JPH03142921A - Manufacturing device for iii-v compound semiconductor thin film - Google Patents

Manufacturing device for iii-v compound semiconductor thin film

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Publication number
JPH03142921A
JPH03142921A JP28240289A JP28240289A JPH03142921A JP H03142921 A JPH03142921 A JP H03142921A JP 28240289 A JP28240289 A JP 28240289A JP 28240289 A JP28240289 A JP 28240289A JP H03142921 A JPH03142921 A JP H03142921A
Authority
JP
Japan
Prior art keywords
target
compound semiconductor
thin film
chamber
iii
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
JP28240289A
Other languages
Japanese (ja)
Inventor
Tamio Yoshida
吉田 多見男
Yutaka Ido
豊 井戸
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP28240289A priority Critical patent/JPH03142921A/en
Publication of JPH03142921A publication Critical patent/JPH03142921A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To make it possible to obtain a high-quality crystal by a method wherein when a III-V compound semiconductor is manufactured by an MBE method, a molecular beam consisting of the element of As or P or a molecular beam consisting of the elements of both of the As and the P is formed by a laser sputtering method. CONSTITUTION:A supporting body (a target holder) 5 for supporting a solid target 4 consisting of at least either one of As or P is provided in a vacuum chamber (a growth chamber) 1 and a laser (a pulsed laser) 6, which irradiates a pulse laser beam on the target 4 on the body 5 through a window 1a, is arranged outside of the chamber 1. The target 4 is sputtered by the irradiation of this laser beam and a molecular beam or an atomic beam consisting of the element of at least either one of the As or the P is formed. That is, when a short pulsed laser beam having a large pulse energy is condensed and irradiated on the metal material, its irradiation part is heated locally and abruptly to a very high temperature and most of evaporation particles which are produced from the metal material are formed into an atomic form. Thereby, a high-quality III-V compound semiconductor thin film can be obtained.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明はAs(ヒ素)やP(リン)を含む化合物半導体
の薄膜を製造する装置に関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to an apparatus for manufacturing a thin film of a compound semiconductor containing As (arsenic) and P (phosphorus).

〈従来の技術〉 化合物半導体の薄膜の製作方法の代表的なものとして、
MBE(分子線エピタキシー)法がある。
<Conventional technology> As a typical method for manufacturing thin films of compound semiconductors,
There is an MBE (molecular beam epitaxy) method.

従来のMBE法においては、K−セル(クヌードセンセ
ル)と呼ばれるるつぼに金属材料を収容し、これを加熱
して分子線を得ている。
In the conventional MBE method, a metal material is placed in a crucible called a K-cell (Knudsen cell) and heated to obtain a molecular beam.

このようなMBE法を用いて■−V族化合物半導体の薄
膜を製作する場合、AsやPの分子線が必要となるが、
金属AsやPを加熱すると、生成される分子線は4原子
分子(Asa、P4)の形となる。
When manufacturing a thin film of ■-V group compound semiconductor using such MBE method, molecular beams of As and P are required.
When metal As or P is heated, the generated molecular beam has the form of a four-atom molecule (Asa, P4).

ところが、このような4原子分子を堆積させるより、2
原子分子線を用いた方が基板への付着確率が高く、結晶
性の良い高品質の膜が作成されることが明らかとなって
いる。
However, rather than depositing such four-atom molecules, two
It has been shown that the use of atomic and molecular beams has a higher probability of adhesion to the substrate and produces high-quality films with good crystallinity.

そこで従来、通常のに一セルからの分子線を更に高温部
を通過させて分解することによって、2原子分子を生成
する方法が採られている。実際には、2つの加熱部を有
するクランキングセルと称されるセルを用いて、一つの
加熱部で生成された4原子分子線をもう一つの加熱部を
通過させることによって2原子分子線を得ている。
Conventionally, therefore, a method has been adopted in which a molecular beam from a normal cell is further passed through a high-temperature section and decomposed, thereby generating diatomic molecules. In reality, a cell called a cranking cell that has two heating sections is used to generate a diatomic molecular beam by passing a four-atom molecular beam generated in one heating section through the other heating section. It has gained.

また、最近では、金属材料の代わりにガスソース(As
HsやPH,)を用い、それらを加熱分解してAs原子
やP原子を得ることも試みられている。
Recently, gas sources (As
Attempts have also been made to obtain As atoms and P atoms by thermally decomposing them using Hs, PH, ).

〈発明が解決しようとする課題〉 以上のような従来のMBE法によって■−V族化合物半
導体の薄膜を製造するとき、通常のに一セルを用いた場
合には、前記したように4原子分子が生成され、良質な
膜を得ることができず、欠陥の多い膜となってしまう。
<Problems to be Solved by the Invention> When manufacturing a thin film of ■-V group compound semiconductor by the conventional MBE method as described above, when a normal cell is used, four-atom molecules are produced as described above. is generated, making it impossible to obtain a high-quality film and resulting in a film with many defects.

また、成長室中に高温部がある関係上、ガス放出量が増
大し、成長室内の超高真空の維持が困難となり、不純物
による汚染の可能性がある。
Furthermore, since there is a high temperature part in the growth chamber, the amount of gas released increases, making it difficult to maintain an ultra-high vacuum in the growth chamber, and there is a possibility of contamination with impurities.

クランキングセルを用いた場合には、K−セルを用いた
場合に比して加熱高温部が増すため、超高真空の維持の
困難性や不純物による汚染の可能性の問題がより顕著と
なる。また、セルの構造が複雑になり、装置トラブルの
原因になりやすいという問題もある。
When using a cranking cell, the number of heated high-temperature parts increases compared to when using a K-cell, so problems such as the difficulty of maintaining an ultra-high vacuum and the possibility of contamination by impurities become more prominent. . Another problem is that the structure of the cell becomes complicated, which tends to cause equipment trouble.

更に、ガスソースを用いた場合には、有毒ガスに対する
危険性があり、その対策が問題となる。
Furthermore, when a gas source is used, there is a risk of toxic gas, and countermeasures against this pose a problem.

本発明の目的は、固体材料を用いて高品質の■−V族化
合物半導体の薄膜を得ることができ、しかも、成長室内
の超高真空の維持の困難性や不純物による汚染の可能性
がきわめて少ない薄膜製造装置を提供することにある。
The object of the present invention is to be able to obtain a thin film of a high-quality ■-V group compound semiconductor using a solid material, and to avoid the difficulty of maintaining an ultra-high vacuum in the growth chamber and the extremely high possibility of contamination by impurities. The object of the present invention is to provide a thin film manufacturing apparatus with a small number of devices.

く課題を解決するための手段〉 上記の目的を達成するための構成を、実施例に対応する
第1図を参照しつつ説明すると、本発明では、薄膜を成
長させるべき真空チャンバ(成長室)を内にAsおよび
Pの少なくともいずれか一方の固体ターゲット4を支持
するための支持体(ターゲットホルダ)5を設けるとと
もに、チャンバ1の外部には、このチャンバ1に形成さ
れた窓1aを介して支持体5上の固体ターゲット4にパ
ルス状のレーザ光を照射するレーザ装置6を配設してい
る。そして、このレーザ光の照射によって固体ターゲッ
ト4をスパッタし、AsおよびPの少なくともいずれか
一方の元素の分子線もしくは原子線を生成するよう構成
している。
Means for Solving the Problems> The configuration for achieving the above objects will be explained with reference to FIG. 1 corresponding to the embodiment. In the present invention, a vacuum chamber (growth chamber) in which a thin film is to be grown A support (target holder) 5 for supporting a solid target 4 of at least one of As and P is provided inside the chamber 1, and a support body (target holder) 5 is provided outside the chamber 1 through a window 1a formed in the chamber 1. A laser device 6 is provided to irradiate a solid target 4 on a support 5 with pulsed laser light. The solid target 4 is sputtered by irradiation with this laser light, and a molecular beam or atomic beam of at least one of As and P is generated.

く作用〉 パルスエネルギの大きな短パルスレーザ光を金属材料に
集光照射すると、その照射部は局部的に急激に非常に高
温にまで加熱され、その金属材料から生成される蒸発(
スパッタ)粒子は大半が原子状となる。
When a metal material is focused and irradiated with short-pulse laser light with high pulse energy, the irradiated area is rapidly locally heated to a very high temperature, causing evaporation (
Most of the sputtered particles are atomic.

ここで、加熱部分は原材料上の局部であって、チャンバ
1内には定常的な加熱部を必要としないので、不純物の
生成が少なく、初期の目的を達成できる。
Here, the heated part is a local part on the raw material, and there is no need for a constant heating part in the chamber 1, so that less impurities are generated and the initial purpose can be achieved.

〈実施例〉 第1図は本発明実施例の構成国である。<Example> FIG. 1 shows the constituent countries of the embodiment of the present invention.

成長室1は真空ポンプ(図示せず)に連通し、超高真空
を維持することのできるチャンバであって、その内部に
は、加熱機能を持ち回転が与えられる基板ホルダ2と、
K−セル3およびシャッタ3a、更に固体ターゲット4
を支持するターゲットホルダ5が配設されている。
The growth chamber 1 is a chamber that is connected to a vacuum pump (not shown) and is capable of maintaining an ultra-high vacuum, and inside thereof is a substrate holder 2 that has a heating function and is rotated.
K-cell 3 and shutter 3a, as well as solid target 4
A target holder 5 is provided to support the target.

このターゲットホルダ5は回動自在の軸の一端において
成長室1内でターゲット4を支持し、かつ、その軸の他
端は成長室1外に伸びて回転駆動機構(図示せず)に接
続されており、ターゲット4を支持した状態で回転が与
えられる。
This target holder 5 supports the target 4 within the growth chamber 1 at one end of a rotatable shaft, and the other end of the shaft extends outside the growth chamber 1 and is connected to a rotation drive mechanism (not shown). The target 4 is rotated while being supported.

成長室1の壁体の一部には透光性の窓1aが装着されて
おり、その外部にはパルスレーザ装置6とレーザ光集光
用レンズ7が配設されている。
A light-transmitting window 1a is attached to a part of the wall of the growth chamber 1, and a pulse laser device 6 and a laser beam condensing lens 7 are disposed outside the window 1a.

レーザ光集光用レンズ7を経たパルスレーザ装置6から
のパルスレーザ光は、窓1aを介してターゲットホルダ
5に支持されたターゲット4上に集光される。
The pulsed laser beam from the pulsed laser device 6 passes through the laser beam focusing lens 7 and is focused onto the target 4 supported by the target holder 5 through the window 1a.

以上の本発明実施例を用いて、GaAs薄膜を作製する
場合、Gaについては従来のMBE装置と同様にに一セ
ル3内に収容して加熱することによって分子線を得ると
ともに、Asについては、金属Asをターゲット4とし
てターゲットホルダ5に装着し、これに回転を与えなが
らその表面にパルスレーザ装置6からのパルスレーザ光
を集光照射する。これによって金属Asはその照射部に
おいて局部的に急激に(数Ions程度)非常に高温に
加熱され、スパッタされる。このパルスレーザスパッタ
によって生成される粒子は、その大半が原子状となり、
残りの殆ども2原子分子となって、4原子分子は殆ど生
成されない。
When producing a GaAs thin film using the above-described embodiment of the present invention, Ga is housed in one cell 3 and heated to obtain a molecular beam as in the conventional MBE apparatus, and as for As, a molecular beam is obtained. A metal As is mounted on a target holder 5 as a target 4, and a pulsed laser beam from a pulsed laser device 6 is condensed and irradiated onto its surface while giving rotation to the target. As a result, the metal As is locally and rapidly heated to a very high temperature (of the order of several ions) in the irradiated area, and is sputtered. Most of the particles generated by this pulsed laser sputtering are atomic,
Most of the remaining molecules become diatomic molecules, and almost no tetraatomic molecules are produced.

第2図は金属A3にパルスレーザ光を照射することによ
ってスパッタされる生成物の質量分析を行った結果を示
すグラフである。この例はエキシマレーザ光をレンズを
介して金属Asの表面に集光照射したもので、Asはそ
の大半が原子状にまで分解されることが立証された。
FIG. 2 is a graph showing the results of mass spectrometry of a product sputtered by irradiating metal A3 with pulsed laser light. In this example, excimer laser light was focused and irradiated onto the surface of metal As through a lens, and it was proven that most of As was decomposed into atoms.

以上のことから、基板ホルダ2上の基板Sの表面にはレ
ーザスパッタによって生成された原子状のものをを主体
とするAsの分子線が導かれることになり、高品質のG
 a A s結晶が生成される。
From the above, the As molecular beam, which is mainly composed of atoms generated by laser sputtering, is guided to the surface of the substrate S on the substrate holder 2, and high-quality G
a As crystals are produced.

なお、レーザ光の照射によってターゲット4から放出さ
れる分子線(蒸発物)の方向は、はぼターゲットの垂線
方向となるので、この点を留意してターゲット4の位置
ないし姿勢を決定することが好ましい。
Note that the direction of the molecular beam (evaporated material) emitted from the target 4 by laser beam irradiation is the perpendicular direction of the target, so the position or attitude of the target 4 should be determined with this in mind. preferable.

また、パルスレーザ装置6としては、パルスエネルギが
大きく、パルス幅の短い光が得られるものが望ましく、
例えばパルスCO!レーザやYAGレーザ、あるいはエ
キシマレーザが適している。
Further, as the pulse laser device 6, it is desirable that the pulse laser device 6 has a large pulse energy and can obtain light with a short pulse width.
For example, Pulse CO! A laser, YAG laser, or excimer laser is suitable.

特に、エキシマレーザからは光子エネルギの大きな紫外
光が得られるため、熱効果以外に光化学効果による分解
も期待できるため、最も適していると思われる。
In particular, excimer lasers are thought to be the most suitable because they can provide ultraviolet light with high photon energy and can be expected to cause decomposition due to photochemical effects in addition to thermal effects.

更に、以上の実施例の構成に加えて、ターゲット4の前
にイオン選択器を配設することにより、ターゲット4か
らのスパッタ粒子のうち、所望の粒子のみを基板2に導
くように構成することができる。
Furthermore, in addition to the configuration of the above embodiment, an ion selector may be provided in front of the target 4 to guide only desired particles from the sputtered particles from the target 4 to the substrate 2. Can be done.

第3図はその例を示す図で、金属Asターゲット4の前
に偏向板10からなるイオン選択器を設け、その偏向板
10への印加電圧■の調節によって、例えばAs、”イ
オンのみを、あるいはA s z ”イオンのみを選択
して基板2に導くように構成している。
FIG. 3 shows an example of this, in which an ion selector consisting of a deflection plate 10 is provided in front of the metal As target 4, and by adjusting the voltage applied to the deflection plate 10, for example, only As ions can be removed. Alternatively, the configuration is such that only A s z '' ions are selected and guided to the substrate 2 .

この第3図の構成では、A s H”とA S g ”
がレーザ光によるスパッタ直後の速度が同じである場合
、つまり初期エネルギが異なる場合に有効であって、両
者の質量の違いによる偏向方向の相違を利用しているが
、スパッタ直後のエネルギが同じ(初速塵が異なる)場
合には、いわゆる磁場型の質量分離器を用いればよい。
In the configuration shown in FIG. 3, A s H” and A S g ”
is effective when the speed immediately after sputtering by the laser beam is the same, that is, when the initial energy is different, and it takes advantage of the difference in the deflection direction due to the difference in mass of the two, but when the energy immediately after sputtering is the same ( If the initial velocity of the dust is different, a so-called magnetic field type mass separator may be used.

このようなイオン選択器を設けることにより、より良好
な結晶が得られる粒子のみを選択的に基板Sに導くこと
が可能となり、より高品質の薄膜を製作することができ
る。
By providing such an ion selector, it becomes possible to selectively guide only particles from which better crystals can be obtained to the substrate S, and a thin film of higher quality can be manufactured.

また、以上のことはPについても同様であって、Pの固
体ターゲットにパルスレーザ光を集光照射することによ
って、生成される粒子は大半が原子状にまで分解され、
■族元素の分子線との組合せによって良好な結晶の■−
V族半導体薄膜が生成される。
The above also applies to P, and by irradiating a P solid target with focused pulsed laser light, most of the particles generated are decomposed into atomic particles.
■-
A Group V semiconductor thin film is produced.

このことから、AsとPの合金をターゲット4として用
い、かつ、第3図のようなイオン選択器を設けることに
よって、基板にAsl’もしくはPl゛を選択的に導く
ことも可能となる。
Therefore, by using an alloy of As and P as the target 4 and providing an ion selector as shown in FIG. 3, it becomes possible to selectively introduce Asl' or Pl' to the substrate.

また、■族元素の分子線については、特にレーザスパッ
タを用いるが故の薄膜の品質に及ぼす効果はないが、こ
れらについてもレーザスパッタ法を用い得ることは勿論
で、成長室内から定常的な熱源を廃して不純物の生成を
少なくするという点での効果は期待できる。
Regarding molecular beams of group Ⅰ elements, there is no effect on the quality of the thin film because laser sputtering is used, but it goes without saying that laser sputtering can be used for these as well, and a steady heat source from within the growth chamber can be used. The effect can be expected in terms of eliminating impurities and reducing the production of impurities.

更に、ターゲットに照射するレーザ光としてはパルスレ
ーザ光が好ましいが、パルスレーザ装置に変えて通常の
レーザ装置を用い、その出力光をチッッピングすること
によっても同様な効果が期待できる。
Furthermore, although pulsed laser light is preferable as the laser light irradiated to the target, similar effects can be expected by using a normal laser device instead of the pulsed laser device and chipping the output light.

更にまた、ターゲット4へのレーザ光照射と同時に、基
板Sへのレーザ光照射を行えば、マイグレーシゴンが促
進され、より高品質の結晶が低温で作製できるようにな
る。
Furthermore, if the substrate S is irradiated with laser light at the same time as the target 4 is irradiated with laser light, migration is promoted and higher quality crystals can be produced at lower temperatures.

また、ターゲットホルダ5は必ずしも回転可能とする必
要はなく、照射レーザ光側を適宜に動かしてターゲット
側を固定してもよいことは言うまでもない。
Further, it goes without saying that the target holder 5 does not necessarily need to be rotatable, and the irradiated laser beam side may be moved as appropriate and the target side may be fixed.

〈発明の効果〉 以上説明したように、本発明によれば、■−■族化合物
半導体をMBE法によって製造する際に、AsまたはP
もしくはその両方の分子線についてはレーザスパック法
で生成するので、原子種を生成でき、従来のに一セルな
いしはグラフキングセルを使用する場合に比して高品質
の結晶が得られる。
<Effects of the Invention> As explained above, according to the present invention, when producing a ■-■ group compound semiconductor by the MBE method, As or P
Or both of the molecular beams are generated by the laser spacing method, so atomic species can be generated, and higher quality crystals can be obtained than in the case of using a conventional Niichi cell or graphing cell.

また、成長室内から定常的な加熱部を削減することがで
き、超高真空を得るのが容易となり、不純物の影響を低
減できる。同時に、励起源が成長室外にあるため、蒸発
源に関するトラブルが少なくなり、装置の稼働率の向上
が期待できる。
Further, it is possible to eliminate the need for a constant heating section in the growth chamber, making it easier to obtain an ultra-high vacuum, and reducing the influence of impurities. At the same time, since the excitation source is located outside the growth chamber, troubles related to the evaporation source are reduced, and an improvement in the operating rate of the apparatus can be expected.

更に、パルスレーザ光のパルス数の制御によって、分子
線量の制御が可能となるため、通常のに−セルを用いた
場合に必要となるセル直前のシャッタ機構が不要となる
とともに、パルス数の制御は正確かつ容易であるため、
分子線量の制御性が向上し、膜厚や組成の制御性が向上
するという利点もある。
Furthermore, the molecular dose can be controlled by controlling the number of pulses of the pulsed laser beam, which eliminates the need for a shutter mechanism just before the cell that is required when using a normal cell, and also makes it possible to control the number of pulses. is accurate and easy, so
There is also the advantage that the controllability of the molecular dose is improved, and the controllability of the film thickness and composition is also improved.

更にまた、ターゲットの前にイオン選択器を設けた場合
には、分子線種の選択が可能となってより高品質の結晶
が得られるとともに、膜形成に及ぼす分子線種の影響を
容易に検討できるという効果もある。
Furthermore, if an ion selector is installed in front of the target, it becomes possible to select the molecular beam type, obtain higher quality crystals, and easily examine the effect of the molecular beam type on film formation. There is also the effect that it can be done.

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

第1図は本発明実施例の成長室近傍の構成図、第2図は
パルスレーザスパッタによって生成される粒子の質量分
析結果を示すグラフ、第3図は本発明の他の実施例の要
部構成図である。 1・・・・成長室 1a・・・・窓 2・・・・基板ホルダ 3・・・・K−セル 3a・・・・シャック 4・・・・ターゲット 5・・・・ターゲットホルダ 6°・・・・パルスレーザ装置 7・・・・レーザ光集光用レンズ 10・・・・偏向板 S・・・・基板
Fig. 1 is a diagram showing the configuration of the vicinity of the growth chamber in an embodiment of the present invention, Fig. 2 is a graph showing the mass spectrometry results of particles generated by pulsed laser sputtering, and Fig. 3 is a main part of another embodiment of the present invention. FIG. 1...Growth chamber 1a...Window 2...Substrate holder 3...K-cell 3a...Shack 4...Target 5...Target holder 6° ... Pulse laser device 7 ... Laser beam focusing lens 10 ... Deflection plate S ... Substrate

Claims (1)

【特許請求の範囲】[Claims]  真空チャンバ内に置かれた基板表面に、III族元素の
分子線と、AsおよびPの少なくともいずれか一方の分
子線を照射することによって、基板表面にIII−V族化
合物半導体の薄膜を成長させる装置において、上記チャ
ンバ内にAsおよびPの少なくともいずれか一方の固体
ターゲットを支持するための支持体を設けるとともに、
上記チャンバの外部には、このチャンバに形成された窓
を介して上記支持体上のターゲットにパルス状のレーザ
光を照射するレーザ装置を配設し、そのレーザ光の照射
によって上記固体ターゲットをスパッタしてAsおよび
Pの少なくともいずれか一方の元素の分子線もしくは原
子線を生成するよう構成したことを特徴とするIII−V
族化合物半導体薄膜製造装置。
A thin film of a III-V compound semiconductor is grown on the substrate surface by irradiating the surface of the substrate placed in a vacuum chamber with a molecular beam of a group III element and a molecular beam of at least one of As and P. In the apparatus, a support for supporting a solid target of at least one of As and P is provided in the chamber, and
A laser device is installed outside the chamber to irradiate the target on the support with pulsed laser light through a window formed in the chamber, and the solid target is sputtered by irradiation with the laser light. III-V characterized in that it is configured to generate a molecular beam or atomic beam of at least one of As and P.
Group compound semiconductor thin film manufacturing equipment.
JP28240289A 1989-10-30 1989-10-30 Manufacturing device for iii-v compound semiconductor thin film Pending JPH03142921A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28240289A JPH03142921A (en) 1989-10-30 1989-10-30 Manufacturing device for iii-v compound semiconductor thin film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28240289A JPH03142921A (en) 1989-10-30 1989-10-30 Manufacturing device for iii-v compound semiconductor thin film

Publications (1)

Publication Number Publication Date
JPH03142921A true JPH03142921A (en) 1991-06-18

Family

ID=17651944

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28240289A Pending JPH03142921A (en) 1989-10-30 1989-10-30 Manufacturing device for iii-v compound semiconductor thin film

Country Status (1)

Country Link
JP (1) JPH03142921A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100384892B1 (en) * 2000-12-01 2003-05-22 한국전자통신연구원 Fabrication method of erbium-doped silicon nano-dots
KR100450749B1 (en) * 2001-12-28 2004-10-01 한국전자통신연구원 Method of manufacturing er-doped silicon nano-dot array and laser ablation apparatus used therein
KR100459880B1 (en) * 1998-05-07 2005-01-15 삼성전기주식회사 Target fixture for apparatus of manufacturing pulsed laser depositon
WO2013071484A1 (en) * 2011-11-15 2013-05-23 中国科学院物理研究所 Film deposition device and film deposition method

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6122618A (en) * 1984-07-10 1986-01-31 Mitsubishi Electric Corp Vapor-phase epitaxial crystal growing device
JPS61146790A (en) * 1984-12-18 1986-07-04 Agency Of Ind Science & Technol Molecular beam epitaxial growth method
JPS6255920A (en) * 1985-09-05 1987-03-11 Nec Corp Molecular beam evaporation source
JPS6272113A (en) * 1985-09-26 1987-04-02 Matsushita Electric Ind Co Ltd Molecular beam crystal growth equipment

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6122618A (en) * 1984-07-10 1986-01-31 Mitsubishi Electric Corp Vapor-phase epitaxial crystal growing device
JPS61146790A (en) * 1984-12-18 1986-07-04 Agency Of Ind Science & Technol Molecular beam epitaxial growth method
JPS6255920A (en) * 1985-09-05 1987-03-11 Nec Corp Molecular beam evaporation source
JPS6272113A (en) * 1985-09-26 1987-04-02 Matsushita Electric Ind Co Ltd Molecular beam crystal growth equipment

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100459880B1 (en) * 1998-05-07 2005-01-15 삼성전기주식회사 Target fixture for apparatus of manufacturing pulsed laser depositon
KR100384892B1 (en) * 2000-12-01 2003-05-22 한국전자통신연구원 Fabrication method of erbium-doped silicon nano-dots
KR100450749B1 (en) * 2001-12-28 2004-10-01 한국전자통신연구원 Method of manufacturing er-doped silicon nano-dot array and laser ablation apparatus used therein
WO2013071484A1 (en) * 2011-11-15 2013-05-23 中国科学院物理研究所 Film deposition device and film deposition method

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