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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Sep 28;69(Pt 10):i71. doi: 10.1107/S1600536813026391

Tetra­yttrium difluoride disilicate orthosilicate, Y4F2[Si2O7][SiO4]

Marion C Schäfer a,b, Ingo Hartenbach b, Thomas Schleid b,*
PMCID: PMC3790338  PMID: 24098160

Abstract

In the crystal structure of Y4F2[Si2O7][SiO4], three fundamental building blocks are present, viz. anionic disilicate and orthosilicate units ([Si2O7]6− and [SiO4]4−) and cationic [F2Y4]10+ entities. The latter are built up by two [FY3]8+ triangles sharing a common edge. The four crystallographically independent Y3+ cations display coordination numbers of eight for one and of seven for the other three cations, provided by oxide and fluoride anions. The overall arrangement of the building blocks can be considered as layer-like parallel to the ac plane.

Related literature  

For isotypic Er4F2[Si2O7][SiO4], see: Müller-Bunz & Schleid (2001). For the minor by-product phase Y3F[Si3O10], see: Müller-Bunz & Schleid (1998). For the crystal structure of allanite (old name orthite), see: Rumanova & Nikoleva (1959).

Experimental  

Crystal data  

  • Y4F2[Si2O7][SiO4]

  • M r = 653.91

  • Triclinic, Inline graphic

  • a = 6.4987 (5) Å

  • b = 6.6196 (5) Å

  • c = 13.2978 (9) Å

  • α = 87.418 (4)°

  • β = 85.702 (4)°

  • γ = 60.854 (3)°

  • V = 498.19 (6) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 23.52 mm−1

  • T = 293 K

  • 0.10 × 0.06 × 0.03 mm

Data collection  

  • Nonius KappaCCD diffractometer

  • Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1995) T min = 0.104, T max = 0.463

  • 12473 measured reflections

  • 2427 independent reflections

  • 1475 reflections with I > 2σ(I)

  • R int = 0.120

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.055

  • wR(F 2) = 0.107

  • S = 0.98

  • 2427 reflections

  • 182 parameters

  • Δρmax = 1.56 e Å−3

  • Δρmin = −1.49 e Å−3

Data collection: COLLECT (Nonius, 1998); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: SCALEPACK and DENZO (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, publication_text. DOI: 10.1107/S1600536813026391/wm2768sup1.cif

e-69-00i71-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813026391/wm2768Isup2.hkl

e-69-00i71-Isup2.hkl (119.2KB, hkl)

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

Acknowledgments

This work was supported by the State of Baden-Württemberg (Stuttgart) and the Deutsche Forschungsgemeinschaft (DFG, Frankfurt/Main) within the funding program Open Access Publishing.

supplementary crystallographic information

1. Comment

Y4F2[Si2O7][SiO4] crystallizes isotypically with the already known erbium analogue Er4F2[Si2O7][SiO4] (Müller-Bunz & Schleid, 2001). The crystal structure comprises two different oxidosilicate anions, namely a pyroanionic bitetrahedral disilicate unit [Si2O7]6– with eclipsed conformation (Fig. 1, top left) and an orthosilicate tetrahedron [SiO4]4– (Fig. 1, top right), just like in the mineral allanite (old name orthite) (Rumanova & Nikoleva, 1959). Together with these two anionic building blocks, discrete cationic [F2Y4]10+ entities (Fig. 1, bottom) complete the crystal structure of Y4F2[Si2O7][SiO4]. For the formation of the latter, two almost planar [FY3]8+ triangles are fused together via one common edge, resulting in a butterfly-shaped [F2Y4]10+ unit comprising an angle between the two triangular planes of 161.65 (5)°. Two of the four crystallographically distinct Y3+ cations (Y2, Y3) display just one fluoride anion in their coordination sphere, while the other two (F1, F4) have contact with two F anions each. O2– anions complete the coordination environments of the yttrium cations resulting in distorted bi- (Y1) or monocapped (Y2-4) trigonal prisms. The cationic [F2Y4]10+ as well as the anionic [Si2O7]6– and [SiO4]4– building blocks are arranged layer-like parallel to the ac plane in the crystal structure of the title compound (Fig. 2).

2. Experimental

Colourless lath-shaped single crystals of Y4F2[Si2O7][SiO4] were obtained by the reaction of yttrium sesquioxide (Y2O3), yttrium trifluoride (YF3), and silicon dioxide (SiO2) in the molar ratio 2:5:3 and an excess of cesium chloride (CsCl) as flux in evacuated silica ampoules within nine days at 973 K and a cooling rate of 10 Kh-1. Due to the stability of the product against air and moisture, the excess flux can the removed by washing with water. Besides the title compound, single crystals of thalenite-type Y3F[Si3O10] (Müller-Bunz & Schleid, 1998) were also found in the product mixture as minor by-product.

3. Refinement

The highest and lowest electron densities are found 1.29 Å from atom F2 and and 1.28 Å from atom O8, respectively.

Figures

Fig. 1.

Fig. 1.

Disilicate ([Si2O7]6–: top left) and orthosilicate units ([SiO4]4–: top right) as well as butterfly-shaped cationic [F2Y4]10+ entities (bottom) in the crystal structure of Y4F2[Si2O7][SiO4]; displacement ellipsoids are drawn at the 80 % probability level.

Fig. 2.

Fig. 2.

View at the crystal structure of Y4F2[Si2O7][SiO4] along [100], emphasizing the layer-like arrangement as line-up of the cationic and anionic building blocks.

Crystal data

Y4F2[Si2O7][SiO4] Z = 2
Mr = 653.91 F(000) = 608
Triclinic, P1 Dx = 4.359 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 6.4987 (5) Å Cell parameters from 5136 reflections
b = 6.6196 (5) Å θ = 0.4–28.3°
c = 13.2978 (9) Å µ = 23.52 mm1
α = 87.418 (4)° T = 293 K
β = 85.702 (4)° Lath-shaped, colourless
γ = 60.854 (3)° 0.10 × 0.06 × 0.03 mm
V = 498.19 (6) Å3

Data collection

Nonius KappaCCD diffractometer 2427 independent reflections
Radiation source: fine-focus sealed tube 1475 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.120
ω and φ mscans θmax = 28.2°, θmin = 1.5°
Absorption correction: numerical (X-SHAPE; Stoe & Cie, 1995) h = −8→8
Tmin = 0.104, Tmax = 0.463 k = −8→8
12473 measured reflections l = −17→17

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.055 w = 1/[σ2(Fo2) + (0.0233P)2] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.107 (Δ/σ)max < 0.001
S = 0.98 Δρmax = 1.56 e Å3
2427 reflections Δρmin = −1.49 e Å3
182 parameters Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraints Extinction coefficient: 0.0029 (6)

Special details

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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
Y1 0.32290 (19) 0.37903 (19) 0.20317 (8) 0.0102 (3)
Y2 0.94009 (19) 0.27320 (19) 0.02756 (8) 0.0083 (3)
Y3 0.21943 (19) 0.21311 (19) 0.52890 (8) 0.0083 (3)
Y4 0.82014 (19) 0.30705 (19) 0.32901 (8) 0.0084 (3)
F1 0.0366 (11) 0.2679 (11) 0.1862 (5) 0.0118 (14)
F2 0.2019 (11) 0.2616 (11) 0.3554 (5) 0.0143 (15)
Si1 0.4925 (5) 0.2508 (5) 0.9343 (2) 0.0098 (7)
Si2 0.2335 (5) 0.1526 (5) 0.7833 (2) 0.0084 (7)
Si3 0.2675 (5) 0.7298 (5) 0.4207 (2) 0.0078 (7)
O1 0.2654 (13) 0.3396 (14) 0.0197 (6) 0.0120 (17)
O2 0.2523 (13) 0.9039 (13) 0.0181 (6) 0.0117 (17)
O3 0.5550 (14) 0.5023 (14) 0.1127 (6) 0.0145 (18)
O4 0.4646 (12) 0.0987 (13) 0.8473 (5) 0.0086 (16)
O5 0.2042 (13) 0.3248 (13) 0.6867 (5) 0.0081 (16)
O6 0.6842 (13) 0.1117 (13) 0.2472 (6) 0.0122 (17)
O7 0.0069 (13) 0.7152 (13) 0.1437 (6) 0.0116 (17)
O8 0.4064 (13) 0.8414 (13) 0.4786 (6) 0.0092 (16)
O9 0.4233 (13) 0.5444 (14) 0.3321 (6) 0.0132 (18)
O10 0.8272 (13) 0.4057 (14) 0.4931 (6) 0.0135 (18)
O11 0.0157 (13) 0.9376 (13) 0.3873 (6) 0.0089 (17)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Y1 0.0090 (5) 0.0126 (6) 0.0088 (6) −0.0050 (4) −0.0027 (4) 0.0019 (4)
Y2 0.0088 (5) 0.0079 (6) 0.0077 (6) −0.0035 (4) −0.0013 (4) −0.0008 (4)
Y3 0.0082 (5) 0.0081 (6) 0.0078 (6) −0.0032 (4) −0.0023 (4) −0.0001 (4)
Y4 0.0079 (5) 0.0088 (6) 0.0076 (6) −0.0034 (4) −0.0011 (4) −0.0008 (4)
F1 0.014 (3) 0.013 (4) 0.009 (3) −0.005 (3) −0.005 (3) −0.001 (3)
F2 0.013 (3) 0.019 (4) 0.012 (4) −0.009 (3) −0.004 (3) 0.003 (3)
Si1 0.0073 (15) 0.0095 (16) 0.0107 (16) −0.0022 (13) −0.0022 (12) −0.0016 (12)
Si2 0.0083 (15) 0.0058 (16) 0.0077 (16) −0.0005 (13) −0.0002 (12) −0.0019 (12)
Si3 0.0079 (15) 0.0083 (16) 0.0077 (16) −0.0044 (13) 0.0006 (12) 0.0002 (12)
O1 0.016 (4) 0.019 (4) 0.009 (4) −0.009 (3) 0.005 (3) −0.003 (3)
O2 0.011 (4) 0.010 (4) 0.016 (4) −0.006 (3) 0.001 (3) 0.001 (3)
O3 0.017 (4) 0.012 (4) 0.010 (4) −0.004 (3) −0.003 (3) 0.006 (3)
O4 0.009 (4) 0.013 (4) 0.011 (4) −0.006 (3) −0.005 (3) 0.003 (3)
O5 0.010 (4) 0.009 (4) 0.009 (4) −0.005 (3) 0.002 (3) −0.002 (3)
O6 0.009 (4) 0.009 (4) 0.019 (4) −0.001 (3) −0.001 (3) −0.004 (3)
O7 0.011 (4) 0.010 (4) 0.009 (4) −0.002 (3) 0.002 (3) 0.002 (3)
O8 0.009 (4) 0.010 (4) 0.012 (4) −0.006 (3) −0.004 (3) −0.002 (3)
O9 0.014 (4) 0.019 (4) 0.009 (4) −0.008 (3) 0.000 (3) −0.004 (3)
O10 0.012 (4) 0.012 (4) 0.009 (4) 0.000 (3) −0.003 (3) −0.001 (3)
O11 0.009 (4) 0.013 (4) 0.010 (4) −0.005 (3) −0.006 (3) 0.001 (3)

Geometric parameters (Å, º)

Y1—O6 2.248 (7) Y3—Si3ii 3.024 (3)
Y1—O3 2.286 (8) Y3—Si2 3.392 (3)
Y1—O7 2.330 (7) Y3—Y3i 3.406 (2)
Y1—F1 2.337 (6) Y3—Si3x 3.431 (3)
Y1—F2 2.353 (6) Y3—Y3ii 3.559 (2)
Y1—O9 2.366 (7) Y4—F1iv 2.223 (6)
Y1—O1 2.540 (8) Y4—O6 2.240 (8)
Y1—O4i 2.856 (8) Y4—O11v 2.269 (8)
Y1—Si2i 3.296 (3) Y4—O9 2.272 (8)
Y1—Si2ii 3.428 (3) Y4—O10 2.316 (8)
Y1—Y4 3.5649 (15) Y4—O5vi 2.364 (7)
Y1—Y2iii 3.7351 (15) Y4—F2iv 2.400 (6)
Y2—O2iii 2.216 (8) Y4—Si3vi 3.352 (3)
Y2—F1iv 2.239 (6) Y4—Y3vi 3.6603 (16)
Y2—O7iii 2.281 (8) Y4—Y3iv 3.6740 (14)
Y2—O2v 2.295 (7) Y4—Y1iv 3.7852 (15)
Y2—O1iii 2.322 (8) F1—Y4xi 2.223 (6)
Y2—O1iv 2.354 (7) F1—Y2xi 2.239 (6)
Y2—O3 2.424 (8) F2—Y4xi 2.400 (6)
Y2—Si1vi 3.064 (3) Si1—O3vi 1.613 (8)
Y2—Si1vii 3.316 (3) Si1—O2vi 1.626 (8)
Y2—Y2viii 3.411 (2) Si1—O4 1.644 (8)
Y2—Y2ix 3.486 (2) Si1—O1xii 1.666 (8)
Y2—Y1iii 3.7351 (15) Si2—O6i 1.622 (8)
Y3—O5 2.236 (7) Si2—O7ii 1.633 (8)
Y3—O8x 2.257 (8) Si2—O5 1.637 (8)
Y3—O8vi 2.273 (7) Si2—O4 1.657 (7)
Y3—O10xi 2.305 (7) Si3—O11 1.621 (7)
Y3—F2 2.319 (6) Si3—O9 1.632 (8)
Y3—O11ii 2.388 (8) Si3—O8 1.660 (7)
Y3—O10vi 2.398 (8) Si3—O10vi 1.684 (8)
O6—Y1—O3 78.8 (3) O6—Y4—O10 138.3 (3)
O6—Y1—O7 163.3 (3) O11v—Y4—O10 84.6 (3)
O3—Y1—O7 85.3 (3) O9—Y4—O10 90.6 (3)
O6—Y1—F1 119.2 (2) F1iv—Y4—O5vi 78.7 (2)
O3—Y1—F1 142.5 (2) O6—Y4—O5vi 136.0 (3)
O7—Y1—F1 76.9 (2) O11v—Y4—O5vi 148.0 (3)
O6—Y1—F2 83.0 (3) O9—Y4—O5vi 78.4 (3)
O3—Y1—F2 151.4 (2) O10—Y4—O5vi 75.9 (3)
O7—Y1—F2 109.4 (2) F1iv—Y4—F2iv 67.0 (2)
F1—Y1—F2 66.0 (2) O6—Y4—F2iv 135.7 (3)
O6—Y1—O9 73.5 (3) O11v—Y4—F2iv 77.8 (2)
O3—Y1—O9 79.2 (3) O9—Y4—F2iv 147.8 (3)
O7—Y1—O9 98.5 (3) O10—Y4—F2iv 70.5 (2)
F1—Y1—O9 135.6 (2) O5vi—Y4—F2iv 71.9 (2)
F2—Y1—O9 74.6 (2) Y4xi—F1—Y2xi 128.6 (3)
O6—Y1—O1 111.4 (3) Y4xi—F1—Y1 112.2 (2)
O3—Y1—O1 75.0 (3) Y2xi—F1—Y1 114.7 (3)
O7—Y1—O1 68.9 (3) Y3—F2—Y1 149.1 (3)
F1—Y1—O1 67.9 (2) Y3—F2—Y4xi 102.2 (2)
F2—Y1—O1 132.7 (2) Y1—F2—Y4xi 105.6 (2)
O9—Y1—O1 152.0 (3) O3vi—Si1—O2vi 115.4 (4)
O6—Y1—O4i 56.4 (2) O3vi—Si1—O4 109.4 (4)
O3—Y1—O4i 103.4 (3) O2vi—Si1—O4 108.6 (4)
O7—Y1—O4i 133.9 (2) O3vi—Si1—O1xii 99.6 (4)
F1—Y1—O4i 68.9 (2) O2vi—Si1—O1xii 113.6 (4)
F2—Y1—O4i 84.1 (2) O4—Si1—O1xii 110.0 (4)
O9—Y1—O4i 127.5 (2) O6i—Si2—O7ii 117.1 (4)
O1—Y1—O4i 70.1 (2) O6i—Si2—O5 114.0 (4)
O2iii—Y2—F1iv 122.9 (3) O7ii—Si2—O5 106.6 (4)
O2iii—Y2—O7iii 79.4 (3) O6i—Si2—O4 97.8 (4)
F1iv—Y2—O7iii 154.6 (3) O7ii—Si2—O4 109.3 (4)
O2iii—Y2—O2v 81.8 (3) O5—Si2—O4 111.9 (4)
F1iv—Y2—O2v 85.6 (2) O11—Si3—O9 114.6 (4)
O7iii—Y2—O2v 86.0 (3) O11—Si3—O8 109.0 (4)
O2iii—Y2—O1iii 108.9 (3) O9—Si3—O8 115.8 (4)
F1iv—Y2—O1iii 106.1 (2) O11—Si3—O10vi 99.8 (4)
O7iii—Y2—O1iii 73.6 (3) O9—Si3—O10vi 107.4 (4)
O2v—Y2—O1iii 154.3 (3) O8—Si3—O10vi 108.9 (4)
O2iii—Y2—O1iv 153.3 (3) Si1vii—O1—Y2iii 99.1 (4)
F1iv—Y2—O1iv 72.8 (2) Si1vii—O1—Y2xi 129.2 (4)
O7iii—Y2—O1iv 82.0 (3) Y2iii—O1—Y2xi 96.4 (3)
O2v—Y2—O1iv 78.1 (3) Si1vii—O1—Y1 120.2 (4)
O1iii—Y2—O1iv 83.6 (3) Y2iii—O1—Y1 100.3 (3)
O2iii—Y2—O3 78.4 (3) Y2xi—O1—Y1 103.8 (3)
F1iv—Y2—O3 78.6 (2) Si1vi—O2—Y2iii 118.5 (4)
O7iii—Y2—O3 121.1 (3) Si1vi—O2—Y2xiii 139.1 (5)
O2v—Y2—O3 142.0 (3) Y2iii—O2—Y2xiii 98.2 (3)
O1iii—Y2—O3 63.6 (3) Si1vi—O3—Y1 133.6 (5)
O1iv—Y2—O3 127.9 (3) Si1vi—O3—Y2 96.7 (4)
O5—Y3—O8x 124.4 (3) Y1—O3—Y2 128.7 (3)
O5—Y3—O8vi 84.1 (3) Si1—O4—Si2 130.4 (5)
O8x—Y3—O8vi 82.5 (3) Si1—O4—Y1i 136.4 (4)
O5—Y3—O10xi 102.1 (3) Si2—O4—Y1i 89.8 (3)
O8x—Y3—O10xi 112.7 (3) Si2—O5—Y3 121.5 (4)
O8vi—Y3—O10xi 154.3 (3) Si2—O5—Y4vi 132.8 (4)
O5—Y3—F2 155.0 (2) Y3—O5—Y4vi 105.4 (3)
O8x—Y3—F2 79.2 (3) Si2i—O6—Y4 138.9 (4)
O8vi—Y3—F2 91.6 (2) Si2i—O6—Y1 115.8 (4)
O10xi—Y3—F2 72.2 (2) Y4—O6—Y1 105.2 (3)
O5—Y3—O11ii 79.8 (3) Si2ii—O7—Y2iii 129.9 (4)
O8x—Y3—O11ii 77.4 (3) Si2ii—O7—Y1 118.8 (4)
O8vi—Y3—O11ii 140.4 (3) Y2iii—O7—Y1 108.2 (3)
O10xi—Y3—O11ii 65.2 (3) Si3—O8—Y3xiv 121.6 (4)
F2—Y3—O11ii 117.1 (2) Si3—O8—Y3vi 135.4 (4)
O5—Y3—O10vi 76.7 (3) Y3xiv—O8—Y3vi 97.5 (3)
O8x—Y3—O10vi 147.8 (3) Si3—O9—Y4 125.0 (4)
O8vi—Y3—O10vi 75.5 (3) Si3—O9—Y1 133.0 (4)
O10xi—Y3—O10vi 81.6 (3) Y4—O9—Y1 100.4 (3)
F2—Y3—O10vi 78.4 (3) Si3vi—O10—Y3iv 97.4 (3)
O11ii—Y3—O10vi 133.8 (3) Si3vi—O10—Y4 112.9 (4)
F1iv—Y4—O6 84.0 (3) Y3iv—O10—Y4 105.3 (3)
F1iv—Y4—O11v 99.0 (3) Si3vi—O10—Y3vi 136.1 (4)
O6—Y4—O11v 74.4 (3) Y3iv—O10—Y3vi 98.4 (3)
F1iv—Y4—O9 119.3 (2) Y4—O10—Y3vi 101.9 (3)
O6—Y4—O9 75.5 (3) Si3—O11—Y4xiii 145.4 (4)
O11v—Y4—O9 127.5 (3) Si3—O11—Y3ii 96.1 (4)
F1iv—Y4—O10 135.4 (2) Y4xiii—O11—Y3ii 116.6 (3)

Symmetry codes: (i) −x+1, −y, −z+1; (ii) −x, −y+1, −z+1; (iii) −x+1, −y+1, −z; (iv) x+1, y, z; (v) x+1, y−1, z; (vi) −x+1, −y+1, −z+1; (vii) x, y, z−1; (viii) −x+2, −y, −z; (ix) −x+2, −y+1, −z; (x) x, y−1, z; (xi) x−1, y, z; (xii) x, y, z+1; (xiii) x−1, y+1, z; (xiv) x, y+1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2768).

References

  1. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  2. Müller-Bunz, H. & Schleid, Th. (1998). Z. Anorg. Allg. Chem. 624, 1082–1084.
  3. Müller-Bunz, H. & Schleid, Th. (2001). Z. Anorg. Allg. Chem. 627, 218–223.
  4. Nonius (1998). COLLECT Nonius BV, Delft, The Netherlands.
  5. Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.
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  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Stoe & Cie (1995). X-SHAPE Stoe & Cie, Darmstadt, Germany.

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, publication_text. DOI: 10.1107/S1600536813026391/wm2768sup1.cif

e-69-00i71-sup1.cif (18.7KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813026391/wm2768Isup2.hkl

e-69-00i71-Isup2.hkl (119.2KB, 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

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