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dc.contributor.authorKiruthiga, J.en_US
dc.contributor.authorCHATTERJI, APRATIMen_US
dc.date.accessioned2019-02-25T09:01:37Z
dc.date.available2019-02-25T09:01:37Z
dc.date.issued2014-02en_US
dc.identifier.citationPhysical Review E, 89(2), 022304.en_US
dc.identifier.issn2470-0045en_US
dc.identifier.issn2470-0053en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/1951-
dc.identifier.urihttps://doi.org/10.1103/PhysRevE.89.022304en_US
dc.description.abstractWe present our conclusions of the investigation of the self-assembly and growth of an array of CdS nanotubes: a consequence of a fine balance of directed motion, diffusion, and aggregation of reacting Cd + 2 and S − 2 ions. In a previous communication [Kiruthiga and Chatterji, J. Chem. Phys. 138, 024905 (2013)], we identified the mechanism of an unexpected growth of a CdS nanocylinder of uniform radial cross section from the end of a nanochannel. Furthermore, the cylinder had a pore along the axis but was closed at one end. This unique phenomenon of self-assembly of very monodisperse CdS nanocylinders had been observed in a rather simple experiment where two chambers containing 0.1M Cd Cl 2 and 0.1M Na 2 S solutions were joined by an array of anodized aluminium oxide (AAO) nanochannels [ and , Phys. Rev. E 85, 056104 (2012)]. Interestingly, the growth of CdS nanotubes was observed only in the Na 2 S chamber. The primary focus of our previous study was on identifying the principles governing the growth of a single nanotube at the exit point of a single AAO nanochannel. In this communication, we identify factors affecting the self-assembly of a nanotube in the presence of other similar neighboring nanotubes growing out from an array of closely spaced AAO nanochannel exit points, a scenario closer to the experimental situation. Our model is not Cd + 2 or S − 2 specific, thus our conclusions suggest that the experimental scheme can be extended to the self-assembly of a general class of reacting-diffusing A and B ions with A (in this case Cd + 2 ions) selectively migrating out from a nanochannel. In particular, we note that after the initial growth of nanotubes for a period of time, there can arise a severe deficiency of B ions ( S − 2 ) near the AAO-nanochannel exits. The low concentration of B near the nanochannel exits impedes further growth of uniform CdS nanotubes. We further identify the parameters which can be tuned to obtain an improved crop of monodisperse nanotubes. Thereby we predict the necessary characteristics of reacting systems which can be self-assembled using suitable adaptations of experiments used to grow CdS cylinders.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectAxial poreen_US
dc.subjectInitial growth of nanotubesen_US
dc.subjectNanocylindersen_US
dc.subject2014en_US
dc.titleSelf-assembly of monodisperse CdS nanocylinders with an axial poreen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Een_US
dc.publication.originofpublisherForeignen_US
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