Jul 26–31, 2026
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Nuclear structure of 94Pd at transition-point between the isoscalar and isovector characteristics

Jul 28, 2026, 6:24 p.m.
1m
Fletcher Challenge Canada (Simon Fraser University Harbour Centre)

Fletcher Challenge Canada

Simon Fraser University Harbour Centre

515 West Hastings St, Vancouver, B.C. V6B 5K3
Posters Poster Session

Speaker

Youngseub Jang (Korea University, Center for Exotic Nuclear Studies, Institute for Basic Science)

Description

Nuclei near the doubly magic nucleus $^{100}$Sn ($N=Z=50$) have been extensively studied to investigate nuclear structure, including shell evolution, seniority effects, and proton–neutron interactions. In this work, $^{94}$Pd with $N=Z+2$ was investigated with a focus on isovector($T=1$) and isoscalar($T=0$) neutron-proton pairing using the fast-timing measurement. Half-lives of yrast excited states in $^{94}$Pd were measured using isomeric decay spectroscopy. The experiment was performed at RIBF (Radioactive Isotope Beam Factory), RIKEN, where $^{94}$Pd ions were produced via in-flight fragmentation of a $^{124}$Xe beam impinging on a $^{9}$Be target. These ions were implanted into the GARi active stopper array, and isomeric delayed $\gamma$ rays were detected with the IDATEN fast-timing array consisting of 48 LaBr$_{3}$(Ce) detectors. The half-lives were determined using the generalized centroid difference method, yielding the $T_{1/2}$ values of $\leq 15$ ps, $13(11)$ ps, $\leq 13$ ps, $693(72)$ ps, and $\leq 19$ ps for the $(2^{+}_{1})$, $(4^{+}_{1})$, $(6^{+}_{1})$, $(8^{+}_{1})$, and $(10^{+}_{1})$ states, respectively. The half-lives of the $(2^{+}_{1})$, $(4^{+}_{1})$ and $(10^{+}_{1})$ states are reported here for the first time, and the uncertainties of the half-lives of the $(6^{+}_{1})$ and $(8^{+}_{1})$ states have been improved compared to previous measurements. Reduced transition probabilities $B(E2)$ were deduced from the measured half-lives and discussed in the context of shell-model calculations employing the JUN45 effective interaction, including $T=0$, $T=1$ and full interaction. The results suggest that $^{94}$Pd, with $N=Z+2$, lies in a transitional regime between the $N=Z$ isoscalar-pairing domain ($^{92}$Pd) and the $N=50$ isovector-dominated region ($^{96}$Pd).

Author

Youngseub Jang (Korea University, Center for Exotic Nuclear Studies, Institute for Basic Science)

Co-authors

Dr Byul Moon (Center for Exotic Nuclear Studies, Institute for Basic Science) Prof. Byungsik Hong (Korea University) Dr Hiroshi Watanabe (Center for Exotic Nuclear Studies, Institute for Basic Science) Mr Jaehwan Lee (Korea University, Center for Exotic Nuclear Studies, Institute for Basic Science) Dr Shunji Nishimura (RIKEN Nishina Center)

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