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Structural, morphological, and electrical properties of silver-substituted ZnAl(2)O(4) nanoparticles

In this paper, nanoparticles of [Image: see text] (x = 0.05 and x = 0.1) were synthesized by the sol–gel auto-combustion method and characterized by various techniques. X-ray diffraction (XRD) for structural characterization confirms the successful formation of a cubic spinel structure with the spac...

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Detalles Bibliográficos
Autores principales: Amghar, Mohamed, Bougoffa, Amira, Trabelsi, Abdessalem, Oueslati, Abderrazek, Dhahri, Essebti
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9135395/
https://www.ncbi.nlm.nih.gov/pubmed/35733679
http://dx.doi.org/10.1039/d2ra01800d
Descripción
Sumario:In this paper, nanoparticles of [Image: see text] (x = 0.05 and x = 0.1) were synthesized by the sol–gel auto-combustion method and characterized by various techniques. X-ray diffraction (XRD) for structural characterization confirms the successful formation of a cubic spinel structure with the space group Fd3̄m. Their morphology was evaluated with a scanning electron microscope (SEM) which shows an agglomeration of nanoparticles. To characterize the electrical behavior of our compounds, we used impedance spectroscopy at temperatures ranging from 313 K to 653 K and frequencies ranging from 0.1 Hz to 1 MHz. The experimental data for the real and imaginary impedance parts were mounted on the equivalent grain resistance (R(g))//fractal capacitance (CPE) circuit. Indeed, the activation energies extracted from the electrical conductivity and the resistance of the grain resistance (R(g)) closed and confirmed a transformation of the electrical behavior confirmed by a decrease in the resistance of the materials. The study of the alternating conductivity shows a Jonscher curve behavior and a thermally activated conduction process. The variation of the exponent “s” as a function of temperature shows, on the one hand, the presence of two models of conduction correlated barrier jump (CBH) and non-overlapping small polaron tunneling (NSPT) for x = 0.05 and, on the other hand, a CBH model for x = 0.1.