Asymmetric excitation profiles in the resonance Raman response of armchair carbon nanotubes

dc.citation.firstpage205446
dc.citation.journalTitlePhysical Review B
dc.citation.volumeNumber91
dc.contributor.authorHároz, Erik H.
dc.contributor.authorDuque, Juan G.
dc.contributor.authorBarros, Eduardo B.
dc.contributor.authorTelg, Hagen
dc.contributor.authorSimpson, Jeffrey R.
dc.contributor.authorWalker, Angela R. Hight
dc.contributor.authorKhripin, Constantine Y.
dc.contributor.authorFagan, Jeffrey A.
dc.contributor.authorTu, Xiaomin
dc.contributor.authorZheng, Ming
dc.contributor.authorKono, Junichiro
dc.contributor.authorDoorn, Stephen K.
dc.date.accessioned2015-07-09T15:30:05Z
dc.date.available2015-07-09T15:30:05Z
dc.date.issued2015
dc.description.abstractWe performed tunable resonance Raman spectroscopy on samples highly enriched in the (5,5), (6,6), (7,7), and (8,8) armchair structures of metallic single-wall carbon nanotubes. We present Raman excitation profiles (REPs) for both the radial breathing mode and G-band phonons of these species. G-band excitation profiles are shown to resolve the expected incoming and outgoing resonances of the scattering process. Notably, the profiles are highly asymmetric, with the higher-energy outgoing resonance weaker than the incoming resonance. These results are comparable to the asymmetric excitation profiles observed previously in semiconducting nanotubes, introduce a different electronic type, and broaden the structural range over which the asymmetry is found to exist. Modeling of the behavior with a third-order quantum model that accounts for the k dependence in energies and matrix elements, without including excitonic effects, is found to be insufficient for reproducing the observed asymmetry. We introduce an alternative fifth-order model in which the REP asymmetry arises from quantum interference introduced by phonon-mediated state mixing between the EM11 and K-momentum excitons. Such state mixing effectively introduces a nuclear coordinate dependence in the transition dipole moment and thus may be viewed as a non-Condon effect from a molecular perspective. This result unifies a molecularlike picture of nanotube transitions (introduced by their excitonic nature) with a condensed matter approach for describing their behavior.
dc.identifier.citationHároz, Erik H., Duque, Juan G., Barros, Eduardo B., et al.. "Asymmetric excitation profiles in the resonance Raman response of armchair carbon nanotubes." <i>Physical Review B,</i> 91, (2015) American Physical Society: 205446. http://dx.doi.org/10.1103/PhysRevB.91.205446.
dc.identifier.doihttp://dx.doi.org/10.1103/PhysRevB.91.205446
dc.identifier.urihttps://hdl.handle.net/1911/80859
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.rightsArticle is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.
dc.titleAsymmetric excitation profiles in the resonance Raman response of armchair carbon nanotubes
dc.typeJournal article
dc.type.dcmiText
dc.type.publicationpublisher version
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