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dc.contributor.authorKumar, R.-
dc.contributor.authorSharma, V.R.-
dc.contributor.authorYadav, A.-
dc.contributor.authorSingh, P.P.-
dc.contributor.authorAgarwal, A.-
dc.contributor.authorAppannababu, S.-
dc.contributor.authorMukherjee, S.-
dc.contributor.authorSingh, B.P.-
dc.contributor.authorAli, R.-
dc.contributor.authorBhowmik, R.K.-
dc.date.accessioned2017-12-21T09:48:38Z-
dc.date.available2017-12-21T09:48:38Z-
dc.date.issued2017-12-21-
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/870-
dc.description.abstractExcitation functions of reaction residues produced in the 14N + 169Tm system have been measured to high precision at energies above the fusion barrier, ranging from 1.04VB to 1.30VB, and analyzed in the framework of the statistical model code PACE4. Analysis of α-emitting channels points toward the onset of incomplete fusion even at slightly above-barrier energies where complete fusion is supposed to be one of the dominant processes. The onset and strength of incomplete fusion have been deduced and studied in terms of various entrance channel parameters. Present results together with the reanalysis of existing data for various projectile-target combinations conclusively suggest strong influence of projectile structure on the onset of incomplete fusion. Also, a strong dependence on the Coulomb effect (ZPZT ) has been observed for the present system along with different projectile-target combinations available in the literature. It is concluded that the fraction of incomplete fusion linearly increases with ZPZT and is found to be more for larger ZPZT values, indicating significantly important linear systematics.en_US
dc.language.isoen_USen_US
dc.titleLow-energy nuclear reaction of the N 14 + Tm 169 system: incomplete fusionen_US
dc.typeArticleen_US
Appears in Collections:Year-2017

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