JPH06310449A - Vapor phase diffusion - Google Patents

Vapor phase diffusion

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Publication number
JPH06310449A
JPH06310449A JP9274393A JP9274393A JPH06310449A JP H06310449 A JPH06310449 A JP H06310449A JP 9274393 A JP9274393 A JP 9274393A JP 9274393 A JP9274393 A JP 9274393A JP H06310449 A JPH06310449 A JP H06310449A
Authority
JP
Japan
Prior art keywords
layer
vapor phase
contact layer
ingaasp
diffusion
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
JP9274393A
Other languages
Japanese (ja)
Inventor
Tomonobu Tsuchiya
朋信 土屋
Toshihiro Kono
敏弘 河野
Takeshi Taniwatari
剛 谷渡
Masaaki Komori
正明 古森
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP9274393A priority Critical patent/JPH06310449A/en
Publication of JPH06310449A publication Critical patent/JPH06310449A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To allow large area diffusion and controllability improvement by supplying the vapor phase atmosphere with DMZn, DEZn, etc., permitting the Zn to be adsorbed to the surface of the INGaAsP crystal of a contact layer and diffusing Zn on the contact layer and a clad layer by using a metal organic vapor deposition device. CONSTITUTION:An undoped InP clad layer 2 and an undoped InGaAsP contact layer 3 are formed on an n-type InP substrate 1. Then, AsH3, PH3, DMZn and hydrogen are permitted to flow by a vapor phase growing device. High concentration Zn vapor phase diffusion is allowed by providing the contact layer 3 with the InGaAsP layer and the high concentration Zn is taken into the InGaAsP layer. Thus, large diffusion area is allowed by using the vapor phase growth device which allows several-inch crystal growth and controllability is improved by the accurate flow control using gas as the material.

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p型コンタクト層を形成
する時の気相拡散方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a vapor phase diffusion method for forming a p-type contact layer.

【0002】[0002]

【従来の技術】従来のp型コンタクト層の形成方法は、
石英のアンプル管内に半導体多層膜と、ZnP2等のZ
n化合物を入れ、高真空中で封じ、次にアンプル管を高
温の炉内に入れ、ZnP2をZnとPに分離させ、この
Znを表面層から結晶内部に拡散させ、高濃度のp型コ
ンタクト層を形成した。この方法はアンプル管を封じ切
るため閉管法もしくは封じ切り法と呼ばれる。この方法
の従来例にはジャーナル・オブ・アプライド・フィジッ
クス第65巻(1989年)553項(Journalof Appl
ied Physics vol.65(1989)pp.553)等がある。
2. Description of the Related Art A conventional method for forming a p-type contact layer is as follows.
A semiconductor multilayer film and ZP such as ZnP 2 in a quartz ampoule tube.
n-compound, sealed in a high vacuum, then the ampoule tube was placed in a high-temperature furnace to separate ZnP 2 into Zn and P, and this Zn was diffused from the surface layer to the inside of the crystal to obtain a high-concentration p-type A contact layer was formed. This method is called the closed tube method or the cut-off method because it seals the ampoule tube. A conventional example of this method is described in Journal of Applied Physics, Volume 65 (1989), Item 553 (Journal of Appl).
ied Physics vol.65 (1989) pp.553).

【0003】[0003]

【発明が解決しようとする課題】上記従来技術では、試
料サイズがアンプル管で制限されるため、数cm2程度
の大きさしか封入できず、大面積化に問題があった。ま
た、拡散濃度、および拡散深さが、微妙な封じ切りの方
法やZnP2の量に依存するため、拡散濃度、拡散深さ
のばらつきが大きく、制御性が極めて悪かった。
In the above prior art, since the sample size is limited by the ampoule tube, only a size of about several cm 2 can be enclosed and there is a problem in increasing the area. Further, since the diffusion concentration and the diffusion depth depend on the delicate sealing method and the amount of ZnP 2 , the diffusion concentration and the diffusion depth vary greatly and the controllability is extremely poor.

【0004】本発明の目的は拡散の大面積化、および制
御性の向上を図ることにある。
An object of the present invention is to increase the area of diffusion and improve controllability.

【0005】[0005]

【課題を解決するための手段】上記目的を達成するため
に、本発明では閉管法ではなく、気相成長装置による開
管法を用い、拡散原料は、ZnP2の代わりにDMZ
n、DEZn等のガス原料を用いた。拡散方法は、気相
雰囲気中にDMZn、DEZn等を供給し、Znをコン
タクト層のInGaAsP、もしくはInGaAs結晶
表面に吸着させ、コンタクト層中、もしくはコンタクト
層からクラッド層へZnを拡散させた。
In order to achieve the above object, the present invention uses not the closed tube method but the open tube method using a vapor phase growth apparatus, and the diffusion raw material is DMZ instead of ZnP 2.
Gas raw materials such as n and DEZn were used. As the diffusion method, DMZn, DEZn, etc. were supplied into the gas phase atmosphere, Zn was adsorbed on the InGaAsP or InGaAs crystal surface of the contact layer, and Zn was diffused in the contact layer or from the contact layer to the cladding layer.

【0006】[0006]

【作用】本発明の原理を図1を用いて説明する。まず、
n型InP基板上に、アンドープInPクラッド層、ア
ンドープInGaAsPコンタクト層を形成した。次に
400℃の気相成長装置で30分間、AsH3、PH3
DMZn、水素を流した。図1はこの時のInGaAs
P、InP層中のZnによるp型キャリア濃度を示す。
InP層中でのp型濃度は1E18であるのに対して、
InGaAsP中でのp型濃度は1E19あり、InG
aAsP層中にZnが高濃度に取り込まれることを示
す。従ってコンタクト層にInGaAsP層を設けるこ
とによって高濃度のZn気相拡散が可能となる。
The principle of the present invention will be described with reference to FIG. First,
An undoped InP clad layer and an undoped InGaAsP contact layer were formed on the n-type InP substrate. Then, using a vapor phase growth apparatus at 400 ° C. for 30 minutes, AsH 3 , PH 3 ,
DMZn and hydrogen were flushed. Figure 1 shows InGaAs at this time.
The p-type carrier concentration due to Zn in the P and InP layers is shown.
While the p-type concentration in the InP layer is 1E18,
The p-type concentration in InGaAsP is 1E19, and InG
It is shown that Zn is incorporated in a high concentration in the aAsP layer. Therefore, by providing an InGaAsP layer in the contact layer, high-concentration Zn vapor phase diffusion becomes possible.

【0007】本方法ではアンプル管では無く、数インチ
の結晶成長可能な気相成長装置を用いているため、大面
積化が可能である。また、原料にガスを用いているため
正確な流量制御ができ、制御性の向上が可能となる。
In this method, a vapor phase growth apparatus capable of growing a crystal of several inches is used instead of an ampoule tube, so that the area can be increased. Further, since gas is used as the raw material, the flow rate can be accurately controlled, and the controllability can be improved.

【0008】[0008]

【実施例】(実施例1)以下、本発明の一実施例を図1
〜図3により説明する。図2に断面を示すように、有機
金属気相成長法によりn−InP基板1上にアンドープ
InP層2を0.8μm、アンドープInGaAsP層
3(波長1.3μm、InPに格子整合)を0.2μm
成長した。この時の成長温度は600℃である。次に試
料を有機金属気相成長装置内に入れ、450℃でPH3
(50%、20cc/min)、DMZn(1000p
pm、1000cc/min)、水素(100%、4リ
ットル/min)を30分間流した。
(Embodiment 1) An embodiment of the present invention will be described below with reference to FIG.
~ It demonstrates by FIG. As shown in the cross section in FIG. 2, an undoped InP layer 2 of 0.8 μm and an undoped InGaAsP layer 3 (wavelength of 1.3 μm, lattice-matched to InP) were formed on the n-InP substrate 1 by a metal organic chemical vapor deposition method. 2 μm
grown. The growth temperature at this time is 600 ° C. Next, the sample is placed in a metalorganic vapor phase epitaxy apparatus and PH 3
(50%, 20 cc / min), DMZn (1000 p
pm, 1000 cc / min) and hydrogen (100%, 4 liters / min) for 30 minutes.

【0009】図1はこの時のZnによるp型キャリア濃
度である。InP層中でのp型濃度は1E18であるの
に対して、InGaAsP中でのp型濃度は1E19あ
り、InGaAsP層中でのZnの取り込まれ率が高い
ことを示す。
FIG. 1 shows the p-type carrier concentration due to Zn at this time. While the p-type concentration in the InP layer is 1E18, the p-type concentration in InGaAsP is 1E19, which shows that the incorporation rate of Zn in the InGaAsP layer is high.

【0010】図2は気相拡散した試料の上にSiO2
スク4を形成し、さらにp側電極(Ti/Pt/Au)
を形成した時の断面図である。これにより、接触比抵抗
を測定したところ、1E−5Ω以下の値が得られた。こ
れは、InP層だけの接触比抵抗1E−4Ωに比べ十分
に低く、閉管法での値と比べても遜色なく、デバイス適
用できる値であった。
In FIG. 2, a SiO 2 mask 4 is formed on a sample which has been vapor-phase diffused, and a p-side electrode (Ti / Pt / Au) is further formed.
It is sectional drawing when forming. As a result, when the contact resistivity was measured, a value of 1E-5Ω or less was obtained. This value was sufficiently lower than the contact specific resistance of 1E-4Ω only for the InP layer, and was comparable to the value in the closed tube method, and was a value applicable to the device.

【0011】本装置では3インチのウエハまで作製する
ことができる。また、最近のCVD装置では多数枚も可
能である。本発明により、従来の閉管法に比べ十倍から
百倍程度の大面積化が可能である。
With this apparatus, up to a 3-inch wafer can be manufactured. Moreover, a large number of recent CVD apparatuses are possible. According to the present invention, it is possible to increase the area by about 10 to 100 times as compared with the conventional closed tube method.

【0012】図3は、実施例1での拡散時間に対する拡
散深さの依存性であり、従来の閉管法に比べ、ばらつき
を1/5程度に抑えることができた。
FIG. 3 shows the dependence of the diffusion depth on the diffusion time in Example 1, and the variation could be suppressed to about 1/5 as compared with the conventional closed tube method.

【0013】尚、本実施例ではコンタクト層に波長1.
3μmのInGaAsP層を用いたが、他の波長、もし
くはInGaAs層においても同等の効果が得られる。
また、拡散条件としてキャリアガスに水素を用いたが、
窒素を用いても同等の効果が得られる。同様に、V族ガ
スとしてAsH3、もしくはAsH3、PH3の混合ガス
を用いても良い。
In this embodiment, the contact layer has a wavelength of 1.
Although the InGaAsP layer of 3 μm is used, the same effect can be obtained at other wavelengths or the InGaAsP layer.
Also, hydrogen was used as the carrier gas as the diffusion condition,
The same effect can be obtained by using nitrogen. Similarly, AsH 3 or a mixed gas of AsH 3 and PH 3 may be used as the group V gas.

【0014】(実施例2)以下、本発明の実施例2を図
4により説明する。図4は本発明をフォトダイオードに
適用した例である。有機金属気相成長法により、n−I
nP基板1上にアンドープInP層2を1μm、アンド
ープInGaAs層6(波長1.67μm、InPに格
子整合)を1μm、アンドープInP層2を1μm、ア
ンドープInGaAsP層7(波長1.10μm、In
Pに格子整合)を0.1μm成長した。次にアンドープ
InGaAsP層7を硫酸系エッチング液により選択的
にエッチングし、部分的にコンタクト層を形成した。多
層構造を気相成長装置に導入し、400℃でPH3(5
0%、10cc/min)、DMZn(2000pp
m、2000cc/min)、水素(100%、4リッ
トル/min)を30分間流した。InGaAsP層7
をマスクとしてp型ハイドープInP拡散層8(Zn濃
度:8E18)を気相拡散により形成した。
(Second Embodiment) A second embodiment of the present invention will be described below with reference to FIG. FIG. 4 shows an example in which the present invention is applied to a photodiode. N-I was obtained by metalorganic vapor phase epitaxy.
On the nP substrate 1, the undoped InP layer 2 is 1 μm, the undoped InGaAs layer 6 (wavelength 1.67 μm, lattice matching with InP) is 1 μm, the undoped InP layer 2 is 1 μm, and the undoped InGaAsP layer 7 (wavelength 1.10 μm, In
0.1 μm was grown to a lattice match with P). Next, the undoped InGaAsP layer 7 was selectively etched with a sulfuric acid-based etching solution to partially form a contact layer. The multilayer structure was introduced into a vapor phase growth apparatus, and PH 3 (5
0%, 10 cc / min), DMZn (2000 pp
m, 2000 cc / min) and hydrogen (100%, 4 l / min) for 30 minutes. InGaAsP layer 7
Using as a mask, a p-type highly doped InP diffusion layer 8 (Zn concentration: 8E18) was formed by vapor phase diffusion.

【0015】本実施例では、従来の閉管法に比べ、10
倍から100倍程度の大面積化が可能となり、ばらつき
の1/5程度に低減できた。
In this embodiment, as compared with the conventional closed tube method, 10
It is possible to increase the area by a factor of 2 to 100 and reduce the variation to about 1/5.

【0016】[0016]

【発明の効果】本装置では3インチのウエハまで作製す
ることができる。また、最近のCVD装置では多数枚も
可能であり、十倍から百倍程度の大面積化が可能であ
る。また、成長中のドーピングでは面内のドーピング濃
度は一様であるが、本発明ではコンタクト層をマスクと
して、面内で選択的なドーピングが可能である。
According to the present apparatus, a 3-inch wafer can be manufactured. In addition, a large number of recent CVD apparatuses are possible, and the area can be increased to about 10 to 100 times. Further, in the case of doping during growth, the in-plane doping concentration is uniform, but in the present invention, the in-plane selective doping can be performed using the contact layer as a mask.

【0017】図3は、実施例1での拡散時間に対する拡
散深さの依存性であり、従来の閉管法でのばらつきを1
/5程度に抑えることができた。
FIG. 3 shows the dependence of the diffusion depth on the diffusion time in the first embodiment, and the variation in the conventional closed tube method is 1
It could be suppressed to about / 5.

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

【図1】実施例1での本発明の原理を示す特性図。FIG. 1 is a characteristic diagram showing the principle of the present invention in a first embodiment.

【図2】接触比抵抗測定用の素子の断面図。FIG. 2 is a sectional view of an element for measuring contact specific resistance.

【図3】本発明の効果を示す、拡散深さの時間依存性の
特性図。
FIG. 3 is a characteristic diagram of time dependence of diffusion depth showing the effect of the present invention.

【図4】本発明をフォトダイオードに適用した例の断面
図。
FIG. 4 is a sectional view of an example in which the present invention is applied to a photodiode.

【符号の説明】[Explanation of symbols]

1…n−InP基板、2…アンドープInP層、3…ア
ンドープInGaAsP層。
1 ... n-InP substrate, 2 ... undoped InP layer, 3 ... undoped InGaAsP layer.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 古森 正明 東京都国分寺市東恋ケ窪1丁目280番地 株式会社日立製作所中央研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Masaaki Furumori 1-280 Higashi Koigokubo, Kokubunji, Tokyo Inside the Central Research Laboratory, Hitachi, Ltd.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】半導体基板上に、p型クラッド層、p型コ
ンタクト層、p型電極を有し、上記p型コンタクト層の
結晶組成がInGaAs、InGaAsPである半導体
装置のp型コンタクト層を、多層成長後に開管法での気
相拡散によりドーピングする工程により形成することを
特徴とするp型コンタクト層の形成方法。
1. A p-type contact layer of a semiconductor device having a p-type cladding layer, a p-type contact layer, and a p-type electrode on a semiconductor substrate, wherein the p-type contact layer has a crystal composition of InGaAs or InGaAsP. A method for forming a p-type contact layer, which is formed by a step of doping by vapor phase diffusion by an open tube method after multi-layer growth.
【請求項2】請求項1において、p型不純物の上記気相
拡散時の原料ガスがDMZn、DEZn等のガスであ
り、これにP、AsのV族ガス、及び水素、窒素等のキ
ャリアガスが加えられていることを特徴とする請求項1
記載のp型コンタクト層の形成方法。
2. The material gas according to claim 1, wherein the source gas at the time of the vapor phase diffusion of p-type impurities is a gas such as DMZn and DEZn, and a group V gas of P and As and a carrier gas such as hydrogen and nitrogen. The method according to claim 1, wherein
The method for forming a p-type contact layer as described above.
JP9274393A 1993-04-20 1993-04-20 Vapor phase diffusion Pending JPH06310449A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9274393A JPH06310449A (en) 1993-04-20 1993-04-20 Vapor phase diffusion

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9274393A JPH06310449A (en) 1993-04-20 1993-04-20 Vapor phase diffusion

Publications (1)

Publication Number Publication Date
JPH06310449A true JPH06310449A (en) 1994-11-04

Family

ID=14062903

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9274393A Pending JPH06310449A (en) 1993-04-20 1993-04-20 Vapor phase diffusion

Country Status (1)

Country Link
JP (1) JPH06310449A (en)

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Cited By (10)

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JP6384646B1 (en) * 2017-05-12 2018-09-05 三菱電機株式会社 Manufacturing method of semiconductor device
WO2018207355A1 (en) * 2017-05-12 2018-11-15 三菱電機株式会社 Semiconductor device production method
CN110603623A (en) * 2017-05-12 2019-12-20 三菱电机株式会社 Method for manufacturing semiconductor device
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JP6509455B1 (en) * 2018-05-24 2019-05-08 三菱電機株式会社 Method of manufacturing III-V compound semiconductor device
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