Younas, M., Nadeem, M., Atif, M., & Grössinger, R. (2011). Metal-semiconductor transition in NiFe₂O₄ nanoparticles due to reverse cationic distribution by impedance spectroscopy. Journal of Applied Physics, 109(9), 093704. https://doi.org/10.1063/1.3582142
E138-03 - Forschungsbereich Functional and Magnetic Materials
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Journal:
Journal of Applied Physics
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ISSN:
0021-8979
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Date (published):
6-May-2011
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Number of Pages:
8
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Publisher:
AMER INST PHYSICS
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Peer reviewed:
Yes
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Keywords:
General Physics and Astronomy
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Abstract:
Metal-semiconductor transition in NiFe2O4 nanoparticles due to reverse
cationic distribution by impedance spectroscopy
M. Younas,1 M. Nadeem,1,a) M. Atif,2 and R. Grossinger2
1EMMG, Physics Division, PINSTECH, P.O. Nilore, Islamabad, Pakistan
2Institute of Solid State Physics, Technical University of Vienna, Wiedner Hauptstrasse 8-10,
A-1040 Vienna, Austria
(Received 1 December 2010; accepted 24 March 2011; published online 6 May 2011)
We have investigated the magnetic and electrical response of the sol-gel synthesized NiFe2O4
nanoparticles. Changes in the impedance plane plots with temperature have been discussed and
correlated to the microstructure of the material. Thermally activated hopping carriers between
Fe3þ-Fe2þ and Ni2þ-Ni3þ ions have been determined for a decrease in the resistance of the sample
and a change in the conduction mechanism around 318 K. The mixed spinel structure and broken
exchange bonds due to small size effects are due to the canted spin structure at the surface of the
nanoparticles. The magnetization is found to be influenced by the surface spin canting and
anisotropy. We have established the semiconducting to metallic transition (SMT) temperature to be
around 358 K in terms of localized and delocalized eg electrons along with a transition from less
conductive [Fe3þ-O2 -Fe3þ] and [Ni2þ-O2 -Ni2þ] linkage to more conductive [Fe3þ-Fe2þ] and
[Ni2þ-Ni3þ] linkage at the octahedral B site. A decrease in the dielectric constant with temperature
has been discussed in terms of the depletion of space charge layers due to the repulsion of
delocalized eg electrons from the grain boundary planes. The anomalies in tangent loss and
conductivity data around 358 K are