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dc.contributor.authorBiswas, Kanishka-
dc.contributor.authorVarghese, Neenu-
dc.contributor.authorRao, C N R-
dc.date.accessioned2012-02-10T07:59:37Z-
dc.date.available2012-02-10T07:59:37Z-
dc.date.issued2008-07-
dc.identifier1005-0302en_US
dc.identifier.citationJournal of Materials Science Technology 24(4), 615-627 (2008)en_US
dc.identifier.urihttps://libjncir.jncasr.ac.in/xmlui/10572/370-
dc.descriptionRestricted Accessen_US
dc.description.abstractIn this article, we report the results of our detailed investigations of the growth kinetics of. zero-dimensional nanocrystals as well as one-dimensional nanorods by the combined use of small angel X-ray scattering (SAXS), transmission electron microscopy (TEM) along with other physical techniques. The study includes growth kinetics of gold nanocrystals formed by the reduction of HAuCl4 by tetrakis(hydroxymethyl) phosphonium chloride in aqueous solution, of CdSe nanocrystals formed by the reaction of cadmium stearate and selenium under solvothermal conditions, and of ZnO nanorods formed by the reaction of zinc acetate with sodium hydroxide under solvothermal conditions in the absence and presence of capping agents. The growth of gold nanocrystals does not follow the diffusion-limited Ostwald ripening, and instead follows a Sigmoidal rate curve. The heat change associated with the growth determined by isothermal titration calorimetry is about 10 kcal.mol(-1) per 1 nm increase in the diameter of the nanocrystals. In the case of CdSe nanocrystals also, the growth mechanism deviates from diffusion-limited growth and follows a combined model containing both diffusion and surface reaction terms. Our study of the growth kinetics of uncapped and poly(vinyl pyrollidone) (PVP)-capped ZnO nanorods has yielded interesting insights. We observe small nanocrystals next to the ZnO nanorods after a lapse of time in addition to periodic focusing and defocusing of the width of the length distribution. These observations lend support to the diffusion-limited growth model for the growth of uncapped ZnO nanorods. Accordingly, the time dependence on the length of uncapped nanorods follows the L-3 law as required for diffusion-limited Ostwald ripening. The PVP-capped nanorods, however, show a time dependence, which is best described by a combination of diffusion (L-3) and surface reaction (L-2) terms.en_US
dc.description.urihttp://www.jmst.org/EN/abstract/abstract8311.shtmlen_US
dc.language.isoenen_US
dc.publisherJournal of Materials Science Technologyen_US
dc.rights© 2008 Journal of Materials Science Technologyen_US
dc.subjectgrowth kineticsen_US
dc.subjectgold nanocrystalsen_US
dc.subjectCdSe nanocrystalsen_US
dc.subjectZnO nanorodsen_US
dc.subjectsmall angle X-ray scatteringen_US
dc.subjecttransmission electron microscopyen_US
dc.subjectOstwald ripening and sigmoidal growthen_US
dc.subjectCdse Nanocrystalsen_US
dc.subjectZno Nanoparticlesen_US
dc.subjectNoncoordinating Solventsen_US
dc.subjectSolvothermal Routeen_US
dc.subjectIn-Situen_US
dc.subjectIi-Vien_US
dc.subjectNucleationen_US
dc.subjectSizeen_US
dc.subjectMechanismen_US
dc.subjectEvolutionen_US
dc.titleGrowth Kinetics of Nanocrystals and Nanorods by Employing Small-angle X-ray Scattering (SAXS) and Other Techniquesen_US
dc.typeArticleen_US
Appears in Collections:Research Papers (Prof. C.N.R. Rao)

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