2016
DOI: 10.1021/acs.nanolett.5b04901
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Ubiquity of Exciton Localization in Cryogenic Carbon Nanotubes

Abstract: We present photoluminescence studies of individual semiconducting single-wall carbon nanotubes at room and cryogenic temperatures. From the analysis of spatial and spectral features of nanotube photoluminescence, we identify characteristic signatures of unintentional exciton localization. Moreover, we quantify the energy scale of exciton localization potentials as ranging from a few to a few tens of millielectronvolts and stemming from both environmental disorder and shallow covalent side-wall defects. Our res… Show more

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Cited by 25 publications
(27 citation statements)
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“…It is noteworthy that the segmentation of the E 11 emission (highlighted in blue) at 4 K originates from random localizations of excitons in long polymer-wrapped SWNTs or from other extrinsic defects introduced during initial processing. They are also present in SWNTs that were not specifically functionalized [39][40][41] . An integrated spectrum of 62 spots closely resembles the ensemble spectrum of a thin film at room temperature (Supplementary Fig.…”
Section: Resultsmentioning
confidence: 99%
“…It is noteworthy that the segmentation of the E 11 emission (highlighted in blue) at 4 K originates from random localizations of excitons in long polymer-wrapped SWNTs or from other extrinsic defects introduced during initial processing. They are also present in SWNTs that were not specifically functionalized [39][40][41] . An integrated spectrum of 62 spots closely resembles the ensemble spectrum of a thin film at room temperature (Supplementary Fig.…”
Section: Resultsmentioning
confidence: 99%
“…One of the many exciting properties of semiconducting SWCNTs is their potential for single-photon emission due to exciton localization even without any intentional functionalization and in seemingly homogeneous environments. [105,106] Early experiments had demonstrated photon antibunching (i.e., vanishing probability of the emission of more than one photon per excitation) in nanotubes at cryogenic temperatures [107] and thus introduced them as strong contenders for single-photon emitters in secure quantum communication and even quantum computing. [108] Carbon nanotubes are particularly attractive for these applications for several reasons.…”
Section: Single-photon Emittersmentioning
confidence: 99%
“…When lower energy states are populated with a certain number of excitons, the subsequent excitons must then occupy higher energy states due to the Pauli principle26. In CNTs, the quasi-1D electronic structure differs from QDs in that excitons are mobile along the tube direction and thereby a new multiexciton ground state could be created at higher energy27. However, if somehow the exciton path is blocked, then the exciton is localized and lower dimensional effects such as state filling become important.…”
Section: Resultsmentioning
confidence: 99%