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<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=158315"><dc:title>Double helix of icosahedra structure and spin glass magnetism of the $\delta$-${\rm Co}_{2.5}{\rm Zn}_{17.5–x}{\rm Mn}_x (x = 0.4–3.5)$ pseudo-binary alloys</dc:title><dc:creator>Mondal,	Amit	(Avtor)
	</dc:creator><dc:creator>Koželj,	Primož	(Avtor)
	</dc:creator><dc:creator>Jagličić,	Zvonko	(Avtor)
	</dc:creator><dc:creator>Meden,	Anton	(Avtor)
	</dc:creator><dc:creator>Pratim Jana,	Partha	(Avtor)
	</dc:creator><dc:creator>Dolinšek,	Janez	(Avtor)
	</dc:creator><dc:subject>chemical structure</dc:subject><dc:subject>crystal structure</dc:subject><dc:subject>nucleic acid structure</dc:subject><dc:subject>quantum mechanics</dc:subject><dc:subject>transition metals</dc:subject><dc:description>We have synthesized $\delta$-${\rm Co}_{2.5}{\rm Zn}_{17.5–x}{\rm Mn}_x (x = 0.4–3.5)$ pseudo-binary alloys of 10 different compositions by a high-temperature solid-state synthetic route, determined their crystal structures and the Mn substitution pattern, and estimated the existence range of the $\delta$-phase. The alloys crystallize in two chiral enantiomorphic space groups $P6_2$ and $P6_4$, where the basic atomic polyhedron of the chiral structure is an icosahedron and the neighboring icosahedra share vertices to form an infinitely long double helix along the hexagonal axis (like in the $\delta$-${\rm Co}_{2.5}{\rm Zn}_{17.5}$ parent binary phase). The alloys are pure $\delta$-phase up to the ${\rm Mn}$ content $x \approx 3.5$. The ${\rm Mn}$ atoms partially substitute ${\rm Zn}$ atoms at particular crystallographic sites located on the icosahedra. The study of magnetism was performed on the ${\rm Co}_{2.5}{\rm Zn}_{17.1}{\rm Mn}_{0.4}$ alloy with the lowest ${\rm Mn}$ content. Contrary to the expectation that structural chirality may induce the formation of a nontrivial magnetic state, a spin glass state with no relation to the structural chirality was found. The magnetic sublattice contains all of the necessary ingredients (randomness and frustration) for the formation of a spin glass state. Typical out-of-equilibrium dynamic phenomena of a spin system with broken ergodicity were detected below the spin freezing temperature $T_f \approx 8$ K.</dc:description><dc:date>2024</dc:date><dc:date>2024-06-05 08:48:52</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>158315</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
