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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 11;67(Pt 7):m903–m904. doi: 10.1107/S1600536811021544

Substitutional disorder in bis­[(cyanato-κO)/hydroxido(0.5/0.5)](5,10,15,20-tetra­phenyl­porphyrinato-κ4 N)tin(IV)

Imen Ben Moussa a, Mohamed Salah Belkhiria a, Shabir Najmudin b, Cecilia Bonifacio c, Habib Nasri a,*
PMCID: PMC3152010  PMID: 21836891

Abstract

The title complex, [SnIV(C44H28N4)(CNO)(OH)], exhibits substitutional disorder of the OH and OCN axial ligands. Thus, the cyanato-O ligand and the hydroxyl group bonded to the central SnIV atom share statistically the axial position. The SnIV ion is hexa­coordinated by the four N atoms of the pyrrole rings of the tetra­phenyl­porphyrin (TPP) and the O atoms of the two disordered OCN and OH axial ligands. The equatorial tin–pyrrole N atom distance (Sn—Np) is 2.100 (2) Å and the axial Sn—O(OCN) or Sn—O(OH) bond length is 2.074 (2) Å.

Related literature

For a review of porphyrin complexes, see: Scheidt (2000). For the synthesis of tin(IV) porphyrin species, see: Fallon et al. (2002); Martelli et al. (2009). For comparative bond lengths, see: Allen et al. (1987); Smith et al. (1991). For a description of the Cambridge Structural Database, see: Allen (2002).graphic file with name e-67-0m903-scheme1.jpg

Experimental

Crystal data

  • [Sn(C44H28N4)(CNO)(OH)]

  • M r = 790.42

  • Monoclinic, Inline graphic

  • a = 11.2943 (6) Å

  • b = 12.6972 (7) Å

  • c = 13.0711 (7) Å

  • β = 114.251 (2)°

  • V = 1709.06 (16) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.80 mm−1

  • T = 293 K

  • 0.20 × 0.18 × 0.12 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2007) T min = 0.870, T max = 0.954

  • 27811 measured reflections

  • 5968 independent reflections

  • 5241 reflections with I > 2σ(I)

  • R int = 0.028

Refinement

  • R[F 2 > 2σ(F 2)] = 0.039

  • wR(F 2) = 0.097

  • S = 1.13

  • 5968 reflections

  • 250 parameters

  • H-atom parameters constrained

  • Δρmax = 0.73 e Å−3

  • Δρmin = −1.34 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SIR2004 (Burla et al., 2005); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEPIII (Burnett & Johnson, 1996) and ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: publCIF (Westrip 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811021544/dn2696sup1.cif

e-67-0m903-sup1.cif (19.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021544/dn2696Isup2.hkl

e-67-0m903-Isup2.hkl (286.3KB, hkl)

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

Acknowledgments

We are grateful to the Fundacão para a Ciência e Tecnologia (FCT, Portugal) for support through projects SFRH/BPD/24889/2005 and PTDC/BIA-PRO/103980/2008 and for funding the purchase of the single-crystal diffractometer. We thank Paula Brandão from the Universidade de Aveiro for the crystal mounting and data collection.

supplementary crystallographic information

Comment

The search in the Cambridge Crystallographic Database (version 5.32 with addenda up to November 26, 2010; Allen, 2002) shows that the majority of the reported X-ray molecular structures of porphyrin tin(IV) complexes are hexa-coordinated type [SnIV(Porph)(X)2] for which X is an anionic unidentate ligand bonded to the tin(IV) ion through the oxygen atom. To the best of our knowledge, there is no X-ray molecular structure of a tin(IV) cyanato-O porphyrin species reported in the literature.

The bis{(cyanato-O)/(hydroxo)(0.5/0.5) }(5,10,15,20-tetraphenylporphyrin)tin(IV) complex [SnIV(C44H28N4)(OCN)(OH)] exhibits substitutional disorder of both thiocyanato-O and hydroxo ligands with equal occupancy factor of 0.5. The tin atom which is octahedrally coordinated lies on an inversion center (Fig. 1).

The equatorial tin–pyrrole N atom distance (Sn—Np) is 2.100 (2) Å which is normal for tin(IV) porphyrin species. The Sn—O(OH) distance is 2.088 (6) Å which is longer than the one of the related species [SnIV(TPP)(OH)2] (2.023 (4) Å) (Smith et al., 1991). The Sn—O(OCN) bond lengh value is 2.059 (8) Å which is close to those of related porphyrin species, i.e, for [SnIV(TTP)(OC6H5)2] (TTP is the meso-tetrakis(p-tolyl)porphyrin) (Fallon et al., 2002) the Sn—O(OPh) distance is 2.055 (2) Å.

There are no intermolecular or intramolecular hydrogen bonds in the structure of (I). The packing diagram for (I) (Fig.2) is simple; there is no evidence for intermolecular π -π bonding between the faces of the porphyrin cores in compound (I). The absence of the π-π interactions results mainly in the steric restrictions requirements of the phenyl groups that determine the packing environment.

Experimental

The reaction of the [SnIV(TPP)(OH)2] complex (30 mg, 0.037 mmol) (Martelli et al., 2009) with an excess of sodium cyanate, NaOCN (85 mg, 1.31 mmol) and 18-crown-6 (90 mg, 0.34 mmol) in dichloromethane (4 ml) give a pink-violet solution. Crystals of the title complex were obtained by diffusion of ether through the dichloromethane solution.

Refinement

The position of the O atoms of the NCO and OH couldn't be separated and were located on the same site using the EXYZ and EADP commands within SHELXL-97 (Sheldrick, 2008).

Hydrogen atoms were placed using assumed geometrically idealized positions (C—H aromatic = 0.95 Å) and constrained to ride on their parent atoms, with U(H) = 1.2Ueq(C). The H atom pertaining to the hydroxo ligand could not be found in a difference Fourier but was introduced in idealized position and treated as riding with U(H) = 1.5Ueq(O)

Figures

Fig. 1.

Fig. 1.

A view of the structure of the complex [SnIV(C44H28N4)(OCN)(OH)] showing the atom numbering scheme. Displacement ellipsoids are drawn at 30%. The O atoms of the hydroxo axial ligands and the H atoms have been omitted for clarity. [Symmetry code: (i) -x + 1,-y, -z + 1]

Fig. 2.

Fig. 2.

A unit cell packing of the title complex viewed down the b axis. H atoms have been omitted for clarity.

Crystal data

[Sn(C44H28N4)(CNO)(OH)] F(000) = 800
Mr = 790.42 Dx = 1.536 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 27811 reflections
a = 11.2943 (6) Å θ = 2.6–32.2°
b = 12.6972 (7) Å µ = 0.80 mm1
c = 13.0711 (7) Å T = 293 K
β = 114.251 (2)° Prism, purple
V = 1709.06 (16) Å3 0.20 × 0.18 × 0.12 mm
Z = 2

Data collection

Bruker APEXII CCD area-detector diffractometer 5968 independent reflections
Radiation source: fine-focus sealed tube 5241 reflections with I > 2σ(I)
graphite Rint = 0.028
φ and ω scans θmax = 32.2°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Bruker, 2007) h = −16→15
Tmin = 0.870, Tmax = 0.954 k = 0→18
27811 measured reflections l = 0→19

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)] = 0.039 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.097 H-atom parameters constrained
S = 1.13 w = 1/[σ2(Fo2) + (0.0357P)2 + 1.5751P] where P = (Fo2 + 2Fc2)/3
5968 reflections (Δ/σ)max < 0.001
250 parameters Δρmax = 0.73 e Å3
0 restraints Δρmin = −1.34 e Å3

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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ 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 0.5000 0.0000 0.5000 0.02969 (7)
N2 0.50052 (16) 0.15106 (14) 0.43522 (13) 0.0276 (3)
N1 0.63300 (16) 0.04991 (14) 0.65913 (13) 0.0269 (3)
O1 0.65060 (16) −0.03859 (15) 0.45502 (15) 0.0389 (4) 0.50
N3 0.8546 (4) 0.0655 (5) 0.5244 (4) 0.0513 (12) 0.50
C23 0.7509 (6) 0.0155 (5) 0.4921 (5) 0.0479 (13) 0.50
O2 0.65060 (16) −0.03859 (15) 0.45502 (15) 0.0389 (4) 0.50
H2A 0.6917 −0.0883 0.4933 0.058* 0.50
C1 0.68716 (18) −0.01306 (15) 0.75191 (15) 0.0245 (3)
C2 0.78155 (19) 0.04888 (16) 0.84031 (15) 0.0259 (4)
H2 0.8319 0.0262 0.9130 0.031*
C3 0.78367 (19) 0.14687 (17) 0.79813 (16) 0.0274 (4)
H3 0.8360 0.2030 0.8365 0.033*
C4 0.68969 (18) 0.14729 (16) 0.68298 (16) 0.0262 (4)
C5 0.66400 (19) 0.23239 (16) 0.60800 (16) 0.0266 (4)
C6 0.57669 (19) 0.23375 (16) 0.49389 (16) 0.0268 (4)
C7 0.55237 (19) 0.32147 (16) 0.41809 (17) 0.0284 (4)
H7 0.5903 0.3878 0.4360 0.034*
C8 0.46382 (19) 0.29004 (16) 0.31546 (16) 0.0279 (4)
H8 0.4310 0.3306 0.2505 0.033*
C9 0.43046 (18) 0.18217 (16) 0.32611 (15) 0.0253 (4)
C10 0.65856 (18) −0.11936 (16) 0.75997 (15) 0.0247 (3)
C11 0.73248 (19) −0.17185 (16) 0.87048 (15) 0.0251 (3)
C12 0.8373 (2) −0.23659 (18) 0.88507 (17) 0.0314 (4)
H12 0.8602 −0.2483 0.8253 0.038*
C13 0.9080 (2) −0.2840 (2) 0.98771 (19) 0.0376 (5)
H13 0.9778 −0.3274 0.9964 0.045*
C14 0.8756 (2) −0.2673 (2) 1.07638 (18) 0.0387 (5)
H14 0.9238 −0.2986 1.1454 0.046*
C15 0.7702 (3) −0.2033 (2) 1.06295 (18) 0.0393 (5)
H15 0.7475 −0.1924 1.1229 0.047*
C16 0.6988 (2) −0.15561 (19) 0.96030 (17) 0.0334 (4)
H16 0.6285 −0.1128 0.9516 0.040*
C17 0.74361 (19) 0.32920 (16) 0.65294 (17) 0.0280 (4)
C18 0.8459 (2) 0.35026 (19) 0.62357 (18) 0.0341 (4)
H18 0.8621 0.3061 0.5740 0.041*
C19 0.9245 (2) 0.4378 (2) 0.6684 (2) 0.0448 (6)
H19 0.9926 0.4522 0.6481 0.054*
C20 0.9024 (3) 0.5030 (2) 0.7422 (3) 0.0563 (8)
H20 0.9560 0.5608 0.7725 0.068*
C21 0.8015 (4) 0.4829 (2) 0.7712 (3) 0.0622 (9)
H21 0.7861 0.5275 0.8208 0.075*
C22 0.7216 (3) 0.3962 (2) 0.7270 (3) 0.0490 (6)
H22 0.6530 0.3831 0.7472 0.059*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Sn1 0.03022 (10) 0.02873 (10) 0.02008 (9) −0.01209 (8) 0.00016 (7) 0.00446 (7)
N2 0.0283 (8) 0.0275 (8) 0.0206 (7) −0.0088 (6) 0.0037 (6) 0.0030 (6)
N1 0.0266 (7) 0.0268 (8) 0.0208 (7) −0.0068 (6) 0.0031 (6) 0.0026 (6)
O1 0.0350 (8) 0.0416 (9) 0.0396 (9) 0.0014 (7) 0.0149 (7) 0.0072 (7)
N3 0.037 (2) 0.076 (4) 0.044 (2) −0.013 (2) 0.0184 (19) −0.005 (2)
C23 0.048 (3) 0.055 (3) 0.040 (3) 0.001 (2) 0.017 (2) 0.005 (2)
O2 0.0350 (8) 0.0416 (9) 0.0396 (9) 0.0014 (7) 0.0149 (7) 0.0072 (7)
C1 0.0231 (8) 0.0279 (9) 0.0195 (7) −0.0017 (7) 0.0057 (6) 0.0009 (6)
C2 0.0249 (8) 0.0288 (9) 0.0202 (7) −0.0008 (7) 0.0055 (6) −0.0021 (7)
C3 0.0247 (8) 0.0305 (10) 0.0224 (8) −0.0054 (7) 0.0049 (7) −0.0033 (7)
C4 0.0240 (8) 0.0283 (9) 0.0221 (8) −0.0063 (7) 0.0054 (6) −0.0011 (7)
C5 0.0257 (8) 0.0256 (9) 0.0248 (8) −0.0073 (7) 0.0066 (7) −0.0009 (7)
C6 0.0257 (8) 0.0264 (9) 0.0241 (8) −0.0074 (7) 0.0060 (7) 0.0018 (7)
C7 0.0287 (9) 0.0254 (9) 0.0280 (9) −0.0068 (7) 0.0085 (7) 0.0032 (7)
C8 0.0283 (9) 0.0278 (9) 0.0254 (8) −0.0035 (7) 0.0088 (7) 0.0053 (7)
C9 0.0247 (8) 0.0268 (9) 0.0217 (7) −0.0038 (7) 0.0068 (6) 0.0031 (6)
C10 0.0237 (8) 0.0288 (9) 0.0196 (7) −0.0027 (7) 0.0070 (6) 0.0020 (6)
C11 0.0268 (8) 0.0247 (8) 0.0199 (7) −0.0035 (7) 0.0056 (6) 0.0005 (6)
C12 0.0309 (9) 0.0356 (11) 0.0238 (8) 0.0024 (8) 0.0072 (7) −0.0005 (7)
C13 0.0311 (10) 0.0377 (12) 0.0327 (10) 0.0004 (9) 0.0017 (8) 0.0033 (9)
C14 0.0376 (11) 0.0405 (12) 0.0259 (9) −0.0074 (10) 0.0008 (8) 0.0086 (8)
C15 0.0485 (13) 0.0441 (13) 0.0249 (9) −0.0062 (11) 0.0148 (9) 0.0042 (9)
C16 0.0388 (11) 0.0375 (11) 0.0264 (9) 0.0011 (9) 0.0159 (8) 0.0033 (8)
C17 0.0271 (8) 0.0241 (9) 0.0266 (8) −0.0052 (7) 0.0049 (7) 0.0009 (7)
C18 0.0323 (10) 0.0344 (11) 0.0311 (10) −0.0076 (8) 0.0084 (8) 0.0010 (8)
C19 0.0340 (11) 0.0420 (13) 0.0462 (13) −0.0153 (10) 0.0042 (10) 0.0105 (11)
C20 0.0528 (16) 0.0293 (12) 0.0615 (18) −0.0169 (11) −0.0019 (13) −0.0039 (12)
C21 0.067 (2) 0.0404 (16) 0.075 (2) −0.0133 (14) 0.0255 (18) −0.0291 (15)
C22 0.0483 (14) 0.0454 (15) 0.0580 (16) −0.0131 (12) 0.0265 (13) −0.0187 (12)

Geometric parameters (Å, °)

Sn1—O2i 2.0737 (18) C8—C9 1.442 (3)
Sn1—O1i 2.0737 (18) C8—H8 0.9300
Sn1—O1 2.0737 (18) C9—C10i 1.408 (3)
Sn1—N2i 2.0976 (17) C10—C9i 1.408 (3)
Sn1—N2 2.0976 (17) C10—C11 1.496 (3)
Sn1—N1 2.1018 (16) C11—C12 1.388 (3)
Sn1—N1i 2.1018 (16) C11—C16 1.390 (3)
N2—C6 1.374 (2) C12—C13 1.386 (3)
N2—C9 1.375 (2) C12—H12 0.9300
N1—C4 1.368 (3) C13—C14 1.368 (4)
N1—C1 1.369 (2) C13—H13 0.9300
O1—C23 1.241 (6) C14—C15 1.391 (4)
O1—H2A 0.8202 C14—H14 0.9300
N3—C23 1.244 (7) C15—C16 1.389 (3)
C23—H2A 1.4810 C15—H15 0.9300
C1—C10 1.402 (3) C16—H16 0.9300
C1—C2 1.442 (3) C17—C18 1.385 (3)
C2—C3 1.365 (3) C17—C22 1.386 (3)
C2—H2 0.9300 C18—C19 1.393 (3)
C3—C4 1.442 (3) C18—H18 0.9300
C3—H3 0.9300 C19—C20 1.370 (5)
C4—C5 1.407 (3) C19—H19 0.9300
C5—C6 1.410 (3) C20—C21 1.364 (5)
C5—C17 1.494 (3) C20—H20 0.9300
C6—C7 1.440 (3) C21—C22 1.390 (4)
C7—C8 1.363 (3) C21—H21 0.9300
C7—H7 0.9300 C22—H22 0.9300
O2i—Sn1—O1i 0.00 (4) C5—C6—C7 126.15 (18)
O2i—Sn1—O1 180.0 C8—C7—C6 107.83 (17)
O1i—Sn1—O1 180.0 C8—C7—H7 126.1
O2i—Sn1—N2i 87.88 (7) C6—C7—H7 126.1
O1i—Sn1—N2i 87.88 (7) C7—C8—C9 107.36 (17)
O1—Sn1—N2i 92.12 (7) C7—C8—H8 126.3
O2i—Sn1—N2 92.12 (7) C9—C8—H8 126.3
O1i—Sn1—N2 92.12 (7) N2—C9—C10i 125.74 (18)
O1—Sn1—N2 87.88 (7) N2—C9—C8 108.13 (16)
N2i—Sn1—N2 180.0 C10i—C9—C8 126.13 (17)
O2i—Sn1—N1 89.10 (7) C1—C10—C9i 126.59 (17)
O1i—Sn1—N1 89.10 (7) C1—C10—C11 116.56 (16)
O1—Sn1—N1 90.90 (7) C9i—C10—C11 116.83 (17)
N2i—Sn1—N1 89.75 (6) C12—C11—C16 119.03 (18)
N2—Sn1—N1 90.25 (6) C12—C11—C10 120.18 (18)
O2i—Sn1—N1i 90.90 (7) C16—C11—C10 120.79 (19)
O1i—Sn1—N1i 90.90 (7) C13—C12—C11 120.7 (2)
O1—Sn1—N1i 89.10 (7) C13—C12—H12 119.7
N2i—Sn1—N1i 90.25 (6) C11—C12—H12 119.7
N2—Sn1—N1i 89.75 (6) C14—C13—C12 120.3 (2)
N1—Sn1—N1i 180.0 C14—C13—H13 119.9
C6—N2—C9 108.73 (16) C12—C13—H13 119.9
C6—N2—Sn1 125.33 (13) C13—C14—C15 119.8 (2)
C9—N2—Sn1 125.86 (13) C13—C14—H14 120.1
C4—N1—C1 109.20 (15) C15—C14—H14 120.1
C4—N1—Sn1 125.12 (13) C16—C15—C14 120.2 (2)
C1—N1—Sn1 125.33 (13) C16—C15—H15 119.9
C23—O1—Sn1 118.8 (3) C14—C15—H15 119.9
C23—O1—H2A 89.5 C15—C16—C11 120.0 (2)
Sn1—O1—H2A 109.4 C15—C16—H16 120.0
O1—C23—N3 175.3 (6) C11—C16—H16 120.0
O1—C23—H2A 33.6 C18—C17—C22 119.0 (2)
N3—C23—H2A 144.8 C18—C17—C5 119.1 (2)
N1—C1—C10 126.57 (17) C22—C17—C5 121.9 (2)
N1—C1—C2 107.80 (17) C17—C18—C19 119.8 (2)
C10—C1—C2 125.62 (17) C17—C18—H18 120.1
C3—C2—C1 107.66 (16) C19—C18—H18 120.1
C3—C2—H2 126.2 C20—C19—C18 120.7 (3)
C1—C2—H2 126.2 C20—C19—H19 119.7
C2—C3—C4 107.30 (17) C18—C19—H19 119.7
C2—C3—H3 126.3 C21—C20—C19 119.8 (2)
C4—C3—H3 126.3 C21—C20—H20 120.1
N1—C4—C5 126.31 (17) C19—C20—H20 120.1
N1—C4—C3 108.03 (17) C20—C21—C22 120.5 (3)
C5—C4—C3 125.64 (18) C20—C21—H21 119.8
C4—C5—C6 126.92 (18) C22—C21—H21 119.8
C4—C5—C17 116.08 (16) C17—C22—C21 120.3 (3)
C6—C5—C17 116.89 (17) C17—C22—H22 119.9
N2—C6—C5 125.89 (18) C21—C22—H22 119.9
N2—C6—C7 107.95 (16)

Symmetry codes: (i) −x+1, −y, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: DN2696).

References

  1. Allen, F. H. (2002). Acta Cryst. B58, 380–388. [DOI] [PubMed]
  2. Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
  3. Bruker (2007). APEX2, SAINT and SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Burla, M. C., Caliandro, R., Camalli, M., Carrozzini, B., Cascarano, G. L., De Caro, L., Giacovazzo, C., Polidori, G. & Spagna, R. (2005). J. Appl. Cryst. 38, 381–388.
  5. Burnett, M. N. & Johnson, C. K. (1996). Report ORNL-6895, Oak Ridge National Laboratory, Tennesse, USA.
  6. Fallon, G. D., Lee, M. A.-P., Langford, S. J. & Nichols, P. J. (2002). Org. Lett. 4, 1895–1998. [DOI] [PubMed]
  7. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  8. Martelli, C., Canning, J., Reimers, J. R., Sintic, M., Stocks, D., Khoury, T. & Crossley, M. J. (2009). J. Am. Chem. Soc. 131, 2925–2933. [DOI] [PubMed]
  9. Scheidt, W. R. (2000). The Porphyrin Handbook, Vol. 3, edited by K. M. Kadish, R. M. Smith & R. Guilard, pp. 49–112. San Diego: Academic Press.
  10. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  11. Smith, G., Arnold, D. P., Kennard, C. H. L. & Mak, T. C. W. (1991). Polyhedron, 10, 509–516.
  12. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

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/S1600536811021544/dn2696sup1.cif

e-67-0m903-sup1.cif (19.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021544/dn2696Isup2.hkl

e-67-0m903-Isup2.hkl (286.3KB, hkl)

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


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