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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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Mohan, Anita
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Publications (7/7 displayed)
- 2023Enhancement of Multiferroic and Optical Properties in BiFeO<sub>3</sub> Due to Different Exchange Interactions Between Transition and Rare Earth Ionscitations
- 2019Effect of Prehot Corrosion on Erosion Behavior of High Chromium Ferritic Steel for Heat Exchangerscitations
- 2017A Study on Mechanical Properties and Strengthening Mechanisms of AA5052/ZrB2 In Situ Compositescitations
- 2017High-Temperature Tribology of AA5052/ZrB2 PAMCscitations
- 2016Wear and Friction of AA5052-Al3Zr In Situ Composites Synthesized by Direct Melt Reactioncitations
- 2016Strengthening mechanisms of (Al<sub>3</sub>Zr<sub>mp</sub> + ZrB<sub>2np</sub>)/AA5052 hybrid compositescitations
- 2012Fabrication and Characterisation of Al-Al<sub>2</sub>O<sub>3</sub> Composite by Mechanical Alloyingcitations
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article
Enhancement of Multiferroic and Optical Properties in BiFeO<sub>3</sub> Due to Different Exchange Interactions Between Transition and Rare Earth Ions
Abstract
<jats:p>An experimental analysis of the Bi<jats:sub>0.90</jats:sub>Tb<jats:sub>0.1</jats:sub>Fe<jats:sub>0.90</jats:sub>Mn<jats:sub>0.1</jats:sub>O<jats:sub>3</jats:sub> system synthesized via the solid‐state method is presented in this report. UV–visible measurements are carried out and a smaller bandgap (i.e., semiconductor‐type behavior) is obtained. The structural phase of the present system is analyzed with X‐ray diffraction and neutron diffraction measurement. Structural‐phase analysis reveals that the system contains two nuclear phases (rhombohedral structure [R3c space group] with orthorhombic [Pn21a space group]). Moreover, also more bending in the bond angle is found, and the existence of a magnetic phase with a nuclear phase for the Bi<jats:sub>0.90</jats:sub>Tb<jats:sub>0.1</jats:sub>Fe<jats:sub>0.90</jats:sub>Mn<jats:sub>0.1</jats:sub>O<jats:sub>3</jats:sub> system is also confirmed by neutron diffraction. The magnetic moment versus temperature (<jats:italic>M</jats:italic>–<jats:italic>T</jats:italic>) curve demonstrates that the system's Néel transition temperature is at 568 K. The magnetization data show enhancement in the magnetic property by displaying the weak ferromagnetic‐type behavior at room temperature in the magnetic field versus magnetic moment (<jats:italic>M</jats:italic>–<jats:italic>H</jats:italic>) curve as compared to the parent compound. From dielectric measurement, the dielectric constant increases while the loss decreases.</jats:p>