Tetrahedral clusters of copper(II): Crystal structures and magnetic properties of Cu2Te2O5X2 (X = Cl, Br)

Citation
M. Johnsson et al., Tetrahedral clusters of copper(II): Crystal structures and magnetic properties of Cu2Te2O5X2 (X = Cl, Br), CHEM MATER, 12(10), 2000, pp. 2853-2857
Citations number
17
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
CHEMISTRY OF MATERIALS
ISSN journal
08974756 → ACNP
Volume
12
Issue
10
Year of publication
2000
Pages
2853 - 2857
Database
ISI
SICI code
0897-4756(200010)12:10<2853:TCOCCS>2.0.ZU;2-3
Abstract
The isostructural compounds of general formula Cu2Te2O5X2 (X = Cl, Br) have been synthesized by chemical transport reaction. They crystallize in the t etragonal system, space group P (4) over bar with alpha = 7.6209(3) Angstro m, c = 6.3200(4) Angstrom, and a = 7.8355(2) Angstrom, c = 6.3785(2) A for Cu2Te2O5Cl2 and Cu2Te2O5Br2 respectively. The three-dimensional network is built up by tetrahedral clusters of copper(II) in distorted square planar c oordination, isolated in the [100] and [010] directions by [Te2O5E2] groups and in the [001] direction by [TeO3E] tetrahedra. This leads to what can b e described as spin tubes in the [001] direction surrounded by large tunnel s where 5s(2) tellurium(IV) lone pairs and chlorine and bromine atoms inter act. A careful analysis of the temperature dependence of the susceptibility reveals that even from the magnetic point of view, the building bricks are tetrahedra with all couplings roughly equivalent, and not squares with sma ll diagonal couplings. These systems are thus expected to have very interes ting magnetic properties, including a large singlet-triplet gap, and a band of singlet states inside this gap.