| Literature DB >> 22807701 |
Faiz Rabbani1, Iwan Zimmermann, Mats Johnsson.
Abstract
The crystal structure of dicobalt(II) divanadium(V) disel-enium(IV) undeca-oxide, Co₂V₂Se₂O₁₁, exhibits a three-dimensional framework, the building units being distorted CoO₆ octa-hedra and VO₅ square pyramids arranged so as to form alternate chains along [010]. The framework has channels along [100] and [010] in which the two Ψ-SeO₃E (site symmetries m; E being the 4s² lone electron pair of Se(IV)) tetra-hedra reside and connect to the other building blocks. The structure contains corner- and edge-sharing CoO₆ octa-hedra, corner- and edge-sharing VO₅ square pyramids and edge-sharing Ψ-SeO₃E tetra-hedra. Co₂V₂Se₂O₁₁ is the first oxide containing all the cations Co(II), V(V) and Se(IV).Entities:
Year: 2012 PMID: 22807701 PMCID: PMC3393144 DOI: 10.1107/S1600536812027286
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| Co2V2Se2O11 | |
| Monoclinic, | Mo |
| Hall symbol: -P 2yb | Cell parameters from 1387 reflections |
| θ = 3.9–32.2° | |
| µ = 14.01 mm−1 | |
| β = 101.115 (5)° | Block, red |
| 0.05 × 0.03 × 0.02 mm | |
| Oxford Diffraction Xcalibur Sapphire3 diffractometer | 1534 independent reflections |
| Radiation source: fine-focus sealed tube | 1023 reflections with |
| Graphite monochromator | |
| Detector resolution: 16.5 pixels mm-1 | θmax = 32.3°, θmin = 3.9° |
| ω scans | |
| Absorption correction: analytical [ | |
| 4219 measured reflections |
| Refinement on | 0 restraints |
| Least-squares matrix: full | Primary atom site location: structure-invariant direct methods |
| Secondary atom site location: difference Fourier map | |
| (Δ/σ)max = 0.001 | |
| 1534 reflections | Δρmax = 1.28 e Å−3 |
| 85 parameters | Δρmin = −0.98 e Å−3 |
| 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 |
| Se1 | 0.38839 (12) | 0.2500 | 0.45047 (6) | 0.00668 (13) | |
| Se2 | 0.14374 (12) | 0.2500 | 0.89926 (5) | 0.00653 (13) | |
| Co1 | 0.95757 (12) | 0.42816 (6) | 0.63219 (5) | 0.00751 (13) | |
| V1 | 0.53298 (15) | 0.56239 (8) | 0.85002 (6) | 0.00660 (15) | |
| O1 | 0.6860 (8) | 0.2500 | 0.5658 (4) | 0.0105 (9) | |
| O6 | 0.7568 (6) | 0.4597 (3) | 0.7887 (3) | 0.0118 (6) | |
| O5 | 0.3738 (6) | 0.4001 (3) | 0.9523 (3) | 0.0107 (6) | |
| O2 | 0.2107 (6) | 0.0989 (3) | 0.4958 (3) | 0.0093 (6) | |
| O3 | 0.1701 (8) | 0.2500 | 0.7454 (4) | 0.0088 (9) | |
| O4 | 0.2448 (6) | 0.5786 (3) | 0.7407 (3) | 0.0132 (7) | |
| O7 | 0.6843 (8) | 0.7500 | 0.8501 (4) | 0.0077 (9) |
| Se1 | 0.0068 (3) | 0.0069 (3) | 0.0064 (3) | 0.000 | 0.0014 (2) | 0.000 |
| Se2 | 0.0080 (3) | 0.0051 (3) | 0.0063 (3) | 0.000 | 0.0008 (2) | 0.000 |
| Co1 | 0.0080 (3) | 0.0063 (3) | 0.0082 (3) | 0.0001 (2) | 0.0016 (2) | 0.0001 (2) |
| V1 | 0.0078 (3) | 0.0063 (3) | 0.0058 (3) | −0.0003 (3) | 0.0017 (3) | 0.0000 (3) |
| O1 | 0.008 (2) | 0.005 (2) | 0.017 (2) | 0.000 | −0.0012 (18) | 0.000 |
| O6 | 0.0140 (16) | 0.0077 (15) | 0.0148 (16) | 0.0010 (12) | 0.0059 (13) | −0.0014 (12) |
| O5 | 0.0153 (16) | 0.0113 (15) | 0.0045 (14) | −0.0088 (12) | −0.0003 (12) | −0.0024 (11) |
| O2 | 0.0106 (15) | 0.0103 (16) | 0.0071 (15) | −0.0021 (12) | 0.0021 (12) | −0.0024 (11) |
| O3 | 0.012 (2) | 0.006 (2) | 0.007 (2) | 0.000 | −0.0022 (17) | 0.000 |
| O4 | 0.0139 (16) | 0.0101 (16) | 0.0132 (16) | −0.0020 (12) | −0.0031 (13) | 0.0025 (12) |
| O7 | 0.009 (2) | 0.005 (2) | 0.010 (2) | 0.000 | 0.0024 (17) | 0.000 |
| Se1—O1 | 1.691 (4) | Co1—O6 | 2.093 (3) |
| Se1—O2 | 1.706 (3) | Co1—O4iv | 2.095 (3) |
| Se1—O2i | 1.706 (3) | Co1—O3iv | 2.122 (3) |
| Se2—O3 | 1.663 (4) | V1—O4 | 1.630 (3) |
| Se2—O5 | 1.750 (3) | V1—O6 | 1.635 (3) |
| Se2—O5i | 1.750 (3) | V1—O7 | 1.8147 (17) |
| Co1—O2ii | 2.074 (3) | V1—O5 | 2.038 (3) |
| Co1—O1 | 2.081 (3) | V1—O5v | 2.086 (3) |
| Co1—O2iii | 2.090 (3) | ||
| O1—Se1—O2 | 101.12 (13) | O2ii—Co1—O3iv | 91.59 (13) |
| O1—Se1—O2i | 101.12 (13) | O1—Co1—O3iv | 80.04 (12) |
| O2—Se1—O2i | 103.52 (19) | O2iii—Co1—O3iv | 172.01 (14) |
| O3—Se2—O5 | 98.85 (13) | O6—Co1—O3iv | 83.90 (13) |
| O3—Se2—O5i | 98.85 (13) | O4iv—Co1—O3iv | 88.29 (11) |
| O5—Se2—O5i | 98.97 (19) | O4—V1—O6 | 107.24 (15) |
| O2ii—Co1—O1 | 95.00 (14) | O4—V1—O7 | 101.71 (16) |
| O2ii—Co1—O2iii | 80.44 (12) | O6—V1—O7 | 102.62 (15) |
| O1—Co1—O2iii | 101.07 (12) | O4—V1—O5 | 95.11 (13) |
| O2ii—Co1—O6 | 171.78 (11) | O6—V1—O5 | 99.22 (13) |
| O1—Co1—O6 | 90.99 (14) | O7—V1—O5 | 146.92 (14) |
| O2iii—Co1—O6 | 103.94 (11) | O4—V1—O5v | 133.61 (14) |
| O2ii—Co1—O4iv | 92.69 (12) | O6—V1—O5v | 117.38 (13) |
| O1—Co1—O4iv | 166.17 (13) | O7—V1—O5v | 81.09 (14) |
| O2iii—Co1—O4iv | 91.51 (11) | O5—V1—O5v | 66.81 (12) |
| O6—Co1—O4iv | 80.34 (11) |