Bibcode
Beck, C.; Rowley, N.; Rousseau, M.; Haas, F.; Bednarczyk, P.; Courtin, S.; Kintz, N.; Hoellinger, F.; Papka, P.; Szilner, S.; Zafra, A. Sanchez I; Hachem, A.; Martin, E.; Stezowski, O.; Diaz-Torres, A.; Souza, F. A.; Szanto De Toledo, A.; Aissaoui, A.; Carlin, N.; Liguori Neto, R.; Munhoz, M. G.; Takahashi, J.; Suade, A. A. P.; De Moura, M. M.; Szanto, E. M.; Hagino, K.; Thompson, I. J.
Bibliographical reference
eprint arXiv:nucl-ex/0411002
Advertised on:
11
2004
Citations
10
Refereed citations
4
Description
The influence on the fusion process of coupling to collective degrees of
freedom has been explored. The significant enhancement of he fusion
cross setion at sub-barrier energies was understood in terms of the
dynamical processes arising from strong couplings to collective
inelastic excitations of the target and projectile. However, in the case
of reactions where breakup becomes an important process, conflicing
model predictions and experimental results have been reported in the
literature. Excitation functions for sub- and near-barrier total
(complete + incomplete) fusion cross sections have been measured for the
$^{6,7}$Li + $^{59}$Co at the Vivitron facility and at the 8UD Pelletron
tandem facility using standard $gamma$-ray techniques. The data extend
to medium-mass systems previous works exploring the coupling effects in
fusion reactions of both lighter and heavier systems. Results of
continuum-discretized coupled channel (CDCC) calculations indicate a
small enhancement of total fusion for the more weakly bound $^{6}$Li at
sub-barrier energies, with similar cross sections for both reactions at
and above the barrier. A systematic study of $^{4,6}$He induced fusion
reactions with the CDCC method is in progress. The understanding of the
reaction dynamics involving couplings to the breakup channels requires
th explicit measurement of precise elastic scattering data as well as
yields leading to the breakup itself. Recent coincidence experiments for
$^{6,7}$Li + $^{59}$Co are addressing this issue. The particle
identification of the breakup products have been achieved by measuring
the three-body final-state correlations.