Materials Map

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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Barwani, Muataz Al

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in Cooperation with on an Cooperation-Score of 37%

Topics

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)1citations
  • 2018Atomistic and ab initio DFT modelling of the defect structures in Al3+/Cr3+-doped and co-doped Y3Fe5O12 9citations
  • 2012Atomistic simulation and ab initio study of the defect structure of spinel-related Li 0.5-0.5xMg xFe 2.5-0.5xO 4 7citations
  • 2012Unusual surface and edge morphologies, sp2 to sp3 hybridized transformation and electronic damage after Ar+ ion irradiation of few-layer graphene surfaces29citations
  • 2011Self-assembly of CuSO 4 nanoparticles and bending multi-wall carbon nanotubes on few-layer graphene surfaces4citations

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Chart of shared publication
Widatallah, H. M.
2 / 5 shared
Elzain, M. E.
1 / 1 shared
Al-Rashdi, K. S.
1 / 1 shared
Moore, E. A.
2 / 3 shared
Widatallah, Hisham M.
1 / 3 shared
Elzain, Mohamed E.
1 / 2 shared
Moore, Elaine A.
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Babo, A. A.
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Elzain, M.
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Anantharaman, Maliemadom Ramaswamy
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Hysen, Thomas
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Koraa, Amal
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Elzain, Mohammed
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Al-Harthi, Salim Hamood
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Myint, Myo Tay Zar
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Al-Harthi, S. H.
1 / 3 shared
Al-Hinai, Ashraf T.
1 / 1 shared
Al-Naamani, N.
1 / 1 shared
Al-Amri, Issa
1 / 1 shared
Hysen, T.
1 / 1 shared
Chart of publication period
2023
2018
2012
2011

Co-Authors (by relevance)

  • Widatallah, H. M.
  • Elzain, M. E.
  • Al-Rashdi, K. S.
  • Moore, E. A.
  • Widatallah, Hisham M.
  • Elzain, Mohamed E.
  • Moore, Elaine A.
  • Babo, A. A.
  • Elzain, M.
  • Anantharaman, Maliemadom Ramaswamy
  • Hysen, Thomas
  • Koraa, Amal
  • Elzain, Mohammed
  • Al-Harthi, Salim Hamood
  • Myint, Myo Tay Zar
  • Al-Harthi, S. H.
  • Al-Hinai, Ashraf T.
  • Al-Naamani, N.
  • Al-Amri, Issa
  • Hysen, T.
OrganizationsLocationPeople

article

Atomistic and ab initio DFT modelling of the defect structures in Al3+/Cr3+-doped and co-doped Y3Fe5O12

  • Widatallah, Hisham M.
  • Elzain, Mohamed E.
  • Moore, Elaine A.
  • Barwani, Muataz Al
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>

Topics
  • impedance spectroscopy
  • defect
  • density functional theory
  • defect structure