Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Aug 31;68(Pt 9):i71. doi: 10.1107/S1600536812037038

Pb6Co9(TeO6)5

Christine Artner a, Matthias Weil a,*
PMCID: PMC3435567  PMID: 22969440

Abstract

Pb6Co9(TeO6)5, hexa­lead(II) nona­cobalt(II) penta­tellur­ate(VI), is isotypic with its nickel(II) analogue. The asymmetric unit contains two Pb atoms (site symmetries .2., ..2), four Co atoms (..2, ..2, 3.., 3.2) two Te atoms (..2, 3..) and six O atoms (all in general positions), with the Te and Co sites in octa­hedral coordination environments. The crystal structure can be subdivided into two types of layers parallel to (001). The first layer at z ≃ 0.25 is made up of edge-sharing [CoO6] and [TeO6] octa­hedra, with 1/6 of the octa­hedral holes not occupied. The second layer, situated at z ≃ 0, consist of an alternating arrangement of PbII atoms and of double octa­hedra that are made up from face-sharing [CoO6] and [TeO6] octa­hedra. The two types of layers are linked together through corner-sharing of [CoO6] and [TeO6] octa­hedra. The PbII atoms are situated in the cavities of the framework and are stereochemically active with one-sided [4]- and [6]-coordinations, respectively.

Related literature  

For the isotypic nickel analogue, see: Wedel et al. (1998). Reviews on the crystal chemistry of oxotellurates(VI) and of the geometry of [CoIIO6] polyhedra are given by Levason (1997) and Wildner (1992), respectively. For Pb5TeO8, see: Artner & Weil (2012). For the bond-valence method, see: Brown (2002).

Experimental  

Crystal data  

  • Pb6Co9(TeO6)5

  • M r = 2891.51

  • Hexagonal, Inline graphic

  • a = 10.3915 (1) Å

  • c = 13.6273 (2) Å

  • V = 1274.37 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 50.89 mm−1

  • T = 293 K

  • 0.07 × 0.06 × 0.05 mm

Data collection  

  • Bruker APEXII CCD diffractometer

  • Absorption correction: numerical (HABITUS; Herrendorf, 1997) T min = 0.123, T max = 0.200

  • 45686 measured reflections

  • 2262 independent reflections

  • 1908 reflections with I > 2σ(I)

  • R int = 0.068

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.025

  • wR(F 2) = 0.056

  • S = 1.09

  • 2262 reflections

  • 81 parameters

  • Δρmax = 2.96 e Å−3

  • Δρmin = −2.59 e Å−3

  • Absolute structure: Flack (1983), 882 Friedel pairs

  • Flack parameter: 0.134 (10)

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ATOMS for Windows (Dowty, 2006); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812037038/br2208sup1.cif

e-68-00i71-sup1.cif (24.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812037038/br2208Isup2.hkl

e-68-00i71-Isup2.hkl (111.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

Te1—O2 1.906 (5)
Te1—O6 1.991 (4)
Te2—O5 1.917 (6)
Te2—O3 1.937 (7)
Te2—O1i 1.939 (5)
Co1—O5ii 2.004 (6)
Co1—O6 2.262 (5)
Co2—O2 2.090 (6)
Co2—O3iii 2.090 (8)
Co2—O1 2.108 (6)
Co3—O3 2.107 (4)
Co4—O2 2.067 (7)
Co4—O1iv 2.071 (4)
Co4—O5v 2.116 (7)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic.

Acknowledgments

The X-ray centre of the Vienna University of Technology is acknowledged for providing access to the single-crystal diffractometer.

supplementary crystallographic information

Comment

Single crystals of the title compound, Pb6Co9(TeO6)5, were serendipitously obtained as a minority phase during phase formation studies in the system PbII/CoII/TeVI/O intended on crystal growth of cubic Pb2CoTeO6.

The crystal structure of Pb6Co9(TeO6)5 is isotypic with its nickel analogue (Wedel et al., 1998). The two Te(VI) and the four Co(II) atoms are in slightly distorted octahedral coordination environments with mean bond lengths of ¯d(Te—O) = 1.940 Å and ¯d(Co—O) = 2.105 Å, both in good agreement with literature data for oxotellurates (Levason, 1997) and for [CoO6] octahedra (Wildner, 1992). The two lead(II) atoms exhibit coordination numbers of four and six. The crresponding Pb—O, Te—O and M—O (M = Co, Ni) bond lengths are very similar in the two isotypic structures.

The crystal structure of Pb6Co9(TeO6)5 can be described in terms of (001) layers A at z≈ 0.25 and B at z≈ 0 that stack alternately along [100] (Fig. 1). In layer A [TeO6] and [CoO6] octahedra share edges with 1/6 of the octahedral holes at the 2c and 2d positions, both with site symmetry 3.2, not occupied. The corresponding vacancies, denominated as X1 at the 2d position and as X2 at the 2c position, have different sizes. X1 has a diagonal diameter of 4.1076 (8) Å whereas X2 is somewhat larger with a diagonal diameter of 4.3258 (8) Å. This difference might be correlated with the size of the surrounding octahedra. Whereas the smaller X1 vacancy is encircled by a ring of six [CoO6] octahedra, the larger X2 is encircled by a ring of three [CoO6] and three slightly smaller [TeO6] octahedra (Fig. 2). Layer B consists of double octahedra that are made up from face-sharing [CoO6] and [TeO6] octahedra, and by surrounding lead(II) atoms (Fig. 3). Adjacent A and B layers are linked together above and below the X1 and X2 vacancies through corner-sharing of [CoO6] and [TeO6] octahedra.

The resulting [Co9Te5O30]12- framework anion leaves space for the stereochemically active lead(II) cations. The oxygen coordination of the two Pb2+ cations is one-sided, with a [4]-coordination for Pb1 and a [6]-coordination for Pb2, if only Pb—O distances less than 2.75 Å are taken into account. The two cations share a common edge (O6—O6') with the lone pair electrons E pointing towards opposite directions. However, a bond valence calculation (Brown, 2002) shows a significant contribution of the four additional Pb—O distances for each of the two Pb atoms if interactions up to 3.5 Å are considered. Inclusion of these bonds increases the bond valence sum at Pb1 from 1.61 valence units (vu) to 1.83 vu and at Pb2 from 1.64 to 1.96 vu. The bond valence sum at O3 is also raised from 1.60 to 1.80 vu. Therefore the overall coordination of Pb1 might be described as [4 + 4] and that of Pb2 as [6 + 4] (Fig. 4).

Experimental

1.281 (5.7 mmol) PbO, 0.216 g (2.9 mmol) CoO and 0.914 g (5.7 mmol) TeO2 were mixed and thoroughly ground and heated in an alumina crucible under atmospheric conditions during 6 h to 1023 K and held at that temperature for 48 h. Then the furnace was shut-off. Several crystal phases could be identified from the cooled reaction mixture by single-crystal diffraction: Dark blue isometric crystals of Pb2CoTeO6, dark-red (nearly black) block-like crystals of Pb5TeO8 (Artner & Weil, 2012), colourless crystals of α-Al2O3 and dark red crystals of Pb6Co9(TeO6)5 with a block-like shape.

Refinement

The highest remaining electron density was found 1.49 Å from atom Pb1 and the lowest remaining electron density 0.52 Å from atom Pb2. The refined Flack parameter indicates racemic twinning with an approximate ratio of 1:6 for the twin components.

Figures

Fig. 1.

Fig. 1.

The crystal structure of Pb6Co9(TeO6)5 in a projection along [010]. Displacement ellipsoids are drawn at the 90% probability level. Letters A and B indicate the two types of layers present in the structure.

Fig. 2.

Fig. 2.

Layer A (situated approximately at z≈ 1/4) in the crystal structure of Pb6Co9(TeO6)5. Colour code and probability of the displacement parameters as in Fig. 1.

Fig. 3.

Fig. 3.

Layer B (situated approximately at z≈ 0) in the crystal structure of Pb6Co9(TeO6)5. Colour code and probability of the displacement parameters as in Fig. 1.

Fig. 4.

Fig. 4.

The coordination spheres around the two lead atoms, considering bond lengths up to 3.5 Å; short Pb—O distances < 2.75 Å are given in black, emphasizing the one-sided [4]-coordination for Pb1 and [6]-coordination for Pb2. Longer bonds augmenting the coordination spheres are given in yellow. Probability of the displacement parameters as in Fig. 1.

Crystal data

Pb6Co9(TeO6)5 Dx = 7.535 Mg m3
Mr = 2891.51 Mo Kα radiation, λ = 0.71073 Å
Hexagonal, P6322 Cell parameters from 6739 reflections
Hall symbol: P 6c 2c θ = 2.8–36.8°
a = 10.3915 (1) Å µ = 50.89 mm1
c = 13.6273 (2) Å T = 293 K
V = 1274.37 (3) Å3 Parallelepiped, dark red
Z = 2 0.07 × 0.06 × 0.05 mm
F(000) = 2470

Data collection

Bruker APEXII CCD diffractometer 2262 independent reflections
Radiation source: fine-focus sealed tube 1908 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.068
ω and φ scans θmax = 37.6°, θmin = 2.3°
Absorption correction: numerical (HABITUS; Herrendorf, 1997) h = −16→17
Tmin = 0.123, Tmax = 0.200 k = −17→17
45686 measured reflections l = −22→23

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0244P)2] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.025 (Δ/σ)max < 0.001
wR(F2) = 0.056 Δρmax = 2.96 e Å3
S = 1.09 Δρmin = −2.59 e Å3
2262 reflections Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
81 parameters Extinction coefficient: 0.00019 (3)
0 restraints Absolute structure: Flack (1983), 882 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.134 (10)

Special details

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 F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq
Pb1 0.26736 (3) 0.26736 (3) 0.0000 0.01216 (6)
Pb2 0.38848 (3) 1.0000 0.0000 0.01881 (8)
Te1 0.3333 0.6667 −0.09611 (4) 0.00407 (10)
Te2 0.16730 (4) 0.33460 (9) 0.2500 0.00433 (8)
Co1 0.3333 0.6667 0.11832 (9) 0.0066 (2)
Co2 0.16885 (10) 0.3377 (2) −0.2500 0.00664 (18)
Co3 0.0000 0.0000 0.2500 0.0087 (3)
Co4 0.00992 (19) 0.50496 (10) −0.2500 0.00566 (18)
O1 0.3366 (5) 0.3241 (5) −0.1717 (3) 0.0077 (8)
O2 0.1726 (7) 0.5050 (6) −0.1628 (3) 0.0083 (10)
O3 0.1702 (7) 0.1801 (6) 0.3277 (3) 0.0105 (9)
O5 0.3239 (8) 0.4818 (6) 0.3295 (3) 0.0076 (10)
O6 0.3481 (4) 0.5265 (4) −0.0034 (4) 0.0069 (6)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Pb1 0.01117 (9) 0.01117 (9) 0.01243 (12) 0.00429 (9) 0.00014 (9) −0.00014 (9)
Pb2 0.01104 (9) 0.01201 (13) 0.03372 (18) 0.00601 (7) −0.00268 (13) −0.0054 (3)
Te1 0.00414 (14) 0.00414 (14) 0.0039 (2) 0.00207 (7) 0.000 0.000
Te2 0.00362 (13) 0.00380 (19) 0.00564 (18) 0.00190 (10) 0.0002 (4) 0.000
Co1 0.0066 (3) 0.0066 (3) 0.0066 (5) 0.00332 (16) 0.000 0.000
Co2 0.0057 (3) 0.0069 (5) 0.0077 (4) 0.0035 (2) 0.0006 (10) 0.000
Co3 0.0061 (4) 0.0061 (4) 0.0140 (7) 0.00305 (19) 0.000 0.000
Co4 0.0031 (5) 0.0045 (3) 0.0089 (4) 0.0015 (2) 0.000 −0.0002 (3)
O1 0.011 (2) 0.008 (2) 0.0048 (15) 0.0055 (14) 0.0003 (13) −0.0022 (13)
O2 0.007 (2) 0.006 (2) 0.012 (2) 0.0022 (17) −0.0001 (16) −0.0034 (15)
O3 0.011 (2) 0.012 (2) 0.0077 (16) 0.0059 (15) 0.0000 (15) 0.0011 (15)
O5 0.004 (2) 0.006 (2) 0.0072 (18) −0.0011 (18) −0.0005 (18) 0.0009 (15)
O6 0.0058 (14) 0.0070 (14) 0.0075 (15) 0.0029 (11) −0.001 (2) 0.002 (2)

Geometric parameters (Å, º)

Pb1—O6i 2.387 (4) Te2—O3iii 1.937 (7)
Pb1—O6 2.387 (4) Te2—O3 1.937 (7)
Pb1—O1i 2.432 (4) Te2—O1xii 1.939 (5)
Pb1—O1 2.432 (4) Te2—O1i 1.939 (5)
Pb1—O3ii 3.327 (7) Co1—O5x 2.004 (6)
Pb1—O3iii 3.327 (7) Co1—O5iii 2.004 (6)
Pb1—O3iv 3.453 (7) Co1—O5xiii 2.004 (6)
Pb1—O3v 3.453 (7) Co1—O6vi 2.262 (5)
Pb1—Pb2vi 3.5764 (4) Co1—O6vii 2.262 (5)
Pb1—Pb2vii 3.5777 (2) Co1—O6 2.262 (5)
Pb2—O6viii 2.420 (3) Co2—O2xiv 2.090 (6)
Pb2—O6vii 2.420 (3) Co2—O2 2.090 (6)
Pb2—O2ix 2.726 (5) Co2—O3i 2.090 (8)
Pb2—O2vi 2.726 (5) Co2—O3iv 2.090 (8)
Pb2—O5x 2.727 (5) Co2—O1 2.108 (6)
Pb2—O5xi 2.727 (5) Co2—O1xiv 2.108 (6)
Pb2—O6vi 3.155 (3) Co3—O3xv 2.107 (4)
Pb2—O6ix 3.155 (3) Co3—O3 2.107 (4)
Pb2—O3xi 3.230 (4) Co3—O3xvi 2.107 (4)
Pb2—O3x 3.230 (4) Co3—O3xvii 2.107 (4)
Te1—O2vi 1.906 (5) Co3—O3iii 2.107 (4)
Te1—O2 1.906 (5) Co3—O3v 2.107 (4)
Te1—O2vii 1.906 (5) Co4—O2 2.067 (7)
Te1—O6vi 1.991 (4) Co4—O2xviii 2.067 (7)
Te1—O6vii 1.991 (4) Co4—O1vi 2.071 (4)
Te1—O6 1.991 (4) Co4—O1xiv 2.071 (4)
Te2—O5 1.917 (6) Co4—O5xix 2.116 (7)
Te2—O5iii 1.917 (6) Co4—O5iv 2.116 (7)
O6i—Pb1—O6 84.58 (16) O5iii—Te2—O1xii 85.9 (2)
O6i—Pb1—O1i 79.26 (18) O3iii—Te2—O1xii 87.0 (2)
O6—Pb1—O1i 77.79 (18) O3—Te2—O1xii 93.7 (2)
O6i—Pb1—O1 77.79 (18) O5—Te2—O1i 85.9 (2)
O6—Pb1—O1 79.26 (18) O5iii—Te2—O1i 93.3 (2)
O1i—Pb1—O1 148.79 (19) O3iii—Te2—O1i 93.7 (2)
O6i—Pb1—O3ii 95.87 (13) O3—Te2—O1i 87.0 (2)
O6—Pb1—O3ii 133.98 (17) O1xii—Te2—O1i 179.0 (3)
O1i—Pb1—O3ii 147.68 (15) O5x—Co1—O5iii 108.14 (14)
O1—Pb1—O3ii 56.26 (15) O5x—Co1—O5xiii 108.14 (14)
O6i—Pb1—O3iii 133.98 (17) O5iii—Co1—O5xiii 108.14 (14)
O6—Pb1—O3iii 95.87 (13) O5x—Co1—O6vi 87.99 (18)
O1i—Pb1—O3iii 56.26 (15) O5iii—Co1—O6vi 85.39 (19)
O1—Pb1—O3iii 147.68 (15) O5xiii—Co1—O6vi 153.55 (18)
O3ii—Pb1—O3iii 114.8 (2) O5x—Co1—O6vii 85.39 (19)
O6i—Pb1—O3iv 138.20 (17) O5iii—Co1—O6vii 153.55 (18)
O6—Pb1—O3iv 95.05 (13) O5xiii—Co1—O6vii 87.99 (18)
O1i—Pb1—O3iv 141.63 (15) O6vi—Co1—O6vii 72.17 (17)
O1—Pb1—O3iv 61.26 (14) O5x—Co1—O6 153.55 (18)
O3ii—Pb1—O3iv 55.44 (13) O5iii—Co1—O6 87.99 (18)
O3iii—Pb1—O3iv 87.73 (10) O5xiii—Co1—O6 85.39 (18)
O6i—Pb1—O3v 95.05 (13) O6vi—Co1—O6 72.17 (17)
O6—Pb1—O3v 138.20 (17) O6vii—Co1—O6 72.17 (17)
O1i—Pb1—O3v 61.26 (14) O2xiv—Co2—O2 87.8 (3)
O1—Pb1—O3v 141.63 (15) O2xiv—Co2—O3i 92.52 (17)
O3ii—Pb1—O3v 87.73 (10) O2—Co2—O3i 174.4 (3)
O3iii—Pb1—O3v 55.44 (13) O2xiv—Co2—O3iv 174.4 (3)
O3iv—Pb1—O3v 111.4 (2) O2—Co2—O3iv 92.52 (17)
O6viii—Pb2—O6vii 83.17 (17) O3i—Co2—O3iv 87.7 (2)
O6viii—Pb2—O2ix 61.34 (16) O2xiv—Co2—O1 89.3 (2)
O6vii—Pb2—O2ix 107.91 (19) O2—Co2—O1 95.5 (2)
O6viii—Pb2—O2vi 107.91 (19) O3i—Co2—O1 78.9 (2)
O6vii—Pb2—O2vi 61.34 (16) O3iv—Co2—O1 96.2 (2)
O2ix—Pb2—O2vi 166.8 (3) O2xiv—Co2—O1xiv 95.5 (2)
O6viii—Pb2—O5x 106.77 (19) O2—Co2—O1xiv 89.3 (2)
O6vii—Pb2—O5x 68.25 (16) O3i—Co2—O1xiv 96.2 (2)
O2ix—Pb2—O5x 66.27 (12) O3iv—Co2—O1xiv 78.9 (2)
O2vi—Pb2—O5x 112.94 (13) O1—Co2—O1xiv 173.3 (3)
O6viii—Pb2—O5xi 68.25 (16) O3xv—Co3—O3 175.2 (5)
O6vii—Pb2—O5xi 106.77 (19) O3xv—Co3—O3xvi 79.5 (4)
O2ix—Pb2—O5xi 112.94 (13) O3—Co3—O3xvi 96.96 (14)
O2vi—Pb2—O5xi 66.27 (12) O3xv—Co3—O3xvii 86.8 (4)
O5x—Pb2—O5xi 173.7 (3) O3—Co3—O3xvii 96.96 (14)
O6viii—Pb2—O6vi 138.39 (2) O3xvi—Co3—O3xvii 96.96 (14)
O6vii—Pb2—O6vi 55.23 (15) O3xv—Co3—O3iii 96.96 (14)
O2ix—Pb2—O6vi 126.25 (15) O3—Co3—O3iii 79.5 (4)
O2vi—Pb2—O6vi 55.67 (17) O3xvi—Co3—O3iii 86.8 (4)
O5x—Pb2—O6vi 60.10 (16) O3xvii—Co3—O3iii 175.2 (5)
O5xi—Pb2—O6vi 120.76 (15) O3xv—Co3—O3v 96.96 (14)
O6viii—Pb2—O6ix 55.23 (15) O3—Co3—O3v 86.8 (4)
O6vii—Pb2—O6ix 138.39 (2) O3xvi—Co3—O3v 175.2 (5)
O2ix—Pb2—O6ix 55.67 (17) O3xvii—Co3—O3v 79.5 (4)
O2vi—Pb2—O6ix 126.25 (15) O3iii—Co3—O3v 96.96 (14)
O5x—Pb2—O6ix 120.76 (15) O2—Co4—O2xviii 89.8 (3)
O5xi—Pb2—O6ix 60.10 (16) O2—Co4—O1vi 96.9 (2)
O6vi—Pb2—O6ix 166.38 (13) O2xviii—Co4—O1vi 91.0 (2)
O6viii—Pb2—O3xi 120.59 (18) O2—Co4—O1xiv 91.0 (2)
O6vii—Pb2—O3xi 121.18 (18) O2xviii—Co4—O1xiv 96.9 (2)
O2ix—Pb2—O3xi 130.9 (2) O1vi—Co4—O1xiv 168.8 (4)
O2vi—Pb2—O3xi 60.21 (13) O2—Co4—O5xix 174.7 (3)
O5x—Pb2—O3xi 132.1 (2) O2xviii—Co4—O5xix 90.92 (16)
O5xi—Pb2—O3xi 53.44 (14) O1vi—Co4—O5xix 77.8 (2)
O6vi—Pb2—O3xi 86.29 (19) O1xiv—Co4—O5xix 94.2 (2)
O6ix—Pb2—O3xi 84.37 (18) O2—Co4—O5iv 90.92 (16)
O6viii—Pb2—O3x 121.18 (18) O2xviii—Co4—O5iv 174.7 (3)
O6vii—Pb2—O3x 120.59 (18) O1vi—Co4—O5iv 94.2 (2)
O2ix—Pb2—O3x 60.21 (13) O1xiv—Co4—O5iv 77.8 (2)
O2vi—Pb2—O3x 130.9 (2) O5xix—Co4—O5iv 88.9 (3)
O5x—Pb2—O3x 53.44 (14) Te2ii—O1—Co4vii 98.54 (19)
O5xi—Pb2—O3x 132.1 (2) Te2ii—O1—Co2 96.67 (17)
O6vi—Pb2—O3x 84.37 (18) Co4vii—O1—Co2 89.3 (2)
O6ix—Pb2—O3x 86.29 (19) Te2ii—O1—Pb1 116.6 (2)
O3xi—Pb2—O3x 93.32 (14) Co4vii—O1—Pb1 136.07 (18)
O2vi—Te1—O2 99.15 (18) Co2—O1—Pb1 110.4 (2)
O2vi—Te1—O2vii 99.15 (18) Te1—O2—Co4 129.1 (3)
O2—Te1—O2vii 99.15 (18) Te1—O2—Co2 130.4 (4)
O2vi—Te1—O6vi 90.7 (2) Co4—O2—Co2 89.87 (19)
O2—Te1—O6vi 85.2 (2) Te1—O2—Pb2vii 95.48 (17)
O2vii—Te1—O6vi 168.4 (2) Co4—O2—Pb2vii 96.4 (2)
O2vi—Te1—O6vii 85.2 (2) Co2—O2—Pb2vii 111.0 (2)
O2—Te1—O6vii 168.4 (2) Te2—O3—Co2xx 97.34 (17)
O2vii—Te1—O6vii 90.7 (2) Te2—O3—Co3 96.2 (2)
O6vi—Te1—O6vii 84.0 (2) Co2xx—O3—Co3 92.8 (3)
O2vi—Te1—O6 168.4 (2) Te2—O5—Co1xiii 125.5 (4)
O2—Te1—O6 90.7 (2) Te2—O5—Co4xx 97.7 (2)
O2vii—Te1—O6 85.2 (2) Co1xiii—O5—Co4xx 120.3 (3)
O6vi—Te1—O6 84.0 (2) Te2—O5—Pb2xxi 117.3 (2)
O6vii—Te1—O6 84.0 (2) Co1xiii—O5—Pb2xxi 97.82 (18)
O5—Te2—O5iii 92.5 (3) Co4xx—O5—Pb2xxi 95.2 (2)
O5—Te2—O3iii 177.8 (2) Te1—O6—Co1 86.54 (14)
O5iii—Te2—O3iii 89.6 (2) Te1—O6—Pb1 136.5 (2)
O5—Te2—O3 89.6 (2) Co1—O6—Pb1 127.8 (2)
O5iii—Te2—O3 177.8 (2) Te1—O6—Pb2vi 103.41 (16)
O3iii—Te2—O3 88.2 (2) Co1—O6—Pb2vi 100.34 (16)
O5—Te2—O1xii 93.3 (2) Pb1—O6—Pb2vi 96.12 (13)

Symmetry codes: (i) y, x, −z; (ii) y, −x+y, z−1/2; (iii) −x+y, y, −z+1/2; (iv) xy, x, z−1/2; (v) x, xy, −z+1/2; (vi) −x+y, −x+1, z; (vii) −y+1, xy+1, z; (viii) −x+1, −x+y+1, −z; (ix) y, x+1, −z; (x) x, xy+1, −z+1/2; (xi) y, −x+y+1, z−1/2; (xii) xy, x, z+1/2; (xiii) −y+1, −x+1, −z+1/2; (xiv) −x+y, y, −z−1/2; (xv) −y, −x, −z+1/2; (xvi) −y, xy, z; (xvii) −x+y, −x, z; (xviii) x, xy+1, −z−1/2; (xix) xy, −y+1, −z; (xx) y, −x+y, z+1/2; (xxi) xy+1, x, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BR2208).

References

  1. Artner, C. & Weil, M. (2012). Z. Kristallogr. Suppl. 32, 99.
  2. Brown, I. D. (2002). In The Chemical Bond in Inorganic Chemistry: The Bond Valence Model Oxford University Press.
  3. Bruker (2004). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Dowty, E. (2006). ATOMS Shape Software, Kingsport, Tennessee, USA.
  5. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  6. Herrendorf, W. (1997). HABITUS University of Giessen, Germany.
  7. Levason, W. (1997). Coord. Chem. Rev. 161, 33–79.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Wedel, B., Sugiyama, K. & Müller-Buschbaum, H. K. (1998). Z. Naturforsch. Teil B, 53, 527–531.
  10. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
  11. Wildner, M. (1992). Z. Kristallogr. 202, 51–70.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812037038/br2208sup1.cif

e-68-00i71-sup1.cif (24.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812037038/br2208Isup2.hkl

e-68-00i71-Isup2.hkl (111.4KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

RESOURCES