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Two-proton pickup in the zirconium region using the (6Li, 8B) reaction

dc.contributor.authorTickle, R. S.en_US
dc.contributor.authorGray, W. S.en_US
dc.contributor.authorBent, R. D.en_US
dc.date.accessioned2006-04-07T17:54:14Z
dc.date.available2006-04-07T17:54:14Z
dc.date.issued1982-03-01en_US
dc.identifier.citationTickle, R. S., Gray, W. S., Bent, R. D. (1982/03/01)."Two-proton pickup in the zirconium region using the (6Li, 8B) reaction." Nuclear Physics A 376(2): 309-324. <http://hdl.handle.net/2027.42/24049>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TVB-471XJ97-24D/2/fbe31d150215f784c8687c936f3b5128en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/24049
dc.description.abstractSpectra at [theta]lab = 8[deg] have been measured for the 92, 94, 96, 98, 100Mo(6Li, 8B)90, 92, 94, 96, 98Zr and 90, 92, 94Zr(6Li, 8B)88, 90, 92Sr two-proton pickup reactions at 90 MeV. The strongest transitions to levels in the Zr isotopes are the 0+ --&gt; 0+ transitions to the g.s. and first excited 0+ states. The salient feature of the five Zr spectra is the large increase in 0+2 transition strength relative to that of the g.s. which is observed in the two heaviest isotopes, 96, 98Zr. In 90Zr, the 0+2 transition is weak whereas it is the dominant transition in 98Zr with twice the g.s. strength. These large variations in relative cross section, which are reproduced by DWBA calculations, are attributed to changing g.s. proton configurations in Zr. In the Sr spectra, which are distinctly different from the Zrspectra, the strongest transitions to excited states are to 2+ rather than 0+ states. The (6Li, 8B) reaction seems to be adequately described as a one-step cluster transfer of a T = 1, S = 0 proton pair. The suitability of this reaction for measurements of two-proton pickup is discussed.en_US
dc.format.extent876013 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleTwo-proton pickup in the zirconium region using the (6Li, 8B) reactionen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelNuclear Engineering and Radiological Sciencesen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Physics, University of Michigan, Ann Arbor, Michigan 48109, USAen_US
dc.contributor.affiliationotherIndiana University Cyclotron Facility, Bloomington, Indiana 47405, USAen_US
dc.contributor.affiliationotherno department founden_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/24049/1/0000298.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0375-9474(82)90067-7en_US
dc.identifier.sourceNuclear Physics Aen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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