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PHYSICS
Atomic order and metallic nanoclusters in Na$_{4}$Ir$_{3}$O$_{8}$
M. V. Talanova, V. B. Shirokovb, V. M. Talanovc a Research Institute of Physics, Southern Federal University,
Rostov-on-Don, Russia
b Southern Scientific Center of Russian Academy of Sciences, Rostov-on-Don, Russia
c South-Russian State Polytechnical University, Novocherkassk, Russia
Abstract:
A theory for forming Ir-atomic nanoclusters in a dielectric matrix of Na$_{4}$Ir$_{3}$O$_{8}$ structure and spinel-like structures is suggested. The atomic order in the Na$_{4}$Ir$_{3}$O$_{8}$ structure is investigated by group-theoretical methods of phase transition theory. The critical irreducible representation $\tau$, generating appearance of enantiomorphic P 4$_{1}$32 (P 4$_{3}$32)-phases from high symmetry spinel-like phase with space group Fd3m, is six dimensional irreducible representation k$_{10}$($\tau_{1}$) (in Kovalev designation). Ir and Na atoms form an intriguing atom ordering, giving rise to a network of corner shared Ir triangles, called a hyperkagome lattice. It is shown that inside the hyperkagome lattice, there are closed metal contours of chemical bonds formed by Ir-clusters - decagons. Unusual physical properties of solid solutions on the basis of Na$_{4}$Ir$_{3}$O$_{8}$ are expected. The existence of hyperkagome lattices in six types in ordered spinel structures is theoretically predicted.
Keywords:
hyper-kagome order, ordered spinels, decagons, nanoclusters.
Received: 07.01.2015 Revised: 24.02.2015
Citation:
M. V. Talanov, V. B. Shirokov, V. M. Talanov, “Atomic order and metallic nanoclusters in Na$_{4}$Ir$_{3}$O$_{8}$”, Nanosystems: Physics, Chemistry, Mathematics, 6:3 (2015), 442–450
Linking options:
https://www.mathnet.ru/eng/nano958 https://www.mathnet.ru/eng/nano/v6/i3/p442
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