2017
DOI: 10.1016/j.radphyschem.2017.01.013
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Uncertainty propagation in activation cross section measurements

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Cited by 96 publications
(35 citation statements)
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“…An additional acquisition of each sample was also carried out about 2 months after the EOB, to further measure the activity of the long-lived 46 Sc. Data analysis, including uncertainty calculations, was performed for each spectrum by using the procedure described by Otuka et al [15], taking into account the nuclear data from the NuDat 2.2 database [16] ( Table 1). The final nat V(p,x) 47 Sc, 46 Sc cross section value related to each target foil was calculated as the weighted average of all single values associated to each counting.…”
Section: Experimental Descriptionmentioning
confidence: 99%
“…An additional acquisition of each sample was also carried out about 2 months after the EOB, to further measure the activity of the long-lived 46 Sc. Data analysis, including uncertainty calculations, was performed for each spectrum by using the procedure described by Otuka et al [15], taking into account the nuclear data from the NuDat 2.2 database [16] ( Table 1). The final nat V(p,x) 47 Sc, 46 Sc cross section value related to each target foil was calculated as the weighted average of all single values associated to each counting.…”
Section: Experimental Descriptionmentioning
confidence: 99%
“…Here m has value equal to total number of measured cross-sections for a particular nuclear reaction and has value equal to total number of attributes in the activation formula. Let us consider x j (j = 1,2,3....n), various variable parameters (which are mentioned above) required in the calculation of the cross-sections, then the covariance matrix (c x ) of these variables can be obtained from the following equation [32];…”
Section: B Covariance Analysismentioning
confidence: 99%
“…The complete covariance matrix for measured cross sections is given by the following relation, (V σ s ) i j r e ir S i jr e jr 1 ≤ i, j ≤ 14, 1 ≤ r ≤ 20 (9) where S i jr is the n × n microcorrelation matrix between ith and jth observations due to the rth attributes, e ir is the partial uncertainty in ith observations due to the rth attributes and similarly for e jr [22]. The uncertainties of different parameters contribute to the total uncertainty of the measured cross section.…”
Section: Uncertainty In the Cross-section Measurementmentioning
confidence: 99%