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Heavy ion reactions around the Coulomb barrier
The angular distributions of fission fragments for the 32 S+ 184 W reaction near Coulomb barrier energies are measured. The experimental fission excitation function is obtained. The measured fission cross sections are decomposed into fusion-fission, quasi-fission and fast fission contributions by th...
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Published in: | Science China. Physics, mechanics & astronomy mechanics & astronomy, 2011-08, Vol.54 (Suppl 1), p.6-13 |
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Main Authors: | , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The angular distributions of fission fragments for the
32
S+
184
W reaction near Coulomb barrier energies are measured. The experimental fission excitation function is obtained. The measured fission cross sections are decomposed into fusion-fission, quasi-fission and fast fission contributions by the dinuclear system (DNS) model. The hindrance to completing fusion both at small and large collision energies is explained. The fusion excitation functions of
32
S+
90,96
Zr in an energy range from above to below the Coulomb barrier are measured and analyzed within a semi-classical model. The obvious effect of positive
Q
-value multi-neutron transfers on the sub-barrier fusion enhancement is observed in the
32
S+
96
Zr system. In addition, the excitation functions of quasi-elastic scattering at a backward angle have been measured with high precision for the systems of
16
O +
208
Pb,
196
Pt,
184
W, and
154,152
Sm at energies well below the Coulomb barrier. Considering the deformed coupling effects, the extracted diffuseness parameters are close to the values extracted from the systematic analysis of elastic and inelastic scattering data. The elastic scattering angular distribution of
17
F+
12
C at 60 MeV is measured and calculated by using the continuum-discretized coupled-channels (CDCC) approach. It is found that the diffuseness parameter of the real part of core-target potential has to be increased by 20% to reproduce the experimental result, which corresponds to an increment of potential depth at the surface region. The breakup cross section and the coupling between breakup and elastic scattering are small. |
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ISSN: | 1674-7348 1869-1927 |
DOI: | 10.1007/s11433-011-4419-5 |