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JPH071241B2 - Method for analyzing composition of object to be measured by X-ray - Google Patents
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JPH071241B2 - Method for analyzing composition of object to be measured by X-ray - Google Patents

Method for analyzing composition of object to be measured by X-ray

Info

Publication number
JPH071241B2
JPH071241B2 JP60082080A JP8208085A JPH071241B2 JP H071241 B2 JPH071241 B2 JP H071241B2 JP 60082080 A JP60082080 A JP 60082080A JP 8208085 A JP8208085 A JP 8208085A JP H071241 B2 JPH071241 B2 JP H071241B2
Authority
JP
Japan
Prior art keywords
ray
measured
transmission line
collimator
energy
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.)
Expired - Lifetime
Application number
JP60082080A
Other languages
Japanese (ja)
Other versions
JPS61240148A (en
Inventor
幸夫 香村
久 小相沢
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.)
Furukawa Electric Co Ltd
Original Assignee
Furukawa Electric Co Ltd
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 Furukawa Electric Co Ltd filed Critical Furukawa Electric Co Ltd
Priority to JP60082080A priority Critical patent/JPH071241B2/en
Publication of JPS61240148A publication Critical patent/JPS61240148A/en
Publication of JPH071241B2 publication Critical patent/JPH071241B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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
    • G01N23/02Investigating 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 transmitting the radiation through the material
    • G01N23/06Investigating 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 transmitting the radiation through the material and measuring the absorption
    • G01N23/083Investigating 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 transmitting the radiation through the material and measuring the absorption the radiation being X-rays

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  • Health & Medical Sciences (AREA)
  • Toxicology (AREA)
  • Physics & Mathematics (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)

Description

【発明の詳細な説明】 『産業上の利用分野』 本考案はX線を利用した非破壊測定手段により被測定物
の組成を分析する方法に関する。
The present invention relates to a method for analyzing the composition of an object to be measured by a nondestructive measuring means utilizing X-rays.

『従来の技術』 X線による非破壊測法は各種の分野で利用されている。"Prior Art" Non-destructive measurement by X-ray is used in various fields.

X線には白色X線、特性X線があり、例えば医療分野に
おいてX線CT装置により断層写真を撮影するとき、白色
X線を人体に対して放射状に照射し、その透過線を主に
Xe電離箱からなる複数の検出器により測定しているが、
かかる測定法では被測定物の組成を精度よく分析するの
が困難であるとされている。
X-rays include white X-rays and characteristic X-rays. For example, when a tomographic photograph is taken by an X-ray CT device in the medical field, white X-rays are radiated radially to the human body, and the transmitted rays are mainly
I am measuring with multiple detectors consisting of Xe ionization chamber,
It is said that it is difficult to accurately analyze the composition of the object to be measured by such a measuring method.

一方、不透明な物体の組成、濃度等につき、アイソトー
プ(Ga Ir Co)などのγ線源を用いて測定分析する方法
も実施されているが、この方法の場合、線源の安定性が
高い反面、半減期、取り扱い上の規制など、制約を受け
るところが多く、そのため工業化がむずかしいとされて
いる。
On the other hand, a method of measuring and analyzing the composition, concentration, etc. of an opaque object using a γ-ray source such as an isotope (Ga Ir Co) has been implemented, but this method has a high stability of the source. However, there are many restrictions such as half-life and restrictions on handling, which makes it difficult to industrialize.

『発明が解決しようとする問題点』 上記に代わるものとして、白色X線を単色化して被測定
物に照射し、その透過線をX線検出器でそ測定する方法
が提案されているが、この種の組成分析法では、一般的
に高い分析精度が要求される。
"Problems to be Solved by the Invention" As an alternative to the above, a method has been proposed in which white X-rays are monochromaticized, and the object to be measured is irradiated, and the transmitted rays thereof are measured by an X-ray detector. This type of composition analysis method generally requires high analysis accuracy.

高い分析精度を確保するためには、X線照射時において
X線源または被測定物のいずれか一方を走査する必要が
生じるが、こうした場合には、走査を要する分だけ測定
時間が長くなり、走査のための設備も大がかりとなる。
In order to secure high analysis accuracy, it is necessary to scan either the X-ray source or the object to be measured during X-ray irradiation, but in such a case, the measurement time becomes longer due to the need for scanning, The equipment for scanning also becomes large-scale.

上記走査を必要としない組成分析を行なおうとしても、
例えば前述したXe検出器ではその精度が低いためこれが
実行できず、走査方式による非測定物の組成分析では、
その被測定物を製造してい際の、すなわちオンラインで
の組成分析がほとんど不可能となる。
Even if you try to perform composition analysis that does not require the above scanning,
For example, the Xe detector described above cannot perform this because its accuracy is low, and in the composition analysis of the non-measured object by the scanning method,
It becomes almost impossible to analyze the composition while manufacturing the measured object, that is, online.

測定時間を短縮しながら精度の高い測定を実現するため
には、被測定物に対するX線の照射量を多くする必要が
あり、そのためには、X線ビームを幅1mm以下、長さ5mm
以上に設定するのがよいが、このような縦長のX線ビー
ムを回折して単色化し得る単結晶、およびその測定器
は、これらを配置すべきスペースの点で困難性をともな
う。
In order to realize highly accurate measurement while shortening the measurement time, it is necessary to increase the amount of X-ray irradiation to the DUT. For that purpose, the X-ray beam width is 1 mm or less and the length is 5 mm.
Although the above setting is preferable, a single crystal capable of diffracting a vertically long X-ray beam into a single color and a measuring instrument therefor are difficult in terms of a space for arranging them.

例えばNaIシンチレーションカウンタの場合、最小寸法
のものでも0.5インチはある。
For example, in the case of NaI scintillation counter, even the smallest size has 0.5 inch.

殊に、二以上の組成からなる光ファイバ用多孔質母材等
の組成を分析するとき、白色X線の分岐後、これを二種
以上の単色X線とし、それぞれの透過線を測定すること
になるので、単結晶の数、X線検出器の数が多くなり、
上記スペースファクタ上の困難度が増す。
In particular, when analyzing the composition of a porous preform for optical fibers, which consists of two or more compositions, after branching the white X-rays, make this into two or more types of monochromatic X-rays and measure the respective transmission lines. Therefore, the number of single crystals and the number of X-ray detectors increase,
The difficulty of the above space factor increases.

本発明は上述した問題点に鑑み、被測定物、X線源等を
走査せずとも、短時間で被測定物の組成分析が行なえ
る、しかもオンライン制御が可能な組成分析方法を提供
しようとするものである。
In view of the above-mentioned problems, the present invention is to provide a composition analysis method capable of performing composition analysis of an object to be measured in a short time without scanning the object to be measured, an X-ray source, etc., and capable of online control. To do.

『問題点を解決するための手段』 本発明のX線による被測定物の組成分析方法は、所期の
目的を達成するために、 被測定物の測定部間全域にわたって白色X線を照射する
ためのX線源と、 被測定物を透過した後の透過線(透過白色X線)を多数
のX線ビームに分岐するためのマルチコリメータであっ
て、(5×幅)<(1×長さ)を満足させる多数の縦長
スリットが幅方向に並んだものと、 マルチコリメータにより分岐された透過線中、低エネル
ギ単色X線を縦長スリットの長さ方向に回折するための
多数の低エネルギX線回折用単結晶と、 マルチコリメータにより分岐された透過線中、強エネル
ギ単色X線を縦長スリットの幅方向に回折するための多
数の強エネルギX線回折用単結晶と、 低エネルギX線回折用単結晶を経て入射される低エネル
ギ透過線を測定するためのX線検出器と、 強エネルギX線回折用単結晶を経て入射される強エネル
ギ透過線を測定するためのX線検出器とを備えているこ
と、および、 X線源から出射される白色X線の照射領域側に配置され
ている低エネルギ透過線測定用のX線検出器と強エネル
ギ透過線測定用のX線検出器とが、相対的な高低差をも
ってそのX線源とそれぞれ対面していること、 被測定物がX線源と各X線検出器との間において定位置
に配置されていること、 マルチコリメータが被測定物と各X線検出器との間に配
置されていること、 マルチコリメータにより分岐された透過線中の低エネル
ギ透過線をこれ用のX線検出器へ入射させるために、低
エネルギX線回折用の各単結晶が、被測定物と低エネル
ギ透過線測定用X線検出器との間に配置されて縦長スリ
ットの幅方向沿いに並び、かつ、これらマルチコリメー
タ、低エネルギ透過線測定用X線検出器とそれぞれ対応
していること、 マルチコリメータにより分岐された透過線中の強エネル
ギ透過線をこれ用のX線検出器へ入射させるために、強
エネルギX線回折用の各単結晶が、被測定物と強エネル
ギ透過線測定用X線検出器との間に配置されて縦長スリ
ットの幅方向沿いに並び、かつ、これらマルチコリメー
タ、強エネルギ透過線測定用X線検出器とそれぞれ対応
していること、および、 上記の手段を介して被測定物の組成を分析するときに、 X線源から出射した白色X線を被測定物の測定部間全域
に照射すること、 被測定物を透過した後の透過線をマルチコリメータによ
り分岐して、(5×幅)<(1×長さ)を満足させる多
数の縦長ビームにすること、 マルチコリメータにより分岐された透過線中の低エネル
ギ透過線をこれ用の単結晶により回折して低エネルギ透
過線測定用X線検出器へ入射させること、 マルチコリメータにより分岐された透過線中の強エネル
ギ透過線をこれ用の単結晶により回折して強エネルギ透
過線測定用X線検出器へ入射させること、 これら低エネルギ透過線、強エネルギ透過線をそれぞれ
のX線検出器により測定して被測定物の組成を分析する
ことを特徴とする。
"Means for Solving Problems" In the composition analysis method of an object to be measured by X-ray according to the present invention, in order to achieve the intended purpose, white X-rays are irradiated over the entire area between the measurement parts of the object to be measured. And a multi-collimator for splitting a transmission line (transmission white X-ray) after passing through the object to be measured into a large number of X-ray beams, (5 × width) <(1 × length A number of longitudinal slits that are aligned in the width direction, and a large number of low-energy X rays for diffracting low-energy monochromatic X-rays in the longitudinal direction of the transmission slit branched by the multi-collimator. Single crystal for line diffraction, a large number of single crystals for strong energy X-ray diffraction for diffracting strong energy monochromatic X-rays in the width direction of a longitudinal slit in a transmission line branched by a multi-collimator, and low energy X-ray diffraction Incident through a single crystal for low An X-ray detector for measuring an energy transmission line, and an X-ray detector for measuring a strong energy transmission line incident through a single crystal for strong energy X-ray diffraction, and X An X-ray detector for measuring low-energy transmission lines and an X-ray detector for measuring high-energy transmission lines, which are arranged on the irradiation region side of white X-rays emitted from the radiation source, have a relative height difference. Face each of the X-ray sources, the object to be measured is placed at a fixed position between the X-ray source and each X-ray detector, and a multi-collimator is provided to the object to be measured and each X-ray detector. And a single crystal for low-energy X-ray diffraction, in order to make the low-energy transmission line in the transmission line branched by the multi-collimator incident on the X-ray detector therefor, X-ray detector for measuring DUT and low energy transmission line Are arranged in the width direction of the longitudinal slit and correspond to the multi-collimator and the X-ray detector for low-energy transmission line measurement, respectively. In order to make the energy transmission line incident on the X-ray detector for this purpose, each single crystal for strong energy X-ray diffraction is arranged between the object to be measured and the X-ray detector for measuring strong energy transmission line. When arranged along the width direction of the longitudinal slits and corresponding to these multi-collimators and X-ray detectors for measuring strong energy transmission lines, and when analyzing the composition of the object to be measured through the above means. The white X-ray emitted from the X-ray source is applied to the entire area between the measurement parts of the object to be measured, and the transmission line after passing through the object to be measured is branched by the multi-collimator, and (5 × width) <( 1 x length) Add a number of longitudinal beams to be added, diffract a low energy transmission line among the transmission lines branched by a multi-collimator into a single crystal for incidence, and make it incident on an X-ray detector for measuring low energy transmission lines. The high-energy transmission line in the transmission line branched by the collimator is diffracted by a single crystal for this and made incident on the X-ray detector for measuring the high-energy transmission line. The X-ray detector is used to analyze the composition of the object to be measured.

『作用』 本発明方法の場合、白色X線を被測定物の測定部間全域
に照射するから、X線源あるいは被測定物を走査する必
要がなく、その透過線をマルチコリメータにより(5×
幅)<(1×長さ)のX線ビームに分岐するから、測定
時間を短縮し、精度の高い測定を実現するための条件を
も満足させることができ、しかも上記透過線中、低エネ
ルギ単色X線を単結晶により縦方向(縦長スリットの長
さ方向)に回折するとともに該透過線中の強エネルギ単
色X線を他の単結晶により横方向(縦長スリットの幅方
向)に回折するから、これと対応する各X検出器も上下
二段のように複数段に配置でき、X線検出器を配置する
際のスペースファクタが緩和される。
[Operation] In the case of the method of the present invention, since white X-rays are applied to the entire area between the measurement parts of the object to be measured, it is not necessary to scan the X-ray source or the object to be measured, and the transmission line thereof is (5 ×
Since the beam is branched into an X-ray beam of (width) <(1 × length), the measurement time can be shortened and the conditions for achieving highly accurate measurement can be satisfied. Since monochromatic X-rays are diffracted by a single crystal in the vertical direction (longitudinal direction of the longitudinal slit), and strong energy monochromatic X-rays in the transmission line are laterally diffracted by another single crystal (in the longitudinal direction of the longitudinal slit). The X detectors corresponding to this can also be arranged in a plurality of stages such as upper and lower two stages, and the space factor when arranging the X-ray detectors is relaxed.

なお、上記において、被測定物を透過した後の透過線を
(5×幅)<(1×長さ)のX線ビームに分岐する理由
は、つぎのとおりである。
In the above, the reason why the transmission line after passing through the object to be measured is branched into the X-ray beam of (5 × width) <(1 × length) is as follows.

X線検出器を介して被測定物の透過線を測定分析する場
合は、X線ビーム幅が小さく、しかも、X線ビーム数が
多いほど、被測定物の分解能が高まるが、その反面、X
線ビーム幅が小さくなると、X線検出器への受光量が減
少するために、X線検出器よる測定精度が低下する。
When measuring and analyzing a transmission line of an object to be measured through an X-ray detector, the smaller the X-ray beam width and the larger the number of X-ray beams, the higher the resolution of the object to be measured.
When the line beam width becomes smaller, the amount of light received by the X-ray detector decreases, and the measurement accuracy of the X-ray detector decreases.

本発明においては、X線ビーム幅を小さくし、X線ビー
ム数を多くした場合に生じる受光量の不足が、X線ビー
ムの長さを大きくすることで補償される。
In the present invention, the shortage of the amount of received light that occurs when the X-ray beam width is reduced and the number of X-ray beams is increased is compensated by increasing the length of the X-ray beam.

かかる分解能と受光量とを満足させるためのX線ビーム
形状は、これの幅:長さの関係であらわした場合に、
(5×幅)<(1×長さ)を満足させることを要する。
The X-ray beam shape for satisfying the resolution and the amount of received light is expressed by the width: length relationship,
It is necessary to satisfy (5 × width) <(1 × length).

『実施例』 以下、本発明方法の実施例につき、図面を参照して説明
する。
[Examples] Examples of the method of the present invention will be described below with reference to the drawings.

第1図、第2図において、1はX線源、2、3はマルチ
コリメータ、4、5は単結晶、6、7はX線検出器であ
る。
In FIGS. 1 and 2, 1 is an X-ray source, 2 and 3 are multi-collimators, 4 and 5 are single crystals, and 6 and 7 are X-ray detectors.

一方のマルチコリメータ2は、幅方向に並んだ多数の縦
長スリット2aを有し、他方のマルチコリメータ3も、幅
方法に並んだ多数の縦長スリット3aを有する。
One multi-collimator 2 has a large number of longitudinal slits 2a arranged in the width direction, and the other multi-collimator 3 also has a large number of longitudinal slits 3a arranged in the width direction.

8は不透明な被測定物である。8 is an opaque measured object.

第1図、第2図において本発明方法を実施するとき、被
測定物7がマルチコリメータ2、3間に配置され、X線
源1から出射された白色X線がマルチコリメータ2によ
り絞られて被測定物8の幅方向全域に照射される。
When carrying out the method of the present invention in FIGS. 1 and 2, the object to be measured 7 is placed between the multi-collimators 2 and 3, and the white X-rays emitted from the X-ray source 1 are focused by the multi-collimator 2. The entire area of the measured object 8 in the width direction is irradiated.

かかる白色X線は被測定物7を透過し、その透過線がマ
ルチコリメータ3により多数の縦長ビーム状に分光され
る。
The white X-rays pass through the object 7 to be measured, and the transmission lines are split into a number of vertically elongated beams by the multi-collimator 3.

ついで、上記透過線のうち、低エネルギ単色X線は単結
晶4により縦方向、例えば第1図のごとき上方、または
図示しない下方へ回折され、これと対応する位置に配置
されたX線検出器6によりそのエネルギ強度が測定され
る。
Then, among the above-mentioned transmitted rays, the low-energy monochromatic X-rays are diffracted by the single crystal 4 in the vertical direction, for example, upward as shown in FIG. 1 or downward (not shown), and the X-ray detector arranged at a position corresponding thereto. 6, its energy intensity is measured.

一方、上記透過線中の強エネルギ単色X線は単結晶4を
透過した後、他の単結晶5により横方向に回折され、か
つ、これと対応する位置に配置されたX線検出器7によ
りそのエネルギ強度が測定される。
On the other hand, the high-energy monochromatic X-rays in the transmission line are transmitted through the single crystal 4 and then laterally diffracted by another single crystal 5, and by the X-ray detector 7 arranged at a position corresponding thereto. Its energy intensity is measured.

こうして各X線検出器6、7により測定された結果が図
示しない電子計算機に入力され、該計算機により被測定
物8の組成が分析される。
In this way, the results measured by the X-ray detectors 6 and 7 are input to an electronic calculator (not shown), and the calculator analyzes the composition of the measured object 8.

なお、前述したX線検出機6、7としてはNaIを積層し
たシンチレーションカウンタが用いられる。
As the X-ray detectors 6 and 7 described above, a scintillation counter in which NaI is laminated is used.

本発明方法において、直径60mmのSiO2−GeO2からなる光
ファイバ用多孔質母材を被測定物とし、これの組成を分
析するとき、下記の条件で実施した。
In the method of the present invention, a porous preform for an optical fiber made of SiO 2 —GeO 2 having a diameter of 60 mm was used as an object to be measured, and the composition thereof was analyzed under the following conditions.

〔X線源1〕 Max160kev、ターゲット=W製 放射角=30度 〔マルチコリメータ2、3〕 幅×長さ=0.5×10にて分光するもの、分光数30 〔単結晶4〕 Si製、幅×長さ×厚さ=1×20×1、30個 〔単結晶5〕 Si製、幅×長さ×厚さ=40×15×1.5、30個 〔X線検出器6〕 NaI製、口径0.5インチ、30個 〔X線検出器7〕 NaI製、口径0.5インチ、30個 なお、X線検出器6、7はフォトマルプリアンプと一体
になったものを使用した。
[X-ray source 1] Max160kev, target = W Radiation angle = 30 degrees [Multi-collimator 2, 3] Spectra for spectroscopy with width x length = 0.5 x 10, spectrum number 30 [single crystal 4] Si, width X Length x Thickness = 1 x 20 x 1, 30 pieces [Single crystal 5] Si, width x length x thickness = 40 x 15 x 1.5, 30 pieces [X-ray detector 6] NaI, caliber 0.5 inch, 30 pieces [X-ray detector 7] NaI, 0.5 inch, 30 pieces X-ray detectors 6 and 7 used were integrated with a Photomul preamplifier.

第1図、第2図で例示した方法を上記の条件により実施
して光ファイバ用多孔質母材の組成を分析するとき、単
結晶5により80kevのエネルギを回折し、単結晶6によ
り200kevのエネルギを回折し、これらを上記X線検出器
で測定した。
When the method illustrated in FIGS. 1 and 2 is performed under the above conditions to analyze the composition of the porous preform for optical fibers, the single crystal 5 diffracts 80 kev of energy and the single crystal 6 of 200 kev. The energy was diffracted and these were measured with the X-ray detector.

この際の測定時間は数分であった。The measurement time at this time was several minutes.

なお、組成分布が軸対称である上記光ファイバ用多孔質
母材を分析するとき、コリメータにより分光されたX線
間の母材組成をも測定することにより分析精度が高ま
る。
When analyzing the above-mentioned optical fiber porous base material having a compositional distribution that is axially symmetric, the analysis accuracy is improved by also measuring the base material composition between the X-rays dispersed by the collimator.

このような場合は、X線源を中心にしてその線源以降の
各機器を水平方向へ少量だけ回転移動すればよい。
In such a case, each device after the X-ray source may be rotated and moved in the horizontal direction by a small amount around the X-ray source.

各機器を回転させるとき、NaIの口径が0.5インチである
ので、精度は要求されない。
When rotating each device, the accuracy of NaI is not required because the diameter of NaI is 0.5 inch.

『発明の効果』 以上説明した通り、本発明方法によるときは、X線源あ
るいは被測定物を走査する必要がないから、被測定物を
オンラインにて分析することができ、透過線をマルチコ
リメータにより所定のX線ビームに分岐するから、測定
時間を短縮し、精度の高い測定を実現することができ、
しかも上記透過線を単結晶による縦長スリットの長さ方
向、幅方向に回折するから、これと対応する各X検出器
も複数段に配置してX線検出器を配置する際のスペース
ファクタをも緩和し得る。
[Effects of the Invention] As described above, according to the method of the present invention, since it is not necessary to scan the X-ray source or the object to be measured, the object to be measured can be analyzed online, and the transmission line is a multi-collimator. Since the beam is branched into a predetermined X-ray beam, the measurement time can be shortened and highly accurate measurement can be realized.
Moreover, since the transmission line is diffracted in the lengthwise direction and the widthwise direction of the vertically elongated slit made of a single crystal, the X detectors corresponding thereto are also arranged in a plurality of stages, and the space factor when arranging the X-ray detectors is also increased. Can be relaxed.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明方法の一実施例を略示した正面図、第2
図は同上の平面図である。 1……X線源 3……マルチコリメータ 3a……縦長スリット 4、5……単結晶 6、7……X線検出器 8……被測定物
FIG. 1 is a front view schematically showing an embodiment of the method of the present invention, and FIG.
The figure is a plan view of the above. 1 ... X-ray source 3 ... Multi-collimator 3a ... Vertical slits 4, 5 ... Single crystal 6, 7 ... X-ray detector 8 ... Object to be measured

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】被測定物の測定部間全域にわたって白色X
線を照射するためのX線源と、 被測定物を透過した後の透過線(透過白色X線)を複数
のX線ビームに分岐するためのマルチコリメータであっ
て、(5×幅)<(1×長さ)を満足させる多数の縦長
スリットが幅方向に並んだものと、 マルチコリメータにより分岐された透過線中、低エネル
ギ単色X線を縦長スリットの長さ方向に回折するための
多数の低エネルギX線回折用単結晶と、 マルチコリメータにより分岐された透過線中、強エネル
ギ単色X線を縦長スリットの幅方向に回折するための多
数の強エネルギX線回折用単結晶と、 低エネルギX線回折用単結晶を経て入射される低エネル
ギ透過線を測定するためのX線検出器と、 強エネルギX線回折用単結晶を経て入射される強エネル
ギ透過線を測定するためのX線検出器とを備えているこ
と、および、 X線源から出射される白色X線の照射領域側に配置され
ている低エネルギ透過線測定用のX線検出器と強エネル
ギ透過線測定用のX線検出器とが、相対的な高低差をも
ってそのX線源とそれぞれ対面していること、 被測定物がX線源と各X線検出器との間において定位置
に配置されていること、 マルチコリメータが被測定物と各X線検出器との間に配
置されていること、 マルチコリメータにより分岐された透過線中の低エネル
ギ透過線をこれ用のX線検出器へ入射させるために、低
エネルギX線回折用の各単結晶が、被測定物と低エネル
ギ透過線測定用X線検出器との間に配置されて縦長スリ
ットの幅方向沿いに並び、かつ、これらマルチコリメー
タ、低エネルギ透過線測定用X線検出器とそれぞれ対応
していること、 マルチコリメータにより分岐された透過線中の強エネル
ギ透過線をこれ用のX線検出器へ入射させるために、強
エネルギX線回折用の各単結晶が、被測定物と強エネル
ギ透過線測定用X線検出器との間に配置されて縦長スリ
ットの幅方向沿いに並び、かつ、これらマルチコリメー
タ、強エネルギ透過線測定用X線検出器とそれぞれ対応
していること、および、 上記の手段を介して被測定物の組成を分析するときに、 X線源から出射した白色X線を被測定物の測定部間全域
に照射すること、 被測定物を透過した後の透過線をマルチコリメータによ
り分岐して、(5×幅)<(1×長さ)を満足させる多
数の縦長ビームにすること、 マルチコリメータにより分岐された透過線中の低エネル
ギ透過線をこれ用の単結晶により回折して低エネルギ透
過線測定用X線検出器へ入射させること、 マルチコリメータにより分岐された透過線中の強エネル
ギ透過線をこれ用の単結晶により回折して強エネルギ透
過線測定用X線検出器へ入射させること、 これら低エネルギ透過線、強エネルギ透過線をそれぞれ
のX線検出器により測定して被測定物の組成を分析する
ことを特徴とするX線による被測定物の組成分析方法。
1. A white X over the entire area between the measurement parts of the object to be measured.
An X-ray source for irradiating X-rays, and a multi-collimator for branching a transmission line (transmission white X-rays) after passing through an object to be measured into a plurality of X-ray beams (5 × width) < A large number of longitudinal slits satisfying (1 x length) are arranged in the width direction, and a large number for diffracting low energy monochromatic X-rays in the longitudinal direction of the longitudinal slit among the transmission lines branched by the multi-collimator. Low-energy X-ray diffraction single crystal, and a large number of high-energy X-ray diffraction single crystals for diffracting high-energy monochromatic X-rays in the transmission line branched by the multi-collimator in the width direction of the longitudinal slit, X-ray detector for measuring low-energy transmission line incident through a single crystal for energy X-ray diffraction, and X for measuring high-energy transmission line incident through a single crystal for strong energy X-ray diffraction Equipped with line detector And an X-ray detector for measuring low-energy transmission lines and an X-ray detector for measuring high-energy transmission lines, which are arranged on the irradiation region side of white X-rays emitted from the X-ray source, The X-ray source and the X-ray source facing each other with a certain height difference, the object to be measured is placed at a fixed position between the X-ray source and each X-ray detector, and the multi-collimator is connected to the object to be measured. It is arranged between each X-ray detector, and in order to make the low-energy transmission line among the transmission lines branched by the multi-collimator incident on the X-ray detector for this, a low-energy X-ray diffraction Each single crystal is arranged between the DUT and the X-ray detector for measuring low-energy transmission lines and arranged along the width direction of the longitudinal slit, and these multi-collimators and X-ray detection for measuring low-energy transmission lines are also provided. That correspond to each In order to make the strong energy transmission line in the transmission line branched by the rutile collimator enter the X-ray detector for this purpose, each single crystal for strong energy X-ray diffraction is for measuring the object to be measured and the strong energy transmission line. It is arranged between the X-ray detector and arranged along the width direction of the longitudinal slit, and corresponds to the multi-collimator and the X-ray detector for measuring the strong energy transmission line, and the above means. When analyzing the composition of the object to be measured through, irradiate the white X-rays emitted from the X-ray source to the entire area between the measurement parts of the object to be measured, and the transmission line after passing through the object to be measured by the multi-collimator. Divide into a number of longitudinal beams satisfying (5 x width) <(1 x length), diffract the low energy transmission line in the transmission line branched by the multi-collimator with a single crystal for this Low energy transmission Incident on the measuring X-ray detector, diffracting the strong energy transmission line in the transmission line branched by the multi-collimator by the single crystal for incidence on the X-ray detector for measuring strong energy transmission line, A method for analyzing the composition of an object to be measured by X-rays, characterized in that the composition of the object to be measured is analyzed by measuring the low energy transmission line and the high energy transmission line by respective X-ray detectors.
【請求項2】被測定物が、上下方向にわたる組成分布の
ほぼ等しい二成分系光ファイバ多孔質母材からなる特許
請求の範囲第1項記載のX線による被測定物の組成分析
方法。
2. The method for analyzing the composition of an object to be measured by X-ray according to claim 1, wherein the object to be measured comprises a binary component optical fiber porous preform having a substantially equal composition distribution in the vertical direction.
【請求項3】二種類の単色X線を別個の多層X線検出器
により測定する特許請求の範囲第1項記載のX線による
被測定物の組成分析方法。
3. The method for analyzing the composition of an object to be measured by X-ray according to claim 1, wherein two types of monochromatic X-rays are measured by separate multi-layer X-ray detectors.
【請求項4】X線源から放射状に出射された白色X線を
被測定物に照射し、かつ、X線源を中心にしてマルチコ
リメータ、各単結晶を少量回転させる特許請求の範囲第
1項記載のX線による被測定物の組成分析方法。
4. A multi-collimator, which rotates a small amount of each single crystal around the X-ray source, by irradiating the object to be measured with white X-rays radially emitted from the X-ray source. A method for analyzing the composition of an object to be measured by X-ray according to the item.
JP60082080A 1985-04-17 1985-04-17 Method for analyzing composition of object to be measured by X-ray Expired - Lifetime JPH071241B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60082080A JPH071241B2 (en) 1985-04-17 1985-04-17 Method for analyzing composition of object to be measured by X-ray

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60082080A JPH071241B2 (en) 1985-04-17 1985-04-17 Method for analyzing composition of object to be measured by X-ray

Publications (2)

Publication Number Publication Date
JPS61240148A JPS61240148A (en) 1986-10-25
JPH071241B2 true JPH071241B2 (en) 1995-01-11

Family

ID=13764476

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Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JPH071241B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2583215B2 (en) * 1986-02-28 1997-02-19 古河電気工業株式会社 X-ray composition analysis method for DUT
CN113805242B (en) * 2021-08-25 2024-07-12 浙江大华技术股份有限公司 Method and device for controlling ray source of security inspection machine, computer equipment and storage medium

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5622925A (en) * 1979-08-01 1981-03-04 Furukawa Electric Co Ltd:The Analytic measurement method for base material for optical fiber

Also Published As

Publication number Publication date
JPS61240148A (en) 1986-10-25

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