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Raman investigations of Zn 1− x Co x O nanocrystals: role of starting precursors on vibrational properties
Author(s) -
Bhargava Richa,
Sharma Prashant K.,
Kumar Sanjeev,
Pandey Avinash C.,
Kumar Naresh
Publication year - 2011
Publication title -
journal of raman spectroscopy
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.748
H-Index - 110
eISSN - 1097-4555
pISSN - 0377-0486
DOI - 10.1002/jrs.2924
Subject(s) - cobalt , raman spectroscopy , dopant , tetrahydrate , doping , inorganic chemistry , nanocrystal , chemistry , materials science , analytical chemistry (journal) , nuclear chemistry , crystallography , crystal structure , nanotechnology , organic chemistry , physics , optoelectronics , optics
The Raman spectra of sol–gel derived Co‐doped ZnO nanoparticles (NPs) in the spectral range 100–1500 cm −1 were investigated. In the sol–gel method, three different series of Co‐doped ZnO particles, i.e. Zn 1− x Co x O ( x = 0.05, 0.10, 0.15, and 0.20), were obtained using three different starting precursors, viz. cobalt chloride hexahydrate, cobalt acetate tetrahydrate, and cobalt nitrate hexahydrate, respectively. It has been observed that cobalt acetate is a better precursor in comparison to cobalt chloride and cobalt nitrate to obtain single‐phase Co‐doped ZnO NPs. As for cobalt acetate‐derived NPs, no hidden secondary phase of Co 3 O 4 was observed for the lower ( x = 0.05) Co concentration. The Fröhlich interaction associated with the longitudinal modes was found to be destroyed with increasing Co concentration due to structural disorder and defects induced by the dopant. In addition to ZnO and Co 3 O 4 vibrational modes, a few additional modes near 550 and 715 cm −1 were also observed in all cases, which could be attributed to the modes due to Co doping in ZnO. Copyright © 2011 John Wiley & Sons, Ltd.
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