JPS6398948A - High frequency inductive coupling plasma/mass spectrometer - Google Patents
High frequency inductive coupling plasma/mass spectrometerInfo
- Publication number
- JPS6398948A JPS6398948A JP61243923A JP24392386A JPS6398948A JP S6398948 A JPS6398948 A JP S6398948A JP 61243923 A JP61243923 A JP 61243923A JP 24392386 A JP24392386 A JP 24392386A JP S6398948 A JPS6398948 A JP S6398948A
- Authority
- JP
- Japan
- Prior art keywords
- plasma
- shield
- high frequency
- plasma torch
- coil
- 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
Links
- 230000008878 coupling Effects 0.000 title abstract 2
- 238000010168 coupling process Methods 0.000 title abstract 2
- 238000005859 coupling reaction Methods 0.000 title abstract 2
- 230000001939 inductive effect Effects 0.000 title abstract 2
- 150000002500 ions Chemical class 0.000 claims abstract description 12
- 238000009616 inductively coupled plasma Methods 0.000 claims description 9
- 230000002265 prevention Effects 0.000 claims description 7
- 238000004458 analytical method Methods 0.000 claims description 4
- 238000010891 electric arc Methods 0.000 claims description 2
- 230000006698 induction Effects 0.000 claims description 2
- 238000000034 method Methods 0.000 claims 1
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 abstract description 12
- 239000007789 gas Substances 0.000 abstract description 10
- 229910052786 argon Inorganic materials 0.000 abstract description 6
- 238000010586 diagram Methods 0.000 description 4
- 239000000443 aerosol Substances 0.000 description 2
- 238000001095 inductively coupled plasma mass spectrometry Methods 0.000 description 2
- 239000003990 capacitor Substances 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000006199 nebulizer Substances 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
- Electron Tubes For Measurement (AREA)
Abstract
Description
【発明の詳細な説明】
〈産業上の利用分野〉
本発明は、高周波誘導結合プラズマと質量分析計を結合
させてなる高周波誘導結合プラズマ・質量分析計(In
ductively Coupled Plasma・
HassSpcctometer 、以下rlcP −
MSJと略す)に関する。[Detailed Description of the Invention] <Industrial Application Field> The present invention relates to a high frequency inductively coupled plasma/mass spectrometer (Industrial Application Field) which combines a high frequency inductively coupled plasma and a mass spectrometer.
ductively coupled plasma・
HassSpcctometer, hereinafter rlcP -
(abbreviated as MSJ).
〈従来の技術〉
ICr’ −MSは、高周波誘導結合プラズマを用いて
試料を励起させ、生じたイオンを、例えばノズルやスキ
マーからなるインターフェイスを介して質量分析計に導
いて、特定質量のイオンを電気的に検出し、該イオン量
を精密に測定することによって、上記試料中の被測定元
素等を分析するように構成されている。第3図は二のよ
うなIcP −MSの従来例要部構成説明図であり、図
中、1は例えば、最外室1a、外室1b、および内室I
Cを有する三重管構造のプラズマトーチ、2は該トーチ
1に巻回された高周波:S導コイル、3は該コイル2に
コンデンサCt、 Cxを介して高周波電流を供給する
高周波電源、4は高周波誘導結合プラズマ、5はノズル
、6はスキマーである。この図において、コイル2の中
に上記高周波電流が流されると該コイル2の周囲に高周
波磁界が形成される。この高周波磁界の近傍でプラズマ
トーチ1内のアルゴンガス中に電子かイオンが植え付け
られると、該高周波磁界の作用で瞬時にプラズマ4が生
じると共に、該プラズマが一定の高周波電位を有するよ
うになる。<Prior art>ICr'-MS uses high-frequency inductively coupled plasma to excite a sample, and the generated ions are guided to a mass spectrometer through an interface consisting of a nozzle or skimmer, and ions of a specific mass are extracted. It is configured to analyze the element to be measured in the sample by electrically detecting and precisely measuring the amount of the ions. FIG. 3 is an explanatory diagram of the main part configuration of a conventional example of IcP-MS as shown in 2. In the figure, 1 indicates, for example, the outermost chamber 1a, the outer chamber 1b, and the inner chamber I.
2 is a high frequency: S conductive coil wound around the torch 1; 3 is a high frequency power source that supplies a high frequency current to the coil 2 via a capacitor Ct and Cx; 4 is a high frequency Inductively coupled plasma, 5 is a nozzle, and 6 is a skimmer. In this figure, when the high frequency current is passed through the coil 2, a high frequency magnetic field is formed around the coil 2. When electrons or ions are planted in the argon gas in the plasma torch 1 near this high frequency magnetic field, plasma 4 is instantaneously generated by the action of the high frequency magnetic field, and the plasma has a constant high frequency potential.
一方、上記プラズマ4と高周波誘導コイル2は容量的に
結合されており、該プラズマ4が高周波電位を有してい
る。これに対し、ノズル5やスキマー6は、通常、アー
ス接続されて接地電位を有しているため、ノズル5やス
キマー6の先端とプラズマ4との間に放電が生ずるよう
になる。また、プラズマ4からスキマー6内に引き出さ
れるイオンは、このような放電等の影りにより、上記プ
ラーシ/
ダマ4内で得られるイオン特性が失われたものとなり究
極的にICP −MSの分析精度を著しく低下させるよ
うになる。このような分析精度の低下を防ぐため、上記
プラズマ4とコイル2の間にシールドを入れる工夫もな
されていた。On the other hand, the plasma 4 and the high frequency induction coil 2 are capacitively coupled, and the plasma 4 has a high frequency potential. On the other hand, since the nozzle 5 and the skimmer 6 are normally connected to the ground and have a ground potential, discharge occurs between the tips of the nozzle 5 and the skimmer 6 and the plasma 4. In addition, the ions extracted from the plasma 4 into the skimmer 6 lose their ion characteristics obtained in the plastic/clump 4 due to the shadow of such discharge, which ultimately impairs the analysis accuracy of ICP-MS. This results in a significant decrease in In order to prevent such a decrease in analysis accuracy, a shield has been installed between the plasma 4 and the coil 2.
〈発明が解決しようとする問題点〉
然し乍ら、上記従来例においては、プラズマ4とコイル
2の間に配設されるシールドを厳重にすればする程上記
プラズマ4が生じなくなるという大きな欠点があった。<Problems to be Solved by the Invention> However, in the conventional example described above, there was a major drawback in that the more severe the shield placed between the plasma 4 and the coil 2, the less the plasma 4 would be generated. .
本発明はかかる従来例の欠点に工みてなされたものであ
り、その目的は、プラズマ4とコイル2の間に配設され
るシールドをff1ff!にし且つプラズマ4を正常に
維持できるようなICP −MSを提供することにある
。The present invention has been devised to overcome the drawbacks of the conventional example, and its purpose is to eliminate the ff1ff! shield disposed between the plasma 4 and the coil 2. The object of the present invention is to provide an ICP-MS that can maintain the plasma 4 normally.
く問題点を解決するための手段〉
上述のような問題点を解決する本発明の#+f徴は、I
cP −MSにおいて、高周波誘導結合プラズマを生じ
させてのちシールド板をプラズマトーチの方向へスライ
ドさせ、アーク防止管とプラズマトーチで形成される間
隙内にシールドをtil!設するように構成したことに
ある。Means for Solving the Problems> The #+f feature of the present invention that solves the above problems is that I
In cP-MS, after generating high-frequency inductively coupled plasma, the shield plate is slid in the direction of the plasma torch, and the shield is tilted into the gap formed between the arc prevention tube and the plasma torch. This is due to the fact that it has been configured to
〈実施例〉
以下、本発明について図を用いて評しく説明する。第1
図は本発明実施例の要部を分解した構成斜視図であり、
図中、第3図と同一記号は同一意味をもたせて使用しこ
こでの重複説明は省略する。<Example> The present invention will be described below with reference to the drawings. 1st
The figure is an exploded configuration perspective view of the main parts of the embodiment of the present invention,
In the figure, the same symbols as in FIG. 3 are used with the same meaning, and repeated explanation will be omitted here.
また、7は例えば石英管でなりアーク放電が生ずるのを
防止するアーク防止管、8はプラズマトーチ1の外側に
挿設されるシールド、9はシールド8の底部8′が例え
ばネジ止め等で画性されたシールド板である。第1図に
おいて、アーク防止管7がコイル2にあらかじめ装設さ
れて固定される。Further, 7 is a quartz tube, for example, and is an arc prevention tube that prevents arc discharge, 8 is a shield inserted outside the plasma torch 1, and 9 is a shield 8 whose bottom 8' is fixed with a screw or the like. This is a shield plate that has been treated with a high-temperature finish. In FIG. 1, an arc prevention tube 7 is installed and fixed to the coil 2 in advance.
その後、コイル2に高周波電流が流され該コイルの周囲
に高周波磁界が形成される。この高周波磁界の近傍でプ
ラズマトーチl内のアルゴンガス中に電子かイオンが植
えつけられると、該高周波磁界の作用で瞬時にプラズマ
4が生じる。この状態で、シールド板9をプラズマトー
チ1の方向へスライドさせ、アーク防止管7(即ち、コ
イル2)とプラズマトーチ1で形成される間隙内にシー
ルド2が挿入される。このようにすることにより、プラ
ズマトーチlの外側にシールド2が挿設される。また、
シールド2が堅牢であるにも拘らずプラズマ4は消えな
い。従って、第1図に示すような要部構成を有するIc
P −MSはシールド8が厳重で且つプラズマ4を正常
に維持できるようになる。Thereafter, a high frequency current is passed through the coil 2 to form a high frequency magnetic field around the coil. When electrons or ions are planted in the argon gas in the plasma torch l near this high frequency magnetic field, plasma 4 is instantaneously generated by the action of the high frequency magnetic field. In this state, the shield plate 9 is slid in the direction of the plasma torch 1, and the shield 2 is inserted into the gap formed between the arc prevention tube 7 (ie, the coil 2) and the plasma torch 1. By doing so, the shield 2 is inserted outside the plasma torch l. Also,
Although the shield 2 is strong, the plasma 4 does not disappear. Therefore, Ic having the main part configuration as shown in FIG.
In P-MS, the shield 8 is strict and the plasma 4 can be maintained normally.
第2図は本発明実施例の全体的な構成説明図であり、図
中、第1図や第3図と同一記号は同一意味をもたせて使
用しここでの重複説明は省略する。FIG. 2 is an explanatory diagram of the overall configuration of an embodiment of the present invention. In the figure, the same symbols as in FIGS. 1 and 3 are used with the same meanings, and redundant explanation will be omitted here.
また、loaはアルゴンガス供給源、IObはガス調節
器、11は試料を貯留する槽、12は試料を1化してエ
アロゾル試料にするネプライザ、13は高周波電源3を
含む駆動部、14はプラズマトーチを収納する筺体、1
5はフォアチャンバー16内を例えば1 torr、ま
で吸引してlJt気する真空ポンプ、17はセンターチ
ャンバー18内を例えばIF ’ torr 、まで吸
引して排気する真空ポンプ、19は例えば四m極マスフ
ィルタでなる質量分析計検出器、20はリアチャンバー
21内を吸引して1ノ[気する真空ポンプ、22は二次
電子増(t!i管、23は演算処理部(例えばマイクロ
コンピュータ)である。このような構成からなる本発明
の実施例において、プラズマトーチlの最外室1aおよ
びIbには、ガス調節器10bを介してガス供給源10
aからアルゴンガスが供給される。また、内室1cには
ネプライザ12からアルゴンガス(上記ガス調節器lO
bを介して供給されるもの)によってエアロゾル試零”
(が搬入される。一方、コイル2には駆動部13内の高
周波電源3によって高周波エネルギーが供給され、該コ
イルの周囲に高周波磁界(図示せず)が形成されている
。このため、上記高周波磁界の作用でプラズマ4が生ず
る。このプラズマ4内のイオンはノズル5を介してスキ
マー6内に引き出され、その後、質量分析計検出器19
によって特定質量のイオンが検出される。該検出信号は
二次電子増倍管22で増幅されてのち演算処理部23に
送出され、R終曲に試料中の被測定元素分析m等を与え
るようになる6
〈発明の効果〉
以上詳しく設問したような本発明によれば、プラズマ4
とコイル20間に配設されるシールドを厳重にし且つプ
ラズマ4を正常に維持できるようなICP −H5が実
現する。In addition, loa is an argon gas supply source, IOb is a gas regulator, 11 is a tank for storing the sample, 12 is a nebulizer that unifies the sample to form an aerosol sample, 13 is a drive unit including a high-frequency power source 3, and 14 is a plasma torch. A housing for storing 1
5 is a vacuum pump that suctions the inside of the forechamber 16 to, for example, 1 torr and generates 1Jt, 17 is a vacuum pump that suctions and exhausts the inside of the center chamber 18 to, for example, IF' torr, and 19 is, for example, a four-m pole mass filter. 20 is a vacuum pump that suctions the inside of the rear chamber 21, 22 is a secondary electron multiplier (t!i tube), and 23 is an arithmetic processing unit (for example, a microcomputer). In the embodiment of the present invention having such a configuration, a gas supply source 10 is connected to the outermost chambers 1a and Ib of the plasma torch 1 via a gas regulator 10b.
Argon gas is supplied from a. In addition, the inner chamber 1c is supplied with argon gas (the gas regulator lO
aerosol sample (supplied via b)
(is carried in. On the other hand, high-frequency energy is supplied to the coil 2 by the high-frequency power supply 3 in the drive unit 13, and a high-frequency magnetic field (not shown) is formed around the coil. A plasma 4 is generated under the action of a magnetic field.The ions within this plasma 4 are drawn out through a nozzle 5 into a skimmer 6 and then into a mass spectrometer detector 19.
ions of a specific mass are detected by The detection signal is amplified by the secondary electron multiplier tube 22 and then sent to the arithmetic processing section 23, and the R final song is given the analysis of the element to be measured m in the sample, etc.6 <Effects of the invention> Questions in detail above According to the present invention, plasma 4
An ICP-H5 is realized in which the shield disposed between the coil 20 and the coil 20 is made strict and the plasma 4 can be maintained normally.
第1図は本発明実施例の妻部構成斜視図、第2図は本発
明実施例の全体的な構成説明図、第3図は従来例の要部
構成説明図である。
1・・・プラズマトーチ、2・・・高層Xa導コイル、
3・・・高周波電源、4・・・高周波誘導結合プラズマ
、7・・・アーク防止管、8・・・シールド、9・・・
シールド板。
′P、2図
#i″3図FIG. 1 is a perspective view of the configuration of the end portion of the embodiment of the present invention, FIG. 2 is an explanatory diagram of the overall configuration of the embodiment of the present invention, and FIG. 3 is an explanatory diagram of the main part configuration of the conventional example. 1... Plasma torch, 2... High-rise Xa conductive coil,
3... High frequency power supply, 4... High frequency inductively coupled plasma, 7... Arc prevention tube, 8... Shield, 9...
shield board. 'P, Figure 2 #i'' Figure 3
Claims (2)
周波磁界を形成して高周波誘導結合プラズマを生じさせ
、該プラズマを用いて試料を励起してイオンを生じさせ
、該イオンをインターフェイスを介して質量分析計に導
いて検出し、前記試料中の被測定元素を分析する分析計
において、前記コイルにあらかじめ装設され前記インタ
ーフェイス先端部と前記プラズマの間に生ずるアーク放
電を防止するアーク防止管と、前記プラズマを生じさせ
るプラズマトーチの外側に挿設されるシールドと、該シ
ールドの底部が固着されたシールド板とを具備し、前記
プラズマを生じさせてのち前記シールド板を前記プラズ
マトーチの方向へスライドさせ、前記アーク防止管とプ
ラズマトーチで形成される間隙内に前記シールドを挿設
するように構成したことを特徴とする高周波誘導結合プ
ラズマ・質量分析計。(1) High-frequency energy is supplied to a high-frequency induction coil to form a high-frequency magnetic field to generate high-frequency inductively coupled plasma, the plasma is used to excite the sample to generate ions, and the ions are subjected to mass analysis via an interface. In the analyzer for detecting and analyzing the elements to be measured in the sample, the analyzer includes: an arc prevention tube installed in the coil in advance to prevent arc discharge occurring between the interface tip and the plasma; The method includes a shield inserted outside a plasma torch that generates plasma, and a shield plate to which the bottom of the shield is fixed, and after generating the plasma, the shield plate is slid in the direction of the plasma torch. . A high frequency inductively coupled plasma/mass spectrometer, characterized in that the shield is inserted into a gap formed between the arc prevention tube and the plasma torch.
る特許請求範囲第(1)項記載の高周波誘導結合プラズ
マ・質量分析計。(2) The high frequency inductively coupled plasma mass spectrometer according to claim (1), wherein the interface comprises a nozzle and a skimmer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61243923A JPH0624113B2 (en) | 1986-10-14 | 1986-10-14 | High frequency inductively coupled plasma / mass spectrometer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP61243923A JPH0624113B2 (en) | 1986-10-14 | 1986-10-14 | High frequency inductively coupled plasma / mass spectrometer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS6398948A true JPS6398948A (en) | 1988-04-30 |
JPH0624113B2 JPH0624113B2 (en) | 1994-03-30 |
Family
ID=17111031
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP61243923A Expired - Fee Related JPH0624113B2 (en) | 1986-10-14 | 1986-10-14 | High frequency inductively coupled plasma / mass spectrometer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0624113B2 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02148648A (en) * | 1988-11-30 | 1990-06-07 | Yokogawa Electric Corp | High frequency inductive bonding plasma mass spectrometer |
JPH0316656U (en) * | 1989-06-30 | 1991-02-19 |
-
1986
- 1986-10-14 JP JP61243923A patent/JPH0624113B2/en not_active Expired - Fee Related
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02148648A (en) * | 1988-11-30 | 1990-06-07 | Yokogawa Electric Corp | High frequency inductive bonding plasma mass spectrometer |
JPH0316656U (en) * | 1989-06-30 | 1991-02-19 |
Also Published As
Publication number | Publication date |
---|---|
JPH0624113B2 (en) | 1994-03-30 |
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