In-beam study of 144Gd

cnea.localizacion02.78.12
cnea.tipodocumentoARTÍCULO CIENTÍFICO
dc.contributor.authorMariscotti, M. A. J.
dc.contributor.authorBeuscherc, H.
dc.contributor.authorDavidsonc, W. F.
dc.contributor.authorGonoc, Y.
dc.contributor.authorJägerc, H. M.
dc.contributor.authorLiederc, R. M.
dc.contributor.authorMüller-Veggianc, M.
dc.contributor.authorNeskakisc, A.
dc.contributor.authorHaennic, D. R.
dc.contributor.authorZolnowski, D. R.
dc.date.accessioned2024-02-14T15:30:59Z
dc.date.available2024-02-14T15:30:59Z
dc.date.issued1978
dc.description.abstractA level scheme of 144Gd has been established using the 144Sm(α, 4nγ) reaction and in-beam spectroscopy methods. Excitation functions, γ-ray angular distributions, γ-γ coincidence spectra, γ-spectra time related to the cyclotron beam bursts and conversion coefficients for the delayed transitions have been measured. The level scheme comprises 11 levels with spins up to I = 12. Two isomers, a 13 ± 2 ns, 7− state at 2471.4 keV and a 145 ± 30 ns, 10+ state at 3433.0 keV have been observed. The former has similar excitation energy as the 7− isomers in 142Sm, 140Nd and 138Ce and it may arise from the configuration although its lifetime seems to indicate some degree of collectivity. The 10+ state has a similar excitation energy as the 10+ isomer found in 138Ce and it may arise from the dominant configuration. Below the 10+ isomer in 144Gd only two excited states have positive parity; the hitherto known first 2+ and 4+ states. The 11+ and 12+ states must include four-particle configurations or they have to be of collective nature. The latter possibility is supported by the considerable E2/M1 mixture (≈ 20 %) observed for the 11+ to 10+ transition. An analysis of the systematics of ground band levels in the N = 80 isotones shows the same gradual behavior between the two VMI solutions previously found for the Te isotopes.
dc.description.institutionalaffiliationFil: Mariscotti, M. A. J. Comisión Nacional de Energía Atómica; Argentina
dc.description.institutionalaffiliationBeuscherc, H. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationDavidsonc, W. F. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationGonoc, Y. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationJägerc, H. M. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationLiederc, R. M. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationMüller-Veggianc, M. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationNeskakisc, A.Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationHaennic, D. R. Institut für Kernphysik, Kernforschungsanlage Jülich, Alemania
dc.description.institutionalaffiliationZolnowski, D. R. Cyclotron Institute, Texas A&M University, College Station, Estados Unidos
dc.format.extent395-412 p.
dc.format.mediumapplication/pdf
dc.identifier.urihttps://doi.org/10.1016/0375-9474(78)90521-3
dc.identifier.urihttps://nuclea.cnea.gob.ar/handle/20.500.12553/4862
dc.language.ISO639-3eng
dc.publisherNorth-Holland Publishing Company
dc.relation.ispartofNuclear Physics A Vol 311, N°3, 1978
dc.rights.accesslevelinfo:eu-repo/semantics/openAccess
dc.rights.urihttps://creativecommons.org/licenses/by-nc-sa/4.0/
dc.subject.keywordREACCIONES NUCLEARES
dc.subject.keywordNUCLEAR REACTIONS
dc.subject.keywordESPECTROSCOPIA SOBRE HAZ
dc.subject.keywordIN-BEAM SPECTROSCOPY
dc.subject.keywordFUNCIONES DE EXCITACIÓN
dc.subject.keywordEXCITATION FUNCTIONS
dc.titleIn-beam study of 144Gd
dc.typeARTÍCULO
dc.type.openaireinfo:eu-repo/semantics/article
dc.type.snrdinfo:ar-repo/semantics/artículo
dc.type.versioninfo:eu-repo/semantics/publishedVersion

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