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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=189519"><dc:title>Structure and spin-glass magnetism of the Fe$_{1.5}$Ni$_{1.5}$Ga$_4$ metallic alloy</dc:title><dc:creator>Buxi,	Krishnendu	(Avtor)
	</dc:creator><dc:creator>Pan,	Rahul	(Avtor)
	</dc:creator><dc:creator>Jagličić,	Zvonko	(Avtor)
	</dc:creator><dc:creator>Jelen,	Andreja	(Avtor)
	</dc:creator><dc:creator>Luzar,	Jože	(Avtor)
	</dc:creator><dc:creator>Mihor,	Peter	(Avtor)
	</dc:creator><dc:creator>Vrtnik,	Stanislav	(Avtor)
	</dc:creator><dc:creator>Koželj,	Primož	(Avtor)
	</dc:creator><dc:creator>Petrović,	Julia	(Avtor)
	</dc:creator><dc:creator>Avdeev,	Maxim	(Avtor)
	</dc:creator><dc:creator>Pratim Jana,	Partha	(Avtor)
	</dc:creator><dc:creator>Dolinšek,	Janez	(Avtor)
	</dc:creator><dc:subject>magnetic properties</dc:subject><dc:subject>alloys</dc:subject><dc:subject>intermetallics</dc:subject><dc:subject>thermodynamic properties</dc:subject><dc:subject>quantum mechanics</dc:subject><dc:description>The Ga-rich region of the Fe−Ni−Ga ternary system was investigated, by exploring a line of compositions Fe$_x$Ni$_{3−x}$Ga$_4$, with 0.5 ≤ x ≤ 2.5. The single-phase cubic material was found only at the composition Fe$_{1.5}$Ni$_{1.5}$Ga$_4$ and its immediate vicinity, representing a new phase in the Fe−Ni−Ga diagram. The homogeneity range of this phase was estimated by additionally exploring a set of compositions Fe$_x$Ni$_y$Ga$_z$ around the central composition Fe$_{1.5}$Ni$_{1.5}$Ga$_4$. The structural model was constructed based on the structure of the binary Ni$_3$Ga$_4$ parent phase, which crystallizes in the cubic Ia$\overline{3}$d space group. We have considered that by substituting Fe for Ni, the Ia$\overline{3}$d structure is preserved, with the Fe and Ni being statistically distributed at their 48g Wyckoff site. The possibility of a symmetry-reduced chiral structural model I4$_1$32 driven by chemical ordering of Fe and Ni cannot be entirely ruled out on the basis of the crystallographic study. The magnetic study of the Fe$_{1.5}$Ni$_{1.5}$Ga$_4$ phase has revealed that the material forms a spin glass phase below the spin freezing temperature T$_f$ ≈ 9 K. Since the spin glass ordering of the Fe and Ni magnetic moments is compatible with their random distribution, the magnetic study supports the disordered cubic Ia$\overline{3}$d model.</dc:description><dc:date>2026</dc:date><dc:date>2026-10-08 11:26:31</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>189519</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
