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dc.contributor.authorRosenbaum, Ren_US
dc.contributor.authorMurphy, Ten_US
dc.contributor.authorBrandt, Ben_US
dc.contributor.authorWang, CRen_US
dc.contributor.authorZhong, YLen_US
dc.contributor.authorWu, SWen_US
dc.contributor.authorLin, STen_US
dc.contributor.authorLin, JJen_US
dc.date.accessioned2014-12-08T15:39:35Z-
dc.date.available2014-12-08T15:39:35Z-
dc.date.issued2004-02-18en_US
dc.identifier.issn0953-8984en_US
dc.identifier.urihttp://dx.doi.org/10.1088/0953-8984/16/6/012en_US
dc.identifier.urihttp://hdl.handle.net/11536/27022-
dc.description.abstractResistivity and magnetoresistance measurements have been performed on insulating icosahedral AlPdRe quasicrystal (QC) bar samples. At temperatures in the range 300 K greater than or equal to T greater than or equal to 50 K, the resistivities follow a simple inverse temperature law: rho(T) rho(0)/T(1.0+/-0.1). Below 1 K, the resistivity of a weakly insulating sample exhibited a simple inverse temperature law where rho(T) = rho0/T-0.33 and not an activated variable-range hopping (VRH) law. Strongly insulating samples exhibit saturation of their resistivities to finite values as T --> 0 K. These saturation resistivity values are believed to arise from the presence of a second metallic phase located within the quasicrystal's structure. By extrapolating the measured resistivities at 22 mK to absolute zero, the saturation conductivity values were estimated at T = 0 K and subtracted from the conductivity data points. These 'corrected' data, corresponding only to the QC phase, were found to follow activated VRH laws, having hopping exponents y that vary in the range 0.18 less than or equal to y less than or equal to 0.43. The activated VRH behaviours are observed only below 1 K. The magnetoresistances (MRs) of these samples are also anomalous. The MRs can be explained by including contributions from both the saturation conductivity values and from the QC MR ratios, estimated using the wavefunction shrinkage model.en_US
dc.language.isoen_USen_US
dc.titleElectronic transport in insulating AlPdRe quasicrystalsen_US
dc.typeArticleen_US
dc.identifier.doi10.1088/0953-8984/16/6/012en_US
dc.identifier.journalJOURNAL OF PHYSICS-CONDENSED MATTERen_US
dc.citation.volume16en_US
dc.citation.issue6en_US
dc.citation.spage821en_US
dc.citation.epage831en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000220021100017-
dc.citation.woscount9-
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