1986
DOI: 10.1154/s0376030800021261
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Use of Scattered Secondary Target Radiation in EDXRF Analysis: A Fundamental-Parameter Method for Matrix Correction

Abstract: A new fundamental-parameter program has been developed which corrects for light element absorption based on the mean atomic number of the sample. The mean atomic number, in turn, is determined from the Compton/Rayleigh scatter intensity ratio. The program is quite flexible with regard to the number and the type of standards which may be used. The accuracy and precision of the method has been evaluated with several geological and biological standards. The results are in good agreement with those obtained by som… Show more

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Cited by 4 publications
(2 citation statements)
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“…The algorithm MARS (Multielement Analysis Routine using Scatter) corrects the light element absorption on the basis of the mean atomic number of the sample, which is determined from the ratio of the incoherently and coherently scattered (Compton and Rayleigh) intensity radiation by the sample. 9 Pure compounds pellets [C 6 H 10 O 5 , H 3 BO 3 , NaNO 3 , (NH 4 2 SO 4 , KNO 3 and CaCO 3 ] were used to establish the correlations between the intensities of the Compton and Rayleigh scattered x-rays of the Ag secondary target by the irradiated sample and the average atomic number (Z). Ratios of the incoherently and coherently scattered x-rays by the sample, using the Ag secondary target, were highly correlated (r D 0.995) with the atomic number, within the range 6.68 < Z < 12.56 ( Fig.…”
Section: Calibration For the Light Matrixmentioning
confidence: 99%
“…The algorithm MARS (Multielement Analysis Routine using Scatter) corrects the light element absorption on the basis of the mean atomic number of the sample, which is determined from the ratio of the incoherently and coherently scattered (Compton and Rayleigh) intensity radiation by the sample. 9 Pure compounds pellets [C 6 H 10 O 5 , H 3 BO 3 , NaNO 3 , (NH 4 2 SO 4 , KNO 3 and CaCO 3 ] were used to establish the correlations between the intensities of the Compton and Rayleigh scattered x-rays of the Ag secondary target by the irradiated sample and the average atomic number (Z). Ratios of the incoherently and coherently scattered x-rays by the sample, using the Ag secondary target, were highly correlated (r D 0.995) with the atomic number, within the range 6.68 < Z < 12.56 ( Fig.…”
Section: Calibration For the Light Matrixmentioning
confidence: 99%
“…This is somewhat arbitrary and other limits can be considered, e.g. the upper limit can be incremented by 2. zb < z l , mean zc (12) Next, the concentration of hypothetical elements can be calculated from the following equations :…”
Section: Calculation Of Average Atomic Numbermentioning
confidence: 99%