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dc.contributor.authorHsu, SYen_US
dc.contributor.authorSheng, PJen_US
dc.contributor.authorLin, JJen_US
dc.date.accessioned2019-04-03T06:39:14Z-
dc.date.available2019-04-03T06:39:14Z-
dc.date.issued1999-08-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.60.3940en_US
dc.identifier.urihttp://hdl.handle.net/11536/31160-
dc.description.abstractWe have measured the electron-phonon scattering rates 1/tau(ep) from a weak-localization study of a series of high-resistivity tin-doped Ti73Al27 alloys. The resistivities of these alloys are essentially the same and are so high that the electron elastic mean free path I approaches the interatomic spacing, resulting in a very small value of q(ph) l approximate to 0.0056 T (q(ph) is the wave number of the thermal phonons, and T is the temperature). Based on as many as about 60 magnetoresistivity measurements between 2 and 22 K, we are able to determine the dependence of 1/tau(ep) on T to within a great degree of accuracy and find that 1/tau(ep) varies essentially with T-2 in the dirty limit (q(ph) l much less than 1). This observation is not understood in terms of the current theoretical concept of electron-phonon interaction in disordered metals. [S0163-1829(99)05030-4].en_US
dc.language.isoen_USen_US
dc.titleQuadratic temperature dependence of the electron-phonon scattering rate in disordered metalsen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.60.3940en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume60en_US
dc.citation.issue6en_US
dc.citation.spage3940en_US
dc.citation.epage3943en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000081997100035en_US
dc.citation.woscount16en_US
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