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JPH041496B2 - - Google Patents
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JPH041496B2 - - Google Patents

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Publication number
JPH041496B2
JPH041496B2 JP20656481A JP20656481A JPH041496B2 JP H041496 B2 JPH041496 B2 JP H041496B2 JP 20656481 A JP20656481 A JP 20656481A JP 20656481 A JP20656481 A JP 20656481A JP H041496 B2 JPH041496 B2 JP H041496B2
Authority
JP
Japan
Prior art keywords
layer
inp
growth
gaxasyp
gaxas
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
JP20656481A
Other languages
Japanese (ja)
Other versions
JPS58107629A (en
Inventor
Kenshin Taguchi
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP56206564A priority Critical patent/JPS58107629A/en
Publication of JPS58107629A publication Critical patent/JPS58107629A/en
Publication of JPH041496B2 publication Critical patent/JPH041496B2/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
    • C30B19/02Liquid-phase epitaxial-layer growth using molten solvents, e.g. flux
    • C30B19/04Liquid-phase epitaxial-layer growth using molten solvents, e.g. flux the solvent being a component of the crystal composition

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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)
  • Semiconductor Lasers (AREA)
  • Led Devices (AREA)

Description

【発明の詳細な説明】 本発明は、InP基板上にIn1-xGaxAs、In1-x
GaxAsyP1-y及びInP等のエピタキシヤル結晶層
を多層成長する液相エピタキシヤル(LPE)成
長方法に関するものである。
[Detailed description of the invention] The present invention provides In 1-x GaxAs, In 1-x GaxAs, In 1-x
This invention relates to a liquid phase epitaxial (LPE) growth method for growing multiple epitaxial crystal layers such as GaxAsyP 1-y and InP.

化合物半導体の多層液相エピタキシヤル成長は
光通信用発光・受光素子である、半導体レーザ
(以下LDと呼ぶ)、発光ダイオード(以下LEDと
呼ぶ)、アバランシ・フオトダイオード(以下
APDと呼ぶ)、フオトダイオード(以下PDと呼
ぶ)等の素子を得るための重要な結晶成長方法で
あり、欠陥の少ない高品質な成長結晶層が得られ
る成長方法の確立が望まれている。現在、光通信
用発光素子としては発振波長が0.8から1.6μm域の
GaAs−GaAlAs系あるいはInP−InGaAsP系の
LD及びLEDの研究開発が主流である。また、
GaAs−GaAlAs系のLD及びLEDの主な発振波長
0.8μm〜0.87μmに対する光検出器としてはSi単結
晶を用いたPDあるいはAPDが広く実用されてい
る。しかしながらSi単結晶では1μm波長以上の光
を検出することは吸収係数が小さくなるために実
用上作製困難であり、光フアイバーの伝送損失の
低い1.1μm〜1.6μm波長域では使用することがで
きない。また1.1μm以上1.5μm波長域用としては
Ge−APDがあるが暗電流と過剰雑音の点で必ず
しも光通信用として最適な光検出器ではない。こ
のため−族化合物半導体等によるPDあるい
はAPDが要求されており、InGaAs、InGaAsP、
GaAlSb、GaAlAsSb、GaSb等による試作報告
例がある。第1図はIn1-xGaxAsyP1-y層を光吸収
層としてInP中にp−n接合を形成したプレーナ
型APDの報告例であり、特願昭54−39169にくわ
しく述べられている。この構造のウエーハの形状
としてはn+−InP基板11上にn+−InPバツフア
ー層12を形成し、次にn型In1-xGaxAsyP1-y
(光吸収層)13を形成した後n型InP層14を
形成したウエーハであり、このウエーハに基本的
には選択拡散によりp+領域15をInP層14中に
形成することにより、低暗電流、高増倍特性の
APDが得られている。これと同様な素子構造を
InPと格子整合するIn1-xGaxAsyP1-yの最長波長
組成に相当するIn1-xGaxAsを光吸収層として、
In1-xGaxAsyP1-yを活性層とするLDあるいは
LED等の光源からの光の全波長光を検出する
APD、PD等を作製する場合には、In1-xGaxAs
上にInP層をエピタキシヤル成長する必要があ
る。しかしながら液相成長方法においては、
In1-xGaxAs上にInPを成長しようとすると、InP
成長用溶液に、逆にIn1-xGaxAs層が溶けてしま
うといういわゆるメルトバツク現象が生じ多層構
造ができない。このためIn1-xGaxAs上にいわゆ
るアンチ・メルトバツクIn1-xGaxAsyP1-y層をエ
ピタキシヤル成長後InP層を成長することにより
層構造が得られている。この場合においても
In1-xGaxAsとIn1-xGaxAsyP1-y界面を良好な鏡
面にするためにアンチ・メルトバツクIn1-x
GaxAsyP1-yの組成としてx0.24、y≧0.55程
度が必要でありこれについては特願昭56−109690
にくわしく述べてある。また、In1-xGaxAsを光
吸収層として1.0μm以上の厚膜成長した上記同様
構造のAPD用ウエーハあるいは、光源としての
LED用として2μm程度の厚膜In1-xGaxAsyP1-y
を活性層として上記In1-xGaxAsyP1-y層上にInP
層を液相エピタキシヤル成長する場合に、作製ウ
エーハの中央領域においては比較的良品質な結晶
層が得られるが、ウエーハの周縁領域ではミスフ
イツト転位が導入され、極端な場合にはヘテロな
層構造をなさないことがある。第2図、第3図に
それを説明するための概略図をIn1-xGaxAsを光
吸層とするAPD用ウエーハの作製例をもとに説
明する。第2図はn+型InP(100)基板21上にn+
−InP22をLPE成長後、成長温度で格子整合条
件を満足するようにn型In1-xGaxAs23を2μm
程度、次にアンチ・メルトバツクn型In0.76Ga0.24
As0.55P0.45層24を0.5μm程度LPE成長した断面
である。このとき、ウエーハの周縁部28では、
In1-xGaxAs層23のいわゆるエツジ・グロース
と呼ばれる異常成長が起つており、In1-xGaxAs
層の層厚を1.0μm以上にしたとき、特に顕著であ
り、数10μmの高さに達することもある。次にこ
の様なウエーハ上にInPを連続しLPE成長した場
合の結果の一例を第3図に示すが、ウエーハの中
央領域20においてはn−InP層25を成長した
後も比較的良好な結晶性を有するのと比較して、
ウエーハの周縁部領域28においては、いつたん
成長したIn1-xGaxAs23及びIn1-xGaxAsyP1-y
24層がInP成長溶液中に溶けこんでなくなつて
しまい、その領域を基点にしてミスフイツト転位
29がInP層25中に多量に発生する。またこの
様なミスフイツト転位はウエーハの中央領域20
まで伸びていることがしばしばあり、良品質を得
る成長方法が望まれている。
Multilayer liquid-phase epitaxial growth of compound semiconductors is used in light-emitting and light-receiving devices for optical communications, such as semiconductor lasers (hereinafter referred to as LDs), light-emitting diodes (hereinafter referred to as LEDs), and avalanche photodiodes (hereinafter referred to as LEDs).
This is an important crystal growth method for obtaining elements such as APD (hereinafter referred to as APD) and photodiodes (hereinafter referred to as PD), and it is desired to establish a growth method that can obtain a high-quality grown crystal layer with few defects. Currently, light emitting devices for optical communications have oscillation wavelengths in the 0.8 to 1.6 μm range.
GaAs-GaAlAs system or InP-InGaAsP system
Research and development of LD and LED is the mainstream. Also,
Main oscillation wavelengths of GaAs-GaAlAs LDs and LEDs
PD or APD using Si single crystal is widely used as a photodetector for 0.8 μm to 0.87 μm. However, it is practically difficult to detect light with a wavelength of 1 μm or more in Si single crystal due to its small absorption coefficient, and it cannot be used in the 1.1 μm to 1.6 μm wavelength range where optical fiber has low transmission loss. Also, for wavelength range of 1.1μm or more and 1.5μm.
Although there is a Ge-APD, it is not necessarily the best photodetector for optical communications due to dark current and excessive noise. For this reason, PDs or APDs using - group compound semiconductors are required, and InGaAs, InGaAsP,
There are reports of prototype production using GaAlSb, GaAlAsSb, GaSb, etc. FIG. 1 is a reported example of a planar type APD in which a p-n junction is formed in InP using an In 1-x GaxAsyP 1-y layer as a light absorbing layer, and is described in detail in Japanese Patent Application No. 39169/1983. The shape of a wafer with this structure is to form an n + -InP buffer layer 12 on an n + -InP substrate 11, then form an n-type In 1-x GaxAsyP 1-y layer (light absorption layer) 13, and then This is a wafer on which an n-type InP layer 14 is formed, and by basically forming a p + region 15 in the InP layer 14 by selective diffusion, low dark current and high multiplication characteristics are achieved.
APD is obtained. A device structure similar to this
In 1-x GaxAs, which corresponds to the longest wavelength composition of In 1- x GaxAsyP 1-y, which is lattice matched to InP, is used as a light absorption layer.
LD with In 1-x GaxAsyP 1-y as active layer or
Detects all wavelengths of light from light sources such as LEDs
When manufacturing APD, PD, etc., In 1-x GaxAs
It is necessary to epitaxially grow an InP layer on top. However, in the liquid phase growth method,
When trying to grow InP on In 1-x GaxAs, InP
Conversely, a so-called meltback phenomenon occurs in which the In 1-x GaxAs layer dissolves in the growth solution, making it impossible to form a multilayer structure. For this reason, a layered structure is obtained by epitaxially growing a so-called anti-meltback In 1-x GaxAsyP 1-y layer on In 1-x GaxAs and then growing an InP layer. Even in this case
In 1-x GaxAs and In 1-x GaxAsyP 1-y Anti-melt back to make the interface a good mirror surface In 1-x
The composition of GaxAsyP 1-y is required to be about x0.24 and y≧0.55, and this is discussed in Japanese Patent Application No. 56-109690.
It is described in detail. In addition, APD wafers with the same structure as above in which In 1-x GaxAs is grown as a light absorption layer with a thickness of 1.0 μm or more, or as a light source.
For LED use, a thick In 1-x GaxAsyP 1-y layer of about 2 μm is used as an active layer, and InP is placed on the In 1-x GaxAsyP 1-y layer.
When a layer is grown by liquid phase epitaxial growth, a crystal layer of relatively good quality is obtained in the central region of the fabricated wafer, but misfit dislocations are introduced in the peripheral region of the wafer, and in extreme cases, a heterogeneous layer structure is obtained. Sometimes it doesn't work. FIGS. 2 and 3 are schematic diagrams for explaining this, based on an example of fabricating an APD wafer using In 1-x GaxAs as a light absorbing layer. Figure 2 shows an n + type on an n + type InP (100) substrate 21.
- After growing InP22 by LPE, grow n-type In 1-x GaxAs23 to 2 μm to satisfy lattice matching conditions at the growth temperature.
degree, then anti-meltback n-type In 0.76 Ga 0.24
This is a cross section of an As 0.55 P 0.45 layer 24 grown by LPE to a thickness of about 0.5 μm. At this time, at the peripheral edge 28 of the wafer,
An abnormal growth called so-called edge growth has occurred in the In 1-x GaxAs layer 23, and the In 1-x GaxAs
This is particularly noticeable when the layer thickness is 1.0 μm or more, and can reach a height of several tens of μm. Next, FIG. 3 shows an example of the results when InP is continuously grown by LPE on such a wafer. In the central region 20 of the wafer, even after growing the n-InP layer 25, relatively good crystallization is observed. Compared to having a gender,
In the peripheral region 28 of the wafer, In 1-x GaxAs 23 and In 1-x GaxAsyP 1-y that have grown over time
The layer 24 dissolves into the InP growth solution and disappears, and a large number of misfit dislocations 29 are generated in the InP layer 25 starting from that region. Furthermore, such misfit dislocations occur in the central region 20 of the wafer.
It is often the case that the plant grows to a certain extent, and a growth method that achieves good quality is desired.

本発明の目的は上記したように特にIn1-x
GaxAsあるいはIn1-xGaxAsyP1-y層の比較的厚
い膜を必要とする多層液相エピタキシヤル成長方
法を工夫して、欠陥が少なく均一性に優れた高品
質エピタキシヤル成長層を形成するものである。
As mentioned above, the object of the present invention is particularly to In 1-x
GaxAs or In 1-x GaxAsyP A method that creates a high-quality epitaxial growth layer with few defects and excellent uniformity by devising a multilayer liquid phase epitaxial growth method that requires a relatively thick film of 1-y layers. It is.

本発明の液相エピタキシヤル成長方法は、少く
とも、InP基板上にIn1-xGaxAsあるいはIn1-x
GaxAsyP1-y(0.47>x≧0.24、1>y≧0.55)液
相エピタキシヤル成長層を形成する工程と、当該
液相エピタキシヤル成長層を形成した基板ウエー
ハをInPエピタキシヤル成長用溶液に接触するこ
となく移動させた後、InPエピタキシヤル成長用
溶液がInPエピタキシヤル成長前の基板ウエーハ
の周縁部に接触することなくInP層を液相エピタ
キシヤル成長する工程とを有する構成となつてい
る。
The liquid phase epitaxial growth method of the present invention includes at least In 1-x GaxAs or In 1-x GaxAs on an InP substrate.
GaxAsyP 1-y (0.47>x≧0.24, 1>y≧0.55) Step of forming a liquid phase epitaxial growth layer and contacting the substrate wafer on which the liquid phase epitaxial growth layer is formed with an InP epitaxial growth solution. After moving the InP epitaxial growth solution without contacting the peripheral edge of the substrate wafer before InP epitaxial growth, the InP layer is liquid-phase epitaxially grown.

次に本発明の優れた利点について一実施例にも
とずいて説明する。本実施例ではIn1-xGaxAsを
光吸収層とするAPD及びPD用ウエーハの結晶成
長例であり、第4図に本発明の方法を実現するた
めの液相エピタキシヤル成長装置の例を示す。成
長用ボート1は、少くともIn1-xGaxAsyP1-y四元
組成xとyがInPと格子整合できるべく調合した
In、GaAs、InP、InAsを混合したIn1-x
GaxAsyP1-y成長溶液2及び前記In1-x
GaxAsyP1-y成長用溶液収容ボート底面より小さ
な寸法底面を有する溶液収容ボート部3を有して
おり、InP基板結晶4を図中矢印5で示した方向
に移動することにより上記In1-xGaxAsyP1-y成長
用溶液2と接触できIn1-xGaxAsyP1-y層がLPE成
長できる。また成長用ボートは前記成長用溶液収
容ボート3上に前記成長用ボート1とは別のボー
ト6を有しておりボート6中にはInとInPを混合
したInP成長用溶液7を備えており、前記InP基
板4が成長用溶液2と接触して所定の時間In1-x
GaxAsyP1-y層をLPE成長後、InP基板4を図中
矢印5の方向に移動することによりInP基板4は
成長用溶液収容ボート部3の下に移行できる。こ
のときInP基板4上のIn1-xGaxAsyP1-y成長層の
周縁が成長用溶液収容ボート部底面に現われない
ことをあらかじめInP基板4の移動(図中矢向
5)距離により確認した後、前記ボート6を図中
矢印8の方向に移動することによりInP成長用溶
液7を成長用溶液収容ボート部3中におとしこ
む。この操作後、所定時間保持することにより所
定厚のInP層が得られ本発明の液相成長方法が実
現できる。第5図にIn1-xGaxAsを光吸収層とす
るAPD及びPD用ウエーハの結晶成長例の概略横
断面を示す。成長用ボートは少くとも上記第4図
で示した構成部品を有する横型スライドボートで
あり、成長方法は例えば650℃飽和温度で1時間
程度保持後、急冷な行ない640℃に達したならば
n+−InP基板31をInPバツフアー層成長用溶液
下に移動することによりn+InPバツフアー層32
を成長し、637℃に達つしたら650℃でIn溶液に
Ga及びAsが一定量仕込まれた溶液下に、前記
InP基板31を移行することによりn+InPバツフ
アー層32の成長を停止し、ひき続きn型In1-x
GaxAs層33を成長する。次に635℃に達つした
ら降下温度を0.2℃/分に移行し、所定時間前記
In1-xGaxAs33を成長後、650℃でIn溶液に、
Ga、As及びPが所定量仕込まれた波長組成
1.3μm相当のIn1-xGaxAsyP1-y成長溶下に前記
InP基板31を移行することによりIn1-xGaxAs
層33上にn型In1-xGaxAsyP1-y層34をLPE成
長する。ここで10秒程度成長することにより
0.5μm程度のIn1-xGaxAsyP1-y層34を得る。こ
の成長が前記第4図で説明した成長用溶液2によ
るLPE成長に対応しており、In1-xGaxAsyP1-y
34をLPE成長後、前記第4図で説明した手順
によりn型P層35を所定時間成長することによ
り第5図のLPE結晶ウエーハができる。本実施
例においてはIn1-xGaxAs層のLPE成長端での異
常成長領域及びそのIn1-xGaxAs上のアンチ・メ
ルトバツクIn1-xGaxAsyP1-y層領域にInP成長用
溶液が接触することなく前記LPE成長異常領域
上を除外した領域にのみInP層をLPE成長するこ
とにより上記第2図及び第3図を用いて説明した
場合と較べて、InP成長層下でのヘテロ層構造の
みだれ及びInP層中へのすべり転位であるところ
のミスフイツト転位の導入が完全に抑止されてお
り高品質なAPD用結晶が得られる。
Next, the advantages of the present invention will be explained based on one embodiment. This example shows an example of crystal growth of an APD and PD wafer using In 1-x GaxAs as a light absorption layer, and Fig. 4 shows an example of a liquid phase epitaxial growth apparatus for realizing the method of the present invention. . Growth boat 1 was prepared so that at least In 1-x GaxAsyP 1-y quaternary composition x and y could be lattice matched with InP.
In 1-x, a mixture of In, GaAs, InP, and InAs
GaxAsyP 1-y growth solution 2 and the In 1-x
It has a solution storage boat part 3 having a smaller bottom surface than the bottom surface of the GaxAsyP 1-y growth solution storage boat, and by moving the InP substrate crystal 4 in the direction shown by the arrow 5 in the figure, the above In 1-x It can be contacted with the GaxAsyP 1-y growth solution 2 and an In 1-x GaxAsyP 1-y layer can be grown by LPE. Further, the growth boat has a boat 6 separate from the growth boat 1 on the growth solution storage boat 3, and the boat 6 is equipped with an InP growth solution 7 containing a mixture of In and InP. , the InP substrate 4 is in contact with the growth solution 2 for a predetermined time In 1-x
After the GaxAsyP 1-y layer is grown by LPE, the InP substrate 4 can be moved under the growth solution storage boat section 3 by moving the InP substrate 4 in the direction of the arrow 5 in the figure. At this time, after confirming in advance that the periphery of the In 1-x GaxAsyP 1-y growth layer on the InP substrate 4 does not appear on the bottom surface of the growth solution storage boat by the distance the InP substrate 4 is moved (arrow direction 5 in the figure), By moving the boat 6 in the direction of arrow 8 in the figure, the InP growth solution 7 is poured into the growth solution storage boat section 3. After this operation, by holding for a predetermined time, an InP layer of a predetermined thickness can be obtained, and the liquid phase growth method of the present invention can be realized. FIG. 5 shows a schematic cross section of an example of crystal growth of an APD and PD wafer using In 1-x GaxAs as a light absorption layer. The growth boat is a horizontal slide boat that has at least the components shown in Figure 4 above, and the growth method is, for example, held at a saturation temperature of 650°C for about an hour, then rapidly cooled, and once the temperature reaches 640°C.
By moving the n + -InP substrate 31 under the InP buffer layer growth solution, the n + InP buffer layer 32 is grown.
Grow the In solution at 650℃ once it reaches 637℃.
Under a solution containing a certain amount of Ga and As,
By transferring the InP substrate 31, the growth of the n + InP buffer layer 32 is stopped, and the n-type In 1-x continues to grow.
GaxAs layer 33 is grown. Next, when the temperature reaches 635℃, the temperature decrease is shifted to 0.2℃/min, and the
After growing In 1-x GaxAs33, it was added to In solution at 650℃.
Wavelength composition containing predetermined amounts of Ga, As, and P
1.3 μm equivalent of In 1-x GaxAsyP 1-y grown under the above-mentioned
In 1-x GaxAs by transferring the InP substrate 31
An n-type In 1-x GaxAsyP 1-y layer 34 is grown on the layer 33 by LPE. By growing here for about 10 seconds
An In 1-x GaxAsyP 1-y layer 34 of about 0.5 μm is obtained. This growth corresponds to the LPE growth using the growth solution 2 explained in FIG. By growing layer 35 for a predetermined period of time, the LPE crystal wafer of FIG. 5 is produced. In this example, the InP growth solution comes into contact with the abnormal growth region at the LPE growth edge of the In 1 -x GaxAs layer and the anti-meltback In 1-x GaxAsyP 1-y layer region on the In 1-x GaxAs. By growing the InP layer by LPE only in the region excluding the abnormal LPE growth region, the heterolayer structure under the InP growth layer can be improved compared to the case explained using FIGS. 2 and 3 above. The introduction of misfit dislocations, which are slip dislocations, into the slant and InP layers is completely suppressed, and a high-quality crystal for APD can be obtained.

尚、実施例ではInP−InGaAs−InGaAsP−InP
層構造を作製する例について述べたが、InP−
InGaAs−InP、InP−InGaAsP−InP層構造を作
製する場合でも同じである。
In the example, InP−InGaAs−InGaAsP−InP
Although we have described an example of creating a layered structure, InP−
The same holds true when producing InGaAs-InP and InP-InGaAsP-InP layer structures.

以上、In1-xGaxAs層を光吸収層としたAPDあ
るいはPD用結晶成長について述べたが、比較的
厚膜を必要とするIn1-xGaxAsyP1-yを光吸収とす
るAPDあるいはIn1-xGaxAsyP1-y層を活性層と
するLED等においても上記In1-xGaxAsyP1-y
上にInP層を液相エピタキシヤル成長する素子構
造においては、0.47>x≧0.24、1>y≧0.55組
成でのIn1-xGaxAsyP1-y液相エピタキシヤル成長
においてウエーハ端での異常成長が大きいことが
知られており、厚膜In1-xGaxAs、あるいはIn1-x
GaxAsyP1-y層を必要とする多層構造液相エピタ
キシヤル成長に有用であり高品質なエピタキシヤ
ル成長層が得られる。
Above, we have described crystal growth for APD or PD using In 1-x GaxAs as the light absorption layer, but APD or In 1 -x GaxAsyP 1-y that requires a relatively thick film as the light absorption Even in LEDs etc. in which the -x GaxAsyP 1-y layer is the active layer, in the device structure where the InP layer is liquid-phase epitaxially grown on the In 1-x GaxAsyP 1-y layer, 0.47>x≧0.24, 1> It is known that abnormal growth at the wafer edge is large in In 1-x Gax AsyP 1-y liquid phase epitaxial growth with a composition of y≧0.55, and thick film In 1-x GaxAs or In 1-x
It is useful for liquid phase epitaxial growth of multilayer structures requiring GaxAsyP 1-y layers, and provides high quality epitaxial growth layers.

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

第1図はIn1-xGaxAsyP1-yを用いたAPDの報
告例であり、11はn+−InP基板、12はn+
InPバツフアー層、13はn型In1-xGaxAsyP1-y
層、14はn型InP層であり、15はp型不純物
を選択拡散技術により前記14層中に形成したも
のである。第2図はIn1-xGaxAs層の液相エピタ
キシヤル成長したときの成長端での異常成長を示
したものであり、21はn+−InP基板、22はn+
−InPバツフアー層、23はn型In1-xGaxAs層、
24はn型In1-xGaxAsyP1-y層である。第3図は
第2図のウエーハ上にn型InP層25を液相成長
した場合のウエーハ断面を示しており、ウエーハ
周縁、特に上記第2図のIn1-xGaxAs23異常成
長領域上にIn1-xGaxAsyP1-y層24を介してInP
層25を成長したときIn1-xGaxAs及びIn1-x
GaxAsyP1-y層がとけ、この領域を起点にしてミ
スフイツトすべり転位がn−InP層25中に伸び
ていることを示している。第4図は本発明の方法
を実現するための液相成長装置を示したものであ
り、 1は液相成長を実施するために用いるボート、
2は成長用溶液、3は2の成長後ひき続きエピタ
キシヤル成長を行なうべき成長用溶液収容ボート
部、4は基板結晶、5は基板結晶の移動方向を示
す矢印である。6はボート1とは別構成のボート
であり、7は成長用溶液、8はボート6を移動す
る方向を示す矢印であり、成長溶液7を成長用溶
液収容ボート部3におとしこむ操作をあらわす。
第5図は、本発明の液相エピタキシヤル成長方法
によつて得られた多層構造ウエーハ断面を示した
ものであり、31はn+型InP基板、32はn+
InP層、33はn型In1-xGaxAs層、34はn型
In1-xGaxAsyP1-y層、35はn型InP層である。
Figure 1 shows a reported example of APD using In 1-x GaxAsyP 1-y , 11 is n + -InP substrate, 12 is n + -
InP buffer layer, 13 is n-type In 1-x GaxAsyP 1-y
Layer 14 is an n-type InP layer, and layer 15 is a layer in which p-type impurities are formed by selective diffusion technology. Figure 2 shows the abnormal growth at the growth edge when an In 1-x GaxAs layer is grown by liquid phase epitaxial growth, 21 is an n + -InP substrate, 22 is an n +
-InP buffer layer, 23 is n-type In 1-x GaxAs layer,
24 is an n-type In 1-x GaxAsyP 1-y layer. FIG. 3 shows a cross section of a wafer when an n-type InP layer 25 is grown in a liquid phase on the wafer shown in FIG . 1-x GaxAsyP 1-y InP via layer 24
When layer 25 is grown, In 1-x GaxAs and In 1-x
This shows that the GaxAsyP 1-y layer has melted and misfit slip dislocations have extended into the n-InP layer 25 starting from this region. FIG. 4 shows a liquid phase growth apparatus for implementing the method of the present invention, in which 1 is a boat used for carrying out liquid phase growth;
2 is a growth solution; 3 is a boat containing a growth solution in which epitaxial growth is to be continued after the growth in 2; 4 is a substrate crystal; and 5 is an arrow indicating the moving direction of the substrate crystal. 6 is a boat having a different configuration from the boat 1, 7 is a growth solution, and 8 is an arrow indicating the direction in which the boat 6 is moved, representing the operation of pouring the growth solution 7 into the growth solution storage boat section 3. .
FIG. 5 shows a cross section of a multilayer structure wafer obtained by the liquid phase epitaxial growth method of the present invention, where 31 is an n + type InP substrate and 32 is an n + − type InP substrate.
InP layer, 33 is n-type In 1-x GaxAs layer, 34 is n-type
In 1-x GaxAsyP 1-y layer, 35 is an n-type InP layer.

Claims (1)

【特許請求の範囲】[Claims] 1 少くともInP基板上にIn1-xGaxAsあるいは
In1-xGaxAsyP1-y(0.47>x0.24、1>y≧
0.55)液相エピタキシヤル成長層を形成する工程
と、当該エピタキシヤル成長層を形成した基板ウ
エーハをInPエピタキシヤル成長用溶液に接触す
ることなく移動した後、InPエピタキシヤル成長
用溶液がInPエピタキシヤル成長前の基板ウエー
ハの液相エピタキシヤル成長層周縁部に接触する
ことなく前記液相エピタキシヤル成長層上にInP
層を液相エピタキシヤル成長する工程とを有する
ことを特徴とする液相エピタキシヤル成長方法。
1 At least In 1-x GaxAs or
In 1-x GaxAsyP 1-y (0.47>x0.24, 1>y≧
0.55) After forming a liquid phase epitaxial growth layer and moving the substrate wafer on which the epitaxial growth layer has been formed without contacting the InP epitaxial growth solution, the InP epitaxial growth solution InP is deposited on the liquid phase epitaxial growth layer without contacting the peripheral edge of the liquid phase epitaxial growth layer of the substrate wafer before growth.
A liquid phase epitaxial growth method comprising the step of liquid phase epitaxial growth of a layer.
JP56206564A 1981-12-21 1981-12-21 Liquid phase epitaxial growth method Granted JPS58107629A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56206564A JPS58107629A (en) 1981-12-21 1981-12-21 Liquid phase epitaxial growth method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56206564A JPS58107629A (en) 1981-12-21 1981-12-21 Liquid phase epitaxial growth method

Publications (2)

Publication Number Publication Date
JPS58107629A JPS58107629A (en) 1983-06-27
JPH041496B2 true JPH041496B2 (en) 1992-01-13

Family

ID=16525476

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56206564A Granted JPS58107629A (en) 1981-12-21 1981-12-21 Liquid phase epitaxial growth method

Country Status (1)

Country Link
JP (1) JPS58107629A (en)

Also Published As

Publication number Publication date
JPS58107629A (en) 1983-06-27

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