JPS6073447A - Light element fluorescent x-ray spectroscope - Google Patents

Light element fluorescent x-ray spectroscope

Info

Publication number
JPS6073447A
JPS6073447A JP58184132A JP18413283A JPS6073447A JP S6073447 A JPS6073447 A JP S6073447A JP 58184132 A JP58184132 A JP 58184132A JP 18413283 A JP18413283 A JP 18413283A JP S6073447 A JPS6073447 A JP S6073447A
Authority
JP
Japan
Prior art keywords
rays
fluorescent
secondary electrons
magnetic field
detector
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
JP58184132A
Other languages
Japanese (ja)
Inventor
Hiroshi Tsunoda
浩 角田
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
Shimazu Seisakusho KK
Original Assignee
Shimadzu Corp
Shimazu Seisakusho KK
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, Shimazu Seisakusho KK filed Critical Shimadzu Corp
Priority to JP58184132A priority Critical patent/JPS6073447A/en
Publication of JPS6073447A publication Critical patent/JPS6073447A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/22Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material
    • G01N23/223Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by measuring secondary emission from the material by irradiating the sample with X-rays or gamma-rays and by measuring X-ray fluorescence
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N2223/00Investigating materials by wave or particle radiation
    • G01N2223/07Investigating materials by wave or particle radiation secondary emission
    • G01N2223/076X-ray fluorescence

Landscapes

  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Analysing Materials By The Use Of Radiation (AREA)

Abstract

PURPOSE:To remove secondary electrons and to improve S/N of a detection signal and the accuracy of analysis with a fluorescent X-ray spectroscope in which total reflection mirrors are used as a spectroscopic means and fluorescent X-rays of the wavelength having a specific value or above are totally reflected by impressing a magnetic field roughly perpendicularly to the fluorescent X-rays incident on the mirrors. CONSTITUTION:Secondary electrons in addition to fluorescent X-rays are generated from a sample excited by X-rays. Since the incident angle of the fluorescent X-rays to mirrors 4 is low, the angle at which the route of the fluorescent X-rays are bent in the midway is small and therefore the probability that the secondary electrons past slits 3 enter a detector 5 is extremely high. Magnetic poles 8, 9 are for shutting off these secondary electrons and generate the magnetic field crossing roughly perpendicularly with the route for the fluorescent X-rays by a U-shaped permanent magnet or electromagnet 10. The magnetic field bends the route for ahe secondary electrons withdout affecting the fluorescent X-rays thereby separating the secondary electrons from the fluorescent X- rays and preventing the secondary electrons from entering the detector 5.

Description

【発明の詳細な説明】 イ)産業上の利用分野 本発明は炭素のような軽元素の分析を行うためのけい光
X線分光器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION A) Field of Industrial Application The present invention relates to a fluorescence X-ray spectrometer for analyzing light elements such as carbon.

(ロ) 従来技術 一般に軽元素をけい光X線を用いて分析する場合はけい
光X線の波長が長いから、試料から出だけい光X線を低
角度でミラーに入射させることによシ、所定の波長以上
のけい光X線を全反射させて分光し、これを検出する方
法がとられる。しかしこの方式は真空中で実施される上
けい光X線が途中で曲げられる角度が小さいために、試
料から出だ二次電子がX線検出器まで到達し易く、これ
がバックグラウンドノイズとして検出されるだめに検出
信号のS / N比が低下するという欠点があった。
(b) Conventional technology Generally, when light elements are analyzed using fluorescent X-rays, since the wavelength of fluorescent X-rays is long, the fluorescent X-rays emitted from the sample are incident on a mirror at a low angle. , a method is used in which fluorescent X-rays of a predetermined wavelength or more are totally reflected, separated into spectra, and detected. However, with this method, the upper fluorescence X-rays are bent in a vacuum and the angle at which they are bent is small, making it easy for secondary electrons emitted from the sample to reach the X-ray detector, which is detected as background noise. However, this method has the disadvantage that the S/N ratio of the detection signal decreases.

(ハ) 目 的 本発明は上記のノイズを取り除いて検出信号のS / 
N比を向上し、軽元素けい光X線分光器の分析精度を高
めることを目的とするものである。
(c) Purpose The present invention removes the above noise and improves the S/S of the detection signal.
The purpose is to improve the N ratio and the analytical accuracy of the light element fluorescence X-ray spectrometer.

(ニ)構 成 本発明は、分光手段として全反射ミラーを使用し波長が
一定値以上のけい光X綜を全反射するようにしたけい光
X線分光器において、ミラーに入射するけい光X線にほ
ぼ直角に磁界を印加することにより、二次電子を除去す
るようにしたものである。
(D) Structure The present invention provides a fluorescent X-ray spectrometer that uses a total reflection mirror as a spectroscopic means to totally reflect fluorescent X-rays having a wavelength of a certain value or more, in which the fluorescent X-rays incident on the mirror are The secondary electrons are removed by applying a magnetic field almost perpendicular to the .

(ホ)実施例 図は本発明の一実施例を示しだものである。図において
、1は励起用X線を発生するX線源であシ、X線を照射
された試料2はけい光X線を発生する。3はスリットで
あシ、このスリット3を通過したけい光X線が所定角度
でミラー4に入射するような位置に配置されている。例
えば炭素を分析する場合に炭素より重い元素の特性X線
はミラー3で反射されずに吸収され、炭素および炭素よ
シ軽い元素の特性X線のみが全反射されて検出器5に入
射するようになっている。6は検出器の前面に設けられ
たスリットである。7は炭素よシも軽い元素すなわち所
定の波長よりも大きい波長のけい光X線を遮断するだめ
のフィルタである。
(e) Embodiment The figure shows one embodiment of the present invention. In the figure, 1 is an X-ray source that generates excitation X-rays, and a sample 2 irradiated with X-rays generates fluorescent X-rays. Reference numeral 3 denotes a slit, which is arranged at a position such that fluorescent X-rays passing through the slit 3 are incident on a mirror 4 at a predetermined angle. For example, when analyzing carbon, the characteristic X-rays of elements heavier than carbon are absorbed by the mirror 3 without being reflected, and only the characteristic X-rays of carbon and elements lighter than carbon are totally reflected and incident on the detector 5. It has become. 6 is a slit provided in the front of the detector. Reference numeral 7 denotes a filter for blocking elements lighter than carbon, that is, fluorescent X-rays having a wavelength larger than a predetermined wavelength.

X線によって励起された試料2からはけい光X線の他に
二次電子も発生している。けい光X線のミラー4への入
射角が低角度であるために、けい光X線の経路が途中で
曲げられる角度は小さく、しだがってスリット3を通っ
た二次電子が検出器5に入射する確率がきわめて高い。
In addition to fluorescent X-rays, secondary electrons are also generated from the sample 2 excited by the X-rays. Since the angle of incidence of the fluorescent X-rays on the mirror 4 is low, the angle at which the path of the fluorescent X-rays is bent midway is small, so that the secondary electrons that have passed through the slit 3 reach the detector 5. There is a very high probability that it will be incident on the

磁極8,9はこれらの二次電子を遮断するだめのもので
、U字形の永久磁石または電磁石10によって、けい光
X線の経路にほぼ直角に鎖交する磁界を発生させる。こ
の磁界はけい光X線には影響を与えずに二次電子の経路
を曲げることによって、二次電子をけい光X線から分離
し、二次電子が検出器5に入射するのを阻止するのであ
る。
The magnetic poles 8 and 9 are used to block these secondary electrons, and a U-shaped permanent magnet or electromagnet 10 generates a magnetic field that intersects approximately perpendicularly to the path of the fluorescent X-rays. This magnetic field bends the path of the secondary electrons without affecting the fluorescence X-rays, thereby separating the secondary electrons from the fluorescence X-rays and preventing the secondary electrons from entering the detector 5. It is.

(へ)効 果 本発明による軽元素けい光X線分光器は上述のように、
全反射ミラーによってけい光X線を分光する方式におい
て、ミラーに入射するけい光X線にその入射方角とほぼ
直角な磁界を印加するようにしたので、けい光X線と共
にスリットを通過した二次電子を、けい光X線の経路に
影響を与えることなく簡単に除去することができ、従来
けい光X線と共に検出器に入射した二次電子によって発
生していたバックグラウンドノイズを取シ除くことによ
って、検出信号のS / N比を向上し得るという利点
がある。
(f) Effects As mentioned above, the light element fluorescence X-ray spectrometer according to the present invention has the following effects:
In the method of dispersing fluorescent X-rays using a total reflection mirror, a magnetic field is applied to the fluorescent X-rays incident on the mirror at a nearly right angle to the direction of incidence, so that the secondary radiation passing through the slit along with the fluorescent X-rays Electrons can be easily removed without affecting the path of fluorescence X-rays, and the background noise that was conventionally generated by secondary electrons that entered the detector along with fluorescence X-rays can be removed. This has the advantage that the S/N ratio of the detection signal can be improved.

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

図は本発明軽元素けい光線分光器の一実施例を示す概略
斜視図である。 l・・・X線源、2・・・試料、3・・・スリット、4
・・・ミラー、5・・・検出器、6・・・検出器用スリ
ット、フ・・・フィルタ、8,9・・・磁極、10・・
・永久磁石または電磁石。 代理人 弁理± 11系 浩 介
The figure is a schematic perspective view showing an embodiment of the light element fluorescence spectrometer of the present invention. l...X-ray source, 2...sample, 3...slit, 4
...Mirror, 5...Detector, 6...Slit for detector, filter, 8,9...Magnetic pole, 10...
・Permanent magnet or electromagnet. Agent Patent Attorney ± 11 series Kosuke

Claims (1)

【特許請求の範囲】[Claims] 試料を励起するX線源と、試料から出たけい光X線を通
過させるスリットと、スリットを通過したけい光X線の
うち所定の波長域のけい光X線を全反射させるミラーと
、全反射されたけい・光X線を検出する検出器とを具え
たけい光X線分光器において、上記ミラーに入射するけ
い光X線にその入射方向とほぼ直角な磁界を印加する磁
極を設けることによシ、試料から出た二次電子を除去す
るようにして成る軽元素けい光X線分光器。
An X-ray source that excites the sample, a slit that passes the fluorescent X-rays emitted from the sample, a mirror that totally reflects the fluorescent X-rays in a predetermined wavelength range among the fluorescent X-rays that have passed through the slit, and In a fluorescence X-ray spectrometer equipped with a detector for detecting reflected fluorescence/optical X-rays, a magnetic pole is provided to apply a magnetic field substantially perpendicular to the direction of incidence of the fluorescence X-rays incident on the mirror. A light element fluorescence X-ray spectrometer that removes secondary electrons emitted from a sample.
JP58184132A 1983-09-30 1983-09-30 Light element fluorescent x-ray spectroscope Pending JPS6073447A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58184132A JPS6073447A (en) 1983-09-30 1983-09-30 Light element fluorescent x-ray spectroscope

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58184132A JPS6073447A (en) 1983-09-30 1983-09-30 Light element fluorescent x-ray spectroscope

Publications (1)

Publication Number Publication Date
JPS6073447A true JPS6073447A (en) 1985-04-25

Family

ID=16147931

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58184132A Pending JPS6073447A (en) 1983-09-30 1983-09-30 Light element fluorescent x-ray spectroscope

Country Status (1)

Country Link
JP (1) JPS6073447A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6355199U (en) * 1986-09-29 1988-04-13
JP2022085853A (en) * 2020-11-27 2022-06-08 日本電子株式会社 X-ray detector and method
US11699567B2 (en) 2020-11-27 2023-07-11 Jeol Ltd. X-ray detection apparatus and method

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6355199U (en) * 1986-09-29 1988-04-13
JP2022085853A (en) * 2020-11-27 2022-06-08 日本電子株式会社 X-ray detector and method
US11699567B2 (en) 2020-11-27 2023-07-11 Jeol Ltd. X-ray detection apparatus and method

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