JPH0754293B2 - Particle measuring device - Google Patents
Particle measuring deviceInfo
- Publication number
- JPH0754293B2 JPH0754293B2 JP1002544A JP254489A JPH0754293B2 JP H0754293 B2 JPH0754293 B2 JP H0754293B2 JP 1002544 A JP1002544 A JP 1002544A JP 254489 A JP254489 A JP 254489A JP H0754293 B2 JPH0754293 B2 JP H0754293B2
- Authority
- JP
- Japan
- Prior art keywords
- cavity
- microwave
- fine particles
- sample gas
- reaction tank
- 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
Links
Landscapes
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
- Physical Vapour Deposition (AREA)
- Chemical Vapour Deposition (AREA)
Description
【発明の詳細な説明】 〈産業上の利用分野〉 本発明はスパッタリング装置、CVD装置等、半導体プロ
セスで成膜装置として使用される装置の反応槽中の微粒
子をインプロセスで検出できる微粒子測定装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION <Industrial field of application> The present invention is a fine particle measuring apparatus capable of in-process detection of fine particles in a reaction tank of an apparatus used as a film forming apparatus in a semiconductor process, such as a sputtering apparatus and a CVD apparatus Regarding
〈従来の技術〉 従来、微粒子測定装置として、反応槽中にレーザ光を照
射し、散乱光に基づきガス中の微粒子の大きさを求める
方法が公知である。しかしながら、この方法は次のよう
な欠点がある。<Prior Art> Conventionally, as a fine particle measuring device, a method is known in which a reaction tank is irradiated with laser light and the size of fine particles in a gas is determined based on scattered light. However, this method has the following drawbacks.
レーザ光の波長の制約から、直径が0.1μm以下の
微粒子の測定は原理的に出来ない。加えて実際の測定で
は測定装置を反応槽外において測定するため窓の汚れ等
によって0.5μm以下の微粒子は測定出来ない。一方、
半導体素子の高集積化は急速に進み、1MビットDRAM、4M
ビットDRAMのプロセスでは管理すべき微粒子の大きさが
0.05μmのレベルとなっている。In principle, it is not possible to measure fine particles with a diameter of 0.1 μm or less due to the restriction of the wavelength of laser light. In addition, in the actual measurement, since the measuring device is measured outside the reaction tank, fine particles of 0.5 μm or less cannot be measured due to stains on the window. on the other hand,
High integration of semiconductor devices has progressed rapidly, and 1Mbit DRAM, 4M
In the bit DRAM process, the size of the fine particles to be controlled is
The level is 0.05 μm.
光学的手法による検出のため微粒子の大きさしか分
らず、微粒子の組成についての情報は得られない。Since it is detected by an optical method, only the size of the fine particles is known, and no information about the composition of the fine particles is obtained.
〈発明が解決しようとする課題〉 本発明の解決しようとする技術的課題は、直径が0.05μ
m程度の微粒子をインラインで検出でき同時に成分の同
定も行える微粒子測定装置を実現することにある。<Problems to be Solved by the Invention> The technical problem to be solved by the present invention is that the diameter is 0.05 μm.
It is to realize a fine particle measuring device capable of detecting fine particles of about m in-line and at the same time identifying components.
〈課題を解決するための手段〉 本発明の構成は、 マイクロ波発生手段と,該マイクロ波発生手段で発生し
たマイクロ波を導入する導波管と,該導波管で導かれた
マイクロ波を一方の端面から導入する筒状のキャビティ
と,該キャビティの外周に設けられ前記マイクロ波の進
行方向と平行方向に磁界を形成する磁石と,前記キャビ
ティの他端付近の外周に設けられプラズマを閉込めるミ
ラー磁場を発生する磁石と,減圧された反応槽1内と前
記キャビティ内を結び反応槽内のサンプルガスを前記キ
ャビティ内に導くキャピラリーチューブと,前記キャビ
ティの他端付近に接続されそのキャビティ内を原子化/
イオン化が可能な程度に前記反応槽内の圧力より低圧に
する手段と,前記サンプルガスに含まれる微粒子により
前記キャビティ内に発生したイオンの発光スペクトルか
ら前記微粒子の定性・定量分析を行う分析装置を備え,
前記マイクロ波を前記キャビティ内でサイクロトロン共
鳴により加速した状態でキャリアガスを導入し,固体を
解離するに十分な励起温度とした後前記サンプルガスを
インラインで導入してサンプルガスに含まれる微粒子の
原子化/イオン化を行うことを特徴とするものである。<Means for Solving the Problems> The structure of the present invention is configured to include a microwave generation unit, a waveguide for introducing the microwave generated by the microwave generation unit, and a microwave guided by the waveguide. A cylindrical cavity introduced from one end face, a magnet provided on the outer periphery of the cavity to form a magnetic field in a direction parallel to the traveling direction of the microwave, and a plasma provided on the outer periphery near the other end of the cavity to close the plasma. A magnet that generates a mirror magnetic field that can be contained, a capillary tube that connects the depressurized reaction tank 1 and the inside of the cavity to guide the sample gas in the reaction tank into the cavity, and the inside of the cavity that is connected near the other end of the cavity. Atomize /
A means for making the pressure lower than the pressure in the reaction tank to the extent that ionization is possible, and an analyzer for performing qualitative / quantitative analysis of the fine particles from the emission spectrum of the ions generated in the cavity by the fine particles contained in the sample gas. Prepare,
Atoms of fine particles contained in the sample gas are introduced by introducing the carrier gas in a state in which the microwave is accelerated in the cavity by cyclotron resonance and making the excitation temperature sufficient to dissociate the solid. It is characterized by performing ionization / ionization.
〈作用〉 前記マイクロ波の周波数と磁界の強さをサイクロトロン
共鳴条件を満足する値に選ぶと電子が加速される。この
状態で前記キャビティ内にアルゴンガス又はヘリウムガ
スのキャリアガスを流すとプラズマが生成される。プラ
ズマは例えば10-2〜10-4Torrの領域では電子密度が低く
低温プラズマとなり固体を解離する能力はない。ミラー
磁場はプラズマを閉込め固体を解離するに充分な高温プ
ラズマを生成する。前記反応槽と前記キャビティとの間
には圧力差があり、この圧力差によってサンプルガスは
プラズマ内に導かれ、サンプルガスに含まれる微粒子が
解離、イオン化する。この場合、微粒子が小さい程、解
離、イオン化し易い。イオン化された微粒子は成分固有
の発光スペクトルを持っているため、例えばこれを分光
器を用いて測定すれば、微粒子の量的測定、及び成分の
同定が同時に行える。<Operation> When the frequency of the microwave and the strength of the magnetic field are selected to values satisfying the cyclotron resonance condition, the electrons are accelerated. In this state, when a carrier gas of argon gas or helium gas is flown into the cavity, plasma is generated. For example, plasma has a low electron density in the region of 10 -2 to 10 -4 Torr and becomes low temperature plasma, which has no ability to dissociate solids. The mirror magnetic field produces a high temperature plasma sufficient to confine the plasma and dissociate the solids. There is a pressure difference between the reaction tank and the cavity, and the sample gas is introduced into the plasma by this pressure difference, and the fine particles contained in the sample gas are dissociated and ionized. In this case, the smaller the particles, the easier the dissociation and ionization. Since the ionized fine particles have an emission spectrum specific to the components, if the fine particles are measured using a spectroscope, for example, the quantitative measurement of the fine particles and the identification of the components can be performed at the same time.
〈実施例〉 以下図面に従い本発明を説明する。図は本発明実施例装
置の構成図である。一点鎖線で囲んだ部分(1)が反応
槽としてのCVD装置である。部分(2)は本発明に関わ
る微粒子測定装置である。部分(1)において、CVD装
置1は、側壁101、石英の窓102、加熱手段としてのラン
プ103、反応槽A内に水平に設置され上面にシリコンウ
エハSが載置されたサセプタ104、SiH4ガス及びNH3ガス
をシリコンウエハS上に導くパイプ105、真空ポンプ106
とより構成される。<Examples> The present invention will be described below with reference to the drawings. The figure is a block diagram of the apparatus of the present invention. The part (1) surrounded by the one-dot chain line is a CVD device as a reaction tank. Part (2) is the particle measuring device according to the present invention. In the portion (1), the CVD apparatus 1 includes a side wall 101, a quartz window 102, a lamp 103 as a heating means, a susceptor 104 horizontally installed in the reaction tank A and having a silicon wafer S mounted on the upper surface, and SiH 4 Pipe 105 for guiding gas and NH 3 gas onto the silicon wafer S, vacuum pump 106
Composed of and.
部分(2)において、微粒子測定装置2は、反応槽内A
からサンプルガスSGを微粒子測定装置に導くキャピラリ
チューブ201、マイクロ波源202、マイクロ波源202から
マイクロ波が導波管203を通して導入され、反応管とし
て使われる円筒状キャビティ204、キャビティ204内に前
記マイクロ波の進行方向と平行に磁界を形成する磁石20
5、キャピラリーチューブ201からのサンプルガスSGとア
ルゴン、ヘリウム等のキャリアガスCGとをキャビティ20
4に導く導入管206、キャビティ204からガスを排気する
排気手段207、キャビティ204の解放端付近に設けられ、
プラズマを閉込めるミラー磁場を発生する磁石208、導
波管203の開口端203aに向けて設けられサンプルガスSG
中の微粒子を定性・定量分析する分析手段209とから構
成されている。尚、本実施例の場合、分析手段209には
回折格子209aを用いた分光分析手段が用いられている。In the part (2), the fine particle measuring apparatus 2 has
A capillary tube 201 that guides the sample gas SG from the sample to the particle measuring apparatus, a microwave source 202, a microwave is introduced from a microwave source 202 through a waveguide 203, and a cylindrical cavity 204 used as a reaction tube, the microwave inside the cavity 204 are used. Magnet 20 that forms a magnetic field parallel to the traveling direction of
5. The sample gas SG from the capillary tube 201 and the carrier gas CG such as argon and helium are stored in the cavity 20.
4, the introduction pipe 206 leading to 4, the exhaust means 207 for exhausting gas from the cavity 204, and the vicinity of the open end of the cavity 204,
Magnet 208 for generating a mirror magnetic field for confining plasma, sample gas SG provided toward the open end 203a of the waveguide 203
It comprises an analysis means 209 for qualitatively and quantitatively analyzing the fine particles therein. In the case of this embodiment, the analyzing means 209 is a spectroscopic analyzing means using a diffraction grating 209a.
このような構成で、CVD装置1においてシリコンウエハ
Sが載せられたサセプタ104をランプ103で加熱し、パイ
プ105よりNH3ガス及びSiH4ガスを導きシリコンウエハS
上に窒化シリコン膜を形成する。反応槽Aとキャビティ
204との間には圧力差があり(反応槽A内:10-1〜1Tor
r、キャビティ204内:10-2〜10-4Torr)、サンプルガス
SGはこの圧力差によってキャビティ204内に導かれる。With such a configuration, in the CVD apparatus 1, the susceptor 104 on which the silicon wafer S is placed is heated by the lamp 103, and NH 3 gas and SiH 4 gas are introduced from the pipe 105 to guide the silicon wafer S.
A silicon nitride film is formed on top. Reaction tank A and cavity
There is a pressure difference with 204 (in reaction tank A: 10 -1 to 1 Tor
r, inside cavity 204: 10 -2 to 10 -4 Torr), sample gas
SG is guided into the cavity 204 by this pressure difference.
マイクロ波源202からマイクロ波が導波管203を通してキ
ャビティ204に導入され、マイクロ波の周波数を2.45GH
z、磁石205による磁場の強度を875ガウスとしたとき、
サイクロトロン共鳴条件が満たされ電子がサイクロトロ
ン運動により加速され、中性粒子の解離効率が高まる。
この状態で導入管206にアルゴンガス又はヘリウムガス
のキャリアガスCGを流すとプラズマPLが形成される。プ
ラズマPLは10-2〜10-4Torrの領域では電子密度は1010個
/cm3程度で、励起温度は1000゜K以下の低温プラズマ
となりこのままでは固体を解離する能力はない。磁石20
8によるミラー磁場によりプラズマを閉込めると電子は
何度もこの領域で加速され高い電子密度が得られ、1012
〜1013個/cm3程度の電子密度になれば固体を解離する
に充分な励起温度となる。プラズマPLに導かれたサンプ
ルガスSG中の微粒子はプラズマによって解離され、イオ
ン化される。このような電子サイクロトロン共鳴による
プラズマによれば減圧下でも直径0.1〜0.05μmの固体
を解離、イオン化させることができる。Microwave from the microwave source 202 is introduced into the cavity 204 through the waveguide 203, and the microwave frequency is changed to 2.45GH.
z, when the strength of the magnetic field by the magnet 205 is 875 Gauss,
The cyclotron resonance condition is satisfied, the electrons are accelerated by the cyclotron motion, and the dissociation efficiency of neutral particles increases.
In this state, when a carrier gas CG of argon gas or helium gas is flown through the introduction pipe 206, plasma PL is formed. The plasma PL has an electron density of about 10 10 electrons / cm 3 in the region of 10 -2 to 10 -4 Torr, and has a low temperature plasma with an excitation temperature of 1000 ° K or less, which has no ability to dissociate solids. Magnet 20
When confining the plasma by a mirror magnetic field due 8 electrons again and high electron density is accelerated in this region is obtained, 10 12
When the electron density is about 10 13 electrons / cm 3, the excitation temperature is sufficient to dissociate the solid. The fine particles in the sample gas SG introduced into the plasma PL are dissociated by the plasma and ionized. Such plasma by electron cyclotron resonance can dissociate and ionize a solid having a diameter of 0.1 to 0.05 μm even under reduced pressure.
イオン化された微粒子は成分固有の発光スペクトルを持
っている。この発光を分析手段209で検出する。スペク
トル強度から微粒子の量的情報が得られ、スペクトルの
波長に基づき成分の同定を行う。尚、分析手段209は分
光器に限らず、質量分析装置を用いて解離した原子イオ
ンを測定しても同様な情報が得られる。また磁石205,20
8に永久磁石を使用すれば装置を小型化することができ
る。The ionized fine particles have an emission spectrum unique to each component. This luminescence is detected by the analysis means 209. Quantitative information of fine particles is obtained from the spectrum intensity, and the component is identified based on the wavelength of the spectrum. The analyzing means 209 is not limited to a spectroscope, and similar information can be obtained by measuring dissociated atomic ions using a mass spectrometer. Also magnet 205,20
If a permanent magnet is used for 8, the device can be downsized.
〈発明の効果〉 本発明によれば以下のような効果を有する。<Effects of the Invention> The present invention has the following effects.
従来の光学的方法によっては原理的に測定が不可能
であった直径が0.1〜0.05μmレベルの微粒子をインラ
インで検出することができる。Fine particles having a diameter of 0.1 to 0.05 μm, which cannot be measured in principle by the conventional optical method, can be detected in-line.
微粒子の量的情報が得られる他、成分の同定も同時
に行える。In addition to obtaining quantitative information of fine particles, identification of components can be performed at the same time.
キャピラリチューブを使って前記反応槽と前記キャ
ビティとの圧力差でサンプリングを行うのでサンプルガ
スを移送する特別の手段が要らない。Since a capillary tube is used to perform sampling by the pressure difference between the reaction tank and the cavity, no special means for transferring the sample gas is required.
電子サイクロトロン共鳴に基づくプラズマ中では微
粒子に径が小さい程、解離、イオン化し易く原理的に径
の小さな微粒子の測定に向いている。In plasma based on electron cyclotron resonance, the smaller the particle size, the easier the particle is to dissociate and ionize, which is in principle suitable for measuring the small particle size.
例えば反応槽内の不純物が一定量を超えたときに、即座
に作業を中止して清掃を行ったり、あるロットの物を不
良品として廃棄することにより、これを組み込む製品の
不良を防止することが出来る。For example, when the amount of impurities in the reaction tank exceeds a certain amount, immediately stop the work and clean it, or discard a certain lot as a defective product to prevent defects in the product incorporating it. Can be done.
図は本発明実施例装置の構成図である。 1……CVD装置、102……石英の窓、103……加熱手段、1
04……サセプタ、106……真空ポンプ、2……微粒子測
定装置、201……キャピラリチューブ、202……マイクロ
波源、203……導波管、204……キャビティ、205……磁
石、206……導入管、207……排気手段、208……ミラー
磁場発生用の磁石、209……分析手段、209a……回折格
子、SG……サンプルガス、CG……キャリアガス、PL……
プラズマThe figure is a block diagram of the apparatus of the present invention. 1 ... CVD device, 102 ... Quartz window, 103 ... Heating means, 1
04 …… Susceptor, 106 …… Vacuum pump, 2 …… Particle measuring device, 201 …… Capillary tube, 202 …… Microwave source, 203 …… Waveguide, 204 …… Cavity, 205 …… Magnet, 206 …… Introduction tube, 207 ... Exhaust means, 208 ... Mirror, magnet for generating magnetic field, 209 ... Analytical means, 209a ... Diffraction grating, SG ... Sample gas, CG ... Carrier gas, PL ...
plasma
Claims (1)
発生手段で発生したマイクロ波を導入する導波管203
と,該導波管で導かれたマイクロ波を一方の端面から導
入する筒状のキャビティ204と,該キャビティの外周に
設けられ前記マイクロ波の進行方向と平行方向に磁界を
形成する磁石205と,前記キャビティの他端付近の外周
に設けられプラズマを閉込めるミラー磁場を発生する磁
石208と,減圧された反応槽1内と前記キャビティ内を
結び反応槽1内のサンプルガスを前記キャビティ内に導
くキャピラリーチューブ201と,前記キャビティの他端
付近に接続されそのキャビティ内を原子化/イオン化が
可能な程度に前記反応槽1内の圧力より低圧にする手段
と,前記サンプルガスに含まれる微粒子により前記キャ
ビティ内に発生したイオンの発光スペクトルから前記微
粒子の定性・定量分析を行う分析装置209を備え,前記
マイクロ波を前記キャビティ内でサイクロトロン共鳴に
より加速した状態でキャリアガスを導入し,固体を解離
するに十分な励起温度とした後前記サンプルガスをイン
ラインで導入してサンプルガスに含まれる微粒子の原子
化/イオン化を行うことを特徴とする微粒子測定装置。1. A microwave generating means 202 and a waveguide 203 for introducing the microwave generated by the microwave generating means.
A cylindrical cavity 204 for introducing the microwave guided by the waveguide from one end face, and a magnet 205 provided on the outer periphery of the cavity for forming a magnetic field in a direction parallel to the traveling direction of the microwave. , A magnet 208 provided on the outer periphery near the other end of the cavity for generating a mirror magnetic field for confining plasma, and connecting the depressurized reaction tank 1 and the inside of the cavity with the sample gas in the reaction tank 1 into the cavity. The capillary tube 201 for guiding, means for connecting the vicinity of the other end of the cavity to lower the pressure in the reaction vessel 1 to the extent that atomization / ionization in the cavity is possible, and the fine particles contained in the sample gas The cavity is provided with an analyzer 209 for performing qualitative / quantitative analysis of the fine particles from the emission spectrum of the ions generated in the cavity. In order to atomize / ionize the fine particles contained in the sample gas, the carrier gas is introduced in a state accelerated by cyclotron resonance at a temperature of, and the sample gas is introduced in-line after the excitation temperature is high enough to dissociate the solid. Characteristic particle measuring device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1002544A JPH0754293B2 (en) | 1989-01-09 | 1989-01-09 | Particle measuring device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1002544A JPH0754293B2 (en) | 1989-01-09 | 1989-01-09 | Particle measuring device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02183140A JPH02183140A (en) | 1990-07-17 |
| JPH0754293B2 true JPH0754293B2 (en) | 1995-06-07 |
Family
ID=11532326
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1002544A Expired - Lifetime JPH0754293B2 (en) | 1989-01-09 | 1989-01-09 | Particle measuring device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0754293B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100253089B1 (en) * | 1997-10-29 | 2000-05-01 | 윤종용 | Chemical vapor deposition apparatus |
| FR2788854B1 (en) * | 1999-01-22 | 2001-05-04 | Cit Alcatel | SYSTEM AND METHOD FOR IDENTIFYING GASEOUS EFFLUENTS, EQUIPMENT PROVIDED WITH SUCH A SYSTEM |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57108655A (en) * | 1980-12-25 | 1982-07-06 | Tsukasa Sotsuken:Kk | Device for measuring air fuel ratio of internal combustion engine or other burning apparatus |
| JPH089778B2 (en) * | 1986-09-29 | 1996-01-31 | 日本電信電話株式会社 | Ion source |
-
1989
- 1989-01-09 JP JP1002544A patent/JPH0754293B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02183140A (en) | 1990-07-17 |
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| FLAMM | AT&T Bell Laboratories, Murray Hill, NJ 07974 and University of California at Berkeley, Berkeley, CA 94720 |