On-line mass separator investigation of the new isotope 2.9-sec I116

G. M. Gowdy, A. C. Xenoulis, J. L. Wood, K. R. Baker, R. W. Fink, J. L. Weil, B. D. Kern, K. J. Hofstetter, E. H. Spejewski, R. L. Mlekodaj, H. K. Carter, W. D. Schmidt-Ott, J. Lin, C. R. Bingham, L. L. Riedinger, E. F. Zganjar, K. S. R. Sastry, A. V. Ramayya, and J. H. Hamilton
Phys. Rev. C 13, 1601 – Published 1 April 1976
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Abstract

Using on-line mass separation I116 has been identified and its half-life determined to be 2.91 ± 0.15 sec. The activity was produced by the Rh103(O16,3n)I116 reaction and by the decay of 57-sec Xe116. The I116 decays primarily to the ground state of Te116 and also to excited states at 678.9 and 1219.1 keV. From positron measurements, a decay energy of QEC=7.71±0.20 MeV is assigned to I116. γ rays of 540.2 and 678.9 keV are observed in this decay and are assigned to depopulate levels in Te116 at 1219.1 and 678.9 keV, respectively. The former is a new level with a probable spin-parity of either 2+ or 0+. From the logft values, a spinparity assignment of 1+ is deduced for the ground state of I116, which is interpreted to have a configuration of [π(d52)ν(d32)]. A decay energy of QEC=4.34±0.20 MeV observed from activity produced by the Pd104 + O16 reaction is assigned to Xe116.

NUCLEAR REACTIONS Rh103(O16,3nγ), E=83 MeV; Pd104(O16,4nγ) and Pd104(O16,p3nγ), E=91 MeV. Natural Rh targets and enriched Pd targets. RADIOACTIVITY I116, Xe116; measured Eγ, Iγ, T12(γ), T12(β+), β+γ coin., β+ end point; Te116 deduced levels, J, π, logft; I116 deduced ground state J, π, logft; Ge(Li) detectors and plastic scintillators; mass separated sources.

  • Received 8 September 1975

DOI:https://doi.org/10.1103/PhysRevC.13.1601

©1976 American Physical Society

Authors & Affiliations

G. M. Gowdy, A. C. Xenoulis*,‡, J. L. Wood, K. R. Baker†,‡, and R. W. Fink

  • School of Chemistry, Georgia Institute of Technology, Atlanta, Georgia 30332

J. L. Weil, B. D. Kern, and K. J. Hofstetter‡,§

  • University of Kentucky, Lexington, Kentucky 40506

E. H. Spejewski, R. L. Mlekodaj, H. K. Carter, and W. D. Schmidt-Ott∥,¶

  • UNISOR, Oak Ridge, Tennessee 37830

J. Lin

  • Tennessee Technological University, Cookeville, Tennessee 38501

C. R. Bingham and L. L. Riedinger

  • University of Tennessee, Knoxville, Tennessee 37916

E. F. Zganjar

  • Louisiana State University, Baton Rouge, Louisiana 70803

K. S. R. Sastry

  • University of Massachusetts, Amherst, Massachusetts 01002

A. V. Ramayya** and J. H. Hamilton**

  • Vanderbilt University, Nashville, Tennessee 37235

  • *Present address: Department of Physics, Demokritos Nuclear Research Center, Athens, Greece.
  • Present address: U. S. Energy Research and Development Administration, Division of Operational Safety, Mail Stop E-166, Washington, D. C. 20545.
  • Work supported in part by the U. S. Energy Research and Development Administration.
  • §Present address: Allied General Nuclear Services, Barnwell, South Carolina 29812.
  • Present address: II. Physikalisches Institut der Universität Gättingen, Göttingen, Germany.
  • UNISOR is a consortium of the University of Alabama at Birmingham, Emory University, Furman University, Georgia Institute of Technology, University of Kentucky, Louisiana State University, University of Massachusetts, Oak Ridge National Laboratory, Oak Ridge Associated Universities, University of South Carolina, University of Tennessee, Tennessee Technological University, Vanderbilt University, and Virginia Polytechnic Institute. It is supported by them and by the U. S. Energy Research and Development Administration.
  • **Work supported in part by a grant from the National Science Foundation.

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Vol. 13, Iss. 4 — April 1976

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