By Ulrich Mosel (auth.), D. Allan Bromley (eds.)
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Additional info for Treatise on Heavy-Ion Science: Volume 2: Fusion and Quasi-Fusion Phenomena
16) with rUt = I If.!. 12) in the barrier region. The low-energy data up to the bend in Ufus vs. m . are thus insensitive to the particular type of dissipation. They are instead determined by the conservative potentials alone. Use of a "reasonable" nucleus-nucleus potential (such as the proximity potential) thus ensures agreement with experiment. 3. Fusion cross sections for the three reactions 16,]7, 18 0 + 27Al at low energies. The lines illustrate the 1/ Ecru. behavior [from Eisen et al. (Ei 77)].
Use of a "reasonable" nucleus-nucleus potential (such as the proximity potential) thus ensures agreement with experiment. 3. Fusion cross sections for the three reactions 16,]7, 18 0 + 27Al at low energies. The lines illustrate the 1/ Ecru. behavior [from Eisen et al. (Ei 77)]. low-energy data. m : The intersect with the l/E axis then gives VB while RBis determined by the slope. This is the type of analysis first performed by Gutbrod et al. (Gu 73). This method has later been refined by Bass (Ba 77a), who takes the fact into account that the location of the interaction barrier will depend on I.
One is the appearance of resonancelike structures in the fusion cross section. These have been observed so far only in reactions involving combinations of 12C and 16 0. With the recent observations of resonance structures in elastic and inelastic channels in heavier systems like 28Si + 28Si (Be 79, Di Sl) it is a natural challenge to look with increased sensitivity also back into the fusion cross sections for these nuclei. It would be extremely interesting to learn about the possible connection of resonant states of the (A p + AT) system with the doorway states to fusion and to identify these latter.
Treatise on Heavy-Ion Science: Volume 2: Fusion and Quasi-Fusion Phenomena by Ulrich Mosel (auth.), D. Allan Bromley (eds.)