The fully energy-damped yields for the 36 Ar ϩ 12 C and 20 Ne ϩ 28 Si reactions at E c.m. ϭ47.0 MeV and 45.5 MeV, respectively, are explored using particle-particle-␥ coincidence data. These reactions reach a similar excitation energy of E CN * ϭ59.5 MeV in the 48 Cr compound nucleus as was obtained in an earlier particleparticle coincidence study of the 24 Mg ϩ 24 Mg reaction. The overall mass and total kinetic energy distributions of the fission fragments are found to be well reproduced by statistical-model calculations. These calculations are also found to reproduce structure seen in the excitation-energy spectra for the 20 Ne ϩ 28 Si and 24 Mg ϩ 24 Mg exit channels for all three reactions. In previous excitation-function measurements, strong heavy-ion resonance behavior has been observed in elastic and inelastic cross sections for the 24 Mg ϩ 24 Mg system. There has been speculation that peaks observed in the corresponding excitation-energy spectra at more negative Q values may also be a consequence of this resonance phenomenon. The observation of very similar behavior with the asymmetric-mass entrance channels makes it less likely, though, that the peaks arise from any special configuration of the compound system. Instead, an analysis of the ␥-ray data and the results of statistical-model calculations support the conclusion that most of the observed high-lying structure can be accounted for in terms of statistical fission from a fully energy-and shape-equilibrated compound nucleus. For the 24 Mg ϩ 24 Mg entrance channel, however, comparisons with the statistical model indicate a reduction of high-angular-momentum partial cross sections, leading to the 24 Mg ϩ 24 Mg fission channel. For the first time, we are able to deduce the nature of the competition between the resonance and statistical-fission mechanisms in this mass region. ͓S0556-2813͑96͒03109-3͔
Statistical y-decay spectra from excited nuclear states are calculated.The spectra reflect the perturbation of the level density by pair correlations and, hence, the stepwise weakening of the pair correlations with increasing quasiparticle number. The level density is obtained by counting manyquasiparticle states from a self-consistent BCS calculation or from a diagonalization of particle numberprojected states. The calculated spectra resemble measured spectra from the decay out of superdeformed bands, but have only -70% of the measured intensity. PACS numbers: 21.10.Ma, 21.60.Ka, 23.20.Lv, 27.80.+w Pair correlations are essential for describing many properties of the low-lying states of nuclei. By applying methods developed to describe superAuidity and superconductivity in condensed matter physics, one can explain the observed moments of inertia of ground state rotational bands, as well as the occurrence of a gap in the energy spectrum of even nuclei between the ground and excited states [1]. With increasing temperature, pair correlations become weaker, and are finally completely quenched, in analogy with the superAuid to normal phase transition in liquids. Because of the mesoscopic (i.e., finite) nature of the nucleus, pairing correlations can be appreciably re-
The single-particle character of states outside the doubly magic (radioactive) nucleus 56 Ni has been determined through a measurement of the ͑d, p͒ neutron transfer reaction using inverse kinematics. From the spectroscopic factors of the low-lying states in 57 Ni, the astrophysically interesting yield for the 56 Ni͑p, g͒ reaction to the mirror nucleus 57 Cu has been calculated, utilizing charge symmetry. The rate for this reaction in the temperature range typical of novae, supernovae, and x-ray bursts is found to be more than 10 times higher than previously assumed. [S0031-9007 (97)05085-0]
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