JPH07104296B2 - X-ray spectroscopic analysis method - Google Patents
X-ray spectroscopic analysis methodInfo
- Publication number
- JPH07104296B2 JPH07104296B2 JP60026858A JP2685885A JPH07104296B2 JP H07104296 B2 JPH07104296 B2 JP H07104296B2 JP 60026858 A JP60026858 A JP 60026858A JP 2685885 A JP2685885 A JP 2685885A JP H07104296 B2 JPH07104296 B2 JP H07104296B2
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- primary measurement
- correction coefficient
- measurement value
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N23/00—Investigating 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
- G01N23/22—Investigating 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
- G01N23/223—Investigating 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
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2223/00—Investigating materials by wave or particle radiation
- G01N2223/07—Investigating materials by wave or particle radiation secondary emission
- G01N2223/076—X-ray fluorescence
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- Analytical Chemistry (AREA)
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Description
【発明の詳細な説明】 イ.産業上の利用分野 本発明は試料中の成分元素の濃度を特性X線の強度から
求める分析方法に関する。Detailed Description of the Invention a. TECHNICAL FIELD The present invention relates to an analytical method for obtaining the concentration of a constituent element in a sample from the intensity of characteristic X-rays.
元素A,B…Nを成分とする試料の各成分元素の特性X線
強度をXa,Xb…Xnとし、各元素の100%濃度の標準試料の
同じ測定条件における特性X線強度を夫々Xao,Xbo,…Xn
oとすると、任意の成分元素の試料における特性X線強
度Xaは、その成分の試料中における濃度と標準試料にお
けるX線強度Xaoとから比例的に計算した値より多少異
って測定される。つまり見掛けの濃度Ka=Xa/Xaoは真の
濃度と異なる。これは主としてZAF効果による。測定さ
れた特性X線強度Xa,Xb…から各成分元素の濃度Ca,Cb…
を求めるには各元素の一次測定値即ち上記見掛けの濃度
Ka,…Kb…に夫々補正係数Ga,Gb…を掛算して Ca=Ga×Ka (1)等 となる。こゝで補正係数Ga,Gb等を求める方法としてZAF
法が知られている。ZAF法と言うのは試料を構成する各
成分元素の原子番号によって決まる電子線の励起効果
(Z),試料において観測される特性X線の共存元素に
よる吸収効果(A),試料の連続X線及び他元素の特性
X線によって励起される蛍光励起効果(F)等の因子に
よって決まり、これらの因子の影響を計算して上述補正
係数を決定する方法である(参考文献1982年、日刊工業
新聞社刊“物理分析講座I,物理分析法総覧「EPMA電子線
マイクロアナリシス」103頁)。所がZAF法を実行するに
は平均原子番号や平均原子量などの値が必要であ
り、やを求めるには各成分元素の濃度Ca,Cb…が必
要である。しかし最初はCa,Cb…が不明なので各成分元
素の一次測定値Ka,Kb…を用いて近似的なやを求め
て計算をスタートさせる。すなわち、直接測定で求まる
のは前述した一次測定値Ka,Kb等であるから、Ka,Kb等を
一応正しい濃度と仮定して補正係数Ga′,Gb′を求め、
これをKa,Kb等に掛算して濃度の近似値Ca′,Cb′等を算
出し、このCa′,Cb′等を用いて再度ZAF計算で補正係数
Ga,Gb等を求めて、これをKa,Kb等に掛算(Ga×Ca′等と
はしない。これはKa等に対する補正係数を求める手続だ
からである)してCa,Cb等を求めると言う逐次近似法を
採る。勿論一回の計算で充分な精度の答が得られる場合
もある。Let Xa, Xb ... Xn be the characteristic X-ray intensities of the respective constituent elements of the sample containing the elements A, B ... N, and Xa, Xb be the characteristic X-ray intensities under the same measurement conditions of the standard sample with 100% concentration of each element. Xbo, ... Xn
Assuming o, the characteristic X-ray intensity Xa of the sample of an arbitrary component element is measured to be slightly different from the value calculated proportionally from the concentration of the component in the sample and the X-ray intensity Xao of the standard sample. That is, the apparent density Ka = Xa / Xao is different from the true density. This is mainly due to the ZAF effect. From the measured characteristic X-ray intensities Xa, Xb ..., the concentration of each component element Ca, Cb ...
To obtain the primary measurement value of each element, that is, the apparent concentration
Multiplying Ka, ... Kb ... by the correction factors Ga, Gb ... respectively, Ca = Ga × Ka (1). ZAF is a method to find the correction factors Ga, Gb, etc. here.
The law is known. The ZAF method refers to the electron beam excitation effect (Z) determined by the atomic number of each component element that constitutes the sample, the absorption effect due to the coexisting element of the characteristic X-ray observed in the sample (A), and the continuous X-ray of the sample. And a factor such as fluorescence excitation effect (F) excited by characteristic X-rays of other elements, and the effect of these factors is calculated to determine the above correction coefficient (reference document 1982, Nikkan Kogyo Shimbun). Published by the company "Physical Analysis Course I, Physical Analysis Method Guidebook" EPMA Electron Beam Microanalysis ", page 103). However, in order to carry out the ZAF method, values such as the average atomic number and the average atomic weight are necessary, and the concentrations Ca, Cb ... Of the respective component elements are necessary to obtain or. However, since Ca, Cb, etc. are unknown at the beginning, the calculation is started by finding the approximate value of p using the primary measured values Ka, Kb, etc. of each component element. That is, since it is the above-mentioned primary measurement values Ka, Kb, etc. that can be obtained by direct measurement, the correction coefficients Ga ', Gb' are obtained by assuming Ka, Kb, etc. as the correct concentration.
Multiply this by Ka, Kb, etc. to calculate the approximate values of concentration Ca ', Cb', etc., and use these Ca ', Cb', etc. again to perform the correction coefficient by ZAF calculation.
Obtain Ga, Gb, etc., and multiply them by Ka, Kb, etc. (not Ga × Ca ', etc. This is because it is a procedure for finding a correction coefficient for Ka, etc.) and then say Ca, Cb, etc. Use the successive approximation method. Of course, there are cases where a sufficiently accurate answer can be obtained with a single calculation.
上述した所から明らかなように、X線分光分析でZAF法
を利用して定量分析をしようとする場合、試料の各成分
元素の特性X線強度が測定されることと、各成分元素に
ついて標準試料が準備できることが必要である。所が水
素とHeは特性X線が存在せず、Liは現在の所特性X線の
測定は不可能であり、このような元素を含んだ試料で
は、それらの元素に関する特性X線データが欠けたもの
となる。また、例えば酸素とか窒素などのように適正な
標準試料が得にくいときに、特性X線は測定しないで定
量分析を進めたい場合がある。本発明はこのような場合
にZAF法を適用して定量分析を行う方法に関するもので
ある。As is clear from the above, when attempting quantitative analysis using the ZAF method in X-ray spectroscopic analysis, the characteristic X-ray intensity of each constituent element of the sample is measured and The sample needs to be ready. However, there is no characteristic X-ray for hydrogen and He, and it is not possible to measure characteristic X-ray for Li at present. In samples containing such elements, characteristic X-ray data for those elements are missing. It becomes a thing. Further, when it is difficult to obtain an appropriate standard sample such as oxygen or nitrogen, it may be desired to proceed with the quantitative analysis without measuring the characteristic X-ray. The present invention relates to a method for carrying out a quantitative analysis by applying the ZAF method in such a case.
ロ.従来の技術 今元素A,B,…Nよりなる試料において、元素Nはこの試
料に含まれていることが知られている、あるいは予測さ
れているが、元素Nの特性X線のデータは欠けていると
する。各元素A,B,…の特性X線強度Xa,Xb…、各元素の1
00%濃度の標準試料の特性X線強度をXao,Xbo…等とす
ると、見掛けの濃度(一次測定値)は Ki=Xi/Xio(i=a,b…) …(2) 従来は元素Nの一次測定値Knを Kn=1−(Ka+Kb+…) ………(3) として、これらKa,Kb…Knを用いてZAF法による各元素A
〜Nの補正係数を計算すると言う方法が用いられてい
た。しかし実際上共存元素の影響は一般に吸収効果が最
も大きく、補正係数は多くの場合1より大きい数であ
る。つまりKiは正しい濃度より小さい。従って上記
(3)式で求まる元素Nの一次測定値は真の濃度より大
きく、ZAF法の計算の出発点として明らかに過大に設定
されている。このため従来法ではしばしば誤った値に収
斂することがあり、また逐次近似の収斂がおそく計算に
時間がかかる問題があった。B. 2. Description of the Related Art It is known or predicted that a sample consisting of the elements A, B, ... N now contains the element N, but the characteristic X-ray data of the element N is missing. Suppose Characteristic X-ray intensity Xa, Xb of each element A, B, ..., 1 of each element
If the characteristic X-ray intensity of a standard sample with a concentration of 00% is Xao, Xbo, etc., the apparent concentration (primary measurement value) is Ki = Xi / Xio (i = a, b ...) (2) Conventionally, the element N The primary measurement value Kn of Kn = 1- (Ka + Kb + ...) (3) is used, and each element A by the ZAF method is calculated using these Ka, Kb ... Kn.
A method of calculating a correction coefficient of ~ N has been used. However, in practice, the coexisting elements generally have the largest absorption effect, and the correction coefficient is a number larger than 1 in many cases. So Ki is smaller than the correct concentration. Therefore, the primary measurement value of the element N obtained by the above equation (3) is larger than the true concentration, and is obviously set too large as a starting point for the calculation of the ZAF method. For this reason, the conventional method often converges to an incorrect value, and the convergence of the iterative approximation slows down the calculation.
ハ.発明が解決しようとする問題点 本発明はX線分光による元素の定量分析で、特性X線の
測定データがない元素があるときにZAF法で各元素の補
正係数を計算する場合における従来方法の欠点を解消
し、誤った値に収斂するようなことをなくし、また逐次
近似の収斂を速めようとするものである。C. DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention The present invention is a quantitative analysis of elements by X-ray spectroscopy, and a conventional method in the case of calculating the correction coefficient of each element by the ZAF method when there is an element for which there is no characteristic X-ray measurement data It aims to solve the drawbacks, eliminate the convergence of wrong values, and speed up the convergence of successive approximation.
ニ.問題点解決のための手段 特性X線の測定データのない元素の一次測定値を測定す
るのに、各元素の特性X線の測定値から求めたそれらの
各元素の一次測定値の和を1から引算した残りの値を以
ってする従来方法を改め、この従来方法によって求めら
れる一次測定値に一定の変換を施したものを、特性X線
の測定データがない元素の一次測定値としてZAF法によ
る各元素の補正係数を求める。D. Means for Solving Problems In order to measure the primary measurement value of an element for which there is no characteristic X-ray measurement data, the sum of the primary measurement values of those elements obtained from the characteristic X-ray measurement value of each element is 1 The conventional method using the remaining value subtracted from is amended, and the primary measurement value obtained by this conventional method is subjected to constant conversion as the primary measurement value of the element for which there is no characteristic X-ray measurement data. Calculate the correction coefficient for each element by the ZAF method.
ホ.作 用 始めに述べたように、特性X線の測定値から求められる
一次測定値は真の濃度とは異なり多くの場合真の濃度よ
り小さく出るので、1からそれらの和を引いた差を、特
性X線の測定値が存在しない元素の一次測定値とすると
過大に設定したことになる。ZAF法の計算にあたって
は、真の平均原子番号と平均原子量が必要であり、
真のとを計算するには真の濃度Cが必要である。し
かし、真の濃度が不明であるため計算のスタートにおい
ては一次測定値を用いている。これは例えば平均原子番
号が次のように近似できることによる。E. As mentioned at the beginning of the operation, the primary measured value obtained from the measured value of the characteristic X-ray is smaller than the true concentration in many cases, and is smaller than the true concentration. Therefore, the difference obtained by subtracting the sum of 1 and If the characteristic X-ray measurement value is the primary measurement value of an element that does not exist, it is set excessively. To calculate the ZAF method, the true average atomic number and average atomic weight are required,
The true concentration C is needed to calculate the true and. However, since the true concentration is unknown, the primary measurement value is used at the start of the calculation. This is because, for example, the average atomic number can be approximated as follows.
こゝでZa,Zb等は成分元素の原子番号、Ca,Cb等はもちろ
ん濃度でCa+Cb+…+Cn=1である。これに対して 上記(5)式はZa,Zb,…の各々にKa,Kb…の重みがかか
っているが、若しKnに対して従来方式のように、 Kn=1−(Ka+Kb+…+Km) ……(6) とすると、Znには他の元素とは異なった重みがかかって
しまう。しかも差 (Ca+Cb+…+Cn)−(Ka+Kb+…+Kn) ……(7) が全部Knに上乗せされた形になって、補正係数における
Knの誤差が大きく、この影響でCa,Cb,…Cnの誤差も大き
くなってしまう。このため適当な変換によってより正し
い値を特性X線の測定データのない元素の一次測定値と
することによって、誤った結果に収斂するのを防ぐこと
ができ、また逐次近似法の収斂を速めることができる。 Here, Za, Zb, etc. are atomic numbers of component elements, and Ca, Cb, etc. are of course Ca + Cb + ... + Cn = 1 in concentration. On the contrary In the above equation (5), each of Za, Zb, ... is weighted by Ka, Kb ..., but if Kn is the same as the conventional method, Kn = 1- (Ka + Kb + ... + Km) ...... ( 6) Then, Zn is weighted differently from other elements. Moreover, the difference (Ca + Cb + ... + Cn)-(Ka + Kb + ... + Kn) (7) is added to Kn, and the correction coefficient
The error of Kn is large, and due to this effect, the error of Ca, Cb, ... Cn also becomes large. For this reason, it is possible to prevent the convergence to an incorrect result and to speed up the convergence of the iterative approximation method by making a more correct value into the primary measurement value of the element having no characteristic X-ray measurement data by appropriate conversion. You can
ヘ.実施例 第2図は本発明方法を実行する装置の概要を示す。1は
X線分析装置、2は装置全体を制御するコンピュータ、
3は試料の各元素の特性X線の測定値のデータを格納し
ておくメモリ、4は演算に必要なデータを格納しておく
データメモリで各元素の標準試料の特性X線の測定値の
データ等が格納される。5は装置の制御及びデータ処理
の演算のプログラムを格納しておくプログラムメモリ
で、6はデータをデータメモリ4に入力するためのキー
ボードで、このキーボードを操作して上記した標準試料
の特性X線の測定値のデータ等を入力する。装置に標準
試料測定モードを設けて、標準試料の特性X線を測定し
て直接データメモリ4に格納するようにしてもよい。F. Embodiment FIG. 2 shows an outline of an apparatus for carrying out the method of the present invention. 1 is an X-ray analysis apparatus, 2 is a computer that controls the entire apparatus,
3 is a memory for storing the data of the measured value of the characteristic X-ray of each element of the sample, and 4 is a data memory for storing the data necessary for the calculation. Data etc. are stored. Reference numeral 5 is a program memory for storing a program for control of the apparatus and calculation of data processing, 6 is a keyboard for inputting data to the data memory 4, and operating the keyboard, the characteristic X-ray of the standard sample described above. Enter the measured value data, etc. The apparatus may be provided with a standard sample measurement mode so that the characteristic X-ray of the standard sample is measured and directly stored in the data memory 4.
実施例1 試料の成分元素は事前の定性分析あるいは材料としての
予測などによってA,B…M,Nであることが分かっているも
のとし、このうち元素A,B…Mについては特性X線の測
定データが実際に得られ、元素Nについては特性X線の
測定データがないものとする。元素A,B…Mの一次測定
値をKa,Kb,…Kmとする。まず Kn′=1−(Ka+Kb+…+Km) ……(8) なるKn′を仮に元素のNの一次測定値として、Ka,Kb,…
Km,Kn′を用いて式(1)の補正係数Gaを求めるのと同
様なZAF法の計算を行い、元素Nの補正係数Gn′を求め
る。その上で元素Nの一次測定値により近い値K*nを K*n=Kn′/Gn′ ……(9) によって求める。これは、Kn′はKnよりもCnに近い値で
あるとの考察に基づき、式(1)の元素Nについての変
形式Kn=Cn/GnのCnをKn′でおきかえ、GnをGn′でおき
かえたものである。この点に付いては後述で詳しく説明
する。ここで求まったK*nを元素Nの一次測定値Knと
見なしてK*nをKnに代入し、このKnと他の各元素の一
次測定値Ka,Kb,…Kmによって、各元素の初回の補正係数
Ga,Gb…Gm,Gn等をZAF法で計算する。各成分元素の濃度C
a,Cb…Cnは、 Cj=GjKj(j=a,b…,m,n) ……(10) で与えられる。上記初回の計算で各成分の濃度が充分な
精度で求まったと認められたときは、初回だけで計算を
終わる。未だ充分な精度に達していないときは上記Ca〜
Cnを用いて再度ZAF法により各元素の補正係数を計算
し、(10)式と同様の計算で各成分の濃度を求め、以後
目標とする精度に達するまで同じ計算を繰返せばよい。Example 1 It is assumed that the constituent elements of the sample are A, B ... M, N by qualitative analysis in advance or prediction as a material, and among them, the elements A, B ... M of the characteristic X-ray It is assumed that the measurement data is actually obtained and that there is no characteristic X-ray measurement data for the element N. The primary measurement values of the elements A, B ... M are Ka, Kb, ... Km. First, Kn '= 1- (Ka + Kb + ... + Km) (8) Let Kn' be the primary measured value of N of the element, Ka, Kb, ...
The correction coefficient Gn 'of the element N is calculated by performing the same ZAF method calculation as the correction coefficient Ga of the equation (1) using Km and Kn'. Then, a value K * n closer to the primary measurement value of the element N is obtained by K * n = Kn '/ Gn' (9). Based on the consideration that Kn ′ is closer to Cn than Kn, replace Cn of Kn = Cn / Gn for element N in Eq. (1) with Kn ′ and replace Gn with Gn ′. It has been replaced. This point will be described in detail later. The K * n obtained here is regarded as the primary measurement value Kn of the element N, K * n is substituted into Kn, and the initial measurement value Ka, Kb, ... Correction factor of
Ga, Gb ... Gm, Gn, etc. are calculated by the ZAF method. Concentration C of each component element
a, Cb ... Cn are given by Cj = GjKj (j = a, b ..., m, n) (10). If it is recognized that the concentrations of the respective components have been obtained with sufficient accuracy in the first calculation, the calculation is completed only in the first calculation. If the accuracy is not yet sufficient, the above Ca ~
The correction coefficient for each element is calculated again by CAF using the ZAF method, the concentration of each component is obtained by the same calculation as in equation (10), and the same calculation is repeated thereafter until the target accuracy is reached.
この方法の考え方は次の通りである。第3図で線分aは
試料の全体を示し長さが“1"でΣCiの範囲が成分A〜M,
Cnの範囲が元素Nの量を示す。線bでΣKiは成分A〜M
の一次測定値の和、Kn′は残りの部分で元素Nの仮の一
次測定値である。今仮に元素Nについて他元素と同様の
正しい一次測定値が得られたとしてこれを線分cの長さ
Knとする。Ki(i=a,b…m)及びKnを用いてZAF法によ
り各元素の補正係数を求め夫々Ki等と掛算すると各成分
の正しい濃度Ci等が求まる。こゝでaの線分におけるCn
の長さを線分cの長さKnで割ったものが元素Nの補正係
数Gnである。こゝで元素Nの補正係数は大勢としては元
素A〜Mの比率で決まり、Nの濃度が多少変化してもGn
の値は殆ど変わらない。従ってGnはKn′=1−ΣKiを一
次測定値として求めた前記Gn′と略々等しい。The idea of this method is as follows. In Fig. 3, the line segment a shows the entire sample, and the length is "1" and the range of ΣCi is the components A to M,
The range of Cn indicates the amount of element N. In line b, ΣKi is the component A to M
The sum of the primary measurement values of Kn ′ is a temporary primary measurement value of the element N in the remaining portion. Assuming that the same primary measurement value as that for other elements is obtained for the element N, this is the length of the line segment c.
Kn. When Ki (i = a, b ... m) and Kn are used to obtain the correction coefficient of each element by the ZAF method and multiplication with Ki etc., the correct concentration Ci etc. of each component is obtained. Cn in the line segment of a here
The correction coefficient Gn of the element N is obtained by dividing the length of the element by the length Kn of the line segment c. Here, the correction coefficient for the element N is mostly determined by the ratio of the elements A to M, and even if the concentration of N changes slightly, Gn
The value of is almost unchanged. Therefore, Gn is substantially equal to Gn 'obtained by using Kn' = 1-ΣKi as the primary measurement value.
所で、第3図bを第3図aおよびcと較べると、Kn′は
一次測定値の近似値と言うより濃度の近似値と言うこと
になる。このことは濃度の和は1であるが一次測定値の
和は1ではない(一般には1よりも小)と言うことから
も考えられる。そこでKnが得られないときに、できるだ
けKnに近い仮想値K*nを設定しようとすると、 K*n=(真の濃度Cn)/(真の補正係数Gn) ≒(仮の濃度Kn′)/(補正係数の近似値Gn′) と考えられるので、 K*n=Kn′/Gn′ ……(11) と近似的におくことができる。By the way, comparing FIG. 3b with FIGS. 3a and 3c, it can be said that Kn 'is an approximate value of the concentration rather than an approximate value of the primary measurement value. This may be because the sum of the densities is 1, but the sum of the primary measurement values is not 1 (generally smaller than 1). Therefore, if Kn cannot be obtained and an attempt is made to set a virtual value K * n as close as possible to Kn, K * n = (true density Cn) / (true correction coefficient Gn) ≈ (temporary density Kn ') Since it is considered to be / (approximate value Gn 'of the correction coefficient), it can be approximated as K * n = Kn' / Gn '(11).
第1図は第2図の装置で上述実施例の補正係数算出動作
のフローチャートである。ステップST1で試料の各成分
A,B,…Mの特性X線強度Xa,Xb,…Xmを測定し、そのデー
タをメモリ3に格納し、ステップST2でメモリ4のデー
タを用いて各成分の一次測定値Ki(i=a,b…m)を算
出し、ステップST3でKn′=1−ΣKiを算出、ステップS
T4でKa,Kb…Km及びKn′を用いて、ZAF法により元素Nの
補正係数Gn′を算出し、ステップST5でK*n=Kn′/G
n′を算出、ステップST6でKa,Kb,…Km及びKnを用いてZA
F法で各元素A〜M,Nの補正係数Ga〜Gnを算出、ステップ
ST7でGj×Kjにより各元素A〜Nの濃度Cjを求める。FIG. 1 is a flow chart of the correction coefficient calculation operation of the above-described embodiment in the apparatus of FIG. Each component of the sample in step ST1
The characteristic X-ray intensities Xa, Xb, ... Xm of A, B, ... M are measured, the data are stored in the memory 3, and the primary measurement value Ki (i = a, b ... m) is calculated, Kn ′ = 1−ΣKi is calculated in step ST3, step S3
The correction coefficient Gn 'of the element N is calculated by the ZAF method using Ka, Kb ... Km and Kn' at T4, and K * n = Kn '/ G at step ST5.
n ′ is calculated, and in step ST6, ZA is calculated using Ka, Kb, ... Km and Kn.
Calculate the correction factors Ga to Gn for each element A to M, N by F method, step
In ST7, the concentration Cj of each element A to N is calculated by Gj × Kj.
実施例2 実施例1と同様にして元素Nの一次測定値KnをKn=をK
n′/Gn′として算出し、Ka〜Km及びKnを用いて各元素A
〜Mの補正係数Gi(i=a,b,…m)を計算し、Ki×Giで
各元素A〜Mの濃度Ciを求め、元素Nの濃度Cnは1−Σ
Ciで計算する。次にこのCiおよびCnを用いてZAF法で各
元素A〜Mの補正係数Giを計算し、上記と同様な式で各
元素A〜Mの濃度Ciと元素Nの濃度Cnを求める。以下適
当なところまで同じ計算方法を繰り返す。この方法の特
徴は、最初に仮の一次測定値Kn′からより確からしい一
次測定値Knを求める点と、その後の計算では元素Nの補
正係数を計算せず、各段階の計算で1から各元素A〜M
の濃度を引いたり残りを元素Nの濃度として次の段のZA
F計算に用いる点にある。この方法もプログラムを変え
るだけで第2図の装置で実行することができる。Example 2 In the same manner as in Example 1, the primary measurement value Kn of the element N is Kn = K
n '/ Gn' is calculated and each element A is calculated using Ka ~ Km and Kn.
~ M correction coefficient Gi (i = a, b, ... m) is calculated, the concentration Ci of each element A ~ M is obtained by Ki × Gi, the concentration Cn of the element N is 1-Σ
Calculate with Ci. Next, using these Ci and Cn, the correction coefficient Gi of each element A to M is calculated by the ZAF method, and the concentration Ci of each element A to M and the concentration Cn of the element N are obtained by the same formula as above. The same calculation method is repeated until an appropriate place. The feature of this method is that first, a more probable primary measurement value Kn is obtained from the tentative primary measurement value Kn ′, and the correction coefficient of the element N is not calculated in the subsequent calculation, and 1 to each is calculated in each step. Elements A to M
ZA of the next stage by subtracting the concentration of
It is used for F calculation. This method can also be executed by the apparatus shown in FIG. 2 simply by changing the program.
以上の説明で一次測定値は或元素の試料における特性X
線強度Xiとその元素の100%濃度の標準試料における特
性X線強度Xioの比Ki=Xi/Xioで与えられるとしたが、
標準試料が化合物又は混合物でその元素の濃度がαであ
るときは、 として、上述各実施例を実行すればよい。In the above explanation, the primary measurement value is the characteristic X in the sample of a certain element.
The ratio of the characteristic X-ray intensity Xio in the standard sample of the line intensity Xi and 100% concentration of the element is given as Ki = Xi / Xio,
When the standard sample is a compound or mixture and the concentration of the element is α, As the above, each of the above embodiments may be executed.
ト.効果 本発明によれば、試料中に特性X線の測定ができないと
か或は適当な標準試料がないとかで一次測定値が決定で
きない元素が含まれている場合でも、その元素の一次測
定値に相当するものが適切に設定されるので、一回の補
正計算でも良い結果が得られ逐次近似を行う場合でも収
斂が速く、計算量が少なくて精度の良い定量分析結果が
得られる。G. Effect According to the present invention, even if an element whose primary measurement value cannot be determined due to the fact that the characteristic X-ray cannot be measured in the sample or there is no suitable standard sample, the primary measurement value of the element is Since the corresponding ones are appropriately set, a good result can be obtained even by one correction calculation, and even if successive approximation is performed, the convergence is fast, the calculation amount is small, and the quantitative analysis result is accurate.
第1図は本発明の一実施例装置の第1実施例の方法を実
行する動作のフローチャート、第2図は上記実施例装置
の構成を示すブロック図、第3図は上記第1実施例方法
の意味を説明するグラフである。FIG. 1 is a flow chart of the operation for executing the method of the first embodiment of the apparatus of the present invention, FIG. 2 is a block diagram showing the configuration of the apparatus of the above embodiment, and FIG. 3 is the method of the first embodiment. It is a graph explaining the meaning of.
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭59−3246(JP,A) 特開 昭60−244844(JP,A) 「放射線計測ハンドブック」(昭和57年 日刊工業新聞社発行)P.607−609 内山郁、渡辺融、紀本静雄「X線マイク ロアナライザ」5版(昭49−10−20)日刊 工業新聞社 P.127−189 鉱物学雑誌、12〔特別〕(1976年3月) 由井、P.66−73 ─────────────────────────────────────────────────── ─── Continuation of the front page (56) References JP 59-3246 (JP, A) JP 60-244844 (JP, A) "Radiation measurement handbook" (published by Nikkan Kogyo Shimbun in 1982) P . 607-609 Ikuyama Iku, Watanabe Toru, Kimoto Shizuo "X-ray Microanalyzer" 5th edition (Sho 49-10-20) Nikkan Kogyo Shimbun P. 127-189 Mineralogy Magazine, 12 [Special] (March 1976) Yui, P .; 66-73
Claims (2)
各元素の一次測定値を求め、それらの値を用いてZAF法
によって各元素の補正係数を計算し、上記各一次測定値
に上記各補正係数を掛算して各元素の濃度を算出する方
法の適用に当たって、 試料中に特性X線の測定に基いて一次測定値が決定でき
ないひとつの元素Nが含まれる場合において、 求まっている各元素の一次測定値の和を1から引算した
残りを上記元素Nの仮の一次測定値として、他の元素の
一次測定値と共に用いてZAF法により元素Nの補正係数
を計算し、上記仮の一次測定値を上記補正係数で割算し
た値を元素Nの一次測定値として他の元素の一次測定値
と共に用い、 ZAF法で各成分元素の補正係数を求めることを特徴とす
るX線分光分析方法。1. A primary measurement value of each element is obtained from the intensity of the characteristic X-ray of the element constituting the sample, and a correction coefficient of each element is calculated by the ZAF method using these values, and the above primary measurement values are obtained. When applying the method of calculating the concentration of each element by multiplying each of the above correction factors, it has been determined in the case where the sample contains one element N whose primary measurement value cannot be determined based on the characteristic X-ray measurement. The sum of the primary measurement values of each element is subtracted from 1, and the remainder is used as the temporary primary measurement value of the above element N, together with the primary measurement values of other elements, and the correction coefficient for the element N is calculated by the ZAF method. A value obtained by dividing the temporary primary measurement value by the correction coefficient as the primary measurement value of the element N together with the primary measurement values of other elements, and obtaining the correction coefficient of each component element by the ZAF method. Spectroscopic method.
各元素の一次測定値を求め、それらの値を用いてZAF法
によって各元素の補正係数を計算し、上記各一次測定値
に上記各補正係数を掛算して各元素の濃度を算出する方
法の適用に当たって、 試料中に特性X線の測定に基いて一次測定値が決定でき
ないひとつの元素Nが含まれる場合において、 求まっている各元素の一次測定値の和を1から引算した
残りを上記元素Nの仮の一次測定値として、他の元素の
一次測定値と共に用いてZAF法により元素Nの補正係数
を計算し、 元素Nの上記仮の一次測定値を元素Nの上記補正係数で
割算した値を元素Nの一次測定値とし、 これを他元素の上記一次測定値と共に用いてNを除く他
元素の補正係数を計算し対応元素の一次測定値に掛算し
てそれらの元素の濃度を計算し、 その和を1から引算して元素Nの濃度とし、 以下前回で求まった各元素の濃度を用いてZAF法によっ
てNを除く他元素の補正係数を算出し、対応元素の一次
測定値に掛けて、それらの元素の濃度を算出し、その和
を1から引算して元素のNの濃度とする計算を必要回数
繰り返すことを特徴とするX線分光分析方法。2. A primary measurement value of each element is obtained from the intensity of the characteristic X-ray of the element constituting the sample, and the correction coefficient of each element is calculated by the ZAF method using these values, and the above primary measurement values are obtained. When applying the method of calculating the concentration of each element by multiplying each of the above correction factors, it has been determined in the case where the sample contains one element N whose primary measurement value cannot be determined based on the characteristic X-ray measurement. Calculate the correction coefficient for element N by the ZAF method, using the remainder obtained by subtracting the sum of the primary measurement values of each element from 1 as the temporary primary measurement value of the above element N together with the primary measurement values of other elements. A value obtained by dividing the above-mentioned temporary primary measurement value of N by the above-mentioned correction coefficient of the element N is taken as the primary measurement value of the element N, and using this together with the above-mentioned primary measurement values of other elements, the correction coefficient of other elements except N is calculated. Calculate and multiply the primary measurements of the corresponding elements by Calculate the concentration of the element, subtract the sum from 1 to obtain the concentration of the element N, and then use the concentration of each element obtained in the previous time to calculate the correction coefficient for other elements except N by the ZAF method. An X-ray spectroscopic analysis method, characterized in that the primary measurement values of the elements are multiplied, the concentrations of these elements are calculated, and the sum is subtracted from 1 to obtain the concentration of N of the element, which is repeated a necessary number of times.
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60026858A JPH07104296B2 (en) | 1985-02-14 | 1985-02-14 | X-ray spectroscopic analysis method |
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| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP60026858A JPH07104296B2 (en) | 1985-02-14 | 1985-02-14 | X-ray spectroscopic analysis method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61186840A JPS61186840A (en) | 1986-08-20 |
| JPH07104296B2 true JPH07104296B2 (en) | 1995-11-13 |
Family
ID=12204973
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP60026858A Expired - Fee Related JPH07104296B2 (en) | 1985-02-14 | 1985-02-14 | X-ray spectroscopic analysis method |
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| Country | Link |
|---|---|
| JP (1) | JPH07104296B2 (en) |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS593246A (en) * | 1982-06-28 | 1984-01-09 | Shimadzu Corp | Real-time elemental quantitative analysis method |
-
1985
- 1985-02-14 JP JP60026858A patent/JPH07104296B2/en not_active Expired - Fee Related
Non-Patent Citations (3)
| Title |
|---|
| 「放射線計測ハンドブック」(昭和57年日刊工業新聞社発行)P.607−609 |
| 内山郁、渡辺融、紀本静雄「X線マイクロアナライザ」5版(昭49−10−20)日刊工業新聞社P.127−189 |
| 鉱物学雑誌、12〔特別〕(1976年3月)由井、P.66−73 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61186840A (en) | 1986-08-20 |
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