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Band structure of 235 U

dc.contributor.authorWard, D
dc.contributor.authorMacchiavelli, A O
dc.contributor.authorClark, R M
dc.contributor.authorCline, D.
dc.contributor.authorCromaz, M.
dc.contributor.authorDeleplanque, M.A.
dc.contributor.authorDiamond, R.M.
dc.contributor.authorFallon, P
dc.contributor.authorGorgen, A
dc.contributor.authorHayes, A.B.
dc.contributor.authorLane, Gregory
dc.contributor.authorLee, I-Y
dc.contributor.authorNakatsukasa, T.
dc.contributor.authorSchmidt, G.
dc.contributor.authorStephens, F.S.
dc.contributor.authorSvensson, C.E.
dc.contributor.authorTeng, R.
dc.contributor.authorVetter, K
dc.contributor.authorWu, C Y
dc.date.accessioned2015-12-10T23:35:21Z
dc.date.issued2012
dc.date.updated2015-12-10T11:40:56Z
dc.description.abstractOver a period of several years we have performed three separate experiments at Lawrence Berkeley National Laboratory's 88-Inch Cyclotron in which 235U (thick target) was Coulomb-excited. The program involved stand-alone experiments with Gammmasphere and with the 8pi Spectrometer using 136Xe beams at 720 MeV, and a CHICO-Gammasphere experiment with a 40Ca beam at 184 MeV. In addition to extending the known negative-parity bands to high spin, we have assigned levels in some seven positive-parity bands which are in some cases (e.g., [631]1/2, [624]7/2, and [622]5/2) strongly populated by E3 excitation. The CHICO data have been analyzed to extract E2 and E3 matrix elements from the observed yields. Additionally, many M1 matrix elements could be extracted from the γ-ray branching ratios. A number of new features have emerged, including the unexpected attenuation of magnetic transitions between states of the same Nilsson multiplet, the breakdown of Coriolis staggering at high spin, and the effect of E3 collectivity on Coriolis interactions.
dc.identifier.issn0556-2813
dc.identifier.urihttp://hdl.handle.net/1885/69827
dc.publisherAmerican Physical Society
dc.rightsAuthor/s retain copyrighten_AU
dc.sourcePhysical Review C: Nuclear Physics
dc.titleBand structure of 235 U
dc.typeJournal article
dcterms.accessRightsOpen Accessen_AU
local.bibliographicCitation.issue6
local.bibliographicCitation.lastpage41
local.bibliographicCitation.startpage1
local.contributor.affiliationWard, D, Lawrence Berkeley National Laboratory
local.contributor.affiliationMacchiavelli, A O, Lawrence Berkeley National Laboratory
local.contributor.affiliationClark, R M, Lawrence Berkeley National Laboratory
local.contributor.affiliationCline, D., University of Rochester
local.contributor.affiliationCromaz, M., Lawrence Berkeley National Laboratory
local.contributor.affiliationDeleplanque, M.A., Lawrence Berkeley National Laboratory
local.contributor.affiliationDiamond, R.M., Lawrence Berkeley National Laboratory
local.contributor.affiliationFallon, P, Lawrence Berkeley National Laboratory
local.contributor.affiliationGorgen, A, Lawrence Berkeley National Laboratory
local.contributor.affiliationHayes, A.B., University of Rochester
local.contributor.affiliationLane, Gregory, College of Physical and Mathematical Sciences, ANU
local.contributor.affiliationLee, I-Y, Lawrence Berkeley National Laboratory
local.contributor.affiliationNakatsukasa, T., RIKEN Nishina Center
local.contributor.affiliationSchmidt, G., Lawrence Livermore National Laboratory
local.contributor.affiliationStephens, F.S., Lawrence Berkeley National Laboratory
local.contributor.affiliationSvensson, C.E., Lawrence Berkeley National Laboratory
local.contributor.affiliationTeng, R., University of Rochester
local.contributor.affiliationVetter, K, Lawrence Berkeley National Laboratory
local.contributor.affiliationWu, C Y, University of Rochester
local.contributor.authoruidLane, Gregory, u4019877
local.description.notesImported from ARIES
local.identifier.absfor020202 - Nuclear Physics
local.identifier.ariespublicationf5625xPUB2133
local.identifier.citationvolume86
local.identifier.doi10.1103/PhysRevC.86.064319
local.identifier.scopusID2-s2.0-84871671060
local.identifier.thomsonID000312698500002
local.type.statusPublished Version

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