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Insights into the Fe(3+) Doping Effects on the Structure and Electron Distribution of Cr(2)O(3) Nanoparticles

Herein, we carefully investigated the Fe(3+) doping effects on the structure and electron distribution of Cr(2)O(3) nanoparticles using X-ray diffraction analysis (XRD), maximum entropy method (MEM), and density functional theory (DFT) calculations. We showed that increasing the Fe doping induces an...

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Detalles Bibliográficos
Autores principales: Santos, Cledson, Attah-Baah, John M., Junior, Romualdo S. Silva, Mâcedo, Marcelo A., Rezende, Marcos V. S., Matos, Robert S., Ţălu, Ştefan, Trong, Dung Nguyen, da Paz, Simone P. A., Angélica, Rômulo S., Ferreira, Nilson S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10059910/
https://www.ncbi.nlm.nih.gov/pubmed/36985876
http://dx.doi.org/10.3390/nano13060980
Descripción
Sumario:Herein, we carefully investigated the Fe(3+) doping effects on the structure and electron distribution of Cr(2)O(3) nanoparticles using X-ray diffraction analysis (XRD), maximum entropy method (MEM), and density functional theory (DFT) calculations. We showed that increasing the Fe doping induces an enlargement in the axial ratio of c/a, which is associated with an anisotropic expansion of the unit cell. We found that as Fe(3+) replaces Cr in the Cr(2)O(3) lattice, it caused a higher interaction between the metal 3d states and the oxygen 2p states, which led to a slight increase in the Cr/Fe–O1 bond length followed by an opposite effect for the Cr/Fe–O2 bonds. Our results also suggest that the excitations characterize a well-localized bandgap region from occupied Cr d to unoccupied Fe d states. The Cr(2)O(3) and Fe-doped Cr(2)O(3) nanoparticles behave as Mott–Hubbard insulators due to their band gap being in the d−d gap, and Cr 3d orbitals dominate the conduction band. These findings suggest that the magnitude and the character of the electronic density near the O atom bonds in Cr(2)O(3) nanoparticles are modulated by the Cr–Cr distances until its stabilization at the induced quasi-equilibrium of the Cr(2)O(3) lattice when the Fe(3+) doping values reaches the saturation level range.