The half-life of 14O and the ft value of the superallowed Fermi decay
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High precision half-life measurement of <sup>125</sup> Cs and <sup>125</sup> Xe with γ-spectroscopy
2019, Nuclear Physics ACitation Excerpt :The slope of the linear fit was always consistent with zero with maximum uncertainty of 0.2% (which is in excellent agreement with a previous work [30]) and this value can be considered as the upper limit of the systematic uncertainty characterizing the counting setup. The pulse pile-up effect can also influence the results of the γ-spectroscopy experiments [34,35]. The initial counting rates characterizing the half-life determination of 125Cs, listed in Table 2, varied between 0.54 kHz and 1.33 kHz.
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1993, Nuclear Inst. and Methods in Physics Research, ASuperallowed <sup>26</sup>Al<sup>m</sup>(β<sup>+</sup> + EC)<sup>26</sup>Mg decay
1991, Nuclear Physics, Section ASuperallowed <sup>42</sup>Sc(β<sup>+</sup>)<sup>42</sup>Ca decay
1989, Nuclear Physics, Section A
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Now at Division of Mineral Physics, CSIRO, North Ryde, NSW, Australia.
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