JPH08201319A - Fluorescent x-ray analyzing method - Google Patents

Fluorescent x-ray analyzing method

Info

Publication number
JPH08201319A
JPH08201319A JP3001495A JP3001495A JPH08201319A JP H08201319 A JPH08201319 A JP H08201319A JP 3001495 A JP3001495 A JP 3001495A JP 3001495 A JP3001495 A JP 3001495A JP H08201319 A JPH08201319 A JP H08201319A
Authority
JP
Japan
Prior art keywords
fluorescent
intensity
ray
measured
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.)
Granted
Application number
JP3001495A
Other languages
Japanese (ja)
Other versions
JP2872926B2 (en
Inventor
Yoshiyuki Kataoka
由行 片岡
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.)
Rigaku Corp
Original Assignee
Rigaku Industrial 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 Rigaku Industrial Corp filed Critical Rigaku Industrial Corp
Priority to JP3001495A priority Critical patent/JP2872926B2/en
Publication of JPH08201319A publication Critical patent/JPH08201319A/en
Application granted granted Critical
Publication of JP2872926B2 publication Critical patent/JP2872926B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Analysing Materials By The Use Of Radiation (AREA)

Abstract

PURPOSE: To provide a fluorescent X-ray analyzing method capable of calculating the accurate contents of contained elements in an analysis object sample even if the measured spectral lines differ for individual elements when the device sensitivity is obtained with a standard sample and when the intensity of the fluorescent X-rays generated from the analysis object sample is measured. CONSTITUTION: The device sensitivity is calculated and stored for individual spectral lines other than the reference spectral line for individual elements on the fluorescent X-rays 6 generated from main constituting elements of a standard sample 3. When the fluorescent X-rays 6 measured with the intensity on an analysis object sample 13 are other than the reference spectral line, each device sensitivity is used.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、組成が既知の標準試料
についての検量線を用いないで、分析対象試料に含まれ
る各元素の含有率を算出する蛍光X線分析方法に関する
ものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a fluorescent X-ray analysis method for calculating the content of each element contained in a sample to be analyzed without using a calibration curve for a standard sample of known composition.

【0002】[0002]

【従来の技術】従来より、この種の分析方法として、試
料の組成を仮定して計算した各含有元素の蛍光X線の理
論強度と、試料に1次X線を照射して発生した各含有元
素の蛍光X線の実測強度とを用い、両強度が一致するよ
うに、前記仮定した組成を構成する各元素の含有率を逐
次近似的に修正計算して、試料の各含有元素の含有率を
算出することにより試料の組成を求める蛍光X線分析方
法、いわゆるファンダメンタルパラメータ法がある。こ
こで、試料から発生する各含有元素の蛍光X線の実測強
度とは、測定された強度そのものではなく、実際には、
例えば、以下のようにして求める。
2. Description of the Related Art Conventionally, as this kind of analysis method, the theoretical intensity of fluorescent X-ray of each contained element calculated assuming the composition of the sample and each content generated by irradiating the sample with primary X-rays Using the measured intensities of the fluorescent X-rays of the elements, the content ratios of the respective elements constituting the assumed composition are sequentially and approximately corrected and calculated so that the two intensities coincide, and the content ratios of the respective contained elements in the sample are calculated. There is a so-called fundamental parameter method, which is a fluorescent X-ray analysis method for obtaining the composition of a sample by calculating Here, the actually measured intensity of the fluorescent X-ray of each contained element generated from the sample is not the measured intensity itself but actually
For example, it is calculated as follows.

【0003】まず、あらかじめ使用する蛍光X線分析装
置において、組成が既知の標準試料について、1次X線
を照射して発生した蛍光X線の強度Im を測定する。一
方、前記既知の組成における含有率での理論強度It
算出する。そして、各元素ごとに、その理論強度It
前記測定強度Im で除したものIt /Im を、装置感度
t /Im として記憶しておく。そして、組成が未知の
分析対象の試料に、1次X線を照射して発生した蛍光X
線の強度im を測定し、その蛍光X線を発生させた元素
ごとに、測定強度im と前記装置感度との積it を次式
のように算出する。 it =im ×(It /Im )=im ×It /Im この積it は、試料から発生した蛍光X線の強度im
いわば理論強度スケールに換算した強度it であり、す
なわち前記実測強度it として用いられる。
First, in a fluorescent X-ray analyzer to be used in advance, the intensity I m of the fluorescent X-ray generated by irradiating the standard X-ray with a standard sample having a known composition is measured. On the other hand, to calculate the theoretical intensity I t in content in the known composition. Then, for each element, a I t / I m that the theoretical intensity I t was divided by the measured intensity I m, is stored as an apparatus sensitivity I t / I m. Then, the fluorescence X generated by irradiating the sample to be analyzed whose composition is unknown with the primary X-ray
Measuring the intensity i m lines, each element that caused the fluorescent X-ray, to calculate the product i t of the system sensitivity as measured intensity i m as the following equation. i t = i m × (I t / I m) = i m × I t / I m The product i t, the intensity i t that speak terms of theoretical intensity scale intensity i m of the fluorescent X-ray generated from the sample , and the other words are used as the measured intensity i t.

【0004】[0004]

【発明が解決しようとする課題】ところが、1元素から
発生する蛍光X線は、1種類すなわち1波長ではなく、
蛍光X線の発生に係わる電子の遷移との関係から、Kα
1 ,Kα2 ,Kβ1 ,Kβ2 ,Kβ3 ,Lα1 ,L
α2 ,Lβ1 ,Lβ2 ,Lβ3 …,Lγ1 ,Lγ2 ,L
γ3 …などと名付けられた複数の波長の相異なる蛍光X
線、すなわち各スペクトル線が発生する。ここで、Kα
1 線とKα2 線とは2重線で一般には分離が困難なた
め、合わせてKα線と呼ばれる。したがって、標準試料
を用いて装置感度を求めたときには、ある元素について
Kα線を基準としてKα線についての装置感度ItA/I
mAを求めたが、分析対象の試料では、Kα線に妨害スペ
クトル線が重なっているため、代わりにKβ1 線につい
てその強度imBを測定したというような事態が生ずる。
However, the fluorescent X-ray generated from one element is not one kind, that is, one wavelength,
From the relationship with the transition of electrons involved in the generation of fluorescent X-ray, Kα
1 , Kα 2 , Kβ 1 , Kβ 2 , Kβ 3 , Lα 1 , L
α 2 , Lβ 1 , Lβ 2 , Lβ 3, ..., Lγ 1 , Lγ 2 , L
Fluorescence X of different wavelengths named γ 3 … etc.
A line, or each spectral line, is generated. Where Kα
The 1- line and the Kα 2 line are double lines and are generally difficult to separate, so they are collectively referred to as the Kα line. Therefore, when the device sensitivity is obtained using a standard sample, the device sensitivity I tA / I for the Kα line with reference to the Kα line for a certain element.
Although seeking mA, the sample to be analyzed, because of overlap interference spectral lines Kα line, a situation such as that to measure the intensity i mB for Kbeta 1 line occurs instead.

【0005】この場合の前記実測強度itBは、前述した
ように、itB=imB×ItB/ImBで求められるが、この
うち標準試料におけるKβ1 線での測定強度ImBは測定
していないので、従来は、これを、標準試料におけるK
α1 線での測定強度ImAと理論強度比ItB/ItAとを用
いてImA×(ItB/ItA)として置き換えていた。その
結果、実測強度itBは、itB=imB×ItA/ImA=imB
×(ItA/ImA)となり、基準となるKα1 線での装置
感度ItA/ImAを、分析対象の試料におけるKβ1 線で
の測定強度imBに対してもそのまま用いることとなって
いた。前記置換は、理論強度比ItB/ItAと測定強度比
mB/ImAが等しいという仮定に基づいているのである
が、以下のような理由で、両者は実際には一致しない。
[0005] The measured intensity i tB in this case, as described above, i tB = i mB × but given by I tB / I mB, measured intensity I mB is measured at Kbeta 1 line Among the standard sample In the past, this was not
It was replaced with I mA × (I tB / I tA ) using the measured intensity I mA at the α 1 ray and the theoretical intensity ratio I tB / I tA . As a result, the measured intensity i tB is i tB = i mB × I tA / I mA = i mB
× (I tA / I mA ), and the device sensitivity I tA / I mA at the reference Kα 1 line is used as it is for the measured intensity i mB at the Kβ 1 line of the sample to be analyzed. Was there. The substitution is based on the assumption that the theoretical intensity ratio I tB / I tA and the measured intensity ratio I mB / I mA are equal, but the two do not actually match for the following reasons.

【0006】まず、第1に、測定強度は、分析装置にお
ける分光結晶等の分光系の波長特性によって異なるが、
理論強度においては、この分光系の波長特性を考慮して
いない。第2に、たとえばKα1 線とKα2 線とは完全
な分離測定が困難なため、理論強度では、それらの加重
平均波長であって合計の強度をもつKα線として扱う
が、実際の測定では、装置の分解能によってKα1 線と
Kα2 線との分離の度合いが異なる。第3に、理論強度
計算に用いる各蛍光X線の発生効率の物理定数が、誤差
を含んでいる。
First, although the measured intensity differs depending on the wavelength characteristics of the spectroscopic system such as the dispersive crystal in the analyzer,
The theoretical intensity does not consider the wavelength characteristic of this spectroscopic system. Secondly, since it is difficult to completely separate and measure Kα 1 and Kα 2 rays, theoretical intensity treats them as Kα rays having a weighted average wavelength and total intensity, but in actual measurement, The degree of separation between the Kα 1 ray and the Kα 2 ray varies depending on the resolution of the apparatus. Thirdly, the physical constant of the generation efficiency of each fluorescent X-ray used for the theoretical intensity calculation contains an error.

【0007】これらの理由から、理論強度比ItB/ItA
と測定強度比ImB/ImAは、実際には一致しない。すな
わち、従来の技術では、標準試料から発生する基準とな
るスペクトル線の強度を測定して装置感度を求めたとき
と、分析対象試料から発生するスペクトル線の強度を測
定したときとにおいて、各元素について測定したスペク
トル線が異なる場合には、分析対象試料の正確な実測強
度が求められず、したがって、各含有元素の正確な含有
率を算出することができない。
For these reasons, the theoretical intensity ratio I tB / I tA
The measured intensity ratio I mB / I mA does not actually match. That is, in the conventional technique, when measuring the intensity of a reference spectral line generated from a standard sample to determine the apparatus sensitivity and when measuring the intensity of a spectral line generated from a sample to be analyzed, each element If the spectrum lines measured for the above are different, the actual measured intensity of the sample to be analyzed cannot be obtained, and therefore the accurate content rate of each contained element cannot be calculated.

【0008】本発明は前記従来の問題に鑑みてなされた
もので、標準試料から発生する基準となるスペクトル線
の強度を測定して装置感度を求めたときと、分析対象試
料から発生するスペクトル線の強度を測定したときとに
おいて、各元素について測定したスペクトル線が異なる
場合においても、分析対象試料における各含有元素の正
確な含有率を算出することができる蛍光X線分析方法を
提供することを目的とする。
The present invention has been made in view of the above-mentioned conventional problems. When the intensity of a reference spectral line generated from a standard sample is measured to determine the sensitivity of the apparatus, the spectral line generated from the sample to be analyzed is obtained. It is possible to provide a fluorescent X-ray analysis method capable of calculating an accurate content rate of each contained element in a sample to be analyzed even when the spectrum line measured for each element is different from that when the intensity of is measured. To aim.

【0009】[0009]

【課題を解決するための手段】前記目的を達成するため
に、請求項1の方法では、X線が照射された試料から発
生する蛍光X線の強度に基づいて試料における元素の含
有率を算出する蛍光X線分析方法において、まず、主た
る構成元素が相異なりその含有率が既知である複数の標
準試料に1次X線を照射して、前記主たる構成元素から
発生する蛍光X線について、各スペクトル線ごとに、そ
の強度を測定し、その測定強度と理論強度とに基づいて
装置感度を算出する。そして、各元素ごとに、前記算出
した装置感度のうち、基準となるスペクトル線について
の装置感度を基準装置感度として記憶するとともに、前
記基準となるスペクトル線以外のスペクトル線について
のそれぞれの装置感度を記憶しておく。
In order to achieve the above object, in the method of claim 1, the content ratio of the element in the sample is calculated based on the intensity of the fluorescent X-ray generated from the sample irradiated with the X-ray. In the fluorescent X-ray analysis method described above, first, a plurality of standard samples having different main constituent elements and having different contents are irradiated with primary X-rays, and the fluorescent X-rays generated from the main constituent elements are The intensity of each spectral line is measured, and the device sensitivity is calculated based on the measured intensity and the theoretical intensity. Then, for each element, among the calculated device sensitivities, the device sensitivities for the reference spectral lines are stored as reference device sensitivities, and the respective device sensitivities for the spectral lines other than the reference spectral lines are stored. Remember.

【0010】次に、構成元素の含有率が未知である分析
対象試料に、1次X線を照射して発生した蛍光X線の強
度を測定し、その蛍光X線を発生させた元素ごとに、強
度を測定した蛍光X線が前記基準となるスペクトル線で
ある場合には前記基準装置感度を用い、強度を測定した
蛍光X線が前記基準となるスペクトル線以外のスペクト
ル線である場合には前記それぞれの装置感度を用いて、
分析対象試料における元素の含有率を算出する。
Next, the intensity of the fluorescent X-ray generated by irradiating the sample to be analyzed whose constituent element content is unknown with the primary X-ray is measured, and the intensity of the fluorescent X-ray is measured for each element. When the fluorescent X-ray whose intensity is measured is the reference spectral line, the reference device sensitivity is used, and when the fluorescent X-ray whose intensity is measured is a spectral line other than the reference spectral line, Using the sensitivity of each of the above,
The content rate of the element in the sample to be analyzed is calculated.

【0011】[0011]

【作用および効果】本発明によれば、標準試料の主たる
構成元素から発生する各スペクトル線について、各元素
ごとに、基準となるスペクトル線以外のスペクトル線に
ついてもそれぞれの装置感度を算出して記憶しておき、
分析対象試料において強度を測定した蛍光X線が基準と
なるスペクトル線以外のものである場合には、前記それ
ぞれの装置感度を用いるので、常に、分析対象試料にお
ける各含有元素の正確な含有率を算出することができ
る。
According to the present invention, with respect to each spectrum line generated from the main constituent elements of the standard sample, the device sensitivity is calculated and stored for each spectrum line other than the reference spectrum line. Well,
When the fluorescent X-ray of which the intensity is measured in the sample to be analyzed is other than the standard spectral line, since the respective device sensitivities are used, the accurate content ratio of each contained element in the sample to be analyzed is always determined. It can be calculated.

【0012】[0012]

【実施例】以下、本発明の実施例を図面にしたがって説
明する。まず、使用する蛍光X線分析装置において、主
たる構成元素が相異なりその含有率が既知である複数の
標準試料3を、順次、図1の試料台8に取り付けて、X
線源1から発生させた1次X線2を照射して、発生した
2次X線4を分光器5に入射させ、分光された主たる構
成元素から発生する蛍光X線6について、各スペクトル
線ごとに、その強度ImA,ImB…を検出器7で測定す
る。一方、前記既知の含有率での理論強度ItA,ItB
を算出し、各スペクトル線6について、その理論強度I
tA,ItB…をそれぞれの測定強度ImA,ImB…で除する
ことにより、それぞれの装置感度ItA/ImA,ItB/I
mB…を算出する。ここで用いる標準試料3は、多くの場
合純物質である。
Embodiments of the present invention will be described below with reference to the drawings. First, in the fluorescent X-ray analyzer to be used, a plurality of standard samples 3 having different main constituent elements and known contents are sequentially attached to the sample stage 8 in FIG.
The primary X-rays 2 generated from the radiation source 1 are irradiated, the generated secondary X-rays 4 are made incident on the spectroscope 5, and the spectral X-rays of the fluorescent X-rays 6 generated from the main constituent elements that are spectrally separated. Each time, the intensity I mA , I mB ... Is measured by the detector 7. On the other hand, the theoretical strengths I tA , I tB ...
And the theoretical intensity I of each spectral line 6 is calculated.
By dividing tA , I tB ... By the respective measurement intensities I mA , I mB ..., The respective device sensitivities I tA / I mA , I tB / I
Calculate mB ... The standard sample 3 used here is often a pure substance.

【0013】この算出を、各標準試料3ごと、すなわ
ち、各元素ごとに行い、また、各元素ごとに、算出した
装置感度ItA/ImA,ItB/ImB…のうち基準となるス
ペクトル線、たとえばKα線での装置感度ItA/ImA
基準装置感度ItA/ImAとして記憶するとともに、基準
となるスペクトル線以外のスペクトル線についてのそれ
ぞれの装置感度ItB/ImB…も記憶しておく。ここで、
この基準となるスペクトル線は、各元素についてたとえ
ば強い強度で測定されたものを採用すればよく、ある元
素についてはKα線で、別の元素についてはKβ1 線で
ある、といったように、元素ごとに異なっていてもよ
い。
This calculation is performed for each standard sample 3, that is, for each element, and for each element, the reference spectrum of the calculated device sensitivities I tA / I mA , I tB / I mB . Line, for example, the device sensitivity I tA / I mA at the Kα line is stored as the reference device sensitivity I tA / I mA , and the device sensitivity I tB / I mB for each spectral line other than the reference spectral line is also stored. Remember. here,
As the reference spectrum line, it is sufficient to adopt, for example, those measured with strong intensity for each element, for example, Kα ray for one element and Kβ 1 ray for another element. May be different.

【0014】次に、同様に、分析対象試料13に1次X
線2を照射して、発生した蛍光X線6の強度を測定す
る。そして、各元素について、その強度を測定した蛍光
X線6が基準となるスペクトル線、たとえばKα線であ
る場合には基準装置感度ItA/ImAを用い、その強度を
測定した蛍光X線6が基準となるスペクトル線すなわち
Kα線以外のスペクトル線である場合にはそれぞれの装
置感度ItB/ImB…を用いて、測定強度との積を実測強
度として算出する。そして、この実測強度と、分析対象
試料13の組成を仮定して計算した各含有元素の蛍光X
線の理論強度とを用い、両強度が一致するように、仮定
した組成を構成する各元素の含有率を逐次近似的に修正
計算して、分析対象試料13の各含有元素の含有率を算
出することにより試料の組成を求める。
Next, similarly, the primary X is added to the sample 13 to be analyzed.
The line 2 is irradiated and the intensity of the generated fluorescent X-ray 6 is measured. Then, for each element, when the fluorescent X-ray 6 whose intensity is measured is a reference spectrum line, for example, Kα ray, the standard device sensitivity I tA / I mA is used, and the fluorescent X-ray 6 whose intensity is measured is used. Is a reference spectrum line, that is, a spectrum line other than the Kα line, the product sensitivity I tB / I mB is used to calculate the product of the measured intensity and the measured intensity. Then, the fluorescence X of each contained element calculated on the assumption of the measured intensity and the composition of the sample 13 to be analyzed.
Using the theoretical strength of the line, the content rates of the respective elements constituting the assumed composition are sequentially and approximately corrected and calculated so that the two strengths match, and the content rates of the respective contained elements of the analysis target sample 13 are calculated. By doing so, the composition of the sample is obtained.

【0015】以上のように、本実施例によれば、標準試
料3の主たる構成元素から発生する各スペクトル線6に
ついて、各元素ごとに、基準となるスペクトル線以外の
スペクトル線についてもそれぞれの装置感度を算出して
記憶しておき、分析対象試料13において強度を測定し
た蛍光X線6が基準となるスペクトル線以外のものであ
る場合には、前記それぞれの装置感度を用いるので、常
に、分析対象試料13の正確な実測強度が求められ、し
たがって、分析対象試料13における各含有元素の正確
な含有率を算出することができる。
As described above, according to the present embodiment, with respect to each spectrum line 6 generated from the main constituent elements of the standard sample 3, for each element, a spectrum line other than the reference spectrum line is also used. When the fluorescent X-ray 6 whose intensity is measured in the analysis target sample 13 is one other than the spectral line serving as the reference, the sensitivity of each device is used, and therefore the sensitivity is always analyzed. An accurate measured intensity of the target sample 13 is obtained, and therefore, an accurate content rate of each contained element in the analysis target sample 13 can be calculated.

【0016】なお、本実施例では、各元素ごとに、基準
となるスペクトル線以外のスペクトル線についても、そ
れぞれの装置感度そのものを算出してかつ記憶したが、
基準となるスペクトル線での装置感度との比を算出して
その装置感度比を記憶し、実測強度を求める際に、その
装置感度比と基準装置感度とからそれぞれの装置感度を
再度算出して用いてもよい。また、これらの装置感度や
装置感度比は、それらを求めるのに用いた蛍光X線分析
装置の特性に依存するものなので、ある1台の装置で求
めておけば、それと同型の他の装置にも用いることがで
きる。また、同一装置においても、X線管の管電圧等の
分析条件が変化しても、用いることができる。
In the present embodiment, for each element, the device sensitivity itself of each spectral line other than the reference spectral line is calculated and stored.
Calculate the ratio with the device sensitivity at the reference spectral line and store the device sensitivity ratio, and when calculating the measured intensity, recalculate each device sensitivity from the device sensitivity ratio and the reference device sensitivity. You may use. Also, these device sensitivities and device sensitivity ratios depend on the characteristics of the fluorescent X-ray analysis device used to obtain them, so if one device is used to obtain the other device of the same type. Can also be used. Further, even in the same apparatus, it can be used even if the analysis conditions such as the tube voltage of the X-ray tube change.

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

【図1】本発明の一実施例を示す側面図である。FIG. 1 is a side view showing an embodiment of the present invention.

【符号の説明】[Explanation of symbols]

2…1次X線、3…標準試料、6…蛍光X線、13…分
析対象試料。
2 ... Primary X-ray, 3 ... Standard sample, 6 ... Fluorescent X-ray, 13 ... Analysis target sample.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 X線が照射された試料から発生する蛍光
X線の強度に基づいて試料における元素の含有率を算出
する蛍光X線分析方法において、 主たる構成元素が相異なりその含有率が既知である複数
の標準試料に1次X線を照射して、前記主たる構成元素
から発生する蛍光X線について、各スペクトル線ごと
に、その強度を測定し、その測定強度と理論強度とに基
づいて装置感度を算出し、 各元素ごとに、前記算出した装置感度のうち、基準とな
るスペクトル線についての装置感度を基準装置感度とし
て記憶するとともに、前記基準となるスペクトル線以外
のスペクトル線についてのそれぞれの装置感度を記憶
し、 構成元素の含有率が未知である分析対象試料に、1次X
線を照射して発生した蛍光X線の強度を測定し、 その蛍光X線を発生させた元素ごとに、強度を測定した
蛍光X線が前記基準となるスペクトル線である場合には
前記基準装置感度を用い、強度を測定した蛍光X線が前
記基準となるスペクトル線以外のスペクトル線である場
合には前記それぞれの装置感度を用いて、 分析対象試料における元素の含有率を算出することを特
徴とする蛍光X線分析方法。
1. In a fluorescent X-ray analysis method for calculating the content of elements in a sample based on the intensity of fluorescent X-rays generated from the sample irradiated with X-rays, the main constituent elements are different and the content is known. Are irradiated with primary X-rays to measure the intensity of each fluorescent X-ray generated from the main constituent element for each spectral line, and based on the measured intensity and the theoretical intensity. The device sensitivity is calculated, and for each element, the device sensitivity for the reference spectral line of the calculated device sensitivity is stored as a reference device sensitivity, and each of the spectral lines other than the reference spectral line is stored. The sensitivity of the device is memorized, and the primary X is added to the sample to be analyzed whose constituent element content is unknown.
The intensity of the fluorescent X-ray generated by irradiating the X-ray is measured, and when the fluorescent X-ray whose intensity is measured is the reference spectral line for each element that generated the fluorescent X-ray, the reference device When the fluorescent X-ray whose intensity is measured using sensitivity is a spectrum line other than the above-mentioned reference spectrum line, the content rate of the element in the sample to be analyzed is calculated using the sensitivity of each of the above devices. X-ray fluorescence analysis method.
JP3001495A 1995-01-25 1995-01-25 X-ray fluorescence analysis method Expired - Fee Related JP2872926B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3001495A JP2872926B2 (en) 1995-01-25 1995-01-25 X-ray fluorescence analysis method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3001495A JP2872926B2 (en) 1995-01-25 1995-01-25 X-ray fluorescence analysis method

Publications (2)

Publication Number Publication Date
JPH08201319A true JPH08201319A (en) 1996-08-09
JP2872926B2 JP2872926B2 (en) 1999-03-24

Family

ID=12292012

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3001495A Expired - Fee Related JP2872926B2 (en) 1995-01-25 1995-01-25 X-ray fluorescence analysis method

Country Status (1)

Country Link
JP (1) JP2872926B2 (en)

Also Published As

Publication number Publication date
JP2872926B2 (en) 1999-03-24

Similar Documents

Publication Publication Date Title
JP3108660B2 (en) X-ray analysis method and apparatus
EP3239702B1 (en) X-ray fluorescence spectrometer
JPH05240808A (en) Method for determining fluorescent x rays
US6173037B1 (en) Method of and apparatus for X-ray fluorescent analysis of thin layers
Zhao et al. Abundances of neutron capture elements in metal-poor dwarfs. I-Yttrium and zirconium
JP3610256B2 (en) X-ray fluorescence analyzer
JPH06123717A (en) Fluorescent x-ray qualitative analytical method under plurality of conditions
JP2872926B2 (en) X-ray fluorescence analysis method
JPH0247542A (en) Quantitative analysis using x-ray spectroscope
EP1521947B1 (en) Scatter spectra method for x-ray fluorescent analysis with optical components
JP4279983B2 (en) X-ray fluorescence analyzer
JPH071311B2 (en) Method for peak separation of fluorescent X-ray spectrum
JP2000097885A (en) Fluorescence x-ray analyzing method, and fluorescence x-ray analyzer
JP3729186B2 (en) X-ray fluorescence analyzer
JP3569734B2 (en) X-ray fluorescence analyzer
JP2645226B2 (en) X-ray fluorescence analysis method
JP2000065765A (en) X-ray fluorescence analyzer
JPH05209847A (en) Fluorescent x-ray spectroscopy method and apparatus
JP2592723B2 (en) Apparatus and method for identifying and analyzing X-ray fluorescence spectrum
JP2003107020A (en) Fluorescent x-ray analysis method for thin film
JP3377328B2 (en) X-ray fluorescence analysis method
JPH06337252A (en) Fluorescent x ray analytic method
JP3389161B2 (en) X-ray fluorescence analyzer and recording medium used therein
JP2002340822A (en) Fluorescent x-ray analyzing device
JP3399861B2 (en) X-ray analyzer

Legal Events

Date Code Title Description
FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20080108

Year of fee payment: 9

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20090108

Year of fee payment: 10

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20090108

Year of fee payment: 10

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20100108

Year of fee payment: 11

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20100108

Year of fee payment: 11

S111 Request for change of ownership or part of ownership

Free format text: JAPANESE INTERMEDIATE CODE: R313111

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20100108

Year of fee payment: 11

R350 Written notification of registration of transfer

Free format text: JAPANESE INTERMEDIATE CODE: R350

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20110108

Year of fee payment: 12

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20120108

Year of fee payment: 13

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20130108

Year of fee payment: 14

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20140108

Year of fee payment: 15

LAPS Cancellation because of no payment of annual fees