Title:
Role of neutron transfer in the sub-barrier fusion cross section in O 18 + Sn 116

dc.contributor.authorNabendu Kumar Deb
dc.contributor.authorKushal Kalita
dc.contributor.authorHarun Al Rashid
dc.contributor.authorS. Nath
dc.contributor.authorJ. Gehlot
dc.contributor.authorN. Madhavan
dc.contributor.authorRohan Biswas
dc.contributor.authorRudra N. Sahoo
dc.contributor.authorPankaj K. Giri
dc.contributor.authorAmar Das
dc.contributor.authorTapan Rajbongshi
dc.contributor.authorAnamika Parihari
dc.contributor.authorNiraj K. Rai
dc.contributor.authorSaumyajit Biswas
dc.contributor.authorKhushboo
dc.contributor.authorAmritraj Mahato
dc.contributor.authorB.J. Roy
dc.contributor.authorA. Vinayak
dc.contributor.authorAnjali Rani
dc.date.accessioned2026-02-07T09:19:49Z
dc.date.issued2020
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 O18 + Sn116 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 O18 + Sn116 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- A nd 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 O16,18-induced reactions. This clearly points to the need for more experimental as well as theoretical investigation in this field. © 2020 American Physical Society.
dc.identifier.doi10.1103/PhysRevC.102.034603
dc.identifier.issn24699985
dc.identifier.urihttps://doi.org/10.1103/PhysRevC.102.034603
dc.identifier.urihttps://dl.bhu.ac.in/bhuir/handle/123456789/35161
dc.publisherAmerican Physical Society
dc.titleRole of neutron transfer in the sub-barrier fusion cross section in O 18 + Sn 116
dc.typePublication
dspace.entity.typeArticle

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