“…The low activity of 177m Lu present in the solution was found to have no effect in determining the half-life of 177 Lu. Dryak et al [18], reported a detection limit of 6 × 10 −9 for 177m Lu when using 177 Lu n.c.a., confirming the results presented in this paper regarding the negligible amount of impurity present in solution for this method of production.…”
Section: Discussionmentioning
confidence: 99%
“…Of these only the measurement reported by Dryak et al [18] has used 177 Lu from production method 2) and therefore not required corrections for the 177m Lu impurity. In a recent evaluation, Kellett [20] identified that the presence of 177m Lu has had a significant influence on the half-life determinations, while Pommé et al [14] observed that the omission of the impurity subtraction led to a 0.5% error in their determined halflife after only 7.6 days in their measurement campaign.…”
Section: Introductionmentioning
confidence: 99%
“…There have been 14 previous publications reporting half-life measurements of 177 Lu [6][7][8][9][10][11][12][13][14][15][16][17][18][19], which are summarised in Table 1. Of these only the measurement reported by Dryak et al [18] has used 177 Lu from production method 2) and therefore not required corrections for the 177m Lu impurity.…”
Abstract. 177 Lu is a medium energy beta-emitter commonly used in Nuclear Medicine for radiotherapeutic applications. In this work, the half-life of 177 Lu has been measured using a re-entrant ionisation chamber over a period of 82 days (approximately 12 half-lives). Unlike the majority of previous studies, the material used in this work was produced via the 176 Yb(n,γ ) 177 Yb reaction followed by the β-decay to 177 Lu, producing insignificant quantities of 177m Lu. This has resulted in the most precise half-life measurement of 177 Lu to date. A half-life of 6.6430 (11) days has been determined. This value is in statistical agreement with the currently recommended half-life of 6.6463 (15) days (z-score = 1.8).
“…The low activity of 177m Lu present in the solution was found to have no effect in determining the half-life of 177 Lu. Dryak et al [18], reported a detection limit of 6 × 10 −9 for 177m Lu when using 177 Lu n.c.a., confirming the results presented in this paper regarding the negligible amount of impurity present in solution for this method of production.…”
Section: Discussionmentioning
confidence: 99%
“…Of these only the measurement reported by Dryak et al [18] has used 177 Lu from production method 2) and therefore not required corrections for the 177m Lu impurity. In a recent evaluation, Kellett [20] identified that the presence of 177m Lu has had a significant influence on the half-life determinations, while Pommé et al [14] observed that the omission of the impurity subtraction led to a 0.5% error in their determined halflife after only 7.6 days in their measurement campaign.…”
Section: Introductionmentioning
confidence: 99%
“…There have been 14 previous publications reporting half-life measurements of 177 Lu [6][7][8][9][10][11][12][13][14][15][16][17][18][19], which are summarised in Table 1. Of these only the measurement reported by Dryak et al [18] has used 177 Lu from production method 2) and therefore not required corrections for the 177m Lu impurity.…”
Abstract. 177 Lu is a medium energy beta-emitter commonly used in Nuclear Medicine for radiotherapeutic applications. In this work, the half-life of 177 Lu has been measured using a re-entrant ionisation chamber over a period of 82 days (approximately 12 half-lives). Unlike the majority of previous studies, the material used in this work was produced via the 176 Yb(n,γ ) 177 Yb reaction followed by the β-decay to 177 Lu, producing insignificant quantities of 177m Lu. This has resulted in the most precise half-life measurement of 177 Lu to date. A half-life of 6.6430 (11) days has been determined. This value is in statistical agreement with the currently recommended half-life of 6.6463 (15) days (z-score = 1.8).
“…With the enhanced rigor in experimental execution and data analysis, the metrological community is currently achieving better consistency at a higher level of accuracy than in the past. Examples of recently achieved convergence are the improved half-life values for 55 Fe [7,8], 109 Cd [9][10][11], 177 Lu [12][13][14][15][16], 209 Po [17][18][19], 225 Ac [20,21], 223 Ra [22,23], and 227 Th [24,25].…”
A least-squares fit of exponential functions to a measured radioactive decay rate curve provides an estimate of the half-life and its statistical uncertainty in the assumption that all deviations from the theoretical curve are purely of a random nature. The result may be biased and the error underestimated as soon as the experiment suffers instabilities that exceed the duration of individual measurements. Contrary to long-term systematic errors, medium-frequency cyclic perturbations may be observable as autocorrelated structures in the residuals. In this work, an empirical decomposition algorithm is used to separate medium-frequency effects from the random statistical component in the fit residuals, such that custom error propagation factors can be calculated. A theoretical study of error propagation is made for sine and square wave perturbations. The empirical decomposition method is demonstrated on a synthetic spectrum, a time series of solar neutrino detection rates, and two experimental decay curves of 134Cs measured in an ionisation chamber.
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