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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Barwani, Muataz Al
in Cooperation with on an Cooperation-Score of 37%
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Publications (5/5 displayed)
- 2023Computational modeling of the defect structure, hyperfine and magnetic properties of the Mn2+-doped magnetite of the composition MnxFe3-yO4 (y = ⅔ x)citations
- 2018Atomistic and ab initio DFT modelling of the defect structures in Al3+/Cr3+-doped and co-doped Y3Fe5O12 citations
- 2012Atomistic simulation and ab initio study of the defect structure of spinel-related Li 0.5-0.5xMg xFe 2.5-0.5xO 4 citations
- 2012Unusual surface and edge morphologies, sp2 to sp3 hybridized transformation and electronic damage after Ar+ ion irradiation of few-layer graphene surfacescitations
- 2011Self-assembly of CuSO 4 nanoparticles and bending multi-wall carbon nanotubes on few-layer graphene surfacescitations
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article
Atomistic and ab initio DFT modelling of the defect structures in Al3+/Cr3+-doped and co-doped Y3Fe5O12
Abstract
<p>The defect structures when Y<sub>3</sub>Fe<sub>5</sub>O<sub>12</sub> is doped with either Al<sup>3+</sup> or Cr<sup>3+</sup>, and evenly co-doped with both, which have been a matter of controversy in the literature, are modeled using atomistic and ab initio DFT methods. When Y<sub>3</sub>Fe<sub>5</sub>O<sub>12</sub> is doped with Al<sup>3+</sup>, the defect reaction energy obtained marginally favors the preferential substitution of Al<sup>3+</sup> for Fe<sup>3+</sup> at the tetrahedral sites as opposed to octahedral ones. This is indicative that for Al<sup>3+</sup>-doped samples processed at elevated temperatures, or containing undetected impurities, the substitution of Al<sup>3+</sup> for octahedral Fe<sup>3+</sup> is likely. To model the defect structure of the Cr<sup>3+</sup> -doped Y<sub>3</sub>Fe<sub>5</sub>O<sub>12</sub>, it was essential that the Cr<sup>3+</sup> ions crystal field stabilization energy (CFSE) and the Fe<sup>3+</sup>-O<sup>2-</sup>- Cr<sup>3+</sup> spin-spin coupling derived from the ab initio DFT calculations,be taken into account. The results show the substitution of the Cr<sup>3+</sup> ion for an octahedral Fe<sup>3+</sup> ion to be energetically favorable relative to its substitution for a tetrahedral Fe<sup>3+</sup> one. It is also shown that the antisite defect, where the Cr<sup>3+</sup> ion substitutes for Y<sup>3+</sup> at a dodecahedral site with the expelled Y<sup>3+</sup> ion substituting for an octahedral Fe<sup>3+</sup> ion, is possible under certain processing conditions. For the Al<sup>3+</sup> /Cr<sup>3+</sup> co-doped Y<sub>3</sub>Fe<sub>5</sub>O<sub>12</sub>, the Al<sup>3+</sup> and Cr<sup>3+</sup> ions were found to, respectively, substitute for the tetrahedral and octahedral Fe<sup>3+</sup> ions. The energy values obtained suggest this defect structure to be insensitive to the processing conditions and/or the presence of undetected impurities. The structural and magnetic implications of these defect structures are discussed.</p>