous addition of zinc (Zn) and tellurium (Te)
After growing a P-type layer from a type growth solution,
After Zn is removed by vacuum treatment and aluminum is added, an N-type layer is successively grown from the same solution, resulting in stable characteristics by preventing various defects from being introduced near the P-N interface.
A method for manufacturing a GaAlAs layer light emitting device is provided.

しかしながらこの場合でもN型層を成長した後
スライドさせることにより溶液の分離させる為
に、多結晶のまき込みによるウエハー表面のキ
ズ、及びウエハー表面に溶液が残留することによ
る表面不良などの発生が問題となる。また横型ス
ライドボート法は上述した以外に下記問題点があ
る。
However, even in this case, since the solution is separated by sliding after growing the N-type layer, there are problems such as scratches on the wafer surface due to the inclusion of polycrystals and surface defects due to the solution remaining on the wafer surface. becomes. In addition to the above-mentioned problems, the horizontal slide boat method also has the following problems.

GaAlAsの液相エピタキシヤル成長の場合、
非常に酸化され易いアルミニウムを溶液に添加
している為に、成長前に十分な空焼きにより溶
液中の酸素及び成長用治具等に吸着した酸素を
十分除去しなければならない。しかしスライト
ボート法では溶液と基板結晶が常に同じ温度ゾ
ーンにある為に溶液の空焼きの時間が余り長く
なると基板結晶の熱劣化の問題が出て来る。し
たがつて、酸素の除去と云う観点だけで空焼き
時間を独立に選択することができない。
In the case of liquid phase epitaxial growth of GaAlAs,
Since aluminum, which is very easily oxidized, is added to the solution, oxygen in the solution and oxygen adsorbed on the growth jig etc. must be sufficiently removed by sufficient dry baking before growth. However, in the Slight Boat method, since the solution and the substrate crystal are always in the same temperature zone, if the solution baking time is too long, the problem of thermal deterioration of the substrate crystal arises. Therefore, the baking time cannot be selected independently from the viewpoint of oxygen removal.

スライドボート法で基板結晶を多数枚チヤー
ジする場合構造が複雑となり、操作性が悪く量
産的な製造方法としては問題がある。
When a large number of substrate crystals are charged by the slide boat method, the structure becomes complicated and the operability is poor, which is problematic as a mass production method.

そこで本発明の第2の発明は、上記事実に鑑み
なされたものである。本発明者は種々の検討の結
果縦型浸漬法を採用することにより上述した問題
の解決を計つたGaAlAs発光素子の量産的な製造
方法を提供するに至つたものである。
Therefore, the second invention of the present invention has been made in view of the above facts. As a result of various studies, the present inventors have succeeded in providing a method for mass-producing GaAlAs light emitting devices that solves the above-mentioned problems by employing a vertical immersion method.

以下図を参照して実施例を説明する。 Examples will be described below with reference to the figures.

実施例 1 第2図は第1の発明の実施において用いた黒鉛
製スライトボートを模式的に示したものである。
下部スライダー1にP型GaAs基板3が設置さ
れ、成長溶液4は金属ガリウム50g、GaAs多結
晶4g、アルミニウム(Al)80mg、亜鉛50mg、
テルル2mgを配合した組成となつている。また上
部スライダー8にはAl9 300mgが設置されてい
る。
Example 1 FIG. 2 schematically shows a graphite slite boat used in the implementation of the first invention.
A P-type GaAs substrate 3 is installed on the lower slider 1, and the growth solution 4 contains 50 g of metallic gallium, 4 g of GaAs polycrystal, 80 mg of aluminum (Al), 50 mg of zinc,
The composition contains 2mg of tellurium. Moreover, 300 mg of Al9 is installed in the upper slider 8.

スライダーをこの状態で電気炉の均熱帯に設置
し真空置換した後、水素ガスを流しながら900℃
まで昇温する。900℃で1時間保持した後スライ
ダー1を移動し、基板4と成長溶液4を接触さ
せ、冷却速度0.5℃/分で860℃まで冷却しP型層
を成長させる。この温度で成長を一時停止し、
Arガスを流しながら約2Torrの減圧下で約2時
間保持し溶液中のZnを除去する。次に常圧に戻
し再び水素ガスを流し、上部スライダー3を移動
しAl9を溶液に追加する。追加後約10分間経た
後、10℃再昇温する。870℃で約10分間保持した
後、再び冷却速度0.5℃/分で830℃まで徐冷し、
N型層を成長させ830℃に達した時スライダー1
を移動し、成長溶液を分離する。この工程によ
り、約20μmのP型層、及び約20μmのN型層が
成長した。EPMAによる組成分析の結果P型層
はGa0.66Al0.34As、N層はGa0.42Al0.58Asであつ
た。得られた発光素子の発光波長は6650Å発光出
力はP型層及びN型層を別個の溶液から成長させ
たもの約1.5倍であつた。
Place the slider in this state in the soaking zone of an electric furnace, perform vacuum replacement, and heat to 900℃ while flowing hydrogen gas.
Increase the temperature to. After holding the temperature at 900°C for 1 hour, the slider 1 is moved to bring the substrate 4 into contact with the growth solution 4, which is then cooled to 860°C at a cooling rate of 0.5°C/min to grow a P-type layer. Growth is suspended at this temperature,
The solution is maintained under a reduced pressure of about 2 Torr for about 2 hours while flowing Ar gas to remove Zn from the solution. Next, the pressure is returned to normal and hydrogen gas is supplied again, and the upper slider 3 is moved to add Al9 to the solution. Approximately 10 minutes after addition, the temperature is raised again by 10°C. After holding at 870℃ for about 10 minutes, slowly cool it again to 830℃ at a cooling rate of 0.5℃/min.
When the N-type layer grows and reaches 830℃, slider 1
and separate the growth solution. Through this step, a P-type layer of about 20 μm and an N-type layer of about 20 μm were grown. As a result of compositional analysis by EPMA, the P-type layer was Ga 0.66 Al 0.34 As, and the N layer was Ga 0.42 Al 0.58 As. The light emission wavelength of the obtained light emitting device was 6650 Å, and the light emission output was about 1.5 times that of the case where the P type layer and the N type layer were grown from separate solutions.

上記例では減圧処理時間を2時間としたが、1
時間の場合はZnの除去が不十分でN型層が得ら
れない場合があり2時間以上の場合はN型層が再
現良く得られた。
In the above example, the decompression treatment time was set to 2 hours, but 1
If the time is longer than 2 hours, the N-type layer may not be obtained due to insufficient removal of Zn, but if the time is 2 hours or more, an N-type layer can be obtained with good reproducibility.

実施例 2 第3図は第2の発明の実施において用いた縦型
浸漬法の装置を模式的に示したものである。電気
炉11及び石英反応管12により構成される。炉
内には、金属ガリウム3Kg、GaAs多結晶240g、
テルル120mgを配合した組成の成長溶液4が、炉
外の反応管上部には、P型GaAs基板3を装着し
た基板ホルダー13が設置されている。また反応
管上部にはZn投入器6及びAl投入器7が設置さ
れている。この状態で、真空置換後水素ガスを流
しながら900℃まで昇温する。900℃で2.5時間保
持した後、Zn投入器6からZn3gをAl投入器7か
らAl4.8gを添加する。更に30分間900℃で保持し
た後、基板ホルダー13を成長溶液の直上部で予
熱した後成長溶液に浸漬し、冷却速度0.5℃/分
で860℃まで徐冷しP型層を成長させる。この温
度で成長を一時停止しArガスを流しながら約
2Torrの減圧下で2時間保持し溶液中のZnを除去
した後、常圧に戻し再び水素ガスを流してAl投
入器7よりAl18gを追加する。追加後30分間経
た後、10℃昇温し870℃で10分間保持して再び冷
却速度0.5℃/分で830℃まで徐冷しN層を成長さ
せ、830℃に達した時基板ホルダー13を成長溶
液より分離して反応管上部まで引き上げる。この
工程により約25μmP型層及び約25μmのN型層
が成長した。またEPMAでの組成分析の結果は
P型層はGa0.68Al0.32As、N型層はGa0.38Al0.62As
であつた。得られた発光素子の発光波長は6700
Å、発光出力は実施例1のものとほぼ同一であつ
た。
Example 2 FIG. 3 schematically shows an apparatus for the vertical dipping method used in the implementation of the second invention. It is composed of an electric furnace 11 and a quartz reaction tube 12. Inside the furnace, 3 kg of metallic gallium, 240 g of GaAs polycrystal,
A substrate holder 13 on which a P-type GaAs substrate 3 is mounted is installed at the top of the reaction tube outside the furnace where a growth solution 4 containing 120 mg of tellurium is mixed. Furthermore, a Zn charger 6 and an Al charger 7 are installed at the top of the reaction tube. In this state, after vacuum replacement, the temperature is raised to 900°C while flowing hydrogen gas. After holding at 900° C. for 2.5 hours, 3 g of Zn was added from the Zn charger 6 and 4.8 g of Al was added from the Al charger 7. After holding the temperature at 900° C. for another 30 minutes, the substrate holder 13 is preheated directly above the growth solution, then immersed in the growth solution, and slowly cooled to 860° C. at a cooling rate of 0.5° C./min to grow a P-type layer. At this temperature, growth is temporarily stopped and while Ar gas is flowing, approximately
After holding the solution under a reduced pressure of 2 Torr for 2 hours to remove Zn from the solution, the pressure is returned to normal pressure, hydrogen gas is flowed again, and 18 g of Al is added from the Al injector 7. After 30 minutes after the addition, the temperature was raised by 10°C, held at 870°C for 10 minutes, and slowly cooled again to 830°C at a cooling rate of 0.5°C/min to grow the N layer. When the temperature reached 830°C, the substrate holder 13 was It is separated from the growth solution and pulled up to the top of the reaction tube. This process resulted in the growth of a P-type layer of approximately 25 μm and an N-type layer of approximately 25 μm. Also, the results of composition analysis by EPMA show that the P-type layer is Ga 0.68 Al 0.32 As, and the N-type layer is Ga 0.38 Al 0.62 As.
It was hot. The emission wavelength of the obtained light emitting device is 6700
Å, the luminous output was almost the same as that of Example 1.

実施例1ではN型層の表面にスライダーによる
キズ溶液の残留による表面不良がみられたが実施
例2ではほぼ完全な鏡面が得られた。
In Example 1, surface defects were observed on the surface of the N-type layer due to scratches caused by the slider and residual solution, but in Example 2, an almost perfect mirror surface was obtained.

同一溶液から連続してP型層及びN型層を成長
させることにより安定した特性のGaAlAs発光素
子の製造が可能となりガリウムの原単位も従来の
約半分となつた。また縦型浸漬法の採用し多数枚
束ねた構造の基板ホルダーを用いることにより、
1回の成長で直径約50mmφのウエハー30枚の処理
が可能となりほぼ完全な鏡面が得られるようにな
つた。
By successively growing a P-type layer and an N-type layer from the same solution, it is possible to manufacture a GaAlAs light-emitting device with stable characteristics, and the gallium consumption rate has also been reduced to about half that of the conventional method. In addition, by adopting the vertical dipping method and using a substrate holder with a structure in which many sheets are bundled,
It has become possible to process 30 wafers with a diameter of approximately 50 mmφ in one growth, and it has become possible to obtain almost perfect mirror surfaces.

上記実施例では発光波長が6600〜6700Åの赤色
発光であつたがP型GaAlAs層のアルミニウムの
組成を変えることにより6500〜9000Åの発光が可
能である。またN型添加剤としてテルル(Te)
を用いたがイオウ(S)、セレン(Se)であつても
良くP型添加剤としてはカドミニウム(Cd)で
あつても良い。
In the above embodiment, red light was emitted with a wavelength of 6,600 to 6,700 Å, but by changing the composition of aluminum in the P-type GaAlAs layer, it is possible to emit light with a wavelength of 6,500 to 9,000 Å. In addition, tellurium (Te) is used as an N-type additive.
was used, but sulfur (S), selenium (Se) may also be used, and the P-type additive may be cadmium (Cd).

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

第1図は従来技術の横型スライドボートを示す
説明図である。 1…下部スライダー、2…上部スライダー、3
…P型GaAs基板、4…P型成長溶液、5…N型
成長溶液。 第2図は本発明に使用する横型スライドボート
の一例を示す図である。 1…下部スライダー、2…中部スライダー、3
…P型GaAs基板、4…成長溶液、8…上部スラ
イダー、9…追加用アルミニウム。 第3図は本発明に使用する縦型浸漬法の装置の
一例を示す図である。 3…P型GaAs基板、4…成長溶液、6…Zn投
入器、7…Al投入器、11…電気炉、12…石
英反応管、13…基板ホルダー。
FIG. 1 is an explanatory diagram showing a conventional horizontal slide boat. 1...Lower slider, 2...Upper slider, 3
...P-type GaAs substrate, 4...P-type growth solution, 5...N-type growth solution. FIG. 2 is a diagram showing an example of a horizontal slide boat used in the present invention. 1...Lower slider, 2...Middle slider, 3
...P-type GaAs substrate, 4...Growth solution, 8...Upper slider, 9...Additional aluminum. FIG. 3 is a diagram showing an example of an apparatus for the vertical dipping method used in the present invention. 3... P-type GaAs substrate, 4... Growth solution, 6... Zn charger, 7... Al charger, 11... Electric furnace, 12... Quartz reaction tube, 13... Substrate holder.

Claims (1)

【特許請求の範囲】 1 P型ヒ化ガリウム基板上に、P型GaAlAs層
さらに該層上にN型GaAlAs層を有するGaAlAs
発光素子を液相エピタキシヤル成長により製造す
るに際して、亜鉛(Zn)とテルル(Te)を添加
したアルミニウム(Al)−ガリウム(Ga)溶液よ
りまずP型GaAlAs層を成長させた後減圧処理に
より溶液中のZnを除去し、次いでAlを追加した
後引き続きN型GaAlAs層を同一溶液から連続し
て成長させることを特徴とするGaAlAs発光素子
の製造方法。 2 液相エピタキシヤル成長に際して、縦型浸漬
法を用いることを特徴とする特許請求の範囲第1
項記載のGaAlAs発光素子の製造方法。
[Claims] 1. GaAlAs having a P-type GaAlAs layer and an N-type GaAlAs layer on the P-type gallium arsenide substrate.
When manufacturing a light emitting device by liquid phase epitaxial growth, a P-type GaAlAs layer is first grown from an aluminum (Al)-gallium (Ga) solution containing zinc (Zn) and tellurium (Te), and then the solution is grown by vacuum treatment. A method for manufacturing a GaAlAs light emitting device, which comprises removing Zn therein, adding Al, and then successively growing an N-type GaAlAs layer from the same solution. 2. Claim 1, characterized in that a vertical dipping method is used during liquid phase epitaxial growth.
A method for manufacturing a GaAlAs light emitting device as described in .
JP59207944A 1984-10-05 1984-10-05 Manufacture of gaalas light emitting semiconductor Granted JPS6186500A (en)

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JP59207944A JPS6186500A (en) 1984-10-05 1984-10-05 Manufacture of gaalas light emitting semiconductor

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Application Number Priority Date Filing Date Title
JP59207944A JPS6186500A (en) 1984-10-05 1984-10-05 Manufacture of gaalas light emitting semiconductor

Publications (2)

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JPS6186500A JPS6186500A (en) 1986-05-01
JPH0522677B2 true JPH0522677B2 (en) 1993-03-30

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Publication number Priority date Publication date Assignee Title
JPS61127699A (en) * 1984-11-26 1986-06-14 Mitsubishi Monsanto Chem Co Gallium arsenide/aluminum mixed crystal epitaxial wafer and its manufacturing method

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