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dc.contributor.authorLin, MFen_US
dc.contributor.authorChuu, DSen_US
dc.contributor.authorHuang, CSen_US
dc.contributor.authorLin, YKen_US
dc.contributor.authorShung, KWKen_US
dc.date.accessioned2019-04-03T06:38:59Z-
dc.date.available2019-04-03T06:38:59Z-
dc.date.issued1996-06-15en_US
dc.identifier.issn0163-1829en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.53.15493en_US
dc.identifier.urihttp://hdl.handle.net/11536/1225-
dc.description.abstractThe inter-pi-band response function of a single-layer carbon nanotube is calculated within the random-phase approximation. Such a cylindrical system exhibits rich inter-pi-band excitations. The decoupled pi plasmons;of different angular momenta (L's) strongly depend on the transferred momenta (q's). Furthermore, they exhibit a dimensionality crossover as the nanotube radius is increased. For small q's and L's, the pi plasmon frequency is similar to 6-8 eV, which is insensitive to the nanotube geometry such as the radius and chiral angle. Comparison with recent experiments is discussed.en_US
dc.language.isoen_USen_US
dc.titleCollective excitations in a single-layer carbon nanotubeen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.53.15493en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume53en_US
dc.citation.issue23en_US
dc.citation.spage15493en_US
dc.citation.epage15496en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:A1996UT77000031en_US
dc.citation.woscount79en_US
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