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dc.contributor.authorChiu, C. W.en_US
dc.contributor.authorShyu, F. L.en_US
dc.contributor.authorChang, C. P.en_US
dc.contributor.authorChuu, D. S.en_US
dc.contributor.authorLin, M. F.en_US
dc.date.accessioned2019-04-03T06:44:51Z-
dc.date.available2019-04-03T06:44:51Z-
dc.date.issued2006-06-01en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.73.235407en_US
dc.identifier.urihttp://hdl.handle.net/11536/12169-
dc.description.abstractTemperature induces some free carriers in moderate-gap carbon nanotubes, which, thus, creates the low-frequency intraband e-h excitations. Such excitations are the effective deexcitation channels for the excited electrons (holes) in conduction (valence) bands, while they are very weak. The Coulomb decay rates of the lowest two conduction bands are sensitive to the changes in wave vector, radius, and temperature. However, those of the band-edge states depend on chirality weakly. These results directly reflect the strong energy dispersions and the temperature-dependent electron distributions. The calculated results are roughly consistent with the experimental measurements from the ultrafast optical spectroscopies.en_US
dc.language.isoen_USen_US
dc.titleCoulomb scattering rates of excited carriers in moderate-gap carbon nanotubesen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.73.235407en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume73en_US
dc.citation.issue23en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000238696600129en_US
dc.citation.woscount1en_US
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