INFLUENCE OF AL3+ DOPING ON THE STRUCTURAL AND ELECTRICAL PROPERTIES OF NANOCRYSTALLINE NI0.7MG0.3ALXFE2-XO4 FERRITES

Razia Nongjai1*, Khalid Mujasam Batoo2, Shakeel Khan3
1Department of Applied Physics, Z.H. College of Engineering & Technology, Aligarh Muslim University Aligarh-202002, India
2Department of Applied Physics, Z.H. College of Engineering & Technology, Aligarh Muslim University Aligarh-202002, India
3Department of Applied Physics, Z.H. College of Engineering & Technology, Aligarh Muslim University Aligarh-202002, India
* Corresponding Author : razianongjai@gmail.com

Received : -     Accepted : -     Published : 15-06-2010
Volume : 1     Issue : 1       Pages : 1 - 3
Nanotechnol Nanosci 1.1 (2010):1-3

Conflict of Interest : None declared

Cite - MLA : Razia Nongjai, et al "INFLUENCE OF AL3+ DOPING ON THE STRUCTURAL AND ELECTRICAL PROPERTIES OF NANOCRYSTALLINE NI0.7MG0.3ALXFE2-XO4 FERRITES." Nanotechnology and Nanoscience 1.1 (2010):1-3.

Cite - APA : Razia Nongjai, Khalid Mujasam Batoo, Shakeel Khan (2010). INFLUENCE OF AL3+ DOPING ON THE STRUCTURAL AND ELECTRICAL PROPERTIES OF NANOCRYSTALLINE NI0.7MG0.3ALXFE2-XO4 FERRITES. Nanotechnology and Nanoscience, 1 (1), 1-3.

Cite - Chicago : Razia Nongjai, Khalid Mujasam Batoo, and Shakeel Khan "INFLUENCE OF AL3+ DOPING ON THE STRUCTURAL AND ELECTRICAL PROPERTIES OF NANOCRYSTALLINE NI0.7MG0.3ALXFE2-XO4 FERRITES." Nanotechnology and Nanoscience 1, no. 1 (2010):1-3.

Copyright : © 2010, Razia Nongjai, et al, Published by Bioinfo Publications. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution and reproduction in any medium, provided the original author and source are credited.

Abstract

Nanoparticles of Ni0.7Mg0.3 AlxFe2-xO4 (0.0 ≤ x ≤ 0.5) were prepared through sol-gel method to study the effect of Al3+ doping on structural and electrical properties using dielectric spectroscopy as a function of frequency at room temperature. The average particle size has been found between 25~30 nm. The dispersion in e’ , e’’, tanδ and σac with frequency shows that the dispersion is due to Maxwell-Wagner type of interfacial polarization in general and the hopping of charge between Fe2+ and Fe3+ as well as between Ni2+ and Ni3+ ions at B-sites.

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