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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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Gainza, Javier
European Synchrotron Radiation Facility
in Cooperation with on an Cooperation-Score of 37%
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Publications (6/6 displayed)
- 2024New insights into the magnetism and magnetic structure of LuCrO<sub>3</sub> perovskitecitations
- 2023Structural stability, optical and thermoelectric properties of the layered RbSn2Br5 halide synthesized using mechanochemistrycitations
- 2022SnSe: Kx intermetallic thermoelectric polycrystals prepared by arc-meltingcitations
- 2021Structural evolution, optical gap and thermoelectric properties of CH3NH3SnBr3 hybrid perovskite, prepared by mechanochemistrycitations
- 2021Synergy of diffraction and spectroscopic techniques to unveil the crystal structure of antimonic acidcitations
- 2018Nanostructured Thermoelectric Chalcogenidescitations
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article
New insights into the magnetism and magnetic structure of LuCrO<sub>3</sub> perovskite
Abstract
<jats:p>A polycrystalline sample LuCrO<jats:sub>3</jats:sub> has been characterized by neutron powder diffraction (NPD) and magnetization measurements. Its crystal structure has been Rietveld refined from NPD data in space group <jats:italic>Pnma</jats:italic>; this perovskite contains strongly tilted CrO<jats:sub>6</jats:sub> octahedra with extremely bent Cr—O—Cr superexchange angles of ∼142°. The NPD data show that below Néel temperature (<jats:italic>T</jats:italic><jats:sub>N</jats:sub> ≃ 131 K), the magnetic structure can be defined as an A-type antiferromagnetic arrangement of Cr<jats:sup>3+</jats:sup> magnetic moments, aligned along the <jats:italic>b</jats:italic> axis, with a canting along the <jats:italic>c</jats:italic> axis. A noticeable magnetostrictive effect is observed in the unit-cell parameters and volume upon cooling down across <jats:italic>T</jats:italic><jats:sub>N</jats:sub>. The AC magnetic susceptibility indicates the onset of magnetic ordering below 112.6 K; the magnetization isotherms below <jats:italic>T</jats:italic><jats:sub>N</jats:sub> show a nonlinear behaviour that is associated with the described canting of the Cr<jats:sup>3+</jats:sup> magnetic moments. From the Curie–Weiss law, the effective moment of the Cr<jats:sup>3+</jats:sup> sublattice is found to be μ<jats:sub>eff</jats:sub> = 3.55 μ<jats:sub>B</jats:sub> (calculated 3.7 μ<jats:sub>B</jats:sub>) while the Θ<jats:sub>CW</jats:sub> parameter yields a value of −155 K, indicating antiferromagnetic interactions. There is a conspicuous increase of <jats:italic>T</jats:italic><jats:sub>N</jats:sub> upon the application of external pressure, which must be due to shortening of the Cr—O bond length under compression that increases the orbital overlap integral.</jats:p>