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Electron dephasing in homogeneous and inhomogeneous indium tin oxide thin films

dc.citation.epage0en_US
dc.citation.issue10en_US
dc.citation.spage0en_US
dc.citation.volume85en_US
dc.citation.woscount18en_US
dc.contributor.authorWu, Chih-Yuanen_US
dc.contributor.authorLin, Bo-Tsungen_US
dc.contributor.authorZhang, Yu-Jieen_US
dc.contributor.authorLi, Zhi-Qingen_US
dc.contributor.authorLin, Juhn-Jongen_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.date.accessioned2019-04-03T06:36:35Z
dc.date.available2019-04-03T06:36:35Z
dc.date.issued2012-03-05en_US
dc.description.abstractThe electron dephasing processes in two-dimensional homogeneous and inhomogeneous indium tin oxide thin films have been investigated in a wide temperature range 0.3-90 K. We found that the small-energy-transfer electron-electron (e-e) scattering process dominated the dephasing from a few kelvins to several tens of kelvins. At higher temperatures, a crossover to the large-energy-transfer e-e scattering process was observed. Below about 1 to 2 K, the dephasing time tau(phi) revealed a very weak temperature dependence, which intriguingly scaled approximately with the inverse of the electron diffusion constant D, i.e., tau(phi)(T approximate to 0.3 K) proportional to 1/D. Theoretical implications of our results are discussed. The reason why the electron-phonon relaxation rate is negligibly weak in this low-carrier-concentration material is presented.en_US
dc.identifier.doi10.1103/PhysRevB.85.104204en_US
dc.identifier.issn1098-0121en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.85.104204en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/15557
dc.identifier.wosnumberWOS:000301111900007en_US
dc.language.isoen_USen_US
dc.titleElectron dephasing in homogeneous and inhomogeneous indium tin oxide thin filmsen_US
dc.typeArticleen_US

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