• Letter

Nuclear rotation at the fission limit in Rf254

D. Seweryniak, T. Huang, K. Auranen, A. D. Ayangeakaa, B. B. Back, M. P. Carpenter, P. Chowdhury, R. M. Clark, P. A. Copp, Z. Favier, K. Hauschild, X.-T. He, T. L. Khoo, F. G. Kondev, A. Korichi, T. Lauritsen, J. Li, C. Morse, D. H. Potterveld, G. Savard, S. Stolze, J. Wu, J. Zhang, and Y.-F. Xu
Phys. Rev. C 107, L061302 – Published 9 June 2023

Abstract

A ground-state rotational band in the fissile nucleus Rf254 was observed for the first time. Levels up to spin 14 and excitation energy of 1.56 MeV were observed. The Rf254 nuclei were produced using the Pb206(Ti50,2n) fusion-evaporation reaction. It is the weakest reaction channel ever studied using in-beam γ-ray spectroscopic methods. The reaction products were separated from the beam in the Argonne gas-filled analyzer (AGFA). The Rf254 nuclei were implanted into a double-sided Si strip detector at the AGFA focal plane and tagged with subsequent ground-state spontaneous fission decays using temporal and spatial correlations. Prompt γ rays in coincidence with the Rf254 recoils were detected in the Gammasphere array of Ge detectors. In order to identify the ground-state rotational band in Rf254, a method for identifying rotational bands in low statistics γ-ray spectra was developed. The deduced Rf254 kinematic moment of inertia is smaller compared to neighboring even-even nuclei. This is most likely associated with a slightly lower quadrupole deformation and stronger pairing correlations in Rf254. The behavior of the moment of inertia as a function of rotational frequency is similar to that of the lighter N=150 isotones Fm250 and No252.

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  • Received 19 January 2022
  • Revised 5 April 2023
  • Accepted 9 May 2023

DOI:https://doi.org/10.1103/PhysRevC.107.L061302

©2023 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

Authors & Affiliations

D. Seweryniak1,*, T. Huang1,2, K. Auranen1, A. D. Ayangeakaa3,4, B. B. Back1, M. P. Carpenter1, P. Chowdhury5, R. M. Clark6, P. A. Copp1, Z. Favier7, K. Hauschild8, X.-T. He9, T. L. Khoo1, F. G. Kondev1, A. Korichi8, T. Lauritsen1, J. Li1, C. Morse6, D. H. Potterveld1, G. Savard1, S. Stolze1, J. Wu1, J. Zhang10, and Y.-F. Xu9

  • 1Argonne National Laboratory, Argonne, Illinois 60439, USA
  • 2Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China
  • 3University of North Carolina, Chapel Hill, North Carolina 27599, USA
  • 4Triangle Universities Nucelar Laboratory, Duke University, Durham, North Carolina 27708, USA
  • 5University of Massachusetts, Lowell, Massachusetts 01854, USA
  • 6Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
  • 7CEA, Département de Physique Nucléaire, Université Paris-Saclay, 91191, Gif-sur-Yvette, France
  • 8CNRS, IJCLab, Université Paris-Saclay, 91405, Orsay, France
  • 9College of Materials Science and Technology, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China
  • 10College of Physics, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China

  • *seweryniak@anl.gov

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Vol. 107, Iss. 6 — June 2023

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