Abstract
Excited states of the neutron-rich niobium isotopes 96,97,98,9941Nb have been populated in two experiments which used fusion-fission and multinucleon binary grazing reactions to populate high-spin yrast states. In the multinucleon-transfer experiment, a 530-MeV beam of 96Zr ions was incident on a thin 124Sn target; projectile-like ejectiles were detected and identified using the PRISMA magnetic spectrometer and the associated 𝛾 rays were detected using the CLARA array of Ge detectors. In the second experiment, the GASP array of escape-suppressed Ge detectors was used to detect 𝛾 rays from fusion-fission products formed following the interaction of a 230-MeV beam of 36S ions with a thick target of 176Yb . Level schemes of 96,97,99Nb were established up to excitation energies of 4545, 5409, and 3814 keV, respectively; states with proposed spin values up to about 15 ℏ were populated. Gamma-ray photopeaks corresponding to transitions in 98Nb were also observed in the PRISMA-CLARA experiment; however, it was not possible, in this case, to produce a level scheme based on 𝛾-ray coincidence data from the GASP experiment. For 96Nb and 97Nb , the level schemes are in agreement with the results of earlier publications. Two new decay sequences have been populated in 99Nb ; tentative 𝐽𝜋 values of the hitherto unobserved states have been assigned through comparisons with 𝐽𝜋 values of neighboring nuclei. In contrast with earlier published studies of the high-spin spectroscopy of 96Nb
and 97Nb , the present work provides an unambiguous association of the observed 𝛾 rays with the 𝐴 and 𝑍 of the excited nucleus. The structure of the yrast states of 96,97,99Nb is discussed within the context of shell-model calculations. The experimental results, supported by model calculations, indicate the first observation of shape coexistence at low spin and low excitation energy in the 𝑁=58 nucleus 99Nb . The results of TRS calculations indicate that the 9/2+ ground state is triaxial, tending to oblate shapes with a transition to a more deformed prolate shape beyond the 17/2+ member of the decay sequence; here the sequence has been observed to (29/2+). On the other hand, the previously unobserved decay sequence based on the 5/2− state at 631 keV exhibits the characteristics of a rotational sequence and has been assigned Nilsson quantum numbers 5/2−[303]. TRS calculations indicate that the 5/2−[303] band is gamma soft and this is consistent with the inability of the particle-rotor model to reproduce the observed behavior of the signature-splitting function.
and 97Nb , the present work provides an unambiguous association of the observed 𝛾 rays with the 𝐴 and 𝑍 of the excited nucleus. The structure of the yrast states of 96,97,99Nb is discussed within the context of shell-model calculations. The experimental results, supported by model calculations, indicate the first observation of shape coexistence at low spin and low excitation energy in the 𝑁=58 nucleus 99Nb . The results of TRS calculations indicate that the 9/2+ ground state is triaxial, tending to oblate shapes with a transition to a more deformed prolate shape beyond the 17/2+ member of the decay sequence; here the sequence has been observed to (29/2+). On the other hand, the previously unobserved decay sequence based on the 5/2− state at 631 keV exhibits the characteristics of a rotational sequence and has been assigned Nilsson quantum numbers 5/2−[303]. TRS calculations indicate that the 5/2−[303] band is gamma soft and this is consistent with the inability of the particle-rotor model to reproduce the observed behavior of the signature-splitting function.
Original language | English |
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Article number | 044313 |
Journal | Physical Review C |
Volume | 108 |
DOIs | |
Publication status | Published - 19 Oct 2023 |