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First Isolated "Hypoelectronic" [In6]6- Cluster in Insulating Cs22In6(SiO4)4

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Nuss,  J.
Abteilung Jansen, Former Departments, Max Planck Institute for Solid State Research, Max Planck Society;
Department Quantum Materials (Hidenori Takagi), Max Planck Institute for Solid State Research, Max Planck Society;

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Wedig,  U.
Abteilung Jansen, Former Departments, Max Planck Institute for Solid State Research, Max Planck Society;
Department Quantum Materials (Hidenori Takagi), Max Planck Institute for Solid State Research, Max Planck Society;

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Jansen,  M.
Abteilung Jansen, Former Departments, Max Planck Institute for Solid State Research, Max Planck Society;

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Citation

Saltykov, V., Nuss, J., Wedig, U., Prasad, D. L. V. K., & Jansen, M. (2011). First Isolated "Hypoelectronic" [In6]6- Cluster in Insulating Cs22In6(SiO4)4. Zeitschrift für anorganische und allgemeine Chemie, 637(7-8), 834-839.


Cite as: https://hdl.handle.net/21.11116/0000-000E-BFEB-3
Abstract
Cs(22)In(6)(SiO(4))(4) was synthesized by the reaction of appropriate starting materials at 673 K, followed by slow cooling to room temperature, in arc-welded tantalum ampoules. According to single-crystal X-ray analysis, the compound crystallizes in a new structure type (P2(1)/n (no. 14), a = 14.3533(4), b = 16.1712(4), c = 25.0135(7) angstrom, beta = 94.368(1), Z = 4), consisting of [In(6)](6) clusters with the shape of a distorted octahedron or more appropriately described as a condensate of three face sharing tetrahedra. The cluster is the first example of a "hypoelectronic" isolated [In(6)](6) indium cluster. The oxosilicate indide can be regarded as a "double salt", Cs(6)In(6) on one hand and the oxosilicate Cs(4)SiO(4) (x 4) on the other, which form the quaternary structure by inhomogeneous intergrowth of partial structures. The electronic structure of Cs(22)In(6)(SiO(4))(4) was examined by DFT calculations and compared to the one of Rb(2)In(3), which exhibits linked In(6) polyhedra. According to the DOS the title compound is a semiconductor with a band gap of 0.5 eV, which is in agreement with its observed insulating character. [In(6)](6) is an "isolated" cluster bearing inert electron pairs at each vertex. In contrast, [In(6)](4) in Rb(2)In(3) only exhibits inert pairs at the apical atoms. The four basal atoms are linked to neighboring clusters by covalent bonds forming a 2D network. These bonding scenarios are supported by the analysis of the projected density of states, the electron localization function and the partitioning of the electron density according to Bader.