Investigating fusion dynamics at high angular momentum via fission cross sections

dc.contributor.authorPalshetkar, C. S.en
dc.contributor.authorHinde, D. J.en
dc.contributor.authorWilliams, E.en
dc.contributor.authorRamachandran, K.en
dc.contributor.authorDasgupta, M.en
dc.contributor.authorCook, K. J.en
dc.contributor.authorWakhle, A.en
dc.contributor.authorJeung, D. Y.en
dc.contributor.authorRafferty, D. C.en
dc.contributor.authorMcNeil, S. D.en
dc.contributor.authorCarter, I. P.en
dc.contributor.authorLuong, D. H.en
dc.date.accessioned2025-12-31T22:41:17Z
dc.date.available2025-12-31T22:41:17Z
dc.date.issued2017-11-22en
dc.description.abstractA quantitative understanding of fusion dynamics at high angular momentum is attempted employing experimental fission cross sections as a probe and carrying out a simultaneous description of the fusion and fission cross sections at above barrier energies. For this, experimental fission fragment angular distributions for three systems: 16O+148Sm, 28Si+136Ba and 40Ca+124Sn, all forming the same compound nucleus 164Yb at similar excitation energies, have been measured at four beam energies above their respective capture barriers. A simultaneous description of the angle integrated fission cross sections and evaporation residue/fusion cross sections available in literature for the systems is carried out using coupled-channels and statistical model calculations. Fission cross sections, which are most sensitive to the changes in angular momentum, provide very stringent constraints for model calculations thus indicating the need of precision evaporation residue as well as fission cross sections in such studies. A large diffuseness (ao>0.65 fm) of the nuclear potential gives the best reproduction of the experimental data. In addition, different coupling schemes give very different angular momentum distributions, which, in turn, give very different fission cross section predictions. Both these observations hint at the explanation that depending on energy dissipation of the interacting nuclei occurring inside or outside the fusion pocket, very different fission cross sections can result due to heavily altered angular momentum and thus justifies the sensitivity of fission cross sections used as probes in the present work.en
dc.description.statusPeer-revieweden
dc.identifier.issn2101-6275en
dc.identifier.otherORCID:/0000-0002-7895-458X/work/161834910en
dc.identifier.otherORCID:/0000-0002-4595-0742/work/162291091en
dc.identifier.otherORCID:/0000-0002-5911-1333/work/162375721en
dc.identifier.scopus85036627011en
dc.identifier.urihttps://hdl.handle.net/1885/733798577
dc.language.isoenen
dc.relation.ispartofseriesFUSION 2017en
dc.rightsPublisher Copyright: © The Authors, published by EDP Sciences, 2017.en
dc.sourceEPJ Web of Conferencesen
dc.titleInvestigating fusion dynamics at high angular momentum via fission cross sectionsen
dc.typeConference paperen
dspace.entity.typePublicationen
local.contributor.affiliationPalshetkar, C. S.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationHinde, D. J.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationWilliams, E.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationRamachandran, K.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationDasgupta, M.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationCook, K. J.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationWakhle, A.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationJeung, D. Y.; Non-Linear Physics Centre, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationRafferty, D. C.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationMcNeil, S. D.; Wearable and Portable Devices, Research School of Chemistry, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationCarter, I. P.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationLuong, D. H.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.identifier.ariespublicationa383154xPUB9091en
local.identifier.citationvolume163en
local.identifier.doi10.1051/epjconf/201716300042en
local.identifier.pure8f0c4909-d4ee-4637-a64b-e3dcfd8dfcc7en
local.identifier.urlhttps://www.scopus.com/pages/publications/85036627011en
local.type.statusPublisheden

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