| People | Locations | Statistics |
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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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Doert, Thomas
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (41/41 displayed)
- 2024Comparison of local structure of CrCl3 bulk and nanocrystals above and below the structural phase transition
- 2023Nano-scale new Heusler compounds NiRh2Sb and CuRh2Sbcitations
- 2023Spontaneous polarization and pyroelectric coefficient of lithium niobate and lithium tantalate determined from crystal structure datacitations
- 2023In situ Investigations of the Formation Mechanism of Metastable γ ‐BiPd Nanoparticles in Polyol Reductions
- 2023Unconventional Spin State Driven Spontaneous Magnetization in a Praseodymium Iron Antimonidecitations
- 2022$mathrm{In}$ $mathrm{situ}$ investigation of the formation mechanism of $α$-Bi$_2$Rh nanoparticles in polyol reductionscitations
- 2022In situ investigation of the formation mechanism of α-Bi2Rh nanoparticles in polyol reductionscitations
- 2022Combined experimental and theoretical study of hydrostatic (He-gas) pressure effects in α-RuCl3citations
- 2021Freestanding Nanolayers of a Wide-Gap Topological Insulator through Liquid-Phase Exfoliationcitations
- 2021Freestanding Nanolayers of a Wide-Gap Topological Insulator through Liquid-Phase Exfoliation
- 2021Formation of Bi2Ir nanoparticles in a microwave-assisted polyol process revealing the suboxide Bi4Ir2Ocitations
- 2021Freestanding few-layer sheets of a dual topological insulatorcitations
- 2021Low Temperature Activation of Tellurium and Resource-Efficient Synthesis of AuTe2 and Ag2Te in Ionic Liquidscitations
- 2021Hydrothermal Synthesis, Crystal Structure, and Magnetism of Na2[Ir(OH)6] and its Dehydration to Na2IrO3citations
- 2021Tunable Potassium Ion Conductivity and Magnetism in Substituted Layered Ferratescitations
- 2021Atypical transport for GdTe1.8 upon substitution with Se: Strong electron-phonon coupling in polaronic conduction
- 2021Formation of Bi$_2$Ir nanoparticles in a microwave-assisted polyol process revealing the suboxide Bi$_4$Ir$_2$Ocitations
- 2021Ba3[Rh(OH)6]2 ⋅ H2O – a Precursor to Barium Oxorhodates with One-dimensional Hydrogen Bonding Systemscitations
- 2020Synthesis of $(Li_{2}Fe_{1–y}Mn_{y})SO$ Antiperovskites with Comprehensive Investigations of $(Li_{2}Fe_{0.5}Mn_{0.5})SO$ as Cathode in Li-ion Batteriescitations
- 2020Hydroflux syntheses and crystal structures of hydrogarnets Ba3[RE(OH)6]2(RE = Sc, Y, Ho-Lu)citations
- 2020The Hydrogarnets Sr3[RE(OH)6]2 (RE = Sc, Y, Ho – Lu): Syntheses, Crystal Structures, and their Thermal Decomposition to Ternary Rare-Earth Metal Oxidescitations
- 2020CaNa[Cr(OH)6] – A Layered Hydroxochromate(III) with Ordered Brucite Structure and its Thermal Decompositioncitations
- 2020The Weak 3D Topological Insulator Bi12Rh3Sn3I9
- 2019Syntheses, Crystal Structures and Physical Properties of Chromium and Rhodium Hydrogarnets Ca 3 [Cr(OH) 6 ] 2 , Sr 3 [Cr(OH) 6 ] 2 and Sr 3 [Rh(OH) 6 ] 2citations
- 2019Mechanism of Bi−Ni Phase Formation in a Microwave-Assisted Polyol Process
- 2018The Intermetalloid Cluster Cation (CuBi8)3+citations
- 2017Optimized Synthesis of the Bismuth Subiodides BmI4 (m = 4, 14, 16, 18) and the Electronic Properties of Bi14I4 and Bi18I4citations
- 2016Jeff Description of the Honeycomb Mott Insulator α-RuCl3citations
- 2016Downscaling Effect on the Superconductivity of Pd3Bi2X2 (X = S or Se) Nanoparticles Prepared by Microwave-Assisted Polyol Synthesiscitations
- 2016Resource-Efficient High-Yield Ionothermal Synthesis of Microcrystalline Cu3-xPcitations
- 2014Synthesis, crystal structures, spectroscopic and electrochemical studies on Cu(II) and Ni(II) complexes with compartmental nitrogen-oxygen mixed donor ligandscitations
- 2014Single-crystal X-ray diffraction investigation of the reversible order-disorder phase transition in iron-deficient TlFe2-xSe2citations
- 2013Tetragonal to orthorhombic phase transition of GdFeAsO studied by single-crystal X-ray diffractioncitations
- 2012Ternary lanthanum sulfide selenides α-LaS2-xSex (0<x<2) with mixed dichalcogenide anions X22- (X=S, Se)citations
- 2011Proliferation, differentiation and gene expression of osteoblasts in boron-containing associated with dexamethasone deliver from mesoporous bioactive glass scaffoldscitations
- 2011Bioactive SrO-SiO<sub>2</sub> glass with well-ordered mesopores: Characterization, physiochemistry and biological propertiescitations
- 2011High-pressure synthesis of rare-earth metal disulfides and diselenides LnX2 (Ln = Sm, Gd, Tb, Dy, Ho, Er and Tm; X = S, Se)citations
- 2005Incommensurately modulated CeSi1.82citations
- 2004Structure-Property Relations and Diffusion Pathways of the Silver Ion Conductor Ag5Te2Clcitations
- 2004Magnetic, electrical resistivity, heat-capacity, and thermopower anomalies in CeCuAs2citations
- 2003Enhanced electrical resistivity before Néel order in the metals RCuAs2 (R = Sm, Gd, Tb, and Dy)citations
Places of action
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article
Unconventional Spin State Driven Spontaneous Magnetization in a Praseodymium Iron Antimonide
Abstract
<jats:title>Abstract</jats:title><jats:p>Consolidating a microscopic understanding of magnetic properties is crucial for a rational design of magnetic materials with tailored characteristics. The interplay of 3d and 4f magnetism in rare‐earth transition metal antimonides is an ideal platform to search for such complex behavior. Here the synthesis, crystal growth, structure, and complex magnetic properties are reported of the new compound Pr<jats:sub>3</jats:sub>Fe<jats:sub>3</jats:sub>Sb<jats:sub>7</jats:sub> as studied by magnetization and electrical transport measurements in static and pulsed magnetic fields up to 56 T, powder neutron diffraction, and Mößbauer spectroscopy. On cooling without external magnetic field, Pr<jats:sub>3</jats:sub>Fe<jats:sub>3</jats:sub>Sb<jats:sub>7</jats:sub> shows spontaneous magnetization, indicating a symmetry breaking without a compensating domain structure. The Fe substructure exhibits noncollinear ferromagnetic order below the Curie temperature <jats:italic>T</jats:italic><jats:sub>C</jats:sub> ≈ 380 K. Two spin orientations exist, which approximately align along the Fe–Fe bond directions, one parallel to the <jats:italic>ab</jats:italic> plane and a second one with the moments canting away from the <jats:italic>c</jats:italic> axis. The Pr substructure orders below 40 K, leading to a spin‐reorientation transition (SRT) of the iron substructure. In low fields, the Fe and Pr magnetic moments order antiparallel to each other, which gives rise to a magnetization antiparallel to the external field. At 1.4 K, the magnetization approaches saturation above 40 T. The compound exhibits metallic resistivity along the <jats:italic>c</jats:italic> axis, with a small anomaly at the SRT.</jats:p>