@Article{Fujita_etal2016,
author="Fujita, Y.
and Rubio, B.
and Molina, F.
and Adachi, T.
and Fujita, H.
and Blank, B.
and Ganioglu, E.
and Gelletly, W.
and Orrigo, S. E. A.",
title="The Tz = {\^A}{\textpm}1 {\^a}{\textdagger}{\textquoteright} 0 and {\^A}{\textpm}2 {\^a}{\textdagger}{\textquoteright}{\^A}{\textpm}1 Mirror Gamow{\^a}{\texteuro}{\textquoteleft}{\textquoteleft}Teller transitions in pf-shell nuclei",
journal="Acta Physica Polonica B",
year="2016",
publisher="Wydawnictwo Uniwersytetu Jagiellonskiego",
volume="47",
number="3",
pages="867--881",
abstract="Gamow-Teller (GT) transitions are the most common weak-interaction processes in the Universe. They play important roles in various processes of nucleosynthesis, for example, in the rapid proton-capture process (rp-process). In the pf-shell region, the rp-process runs through neutron-deficient nuclei with T-z = -2, -1, and 0 mainly by means of GT and Fermi transitions, where T-z is the z component of isospin T defined by T-z = (N = Z)/2. Under the assumption of isospin symmetry, mirror nuclei with reversed Z and N numbers, and thus with opposite signs of T-z, have the same structure. Therefore, symmetry is also expected for the GT transitions starting from and ending up in mirror nuclei. We have been studying the T-z = -2 -> -1 and -1 -> 0 GT transitions in beta decays, while those from stable T-z = +2 and +1 nuclei by means of hadronic (He-3; t) charge-exchange (CE) reactions. The results from these studies are compared in order to examine the mirror-symmetry structure in nuclei. In addition, these results are combined for the better understanding of GT transitions in the pf-shell region.",
optnote="WOS:000373495500033",
optnote="exported from refbase (https://references.ific.uv.es/refbase/show.php?record=2626), last updated on Fri, 29 Apr 2016 14:57:23 +0000",
issn="0587-4254",
doi="10.5506/APhysPolB.47.867",
opturl="https://doi.org/10.5506/APhysPolB.47.867",
language="English"
}