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dc.contributor.authorChiu, CWen_US
dc.contributor.authorShyu, FLen_US
dc.contributor.authorChang, CPen_US
dc.contributor.authorChuu, DSen_US
dc.contributor.authorLin, MFen_US
dc.date.accessioned2014-12-08T15:37:20Z-
dc.date.available2014-12-08T15:37:20Z-
dc.date.issued2004-11-01en_US
dc.identifier.issn0031-9015en_US
dc.identifier.urihttp://dx.doi.org/10.1143/JPSJ.73.2936en_US
dc.identifier.urihttp://hdl.handle.net/11536/25666-
dc.description.abstractThe excited conduction electrons in metallic armchair carbon nanotubes can decay by inelastic electron-electron scattering. The deexcitation channels include the single-particle and collective excitations of different angular momenta. The higher conduction subbands have more deexcitation channels, or shorter electron lifetimes. Each conduction subband has certain states with very long lifetimes, and a simple relationship between the inverse electron lifetime and the state energy is absent. Such results directly reflect the characteristics of the ID excitation spectra. The inverse electron lifetime contrasts sharply with those of semiconducting carbon nanotubes, graphite, and 2D and 3D metallic systems. Dimensionalities play an important role in the many-body effects. The predicted results could be verified by femtosecond time-resolved optical spectroscopy.en_US
dc.language.isoen_USen_US
dc.subjectcarbon nanotubesen_US
dc.subjectinelastic electron-electron scatteringen_US
dc.subjectelectron lifetimeen_US
dc.titleElectron lifetime in armchair carbon nanotubesen_US
dc.typeArticleen_US
dc.identifier.doi10.1143/JPSJ.73.2936en_US
dc.identifier.journalJOURNAL OF THE PHYSICAL SOCIETY OF JAPANen_US
dc.citation.volume73en_US
dc.citation.issue11en_US
dc.citation.spage2936en_US
dc.citation.epage2939en_US
dc.contributor.department物理研究所zh_TW
dc.contributor.departmentInstitute of Physicsen_US
dc.identifier.wosnumberWOS:000225352200006-
dc.citation.woscount6-
Appears in Collections:Articles