2012
DOI: 10.1103/physrevb.85.033409
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Exciton-phonon sidebands in metallic carbon nanotubes studied using semiconductor Bloch equations

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Cited by 5 publications
(3 citation statements)
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“…The weaker, higherenergy feature alongside each excitonic transition has been attributed to a phonon sideband arising from the longitudinal optical phonon. This is supported by recent theoretical work by Bobkin et al 134 and earlier less denitive experimental claims. 82,110 Finally, with these facts in hand, the true armchair absorption spectrum line shape can be investigated.…”
Section: Optical Absorption and Colors Of Armchair Carbon Nanotubessupporting
confidence: 75%
“…The weaker, higherenergy feature alongside each excitonic transition has been attributed to a phonon sideband arising from the longitudinal optical phonon. This is supported by recent theoretical work by Bobkin et al 134 and earlier less denitive experimental claims. 82,110 Finally, with these facts in hand, the true armchair absorption spectrum line shape can be investigated.…”
Section: Optical Absorption and Colors Of Armchair Carbon Nanotubessupporting
confidence: 75%
“…While further refinements will be important, as presented our fifth-order model addresses the shortcomings of the molecular approach and that of Moura et al by accounting for excitons as discrete states and in providing a physical origin for the observed asymmetries that may be applied generally for both metallic and semiconducting SWCNTs. Such generality further supports the assignment of the absorption sideband in armchair SWCNTs as a K-momentum phonon sideband 20,38,39,46 . This picture provides predictive capability for understanding relative differences in REP asymmetries that may be found for different phonons (RBM, TO, LO), which is the subject of ongoing work.…”
Section: Fifth-order Raman Processesmentioning
confidence: 54%
“…The phonon population n α q follows the Bose-Einstein statistics. We solve the coupled system of differential equations (B1)-(B3) by Fourier transformation considering non-Markovian processes 40 . Inserting the phonon-assisted polarizations in Eq.…”
Section: Appendix B: Computation Of the Inhomogeneous Broadened Spectrummentioning
confidence: 99%