JPH0718823B2 - X-ray analyzer - Google Patents
X-ray analyzerInfo
- Publication number
- JPH0718823B2 JPH0718823B2 JP63273590A JP27359088A JPH0718823B2 JP H0718823 B2 JPH0718823 B2 JP H0718823B2 JP 63273590 A JP63273590 A JP 63273590A JP 27359088 A JP27359088 A JP 27359088A JP H0718823 B2 JPH0718823 B2 JP H0718823B2
- Authority
- JP
- Japan
- Prior art keywords
- vacuum
- output
- ray
- degree
- measured
- 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
Links
Landscapes
- 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) 本発明は、X線分析装置をおいて特に真空度補正手段に
関する。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an X-ray analyzer, and more particularly to a vacuum degree correcting means.
(従来の技術) 軽元素の蛍光X線分析は、X線の空気による吸収があ
り、真空度によって測定値が異なる。その影響を無くす
ために、測定中は一定の真空度を保つようににしてい
る。この分析装置の真空度を保つ方法は、機械方式でし
かもON・OFF制御によって行っているために、真空度の
安定性に問題が残り、最近LSAの発展によって可能とな
ってきたB,N,C等の超軽元素の分析においては、真空中
の残留空気によるX線の吸収が大きな問題となってきて
いる。そのために真空度の安定化が必要であるが、上記
したように従来の真空度制御では、高精度の安定を計る
のは難しい状態である。(Prior Art) In X-ray fluorescence analysis of light elements, there is absorption of X-rays by air, and the measured value differs depending on the degree of vacuum. In order to eliminate the influence, a constant degree of vacuum is maintained during measurement. Since the method of maintaining the degree of vacuum of this analyzer is a mechanical method and is controlled by ON / OFF control, there remains a problem in the stability of the degree of vacuum, which has recently become possible due to the development of LSA. In the analysis of ultra-light elements such as C, absorption of X-rays due to residual air in vacuum has become a big problem. Therefore, it is necessary to stabilize the degree of vacuum, but as described above, it is difficult to measure with high accuracy by the conventional vacuum degree control.
また、真空度の違いによる測定値の違いを真空度に基づ
く補正によって是正しようとする方法もあるが、真空計
毎に感度特性がばらついており、しかも真空計には寿命
があって、時々取換える必要があるが、完全に較正され
ている真空計を手に入れるのは難しく、また、真空計の
較正にも労力を必要とするために、簡単に高精度で絶対
真空度を測定するのは難しいので、実際の問題として
は、高精度の真空度安定が必要な軟X線測定において
は、測定値の精度は余り期待できないのが現状である。There is also a method to correct the difference in measured values due to the difference in vacuum degree by correction based on the vacuum degree, but the sensitivity characteristics vary from vacuum gauge to vacuum gauge, and the vacuum gauge has a limited lifespan. However, it is difficult to get a fully calibrated vacuum gauge, and the labor required to calibrate the vacuum gauge makes it easy to measure absolute vacuum with high accuracy. However, as a practical problem, in the soft X-ray measurement that requires highly accurate vacuum degree stability, the accuracy of measured values cannot be expected so much at present.
(発明が解決しようとする課題) 本発明は、真空度の影響が大きい波長領域のX線分析に
おいて、高精度の真空安定性を必要とせずに高精度のX
線分析を可能とすることを目的とする。(Problems to be Solved by the Invention) In the present invention, in X-ray analysis in a wavelength region where the influence of the degree of vacuum is large, it is possible to obtain high-precision X
The purpose is to enable line analysis.
(課題を解決するための手段) X線分析装置において、1つの元素の標準試料について
のX線検出出力と真空計の出力とから、絶対真空度と真
空計出力との関係を決定するプログラムを有し、この関
係式を記憶し、基準濃度の各元素のX線強度と絶対真空
度との関係を予め記憶し、被測定試料測定時真空計の出
力から、上記絶対真空度と真空計出力との関係により、
絶対真空度を算出し、予め記憶している上記目的元素の
上記X線強度と絶対真空度との関係を用いて、被測定試
料のX線強度から目的元素の濃度を決定するプログラム
を有するデータ処理手段を備えるか、又は、各元素の基
準濃度の標準試料について、X線検出出力と真空計の出
力との関係を実測記憶し、被測定試料測定時は、X線検
出出力と真空計の出力とにより、目的元素についての上
記関係から、目的元素の濃度を決定するプログラムを有
するデータ処理手段を備えた。(Means for Solving the Problem) In the X-ray analyzer, a program for determining the relationship between the absolute vacuum degree and the vacuum gauge output from the X-ray detection output and the output of the vacuum gauge for the standard sample of one element is provided. This relational expression is stored, the relationship between the X-ray intensity of each element of the reference concentration and the absolute vacuum degree is stored in advance, and the absolute vacuum degree and the vacuum gauge output are calculated from the output of the vacuum gauge when measuring the sample to be measured. Because of the relationship with
Data having a program for calculating the absolute vacuum degree and determining the concentration of the target element from the X-ray intensity of the sample to be measured by using the relationship between the X-ray intensity of the target element and the absolute vacuum degree stored in advance. A relation between the X-ray detection output and the output of the vacuum gauge is actually measured and stored for a standard sample having a processing element or a reference concentration of each element, and the X-ray detection output and the vacuum gauge A data processing means having a program for determining the concentration of the target element from the above relations with respect to the target element based on the output is provided.
(作用) 空気によるX線の吸収度は、空気の密度即ち真空度とX
線の波長と光路長によって決定され、光路長は分光器の
構造で決まっているので、既知試料についてX線の吸収
度が分かれば、真空度を逆算することが可能であり、す
でにその関係は公式化されているので、真空計の検出値
に対応する標準試料のX線の吸収度を測定することによ
り上記公式から真空計の較正を容易に行うことができ
る。(Operation) The degree of absorption of X-rays by air is the density of air, that is, the degree of vacuum and X
It is determined by the wavelength of the line and the optical path length, and the optical path length is determined by the structure of the spectroscope. Therefore, if the X-ray absorption of a known sample is known, the vacuum degree can be calculated backward, and the relationship is already established. Since it has been formulated, the vacuum gauge can be easily calibrated from the above formula by measuring the X-ray absorption of a standard sample corresponding to the detected value of the vacuum gauge.
従って、上記較正式をCPUに記憶させておき、真空計の
検出値を較正して絶対真空度を求め、この絶対真空度を
基にして、試料についてのX線測定値に対して真空度補
正を行い、試料中の目的元素の正しい濃度を決定するこ
とができる。Therefore, the above calibration formula is stored in the CPU, the detected value of the vacuum gauge is calibrated to obtain the absolute degree of vacuum, and the degree of vacuum is corrected for the X-ray measurement value of the sample based on this absolute degree of vacuum. Can be performed to determine the correct concentration of the target element in the sample.
ユーザ側は一定の標準試料を所持していれば何時でも容
易に真空計の較正ができる。また、真空計の表示真空度
と各元素標準試料のX線検出強度との関係を測定記憶し
ておけば、被測定試料の或る元素のX線強度と同じ真空
計表示値に対応する同じ元素の標準試料のX線線強度と
の比により被測定試料における同元素の濃度を決定する
ことができる。真空度が問題になる元素の数は限られて
いるので、それらの元素の標準試料を予め用意しておく
ことは容易であり、ユーザ側での実施も容易である。The user can easily calibrate the vacuum gauge at any time if he has a fixed standard sample. Further, if the relationship between the display vacuum degree of the vacuum gauge and the X-ray detection intensity of each element standard sample is measured and stored, the same X-ray intensity of a certain element of the sample to be measured corresponds to the same vacuum gauge display value. The concentration of the element in the sample to be measured can be determined by the ratio of the element to the X-ray intensity of the standard sample. Since the number of elements in which the degree of vacuum is a problem is limited, it is easy to prepare standard samples of these elements in advance, and it is easy for the user to implement them.
本願第1の発明についてもう少し詳説する。今1つの元
素の標準試料で、その元素の濃度をC0とする。この標準
試料を用い、X線分析装置の真空度を変えながら、真空
計の読みとQとX線検出強度Wとを測定する。絶対真空
度をPとし、装置内のX線光路長をt、空気の上記元素
の特性X線に対する質量吸収係数をμとすると、 W=W0e−ρμt 但し、ρ=P×1.146×10-10 ∴LogW=LogW0−ρμt これより絶対真空度Pは、 P=(LogW0−LogW)/1.146×10-10μt 上式でW0およびμtは装置と試料によって決まる値で、
今の場合、試料は標準試料であるから、LogW0および1.1
46×10-10μtはメーカ側で予め実測決定しておくこと
ができる。そこで、 LogW0=A 1.146×10-10μt=B とすると、 P=A/B−LogW/B ………(1) により絶対真空度Pが求まる。他方そのPに対応する真
空計の読みQが測定されているので、P=f(Q)なる
実験式を決定することができる。装置メーカにおいて装
置制御用CPUに上記定数A,B及び(1)式により、Wから
Pを求める演算プログラムを与えておくと、ユーザ側で
は随時同種標準試料を用い、上述と同じ操作で(1)式
により実測Wの値とQの値とからf(Q)の演算式を作
ることができ、このf(Q)により真空計の表示値から
絶対真空度Pを決定することができる。これにより、被
測定試料につき測定時、真空計の出力から絶対真空度が
求まると、予め与えられている基準波長の各元素のX線
強度と絶対真空度との関係により、被測定試料の定量目
的元素のX線強度から目的元素の濃度が求められる。The first invention of the present application will be described in more detail. Let's use the standard sample of one element and the concentration of that element as C 0 . Using this standard sample, the reading of the vacuum gauge and Q and the X-ray detection intensity W are measured while changing the degree of vacuum of the X-ray analyzer. Assuming that the absolute vacuum degree is P, the X-ray optical path length in the apparatus is t, and the mass absorption coefficient of air with respect to the characteristic X-rays of air is μ, then W = W 0 e −ρμt, where ρ = P × 1.146 × 10 -10 ∴LogW = LogW 0 −ρμt From this, the absolute vacuum degree P is P = (LogW 0 −LogW) /1.146×10 −10 μt In the above formula, W 0 and μt are values determined by the device and sample,
In this case, since the sample is a standard sample, LogW 0 and 1.1
46 × 10 -10 μt can be measured and determined in advance by the manufacturer. Therefore, if LogW 0 = A 1.146 × 10 −10 μt = B, then P = A / B−LogW / B (1) to obtain the absolute vacuum degree P. On the other hand, since the vacuum gauge reading Q corresponding to the P is being measured, the empirical formula P = f (Q) can be determined. If the equipment manufacturer gives the equipment control CPU an arithmetic program for obtaining P from W according to the above constants A, B and the equation (1), the user will always use the same kind of standard sample and perform the same operation as above (1). ), An arithmetic expression of f (Q) can be created from the value of the actually measured W and the value of Q, and the absolute vacuum degree P can be determined from the displayed value of the vacuum gauge by this f (Q). As a result, when the absolute vacuum degree is obtained from the output of the vacuum gauge during the measurement of the sample to be measured, the quantitative measurement of the sample to be measured is made based on the relationship between the X-ray intensity of each element having a predetermined reference wavelength and the absolute vacuum degree. The concentration of the target element can be calculated from the X-ray intensity of the target element.
(実施例) 第1図に本発明の一実施例を示す。第1図において、B
は励起X線、Sは試料、1は励起X線Bによって試料S
から放出される蛍光X線を分光する分光器、2は分光器
1で分光された蛍光X線を検出する検出器、3は検出器
2から出力されるX線検出パルスを計数するスケーラ、
4は分光器内の真空度を計るピラニー真空計、5は真空
計で測定された検出値をデジタル信号に変換するA/D変
換器、6はスケーラ3から出力されるX線検出信号に対
して補正演算を行うCPUで、A/D変換器5から出力される
真空度検出信号から予め求めた相関式により絶対真空度
を求め、同絶対真空度に基づいて事前に設定された補正
式によりX線検出信号に対し補正演算をする。上記演算
に必要な諸定数例えば前記A,B等も予めCPU6に記憶させ
てある。7はCPU6から出力される補正されたX線量を表
示する表示装置である。(Embodiment) FIG. 1 shows an embodiment of the present invention. In FIG. 1, B
Is an excited X-ray, S is a sample, 1 is an excited X-ray B, and a sample S
A spectroscope for separating the fluorescent X-rays emitted from the detector, 2 a detector for detecting the fluorescent X-rays dispersed by the spectroscope 1, 3 a scaler for counting the X-ray detection pulses output from the detector 2,
4 is a Pirani vacuum gauge for measuring the degree of vacuum in the spectroscope, 5 is an A / D converter for converting the detection value measured by the vacuum gauge into a digital signal, and 6 is an X-ray detection signal output from the scaler 3. In the CPU that performs the correction calculation, the absolute vacuum degree is obtained from the correlation equation obtained in advance from the vacuum degree detection signal output from the A / D converter 5, and the correction equation preset based on the absolute vacuum degree is used. Correction calculation is performed on the X-ray detection signal. Various constants required for the above calculation, such as A and B, are stored in the CPU 6 in advance. A display device 7 displays the corrected X-ray dose output from the CPU 6.
真空計4の較正方法を説明する。真空度を徐々に下げな
がら、或は装置を最終的な到達真空度まで徐々に空気を
漏入させながら、ピラニー真空計4の出力と同出力に対
する検出器2の元素およびその濃度既知の1つの標準試
料に対するX線検出出力をCPU6に記憶する。測定後、X
線検出器の上記検出出力により、前記(1)式を用いて
絶対真空度を計算し、求めた絶対真空度と真空計の出力
との相関式を求める。その求め方を説明すると、一つの
標準試料を用いて真空度を減圧させながら測定したX線
検出出力から、上記の(1)式によって求めた絶対真空
度Pと、その絶対真空度に対応する真空計4の出力値と
によって相関曲線を描くと第2図のようになる。この相
関曲線により絶対真空度Pとその絶対真空度に対応する
真空計の出力値との相関式を例えば3次式と仮定して最
小二乗法等により3次式の各係数を求めて、CPU6に記憶
する。A method of calibrating the vacuum gauge 4 will be described. While gradually lowering the degree of vacuum or allowing air to leak into the apparatus to the final ultimate degree of vacuum, the output of the Pirani vacuum gauge 4 and the element of the detector 2 corresponding to the same output and one of its known concentrations The X-ray detection output for the standard sample is stored in the CPU6. After measurement, X
Based on the detection output of the line detector, the absolute vacuum degree is calculated using the equation (1), and the correlation equation between the obtained absolute vacuum degree and the output of the vacuum gauge is obtained. Explaining how to obtain it, it corresponds to the absolute vacuum degree P obtained by the above formula (1) from the X-ray detection output measured while depressurizing the vacuum degree using one standard sample, and the absolute vacuum degree. FIG. 2 shows a correlation curve drawn with the output value of the vacuum gauge 4. Based on this correlation curve, it is assumed that the correlation equation between the absolute vacuum degree P and the output value of the vacuum gauge corresponding to the absolute vacuum degree is, for example, a cubic equation, and each coefficient of the cubic equation is obtained by the least square method or the like. Remember.
任意の試料を実測する場合には、真空計の読みから絶対
真空度を上記真空度較正式により求め、定量目的元素の
基準濃度におけるX線強度Wiと絶対真空度との関係式、 Wi=Wi0e−ρμ′t ………(2) 但し、ρは前記P×1.146×10-10,μ′は目的元素の質
量吸収係数 に上記絶対真空度を代入してWiを求め、Wiと実測X線強
度との比により、被測定試料中の目的元素の濃度を決定
する。(2)式におけるμ′tおよびWi0は装置と元素
によって決まる定数であり、真空度補正を要する軽元素
について、予めCPU6に記憶させてある。When actually measuring an arbitrary sample, the absolute vacuum degree is obtained from the reading of the vacuum gauge by the above vacuum degree calibration formula, and the relational expression between the X-ray intensity Wi and the absolute vacuum degree at the reference concentration of the quantitative target element, Wi = Wi 0 e −ρμ′t (2) where ρ is P × 1.146 × 10 −10 and μ ′ is the mass absorption coefficient of the target element and the above absolute vacuum degree is substituted for Wi to obtain Wi, and Wi is measured. The concentration of the target element in the sample to be measured is determined by the ratio with the X-ray intensity. Μ't and Wi 0 in the equation (2) are constants determined by the device and the elements, and the light elements requiring vacuum degree correction are stored in the CPU 6 in advance.
実際の測定に当たっては、真空度は時間によって変化す
るので、X線検出信号積分時間Tの間の平均透過率Hm
を、分析時間中に一定時間置きにN回真空度Pを測定し
て、透過率H(P)を算出して、N回の合計を平均し
て、 Hm=[ΣH(P)]/N で算出し、この平均透過率Hmを用いて、 Wo=W×[1/Hm] により求める。In actual measurement, since the vacuum degree changes with time, the average transmittance Hm during the X-ray detection signal integration time T
The vacuum degree P is measured N times at regular intervals during the analysis time, the transmittance H (P) is calculated, and the N times are averaged to obtain Hm = [ΣH (P)] / N Then, using this average transmittance Hm, W o = W × [1 / Hm]
(別実施例) この実施例は、装置構成は第1図と同じであるが、真空
計の読みから絶対真空度を算出すると云う手数をふま
ず、各元素の標準試料について、随時装置真空度を変え
ながらX線強度と真空計の読みとの関係を実測し、各元
素の基準濃度Cにおける実測X線強度Wとそのときの真
空計の出力Qとの関係実験式W=g(Q)を決めて、CP
U6に記憶させておき、任意試料についてのX線強度実測
値W′とそのときの真空計の出力Qとから、目的元素の
濃度C′を、 C′=C×W′/g(Q) によって求めるものである。実際の測定に当たってX線
検出信号積分時間中の真空度の時間的変化に対する装置
は前実施例と同じである。この実施例では真空度補正を
要する各元素について夫々標準試料を用意している必要
はあるが、データ処理は前実施例より簡単である。(Other Example) In this example, the apparatus configuration is the same as that in FIG. 1, but the trouble of calculating the absolute vacuum degree from the reading of the vacuum gauge is not taken into consideration, and the apparatus vacuum degree is changed from time to time for the standard sample of each element. The relationship between the X-ray intensity and the reading of the vacuum gauge was measured while changing the, and the relationship between the measured X-ray intensity W at the reference concentration C of each element and the output Q of the vacuum gauge at that time Empirical formula W = g (Q) Decide CP
It is stored in U6, and the concentration C ′ of the target element is calculated from the measured X-ray intensity value W ′ of an arbitrary sample and the output Q of the vacuum gauge at that time, C ′ = C × W ′ / g (Q) It is what you ask for. In the actual measurement, the apparatus for the temporal change of the degree of vacuum during the X-ray detection signal integration time is the same as in the previous embodiment. In this embodiment, it is necessary to prepare a standard sample for each element requiring vacuum correction, but the data processing is simpler than in the previous embodiment.
(発明の効果) 本発明によれば、高精度で絶対真空度を測定することが
可能になったことで、真空度による測定値の補正がより
高精度となり、測定精度の向上が計れた。また、高真空
になる迄待つことなく、高精度で測定することができる
ようになったことで測定能力が向上した。(Effects of the Invention) According to the present invention, the absolute vacuum degree can be measured with high accuracy, so that the correction of the measured value by the vacuum degree becomes more accurate, and the measurement accuracy can be improved. In addition, the ability to measure with high precision has been improved without having to wait until a high vacuum has been achieved, which has improved the measurement capability.
第1図は本発明の一実施例の構成図、第2図は真空計の
出力値と絶対真空度との相関曲線図、第3図は実測真空
度に対するX線検出強度曲線図である。 B…励起X線、S…試料、1…分光器、2…検出器、3
…スケーラ、4…真空計、5…A/D変換器、6…CPU、7
…表示装置。FIG. 1 is a configuration diagram of an embodiment of the present invention, FIG. 2 is a correlation curve diagram between an output value of a vacuum gauge and an absolute vacuum degree, and FIG. 3 is an X-ray detection intensity curve chart with respect to an actually measured vacuum degree. B ... Excited X-ray, S ... Sample, 1 ... Spectrometer, 2 ... Detector, 3
... scaler, 4 ... vacuum gauge, 5 ... A / D converter, 6 ... CPU, 7
... display device.
Claims (2)
出力と真空計の出力とから、絶対真空度と真空計出力と
の関係を決定するプログラムを有し、この関係式を記憶
し、 基準濃度の各元素のX線強度と絶対真空度との関係を予
め記憶し、 被測定試料測定時真空計の出力から、上記絶対真空度と
真空計出力との関係により、絶対真空度を算出し、予め
記憶している上記目的元素の上記X線強度と絶対真空度
との関係を用いて、被測定試料のX線強度から目的元素
の濃度を決定するプログラムを有するデータ処理手段を
備えたことを特徴とするX線分析装置。1. A program for determining a relationship between an absolute vacuum degree and a vacuum gauge output from an X-ray detection output and a vacuum gauge output for a standard sample of one element, and storing this relational expression, The relationship between the X-ray intensity of each element at the reference concentration and the absolute vacuum degree is stored in advance, and the absolute vacuum degree is calculated from the output of the vacuum gauge when measuring the sample to be measured, based on the relationship between the absolute vacuum degree and the vacuum gauge output. Then, a data processing means having a program for determining the concentration of the target element from the X-ray intensity of the sample to be measured by using the relationship between the X-ray intensity of the target element and the absolute vacuum degree stored in advance is provided. An X-ray analyzer characterized by the above.
線検出出力と真空計の出力との関係を実測記憶し、被測
定試料測定時は、X線検出出力と真空計の出力とによ
り、目的元素についての上記関係から、目的元素の濃度
を決定するプログラムを有するデータ処理手段を備えた
ことを特徴とするX線分析装置。2. A standard sample having a standard concentration of each element, X
The relationship between the X-ray detection output and the output of the vacuum gauge is actually measured and stored, and when measuring the sample to be measured, the concentration of the target element is determined from the above-mentioned relationship of the target element by the X-ray detection output and the output of the vacuum gauge. An X-ray analysis apparatus comprising a data processing unit having a program.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63273590A JPH0718823B2 (en) | 1988-10-28 | 1988-10-28 | X-ray analyzer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63273590A JPH0718823B2 (en) | 1988-10-28 | 1988-10-28 | X-ray analyzer |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02118440A JPH02118440A (en) | 1990-05-02 |
| JPH0718823B2 true JPH0718823B2 (en) | 1995-03-06 |
Family
ID=17529909
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63273590A Expired - Lifetime JPH0718823B2 (en) | 1988-10-28 | 1988-10-28 | X-ray analyzer |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0718823B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2020066100A1 (en) * | 2018-09-28 | 2020-04-02 | 株式会社島津製作所 | X-ray fluorescence spectrometer |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5786030A (en) * | 1980-11-17 | 1982-05-28 | Idemitsu Kosan Co Ltd | Method and apparatus for analysis of fluorescence x-rays |
-
1988
- 1988-10-28 JP JP63273590A patent/JPH0718823B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02118440A (en) | 1990-05-02 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Kessler Jr et al. | The deuteron binding energy and the neutron mass | |
| KR0124507B1 (en) | Test method and apparatus for transfer of calibration data between calibrated measuring instruments | |
| EP0250959B1 (en) | Method of calibrating reflectance measuring devices | |
| EP0075190B1 (en) | Apparatus for measuring thickness | |
| EP1054254B1 (en) | Data processor for X-ray fluorescence spectroscopy taking into account the element sensitivities of the measuring device independent of measurement conditions | |
| CN117129371B (en) | Calibration method, device and readable storage medium for surface density measuring instrument | |
| EP0360799B1 (en) | Measuring apparatus | |
| TW201947200A (en) | Method and apparatus for partial pressure detection | |
| AU616979B2 (en) | Asphalt content gauge with compensation for sample temperature deviations | |
| GB2195448A (en) | Flowmeter calibration | |
| JPH0718823B2 (en) | X-ray analyzer | |
| JP2000065765A (en) | X-ray fluorescence analyzer | |
| JP3333940B2 (en) | Apparatus and method for calibrating apparatus for measuring layer thickness using X-rays | |
| JP2927654B2 (en) | Method and apparatus for correcting bias in X-ray fluorescence analysis | |
| JP2921923B2 (en) | Radiation detector sensitivity calibration device | |
| JP2971772B2 (en) | Fluorescent glass dosimeter measuring device | |
| JP2671293B2 (en) | X-ray analyzer | |
| JPH05119000A (en) | Fluorescent x-ray analyzing device | |
| JP2896904B2 (en) | Calibration curve creation method for fluorescent X-ray film thickness measurement | |
| JP3205603B2 (en) | Mass calibration method for magnetic field type mass spectrometer | |
| JP2857296B2 (en) | Glass dosimeter | |
| SU565234A1 (en) | Method for calibrating infrared gas analyzer | |
| JPH05150050A (en) | Measurement data correction method | |
| JPH01319238A (en) | X-ray spectrum analyzer | |
| JPH06102031A (en) | Radiation thickness gauge |