JPH02168548A - Charged particle beam irradiation type X-ray analyzer - Google Patents

Charged particle beam irradiation type X-ray analyzer

Info

Publication number
JPH02168548A
JPH02168548A JP63322915A JP32291588A JPH02168548A JP H02168548 A JPH02168548 A JP H02168548A JP 63322915 A JP63322915 A JP 63322915A JP 32291588 A JP32291588 A JP 32291588A JP H02168548 A JPH02168548 A JP H02168548A
Authority
JP
Japan
Prior art keywords
ray
charged particle
particle beam
hole
sample
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
JP63322915A
Other languages
Japanese (ja)
Inventor
Shigeki Hayashi
茂樹 林
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 JP63322915A priority Critical patent/JPH02168548A/en
Publication of JPH02168548A publication Critical patent/JPH02168548A/en
Pending legal-status Critical Current

Links

Landscapes

  • Analysing Materials By The Use Of Radiation (AREA)

Abstract

PURPOSE:To make measurement with good S/N ratio by arranging the X-ray incident surface of a sensing element, wherein a through hole is provided in the center of the X-ray incident surface, so as to face the specimen surface, and permitting a charged particle beam to penetrate this through hole. CONSTITUTION:A charged particle beam BB penetrates a through hole (h) provided in the center of a disc-shaped semiconductor X-ray sensing element D. X-ray emitted from a specimen S is irradiated onto the sensing element D, which generates panel current with an intensity proportional to the energy for the incident X-ray light quantum. The pulse current signal is amplified by a preamplifier PA and a proportional amplifier LA, and the pulse signals in a wave height range corresponding to the energy of characteristic X-ray to be measured are taken out and counted by a counter C. This constitution enables approach of the X-ray sensing surface to the specimen surface, allows easy enlargement of the stereophonic angle formed by the specimen surface with respect to the beam irradiation point O, accomplishes good X-ray incident efficiency, and enchances the analytical sensitivity and the accuracy.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明はXMマイクロアリ−ライザのような荷電粒子(
電子、イオン)ビームで試料を照射し、試料から放射さ
れるX線を分光して試料の元素分析とか構造解析を行う
X線分析装置のX!l!i1分光検出手段に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention is directed to the application of charged particles (
The X! l! This invention relates to i1 spectral detection means.

(従来の技術) 上述したような分析装置においてはX線分光法として分
光結晶を用いる波長分散方式或は入射X線の光子エネル
ギーに比例した波高のパルスを出力する比例計数管或は
半導体検出器を用いるエネルギー分散方式が用いられて
いるが、従来は何れの方式による場合ではも、X線分光
検出手段は試料照射ビームとは異る方向から試料のビー
ム照射点を望むように設置されていた。
(Prior art) In the above-mentioned analysis device, X-ray spectroscopy uses a wavelength dispersion method using a spectroscopic crystal, or a proportional counter or semiconductor detector that outputs a pulse with a wave height proportional to the photon energy of incident X-rays. An energy dispersive method is used, but conventionally, with either method, the X-ray spectroscopic detection means was installed so that it looked at the beam irradiation point on the sample from a direction different from the sample irradiation beam. .

このような従来のX線分光検出手段は試料のビーム照射
点から離れていて、試料のビーム照射点に対して張る立
体角が小さくそのためX線の入射効率が低くなっており
、また試料から放射される特性X線を測定する場合バッ
クグラウンドとなる試料照射粒子の制動輻射による連続
X線強度に対する特性X線の強度の比は照射ビームの照
射方向と反対方向で最大であり、垂直から離れるに従い
小さくなるが、従来方法ではこの照射ビームからかなり
離れた方向でX線を検出しているので、測定のS/N比
が低くなっていた。
Such conventional X-ray spectroscopy detection means are located far from the beam irradiation point on the sample, and the solid angle with respect to the sample beam irradiation point is small, resulting in low X-ray incidence efficiency, and the radiation from the sample is small. When measuring characteristic X-rays, the ratio of the intensity of the characteristic X-rays to the continuous X-ray intensity due to the bremsstrahlung radiation of sample irradiation particles, which serves as the background, is maximum in the direction opposite to the irradiation direction of the irradiation beam, and increases as the distance from the vertical direction increases. However, in the conventional method, X-rays are detected in a direction far away from this irradiation beam, resulting in a low measurement S/N ratio.

(発明が解決しようとする課題) 本発明は荷電粒子ビームで試料面を照射し、試料から放
射されるX線を分光検出する装置において、X線の入射
効率を高め、S/N比の良好ならしめたX線の分光検出
装置を提供しようとするものである。
(Problems to be Solved by the Invention) The present invention improves the incidence efficiency of X-rays and improves the S/N ratio in a device that irradiates a sample surface with a charged particle beam and spectrally detects the X-rays emitted from the sample. The present invention aims to provide a standardized X-ray spectroscopic detection device.

(課題を解決するための手段) X線入射面の中央に透孔を有するX線検出素子を試料を
照射する荷電粒子ビームが上記透孔を通過するようにし
、X線入射面を試料面に向けて配置した。
(Means for Solving the Problem) An X-ray detection element having a through hole in the center of the X-ray entrance surface is arranged so that the charged particle beam that irradiates the sample passes through the hole, and the X-ray entrance surface is made to face the sample surface. It was placed towards.

(作用) 本発明によればX線検出素子は試料を照射する荷電粒子
ビームを囲んで配置され、X線入射面を試料に向けてい
るから、試料面からのX線取出し角は90°に近(、従
ってS/N比の良い特性X線検出ができ、従来のように
斜めから試料を望むのに比し、X線検出素子の配直に構
造的な制約が少(、X線入射面の試料のビーム照射点に
対して張る立体角を従来より容易に大きくできて、X線
入射効率が高められる。
(Function) According to the present invention, the X-ray detection element is arranged surrounding the charged particle beam that irradiates the sample, and the X-ray incident surface is directed toward the sample, so the X-ray extraction angle from the sample surface is 90°. Therefore, characteristic X-rays can be detected with a good S/N ratio, and there are fewer structural restrictions on the arrangement of the The solid angle formed with respect to the beam irradiation point of the sample on the surface can be made larger than before, and the X-ray incidence efficiency can be increased.

(実施例) 図は本発明の一実施例装置を示す。図でBは試料を照射
する荷電粒子ビーム、Lは対物レンズでSは試料である
。Dが本発明に係るX線検出素子で円板状に形成された
半導体X線検出素子であり、中央に透孔りが設けられて
いて荷電粒子ビームBが通過するようになっている。試
料から放射されるX線は図に矢印Xで示すようにX線検
出素子りに入射する。半導体X線検出素子では入射した
X線光子に対し、そのエネルギーに比例した強さのパル
ス電流を発生する。このパルス電流信号はプリアンプP
A比例アンプLAで増幅された後、波高分析器PICA
により測定しようとする特11X線のエネルギーに相当
する波高範囲のパルス信号が取出されてカウンタCによ
り計数される。
(Embodiment) The figure shows an apparatus according to an embodiment of the present invention. In the figure, B is the charged particle beam that irradiates the sample, L is the objective lens, and S is the sample. D is an X-ray detection element according to the present invention, which is a semiconductor X-ray detection element formed in a disk shape, and has a hole in the center so that the charged particle beam B can pass through. X-rays emitted from the sample enter the X-ray detection element as shown by arrows X in the figure. In response to incident X-ray photons, a semiconductor X-ray detection element generates a pulse current whose strength is proportional to the energy of the incident X-ray photons. This pulse current signal is the preamplifier P
After being amplified by the A proportional amplifier LA, the pulse height analyzer PICA
A pulse signal having a wave height range corresponding to the energy of the X-ray to be measured is extracted and counted by a counter C.

(発明の効果) 従来のこの種装置では図で鎖線で示すような方向にX線
を取出していたが、本発明では図から明らかなように試
料照射ビームの入射方向と反対方向に放射されるX線を
検出するので、連8% X Mバックグラウンドに対す
る試料の特性X線強度の比が従来例より高くなり、S/
N比の良好な測定ができ、xvA検出素子は試料照射ビ
ームを囲んで、同ビームに近接して配置されるので、X
線検出素子の配置についての構造的制約が少く、X線検
出面を試料面に近付づけ、試料面のビーム照射点Oに対
して張る立体角を容易に大きくすることが太き(するこ
とができるからX線入射効率が良く、従来より分析感度
9分析器度が向」二し、しかも構造的に簡単なものとな
る。
(Effects of the Invention) Conventional devices of this type emit X-rays in the direction shown by the chain line in the figure, but in the present invention, as is clear from the figure, the X-rays are emitted in the opposite direction to the incident direction of the sample irradiation beam. Since X-rays are detected, the ratio of the characteristic X-ray intensity of the sample to the background is higher than that of the conventional example, and S/
Good N-ratio measurements can be made, and since the xvA detection element is placed surrounding the sample irradiation beam and close to it,
There are few structural restrictions on the arrangement of the radiation detection element, and it is possible to bring the X-ray detection surface closer to the sample surface and easily increase the solid angle with respect to the beam irradiation point O on the sample surface. Because of this, the X-ray incidence efficiency is good, the analytical sensitivity is 9.2 times higher than that of the conventional analyzer, and the structure is simpler.

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

図面は本発明の一実施例装置の側面図である。 B・・・荷電粒子ビーム、L・・・対物レンズ、S・・
・試料、D・・・X線検出器、h・・・透孔、PHA・
・・波高分析器、C・・・カウンタ。 代理人  弁理士 縣  浩 介
The drawing is a side view of an apparatus according to an embodiment of the present invention. B...Charged particle beam, L...Objective lens, S...
・Sample, D...X-ray detector, h...Through hole, PHA・
... Wave height analyzer, C... Counter. Agent Patent Attorney Kosuke Agata

Claims (1)

【特許請求の範囲】[Claims] X線入射面の中央に透孔を有するX線検出素子をそのX
線入射面を試料に向け、試料面を照射する荷電粒子ビー
ムが上記透孔を通過するように配置したことを特徴とす
る荷電粒子ビーム照射型X線分析装置。
An X-ray detection element with a through hole in the center of the X-ray incident surface is
A charged particle beam irradiation type X-ray analyzer characterized in that the ray incidence surface is directed toward the sample and the charged particle beam irradiating the sample surface is arranged so as to pass through the through hole.
JP63322915A 1988-12-20 1988-12-20 Charged particle beam irradiation type X-ray analyzer Pending JPH02168548A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63322915A JPH02168548A (en) 1988-12-20 1988-12-20 Charged particle beam irradiation type X-ray analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63322915A JPH02168548A (en) 1988-12-20 1988-12-20 Charged particle beam irradiation type X-ray analyzer

Publications (1)

Publication Number Publication Date
JPH02168548A true JPH02168548A (en) 1990-06-28

Family

ID=18149048

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63322915A Pending JPH02168548A (en) 1988-12-20 1988-12-20 Charged particle beam irradiation type X-ray analyzer

Country Status (1)

Country Link
JP (1) JPH02168548A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS553129A (en) * 1978-06-21 1980-01-10 Jeol Ltd X-ray analyzer for scanning electron microscope or the like
JPS6136955B2 (en) * 1978-02-28 1986-08-21 Yaskawa Denki Seisakusho Kk

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6136955B2 (en) * 1978-02-28 1986-08-21 Yaskawa Denki Seisakusho Kk
JPS553129A (en) * 1978-06-21 1980-01-10 Jeol Ltd X-ray analyzer for scanning electron microscope or the like

Similar Documents

Publication Publication Date Title
Chance Rapid and sensitive spectrophotometry. III. A double beam apparatus
US6108398A (en) X-ray microfluorescence analyzer
US7583788B2 (en) Measuring device for the shortwavelength x ray diffraction and a method thereof
CN107462566B (en) Raman spectrometer for detecting specific narrow wavenumber range
US3936638A (en) Radiology
US3562525A (en) X-ray fludrescence gauging employing a single x-ray source and a reference sample for comparative measurements
JP3511826B2 (en) X-ray fluorescence analyzer
CN100473981C (en) X-ray absorption spectrum detector for chemical valence state research and method thereof
JP2002189004A (en) X-ray analyzer
Belogurov et al. CsI (Tl) infrared scintillation light yield and spectrum
JPH02168548A (en) Charged particle beam irradiation type X-ray analyzer
US7321652B2 (en) Multi-detector EDXRD
US3376415A (en) X-ray spectrometer with means to vary the spacing of the atomic planes in the analyzing piezoelectric crystal
JPH0263180B2 (en)
CN110044938A (en) A kind of uranium concentration measuring device of spentnuclear fuel extract liquor
US4171912A (en) Element analyzer exploiting a magneto-optic effect
CN119413415B (en) Scintillation optical fiber performance test system and method
USH922H (en) Method for analyzing materials using x-ray fluorescence
JP2799994B2 (en) X-ray detector
CN109187369A (en) A kind of oil plant detection device and detection method applying associated detection technique
JPH05296947A (en) Electron diffraction analyzer
JPS62226048A (en) Spectrochemical analysis of crystal solid
JP2880381B2 (en) X-ray fluorescence analyzer
SU1276960A1 (en) Method of measuring size and concentration of aerosol particles
JPH01141344A (en) Fluorescent x-ray analyzer