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Lifetime measurements in the transitional nucleus 138Gd

dc.contributor.authorProcter, M.G.
dc.contributor.authorCullen, D M
dc.contributor.authorRuotsalainen, P.
dc.contributor.authorBraunroth, T.
dc.contributor.authorDewald, A
dc.contributor.authorFransen, C.
dc.contributor.authorGrahn, T.
dc.contributor.authorGreenlees, P.T.
dc.contributor.authorHackstein, M.
dc.contributor.authorNieminen, Paivi
dc.contributor.authorReed, Matthew
dc.contributor.authorVitturi, A.
dc.date.accessioned2015-12-13T22:42:05Z
dc.date.issued2011
dc.date.updated2015-12-11T10:05:34Z
dc.description.abstractLifetime measurements have been made in the ground-state band of the transitional nucleus 138Gd from coincidence recoil-distance Doppler-shift data. 138Gd nuclei were produced using the 106Cd (36Ar, 2p2n) reaction with a beam energy of 190 MeV. Reduced transition probabilities have been extracted from the lifetime data collected with the Köln plunger placed at the target position of the JUROGAM-II array. The B(E2) values have been compared with predictions from X(5) critical-point calculations, which describe the phase transition between vibrational and axially symmetric nuclear shapes, as well as with IBM-1 calculations at the critical point. While the excitation energies in 138Gd are consistent with X(5) predictions, the large uncertainties associated with the measured B(E2) values cannot preclude vibrational and rotational contributions to the low-lying structure of 138Gd. Although experimental knowledge for the low-lying γ and β-vibrational bands in 138Gd is limited, potential-energy surface calculations suggest an increase in γ softness in the ground-state band. In order to more fully account for the effects of γ softness, the X(5) and IBM-1 calculations need to be extended to include the γ degree of freedom for 138Gd.
dc.identifier.issn0556-2813
dc.identifier.urihttp://hdl.handle.net/1885/78814
dc.publisherAmerican Physical Society
dc.sourcePhysical Review C: Nuclear Physics
dc.titleLifetime measurements in the transitional nucleus 138Gd
dc.typeJournal article
local.bibliographicCitation.issue2
local.contributor.affiliationProcter, M.G., the University of Manchester
local.contributor.affiliationCullen, D M, University of Manchester
local.contributor.affiliationRuotsalainen, P., University of Jyvaskyla
local.contributor.affiliationBraunroth, T., University of Cologne
local.contributor.affiliationDewald, A, University of Cologne
local.contributor.affiliationFransen, C., University of Cologne
local.contributor.affiliationGrahn, T., University of Jyvaskyla
local.contributor.affiliationGreenlees, P.T., University of Jyvaskyla
local.contributor.affiliationHackstein, M., University of Cologne
local.contributor.affiliationNieminen, Paivi, College of Physical and Mathematical Sciences, ANU
local.contributor.affiliationReed, Matthew, College of Physical and Mathematical Sciences, ANU
local.contributor.affiliationVitturi, A., Physics Department and INFA
local.contributor.authoruidNieminen, Paivi, a243931
local.contributor.authoruidReed, Matthew, u5217955
local.description.embargo2037-12-31
local.description.notesImported from ARIES
local.identifier.absfor020200 - ATOMIC, MOLECULAR, NUCLEAR, PARTICLE AND PLASMA PHYSICS
local.identifier.ariespublicationf5625xPUB7386
local.identifier.citationvolume84
local.identifier.doi10.1103/PhysRevC.84.024314
local.identifier.scopusID2-s2.0-80052190514
local.type.statusPublished Version

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