RUS  ENG
Full version
JOURNALS // Nanosystems: Physics, Chemistry, Mathematics // Archive

Nanosystems: Physics, Chemistry, Mathematics, 2015 Volume 6, Issue 3, Pages 442–450 (Mi nano958)

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.

PACS: 61.50.Ks; 36.40.-c

Received: 07.01.2015
Revised: 24.02.2015

Language: English

DOI: 10.17586/2220-8054-2015-6-3-442-450



Bibliographic databases:


© Steklov Math. Inst. of RAS, 2024