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dc.contributor.authorDeb, N. K.-
dc.contributor.authorKalita, K.-
dc.contributor.authorRashid, H. I.-
dc.contributor.authorNath, S.-
dc.contributor.authorGehlot, J.-
dc.contributor.authorMadhavan, N.-
dc.contributor.authorBiswas, R.-
dc.contributor.authorSahoo, R. N.-
dc.contributor.authorGiri, P. K.-
dc.contributor.authorDas, A.-
dc.contributor.authorRajbongshi, T.-
dc.contributor.authorParihari, A.-
dc.contributor.authorRai, N. K.-
dc.contributor.authorBiswas, S.-
dc.contributor.authorKhushboo-
dc.contributor.authorMahato, A.-
dc.contributor.authorRoy, B. J.-
dc.contributor.authorVinayak, A.-
dc.contributor.authorRani, A.-
dc.date.accessioned2021-06-12T09:17:31Z-
dc.date.available2021-06-12T09:17:31Z-
dc.date.issued2021-06-12-
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/1797-
dc.description.abstractBackground: In heavy-ion-induced fusion reactions, cross sections in the sub-barrier region are enhanced compared to predictions of the one-dimensional barrier penetration model. This enhancement is often understood by invoking deformation and coupling of the relative motion with low-lying inelastic states of the reaction partners. However, effects of nucleon transfer on fusion below the barrier, especially for the systems having positive Q value neutron transfer (PQNT) channels, are yet to be disentangled completely. Purpose: We intend to study the role of the PQNT effect on the sub-barrier fusion of the 18O + 116Sn system having positive Q value for the two-neutron stripping channel. Also we reflect on the interplay of couplings involved in the system around the Coulomb barrier. Method: The fusion excitation function was measured at energies from 11% below to 46% above the Coulomb barrier for 18O + 116Sn using a recoil mass spectrometer, viz., the Heavy-Ion Reaction Analyser (HIRA). Fusion barrier distributions were extracted from the data. Results from the experiment were analyzed within the framework of the coupled-channels model. Results: Fusion cross sections at energies below the Coulomb barrier showed strong enhancement compared to predictions of the one-dimensional barrier penetration model. The fusion process is influenced by couplings to the collective excitations with coupling to single- and two-phonon vibrational states of the target and the projectile respectively. Inclusion of the two-neutron transfer channel in the calculation along with these couplings could reproduce the data satisfactorily. Conclusions: The significant role of PQNT in enhancing the sub-barrier fusion cross section for the chosen system is not observed. It simply reduced the sub-barrier fusion cross section. Therefore, a consistent link between PQNT and sub-barrier fusion enhancement could not be established vividly while comparing the fusion excitation function from this work with the same from other 16,18O-induced reactions. This clearly points to the need for more experimental as well as theoretical investigation in this field.en_US
dc.language.isoen_USen_US
dc.titleRole of neutron transfer in the sub-barrier fusion cross section in 18O+116Snen_US
dc.typeArticleen_US
Appears in Collections:Year-2020

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