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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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Schnelle, Walter
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (20/20 displayed)
- 2024Enhancement of the anomalous Hall effect by distorting the Kagome lattice in an antiferromagnetic materialcitations
- 2023Bismuth-Rich Intermetallic Rods with a Note of Zintl-Phasecitations
- 2023Nano-scale new Heusler compounds NiRh2Sb and CuRh2Sbcitations
- 2022Spiral magnetism, spin flop, and pressure-induced ferromagnetism in the negative charge-transfer-gap insulator Sr$_2$FeO$_4$citations
- 2022Spiral magnetism, spin flop, and pressure-induced ferromagnetism in the negative charge-transfer-gap insulator Sr2FeO4citations
- 2019Complex magnetic phase diagram of metamagnetic MnPtSi
- 2019Complex magnetic phase diagram of metamagnetic MnPtSi.citations
- 2018Local magnetism in MnSiPt rules the chemical bondcitations
- 2018Anomalous Hall effect in Weyl semimetal half-Heusler compounds RPtBi (R = Gd and Nd)citations
- 2016Superconductivity in Weyl semimetal candidate MoTe2citations
- 2014Ca3Pt4+xGe13−y and Yb3Pt4Ge13: new derivatives of the Pr3Rh4Sn13 structure typecitations
- 2012Dy₀.₆₄{Dy₅[Fe₂C₉]} : A complex carbide with a composite structurecitations
- 2012Dy0.64Dy5Fe2C9 : A complex carbide with a composite structurecitations
- 2010Thermal, Magnetic, Electronic and Superconducting Properties of Rare-Earth Metal Pentagermanides REGe5 (RE = La, Nd, Sm, Gd) and Synthesis of TbGe5citations
- 2010Valence of cerium ions in selected ternary compounds from the system Ce-Rh-Sn
- 2009Cationic Clathrate I Si46-xPxTey (6.6(1) < y < 7.5(1), x < 2y) : Crystal Structure, Homogeneity Range, and Physical Propertiescitations
- 2009The polar mixed-valent lanthanum iron(II, III) sulfide La3Fe2-δS7citations
- 2008The first silicon-based cationic clathrate III with high thermal stability: Si172-xPxTey (x=2y, y>20).citations
- 2008The layered metal Ti2PTe2citations
- 2007Sn20.5□3.5As22I8: A Largely Disordered Cationic Clathrate with a New Type of Superstructure and Abnormally Low Thermal Conductivitycitations
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article
The polar mixed-valent lanthanum iron(II, III) sulfide La3Fe2-δS7
Abstract
<p>La<sub>3</sub>Fe<sub>2-δ</sub>S<sub>7</sub> (δ=0.042(6)) was synthesized through a reaction of the elements in a LiCl/KCl flux at 970 K, and its structure was determined by single-crystal X-ray diffraction. The compound crystallizes in the polar hexagonal space group P6<sub>3</sub> with a=10.1906(6), c=5.9543(4) Å and Z=2, and adopts the Ce<sub>6</sub>Al<sub>10/3</sub>S<sub>14</sub> structure type. The structure contains both octahedral and tetrahedral iron sites: one-dimensional rods of face-sharing FeS<sub>6</sub> octahedra run along the 6<sub>3</sub> screw axis of the cell; FeS<sub>4</sub> tetrahedra, all pointing in the same direction, are stacked along the threefold rotation axes. The iron-centered polyhedra are linked by lanthanum atoms, which are coordinated by [7+1] sulfur atoms in a bicapped trigonal prismatic arrangement. <sup>57</sup>Fe Mößbauer spectroscopy confirms that Fe<sup>III</sup> and Fe<sup>II</sup> cations occupy the tetrahedral and octahedral iron sites, respectively. Magnetic susceptibility data indicate an antiferromagnetic transition at T<sub>N</sub>≈155 K. Density functional band structure calculations within the local density approximation reveal two covalent Fe-S subsystems within the compound that mix only weakly. A large anisotropy is indicated by bands that disperse predominantly along the hexagonal axis. The electronic band structure suggests pseudo-one-dimensional metallic conductivity along the rods of face-sharing FeS<sub>6</sub> octahedra. However, due to the defects on the Fe<sup>II</sup> positions, La<sub>3</sub>Fe<sub>2-δ</sub>S<sub>7</sub> shows an activated conducting behavior.</p>