dc.contributor.author |
Biswas, Kanishka
|
|
dc.contributor.author |
Varghese, Neenu
|
|
dc.contributor.author |
Rao, C N R
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|
dc.date.accessioned |
2012-02-10T07:59:37Z |
|
dc.date.available |
2012-02-10T07:59:37Z |
|
dc.date.issued |
2008-07 |
|
dc.identifier |
1005-0302 |
en_US |
dc.identifier.citation |
Journal of Materials Science Technology 24(4), 615-627 (2008) |
en_US |
dc.identifier.uri |
https://libjncir.jncasr.ac.in/xmlui/10572/370 |
|
dc.description |
Restricted Access |
en_US |
dc.description.abstract |
In 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.uri |
http://www.jmst.org/EN/abstract/abstract8311.shtml |
en_US |
dc.language.iso |
en |
en_US |
dc.publisher |
Journal of Materials Science Technology |
en_US |
dc.rights |
© 2008 Journal of Materials Science Technology |
en_US |
dc.subject |
growth kinetics |
en_US |
dc.subject |
gold nanocrystals |
en_US |
dc.subject |
CdSe nanocrystals |
en_US |
dc.subject |
ZnO nanorods |
en_US |
dc.subject |
small angle X-ray scattering |
en_US |
dc.subject |
transmission electron microscopy |
en_US |
dc.subject |
Ostwald ripening and sigmoidal growth |
en_US |
dc.subject |
Cdse Nanocrystals |
en_US |
dc.subject |
Zno Nanoparticles |
en_US |
dc.subject |
Noncoordinating Solvents |
en_US |
dc.subject |
Solvothermal Route |
en_US |
dc.subject |
In-Situ |
en_US |
dc.subject |
Ii-Vi |
en_US |
dc.subject |
Nucleation |
en_US |
dc.subject |
Size |
en_US |
dc.subject |
Mechanism |
en_US |
dc.subject |
Evolution |
en_US |
dc.title |
Growth Kinetics of Nanocrystals and Nanorods by Employing Small-angle X-ray Scattering (SAXS) and Other Techniques |
en_US |
dc.type |
Article |
en_US |