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On the decay of compound nuclei following alpha-particle and12C induced reactions
Authors:S. A. Hjorth  A. Johnson  A. Kerek  W. Klamra  Th. Lindblad  S. Messelt  C. Pomar  W. Walus  Ö. Skeppstedt  Z. Sujkowski  A. Zglinski  L. Carlén  H. Ryde  M. Piiparinen
Affiliation:1. Research Institute of Physics, Stockholm, Sweden
5. Chalmers University of Technology, Gothenburg, Sweden
6. Institute of Nuclear Research, Swierk, Poland
7. Department of Physics, University of Lund, Lund, Sweden
8. Department of Physics, University of Jyv?skyl?, Jyv?skyl?, Finland
Abstract:Multiple coincidence rates have been measured using a detector system consisting of a Ge(Li) spectrometer and eight NaI(Tl) or eight liquid scintillators. Reactions induced byα-particles with energies of 51–55 MeV and 118 MeV12C ions are studied. The data are analysed to give the first and second central moments of the distribution of the number ofγ-rays feeding individual levels in the final nuclei. When these numbers are compared to spin distributions calculated with the statistical model code GROGI the relative importance of dipole and quadrupole deexcitation modes can be ascertained. In particular, in the122Te(α, 4n)122Xe reaction theγ-decay prior to the entry into the ground band is well described as a statistical process proceeding to 50% by dipole and 50% by quadrupole radiation. In the166Er(α,4n)166Yb and192Os(α,4n)192Pt reactions the relative amount of quadrupole radiation is larger and it seems that the dipole and quadrupole decay takes place via separate cascades. In the164Dy(12C, 7-8n) reactions the average multiplicity is independent of spin, suggesting that the nucleus forgets the spin of the entry state before the process enters into the ground band. In the176Yb(12C, 8n)180Os reaction, finally, the nucleus definitely retains memory of the entry state during the decay. In this last case the multiplicity measurement is combined with aγ-ray singles measurement to give an average excitation energy prior to theα-decay and the average moment of inertia characterising the decay of the high-spin states.
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