Lifetime of the recently identified 10+ isomeric state at 3279 keV in the Nd136 nucleus

A. Tucholski, Ch. Droste, J. Srebrny, C. M. Petrache, J. Skalski, P. Jachimowicz, M. Fila, T. Abraham, M. Kisieliński, A. Kordyasz, M. Kowalczyk, J. Kownacki, T. Marchlewski, P. J. Napiorkowski, L. Próchniak, J. Samorajczyk-Pyśk, A. Stolarz, A. Astier, B. F. Lv, E. Dupont, S. Lalkovski, P. Walker, E. Grodner, and Z. Patyk
Phys. Rev. C 100, 014330 – Published 31 July 2019

Abstract

Background: The γ softness of Nd136 makes it possible to study the shape changes induced by two-proton or two-neutron excitation.

Purpose: We measure the lifetimes of two-quasiparticle states of the bands based on the 10+ states at 3296 and 3279 keV to investigate the shape change induced by the alignment of two protons or two neutrons in the h11/2 orbital.

Methods: The recoil-distance Doppler shift method was used for the study of Nd136 studies, which was formed by the fusion reaction Sn120(Ne20,4n)Nd136, at Ebeam=85 MeV. Calculations were performed within the microscopic-macroscopic approach, based on the deformed Woods-Saxon single-particle potential and the Yukawa-plus-exponential macroscopic energy.

Results: The lifetime of the 10+ state at 3279 keV of Nd136 was measured to be T1/210+=1.63(9) ns. The lifetimes of the 2+ state at 374 keV and of the 12+ state at 3686 keV of the ground band were also measured to be T1/22+=26.5(14) ps and T1/212+=22.5(14) ps.

Conclusions: The measured lifetime of 10+ the state at 3279 keV together with other observables confirm the structure change in Nd136. A rather small reduced hindrance of the electromagnetic decay of the 10+ state at 3279 keV would be consistent with its K-mixed character.

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  • Received 6 June 2019

DOI:https://doi.org/10.1103/PhysRevC.100.014330

©2019 American Physical Society

Physics Subject Headings (PhySH)

Nuclear Physics

Authors & Affiliations

A. Tucholski1, Ch. Droste2, J. Srebrny1, C. M. Petrache3, J. Skalski4, P. Jachimowicz5, M. Fila2, T. Abraham1, M. Kisieliński1, A. Kordyasz1, M. Kowalczyk1, J. Kownacki1, T. Marchlewski1, P. J. Napiorkowski1, L. Próchniak1, J. Samorajczyk-Pyśk1, A. Stolarz1, A. Astier3, B. F. Lv3, E. Dupont3, S. Lalkovski6, P. Walker7, E. Grodner4, and Z. Patyk4

  • 1Heavy Ion Laboratory, University of Warsaw, Pasteura 5a, 02-093 Warsaw, Poland
  • 2Faculty of Physics, University of Warsaw, Pasteura 5, 02-093 Warszawa, Poland
  • 3Centre de Sciences Nuclaires et Sciences de la Matire, CNRS/IN2P3, Université Paris-Saclay, Batiment 104-108, 91405 Orsay, France
  • 4National Centre for Nuclear Research, Hoża 69, 00-681 Warsaw, Poland
  • 5Faculty of Physics and Astronomy, University of Zielona Gora, Licealna 9, 65-417 Zielona Gora, Poland
  • 6Nuclear Engineering, Faculty of Physics, Sofia University “St. Kl. Ohridski”, 5 James Bourchier Boulevard, Sofia 1164, Bulgaria
  • 7Department of Physics, University of Surrey, Guildford GU2 7XH, United Kingdom

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Issue

Vol. 100, Iss. 1 — July 2019

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