| 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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Smetana, Volodymyr
Stockholm University
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (55/55 displayed)
- 2024La-Ni-Si:A Gold Mine with a Diamond
- 2024Unusual superconductivity in crystallographically disordered RT2−xSn2 compounds
- 2024The crystal and electronic structure of RE$_{23}$Co$_{6.7}$In$_{20.3}$ (RE = Gd–Tm, Lu) : a new structure type based on intergrowth of AlB$_{2}$- and CsCl-type related slabscitations
- 2024The crystal and electronic structure of RE23Co6.7In20.3 (RE = Gd–Tm, Lu)citations
- 2024La-Ni-Si : a gold mine with a diamond
- 2024Intermetallics of 4:4:1 and 3:3:1 series in La–(Co,Ni)–M (M = Bi, Pb, Te, Sb, Sn and Ga, Al) systems and their propertiescitations
- 2024Unusual superconductivity in crystallographically disordered RT 2−x Sn 2 compounds
- 2024Ternary gallide Zr 7 Pd 7–x Ga 3+x (0 ≤ x ≤ 1.8):Synthesis, crystal and electronic structurescitations
- 2024La-Ni-Si: A Gold Mine with a Diamond
- 2023The Prolific Ternary System Pt/Sn/Ndcitations
- 2023Solubility limits, magnetic and magnetocaloric properties of MoB-type GdCo x Ni 1−x (0.47 ≤ x ≤ 0.72)citations
- 2023Investigation of the role of hydrogen bonding in ionic liquid-like salts with both N- and S-soft donorscitations
- 2023Crystal and electronic structures of the new ternary gallide Zr12Pd40−xGa31+y (x = 0–1.5, y = 0–0.5)citations
- 2023Enhanced stability and complex phase behaviour of organic-inorganic green-emitting ionic manganese halidescitations
- 2023Crystal and electronic structures of the new ternary gallide Zr 12 Pd 40−x Ga 31+y (x = 0–1.5, y = 0–0.5)citations
- 2023The Prolific Ternary System Pt/Sn/Nd:Insertion of Pt into the Structures of Sn/Nd Intermetallics Yields Structural Complexity and Wealthcitations
- 2023Honeycomb Constructs in the La-Ni Intermetallics : Controlling Dimensionality via p-Element Substitutioncitations
- 2022Four ternary silicides in the La-Ni-Si system:from polyanionic layers to frameworkscitations
- 2022Four ternary silicides in the La-Ni-Si system : from polyanionic layers to frameworkscitations
- 2022Crystal and electronic structures of a new hexagonal silicide Sc 38 Co 144 Si 97
- 2022Crystal and electronic structures of a new hexagonal silicide Sc38Co144Si97
- 2022Four ternary silicides in the La-Ni-Si systemcitations
- 2021New intermetallics R1+xZr1−xNi (R = Er–Tm, x ~ 0.5) with the TiNiSi type of structurecitations
- 2021Crystal and Magnetic Structures of the Ternary Ho2Ni0.8Si1.2and Ho2Ni0.8Ge1.2 Compoundscitations
- 2021Crystal and Magnetic Structures of the Ternary Ho2Ni0.8Si1.2 and Ho2Ni0.8Ge1.2 Compounds: An Example of Intermetallics Crystallizing with the Zr2Ni1{textendash}{xP} Prototypecitations
- 2020Metallic alloys at the edge of complexitycitations
- 2020A fivefold UO22+ node is a path to dodecagonal quasicrystal approximants in coordination polymerscitations
- 2020Binary Intermetallics in the 70 atom % R Region of Two R-Pd Systems (R = Tb and Er)citations
- 2020Ternary Polar Intermetallics within the Pt/Sn/R Systems (R = La-Sm)citations
- 2020Fluorinated Cationic Iridium(III) Complex Yielding an Exceptional, Efficient, and Long-Lived Red-Light-Emitting Electrochemical Cellcitations
- 2020Forcing Dicyanamide Coordination to f-Elements by Dissolution in Dicyanamide-Based Ionic Liquidscitations
- 2020Dehydration of UO2Cl2·3H2O and Nd(NO3)3·6H2O with a Soft Donor Ligand and Comparison of Their Interactions through X-ray Diffraction and Theoretical Investigationcitations
- 2019Alternative to the Popular Imidazolium Ionic Liquidscitations
- 2019Ionothermal Synthesis, Structures, and Magnetism of Three New Open Framework Iron Halide-Phosphatescitations
- 2018Supramolecularly Caged Green-Emitting Ionic Ir(III)-Based Complex with Fluorinated C^N Ligands and Its Application in Light-Emitting Electrochemical Cellscitations
- 2018R14(Au, M)51 (R = Y, La-Nd, Sm-Tb, Ho, Er, Yb, Lu; M = Al, Ga, Ge, In, Sn, Sb, Bi)citations
- 2018Controlling magnetism via transition metal exchange in the series of intermetallics Eu(T1, T2)5In (T = Cu, Ag, Au)citations
- 2018R14(Au, M)51(R = Y, La-Nd, Sm-Tb, Ho, Er, Yb, Lu; M = Al, Ga, Ge, In, Sn, Sb, Bi): Stability Ranges and Site Preference in the Gd14Ag51Structure Typecitations
- 2018Bringing order to large-scale disordered complex metal alloyscitations
- 2018From the Nonexistent Polar Intermetallic Pt3Pr4 via Pt2- xPr3 to Pt/Sn/Pr Ternariescitations
- 2018An Obscured or Nonexistent Binary Intermetallic, CO7Pr17, Its Existent Neighbor Co2Pr5, and Two New Ternaries in the System Co/Sn/Pr, CoSn3Pr1−x, and Co2−xSn7Pr3citations
- 2017Layered Structures and Disordered Polyanionic Nets in the Cation-Poor Polar Intermetallics CsAu1.4Ga2.8 and CsAu2Ga2.6citations
- 2017Gold Polar Intermetallicscitations
- 2017R3Au9Pn (R = Y, Gd-Tm; Pn = Sb, Bi): A Link between Cu10Sn3 and Gd14Ag51citations
- 2017R3Au9Pn (R = Y, Gd-Tm; Pn = Sb, Bi)citations
- 2016New R3Pd5 Compounds (R = Sc, Y, Gd-Lu)citations
- 2016New R3Pd5Compounds (R = Sc, Y, Gd–Lu): Formation and Stability, Crystal Structure, and Antiferromagnetismcitations
- 2016Gold in the Layered Structures of R3Au7Sn3: From Relativity to Versatilitycitations
- 2016Gd3Ni2 and Gd3CoxNi2-xcitations
- 2016Gd3Ni2and Gd3CoxNi2−x: magnetism and unexpected Co/Ni crystallographic orderingcitations
- 2016Gold in the Layered Structures of R3Au7Sn3citations
- 2015Cation-Poor Complex Metallic Alloys in Ba(Eu)-Au-Al(Ga) Systemscitations
- 2015Crystal Structure and Bonding in BaAu5Ga2 and AeAu4+ xGa3- x (Ae = Ba and Eu)citations
- 2015Gold-rich R3Au7Sn3: establishing the interdependence between electronic features and physical propertiescitations
- 2015Gold-rich R3Au7Sn3citations
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article
Gd3Ni2 and Gd3CoxNi2-x
Abstract
<p>The crystal structure, composition and physical properties of Gd<sub>3</sub>Ni<sub>2</sub>, which was earlier reported to exist in the Gd-Ni system without any details of its structure and properties, have been determined. This rare earth binary compound is a high-temperature phase: it forms via a peritectic reaction at 988 K (715 °C) and decomposes below ≈923 K (650 °C). The compound can be retained at room temperature as a metastable phase by quenching after high temperature annealing. Gd<sub>3</sub>Ni<sub>2</sub> crystallizes in the monoclinic Dy<sub>3</sub>Ni<sub>2</sub> structure type [mS20, C2/m (No. 12), Z = 4; with lattice parameters a = 13.418(3) Å, b = 3.720(1) Å, c = 9.640(2) Å, β = 106.250(3)°]. Ni can be substituted by Co up to 50% (i.e. up to and including Gd<sub>3</sub>CoNi) with no change in the structural prototype; the substitution of Co for Ni stabilizes the R<sub>3</sub>Co<sub>x</sub>Ni<sub>2-x</sub> phases down to room temperature. The crystal structure, magnetic properties and magnetocaloric effect (MCE) have been investigated for both Gd<sub>3</sub>Ni<sub>2</sub> and the related Gd<sub>3</sub>Co<sub>x</sub>Ni<sub>2-x</sub> solid solution alloys (0 ≤ x ≤ 1). The crystal structure of the Gd<sub>3</sub>CoNi is a ternary ordered derivative of the monoclinic Dy<sub>3</sub>Ni<sub>2</sub>-type, where Co fully occupies only one of the two 4i Wyckoff sites available for the transition metal. To the best of our knowledge, this is the first example of an intermetallic phase showing ordered site occupations by the chemically quite similar elements Co and Ni. All compounds show long range ferromagnetic ordering, with T<sub>C</sub> progressively increasing from 147 K (for Gd<sub>3</sub>Ni<sub>2</sub>) to 176 K (for Gd<sub>3</sub>CoNi) as a cubic function of the Co content. Evidence of Co contributing to the magnetic interactions in these compounds has been found. First-principles total energy calculations predicted the ordered occupation of Co and Ni at the crystallographic sites of Gd<sub>3</sub>CoNi, which was later confirmed by single crystal X-ray diffraction. The increased conduction electronic state (3d) exchange splitting at the Fermi level supports the experimentally observed enhanced Curie temperature in Gd<sub>3</sub>CoNi compared to Gd<sub>3</sub>Ni<sub>2</sub>.</p>