JPH01137553A - Mass spectrometer - Google Patents

Mass spectrometer

Info

Publication number
JPH01137553A
JPH01137553A JP62294660A JP29466087A JPH01137553A JP H01137553 A JPH01137553 A JP H01137553A JP 62294660 A JP62294660 A JP 62294660A JP 29466087 A JP29466087 A JP 29466087A JP H01137553 A JPH01137553 A JP H01137553A
Authority
JP
Japan
Prior art keywords
voltage
mass
mass spectrometer
mode
ion
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
JP62294660A
Other languages
Japanese (ja)
Inventor
Atsushi Hosoi
淳 細井
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
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP62294660A priority Critical patent/JPH01137553A/en
Publication of JPH01137553A publication Critical patent/JPH01137553A/en
Pending legal-status Critical Current

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  • Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
  • Electron Tubes For Measurement (AREA)

Abstract

PURPOSE:To make a mass spectrometer small-sized and reduce the cost by switching it to a mode superimposedly applying the DC voltage and the RF voltage to a quadruple-electrode section and a mode applying only the RF voltage. CONSTITUTION:A measurement mode scanning only the RF voltage can be switched in addition to the normal measurement mode applying the voltage superimposed with the DC voltage and the RF voltage to a quadruple-electrode section and scanning the voltage while the Vdc/Vrf ratio is kept constant to measure the mass spectrum. The measurement with no reduction of the ion permeation efficiency can be performed, and high-mass ions generated by an FAB ion source are efficiently measured. The mass spectrometry on a nonvolatile or thermally unstable sample with the FAB ion source can be thereby performed with a small-sized and inexpensive quadruple-electrode type mass spectrometer.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は熱的に不安定な化合物や難揮発性化合物を対象
とする質量分析装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a mass spectrometer that targets thermally unstable compounds and poorly volatile compounds.

[従来技術] 複雑混合物試料の分離分析にガスクロマトグラフ質量分
析装置(GCMS)が用いられているが、原理的に揮発
性を有する試料に限定される。生体関連成分は熱的に不
安定なものや難揮発性のものが多く、GCMSでは分析
が困難である。これらを対象とする質量分析を可能とす
る為、各種のイオン化法が開発されGCMSの付加機能
として用いられている。高速中性原子衡撃(Fast 
Atom Bombardment、FAB)イオン源
もその目的で開発されたもので現在実用されるに至うて
いる。
[Prior Art] Gas chromatograph mass spectrometers (GCMS) are used for the separation and analysis of complex mixture samples, but in principle they are limited to volatile samples. Many biological components are thermally unstable or poorly volatile, making analysis difficult with GCMS. In order to enable mass spectrometry targeting these, various ionization methods have been developed and used as additional functions of GCMS. Fast neutral atomic bombardment
Atom bombardment (FAB) ion sources were also developed for this purpose and are now in practical use.

[発明が解決しようとする問題点] 四重種型質量分析装置は従来の磁場セクター形に比して
小形で低価格な事からその利用が進んでいるが、最大の
問題点は質量数の増加と共にイオンの透過効率が低下し
、測定質量範囲が磁場セクター形に比して制限される点
である。その為現状ではFABイオン源も磁場セクター
との絹合わせで用いられている。換言すれば、FABイ
オン化法を用いて大きい分子を対象として分析しようと
すれば、大形で高価な磁場セクター形の装置を用いねば
ならない。
[Problems to be solved by the invention] Quadruple seed mass spectrometers are being used more and more because they are smaller and cheaper than conventional magnetic field sector mass spectrometers, but the biggest problem is that As the ion transmission efficiency increases, the ion transmission efficiency decreases, and the measurement mass range is limited compared to the magnetic field sector type. Therefore, at present, FAB ion sources are also used in combination with magnetic field sectors. In other words, if a large molecule is to be analyzed using the FAB ionization method, a large and expensive magnetic field sector type device must be used.

本発明の目的は上記背景に鑑み、FABイオン源と四重
極形質量分析装置の組合わせでもって充分な実用性能を
発揮する小形・低価格な質量分析装置を提供する事にあ
る。
In view of the above background, an object of the present invention is to provide a compact, low-cost mass spectrometer that exhibits sufficient practical performance by combining an FAB ion source and a quadrupole mass spectrometer.

〔問題点を解決するための手段] 四重極形質量分析装置では、通常四重極電極に直流(d
c)電圧と高周波(rf)電圧を重畳させた電圧を印加
し、この両者の比(Vdc/Vrf比)を一定に保持し
た状態で電圧を走査する事により質量スペクトルを測定
するものである。本発明の特徴は、この通常の測定モー
ドの他に、高周波電圧のみを走査する測定モードに切替
えを行う事で、イオン透過効率の低下のない測定を可能
にし、FABイオン源で生成した高質量イオンを効率良
く測定できるようにした装置構成方法にある。
[Means for solving the problem] In quadrupole mass spectrometers, direct current (d
c) A mass spectrum is measured by applying a voltage that is a superimposed voltage and a radio frequency (RF) voltage, and scanning the voltage while keeping the ratio of both (Vdc/Vrf ratio) constant. A feature of the present invention is that in addition to this normal measurement mode, switching to a measurement mode that scans only high-frequency voltage enables measurement without deterioration of ion transmission efficiency. The method of configuring the device enables efficient measurement of ions.

〔発明の実施例〕[Embodiments of the invention]

以下本発明の実施例を第1図〜第5図により説明する。 Embodiments of the present invention will be described below with reference to FIGS. 1 to 5.

先ず第1図は四重極形質量分析装置の動作原理に関する
特性線図で、一般に安定線図と呼ばれている。四重極電
極の中心軸に沿って入射したイオンは高周波電場により
振動しながら軸方向に進行するが、特定の条件を満足す
るイオンのみが安定振動となり、四重極部を通過し、検
出器に到達する。それ以外のイオンは不安定振動となり
途中で電極に衝突し、失われる。図の斜線の部分が安定
振動条件を満足する領域に相当する。図中のa/q=−
定の直線は動作線と呼ばれ、Vdc/Vrfの比を一定
に保持しながら電圧を走査するとa+Qはこの動作線上
を動き、この直線が安定領域に入っている間のみ質ff
1Mのイオンが検出される。この場合ここて、Vrf:
高周波電圧(V) 、 r :四重極電極の内接円半径
(m) 、 f :周波数(H2)rは装置により決ま
る定数であり、fを一定とすれば、MはVrfに比例す
るので、この電圧走査により質量スペクトルを測定する
事ができ゛る。以上は四重極質量分析装置の通常測定モ
ードであり、イオン質量に対するバンドパス・ブイ11
夕として働く。これに対して、本発明の要点である高周
波電圧のみによる電圧走査ではバイパス・フィルタとし
て働き、その臨界質量は次式で与えられる。
First, FIG. 1 is a characteristic diagram relating to the operating principle of a quadrupole mass spectrometer, and is generally called a stability diagram. Ions incident along the central axis of the quadrupole electrode travel in the axial direction while vibrating due to the high-frequency electric field, but only ions that satisfy certain conditions become stable vibrations, pass through the quadrupole part, and are detected by the detector. reach. Other ions become unstable vibrations and collide with the electrodes on the way and are lost. The shaded area in the figure corresponds to the area that satisfies the stable vibration conditions. a/q=- in the figure
A constant straight line is called an operating line, and when the voltage is scanned while keeping the ratio of Vdc/Vrf constant, a+Q moves on this operating line, and only while this straight line is in the stable region, the quality ff
1M ions are detected. In this case, Vrf:
High frequency voltage (V), r: Radius of inscribed circle of quadrupole electrode (m), f: Frequency (H2) r is a constant determined by the device, and if f is constant, M is proportional to Vrf, so , mass spectra can be measured by this voltage scanning. The above is the normal measurement mode of the quadrupole mass spectrometer, and the bandpass buoy 11 for ion mass
Work as a night. On the other hand, in voltage scanning using only high-frequency voltage, which is the main point of the present invention, it functions as a bypass filter, and its critical mass is given by the following equation.

Mcutoff=0.77 ・M 第2図はその特性を示したもので、Mcutoff以上
の質量数のイオンは聡で四重極電極部を通過し検出され
るので、通常モードにおける高質量になる程透過効率が
低下する現象いわゆるmass−d 1scr 11n
inationは問題とならず、高質量イオンも効率良
く検出する事ができる第3図は高周波電圧のみを走査し
た場合の検出イオン信号を示すもので、Mに対するイオ
ン信号の変化は、図の(a)に見るような階段状の応答
、いわゆる積分曲線となる。
Mcutoff=0.77 ・M Figure 2 shows its characteristics. Ions with a mass number greater than Mcutoff pass through the quadrupole electrode section and are detected, so the higher the mass in normal mode, the higher the Phenomenon where transmission efficiency decreases, so-called mass-d 1scr 11n
ion is not a problem, and even high-mass ions can be detected efficiently. Figure 3 shows the detected ion signal when only the high-frequency voltage is scanned. The change in the ion signal with respect to M is shown in (a) of the figure ), resulting in a step-like response, a so-called integral curve.

図の(b)は微分回路により得られる微分曲線であり、
 マススペクトル ζこ対応する。
(b) in the figure is a differential curve obtained by a differential circuit,
Corresponds to the mass spectrum ζ.

次に第4図に本発明の一実施例の装置構成を示す。1は
高速中性原子イオン源であり、測定試料は8の直接試料
導入部からイオン源内に導入される。イオン源部の構造
略図を示したのが第5図である。11は高速中性原子ビ
ームガンである。通常キセノンガスを用いてイオンガン
でキセノンイオンを生成し、このイオンビームを同種ガ
スを送入したガスチャンバーへ導入すると電荷交換反応
により生じる高速キセノン原子ビームを試料を塗付した
ターゲットに衡撃させて試料をイオン化するものである
。12は通常の電子衡撃イオン源又13は生成したイオ
ンビームを収束する為のイオンレンズ部である。イオン
レンズの右側に四重極電極が設けられる(図示せず)。
Next, FIG. 4 shows the configuration of an apparatus according to an embodiment of the present invention. 1 is a fast neutral atom ion source, and a measurement sample is introduced into the ion source from a direct sample introduction section 8. FIG. 5 shows a schematic structural diagram of the ion source section. 11 is a fast neutral atom beam gun. Normally, xenon ions are generated using an ion gun using xenon gas, and when this ion beam is introduced into a gas chamber containing the same type of gas, a high-speed xenon atomic beam generated by a charge exchange reaction is made to strike the target coated with the sample. It ionizes the sample. Reference numeral 12 designates an ordinary electron striking ion source, and reference numeral 13 designates an ion lens section for converging the generated ion beam. A quadrupole electrode is provided to the right of the ion lens (not shown).

14は試料導入プローブでありその先端にターゲットが
取付けられている。試料導入プローブは直接試料導入装
置1を用いて挿入される。第4図の2は四重極形質量分
析部、3はイオン検出器である。4はイオン信号の増幅
測定回路及び微分回路である。5は制御部であり、真空
排気系の制御、加熱制御、モード切替え、分析条件制御
等を行う。6は四重極電極に印加する直流及び高周波電
圧電源部である。7はコンピューター・システムで、デ
ータ処理及び装置操作を行う。本装置構成でもって直流
電圧と高周波電圧を共に走査する通常モードと高周波電
圧のみを走査するモードを任意に切替えて質量分析を行
う事ができる。従って、揮発性試料の分析に対しては通
常の電子衡撃イオン源と通常モードによる四重極形質量
分析装置により分析を行い、難揮発性あるいは熱不安定
性試料に対してはFA8イオン源と高周波電圧のみを走
査するモードによる四正極質量分析装置により分析を行
う事ができ、従来、四重極形質量分析装置の質量制限に
より困難であったFABイオン源ど四重極質量分析装置
の紹合わせによっても実用上充分な性能を得る事ができ
る。
14 is a sample introduction probe, and a target is attached to its tip. The sample introduction probe is directly inserted using the sample introduction device 1. 2 in FIG. 4 is a quadrupole mass spectrometer, and 3 is an ion detector. 4 is an ion signal amplification measurement circuit and a differentiation circuit. Reference numeral 5 denotes a control section, which controls the evacuation system, heating control, mode switching, analysis condition control, etc. 6 is a direct current and high frequency voltage power supply section that applies to the quadrupole electrodes. 7 is a computer system that performs data processing and equipment operation. With this device configuration, mass spectrometry can be performed by arbitrarily switching between a normal mode in which both DC voltage and high-frequency voltage are scanned, and a mode in which only high-frequency voltage is scanned. Therefore, volatile samples are analyzed using a normal electron equilibrium ion source and a quadrupole mass spectrometer in normal mode, while non-volatile or thermally unstable samples are analyzed using an FA8 ion source. Introduction to quadrupole mass spectrometers such as the FAB ion source, which can perform analysis using a quadrupole mass spectrometer in a mode that scans only high-frequency voltage, which was previously difficult due to mass limitations of quadrupole mass spectrometers. Practically sufficient performance can also be obtained by combining them.

本実施例は質量分析装置への適用例を説明したが、勿論
、ガスクロマトグラフ質量分析装置にも容易に適用可能
である。
Although this embodiment describes an example of application to a mass spectrometer, it is of course easily applicable to a gas chromatograph mass spectrometer.

〔発明の効果〕〔Effect of the invention〕

本発明により難揮発性あるいは熱的不安定性試料を対象
としてFARイオン源を用いた質量分析を小形で低価格
な四重極形質量分析装置で行う事ができる。
According to the present invention, mass spectrometry using a FAR ion source can be performed on non-volatile or thermally unstable samples using a small and inexpensive quadrupole mass spectrometer.

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

第1図、第2図は本発明の原理説明図、第3図は本発明
によるマススペクトI#測定説明図、第4図、第5図は
本発明実施例である装置構成図である。 ■、・・・FABイオン源、2.・・・四重様質量分析
部、3゜・・・イオン検出器、4.・・・イオン信号測
定回路部、5.・・・制御部、6.・・・高圧電源部、
7.・・・コンピューター・E/スyム、8.・・・直
接試料導入部11.・・・高速中性原子銃、12.・・
・ 電子衡撃イオン源、13.・・・イオン収束レンズ
部 14、・・・試料導入プローブ し13;、;i士
FIGS. 1 and 2 are diagrams explaining the principle of the present invention, FIG. 3 is a diagram explaining mass spectrum I# measurement according to the present invention, and FIGS. 4 and 5 are diagrams showing the configuration of an apparatus that is an embodiment of the present invention. ■,...FAB ion source, 2. ... Quadruple-like mass spectrometer, 3゜... Ion detector, 4. ...Ion signal measurement circuit section, 5. ...control unit, 6. ...High voltage power supply section,
7. ...Computer E/Sym, 8. ...Direct sample introduction section 11. ...high-speed neutral atomic gun, 12.・・・
- Electron bombardment ion source, 13. . . . ion focusing lens section 14, . . . sample introduction probe 13;

Claims (1)

【特許請求の範囲】[Claims] 1、高速中性原子衡撃イオン源を装着した四重極形質量
分析装置において、四重極部に直流電圧と高周波電圧を
重畳して印加するモードと高周波電圧のみを印加するモ
ードとの切り替え機構を備えた事を特徴とする質量分析
装置
1. In a quadrupole mass spectrometer equipped with a fast neutral bombardment ion source, switching between a mode in which DC voltage and high-frequency voltage are applied in a superimposed manner to the quadrupole section and a mode in which only high-frequency voltage is applied A mass spectrometer characterized by having a mechanism
JP62294660A 1987-11-20 1987-11-20 Mass spectrometer Pending JPH01137553A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62294660A JPH01137553A (en) 1987-11-20 1987-11-20 Mass spectrometer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62294660A JPH01137553A (en) 1987-11-20 1987-11-20 Mass spectrometer

Publications (1)

Publication Number Publication Date
JPH01137553A true JPH01137553A (en) 1989-05-30

Family

ID=17810646

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62294660A Pending JPH01137553A (en) 1987-11-20 1987-11-20 Mass spectrometer

Country Status (1)

Country Link
JP (1) JPH01137553A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6956205B2 (en) 2001-06-15 2005-10-18 Bruker Daltonics, Inc. Means and method for guiding ions in a mass spectrometer
JP2008130469A (en) * 2006-11-24 2008-06-05 Hitachi High-Technologies Corp Mass spectrometer and mass spectrometry

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6956205B2 (en) 2001-06-15 2005-10-18 Bruker Daltonics, Inc. Means and method for guiding ions in a mass spectrometer
JP2008130469A (en) * 2006-11-24 2008-06-05 Hitachi High-Technologies Corp Mass spectrometer and mass spectrometry

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