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AbstractAbstract
[en] Neutron activation analysis (NAA) is a physical technique used for the absolute measurement of the concentration of substances in solids and liquids. The method uses neutron irradiation which is commonly realised using a nuclear reactor in order to activate (make radioactive) different isotopes of the elements present in the sample. The radionuclides produced in this way emit gamma-rays that are characteristic of the elements present in the sample. Using gamma-ray spectrometry these radionuclides can then be identified and quantified, and hence their concentration in the sample can be determined. Although NAA is a straightforward method it requires a sound control of the many physical parameters involved to obtain accurate results and to guarantee a set accuracy in routine analysis. The accuracy of NAA depends on the specific measurement method used. One can perform NAA in a relative way by co-irradiating a known standard and the unknown sample in the same conditions and by comparing the ratio of gamma-rays they emit. Relative NAA has limited applicability since it requires reference standards with a comparable composition as the unknown. A more generally applicable method is the k0-NAA method. In the k0-NAA method all measurements are relative to the element Au resulting in 198Au when irradiated. The k0-NAA method further relies on the fact that the neutron energy spectrum produced in a given position in the reactor can be parameterised with two parameters: the shape factor of the epithermal neutron flux, indicating the deviation of the epithermal neutron spectrum from the ideal 1/E shape approximated by a 1/E1+a distribution, with E the neutron energy; f: the thermal-to-epithermal neutron flux ratio. The parameters f and a are characteristic for the irradiation facility (reactor and irradiation channels) and may change or fluctuate in time according to the irradiation conditions. The way elements activate (become radioactive) when interacting with neutrons is determined by the nuclear cross sections. The cross sections depend on the neutron energy E and also these physical properties are parameterised in the k0-NAA method resulting in the so-called k0-factors for each element and for the different isotopes of an element. The quantification of an element then involves the use of a ratio of k0-factors in which one k0-factor is the one for 198Au. In practice, ratios of k0-factors accounting for the energy spectrum of the neutrons (f, a) are used in an analysis. These ratios are called the comparator factor FC. It is clear that the quality assurance of the k0-NAA method requires the control of the parameters f and a for each irradiation of samples. This is generally realised by using several flux monitors e.g. a set of Zr and Au monitors which are co-irradiated with the samples to analyse. However, this approach is quite labour intensive and recently we started investigating an approach based on co-irradiation of Synthetic Multi-Element Standards (SMELS) for this purpose. SMELS contain different elements in known concentrations, and three types of materials exist: Type I (elements forming short-lived radionuclides), Type II (elements forming medium lived radionuclides) and Type III (elements forming long lived radionuclides). Au was added to all three SMELS types and Zr in type III. The objectives are to optimise the ratio of quality of analysis to workload by appropriate quality control methods to determine and monitor the irradiation parameters (f, a) using SMELS and to set up a Quality Control (QC) system for the complete measurement and analysis process for k0-NAA
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Belgian Nuclear Research Center SCK-CEN, Mol (Belgium); 146 p; Sep 2007; p. 80-81; Available online at the Web site of the Belgian Nuclear Research Center http://www.sckcen.be/; The abstract is a contribution to the 2006 Scientific Report of the Belgian Nuclear Research Centre SCK-CEN
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