Please use this identifier to cite or link to this item: https://physrep.ff.bg.ac.rs/handle/123456789/289
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dc.contributor.authorMaultzsch, J.en
dc.contributor.authorReich, S.en
dc.contributor.authorThomsen, C.en
dc.contributor.authorDobardžić, Ediben
dc.contributor.authorMilošević, I.en
dc.contributor.authorDamnjanović, M.en
dc.date.accessioned2022-07-05T17:30:37Z-
dc.date.available2022-07-05T17:30:37Z-
dc.date.issued2002-03-07en
dc.identifier.issn0038-1098en
dc.identifier.urihttps://physrep.ff.bg.ac.rs/handle/123456789/289-
dc.description.abstractWe present the phonon dispersion relations of single-wall carbon nanotubes calculated within a force-constants approach. By using the full symmetry group of the tubes, we are able to calculate the dispersion relations for any chirality starting from one single carbon atom. We find an overbending in the highest optical branch between 6 and 12 cm-1 independent of the tube diameter. The order of the high-energy modes at the Γ-point differs from the results derived from simple zone folding. The splitting between the two Raman active optical modes with A1 symmetry at the Γ-point of chiral tubes is ≈ 4 cm-1 for typical diameters; it increases with decreasing tube diameter. © 2002 Elsevier Science Ltd. All rights reserved.en
dc.relation.ispartofSolid State Communicationsen
dc.subjectA. Carbon nanotubesen
dc.subjectD. Phononsen
dc.titlePhonon dispersion of carbon nanotubesen
dc.typeArticleen
dc.identifier.doi10.1016/S0038-1098(02)00025-Xen
dc.identifier.scopus2-s2.0-0037034746en
dc.identifier.urlhttps://api.elsevier.com/content/abstract/scopus_id/0037034746en
dc.relation.issue9-10en
dc.relation.volume121en
dc.relation.firstpage471en
dc.relation.lastpage474en
item.openairetypeArticle-
item.cerifentitytypePublications-
item.fulltextNo Fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.grantfulltextnone-
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