JPS6232607A - Growth and analysis instrument - Google Patents
Growth and analysis instrumentInfo
- Publication number
- JPS6232607A JPS6232607A JP17211485A JP17211485A JPS6232607A JP S6232607 A JPS6232607 A JP S6232607A JP 17211485 A JP17211485 A JP 17211485A JP 17211485 A JP17211485 A JP 17211485A JP S6232607 A JPS6232607 A JP S6232607A
- Authority
- JP
- Japan
- Prior art keywords
- window
- growth
- laser beam
- laser
- radiation
- 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
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- Physical Deposition Of Substances That Are Components Of Semiconductor Devices (AREA)
- Crystals, And After-Treatments Of Crystals (AREA)
- Testing Or Measuring Of Semiconductors Or The Like (AREA)
Abstract
Description
【発明の詳細な説明】
〔概要〕
真空室を共有する成長・分析装置の分析用の放射線を導
入する放射窓が成長物質の付着により汚染されて曇るた
め、清浄化する必要がある。そのためレーザビームによ
る加熱で汚染を除去できる機構を具備する装置を提案す
る。[Detailed Description of the Invention] [Summary] The radiation window through which radiation for analysis is introduced in the growth/analysis apparatus that shares a vacuum chamber becomes contaminated and cloudy due to adhesion of growth substances, and therefore needs to be cleaned. Therefore, we propose an apparatus equipped with a mechanism that can remove contamination by heating with a laser beam.
r産業上の利用分野〕 浄化する機構を備えた成長・分析装置に関する。r Industrial application field] This invention relates to a growth/analysis device equipped with a purification mechanism.
従来は上記放射窓は成長物質が付着して、放射線の透過
率を減衰させるため、成長と分析をそれぞれ別々の真空
室で行い、即時分析ができなかった。そのため、成長中
に同時に分析ができる装置が要望されている。Conventionally, growth substances adhered to the radiation window and attenuated the radiation transmittance, so growth and analysis were performed in separate vacuum chambers, making immediate analysis impossible. Therefore, there is a need for an apparatus that can perform analysis simultaneously during growth.
第2図は従来の成長・分析装置の構成を説明する概念的
な断面図である。FIG. 2 is a conceptual cross-sectional view illustrating the configuration of a conventional growth/analysis apparatus.
図において、21は成長室、22は分析室、23は試料
移動機構を有する試料移動室である。In the figure, 21 is a growth chamber, 22 is an analysis chamber, and 23 is a sample movement chamber having a sample movement mechanism.
上記の構成では、試料を分析するときは成長を中断して
、試料を試料移動室23を経由して分析室22に移動さ
せる必要があった。In the above configuration, when analyzing a sample, it was necessary to interrupt the growth and move the sample to the analysis chamber 22 via the sample transfer chamber 23.
分析と成長を同一真空室内で行えなかった原因は前述の
ように分析用の放射線を導入する放射窓に成長物質が付
着して放射線の透過率を減衰させるためであった。The reason why analysis and growth could not be performed in the same vacuum chamber was because, as mentioned above, the growth material adhered to the radiation window through which radiation for analysis was introduced, attenuating the transmittance of the radiation.
即時分析を可能とするため、分析と成長を同一真空室内
で行うと放射窓に成長物質が付着して放射線の透過率を
減衰させるという欠点があった。To enable immediate analysis, if analysis and growth were performed in the same vacuum chamber, the growth material would adhere to the emission window and attenuate the radiation transmittance.
上記問題点の解決は、分析用の放射線を導入する放射窓
(1)とレーザ光を専大するレーザ用窓(2)を有する
真空室(3)内に成長機構(4)を設けてなり、かつ、
外部より該レーザ用窓(2)を経由してレーザ光を該真
空室(3)内に導き該放射窓(1)に照射して、該放射
窓(1)の表面の汚染物質を選択的に加熱することによ
り、該汚染物質を蒸発させて該放射窓(1)の表面を清
浄化する機構を有する本発明による成長・分析装置によ
り達成される。The solution to the above problem is to provide a growth mechanism (4) within a vacuum chamber (3) having a radiation window (1) for introducing radiation for analysis and a laser window (2) for exclusively transmitting laser light. and,
Laser light is guided from the outside through the laser window (2) into the vacuum chamber (3) and irradiated onto the emission window (1) to selectively remove contaminants on the surface of the emission window (1). This is achieved by the growth and analysis apparatus according to the present invention, which has a mechanism for cleaning the surface of the emission window (1) by evaporating the contaminants by heating to .
本発明は、
(11放射窓表面に付着する汚染物質の光学的吸収係数
が高いため、ここに選択的にレーザ光を吸収し、
(2)かつ窓ガラスの熱伝導率が低いためにレーザ光を
照射した部分だけが局部的に温度上昇し、(3) さ
らに汚染物質の多(は蒸発しやすい(例えば、燐、砒素
等は蒸気圧が高い)、
等の作用を利用して、レーザ光の照射により汚染を除去
する機構を設けた。(11) Since the optical absorption coefficient of contaminants adhering to the emission window surface is high, the laser beam is selectively absorbed there; (2) The thermal conductivity of the window glass is low, so the laser beam The temperature rises locally only in the area that is irradiated with the laser beam, and (3) furthermore, many contaminants are easily evaporated (e.g., phosphorus, arsenic, etc. have high vapor pressure). A mechanism was installed to remove contamination by irradiation.
第1図は本発明の成長・分析装置の構成を説明する概念
的な断面図である。FIG. 1 is a conceptual cross-sectional view illustrating the structure of the growth/analysis apparatus of the present invention.
図において、1は分析用の放射線を導入する放射窓で、
アルミニウム(Al)とマグネシウム(Mg)のターゲ
ットをもつ、一般によく使われる光電子分光装置のX線
源の窓である。In the figure, 1 is a radiation window that introduces radiation for analysis.
This is the window of the X-ray source of a commonly used photoelectron spectrometer, which has aluminum (Al) and magnesium (Mg) targets.
波長5145人のアルゴン(八r)イオンレーザ5より
出る光を入射角60°で放射窓1を照射できるように、
真空室3にレーザ用窓2と、ミラー6.7を配置した。In order to irradiate the radiation window 1 with the light emitted from the argon (8R) ion laser 5 with a wavelength of 5145 at an incident angle of 60°,
A laser window 2 and a mirror 6.7 were placed in the vacuum chamber 3.
8はシャッタである。8 is a shutter.
4はガリウム砒素(GaAs)の分子線エピタキシャル
(MBE) 成長用のセルである。4 is a cell for molecular beam epitaxial (MBE) growth of gallium arsenide (GaAs).
この装置内で、GaAsのMBE成長と光電子分光測定
を行って本発明の効果を確かめた。In this apparatus, MBE growth of GaAs and photoelectron spectroscopy were performed to confirm the effects of the present invention.
GaAsの成長は通常、Gaに対するAsビームの流量
比が50倍以上と大きいため、真空室3内にはアモルフ
ァス状、または金属状のAsが付着する。When growing GaAs, the flow rate ratio of the As beam to Ga is usually as large as 50 times or more, so that amorphous or metallic As adheres to the inside of the vacuum chamber 3.
X線電子分光測定はAIの励起線(Kα)でGa2p3
/2準位(結合エネルギ1115eV)について行った
。X-ray electron spectroscopy measures Ga2p3 using the excitation line (Kα) of AI.
/2 level (binding energy 1115 eV).
GaAsの成長を100時間以上行い、Gaピークの強
度(I G−)が初期強度CrG−0)の70%に減少
した状態で、放射窓(X線窓)■にレーザビームを照射
した。GaAs was grown for more than 100 hours, and the emission window (X-ray window) was irradiated with a laser beam while the Ga peak intensity (I G-) was reduced to 70% of the initial intensity CrG-0).
第3図は放射窓に照射したレーザパワー密度とGaピー
クの強度比(I c−/ I c−0)の関係を示す図
である。FIG. 3 is a diagram showing the relationship between the laser power density irradiated onto the emission window and the Ga peak intensity ratio (I c-/I c-0).
ここで、レーザビームの照射時間は10分間である。Here, the laser beam irradiation time is 10 minutes.
図より、レーザビームの強度が10:lW/cm2以上
になるとGaピークの強度の増加がみられ、10’W/
cm2の照射で強度比が95%に改善される。From the figure, an increase in the intensity of the Ga peak is seen when the laser beam intensity increases to 10:1W/cm2 or more, and 10'W/cm2 or more is observed.
The intensity ratio is improved to 95% with irradiation of cm2.
これは、レーザビームの照射前は成長中のAsビームの
一部が放射窓1に付着し、AIKα励起線を吸収し、試
料の励起線強度を小さくしていたためと考えられる。This is considered to be because, before the laser beam irradiation, a part of the As beam during growth adhered to the emission window 1, absorbed the AIKα excitation line, and reduced the excitation line intensity of the sample.
レーザビームを照射することにより、放射窓1に付着し
たAsが選択的にレーザ光を吸収して、温度が上昇し再
蒸発させる効果があったことを、この実施例は示してい
る。This example shows that by irradiating the laser beam, As adhered to the emission window 1 selectively absorbed the laser beam, increasing the temperature and causing re-evaporation.
実施例ではAsを含む材料について述べたが、これの代
わりに蒸気圧の高い他の元素を含む材料による汚染に対
しても本発明は当然効果がある。Although the embodiments have been described with respect to materials containing As, the present invention is naturally effective against contamination caused by materials containing other elements with high vapor pressure instead.
以上詳細に説明したように本発明によれば、成長後の放
射窓の清浄が可能であるだけでなく、成長中にレーザ光
を照射することにより窓の汚染が防止できる。さらに成
長中に表面分析を同時に行うことが可能となる。As described in detail above, according to the present invention, it is not only possible to clean the emission window after growth, but also to prevent contamination of the window by irradiating the window with laser light during growth. Furthermore, it becomes possible to perform surface analysis simultaneously during growth.
第1図は本発明の成長・分析装置の構成を説明する概念
的な断面図、
第2図は従来の成長・分析装置の構成を説明する概念的
な断面図、
第3図は放射窓に照射したレーザパワー密度とGaピー
クの強゛度比(r 、、/ I G、、)の関係を示す
図である。
図において、
1は分析用の放射線を導入する放射窓で光電子分光装置
のX線源の窓、
2はし・−ザ用窓、
3は真空室、
4はGaAsのMBE成長用のセル、
5はアルゴンイオンレーザ、
6.7はミラー、
8はシャンクFigure 1 is a conceptual cross-sectional view explaining the configuration of the growth/analysis apparatus of the present invention, Figure 2 is a conceptual cross-sectional view explaining the configuration of a conventional growth/analysis apparatus, and Figure 3 is a conceptual cross-sectional view explaining the configuration of the growth/analysis apparatus of the present invention. FIG. 3 is a diagram showing the relationship between the irradiated laser power density and the Ga peak intensity ratio (r, , / I G,,). In the figure, 1 is a radiation window that introduces radiation for analysis; 2 is a window for the X-ray source of the photoelectron spectrometer; 3 is a vacuum chamber; 4 is a cell for GaAs MBE growth; 5 is argon ion laser, 6.7 is mirror, 8 is shank
Claims (1)
入するレーザ用窓(2)を有する真空室(3)内に成長
機構(4)を設けてなり、 かつ、外部より該レーザ用窓(2)を経由してレーザ光
を該真空室(3)内に導き該放射窓(1)に照射して、
該放射窓(1)の表面の汚染物質を選択的に加熱するこ
とにより、該汚染物質を蒸発させて該放射窓(1)の表
面を清浄化する機構を有することを特徴とする成長・分
析装置。[Claims] A growth mechanism (4) is provided in a vacuum chamber (3) having a radiation window (1) for introducing radiation for analysis and a laser window (2) for introducing laser light, and , leading a laser beam from the outside through the laser window (2) into the vacuum chamber (3) and irradiating the emission window (1);
Growth and analysis characterized by having a mechanism for selectively heating contaminants on the surface of the emission window (1) to evaporate the contaminants and clean the surface of the emission window (1). Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17211485A JPS6232607A (en) | 1985-08-05 | 1985-08-05 | Growth and analysis instrument |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17211485A JPS6232607A (en) | 1985-08-05 | 1985-08-05 | Growth and analysis instrument |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS6232607A true JPS6232607A (en) | 1987-02-12 |
Family
ID=15935813
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17211485A Pending JPS6232607A (en) | 1985-08-05 | 1985-08-05 | Growth and analysis instrument |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6232607A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2015531743A (en) * | 2012-08-30 | 2015-11-05 | トゥーエイ テクノロジーズ プライベート リミテッド | Apparatus and method for generating diamond and performing real-time field analysis |
-
1985
- 1985-08-05 JP JP17211485A patent/JPS6232607A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2015531743A (en) * | 2012-08-30 | 2015-11-05 | トゥーエイ テクノロジーズ プライベート リミテッド | Apparatus and method for generating diamond and performing real-time field analysis |
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