Non-Fermi-liquid scaling in ( x = 1, 1.5)
dc.contributor.author | Aronson, M. C. | en_US |
dc.contributor.author | Maple, M. B. | en_US |
dc.contributor.author | Chau, R. | en_US |
dc.contributor.author | Georges, A. | en_US |
dc.contributor.author | Tsvelik, A. M. | en_US |
dc.contributor.author | Osborn, Richard K. | en_US |
dc.date.accessioned | 2006-12-19T18:55:52Z | |
dc.date.available | 2006-12-19T18:55:52Z | |
dc.date.issued | 1996-11-25 | en_US |
dc.identifier.citation | Aronson, 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.issn | 0953-8984 | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/48876 | |
dc.description.abstract | We 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.extent | 3118 bytes | |
dc.format.extent | 271387 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.language.iso | en_US | |
dc.publisher | IOP Publishing Ltd | en_US |
dc.title | Non-Fermi-liquid scaling in ( x = 1, 1.5) | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | The Harrison M Randall Laboratory of Physics, University of Michigan, Ann Arbor, MI 48109-1120, USA | en_US |
dc.contributor.affiliationum | The 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, USA | en_US |
dc.contributor.affiliationother | Department of Physics and Institute for Pure and Applied Research, University of California at San Diego, La Jolla, California 92093, USA | en_US |
dc.contributor.affiliationother | Department of Physics and Institute for Pure and Applied Research, University of California at San Diego, La Jolla, California 92093, USA | en_US |
dc.contributor.affiliationother | Laboratoire de Physique Theorique, Ecole Normale Supérieure, 75231 Paris Cedex 05, France | en_US |
dc.contributor.affiliationother | Argonne National Laboratory, Argonne, IL 60349-4845, USA | en_US |
dc.contributor.affiliationumcampus | Ann Arbor | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/48876/2/c64810.pdf | en_US |
dc.identifier.doi | http://dx.doi.org/10.1088/0953-8984/8/48/011 | en_US |
dc.identifier.source | Journal of Physics: Condensed Matter. | en_US |
dc.owningcollname | Interdisciplinary and Peer-Reviewed |
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