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dc.contributor.authorAllione, Marco
dc.contributor.authorBallester Caudet, Ana
dc.contributor.authorLi, Hongbo
dc.contributor.authorComin, Alberto
dc.contributor.authorMovilla Rosell, José Luis
dc.contributor.authorClimente Plasencia, Joan Ignasi
dc.contributor.authorManna, Liberato
dc.contributor.authorMoreels, Iwan
dc.date.accessioned2014-03-21T11:24:24Z
dc.date.available2014-03-21T11:24:24Z
dc.date.issued2013-03
dc.identifier.citationACS NANO, 7(3) (2013), p. 24413-2452ca_CA
dc.identifier.urihttp://hdl.handle.net/10234/88110
dc.description.abstractThe spectral dependence of the two-photon absorption in CdSe/CdS core/shell nanocrystal heterorods has been studied via two-photon-induced luminescence excitation spectroscopy. We verified that the two-photon absorption in these samples is a purely nonlinear phenomenon, excluding the contribution from multistep linear absorption mediated by defect states. A large absorption cross section was observed for CdSe/CdS core/shell quantum rods, in the range of 105 GM (1 GM = 10–50 cm4 s phot–1), scaling with the total nanocrystal volume and thus independent of the core emission wavelength. In the two-photon luminescence excitation spectra, peaks are strongly blue-shifted with respect to the one-photon absorption peaks, for both core and shell transitions. The experimental results are confirmed by k·p calculations, which attribute the shift to both different parity selection rules that apply to one-photon and two-photon transitions and a low oscillator strength for two-photon transitions close to the ground-state one-photon absorption. In contrast with lead chalcogenide quantum dots, we found no evidence of a breakdown of the optical selection rules, despite the presence of band anisotropy, via the anisotropic hole masses, and the explicitly induced reduction of the electron wave function symmetry via the rod shape of the shell. The anisotropy does lead to an unexpected splitting of the electron P-states in the case of a large CdSe core encapsulated in a thin CdS shell. Hence, tuning of the core and shell dimensions and the concurrent transition from type I to quasi-type II carrier localization enables unprecedented control over the band-edge two-photon absorption.ca_CA
dc.format.extent27 p.ca_CA
dc.format.mimetypeapplication/pdfca_CA
dc.language.isoengca_CA
dc.publisherAmerican Chemical Societyca_CA
dc.rightsAttribution-NonCommercial-ShareAlike 3.0 Spain*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/3.0/es/*
dc.subjectII - VI nanocrystalsca_CA
dc.subjectQuantum dotsca_CA
dc.subjectTwo-photon absorptionca_CA
dc.subjectOptical selection rulesca_CA
dc.subjectK.p calculationsca_CA
dc.subjectEffective mass approximationca_CA
dc.titleTwo-Photon Induced Blue Shift of Core and Shell Optical Transitions in Colloidal CdSe/CdS quasi-type II Quantum Rodsca_CA
dc.typeinfo:eu-repo/semantics/articleca_CA
dc.identifier.doihttp://dx.doi.org/10.1021/nn3057559
dc.rights.accessRightsinfo:eu-repo/semantics/openAccessca_CA
dc.relation.publisherVersionhttp://pubs.acs.org/doi/ipdf/10.1021/nn3057559ca_CA


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