Fusion Hindrance and Pauli Blocking in 58 Ni + 64 Ni

58 Ni + 64 Ni is the first case where the influence of positive Q-value transfer channels on sub-barrier fusion was evidenced, in a very well known experiment by Beckerman et al., by comparing with the two systems 58 Ni + 58 Ni and 64 Ni+ 64 Ni. Subsequent measurements on 64 Ni + 64 Ni showed that f...

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Published in:EPJ Web of conferences Vol. 223; p. 1062
Main Authors: Stefanini, Alberto M., Montagnoli, Giovanna, Del Fabbro, Mirco, Colucci, Giulia, Čolović, Petra, Corradi, Lorenzo, Fioretto, Enrico, Galtarossa, Franco, Goasduff, Alain, Grebosz, Jerzy, Heine, Marcel, Jaworski, Grzegorz, Mazzocco, Marco, Mijatović, Tea, Szilner, Suzana, Bajzek, Martin, Brugnara, Daniele, Siciliano, Marco, Zanon, Irene
Format: Journal Article
Language:English
Published: 2019
Online Access:Get full text
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Summary:58 Ni + 64 Ni is the first case where the influence of positive Q-value transfer channels on sub-barrier fusion was evidenced, in a very well known experiment by Beckerman et al., by comparing with the two systems 58 Ni + 58 Ni and 64 Ni+ 64 Ni. Subsequent measurements on 64 Ni + 64 Ni showed that fusion hindrance is clearly present in this case. On the other hand, no indication of hindrance can be observed for 58 Ni + 64 Ni down to the measured level of 0.1 mb. In the present experiment the excitation function has been extended by two orders of magnitude downward. The cross sections for 58 Ni + 64Ni continue decreasing very smoothly below the barrier, down to '1 µb. The logarithmic slope of the excitation function increases slowly, showing a tendency to saturate at the lowest energies. No maximum of the astrophysical S -factor is observed. Coupled-channels (CC) calculations using a Woods-Saxon potential and includinginelastic excitations only, underestimate the sub-barrier cross sections by a large amount. Good agreement is found by adding two-neutron transfer couplings to a schematical level. This behaviour is quite different from what already observed for 64 Ni+ 64 Ni (no positive Q -value transfer channels available), where a clear low-energy maximum of the S -factorappears, and whose excitation function is overestimated by a standard Woods-Saxon CC calculation. No hindrance effect is observed in 58 Ni+ 64 Ni in the measured energy range. This trend at deep sub-barrier energies reinforces the recent suggestion that the availability of several states following transfer with Q >0, effectively counterbalances the Pauli repulsion that, in general, is predicted to reduce tunneling probability inside the Coulomb barrier.
ISSN:2100-014X
2100-014X
DOI:10.1051/epjconf/201922301062