Guttormsen, M.; Atac, A.; Ingebretsen, F.; Messelt, S.; Olsen, J.; Ramsoey, T.; Rekstad, J.; Roenning, L.A.; Loevhoeiden, G.; Roedland, T.; Thorsteinsen, T.F.
Oslo Univ. (Norway). Fysisk Inst1985
Oslo Univ. (Norway). Fysisk Inst1985
AbstractAbstract
[en] The γ-decay following the 27Al(tau,α), 27Al(tau,tau) and 27Al(tau,t) reactions has been studied using Esub(tau) = 45 MeV. For all three reactions a maximum mean γ-ray multiplicity of < Msub(γ)> = 1.8 +- 0.2 is observed in good agreement with the Fermi gas model. The variation of < Msub(γ)>with excitation energy for the 27Al(tau,tau)27Al reaction, however, shows considerable deviations from the decay pattern expected for a statistical system. From a comparison with other reaction channels, it is suggested that the selectivity in the excitation of states in the inelastic process is responsible for this non-statistical pattern
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Dec 1985; 27 p
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ALUMINIUM ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, CHARGED PARTICLES, DECAY, ELEMENTARY PARTICLES, ENERGY LEVELS, ENERGY RANGE, EVEN-ODD NUCLEI, FERMIONS, HEAVY LEPTONS, HELIUM IONS, IONIZING RADIATIONS, IONS, ISOTOPES, LEPTONS, LIGHT NUCLEI, MATHEMATICAL MODELS, MEV RANGE, NUCLEAR DECAY, NUCLEAR MODELS, NUCLEAR REACTIONS, NUCLEI, ODD-ODD NUCLEI, RADIATIONS, RADIOISOTOPES, SECONDS LIVING RADIOISOTOPES, SILICON ISOTOPES, TARGETS, YEARS LIVING RADIOISOTOPES
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AbstractAbstract
[en] The γ-decay following the 27Al(tau,α), 27Al(tau,tau) and 27Al(tau,t) reactions has been studied using Esub(tau)=45 Mev. For all three reactions a maximum mean γ-ray multiplicity of < Mγ>=1.8+-0.2 is observed, in good agreement with the Fermi gas model. The variation of < Msub(γ)> with excitation energy for the 27Al(tau,tau)27Al reaction, however, shows considerable deviations from the decay pattern expected for a statistical system. From a comparison with other reaction channels, we suggest that the selectivity in the excitation of states in the inelastic process is responsible for this non-statistical pattern. (orig).
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