JPH0322410A - Formation of semiconductor thin film - Google Patents
Formation of semiconductor thin filmInfo
- Publication number
- JPH0322410A JPH0322410A JP15789389A JP15789389A JPH0322410A JP H0322410 A JPH0322410 A JP H0322410A JP 15789389 A JP15789389 A JP 15789389A JP 15789389 A JP15789389 A JP 15789389A JP H0322410 A JPH0322410 A JP H0322410A
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- film
- molecular beam
- thin film
- semiconductor thin
- 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
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 14
- 239000010409 thin film Substances 0.000 title claims abstract description 13
- 230000015572 biosynthetic process Effects 0.000 title 1
- 239000000758 substrate Substances 0.000 claims abstract description 38
- 239000010408 film Substances 0.000 claims abstract description 25
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 claims abstract description 22
- 238000000034 method Methods 0.000 claims abstract description 20
- 229910052751 metal Inorganic materials 0.000 claims abstract description 16
- 239000002184 metal Substances 0.000 claims abstract description 16
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims abstract description 14
- 229910052786 argon Inorganic materials 0.000 claims abstract description 11
- RBFQJDQYXXHULB-UHFFFAOYSA-N arsane Chemical compound [AsH3] RBFQJDQYXXHULB-UHFFFAOYSA-N 0.000 claims abstract description 9
- RGGPNXQUMRMPRA-UHFFFAOYSA-N triethylgallium Chemical compound CC[Ga](CC)CC RGGPNXQUMRMPRA-UHFFFAOYSA-N 0.000 claims abstract description 8
- 239000013078 crystal Substances 0.000 claims abstract description 5
- 230000001678 irradiating effect Effects 0.000 claims abstract description 5
- 150000004678 hydrides Chemical class 0.000 claims abstract description 4
- 125000002524 organometallic group Chemical group 0.000 claims description 12
- 238000001451 molecular beam epitaxy Methods 0.000 claims description 3
- 230000003287 optical effect Effects 0.000 abstract description 5
- 239000007789 gas Substances 0.000 abstract description 3
- 238000001741 metal-organic molecular beam epitaxy Methods 0.000 abstract description 3
- 229910052785 arsenic Inorganic materials 0.000 description 5
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 description 5
- 238000005516 engineering process Methods 0.000 description 5
- 238000000197 pyrolysis Methods 0.000 description 4
- 239000002994 raw material Substances 0.000 description 4
- 150000001875 compounds Chemical class 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 238000001459 lithography Methods 0.000 description 3
- 101100215641 Aeromonas salmonicida ash3 gene Proteins 0.000 description 2
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- 229910052733 gallium Inorganic materials 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 238000002488 metal-organic chemical vapour deposition Methods 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- LULLIKNODDLMDQ-UHFFFAOYSA-N arsenic(3+) Chemical compound [As+3] LULLIKNODDLMDQ-UHFFFAOYSA-N 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000012528 membrane Substances 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 239000000178 monomer Substances 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 238000005979 thermal decomposition reaction Methods 0.000 description 1
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は、基板上の任意の場所に組或が制御された化合
物半導体薄膜を形或する方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention relates to a method for forming a compound semiconductor thin film with a controlled structure at any location on a substrate.
(従来の技術)
半導体素子の高度化、高機能化は時代の趨勢である。こ
れにともない、素子の構造はより細かくより複雑となっ
ている。この要求に答えるために従来は、面内に一様な
厚さ・組或の膜を形成したのち、高度なリソグラフ技術
を用いて面内に複雑な凹凸を有する素子構造を作製して
いた。最近、複雑なプロセス行程を簡素化するため、薄
膜形戒時に面内の一部の場所の厚さを制御しようとする
試みがなされている。たとえばアブライドフイジックス
レターズ( Applied Physics Let
ters) 47巻1985年p.95にあるように、
有機金属熱分解法(以下MOCVDと略す)を用いて、
GaAs膜を形成する際に基板にアルゴンレーザを照射
することにより、照射部分にのみ膜形或を行う技術が開
発されている。選択或長ずる理由は原料の有機金属が光
照射によって分解されるからである。光源としてはアル
ゴンレーザばかりでなく低圧水銀ランプ、エキシマレー
ザなどでも効果があることが報告されている。ただし、
エキシマレーザには2つの欠点がある。第一に、レーザ
の波長が有機金属の吸収波長に一致するので、有機金属
は基板上ばかりでなく、雰囲気中でも分解される。第二
に、パルス発振レーザであるためパルスのエネルギが非
常に大きく、レーザ照射にともなう温度上昇が顕著とな
る。このような欠点を有するため光分布どうりのパター
ンは得られていない。(Conventional Technology) Semiconductor devices are becoming more sophisticated and highly functional as a trend of the times. Along with this, the structure of elements has become finer and more complex. In order to meet this demand, in the past, a film with a uniform thickness and composition was formed within the plane, and then an element structure having complex irregularities within the plane was fabricated using advanced lithography technology. Recently, attempts have been made to control the thickness at some locations within the plane of a thin film in order to simplify complex process steps. For example, Applied Physics Letters
ters) Volume 47, 1985, p. As stated in 95,
Using metal organic pyrolysis method (hereinafter abbreviated as MOCVD),
A technique has been developed in which when forming a GaAs film, the substrate is irradiated with an argon laser to form the film only on the irradiated area. The reason for this selection is that the organometallic material is decomposed by light irradiation. It has been reported that not only argon lasers but also low-pressure mercury lamps, excimer lasers, and the like are effective as light sources. however,
Excimer lasers have two drawbacks. First, since the wavelength of the laser matches the absorption wavelength of the organic metal, the organic metal is decomposed not only on the substrate but also in the atmosphere. Second, since it is a pulse oscillation laser, the energy of the pulse is very large, and the temperature rise due to laser irradiation is significant. Due to these drawbacks, a pattern with the same light distribution cannot be obtained.
(発明が解決しようとする課題)
これまでの光照射による選択或長では膜威長法にもっぱ
らMOCVDが用いられてきた。このため細かいパター
ンを形成出来ないという欠点があった。(Problems to be Solved by the Invention) Up to now, MOCVD has been exclusively used for the film length method for selection and length by light irradiation. For this reason, there was a drawback that fine patterns could not be formed.
その原因は、(a) Mocvo,法では数10−76
0 Torrの圧力の水素ガス雰囲気下で膜威長を行う
ため、基板上で有機金属の流れが生じ、その結果、選択
膜の形状がなだらかになる、(b)威長容器つまり反応
管はガラス製の円筒形であるため、微細な光干渉パター
ンを基板に投影出来ないからである。さらに、選択威長
の可否は基板の伝導型にも依存し、n型では可能である
が、半絶縁性基板では選択威長しない。これは、選択或
長をテバイスに応用するときに、おおきな制約となる。The reason is (a) Mocvo, the number 10-76 in the method
Since the film lengthening is performed in a hydrogen gas atmosphere at a pressure of 0 Torr, a flow of organic metal occurs on the substrate, and as a result, the shape of the selective membrane becomes gentle. (b) The lengthening container, that is, the reaction tube is made of glass. This is because the cylindrical shape of the substrate makes it impossible to project a fine optical interference pattern onto the substrate. Furthermore, whether or not selective strength is possible depends on the conductivity type of the substrate; it is possible with n-type substrates, but not with semi-insulating substrates. This is a major constraint when applying selection or length to devices.
(発明の目的)
本発明は上記の欠点を改善するために提案されたもので
、その目的はリソグラフ技術を用いることなく微細なパ
ターンを有する半導体膜を形成できる半導体薄膜形或法
を提供することにある。(Objective of the Invention) The present invention was proposed in order to improve the above-mentioned drawbacks, and its purpose is to provide a semiconductor thin film form or method that can form a semiconductor film having a fine pattern without using lithography technology. It is in.
(課題を゛解決するための手段)
上記の目的を達威するため本発明は真空容器内で有機金
属であるトリエチルガリウム( TEGa )の分子線
とアルシン( ASH3 )を熱分解した水素化物の分
子線を用いて単結晶基板上に半導体薄膜を形成する有機
金属分子線エピタキシ法において、真空容器外からアル
ゴンレーザビームを前記基板上に照射しながら、GaA
s膜威長を行うことを特徴とする半導体薄膜形或法を発
明の要旨とするものである。(Means for Solving the Problems) In order to achieve the above object, the present invention uses molecular beams of triethyl gallium (TEGa), an organic metal, and molecules of hydride obtained by thermally decomposing arsine (ASH3) in a vacuum container. In the organometallic molecular beam epitaxy method, in which a semiconductor thin film is formed on a single crystal substrate using a GaA
The gist of the invention is a semiconductor thin film structure or method that is characterized by performing S film lengthening.
(作 用)
本発明は膜威長法に有機金属分子線法(以後MOMBE
と略す)を用いており、MOMB[!では10−4To
rr以下の真空度で膜威長を行うため、有機金属分子線
は残留ガスに衝突することなく基板に到達し、個々の有
機金属分子は基板表面でほとんど移動しない。またレー
ザビームを導入する窓は平板であるため、微細な光学パ
ターンを変形すること3
なく基板上に投影できる作用を有する。換言すれば、本
発明はMO?IBEに^rレーザを照射させることによ
り、微細パターンの半導体薄膜かえられる特徴を有する
ものである。(Function) The present invention combines the film length method with the organometallic molecular beam method (hereinafter referred to as MOMBE).
) is used, and MOMB[! Then 10-4To
Since film lengthening is performed at a vacuum degree of rr or less, the organometallic molecular beam reaches the substrate without colliding with residual gas, and individual organometallic molecules hardly move on the substrate surface. Furthermore, since the window through which the laser beam is introduced is a flat plate, it has the effect of projecting a minute optical pattern onto the substrate without deforming it. In other words, is the present invention MO? By irradiating an IBE with a ^r laser, a semiconductor thin film with a fine pattern can be changed.
(実施例) 次に本発明の実施例について説明する。(Example) Next, examples of the present invention will be described.
なお実施例は一つの例示であって、本発明の精神を逸脱
しない範囲で、種々の変更あるいは改良を行いうること
は云うまでもない。It should be noted that the embodiments are merely illustrative, and it goes without saying that various changes and improvements can be made without departing from the spirit of the present invention.
第l図は本発明の実施例を説明するための構威図であっ
て、図において、1は真空容器、2はアルシンボンベ、
3と7はマスフローコントローラ(以下MFCと略す)
、4は熱分解セル、5はGaAs基板、6は有機金属ボ
ンベ、8は有機金属用分子線セル、9はアルゴンレーザ
、IOはレンズ、llは窓である。FIG. 1 is a structural diagram for explaining an embodiment of the present invention, and in the figure, 1 is a vacuum container, 2 is an arsine cylinder,
3 and 7 are mass flow controllers (hereinafter abbreviated as MFC)
, 4 is a pyrolysis cell, 5 is a GaAs substrate, 6 is an organometallic cylinder, 8 is an organometallic molecular beam cell, 9 is an argon laser, IO is a lens, and 11 is a window.
(実施例1)
アルゴンレーザを用いてスポット状のGaAslliの
選択或長を行った例を述べる。まず真空容器lを1 0
−” Torrの高真空にひいた。ヒ素原料のハイ4
ドライドガスには100%の濃度のアルシンを用いた。(Example 1) An example in which a spot-shaped GaAslli was selected or lengthened using an argon laser will be described. First, vacuum container l is 1 0
-'' Torr high vacuum. 100% arsine was used as the arsenic raw material Hi-4 dry gas.
ボンベ2からアルシンの流量をMFC3ヲ用いて6cc
/分に設定し、950℃に加熱した熱分解セル4でヒ素
分子線を形成した。熱分解のとき水素が生威されるため
真空容器の真空度は約10−4Torrまで増加した。The flow rate of arsine from cylinder 2 is 6cc using MFC3.
An arsenic molecular beam was formed in the pyrolysis cell 4, which was set at 950°C and heated at 950°C. Since hydrogen was produced during thermal decomposition, the degree of vacuum in the vacuum vessel increased to about 10-4 Torr.
ヒ素分子線を照射しながらGaAs基板5を600℃ま
で加熱して基板表面を清浄化し、ヒ素分子線をあてなが
ら基板温度を425゜Cに降温した。ガリウムの原料の
有機金属にはトリエチルガリウム(以下TEGと略す)
を用い、TEGボンベ6を開けて、その流量を?lFC
7でlcc/分で調整し、有機金属用分子線セル8か
らTEG分子線を基板にむけて照射した。このようにし
てGaAs膜の戒長を開始した。数分後に、アルゴンレ
ーザ9から強度500mWのレーザビームを出射した。The GaAs substrate 5 was heated to 600° C. while being irradiated with an arsenic molecular beam to clean the substrate surface, and the substrate temperature was lowered to 425° C. while being irradiated with an arsenic molecular beam. Triethyl gallium (hereinafter abbreviated as TEG) is an organic metal used as a raw material for gallium.
Open TEG cylinder 6 using , and check the flow rate? lFC
7, and the TEG molecular beam was irradiated toward the substrate from the organometallic molecular beam cell 8. In this way, we began to refine the GaAs film. After several minutes, a laser beam with an intensity of 500 mW was emitted from the argon laser 9.
レーザビームはレンズ10を用いて集束し、窓11を通
してGaAs基板に垂直に照射した。その際、レーザビ
ームの直径が400μmになるように調整した。一時間
後にT[!Gの供給をとめて、GaAs膜の成長を終了
した。これと同時にレーザビ一ムの照射も停止した。こ
のようにして作製した膜のレーザ照射部分にはスポット
状の突起が見られた。The laser beam was focused using a lens 10 and irradiated perpendicularly onto the GaAs substrate through a window 11. At that time, the diameter of the laser beam was adjusted to 400 μm. An hour later T[! The supply of G was stopped, and the growth of the GaAs film was completed. At the same time, the laser beam irradiation also stopped. Spot-like protrusions were observed in the laser irradiated portion of the film thus produced.
第2図はスポットの断面の高さ分布である。レーザの光
強度分布を反映して直径400μmのガウス型分布して
いる。FIG. 2 shows the height distribution of the spot cross section. Reflecting the laser light intensity distribution, there is a Gaussian distribution with a diameter of 400 μm.
図に示すように、スポットの高さはレーザ強度に正比例
して増加する。これは、本方法によるGaAsの威長速
度の増加は光反応であることを意味する。なお、アルゴ
ンレーザ照射による威長速度の増加は、ガリウム原料に
TEG 、ヒ素原料にアルシンのかわりに金属ヒ素を用
いた場合にも、同様にみられた。As shown in the figure, the spot height increases in direct proportion to the laser intensity. This means that the increase in the growth rate of GaAs by this method is a photoreaction. Incidentally, the increase in growth rate due to argon laser irradiation was similarly observed when TEG was used as the gallium raw material and metallic arsenic was used instead of arsine as the arsenic raw material.
第3図(イ)はレーザ照射部分と非照射部分の威長速度
の基板温度依存性を示す。(TI)図は基板上の薄膜の
威長速度を示す。上記の結果からレーザ照射の効果は基
板温度400−550℃範囲が好ましい。この温度依存
性はn型、p型および半絶縁性基板でまったく同一であ
った。FIG. 3(A) shows the substrate temperature dependence of the elongation speed of the laser irradiated part and the non-irradiated part. The (TI) diagram shows the growth rate of the thin film on the substrate. From the above results, the effect of laser irradiation is preferably achieved when the substrate temperature is in the range of 400 to 550°C. This temperature dependence was exactly the same for n-type, p-type, and semi-insulating substrates.
第4図はレーザ電力と選択的威長速度との関係を示す。FIG. 4 shows the relationship between laser power and selective elongation velocity.
この場合のレーザビームの直径は400μmである。The diameter of the laser beam in this case is 400 μm.
(実施例2)
次に縞状のパターンを形成した例について述べる。第5
図に本発明に用いられた装置の構威図を示す。(Example 2) Next, an example in which a striped pattern is formed will be described. Fifth
The figure shows a diagram of the configuration of the device used in the present invention.
図においてlは真空容器、2はアルシンボンベ、3はマ
スフローコントローラ) 、5 ハGaAsaFi、6
は有機金属ボンへ、7はマスフローコントローラ、8は
有機金属用分子線セル、9はアルゴンレーザ、10はレ
ンズ、11は窓、l2はビームエクスパンダ、 l3
はマスクを示す。In the figure, l is a vacuum container, 2 is an arsine cylinder, 3 is a mass flow controller), 5 is GaAsaFi, 6
is an organometallic bomb, 7 is a mass flow controller, 8 is a molecular beam cell for organometallic, 9 is an argon laser, 10 is a lens, 11 is a window, l2 is a beam expander, l3
indicates a mask.
実施例1と同一の手順でGaAs基板を用意し、TEG
を照射してGaAsの膜を作製した。ただし、レーザビ
ームは、レーザビームをいったんビームエクスパンダ1
2を用いて直径5mに拡大し、その後1mmピッチの縞
状に金属が塗布されたガラス板、つまりマスクを通過さ
せることによってレーザビームを回折させ、さらにレン
ズ10を用いて、基板上に回折パターンを集束した。A GaAs substrate was prepared in the same manner as in Example 1, and TEG
A GaAs film was fabricated by irradiating with . However, once the laser beam is transferred to the beam expander 1,
The laser beam is enlarged to a diameter of 5 m using a lens 10, and then is diffracted by passing through a glass plate coated with metal in stripes with a pitch of 1 mm, that is, a mask, and then a diffraction pattern is formed on the substrate using a lens 10. focused.
7
第6図(イ)図はレーザ照射部分の膜の断面形状で、幅
90μmの線が7本みられる。この形状は、([I)図
にしめした光強度分布とよく一致していた。7 Figure 6(a) shows the cross-sectional shape of the film in the laser irradiated area, and seven lines with a width of 90 μm can be seen. This shape matched well with the light intensity distribution shown in Figure ([I).
したがって、所望のパターンを種々の光学機器を用いて
形成すれば、そのとうりのパターンを持つ膜を形或でき
る。実際、ホログラフ技術を用いて微細パターン形成し
た結果、4もクロンピッチの縞を持つ膜を得ることがで
きた。Therefore, by forming a desired pattern using various optical devices, a film having the desired pattern can be formed. In fact, as a result of forming a fine pattern using holographic technology, we were able to obtain a film with stripes of 4 chron pitch.
(発明の効果)
以上説明したように、本発明によれば真空容器内で有機
金属であるトリエチルガリウム( TEGa )の分子
線とアルシン( ASH3 )を熱分解した水素化物の
分子線を用いて単結晶基板上に半導体薄膜を形或する有
機金属分子線エピタキシ法において、真空容器外からア
ルゴンレーザビームを前記基板上に照射しながら、Ga
As膜威長を行うことにより、基板上に所望な場所に複
雑な凹凸有するパターンを、リソグラフ技術を用いるこ
となく、形成できる。光・電子集積回路( OEIC
)は、将来のキーデバイスとして期待されているが、こ
れを作製す8
るには、膜威長・プロセスを数回繰り返す必要がある。(Effects of the Invention) As explained above, according to the present invention, a monomer is produced using a molecular beam of triethyl gallium (TEGa), which is an organic metal, and a molecular beam of a hydride obtained by thermally decomposing arsine (ASH3) in a vacuum container. In the organometallic molecular beam epitaxy method for forming a semiconductor thin film on a crystal substrate, Ga is
By performing As film lengthening, a pattern having complex irregularities at desired locations on the substrate can be formed without using lithography technology. Optical/electronic integrated circuit (OEIC)
) is expected to be a key device in the future, but to fabricate it, it is necessary to repeat the film lengthening process several times.
再或長の界面には多くの結晶欠陥が発生し、素子の性能
低下の最大の原因となっている。本発明方法をOEIC
に応用すれば、工程が大幅に削減できるばかりでなく、
界面に欠陥を発生することもないため、素子の性能向上
・信頼性向上におおいに役立つ。Many crystal defects occur at the re-elongated interface, which is the biggest cause of deterioration in device performance. The method of the present invention is OEIC
If applied to
Since no defects are generated at the interface, it is extremely useful for improving the performance and reliability of devices.
なお実施例では、GaAsの作製例をしめしたが、In
P , GaP 、などの2元系化合物で選択威長を確
認している。これらの結果から3元、4元化合物の選沢
威長が可能であることは容易に予想される。In the example, an example of manufacturing GaAs was shown, but In
Selective strength has been confirmed in binary compounds such as P and GaP. From these results, it is easily predicted that it is possible to select ternary and quaternary compounds.
第1図は本発明に用いられる装置、第2図はスポットの
断面の高さ分布、第3図(イ)はレーザ照射部分と非照
射部分の威長速度と基板温度との関係、([I)は基板
上の薄膜の成長速度、第4図はレーザ電力と選択的威長
速庫との関係、第5図は本発明の第2実施例に用いる装
置、第6図(イ)はレーザ照射部分の膜の断面形状、(
El)は光強度分布を示す。
1・・・真空容器、2・・・アルシンボンベ、3,7・
・・マスフロコントローラ、4・・・熱分解セル、5・
・・GaAs基板、6・・・有機金属ボンベ、8・・・
有機金属用ボンベ、9・・・アルゴンレーザ、10・・
・レンズ、11・・・窓、l2・・・ビームエクスパン
ダ、13・・・マスク。Fig. 1 shows the apparatus used in the present invention, Fig. 2 shows the height distribution of the cross section of the spot, and Fig. 3 (a) shows the relationship between the elongation velocity of the laser irradiated part and the non-irradiated part and the substrate temperature, ([ I) is the growth rate of the thin film on the substrate, FIG. 4 is the relationship between laser power and selective growth rate, FIG. 5 is the apparatus used in the second embodiment of the present invention, and FIG. Cross-sectional shape of the film in the laser irradiated area, (
El) indicates the light intensity distribution. 1...Vacuum container, 2...Arsine cylinder, 3,7.
... Mass flow controller, 4... Pyrolysis cell, 5.
...GaAs substrate, 6...Organic metal cylinder, 8...
Organic metal cylinder, 9... Argon laser, 10...
・Lens, 11...Window, l2...Beam expander, 13...Mask.
Claims (1)
Ga)の分子線とアルシン(AsH_3)を熱分解した
水素化物の分子線を用いて単結晶基板上に半導体薄膜を
形成する有機金属分子線エピタキシ法において、真空容
器外からアルゴンレーザビームを前記基板上に照射しな
がら、GaAs膜成長を行うことを特徴とする半導体薄
膜形成法。Triethylgallium (TE), an organic metal, is
In the organometallic molecular beam epitaxy method, which forms a semiconductor thin film on a single crystal substrate using a molecular beam of Ga) and a molecular beam of hydride obtained by thermally decomposing arsine (AsH_3), an argon laser beam is applied to the substrate from outside the vacuum chamber. A semiconductor thin film forming method characterized by growing a GaAs film while irradiating the top.
Priority Applications (5)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15789389A JPH0322410A (en) | 1989-06-19 | 1989-06-19 | Formation of semiconductor thin film |
PCT/JP1989/000827 WO1990001794A1 (en) | 1988-08-15 | 1989-08-15 | Method of forming a semiconductor thin film and apparatus therefor |
US07/477,870 US5186750A (en) | 1988-08-15 | 1989-08-15 | Method and apparatus for forming semiconductor thin films |
EP89909240A EP0394462B1 (en) | 1988-08-15 | 1989-08-15 | Method of forming a semiconductor thin film and apparatus therefor |
US07/935,067 US5273932A (en) | 1988-08-15 | 1992-08-25 | Method for forming semiconductor thin films where an argon laser is used to suppress crystal growth |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15789389A JPH0322410A (en) | 1989-06-19 | 1989-06-19 | Formation of semiconductor thin film |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0322410A true JPH0322410A (en) | 1991-01-30 |
Family
ID=15659722
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15789389A Pending JPH0322410A (en) | 1988-08-15 | 1989-06-19 | Formation of semiconductor thin film |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0322410A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06236849A (en) * | 1993-02-10 | 1994-08-23 | Hikari Gijutsu Kenkyu Kaihatsu Kk | Growth method of compound semiconductor crystal |
WO2001023648A1 (en) * | 1999-09-30 | 2001-04-05 | Prowtech Inc. | Apparatus and method for forming single crystalline nitride substrate using hydride vapor phase epitaxy and laser beam |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59111322A (en) * | 1982-12-16 | 1984-06-27 | Agency Of Ind Science & Technol | Manufacture of thin-film |
JPS59148325A (en) * | 1983-02-14 | 1984-08-25 | Sanyo Electric Co Ltd | Method and device for growing single crystal thin film of compound semiconductor |
-
1989
- 1989-06-19 JP JP15789389A patent/JPH0322410A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS59111322A (en) * | 1982-12-16 | 1984-06-27 | Agency Of Ind Science & Technol | Manufacture of thin-film |
JPS59148325A (en) * | 1983-02-14 | 1984-08-25 | Sanyo Electric Co Ltd | Method and device for growing single crystal thin film of compound semiconductor |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH06236849A (en) * | 1993-02-10 | 1994-08-23 | Hikari Gijutsu Kenkyu Kaihatsu Kk | Growth method of compound semiconductor crystal |
WO2001023648A1 (en) * | 1999-09-30 | 2001-04-05 | Prowtech Inc. | Apparatus and method for forming single crystalline nitride substrate using hydride vapor phase epitaxy and laser beam |
US6750121B1 (en) | 1999-09-30 | 2004-06-15 | Protech Inc. | Apparatus and method for forming single crystalline nitride substrate using hydride vapor phase epitaxy and laser beam |
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