JPS6235514A - Molecular beam crystal growth method - Google Patents

Molecular beam crystal growth method

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Publication number
JPS6235514A
JPS6235514A JP17478985A JP17478985A JPS6235514A JP S6235514 A JPS6235514 A JP S6235514A JP 17478985 A JP17478985 A JP 17478985A JP 17478985 A JP17478985 A JP 17478985A JP S6235514 A JPS6235514 A JP S6235514A
Authority
JP
Japan
Prior art keywords
substrate
thermal conductivity
gap
plane
plate
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.)
Granted
Application number
JP17478985A
Other languages
Japanese (ja)
Other versions
JPH0319693B2 (en
Inventor
Shigeru Kuroda
黒田 滋
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP17478985A priority Critical patent/JPS6235514A/en
Publication of JPS6235514A publication Critical patent/JPS6235514A/en
Publication of JPH0319693B2 publication Critical patent/JPH0319693B2/ja
Granted legal-status Critical Current

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  • Crystals, And After-Treatments Of Crystals (AREA)
  • Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)

Abstract

PURPOSE:To exclude the use of an indium solder and to obtain the uniformity in a plane of a grown film by interposing a thermal conductive plate having thermal conductivity anisotropy in which thermal conductivity is large in the plane direction between a substrate and a heater through a gap on the substrate. CONSTITUTION:A heating plate 7 having thermal conductivity anisotropy that thermal conductivity is large in plane direction is interposed between a substrate S and a heater 6 for heating the substrate S through a gap G on the substrate S, and a growing substance is accumulated on the substrate S. The material of the plate 7 is preferably pyrolytic boron nitride (pBN). Since thermal transfer from the plate 7 to the substrate S is by heat radiation due to the presence of the gap G, it is not necessary to use an indium solder. Since the plate 7 has thermal conductivity anisotropy that the thermal conductivity is large in plane direction, even if the planar distribution of the heat received from the heater 6 is irregular, the temperature distribution of the plane opposed to the substrate S becomes uniform, the uniformity in the plane of the temperature of the substrate S is obtained to obtain a preferably grown film.

Description

【発明の詳細な説明】 〔概要〕 分子線結晶成長方法における成長物質を堆積させる基板
の支持方法において、 基板とヒータとの間に熱伝導率が面方向に大なる熱伝導
率異方性を有する熱伝導板を該基板に対して間隙を設け
て介在させることにより、インジウム半田の使用を排除
し且つ成長膜の面内均一性を確保したものである。
[Detailed Description of the Invention] [Summary] In a method for supporting a substrate on which a growth substance is deposited in a molecular beam crystal growth method, the thermal conductivity between the substrate and the heater has a large thermal conductivity anisotropy in the in-plane direction. By interposing the heat conductive plate with the substrate with a gap therebetween, the use of indium solder can be eliminated and the in-plane uniformity of the grown film can be ensured.

〔産業上の利用分野〕[Industrial application field]

分子線結晶成長法(MBE)は、基板上に堆積される成
長膜に対して例えば10人程度の膜厚制御が可能であり
、然も多層構成の膜成長を連続して行うことが出来ると
言う際立った特徴を有するため、近年、半導体素子の形
成に使用される化合物半導体の結晶成長において注目さ
れるようになってきた。
Molecular beam crystal growth (MBE) allows the thickness of a grown film deposited on a substrate to be controlled by, for example, about 10 people, and it is also possible to continuously grow a multilayered film. Due to these outstanding characteristics, in recent years, it has attracted attention in the crystal growth of compound semiconductors used in the formation of semiconductor devices.

そして、成長膜の面内均一性を確保したうえで、成長後
に成長膜を汚染させないないような基板の取扱いが出来
るようにすることが望まれている。
It is desired to ensure in-plane uniformity of the grown film and to be able to handle the substrate in a manner that does not contaminate the grown film after growth.

〔従来の技術〕[Conventional technology]

MBEは1.第5図の側断面図に示す如く、超高真空の
チャンバ1の中において、基板支持器2に支持され加熱
された基板Sに分子線源3から放射させた成長物質の分
子線を矢印のように基板Sに照射し、基板Sの表面上に
該成長物質を堆積させて結晶成長膜を形成する結晶成長
法である。
MBE is 1. As shown in the side sectional view of FIG. 5, in the ultra-high vacuum chamber 1, the molecular beams of the growth material radiated from the molecular beam source 3 are directed to the heated substrate S supported by the substrate supporter 2, as indicated by the arrow. This is a crystal growth method in which a crystal growth film is formed by irradiating the substrate S to deposit the growth material on the surface of the substrate S.

この際の基板Sの支持は、従来、第6図の側断面図に示
すように行っている。
Conventionally, the substrate S is supported at this time as shown in the side cross-sectional view of FIG.

同図において、4はモリブデン(hO)からなり円板状
をなし基板支持器2の正面に取付けられる基板支持板、
5は基板支持板4に基板Sを貼着するインジウム半田、
6は基板支持板4の背後に配置されるヒータ、である。
In the figure, 4 is a disk-shaped substrate support plate made of molybdenum (hO) and attached to the front of the substrate support 2;
5 is indium solder for attaching the substrate S to the substrate support plate 4;
6 is a heater arranged behind the substrate support plate 4.

基板支持板4の大きさは、例えば外径が約601亀φで
厚さが凡そ2〜31mである。
The size of the substrate support plate 4 is, for example, an outer diameter of about 601 mm and a thickness of about 2 to 31 m.

ヒータ6は、基板支持板4とインジウム半田5とを介し
て基板Sを加熱するが、基板支持板4の中で温度分布が
略均−になりその熱は熱伝導により基板Sに伝わり基板
Sの面内温度分布を略均−にしている。基板Sの温度の
面内均一性は、成長膜の面内均一性を得るために必要な
ものである。
The heater 6 heats the substrate S via the substrate support plate 4 and the indium solder 5, but the temperature distribution within the substrate support plate 4 is approximately uniform, and the heat is transferred to the substrate S by thermal conduction. The in-plane temperature distribution is approximately equal. In-plane uniformity of the temperature of the substrate S is necessary to obtain in-plane uniformity of the grown film.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

インジウム半田5を用いて基板Sを基板支持板4に貼付
するのは、基板Sにインジウム半田5を塗付けこれを基
板支持板4に貼付しているが、この塗付けには熟練を要
し、基板Sと基板支持板4との間がインジウムはんだ5
で完全に充填されない場合がある。
Attaching the substrate S to the substrate support plate 4 using indium solder 5 involves applying the indium solder 5 to the substrate S and attaching it to the substrate support plate 4, but this application requires skill. , indium solder 5 between the substrate S and the substrate support plate 4
It may not be completely filled.

このようになると、基板支持板4から基板Sへの熱伝達
のむらにより、成長膜表面に鐘状の凹凸(所謂クロスハ
ツチ)が生じて均一な成長膜が得られなくなる。
In this case, unevenness in heat transfer from the substrate support plate 4 to the substrate S causes bell-shaped irregularities (so-called cross hatches) on the surface of the grown film, making it impossible to obtain a uniform grown film.

また、基板Sが化合物半導体例えばガリウム砒素(Ga
As)などの如く脆い場合には上記貼付作業中に基板S
を破損させることがあり、特に基板Sが大型の場合に顕
著で、歩留り上の問題となる。
Further, the substrate S is a compound semiconductor such as gallium arsenide (Ga).
If the substrate S is fragile such as As), the substrate S
This is particularly noticeable when the substrate S is large in size, resulting in a yield problem.

更にインジウム半田5を用いる上記方法では、結晶成長
の後にインジウム半田5を基板Sから除去する必要があ
り、このためエツチングとラフピングなどを行っている
が、この作業中に肝心の成長膜が汚染される問題がある
Furthermore, in the above method using indium solder 5, it is necessary to remove the indium solder 5 from the substrate S after crystal growth, and etching and roughening are performed for this purpose, but the important grown film is contaminated during this process. There is a problem.

〔問題点を解決するための手段〕[Means for solving problems]

第1図は本発明の要旨を示す側断面図である。 FIG. 1 is a side sectional view showing the gist of the present invention.

上記問題点は、第1図に示す如く、基Fisと基板Sを
加熱するヒータ6との間に、熱伝導率が面方向に大なる
熱伝導率異方性を有する加熱板7を基板Sに対し間隙G
を設けて介在させ、基板S−ヒに成長物質を堆積させる
本発明の分子線結晶成長方法によって解決される。
As shown in FIG. 1, the above problem is such that a heating plate 7 having a large thermal conductivity anisotropy in the plane direction is placed between the substrate Fis and the heater 6 that heats the substrate S. Gap G
This problem is solved by the molecular beam crystal growth method of the present invention, in which a growth material is deposited on a substrate S-H by providing an intervening film.

本発明によれば上記加熱板7の材料は、パイロリテイッ
ク・ボロンナイトライド(pBN)であるのが望ましい
According to the present invention, the material of the heating plate 7 is preferably pyrolytic boron nitride (pBN).

〔作用〕[Effect]

本発明の方法は、ヒータ6は加熱板7と上記間隙Gとを
介して基板Sを加熱するが、間隙Gの存在のため加熱板
7から基板Sへの熱伝達は熱輻射によっているため、従
来のようにインジウム半田を使用する必要がない。
In the method of the present invention, the heater 6 heats the substrate S through the heating plate 7 and the gap G, but due to the existence of the gap G, heat transfer from the heating plate 7 to the substrate S is by thermal radiation. There is no need to use indium solder as in the past.

このことにより、従来方法で問題になったインジウム半
田の塗付けの際の基板破損、熱伝達のむらによるクロス
ハツチの発生、インジウム半田除去の際の成長膜汚染を
排除することが出来る。
This eliminates the problems associated with conventional methods, such as damage to the substrate when applying indium solder, occurrence of cross-hatching due to uneven heat transfer, and contamination of the grown film when removing indium solder.

また加熱板7は、熱伝導率が面方向に大なる熱伝導率異
方性を有するため、ヒータ6から受ける熱の面方向分布
にむらがあっても基板Sに対向する面の温度分布は均一
になり、基板Sの温度の面内均一性が確保される。
Furthermore, since the heating plate 7 has a large thermal conductivity anisotropy in the plane direction, even if the distribution of the heat received from the heater 6 in the plane direction is uneven, the temperature distribution on the surface facing the substrate S is The temperature of the substrate S becomes uniform, and the in-plane uniformity of the temperature of the substrate S is ensured.

特に加熱板7にpBN板を用いた場合には、結晶成長時
の加熱温度例えば500〜800℃におけるその面方向
の熱伝導率が面に垂直な方向の熱伝導率の20〜30倍
あるので、基板Sの温度の面内均一性は極めて優れたも
のになり、面内均一性の良好な成長膜を得ることが出来
る。
In particular, when a pBN plate is used as the heating plate 7, the thermal conductivity in the plane direction is 20 to 30 times the thermal conductivity in the direction perpendicular to the plane at a heating temperature of, for example, 500 to 800°C during crystal growth. , the in-plane temperature uniformity of the substrate S is extremely excellent, and a grown film with good in-plane uniformity can be obtained.

〔実施例〕〔Example〕

第2図は本発明の方法の実施例を示す側Vj?面図、第
3図は第2図図示実施例の要部分解斜視図、第4図は第
2図図示実施例と第6図図示従来方法との比較を示す成
長膜例の特性図、である。
FIG. 2 shows an embodiment of the method of the invention on the side Vj? 3 is an exploded perspective view of essential parts of the embodiment shown in FIG. 2, and FIG. 4 is a characteristic diagram of an example of a grown film showing a comparison between the embodiment shown in FIG. 2 and the conventional method shown in FIG. be.

第2図および第3図において、2は第6図に示した基板
支持器、6は同じくヒータ、7は厚さ約0.5flのp
BN&(例えばユニオンカーバイト社製“ボラロイ”坂
)でなる加熱板、8はMoでなる基板支持環、9はpB
Nでなり基板Sと加pA板7との間隙を設定する案内環
、lOはタングステン(W)またはタンタル(Ta)で
なり案内環9と加熱板7を基板支持環8に固定する環状
の押えばね、である。
In FIGS. 2 and 3, 2 is the substrate support shown in FIG.
A heating plate made of BN& (for example, "Bolloy" slope made by Union Carbide), 8 a substrate support ring made of Mo, 9 a pB
A guide ring is made of N and sets the gap between the substrate S and the pA plate 7, and lO is an annular presser made of tungsten (W) or tantalum (Ta) that fixes the guide ring 9 and the heating plate 7 to the substrate support ring 8. It is a spring.

基板支持環8は、案内環9、基板S、加熱板7および押
えばね10が挿入された後、基板支持器2の正面に第6
図図示の基板支持板4と同様に固定される。
After the guide ring 9, the substrate S, the heating plate 7 and the pressing spring 10 are inserted into the substrate support ring 8, a sixth
It is fixed in the same manner as the substrate support plate 4 shown in the figure.

案内環9における段差寸法aは、本実施例では基板Sの
厚さ約450μmに基板Sと加熱v!j、7との間隙G
の寸法約50μmを加えた寸法即ち約500μmにしで
ある。ここで重要なのは基板Sと加熱板7が接触しない
ように間隙Gの寸法を設定することで、間隙Gの寸法は
上記50μmに限定されるものではない。
In this embodiment, the step dimension a in the guide ring 9 is determined by heating v! Gap between j and 7
This is the sum of approximately 50 μm, that is, approximately 500 μm. What is important here is to set the size of the gap G so that the substrate S and the heating plate 7 do not come into contact with each other, and the size of the gap G is not limited to the above-mentioned 50 μm.

そして、基板Sの厚さや間隙Gの寸法が上述と異なる場
合は、それに見合った段差寸法aを有する案内環9を用
意すれば良い。
If the thickness of the substrate S or the dimensions of the gap G are different from those described above, it is sufficient to prepare a guide ring 9 having a corresponding step dimension a.

この構成の場合、間隙Gを積極的に保持出来るような介
在部材を設けていないが、本実施例を通用したMBEに
おいては、第5図に示す如く基板Sがやや下向きになた
め、基板Sの自重により間隙Gが保持される。このよう
にすることが困難な場合には例えばMoなどからなる介
在部材を基板Sの周辺部に設ければ良い。
In the case of this configuration, an intervening member that can actively maintain the gap G is not provided, but in the MBE that was used in this embodiment, the substrate S is oriented slightly downward as shown in FIG. The gap G is maintained by its own weight. If this is difficult, an intervening member made of Mo or the like may be provided around the substrate S.

またこの構成では、間隙Gは略閉じられた空間゛になっ
ている。これは、加熱された基板Sの裏面から蒸気圧の
高い物質例えばGaAsにおける砒素(八S)が蒸発し
てその面が荒れるのを防ぐ作用をなしている。
Further, in this configuration, the gap G is a substantially closed space. This serves to prevent a substance with a high vapor pressure, such as arsenic (8S) in GaAs, from evaporating from the back surface of the heated substrate S and causing the surface to become rough.

上記構成によりヒータ6で基板Sを加熱した際の熱の伝
達状況は先に説明した如くである。この場合の加熱板7
の熱伝導率異方性は気相成長により製造されたpBNの
特質であって、粉末成形により製造されたボロンナイト
ライド(B N) は、熱伝導率異方性がなく加熱板7
に用いるのに適切でない。
The heat transfer situation when the substrate S is heated by the heater 6 with the above configuration is as described above. Heating plate 7 in this case
Thermal conductivity anisotropy is a characteristic of pBN produced by vapor phase growth, whereas boron nitride (BN) produced by powder compaction has no thermal conductivity anisotropy and is
unsuitable for use in

第4図は第2図図示実施例と第6図図示従来方法とを用
い、2ニジ径のGaAs基板にシリコン(St)ドープ
のn型GaAsを成長した際のキャリア濃度(Nd)の
面内分布を一直径上で比較した特性図であり、実線(○
印)は第2図図示実施例によるもの、破線(×印)は第
6図図示従来方法によるものである。なお、従来方法に
よる場合は、インジウム半田による貼付を確実なものに
し、クロスハツチの発生がないようにしである。
Figure 4 shows the in-plane carrier concentration (Nd) when silicon (St)-doped n-type GaAs is grown on a 2-diameter GaAs substrate using the embodiment shown in Figure 2 and the conventional method shown in Figure 6. This is a characteristic diagram comparing the distribution on one diameter, and the solid line (○
2), and the broken line (x) indicates the conventional method shown in FIG. 6. Note that when using the conventional method, the attachment using indium solder is ensured and cross-hatching is prevented from occurring.

この特性図から明らかなように本実施例では、インジウ
ム半田を使用した従来方法より成長膜の面内均一性が向
−ヒしている。ちなみにデータから標準偏差σを求めて
均一性を示す σ/Ndの平均値 を求めると、その値
は、従来方法では9.0%であるのに対して実施例では
6.7%に向上している。
As is clear from this characteristic diagram, the in-plane uniformity of the grown film is better in this example than in the conventional method using indium solder. By the way, when the standard deviation σ is calculated from the data and the average value of σ/Nd, which indicates uniformity, is calculated, the value is 9.0% in the conventional method, but it improves to 6.7% in the example. ing.

そして言うまでもなく、上記実施例の場合インジウム半
田を用いていないので、・基板の破損、クロスハツチの
発生、成長膜の汚染の心配がない。
Needless to say, since indium solder is not used in the above embodiment, there is no fear of damage to the substrate, occurrence of cross-hatching, or contamination of the grown film.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明の構成によれば、MBEにお
ける成長物質を堆積させる基板の支持方法において、イ
ンジウム半田の使用を排除し且つ成長膜の面内均一性を
確保することが出来て、インジウム半田を使用すること
による問題点例えば基板の破損、クロスハツチの発生、
成長膜の汚染などを回避し、良質な成長膜の安定提供を
可能にさせる効果がある。
As explained above, according to the configuration of the present invention, in a method for supporting a substrate on which a growth material is deposited in MBE, it is possible to eliminate the use of indium solder and ensure in-plane uniformity of the grown film, and Problems caused by using solder, such as damage to the board, occurrence of cross hatches,
This has the effect of avoiding contamination of the grown film and making it possible to stably provide a high-quality grown film.

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

第1図は本発明の要旨を示す側断面図、第2図は本発明
の方法の実施例を示す側断面図、第3図は第2図図示実
施例の要部分解斜視図、第4図は第2図図示実施例と従
来方法との比較を示す成長膜例の特性図、 第5図はMBEの要部構成を示す側断面図、第6図は従
来の基板支持方法を示す側断面図、である。 図において、 2は基板支持器、 4は基板支持板・ 5はインジウム半田、 6はヒータ、 7は加熱板、 8は基板支持環、 9は案内環、 10は押えばね、 Gは間隙、 Sは基板、 である。 昇2 z 1p方柾分りとも狛来方2をとぐ比や交ダテ、すが1(
所瞬少・トカオ斗1・±間第47 第5 図 MBE  e+  ’! ’AfP394n−X 7L
  T ’Il’lVh面 間第5図 イ羨来刀系メ反身1多方りI示Tイい・1噌面図亮6 
FIG. 1 is a side sectional view showing the gist of the present invention, FIG. 2 is a side sectional view showing an embodiment of the method of the present invention, FIG. 3 is an exploded perspective view of a main part of the embodiment shown in FIG. Figure 2 is a characteristic diagram of a grown film example showing a comparison between the illustrated embodiment and the conventional method, Figure 5 is a side sectional view showing the main structure of MBE, and Figure 6 is a side view showing the conventional substrate support method. It is a sectional view. In the figure, 2 is a substrate supporter, 4 is a substrate support plate, 5 is indium solder, 6 is a heater, 7 is a heating plate, 8 is a substrate support ring, 9 is a guide ring, 10 is a pressing spring, G is a gap, and S is the substrate, and . Ascendance 2 z 1p direction 1st direction and also Komaraigata 2 toggle ratio and exchange date, Suga 1 (
Shunsho Tokoro Tokaoto 1 ± between 47th Figure 5 MBE e+ '! 'AfP394n-X 7L
T 'Il'lVh side Figure 5 I envy sword type me anti body 1 many directions I show T Ii 1 So side figure 6
figure

Claims (1)

【特許請求の範囲】 1)基板(S)と該基板(S)を加熱するヒータ(6)
との間に、熱伝導率が面方向に大なる熱伝導率異方性を
有する加熱板(7)を該基板(S)に対し間隙(G)を
設けて介在させ、該基板(S)上に成長物質を堆積させ
ることを特徴とする分子線結晶成長方法。 2)上記加熱板(7)の材料は、パイロリテイック・ボ
ロンナイトライドであることを特徴とする特許請求の範
囲第1項記載の分子線結晶成長方法。
[Claims] 1) A substrate (S) and a heater (6) that heats the substrate (S)
A heating plate (7) having a large thermal conductivity anisotropy in the plane direction is interposed between the substrate (S) and the substrate (S) with a gap (G) between the substrate (S) and the substrate (S). A molecular beam crystal growth method characterized by depositing a growth material on top. 2) The molecular beam crystal growth method according to claim 1, wherein the material of the heating plate (7) is pyrolytic boron nitride.
JP17478985A 1985-08-08 1985-08-08 Molecular beam crystal growth method Granted JPS6235514A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17478985A JPS6235514A (en) 1985-08-08 1985-08-08 Molecular beam crystal growth method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17478985A JPS6235514A (en) 1985-08-08 1985-08-08 Molecular beam crystal growth method

Publications (2)

Publication Number Publication Date
JPS6235514A true JPS6235514A (en) 1987-02-16
JPH0319693B2 JPH0319693B2 (en) 1991-03-15

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP17478985A Granted JPS6235514A (en) 1985-08-08 1985-08-08 Molecular beam crystal growth method

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JP (1) JPS6235514A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011526222A (en) * 2008-07-03 2011-10-06 イーオーエス ゲゼルシャフト ミット ベシュレンクテル ハフツング イレクトロ オプティカル システムズ Equipment for manufacturing three-dimensional objects one by one

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5730320A (en) * 1980-07-29 1982-02-18 Fujitsu Ltd Substrate holder for molecular beam epitaxy

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5730320A (en) * 1980-07-29 1982-02-18 Fujitsu Ltd Substrate holder for molecular beam epitaxy

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2011526222A (en) * 2008-07-03 2011-10-06 イーオーエス ゲゼルシャフト ミット ベシュレンクテル ハフツング イレクトロ オプティカル システムズ Equipment for manufacturing three-dimensional objects one by one

Also Published As

Publication number Publication date
JPH0319693B2 (en) 1991-03-15

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