γ Rays Following Neutron Capture in U235 and the Spins of U235 Resonances

R. G. Graves, R. E. Chrien, D. I. Garber, G. W. Cole, and O. A. Wasson
Phys. Rev. C 8, 781 – Published 1 August 1973
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Abstract

Capture and fission γ rays from epithermal neutron irradiation of U235 have been identified. The capture γ rays were used to construct a level diagram for U236 and to determine the spins of the U235 resonances. Coincidence γ-ray spectra, taken with a large 4π fission neutron detector and Ge(Li) crystal were used to identify prompt-fission γ rays. This apparatus was also used to suppress the background of prompt-fission γ rays in the resonance spectra and to increase the probability of seeing capture γ rays.

Energies of high-energy γ rays identified as due to resonant neutron capture in U235 are 6396, 5588, 5546, 5487, 5417, and 5292 keV; these populate excited states in U236 at 149, 957, 999, 1058, 1128, and 1253 keV. Many of the 14 low-energy γ rays identified as capture have been assigned as those representing transitions between these low-lying excited states. On the basis of observing the 5588-keV γ ray, which populates a 2+ final state in U236, the spin-parity of the 2.040-, 12.39-, 14.53-, and 32.05-eV resonances have been assigned as 3. We assigned 4 to resonances at 11.67 and 16.10 eV by placing a 5+ state at 1128 keV. From the work of Schermer et al. and our 3 assignment for the 2.040-eV resonance, we conclude that the 0.290- and 1.14-eV resonances are 3 and 4, respectively.

On the basis of level systematics in even uranium isotopes and our high- and low-energy capture γ rays, we propose that the 1128-keV level in U236 is most likely the 5+ member of the Kπ, Jπ=2+, 2+ γ-vibrational band.

[NUCLEAR REACTIONS U235 measured Iγ, slow neutrons (n,γ) (n,F); deduced J U235 resonances 0-30 eV, U236 levels to 1300 keV, delayed-, prompt-fission γ's.]

  • Received 5 March 1973

DOI:https://doi.org/10.1103/PhysRevC.8.781

©1973 American Physical Society

Authors & Affiliations

R. G. Graves*, R. E. Chrien, D. I. Garber, G. W. Cole, and O. A. Wasson

  • Brookhaven National Laboratory, Upton, New York 11973

  • *Based, in part, on a doctoral dissertation submitted by R. G. Graves to State University of New York at Stony Brook, Stony Brook, New York. Present address: Cyclotron Institute, Texas A & M University, College Station, Texas.

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Vol. 8, Iss. 2 — August 1973

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