Penning trap mass spectrometry of neutron-rich Fe and Co isotopes around N=40 with the LEBIT mass spectrometer

R. Ferrer, M. Block, C. Bachelet, B. R. Barquest, G. Bollen, C. M. Campbell, M. Facina, C. M. Folden, III, C. Guénaut, A. A. Kwiatkowski, D. L. Lincoln, D. J. Morrissey, G. K. Pang, A. M. Prinke, R. Ringle, J. Savory, P. Schury, and S. Schwarz
Phys. Rev. C 81, 044318 – Published 29 April 2010

Abstract

Penning trap mass spectrometry is presented as a complementary tool to nuclear spectroscopy experiments for the study of nuclear structure in the vicinity of N=40, Z=28. High-precision mass measurements of the Fe6366 and Co6467 isotopes have been carried out with the Low Energy Beam and Ion Trap (LEBIT) Penning trap mass spectrometer. The newly obtained mass values for Fe66 and Co67 are presented, together with the previously reported LEBIT mass measurements in this region. In the case of Fe65 the existence of a new isomer is reported, and an isomer recently discovered by decay spectroscopy in Co67 is confirmed. Relative mass uncertainties as low as 4×108 are obtained. All mass values are found to be in good agreement with previous experimental results with the exception of Co64, where a 5σ deviation is observed. Using these data the two neutron separation energies S2n are calculated. However, the large error bars in the mass values of the neighbor Fe and Co isotopes with N>40 complicate the validation of a weak subshell closure at N=40 for the Co isotopes or the possible reduction in the neutron shell gap in the case of the Fe isotopes, in accordance with the theoretical predictions of an onset of deformation in the region.

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  • Received 15 January 2010

DOI:https://doi.org/10.1103/PhysRevC.81.044318

©2010 American Physical Society

Authors & Affiliations

R. Ferrer1,*, M. Block1,†, C. Bachelet1,‡, B. R. Barquest1,2, G. Bollen1,2, C. M. Campbell1, M. Facina1,§, C. M. Folden, III1,∥, C. Guénaut1,¶, A. A. Kwiatkowski1,2, D. L. Lincoln1,2, D. J. Morrissey1,3, G. K. Pang1,3, A. M. Prinke1,2, R. Ringle1,2, J. Savory1,2,**, P. Schury1,2,††, and S. Schwarz1

  • 1National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
  • 2Department of Physics and Astronomy, East Lansing, Michigan 48824, USA
  • 3Department of Chemistry, East Lansing, Michigan 48824, USA

  • *Ferrer@nscl.msu.edu
  • Present address: GSI, Planckstrasse 1, D-64291 Darmstadt, Germany.
  • Present address: CSNSM-IN2P3/CNRS, Bat. 108 Université de Paris Sud, F-91405 Orsay, France.
  • §Present address: Bubble Technology Industries, Chalk River, Ontario, Canada.
  • Present address: Cyclotron Institute, Texas A&M University, College Station, Texas 77843-3366, USA.
  • Present address: Comissariat á l’Energie Atomique, CEA-Saclay, F-91191 Gif sur Yvette Cedex, France.
  • **Present address: B238 NHMFL FSU, 1800 East Paul Dirac Drive, Tallahassee, Florida 32310-3706, USA.
  • ††Present address: Tsukuba University, Tennoudai 1-1-1, Ibaraki, Japan.

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Vol. 81, Iss. 4 — April 2010

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