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Non-Fermi-liquid scaling in ( x = 1, 1.5)

dc.contributor.authorAronson, M. C.en_US
dc.contributor.authorMaple, M. B.en_US
dc.contributor.authorChau, R.en_US
dc.contributor.authorGeorges, A.en_US
dc.contributor.authorTsvelik, A. M.en_US
dc.contributor.authorOsborn, Richard K.en_US
dc.date.accessioned2006-12-19T18:55:52Z
dc.date.available2006-12-19T18:55:52Z
dc.date.issued1996-11-25en_US
dc.identifier.citationAronson, M C; Maple, M B; Chau, R; Georges, A; Tsvelik, A M; Osborn, R (1996). "Non-Fermi-liquid scaling in ( x = 1, 1.5) ." Journal of Physics: Condensed Matter. 8(48): 9815-9823. <http://hdl.handle.net/2027.42/48876>en_US
dc.identifier.issn0953-8984en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/48876
dc.description.abstractWe review the compiled measurements of the imaginary part of the dynamical magnetic susceptibility , static susceptibility , electrical resistivity and specific heat C(T) in the uranium intermetallics (x = 1, 1.5). We assess the temperature- and energy-dependences predicted by single-ion and disorder-dominated models and compare these results to experiments. For temperatures T and excitation energies in the range , T < 150 K, our analysis suggests that the dynamics of isolated uranium ions are responsible for the observed temperature and frequency scaling, although inter-ion interactions may become important at lower temperatures and frequencies.en_US
dc.format.extent3118 bytes
dc.format.extent271387 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.language.isoen_US
dc.publisherIOP Publishing Ltden_US
dc.titleNon-Fermi-liquid scaling in ( x = 1, 1.5)en_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumThe Harrison M Randall Laboratory of Physics, University of Michigan, Ann Arbor, MI 48109-1120, USAen_US
dc.contributor.affiliationumThe Harrison M Randall Laboratory of Physics, University of Michigan, Ann Arbor, MI 48109-1120, USA Department of Physics and Institute for Pure and Applied Research, University of California at San Diego, La Jolla, California 92093, USA Laboratoire de Physique Theorique, Ecole Normale Supérieure, 75231 Paris Cedex 05, France Department of Physics, University of Oxford, 1 Keble Road, Oxford OX1 3NP, UK Argonne National Laboratory, Argonne, IL 60349-4845, USAen_US
dc.contributor.affiliationotherDepartment of Physics and Institute for Pure and Applied Research, University of California at San Diego, La Jolla, California 92093, USAen_US
dc.contributor.affiliationotherDepartment of Physics and Institute for Pure and Applied Research, University of California at San Diego, La Jolla, California 92093, USAen_US
dc.contributor.affiliationotherLaboratoire de Physique Theorique, Ecole Normale Supérieure, 75231 Paris Cedex 05, Franceen_US
dc.contributor.affiliationotherArgonne National Laboratory, Argonne, IL 60349-4845, USAen_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/48876/2/c64810.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1088/0953-8984/8/48/011en_US
dc.identifier.sourceJournal of Physics: Condensed Matter.en_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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