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dc.contributor.authorLin, JJen_US
dc.contributor.authorKao, LYen_US
dc.date.accessioned2014-12-08T15:44:12Z-
dc.date.available2014-12-08T15:44:12Z-
dc.date.issued2001-02-05en_US
dc.identifier.issn0953-8984en_US
dc.identifier.urihttp://dx.doi.org/10.1088/0953-8984/13/5/102en_US
dc.identifier.urihttp://hdl.handle.net/11536/29853-
dc.description.abstractWe have systematically investigated the low-temperature electron dephasing times tau (phi) in more than 40 three-dimensional polycrystalline impure metals with distinct material characteristics. In all cases, a saturation of the dephasing time is observed below about a (few) degree(s) Kelvin, depending on samples. The value of the saturated dephasing time tau (0) [= tau (phi)(T --> 0 K)] falls basically in the range 0.005 to 0.5 ns for all samples. Particularly, we find that so scales with the electron diffusion constant D as tau (0) similar to D-alpha, with alpha close to or slightly larger than 1, for over two decades of D from about 0.1 to 10 cm(2) s(-1). Our observation implies an essentially constant saturated dephasing length of rootD tau (0) similar to 1000 Angstrom in three-dimensional polycrystalline disordered metals. A complete theoretical explanation is not yet available.en_US
dc.language.isoen_USen_US
dc.titleSaturation of electron dephasing in three-dimensional polycrystalline disordered metalsen_US
dc.typeLetteren_US
dc.identifier.doi10.1088/0953-8984/13/5/102en_US
dc.identifier.journalJOURNAL OF PHYSICS-CONDENSED MATTERen_US
dc.citation.volume13en_US
dc.citation.issue5en_US
dc.citation.spageL119en_US
dc.citation.epageL125en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000167072500002-
dc.citation.woscount31-
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