Hauptseite > Publikationsdatenbank > High-precision Q$_{EC}$ values of superallowed $0^+ \to$ 0$^+ \beta$-emitters $^{46}$Cr, $^{50}$Fe and $^{54}$Ni > print

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024 7 _ |2 doi
|a 10.1016/j.physletb.2017.01.039
024 7 _ |2 ISSN
|a 0370-2693
024 7 _ |2 ISSN
|a 1873-2445
024 7 _ |2 datacite_doi
|a 10.15120/GSI-2018-00147
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037 _ _ |a GSI-2018-00147
041 _ _ |a English
082 _ _ |a 530
100 1 _ |0 P:(DE-HGF)0
|a Zhang, P.
|b 0
245 _ _ |a High-precision Q$_{EC}$ values of superallowed $0^+ \to$ 0$^+ \beta$-emitters $^{46}$Cr, $^{50}$Fe and $^{54}$Ni
260 _ _ |a Amsterdam
|b North-Holland Publ.
|c 2017
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500 _ _ |a Open Access funded by SCOAP³ - Sponsoring Consortium for Open Access Publishing in Particle Physics "Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3."
520 _ _ |a Short-lived 46 Cr, 50 Fe and 54 Ni were studied by isochronous mass spectrometry at the HIRFL-CSR facility in Lanzhou. The measured precision mass excesses (ME) of 46Cr, 50Fe and 54Ni are −29471(11) keV, −34477(6) keV and −39278(4) keV, respectively. The superallowed 0+ → 0+ β-decay Q values were derived to be Q EC (46 Cr) = 7604(11) keV, Q EC (50 Fe) = 8150(6) keV and Q EC (54 Ni) = 8731(4) keV. The values for 50Fe and 54Ni are by one order of magnitude more precise than the adopted literature values. By combining the existing half-lives and branching ratios, we obtained the corrected Ft values to be Ft(50Fe) = 3103(70) s and Ft(54Ni) = 3076(50) s. The main contribution to the Ft uncertainties is now due to β-decay branching ratios, still, more high-precision measurements of the half-lives, the masses, and especially the branching ratios are needed in order to satisfy the requirements for a stringent CVC test.
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