JPH02304400A - X-ray spectroscopic device - Google Patents
X-ray spectroscopic deviceInfo
- Publication number
- JPH02304400A JPH02304400A JP1124894A JP12489489A JPH02304400A JP H02304400 A JPH02304400 A JP H02304400A JP 1124894 A JP1124894 A JP 1124894A JP 12489489 A JP12489489 A JP 12489489A JP H02304400 A JPH02304400 A JP H02304400A
- Authority
- JP
- Japan
- Prior art keywords
- ray
- crystal
- measurement
- rays
- spectral crystal
- 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
Links
- 239000013078 crystal Substances 0.000 claims abstract description 35
- 238000005259 measurement Methods 0.000 claims abstract description 17
- 238000000441 X-ray spectroscopy Methods 0.000 claims abstract description 5
- 238000010894 electron beam technology Methods 0.000 abstract description 4
- 238000004611 spectroscopical analysis Methods 0.000 abstract description 4
- 230000003595 spectral effect Effects 0.000 abstract 5
- 230000001678 irradiating effect Effects 0.000 abstract 1
- 238000004458 analytical method Methods 0.000 description 1
- 238000012790 confirmation Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
Landscapes
- Analysing Materials By The Use Of Radiation (AREA)
Abstract
Description
【発明の詳細な説明】 (産業上の利用分野) 本発明は分光結晶を用いたX線分光装置に関する。[Detailed description of the invention] (Industrial application field) The present invention relates to an X-ray spectrometer using a spectroscopic crystal.
(従来の技術)
分光結晶を用いたX線分光装置は従来、使用時だけ分光
結晶はX線の照射を受けると云う使い方がなされていた
。所が分光結晶はX &’it照射を受けることにより
格子面間隔および反射X線強度が変化して徐々に一定に
近づいて行く。従って測定を開始してから、分光結晶の
変化が落着(までの間は頻繁に分光器の波畏の合せ直し
およびX線検出感度の確認を行わねばならず、大へん面
倒でしかも精度の良い測定を行うのが困難であった。(Prior Art) Conventionally, an X-ray spectrometer using a spectroscopic crystal has been used in such a way that the spectroscopic crystal is irradiated with X-rays only when in use. However, when a spectroscopic crystal is exposed to X&'it irradiation, the lattice spacing and reflected X-ray intensity change and gradually approach a constant value. Therefore, after starting the measurement, until the changes in the spectroscopic crystal settle down, it is necessary to frequently readjust the spectrometer's waveform and check the X-ray detection sensitivity, which is very troublesome and requires high accuracy. It was difficult to make measurements.
(発明が解決しようとする課題)
分光結晶を用いたX線分光装置で毎回測定開始から直ち
に安定した状態で測定を行い得るようにしようとするも
のである
(課題を解決するための手段)
X線分光装置において、X線分光用結晶に常にX線を照
射してお(ようにした。(Problem to be solved by the invention) This is an attempt to enable an X-ray spectrometer using a spectroscopic crystal to perform measurements in a stable state immediately from the start of each measurement (Means for solving the problem) In the ray spectrometer, the crystal for X-ray spectroscopy was constantly irradiated with X-rays.
(作用)
分光結晶を用いたX線分光装置の不安定の原因は前述し
たように分光結晶がX線の照射を受けることにより格子
面間隔が徐々に変化する所にある。従って予め分光結晶
にX線を照射して分光結晶を終着状態まで変化させてお
けば直ちに安定した状態で測定を開始することができる
。X線照射を中断すると分光結晶が元に戻るが、常時X
線を照射しておけば、分光結晶はX線照射による安定状
態に落着いているので、何時でも測定を行うことができ
る。(Function) As described above, the cause of the instability of an X-ray spectrometer using a spectroscopic crystal is that the lattice spacing of the spectroscopic crystal gradually changes when the spectroscopic crystal is irradiated with X-rays. Therefore, if the spectroscopic crystal is irradiated with X-rays in advance to change the spectroscopic crystal to the final state, measurement can be started immediately in a stable state. When X-ray irradiation is interrupted, the spectroscopic crystal returns to its original state, but the
Once irradiated with X-rays, the spectroscopic crystal has settled into a stable state due to the X-ray irradiation, so measurements can be taken at any time.
(実施例)
図面に本発明の一実施例を示す。この実施例はX線マイ
クロアナライザに本発明を適用した例である。図でeは
電子ビームで試料表面に収束せしめられている。Cは分
光結晶で、試料面の電子ビーム照射点を通る固定直線り
に沿って移動するようになっている。DはX線検出器で
、その前面に置かれた分光用スリットDsと一体化され
ており、このスリブ!・が試料Sの電子ビーム照射点と
分光結晶Cの中心を通る一定半径の円周(1コ一ランド
円)上に常に位置しているように分光結晶Cと機構的に
連結されている。GはX線源で上記機構上に取付けられ
ており、分光結晶Cに軟X線を照射している。(Example) An example of the present invention is shown in the drawings. This embodiment is an example in which the present invention is applied to an X-ray microanalyzer. In the figure, e indicates an electron beam focused on the sample surface. C is a spectroscopic crystal that moves along a fixed straight line passing through the electron beam irradiation point on the sample surface. D is an X-ray detector, which is integrated with a spectroscopy slit Ds placed in front of it, and this slit! is mechanically connected to the spectroscopic crystal C so that it is always located on the circumference of a constant radius (one co-land circle) passing through the electron beam irradiation point of the sample S and the center of the spectroscopic crystal C. G is an X-ray source mounted on the above mechanism, and irradiates the spectroscopic crystal C with soft X-rays.
この実施例では上述した機構は、直線りに沿って固定さ
れた分光結晶ガイド1と、このガイドに沿って摺動する
分光結晶台2と台2から一体的に延出された腕3と、同
じく台2に対し回動可能な腕4と、ガイド1および腕4
に一端が枢支され、夫々の他端が互いに連結されたリン
ク6.7と、腕3の端とスリットDsとを結ぶリンクと
よりなっており、X!l!i1検出器りとスリットDs
の一体物は腕4上を摺動可能であり、腕3とリンク8と
は夫々長さがローランド円の半径に等しくしてあり、リ
ンク6.7の結合ビンpを腕3の摺動溝内に摺動させる
ことで分光結晶Cの中心法線が常にローランド円の中心
に向っているようにしである。この構成により、分光結
晶Cを送りねじによってガイド1に沿い移動させること
によって波長走査が行われる。X線源Gは腕3に固定さ
れているので、分光結晶Cとの位置関係は常に一定とな
っている。かつX線源Gは腕3の中心線上よりや\腕4
に近い側に片寄せて取付けである。このようにしておく
と、X線源Gから放射されたX線が分光結晶で反射され
ても検出器とは反対側に反射されるので、測定中のバッ
クグラウンド上昇を低く抑えることができる。X線源G
から放射されるX線は実際のX線分光測定におけるX線
の波長範囲よりも長波長側に選定しである。X線検出器
に比例計数管のようなエネルギー分析機能を有する検出
器を用いることにより、測定時にもX線源Gから放射さ
れているX線によるバックグラウンド上昇は更に低(抑
えられる。測定中はX線源Gの作動を停止させておいて
もよい。In this embodiment, the above-mentioned mechanism includes a spectroscopic crystal guide 1 fixed along a straight line, a spectroscopic crystal stand 2 that slides along this guide, and an arm 3 integrally extended from the stand 2. An arm 4 that is also rotatable with respect to the base 2, a guide 1 and an arm 4
The X! l! i1 detector and slit Ds
The integrated body can slide on the arm 4, and the length of the arm 3 and the link 8 is equal to the radius of the Roland circle, and the connecting pin p of the link 6.7 is inserted into the sliding groove of the arm 3. By sliding it inward, the center normal of the spectroscopic crystal C is always directed toward the center of the Rowland circle. With this configuration, wavelength scanning is performed by moving the spectroscopic crystal C along the guide 1 using the feed screw. Since the X-ray source G is fixed to the arm 3, its positional relationship with the spectroscopic crystal C is always constant. And the X-ray source G is from above the center line of arm 3 or from the center line of arm 4.
It is installed off to the side closest to the By doing so, even if the X-rays emitted from the X-ray source G are reflected by the spectroscopic crystal, they are reflected to the side opposite to the detector, so that background rise during measurement can be suppressed to a low level. X-ray source G
The X-rays emitted from the X-rays are selected to have longer wavelengths than the wavelength range of X-rays in actual X-ray spectrometry. By using a detector with an energy analysis function such as a proportional counter for the X-ray detector, the background increase due to the X-rays emitted from the X-ray source G can be further reduced (suppressed) during measurement. The operation of the X-ray source G may be stopped.
(発明の効果)
本発明によれば、測定前に分光結晶は既にX線照射を受
けていて変化が安定しているので、測定開始後更めで波
長合せや強度確認を繰返す必要がな(、測定操作が簡単
かつ能率的になり、また分光結晶が安定しているので高
精度の測定ができる。(Effects of the Invention) According to the present invention, the spectroscopic crystal has already been irradiated with X-rays before measurement and changes are stable, so there is no need to repeat wavelength alignment and intensity confirmation after the start of measurement. Measurement operations are simple and efficient, and the spectroscopic crystal is stable, allowing highly accurate measurements.
図面は本発明の一実施例装置の側面図である。
e・・・電子ビ、−ム、S・・・試料、C・・・分光結
晶、D・・・X線検出器、Ds・・・分光用スリット、
G・・・X線源。
代理人 弁理士 縣 浩 介
り固定1線The drawing is a side view of an apparatus according to an embodiment of the present invention. e...electronic beam, S...sample, C...spectroscopy crystal, D...X-ray detector, Ds...spectroscopy slit,
G...X-ray source. Agent: Patent Attorney Hiroshi Agata Fixed 1 line
Claims (1)
にしたことを特徴とするX線分光装置。An X-ray spectrometer characterized in that a crystal for X-ray spectroscopy is irradiated with X-rays before measurement.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1124894A JPH02304400A (en) | 1989-05-18 | 1989-05-18 | X-ray spectroscopic device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1124894A JPH02304400A (en) | 1989-05-18 | 1989-05-18 | X-ray spectroscopic device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02304400A true JPH02304400A (en) | 1990-12-18 |
Family
ID=14896738
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1124894A Pending JPH02304400A (en) | 1989-05-18 | 1989-05-18 | X-ray spectroscopic device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02304400A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006337301A (en) * | 2005-06-06 | 2006-12-14 | Shimadzu Corp | X-ray analyzer |
-
1989
- 1989-05-18 JP JP1124894A patent/JPH02304400A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006337301A (en) * | 2005-06-06 | 2006-12-14 | Shimadzu Corp | X-ray analyzer |
JP4639971B2 (en) * | 2005-06-06 | 2011-02-23 | 株式会社島津製作所 | X-ray analyzer |
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