| Literature DB >> 21202162 |
Abstract
Single crystals of dizinc tellurium dibromide trioxide, Zn(2)(TeO(3))Br(2), were synthesized via a transport reaction in sealed evacuated silica tubes. The compound has a layered crystal structure in which the building units are [ZnO(4)Br] distorted square pyramids, [ZnO(2)Br(2)] distorted tetra-hedra, and [TeO(3)E] tetra-hedra (E being the 5s(2) lone pair of Te(4+)) joined through sharing of edges and corners to form layers of no net charge. Bromine atoms and tellurium lone pairs protrude from the surfaces of each layer towards adjacent layers. This new compound Zn(2)(TeO(3))Br(2) is isostructural with the synthetic compounds Zn(2)(TeO(3))Cl(2), CuZn(TeO(3))(2), Co(2)(TeO(3))Br(2) and the mineral sophiite, Zn(2)(SeO(3))Cl(2).Entities:
Year: 2008 PMID: 21202162 PMCID: PMC2961122 DOI: 10.1107/S1600536808011252
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| Zn2(TeO3)Br2 | |
| Orthorhombic, | Mo |
| Hall symbol: -P 2ab 2ac | Cell parameters from 13770 reflections |
| θ = 3.7–33.2° | |
| µ = 23.79 mm−1 | |
| Block, colourless | |
| 0.21 × 0.16 × 0.04 mm |
| Oxford Diffraction Xcalibur3 diffractometer | 1290 independent reflections |
| Radiation source: fine-focus sealed tube | 1201 reflections with |
| graphite | |
| φ and ω scans | θmax = 26.3°, θmin = 4.1° |
| Absorption correction: analytical ( | |
| 15561 measured reflections |
| Refinement on | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| (Δ/σ)max = 0.001 | |
| Δρmax = 1.08 e Å−3 | |
| 1290 reflections | Δρmin = −0.82 e Å−3 |
| 74 parameters | Extinction correction: |
| 0 restraints | Extinction coefficient: 0.00342 (15) |
| Experimental. a multifaceted crystal model based on expressions derived by Clark & Reid (1995)] |
| Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
| Refinement. Refinement of |
| Te | 0.02983 (3) | 0.592957 (18) | 0.21187 (3) | 0.01207 (12) | |
| Zn1 | −0.00948 (6) | 0.39234 (4) | 0.34333 (7) | 0.01639 (15) | |
| Zn2 | 0.26526 (5) | 0.52410 (4) | 0.39968 (7) | 0.01671 (16) | |
| Br2 | 0.20748 (5) | 0.37261 (3) | 0.43887 (7) | 0.02286 (16) | |
| Br1 | −0.08838 (7) | 0.29014 (3) | 0.15586 (7) | 0.03163 (18) | |
| O2 | 0.1882 (3) | 0.5524 (2) | 0.1440 (4) | 0.0160 (7) | |
| O1 | −0.0568 (3) | 0.4903 (2) | 0.1969 (4) | 0.0155 (7) | |
| O3 | 0.0906 (3) | 0.5786 (2) | 0.4378 (4) | 0.0158 (7) |
| Te | 0.0105 (2) | 0.01301 (18) | 0.01267 (17) | 0.00006 (11) | −0.00162 (10) | 0.00168 (10) |
| Zn1 | 0.0188 (3) | 0.0174 (3) | 0.0130 (3) | 0.0018 (2) | 0.0002 (2) | −0.0011 (2) |
| Zn2 | 0.0110 (3) | 0.0260 (3) | 0.0132 (3) | 0.0033 (2) | −0.0005 (2) | −0.0016 (2) |
| Br2 | 0.0163 (3) | 0.0204 (3) | 0.0318 (3) | 0.0013 (2) | −0.00128 (19) | 0.00377 (19) |
| Br1 | 0.0530 (4) | 0.0191 (3) | 0.0227 (3) | −0.0070 (3) | −0.0101 (2) | −0.0017 (2) |
| O2 | 0.0094 (17) | 0.0266 (19) | 0.0120 (14) | 0.0012 (14) | 0.0001 (12) | −0.0007 (13) |
| O1 | 0.0125 (18) | 0.0165 (16) | 0.0174 (15) | −0.0034 (14) | −0.0037 (13) | 0.0013 (13) |
| O3 | 0.0138 (18) | 0.0230 (18) | 0.0105 (15) | 0.0024 (15) | −0.0023 (12) | −0.0016 (12) |
| Te—O2 | 1.867 (3) | Zn1—Br2 | 2.4247 (8) |
| Te—O3 | 1.873 (3) | Zn2—O2ii | 2.002 (3) |
| Te—O1 | 1.891 (3) | Zn2—O1iii | 2.033 (3) |
| Zn1—O3i | 1.952 (3) | Zn2—O3 | 2.061 (3) |
| Zn1—O1 | 2.004 (3) | Zn2—O2 | 2.184 (3) |
| Zn1—Br1 | 2.3438 (8) | Zn2—Br2 | 2.5310 (8) |
| O2—Te—O3 | 85.00 (14) | O2ii—Zn2—O3 | 89.30 (13) |
| O2—Te—O1 | 96.31 (15) | O1iii—Zn2—O3 | 157.82 (14) |
| O3—Te—O1 | 96.55 (14) | O2ii—Zn2—O2 | 153.62 (18) |
| O3i—Zn1—O1 | 101.01 (14) | O1iii—Zn2—O2 | 92.03 (12) |
| O3i—Zn1—Br1 | 123.23 (11) | O3—Zn2—O2 | 73.00 (12) |
| O1—Zn1—Br1 | 96.62 (10) | O2ii—Zn2—Br2 | 99.54 (10) |
| O3i—Zn1—Br2 | 100.43 (10) | O1iii—Zn2—Br2 | 98.97 (10) |
| O1—Zn1—Br2 | 120.65 (10) | O3—Zn2—Br2 | 100.22 (10) |
| Br1—Zn1—Br2 | 115.54 (3) | O2—Zn2—Br2 | 102.69 (10) |
| O2ii—Zn2—O1iii | 98.37 (13) |