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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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Latturner, Susan E.
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Topics
Publications (4/4 displayed)
- 2011Influence of the La/M Network on Magnetic Properties of Mn4 Tetrahedra in Intermetallic Compounds La21−δMn8M7C12 (M = Ge, Sn, Sb, Te, Bi)citations
- 2010Ca2LiC3H: a new complex carbide hydride phase grown in metal flux.citations
- 2010Ruthenium intermetallics grown from La-Ni flux: synthesis, structure, and physical properties.citations
- 2010Structural relationships between new carbide La14Sn(MnC6)3 and fully ordered La11(MnC6)3citations
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article
Ruthenium intermetallics grown from La-Ni flux: synthesis, structure, and physical properties.
Abstract
Crystals of three new intermetallic compounds were grown from reactions of ruthenium with other elements in La(0.8)Ni(0.2) eutectic flux. The new boride LaRu(2)Al(2)B crystallizes in a filled CeMg(2)Si(2) structure type (P4/mmm, a = 4.2105(5) A, c = 5.6613(8); Z = 1, R(1) = 0.014), with Ru atoms forming a planar square net; B atoms center alternating Ru squares, which is an unusual coordination of boron by transition metals. Al atoms connect the Ru(2)B layers, forming large voids where La ions reside. The chemical bonding analysis using the electron localization function (ELF) reveals two-center covalent bonding between Al atoms, an absence of direct Ru-Ru interactions, and three-centered bonds between Ru and B or Al atoms. The band structure calculation shows LaRu(2)Al(2)B to be metallic, which is in agreement with the observed temperature independent paramagnetism and heat capacity data. The crystal structure of La(2)Ni(2-x)Ru(x)Al (HT-Pr(2)Co(2)Al-type; x = 0.21(1) and x = 0.76(1); C2/c; a = 9.9001(3) A, b = 5.7353(1) A, c = 7.8452(2) A, beta = 104.275(1); Z = 4, R(1) = 0.016 for x = 0.76(1)) features infinite [Ni(2-x)Ru(x)Al] spiral-twisted chains composed of Al(2)M(2)-rhombic units (M = Ni/Ru) seen in many La-Ni-Al intermetallics. The structure of La(6)SnNi(3.67)Ru(0.76)Al(3.6) (Nd(6)Co(5)Ge(2.2)-type; P6m2, a = 9.620(1) A, c = 4.2767(9) A; Z = 1, R(1) = 0.015) is composed of a three-dimensional [Ni(3.67)Ru(0.76)Al(3.6)](3)(infinity) network with large hexagonal channels accommodating interconnected tin-centered lanthanum clusters Sn@La(9).