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Activation cross section and isomeric cross-section ratio for the (n,2n) reaction on Ir191

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dc.contributor.author Patronis, N en
dc.contributor.author Papadopoulos, CT en
dc.contributor.author Galanopoulos, S en
dc.contributor.author Kokkoris, M en
dc.contributor.author Perdikakis, G en
dc.contributor.author Vlastou, R en
dc.contributor.author Lagoyannis, A en
dc.contributor.author Harissopulos, S en
dc.date.accessioned 2014-03-01T01:25:52Z
dc.date.available 2014-03-01T01:25:52Z
dc.date.issued 2007 en
dc.identifier.issn 0556-2813 en
dc.identifier.uri https://dspace.lib.ntua.gr/xmlui/handle/123456789/17782
dc.subject Cross Section en
dc.subject.classification Physics, Nuclear en
dc.subject.other N,2N REACTIONS en
dc.subject.other SYSTEMATICS en
dc.subject.other DENSITY en
dc.subject.other ENERGY en
dc.subject.other MASSES en
dc.title Activation cross section and isomeric cross-section ratio for the (n,2n) reaction on Ir191 en
heal.type journalArticle en
heal.identifier.primary 10.1103/PhysRevC.75.034607 en
heal.identifier.secondary http://dx.doi.org/10.1103/PhysRevC.75.034607 en
heal.identifier.secondary 034607 en
heal.language English en
heal.publicationDate 2007 en
heal.abstract The Ir191(n,2n)Ir190 cross section was measured by means of the activation technique at four neutron energies in the range 10.0-11.3 MeV. The quasimonoenergetic neutron beam was produced via the H2(d,n)He3 reaction at the 5.5 MV Tandem Van de Graaff accelerator of NCSR ""Demokritos."" The cross section for the population of the second high spin (11-) isomeric state was measured along with the sum of the reaction cross section populating both the ground (4-) and the first isomeric state (1-). Statistical model calculations taking into account pre-equilibrium emission were performed and compared with all the available experimental data. The experimentally deduced excitation function for populating both the ground and first isomeric state was well reproduced by the theoretical calculations. The statistical model calculations of populating the second metastable state revealed its strong dependence on the details of the introduced level scheme, as well as on the ratio between the effective moment of inertia and the rigid body moment of inertia of the residual nucleus. The experimental cross-section data corresponding to the second isomeric state and to the isomeric ratio were reproduced in a quite consistent way by the calculations. © 2007 The American Physical Society. en
heal.publisher AMERICAN PHYSICAL SOC en
heal.journalName Physical Review C - Nuclear Physics en
dc.identifier.doi 10.1103/PhysRevC.75.034607 en
dc.identifier.isi ISI:000245332200036 en
dc.identifier.volume 75 en
dc.identifier.issue 3 en


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