Skip to main content
Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Sep 20;67(Pt 10):i56. doi: 10.1107/S1600536811037263

A new langbeinite-type phosphate: K2AlSn(PO4)3

Hai-Yan Li a,*, Dan Zhao a
PMCID: PMC3201338  PMID: 22058680

Abstract

Single crystals of the title compound, dipotassium aluminium tin(IV) tris­[phosphate(V)], K2AlSn(PO4)3, were synthesized by a high temperature reaction in a platinum crucible. In the structure, the AlIII and SnIV atoms occupy the same site on a threefold rotation axis with occupational disorder in a 1:1 ratio. In the three-dimensional structure, Al/SnO6 octa­hedra and PO4 tetra­hedra are inter­connected via their vertices, yielding a [Al/SnP3O12]n framework. The K atoms (site symmetry 3) reside in the large cavities delimited by the [Al/SnP3O12]n framework, and are surrounded by 12 O atoms.

Related literature

For the mineral langbeinite, K2Mg2(SO4)3, see: Zemann & Zemann (1957). For related langbeinite-type compounds, see: Aatiq et al. (2006); Norberg (2002); Ogorodnyk et al. (2006); Orlova et al. (2003); Zatovsky et al. (2007); Zhao et al. (2009).

Experimental

Crystal data

  • K2AlSn(PO4)3

  • M r = 508.78

  • Cubic, Inline graphic

  • a = 9.7980 (8) Å

  • V = 940.62 (13) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 4.28 mm−1

  • T = 296 K

  • 0.15 × 0.05 × 0.05 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.566, T max = 0.815

  • 6146 measured reflections

  • 811 independent reflections

  • 782 reflections with I > 2σ(I)

  • R int = 0.065

Refinement

  • R[F 2 > 2σ(F 2)] = 0.029

  • wR(F 2) = 0.074

  • S = 1.18

  • 811 reflections

  • 59 parameters

  • Δρmax = 0.53 e Å−3

  • Δρmin = −0.60 e Å−3

  • Absolute structure: Flack (1983), 340 Friedel pairs

  • Flack parameter: −0.05 (7)

Data collection: APEX2 (Bruker, 2008); cell refinement: SAINT (Bruker, 2008); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811037263/fi2112sup1.cif

e-67-00i56-sup1.cif (24.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811037263/fi2112Isup2.hkl

e-67-00i56-Isup2.hkl (40.5KB, hkl)

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

Acknowledgments

The authors acknowledge the Doctoral Foundation of Henan Polytechnic University (grant No. B2010–92, 648483).

supplementary crystallographic information

Comment

Langbeinite-type (K2Mg2(SO4)3, Zemann & Zemann, 1957) compounds with the simplest generic formula A2B2(XO4)3 are an important and well studied family of inorganic solids with respect to minerals. Among Langbeinite-based phosphates, whose coordination networks are based on [M2(PO4)3] fragments, may result in diverse structure types due to the 'M2' sites occupied by various types of tetravalent and bi- or trivalent metal pairs. For example, the structures K2MTi(PO4)3(M = Y, Yb, Er) (Norberg, 2002), K2FeZr(PO4)3 (Orlova et al., 2003), K2MSn(PO4)3 (M = Fe, Yb) (Aatiq et al., 2006), K2AlTi(PO4)3 (Zhao et al., 2009), K2FeSn(PO4)3 (Zatovsky et al., 2007) and K2Mn0.5Ti1.5(PO4)3 (Ogorodnyk et al., 2006), have been reported. Herein we report the single-crystal growth and structure investigation of title compound K2AlSn(PO4)3.

In the structure of title compound, K, Al and Sn atoms lie on the 3-fold rotation axes in 4a positions, while P and O atoms are located at general 12b positions. Due to the similar ionic radii of Al and Sn atoms, they occupy the same sites in a substituent disordered manner, denoted as M atoms. The three-dimensional structure contains MO6 octahedra and PO4 tetrahedra which are connected via vertices. Two nearest [MO6] octahedra are joined to each other by three bridging orthophosphate tetrahedra forming [Al/SnP3O12]n framework, which penetrate with large closed cavities. Two independent potassium atoms are located in each cavity. K1 and K2 atoms are 12-coordinated by O atoms.

Experimental

Single crystals of K2AlSn(PO4)3 have been prepared by a high-temperature method in air. A powder mixture of K2CO3, Al2O3, SnO2 and NH4H2PO4 in the molar ratio of K: Al: Sn: P = 10: 1:: 1 15 was first ground in an agate mortar and then transferred to a platinum crucible. The sample was gradually heated in air at 1173 K for 24 h. After that, the intermediate product was slowly cooled to 673 K at the rate of 2 K h-1. It was kept at 673 K for another 10 h and then quenched to room temperature. The obtained crystals were colorless with a prismatic shape.

Refinement

The atomic position and anisotropic displacement parameters of Al and Sn in the same sites were constrained to be identical, and the Al/Sn disorder with a relative occupancy of 1/1. The highest peak in the difference electron density map equals to 0.53 e/Å3 at the distance of 1.09 Å from Al2/Sn2 site while the deepest hole equals to -0.60 e/Å3 at the distance of 1.78 Å from K2 site.

Figures

Fig. 1.

Fig. 1.

A view of the asymmetric unit of K2AlSn(PO4)3 showing the coordination environments of the P and Al/Sn atoms.. Displacement ellipsoids are drawn at the 50% probability level. [Symmetry codes: (i) -x + 1, y + 1/2, -z + 1/2; (ii) z, x, y; (iii) -y + 1/2, -z + 1, x - 1/2; (iv) -z + 1/2, -x + 1, y - 1/2; (v) -y + 1, z + 1/2, -x + 1/2; (viii) y, z, x; (ix) -z, x - 1/2, -y + 1/2; (x) -y + 1/2, -z, x - 1/2; (xi) x - 1/2, -y + 1/2, -z.]

Fig. 2.

Fig. 2.

View of the crystal structure of K2AlSn(PO4)3 along [010]. PO4 and Al/SnO6 units are given in the polyhedral representation.

Crystal data

K2AlSn(PO4)3 Dx = 3.593 Mg m3
Mr = 508.78 Mo Kα radiation, λ = 0.71073 Å
Cubic, P213 Cell parameters from 2030 reflections
Hall symbol: P 2ac 2ab 3 θ = 3.6–28.5°
a = 9.7980 (8) Å µ = 4.28 mm1
V = 940.62 (13) Å3 T = 296 K
Z = 4 Prism, colourless
F(000) = 968 0.15 × 0.05 × 0.05 mm

Data collection

Bruker SMART APEXII CCD area-detector diffractometer 811 independent reflections
Radiation source: fine-focus sealed tube 782 reflections with I > 2σ(I)
graphite Rint = 0.065
Detector resolution: 83.33 pixels mm-1 θmax = 28.5°, θmin = 2.9°
ω scans h = −13→6
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) k = −12→12
Tmin = 0.566, Tmax = 0.815 l = −12→10
6146 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full w = 1/[σ2(Fo2) + (0.0208P)2 + 3.2535P] where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.029 (Δ/σ)max < 0.001
wR(F2) = 0.074 Δρmax = 0.53 e Å3
S = 1.18 Δρmin = −0.60 e Å3
811 reflections Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
59 parameters Extinction coefficient: 0.0076 (10)
0 restraints Absolute structure: Flack (1983), 340 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: −0.05 (7)

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 Occ. (<1)
Sn1 0.39682 (6) 0.60318 (6) 0.10318 (6) 0.0091 (2) 0.50
Sn2 0.16412 (6) 0.16412 (6) 0.16412 (6) 0.0104 (2) 0.50
Al1 0.39682 (6) 0.60318 (6) 0.10318 (6) 0.0091 (2) 0.50
Al2 0.16412 (6) 0.16412 (6) 0.16412 (6) 0.0104 (2) 0.50
P1 0.47928 (15) 0.29006 (15) 0.12495 (15) 0.0133 (3)
K1 0.18221 (14) 0.81779 (14) 0.31779 (14) 0.0268 (5)
K2 0.54175 (17) −0.04175 (17) 0.04175 (17) 0.0305 (6)
O1 0.3329 (4) 0.2484 (4) 0.1004 (5) 0.0231 (9)
O2 0.4861 (4) 0.4378 (4) 0.1734 (5) 0.0198 (9)
O3 0.5491 (5) 0.1991 (4) 0.2297 (4) 0.0214 (9)
O4 0.5569 (5) 0.2684 (5) −0.0094 (5) 0.0276 (11)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.0091 (2) 0.0091 (2) 0.0091 (2) 0.0000 (2) 0.0000 (2) 0.0000 (2)
Sn2 0.0104 (2) 0.0104 (2) 0.0104 (2) −0.0010 (2) −0.0010 (2) −0.0010 (2)
Al1 0.0091 (2) 0.0091 (2) 0.0091 (2) 0.0000 (2) 0.0000 (2) 0.0000 (2)
Al2 0.0104 (2) 0.0104 (2) 0.0104 (2) −0.0010 (2) −0.0010 (2) −0.0010 (2)
P1 0.0142 (7) 0.0131 (7) 0.0126 (7) 0.0002 (5) −0.0001 (5) 0.0010 (5)
K1 0.0268 (5) 0.0268 (5) 0.0268 (5) 0.0031 (6) 0.0031 (6) −0.0031 (6)
K2 0.0305 (6) 0.0305 (6) 0.0305 (6) 0.0013 (6) −0.0013 (6) 0.0013 (6)
O1 0.016 (2) 0.024 (2) 0.030 (2) −0.0048 (18) −0.006 (2) 0.0024 (19)
O2 0.021 (2) 0.014 (2) 0.025 (2) −0.0009 (16) −0.0065 (19) −0.0067 (17)
O3 0.025 (2) 0.021 (2) 0.018 (2) −0.0001 (18) −0.0077 (18) 0.0088 (18)
O4 0.038 (3) 0.028 (3) 0.017 (2) 0.007 (2) 0.011 (2) 0.003 (2)

Geometric parameters (Å, °)

Sn1—O3i 1.961 (4) K1—O4xii 3.011 (6)
Sn1—O3ii 1.961 (4) K1—O4xi 3.011 (6)
Sn1—O3iii 1.961 (4) K1—O4ii 3.208 (5)
Sn1—O2iv 1.966 (4) K1—O4i 3.208 (5)
Sn1—O2v 1.966 (4) K1—O4iii 3.208 (5)
Sn1—O2 1.966 (4) K2—O2xiii 2.811 (5)
Sn2—O1 1.951 (4) K2—O2xiv 2.811 (5)
Sn2—O1ii 1.951 (4) K2—O2xv 2.811 (5)
Sn2—O1vi 1.951 (4) K2—O3ix 2.994 (5)
Sn2—O4vii 1.960 (5) K2—O3xvi 2.994 (5)
Sn2—O4viii 1.960 (5) K2—O3 2.994 (5)
Sn2—O4ix 1.960 (5) K2—O4xvi 3.084 (5)
P1—O1 1.511 (4) K2—O4ix 3.084 (5)
P1—O2 1.525 (4) K2—O4 3.084 (5)
P1—O3 1.521 (4) O1—K1xvii 2.847 (5)
P1—O4 1.535 (5) O2—K2xviii 2.811 (5)
K1—O1x 2.847 (5) O3—Al1vi 1.961 (4)
K1—O1xi 2.847 (5) O3—Sn1vi 1.961 (4)
K1—O1xii 2.847 (5) O3—K1vi 2.915 (5)
K1—O3ii 2.916 (5) O4—Al2xvi 1.960 (5)
K1—O3iii 2.916 (5) O4—Sn2xvi 1.960 (5)
K1—O3i 2.916 (5) O4—K1xvii 3.011 (6)
K1—O4x 3.011 (6) O4—K1vi 3.208 (5)
O3i—Sn1—O3ii 87.42 (19) O4x—K1—O4xii 86.48 (14)
O3i—Sn1—O3iii 87.42 (19) O1x—K1—O4xi 52.14 (13)
O3ii—Sn1—O3iii 87.42 (19) O1xi—K1—O4xi 49.38 (13)
O3i—Sn1—O2iv 175.0 (2) O1xii—K1—O4xi 114.88 (15)
O3ii—Sn1—O2iv 89.00 (17) O3ii—K1—O4xi 132.86 (13)
O3iii—Sn1—O2iv 88.90 (18) O3iii—K1—O4xi 95.45 (12)
O3i—Sn1—O2v 88.90 (19) O3i—K1—O4xi 140.66 (13)
O3ii—Sn1—O2v 175.0 (2) O4x—K1—O4xi 86.48 (14)
O3iii—Sn1—O2v 89.00 (17) O4xii—K1—O4xi 86.48 (14)
O2iv—Sn1—O2v 94.46 (18) O1x—K1—O4ii 156.33 (13)
O3i—Sn1—O2 88.99 (17) O1xi—K1—O4ii 55.82 (12)
O3ii—Sn1—O2 88.90 (18) O1xii—K1—O4ii 86.26 (12)
O3iii—Sn1—O2 175.0 (2) O3ii—K1—O4ii 46.65 (11)
O2iv—Sn1—O2 94.46 (18) O3iii—K1—O4ii 88.29 (13)
O2v—Sn1—O2 94.45 (18) O3i—K1—O4ii 100.74 (13)
O3i—Sn1—K1 52.93 (13) O4x—K1—O4ii 136.85 (10)
O3ii—Sn1—K1 52.93 (13) O4xii—K1—O4ii 53.57 (17)
O3iii—Sn1—K1 52.93 (13) O4xi—K1—O4ii 104.39 (2)
O2iv—Sn1—K1 122.05 (13) O1x—K1—O4i 86.26 (12)
O2v—Sn1—K1 122.05 (13) O1xi—K1—O4i 156.33 (13)
O2—Sn1—K1 122.05 (13) O1xii—K1—O4i 55.82 (12)
O3i—Sn1—K2ii 129.38 (14) O3ii—K1—O4i 88.29 (13)
O3ii—Sn1—K2ii 51.14 (14) O3iii—K1—O4i 100.74 (13)
O3iii—Sn1—K2ii 66.00 (13) O3i—K1—O4i 46.65 (11)
O2iv—Sn1—K2ii 45.73 (13) O4x—K1—O4i 53.57 (17)
O2v—Sn1—K2ii 130.02 (13) O4xii—K1—O4i 104.39 (3)
O2—Sn1—K2ii 114.01 (13) O4xi—K1—O4i 136.85 (10)
K1—Sn1—K2ii 77.229 (18) O4ii—K1—O4i 115.74 (6)
O3i—Sn1—K2xix 66.00 (13) O1x—K1—O4iii 55.82 (12)
O3ii—Sn1—K2xix 129.38 (14) O1xi—K1—O4iii 86.26 (12)
O3iii—Sn1—K2xix 51.14 (14) O1xii—K1—O4iii 156.33 (13)
O2iv—Sn1—K2xix 114.01 (13) O3ii—K1—O4iii 100.74 (13)
O2v—Sn1—K2xix 45.73 (13) O3iii—K1—O4iii 46.65 (11)
O2—Sn1—K2xix 130.02 (13) O3i—K1—O4iii 88.29 (13)
K1—Sn1—K2xix 77.229 (18) O4x—K1—O4iii 104.39 (2)
K2ii—Sn1—K2xix 115.259 (13) O4xii—K1—O4iii 136.85 (10)
O3i—Sn1—K2xviii 51.14 (14) O4xi—K1—O4iii 53.57 (17)
O3ii—Sn1—K2xviii 66.00 (13) O4ii—K1—O4iii 115.74 (6)
O3iii—Sn1—K2xviii 129.38 (14) O4i—K1—O4iii 115.74 (6)
O2iv—Sn1—K2xviii 130.02 (13) O2xiii—K2—O2xiv 91.85 (14)
O2v—Sn1—K2xviii 114.01 (13) O2xiii—K2—O2xv 91.85 (14)
O2—Sn1—K2xviii 45.73 (13) O2xiv—K2—O2xv 91.85 (14)
K1—Sn1—K2xviii 77.229 (18) O2xiii—K2—O3ix 147.18 (15)
K2ii—Sn1—K2xviii 115.259 (13) O2xiv—K2—O3ix 56.50 (11)
K2xix—Sn1—K2xviii 115.259 (13) O2xv—K2—O3ix 81.71 (12)
O1—Sn2—O1ii 92.8 (2) O2xiii—K2—O3xvi 56.50 (11)
O1—Sn2—O1vi 92.8 (2) O2xiv—K2—O3xvi 81.71 (12)
O1ii—Sn2—O1vi 92.8 (2) O2xv—K2—O3xvi 147.18 (15)
O1—Sn2—O4vii 93.7 (2) O3ix—K2—O3xvi 119.27 (3)
O1ii—Sn2—O4vii 82.5 (2) O2xiii—K2—O3 81.71 (12)
O1vi—Sn2—O4vii 172.2 (2) O2xiv—K2—O3 147.18 (15)
O1—Sn2—O4viii 172.2 (2) O2xv—K2—O3 56.50 (11)
O1ii—Sn2—O4viii 93.7 (2) O3ix—K2—O3 119.27 (3)
O1vi—Sn2—O4viii 82.5 (2) O3xvi—K2—O3 119.27 (3)
O4vii—Sn2—O4viii 91.5 (2) O2xiii—K2—O4xvi 103.66 (12)
O1—Sn2—O4ix 82.5 (2) O2xiv—K2—O4xvi 82.44 (13)
O1ii—Sn2—O4ix 172.2 (2) O2xv—K2—O4xvi 163.58 (13)
O1vi—Sn2—O4ix 93.7 (2) O3ix—K2—O4xvi 82.31 (13)
O4vii—Sn2—O4ix 91.5 (2) O3xvi—K2—O4xvi 47.30 (12)
O4viii—Sn2—O4ix 91.5 (2) O3—K2—O4xvi 130.38 (15)
O1—Sn2—K1xx 128.15 (13) O2xiii—K2—O4ix 163.58 (13)
O1ii—Sn2—K1xx 49.01 (14) O2xiv—K2—O4ix 103.66 (12)
O1vi—Sn2—K1xx 118.40 (13) O2xv—K2—O4ix 82.44 (13)
O4vii—Sn2—K1xx 53.89 (16) O3ix—K2—O4ix 47.30 (12)
O4viii—Sn2—K1xx 59.65 (16) O3xvi—K2—O4ix 130.38 (15)
O4ix—Sn2—K1xx 130.31 (15) O3—K2—O4ix 82.31 (13)
O1—Sn2—K1xxi 118.40 (13) O4xvi—K2—O4ix 83.98 (16)
O1ii—Sn2—K1xxi 128.15 (13) O2xiii—K2—O4 82.44 (13)
O1vi—Sn2—K1xxi 49.01 (14) O2xiv—K2—O4 163.58 (13)
O4vii—Sn2—K1xxi 130.31 (15) O2xv—K2—O4 103.66 (12)
O4viii—Sn2—K1xxi 53.89 (16) O3ix—K2—O4 130.38 (15)
O4ix—Sn2—K1xxi 59.65 (16) O3xvi—K2—O4 82.31 (13)
K1xx—Sn2—K1xxi 113.210 (15) O3—K2—O4 47.30 (12)
O1—Sn2—K1xvii 49.01 (14) O4xvi—K2—O4 83.98 (16)
O1ii—Sn2—K1xvii 118.40 (13) O4ix—K2—O4 83.98 (16)
O1vi—Sn2—K1xvii 128.15 (13) O2xiii—K2—P1 93.94 (9)
O4vii—Sn2—K1xvii 59.65 (16) O2xiv—K2—P1 169.50 (10)
O4viii—Sn2—K1xvii 130.31 (15) O2xv—K2—P1 79.23 (9)
O4ix—Sn2—K1xvii 53.89 (16) O3ix—K2—P1 116.07 (10)
K1xx—Sn2—K1xvii 113.210 (15) O3xvi—K2—P1 108.78 (10)
K1xxi—Sn2—K1xvii 113.210 (15) O3—K2—P1 26.50 (8)
O1—P1—O2 110.3 (3) O4xvi—K2—P1 104.63 (13)
O1—P1—O3 112.1 (3) O4ix—K2—P1 69.91 (10)
O2—P1—O3 109.1 (3) O4—K2—P1 26.76 (9)
O1—P1—O4 107.2 (3) O2xiii—K2—P1ix 169.50 (10)
O2—P1—O4 112.1 (3) O2xiv—K2—P1ix 79.23 (9)
O3—P1—O4 105.9 (3) O2xv—K2—P1ix 93.94 (9)
O1—P1—K1vi 168.93 (19) O3ix—K2—P1ix 26.50 (8)
O2—P1—K1vi 80.16 (17) O3xvi—K2—P1ix 116.07 (10)
O3—P1—K1vi 59.55 (18) O3—K2—P1ix 108.78 (10)
O4—P1—K1vi 70.5 (2) O4xvi—K2—P1ix 69.91 (10)
O1—P1—K2 82.78 (18) O4ix—K2—P1ix 26.76 (9)
O2—P1—K2 166.53 (19) O4—K2—P1ix 104.63 (13)
O3—P1—K2 61.42 (18) P1—K2—P1ix 95.73 (6)
O4—P1—K2 64.79 (19) O2xiii—K2—P1xvi 79.23 (9)
K1vi—P1—K2 86.56 (5) O2xiv—K2—P1xvi 93.94 (9)
O1—P1—K1xvii 50.43 (19) O2xv—K2—P1xvi 169.50 (10)
O2—P1—K1xvii 124.36 (19) O3ix—K2—P1xvi 108.78 (10)
O3—P1—K1xvii 126.57 (19) O3xvi—K2—P1xvi 26.50 (8)
O4—P1—K1xvii 56.9 (2) O3—K2—P1xvi 116.07 (10)
K1vi—P1—K1xvii 126.95 (5) O4xvi—K2—P1xvi 26.76 (9)
K2—P1—K1xvii 66.07 (6) O4ix—K2—P1xvi 104.63 (13)
O1—P1—K2xviii 102.1 (2) O4—K2—P1xvi 69.91 (10)
O2—P1—K2xviii 45.40 (18) P1—K2—P1xvi 95.73 (6)
O3—P1—K2xviii 71.80 (18) P1ix—K2—P1xvi 95.73 (6)
O4—P1—K2xviii 148.7 (2) P1—O1—Sn2 150.2 (3)
K1vi—P1—K2xviii 82.58 (4) P1—O1—K1xvii 105.4 (2)
K2—P1—K2xviii 130.74 (6) Sn2—O1—K1xvii 99.85 (17)
K1xvii—P1—K2xviii 149.53 (5) P1—O2—Sn1 130.9 (3)
O1x—K1—O1xi 100.53 (12) P1—O2—K2xviii 111.9 (2)
O1x—K1—O1xii 100.53 (12) Sn1—O2—K2xviii 104.22 (16)
O1xi—K1—O1xii 100.53 (12) P1—O3—Al1vi 164.9 (3)
O1x—K1—O3ii 149.59 (14) P1—O3—Sn1vi 164.9 (3)
O1xi—K1—O3ii 96.38 (13) Al1vi—O3—Sn1vi 0.00 (5)
O1xii—K1—O3ii 100.99 (13) P1—O3—K1vi 93.7 (2)
O1x—K1—O3iii 96.38 (13) Al1vi—O3—K1vi 94.60 (17)
O1xi—K1—O3iii 100.99 (13) Sn1vi—O3—K1vi 94.60 (17)
O1xii—K1—O3iii 149.59 (14) P1—O3—K2 92.1 (2)
O3ii—K1—O3iii 55.40 (14) Al1vi—O3—K2 98.18 (17)
O1x—K1—O3i 100.99 (13) Sn1vi—O3—K2 98.18 (17)
O1xi—K1—O3i 149.59 (14) K1vi—O3—K2 103.77 (14)
O1xii—K1—O3i 96.38 (13) P1—O4—Al2xvi 152.0 (3)
O3ii—K1—O3i 55.40 (14) P1—O4—Sn2xvi 152.0 (3)
O3iii—K1—O3i 55.40 (14) Al2xvi—O4—Sn2xvi 0.000 (18)
O1x—K1—O4x 49.38 (13) P1—O4—K1xvii 97.8 (2)
O1xi—K1—O4x 114.88 (15) Al2xvi—O4—K1xvii 94.39 (18)
O1xii—K1—O4x 52.14 (13) Sn2xvi—O4—K1xvii 94.39 (18)
O3ii—K1—O4x 140.66 (13) P1—O4—K2 88.5 (2)
O3iii—K1—O4x 132.86 (13) Al2xvi—O4—K2 118.9 (2)
O3i—K1—O4x 95.45 (12) Sn2xvi—O4—K2 118.9 (2)
O1x—K1—O4xii 114.88 (15) K1xvii—O4—K2 77.14 (14)
O1xi—K1—O4xii 52.14 (13) P1—O4—K1vi 82.7 (2)
O1xii—K1—O4xii 49.38 (13) Al2xvi—O4—K1vi 88.54 (19)
O3ii—K1—O4xii 95.45 (12) Sn2xvi—O4—K1vi 88.54 (19)
O3iii—K1—O4xii 140.66 (13) K1xvii—O4—K1vi 172.37 (18)
O3i—K1—O4xii 132.86 (12) K2—O4—K1vi 95.27 (14)

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FI2112).

References

  1. Aatiq, A., Haggouch, B., Bakri, R., Lakhdar, Y. & Saadoune, I. (2006). Powder Diffr. 21, 214–219.
  2. Bruker (2008). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Flack, H. D. (1983). Acta Cryst. A39, 876–881.
  4. Norberg, S. T. (2002). Acta Cryst. B58, 743–749. [DOI] [PMC free article] [PubMed]
  5. Ogorodnyk, I. V., Zatovsky, I. V., Slobodyanik, N. S., Baumer, V. N. & Shishkin, O. V. (2006). J. Solid State Chem. 179, 3461–3466.
  6. Orlova, A. I., Trubach, I. G., Kurazhkovskaya, V. S., Pertierra, P., Salvado, M. A., Garcia-Granda, S., Khainakov, S. A. & Garcia, J. R. (2003). J. Solid State Chem. 173, 314–318.
  7. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Zatovsky, I. V., Yatskin, M. M., Baumer, V. N., Slobodyanik, N. S. & Shishkin, O. V. (2007). Acta Cryst. E63, i199.
  10. Zemann, A. & Zemann, J. (1957). Acta Cryst. 10, 409–413.
  11. Zhao, D., Zhang, H., Huang, S. P., Zhang, W. L., Yang, S. L. & Cheng, W. D. (2009). J. Alloys Compd, 477, 795–799.

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/S1600536811037263/fi2112sup1.cif

e-67-00i56-sup1.cif (24.8KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811037263/fi2112Isup2.hkl

e-67-00i56-Isup2.hkl (40.5KB, 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