Physics Letters B (Aug 2024)

The shape of the Tz = +1 nucleus 94Pd and the role of proton-neutron interactions on the structure of its excited states

  • A. Yaneva,
  • S. Jazrawi,
  • M. Mikołajczuk,
  • M. Górska,
  • P.H. Regan,
  • B. Das,
  • H.M. Albers,
  • S. Alhomaidhi,
  • T. Arici,
  • A. Banerjee,
  • G. Benzoni,
  • B. Cederwall,
  • M.M.R. Chishti,
  • D.D. Dao,
  • T. Davinson,
  • A. Gargano,
  • J. Gerl,
  • O. Hall,
  • N. Hubbard,
  • J. Jolie,
  • I. Kojouharov,
  • A.K. Mistry,
  • F. Nowacki,
  • M. Polettini,
  • M. Rudigier,
  • E. Şahin,
  • H. Schaffner,
  • A. Sharma,
  • M. Armstrong,
  • H.J. Wollersheim,
  • P. Boutachkov,
  • T. Dickel,
  • E. Haettner,
  • H. Heggen,
  • Ch. Hornung,
  • R. Knöbel,
  • D. Kostyleva,
  • N. Kurz,
  • N. Kuzminchuk,
  • I. Mukha,
  • S. Pietri,
  • W.R. Plass,
  • Zs. Podolyák,
  • C. Scheidenberger,
  • Y.K. Tanaka,
  • J. Vesic,
  • H. Weick,
  • U. Ahmed,
  • Ö. Aktas,
  • A. Algora,
  • C. Appleton,
  • J. Benito,
  • A. Blazhev,
  • A. Bracco,
  • A.M. Bruce,
  • M. Brunet,
  • R. Canavan,
  • A. Esmaylzadeh,
  • L.M. Fraile,
  • G. Häfner,
  • K.P. Hucka,
  • P.R. John,
  • D. Kahl,
  • V. Karayonchev,
  • R. Kern,
  • G. Košir,
  • R. Lozeva,
  • P. Napiralla,
  • B.S. Nara Singh,
  • R. Page,
  • C.M. Petrache,
  • N. Pietralla,
  • J.-M. Régis,
  • H. Rösch,
  • P. Ruotsalainen,
  • V. Sanchez-Temble,
  • L. Sexton,
  • R. Shearman,
  • M. Si,
  • V. Werner,
  • J. Wiederhold,
  • K. Wimmer,
  • W. Witt,
  • P. Woods,
  • G. Zimba

Journal volume & issue
Vol. 855
p. 138805

Abstract

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Reduced transition probabilities have been extracted between excited, yrast states in the N=Z+2 nucleus 94Pd. The transitions of interest were observed following decays of the Iπ=14+, Ex=2129-keV isomeric state, which was populated following the projectile fragmentation of a 124Xe primary beam at the GSI Helmholtzzentrum für Schwerionenforschung accelerator facility as part of FAIR Phase-0. Experimental information regarding the reduced E2 transition strengths for the decays of the yrast 8+ and 6+ states was determined following isomer-delayed Eγ1−Eγ2−△T2,1 coincidence method, using the LaBr3(Ce)-based FATIMA fast-timing coincidence gamma-ray array, which allowed direct determination of lifetimes of states in 94Pd using the Generalized Centroid Difference (GCD) method. The experimental value for the half-life of the yrast 8+ state of 755(106) ps results in a reduced transition probability of B(E2:8→+6+) = 205−25+34 e2fm4, which enables a precise verification of shell-model calculations for this unique system, lying directly between the N=Z line and the N=50 neutron shell closure. The determined B(E2) value provides an insight into the purity of (g9/2)n configurations in competition with admixtures from excitations between the (lower) N=3pf and (higher) N=4gds orbitals for the first time. The results indicate weak collectivity expected for near-zero quadrupole deformation and an increasing importance of the T=0 proton-neutron interaction at N=48.

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