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2005
DOI: 10.1103/physrevlett.95.247401
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Direct Experimental Evidence of Exciton-Phonon Bound States in Carbon Nanotubes

Abstract: We present direct experimental observation of exciton-phonon bound states in the photoluminescence excitation spectra of isolated single-walled carbon nanotubes (SWNT) in aqueous suspension. The photoluminescence excitation spectra from several distinct SWNTs show the presence of at least one sideband related to the tangential modes, lying 0.2 eV above the main absorption or emission peak. Both the energy position and line shapes of the sidebands are in excellent agreement with recent calculations [Phys. Rev. … Show more

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Cited by 109 publications
(133 citation statements)
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“…From the value of the zone-edge optical phonon (as measured from the D band Raman line), we deduce that the splitting between this KK 0 exciton and the bright exciton is also on the order of 35 meV for upper sub-bands. This value, very similar to the one reported for S 11 and S 22 [24,28], is quite surprising since this splitting was expected to depend on the diameter and the transition order. We attribute the coincidence to an accidental compensation of the scalings with the diameter and the local dielectric constant.…”
Section: Semi-conducting Nanotubessupporting
confidence: 58%
See 1 more Smart Citation
“…From the value of the zone-edge optical phonon (as measured from the D band Raman line), we deduce that the splitting between this KK 0 exciton and the bright exciton is also on the order of 35 meV for upper sub-bands. This value, very similar to the one reported for S 11 and S 22 [24,28], is quite surprising since this splitting was expected to depend on the diameter and the transition order. We attribute the coincidence to an accidental compensation of the scalings with the diameter and the local dielectric constant.…”
Section: Semi-conducting Nanotubessupporting
confidence: 58%
“…They lead to phonon-side bands in absorption and PL spectroscopy. Such side-bands have been first reported by several teams [24][25][26][27]. The key point is that these side-bands are not symmetrical (in energy) with respect to the bright state but rather with respect to the KK 0 dark ones (which are degenerate in energy).…”
Section: Excitonsmentioning
confidence: 86%
“…In this case λ ex corresponds to the energy of the excitonic states eh ii associated with the ith electronic interband transitions E ii (i=1, 2, 3, 4) in the single particle picture [3,17], while λ em is the emission energy of the lowest exciton transition eh 11 . Other spots in Fig.1a are related to excitonphonon sidebands [18,19,20]. The spectral features in Fig.1a are summarized in Fig.2.…”
mentioning
confidence: 90%
“…Notably, these three peaks do not correspond to any of the known exciton-exciton resonances of SWNTs in this spectral range [3,17]. The (980nm, 1118nm) peak is not assigned to a D phonon sideband of (8,4), (7,6) or (9, 4) tubes, due to the lack of such sideband in previous investigations of these and other tubes [18,19,23,24]. Indeed, the excitation energies of the (980nm, 1118nm), (568nm, 1118nm) and (346nm, 1118nm) bands match, respectively, the eh 11 , eh 22 and eh 33 transitions of (6,5) tubes [3], whereas their emission around 1118 nm is consistent with (8,4), (7,6), (9, 4) eh 11 .…”
mentioning
confidence: 99%
“…As micelas formadas por surfactante e nanotubos formam dispersões estáveis em meio aquoso. As miscelas mantêm os nanotubos de carbono isolados uns dos outros, permitindo o estudo das propriedades fotofísicas (absorção, emissão, "excitons") de cada nanotubo e a correlação dessas propriedades físicas com a estrutura atômica, ou seja, com os ín-dices n e m [61][62][63] . A interação dos SWNTs com seqüências de oligonucleotídeos (Figura 7) tem sido um dos métodos mais utilizados e com maior sucesso para a separação de nanotubos metáli-cos de nanotubos semicondutores e, também, na separação de nanotubos pelo diâmetro e comprimento 63,64 .…”
Section: Figura 5 Espectros Raman De Nanotubos De Paredes Duplas Purunclassified