Abstract
The title compound, cis-[RuCl2(C3H9P)4]·2C6H6, contains a complex molecule with a crystallographic mirror plane passing through the RuII atom, the two cis-disposed Cl ligands and two P atoms of the two cis-disposed P(CH3)3 ligands. The RuII atom adopts a distorted octahedral RuCl2P4 coordination geometry with the two trans-disposed P atoms occupying the axial positions. The packing of the structure is accomplished through non-classical C—H⋯Cl hydrogen bonds between the benzene solvent molecule and one of the Cl ligands.
Related literature
For general background to trans-[RuCl2(P(CH3)3)4], see: Csok et al. (2007 ▶); Gotzig et al. (1985 ▶); Hartwig et al. (1991 ▶); Hirano et al. (2010 ▶); Kohlmann & Werner (1993 ▶). For a related structure, see: Joo et al. (1994 ▶).
Experimental
Crystal data
[RuCl2(C3H9P)4]·2C6H6
M r = 632.47
Orthorhombic,
a = 17.6243 (15) Å
b = 18.1889 (19) Å
c = 9.4610 (11) Å
V = 3032.9 (5) Å3
Z = 4
Mo Kα radiation
μ = 0.92 mm−1
T = 173 K
0.18 × 0.12 × 0.06 mm
Data collection
Oxford Diffraction Gemini S Ultra diffractometer
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008 ▶) T min = 0.949, T max = 1.000
14352 measured reflections
3550 independent reflections
1653 reflections with I > 2σ(I)
R int = 0.148
Refinement
R[F 2 > 2σ(F 2)] = 0.058
wR(F 2) = 0.081
S = 0.82
3550 reflections
139 parameters
H-atom parameters constrained
Δρmax = 0.97 e Å−3
Δρmin = −0.57 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2008 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2008 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810049706/wm2431sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049706/wm2431Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Ru1—P1 | 2.2690 (19) |
| Ru1—P2 | 2.297 (2) |
| Ru1—P3 | 2.3819 (14) |
| Ru1—Cl1 | 2.479 (2) |
| Ru1—Cl2 | 2.5038 (19) |
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C4S—H4SA⋯Cl2 | 0.93 | 2.83 | 3.710 (5) | 159 |
Acknowledgments
The authors acknowledge financial support from the Young Talent Project of Department of Science & Technology of Fujian Province (grant No. 2007 F3095).
supplementary crystallographic information
Comment
The ruthenium(II) complex trans-[RuCl2(PMe3)4], which can be readily prepared from the reaction of RuCl2(PPh3)3 with PMe3 in hexane at room temperature (Gotzig et al., 1985), has proved to be a useful precursor for a wide variety of ruthenium compounds (Hartwig et al., 1991; Kohlmann & Werner, 1993; Csok et al., 2007; Hirano et al., 2010). However, its geometrical isomer, cis-[RuCl2(PMe3)4], has not been reported yet. During our preparation of ruthenium compounds with phosphine ligands using trans-[RuCl2(PMe3)4] as the starting material, we found that the trans-isomer slowly isomerizes to the cis-isomer, the structure of which we report here as the benzene disolvate.
As shown in Fig.1, the structure of the title complex possesses a crystallographic mirror plane passing through the RuII atom, the two cis-disposed Cl ligands and the two P atoms as well as two C atoms of the two cis-disposed PMe3 ligands. Thus the asymmetric unit of the structure contains half of a molecule. The RuII atom adopts a distorted octahedral geometry with the two trans-disposed P atoms occupying the axial positions. The bond lengths of the two axial Ru—P bonds (2.3819 (14) Å), which are actually image-related, are slightly longer than those of the two equatorial Ru—P bonds which are trans to the Cl ligands (2.2690 (19) and 2.297 (2) Å, respectively). The two Ru—Cl bond lengths are 2.479 (2) and 2.5038 (19) Å, respectively, while the Cl(1)—Ru(1)—Cl(2) bond angle is 86.20 (7)°. These geometric values are similar to those reported for the only example of a sructurally characterized monodentate tetrakis(phosphine)-cis-dichlorido-ruthenium(II) complex, viz. [cis-RuCl2(PTA)4] (PTA = 1,3,5-triaza-7-phospha-adamantane-κP); 2.488 (2) and 2.503 (2) Å, 84.2 (1) °; Joo et al., 1994).
The packing of the structure (Fig. 2) is accomplished through non-classical C—H···Cl hydrogen bonds between the benzene solvent molecule and one of the Cl ligands (Table 2).
Experimental
Route A: To a solution of RuCl2(PPh3)3 (0.25 g, 0.24 mmol) in toluene (8 ml) under nitrogen atmosphere was added PMe3 (0.27 ml, 2.5 mmol) and the resulting yellow solution was refluxed for 20 h. The solvent was removed under vacuum, and the solid residue was washed with n-hexane, and dried under vacuum to afford a white solid. Yield: 90 mg, 80%. Route B: A solution of trans-[RuCl2(PMe3)4] (100 mg, 0.21 mmol) in benzene (5 ml) was refluxed for 12 h under nitrogen atmosphere. After the solution was cooled to ambient temperature, a white solid was precipitated, which was collected by filtration, washed with n-hexane, and dried under vacuum. Yield: 72 mg, 72%. Crystals suitable for X-ray analysis were obtained from standing a solution of trans-[RuCl2(PMe3)4] in benzene at room temperature for 2 weeks.
Refinement
The benzene solvent molecule was treated as a rigid body. All non-hydrogen atoms were refined anisotropically. The hydrogen atoms were positioned geometrically (C—H = 0.96 or 0.93 Å for methyl or phenyl H atoms, respectively) and were included in the refinement in the riding model approximation. The displacement parameters of methyl H atoms were set to 1.5Ueq(C), while those of the phenyl H atoms were set to 1.2Ueq(C). In the final Fourier map the highest peak is 0.04 Å from atom Ru1 and the deepest hole is 0.71 Å from atom Ru1.
Figures
Fig. 1.
The coordination of the RuII atom in the structure of cis-[RuCl2(P(CH3)3)4] with the atom labelling and displacement ellipsoids drawn at the 30% probability level. H atoms have been omitted for clarity. [Symmetry code: (A) x, -y+1/2, z.]
Fig. 2.
The packing diagram of the structure viewed down the c axis, showing the non-classical C—H···Cl hydrogen bonds between the benzene solvent molecule and one of the Cl ligands of the complex molecule.
Crystal data
| [RuCl2(C3H9P)4]·2C6H6 | F(000) = 1320 |
| Mr = 632.47 | Dx = 1.385 Mg m−3 |
| Orthorhombic, Pnma | Mo Kα radiation, λ = 0.7107 Å |
| Hall symbol: -P 2ac 2n | Cell parameters from 1376 reflections |
| a = 17.6243 (15) Å | θ = 2.3–28.9° |
| b = 18.1889 (19) Å | µ = 0.92 mm−1 |
| c = 9.4610 (11) Å | T = 173 K |
| V = 3032.9 (5) Å3 | Block, colorless |
| Z = 4 | 0.18 × 0.12 × 0.06 mm |
Data collection
| Oxford Diffraction Gemini S Ultra diffractometer | 3550 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 1653 reflections with I > 2σ(I) |
| graphite | Rint = 0.148 |
| Detector resolution: 16.1930 pixels mm-1 | θmax = 27.5°, θmin = 2.3° |
| ω scans | h = −22→21 |
| Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008) | k = −23→22 |
| Tmin = 0.949, Tmax = 1.000 | l = −10→12 |
| 14352 measured reflections |
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)] = 0.058 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.081 | H-atom parameters constrained |
| S = 0.82 | w = 1/[σ2(Fo2) + (0.0104P)2] where P = (Fo2 + 2Fc2)/3 |
| 3550 reflections | (Δ/σ)max = 0.003 |
| 139 parameters | Δρmax = 0.97 e Å−3 |
| 0 restraints | Δρmin = −0.57 e Å−3 |
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 | ||
| Ru1 | 0.54358 (3) | 0.2500 | 0.30360 (7) | 0.01803 (17) | |
| Cl1 | 0.47805 (10) | 0.2500 | 0.0718 (2) | 0.0308 (6) | |
| Cl2 | 0.41377 (9) | 0.2500 | 0.4111 (2) | 0.0347 (6) | |
| P1 | 0.66211 (10) | 0.2500 | 0.2100 (2) | 0.0221 (5) | |
| P2 | 0.57932 (10) | 0.2500 | 0.5371 (2) | 0.0233 (6) | |
| P3 | 0.53321 (8) | 0.37973 (7) | 0.27518 (17) | 0.0273 (4) | |
| C11 | 0.6660 (4) | 0.2500 | 0.0209 (8) | 0.032 (2) | |
| H11A | 0.7178 | 0.2500 | −0.0104 | 0.049* | |
| H11B | 0.6408 | 0.2069 | −0.0142 | 0.049* | |
| C12 | 0.7266 (2) | 0.3256 (2) | 0.2488 (6) | 0.0303 (17) | |
| H12A | 0.7740 | 0.3175 | 0.2015 | 0.045* | |
| H12B | 0.7350 | 0.3282 | 0.3489 | 0.045* | |
| H12C | 0.7047 | 0.3709 | 0.2165 | 0.045* | |
| C21 | 0.6769 (3) | 0.2500 | 0.5976 (8) | 0.036 (2) | |
| H21A | 0.6785 | 0.2500 | 0.6990 | 0.055* | |
| H21B | 0.7020 | 0.2069 | 0.5623 | 0.055* | |
| C22 | 0.5445 (3) | 0.3255 (3) | 0.6447 (6) | 0.057 (2) | |
| H22A | 0.5627 | 0.3200 | 0.7397 | 0.086* | |
| H22B | 0.4900 | 0.3252 | 0.6447 | 0.086* | |
| H22C | 0.5624 | 0.3713 | 0.6065 | 0.086* | |
| C31 | 0.5557 (3) | 0.4150 (3) | 0.1015 (6) | 0.0368 (16) | |
| H31A | 0.5499 | 0.4675 | 0.1010 | 0.055* | |
| H31B | 0.5221 | 0.3936 | 0.0331 | 0.055* | |
| H31C | 0.6072 | 0.4027 | 0.0781 | 0.055* | |
| C32 | 0.4370 (2) | 0.4140 (3) | 0.2916 (7) | 0.0447 (18) | |
| H32A | 0.4369 | 0.4664 | 0.2789 | 0.067* | |
| H32B | 0.4177 | 0.4023 | 0.3837 | 0.067* | |
| H32C | 0.4056 | 0.3916 | 0.2208 | 0.067* | |
| C33 | 0.5837 (3) | 0.4488 (3) | 0.3798 (6) | 0.046 (2) | |
| H33A | 0.5700 | 0.4971 | 0.3476 | 0.069* | |
| H33B | 0.6374 | 0.4420 | 0.3690 | 0.069* | |
| H33C | 0.5703 | 0.4436 | 0.4776 | 0.069* | |
| C1S | 0.2535 (3) | 0.4577 (2) | 0.8727 (8) | 0.069 (3) | |
| H1SA | 0.2273 | 0.4919 | 0.9273 | 0.082* | |
| C2S | 0.3127 (4) | 0.4177 (4) | 0.9316 (4) | 0.073 (3) | |
| H2SA | 0.3263 | 0.4251 | 1.0255 | 0.088* | |
| C3S | 0.3518 (2) | 0.3667 (3) | 0.8500 (8) | 0.068 (3) | |
| H3SA | 0.3915 | 0.3399 | 0.8894 | 0.081* | |
| C4S | 0.3316 (3) | 0.3557 (2) | 0.7096 (8) | 0.059 (2) | |
| H4SA | 0.3578 | 0.3215 | 0.6550 | 0.071* | |
| C5S | 0.2724 (3) | 0.3957 (3) | 0.6507 (4) | 0.059 (2) | |
| H5SA | 0.2589 | 0.3883 | 0.5567 | 0.071* | |
| C6S | 0.23327 (19) | 0.4467 (3) | 0.7323 (8) | 0.064 (3) | |
| H6SA | 0.1936 | 0.4735 | 0.6929 | 0.076* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Ru1 | 0.0145 (3) | 0.0200 (3) | 0.0196 (4) | 0.000 | −0.0017 (4) | 0.000 |
| Cl1 | 0.0333 (12) | 0.0318 (13) | 0.0275 (14) | 0.000 | −0.0146 (10) | 0.000 |
| Cl2 | 0.0154 (11) | 0.0489 (14) | 0.0398 (15) | 0.000 | −0.0001 (10) | 0.000 |
| P1 | 0.0212 (10) | 0.0254 (12) | 0.0197 (14) | 0.000 | 0.0015 (11) | 0.000 |
| P2 | 0.0181 (11) | 0.0330 (14) | 0.0187 (14) | 0.000 | 0.0012 (10) | 0.000 |
| P3 | 0.0230 (8) | 0.0249 (8) | 0.0339 (11) | 0.0015 (7) | −0.0029 (8) | −0.0031 (8) |
| C11 | 0.029 (5) | 0.036 (6) | 0.032 (6) | 0.000 | 0.012 (4) | 0.000 |
| C12 | 0.026 (3) | 0.029 (3) | 0.036 (5) | 0.002 (3) | 0.003 (3) | 0.000 (3) |
| C21 | 0.023 (5) | 0.073 (7) | 0.013 (5) | 0.000 | −0.004 (4) | 0.000 |
| C22 | 0.059 (4) | 0.081 (5) | 0.032 (4) | 0.027 (4) | −0.006 (4) | −0.018 (4) |
| C31 | 0.048 (4) | 0.027 (3) | 0.035 (4) | −0.003 (3) | −0.002 (3) | 0.008 (3) |
| C32 | 0.039 (4) | 0.031 (3) | 0.064 (5) | 0.009 (3) | −0.008 (4) | −0.001 (4) |
| C33 | 0.039 (4) | 0.033 (4) | 0.066 (6) | −0.007 (3) | 0.003 (3) | −0.013 (4) |
| C1S | 0.085 (6) | 0.053 (6) | 0.067 (7) | −0.029 (5) | 0.050 (5) | −0.019 (6) |
| C2S | 0.099 (7) | 0.091 (8) | 0.029 (5) | −0.066 (5) | −0.019 (5) | 0.026 (6) |
| C3S | 0.039 (4) | 0.063 (6) | 0.101 (9) | −0.009 (4) | −0.006 (5) | 0.041 (6) |
| C4S | 0.056 (5) | 0.026 (4) | 0.097 (8) | −0.004 (3) | 0.049 (5) | −0.009 (5) |
| C5S | 0.087 (6) | 0.059 (6) | 0.033 (5) | −0.050 (4) | −0.003 (5) | 0.007 (5) |
| C6S | 0.035 (4) | 0.037 (5) | 0.119 (10) | −0.007 (3) | 0.010 (5) | 0.029 (6) |
Geometric parameters (Å, °)
| Ru1—P1 | 2.2690 (19) | C22—H22B | 0.9600 |
| Ru1—P2 | 2.297 (2) | C22—H22C | 0.9600 |
| Ru1—P3i | 2.3819 (14) | C31—H31A | 0.9600 |
| Ru1—P3 | 2.3819 (14) | C31—H31B | 0.9600 |
| Ru1—Cl1 | 2.479 (2) | C31—H31C | 0.9600 |
| Ru1—Cl2 | 2.5038 (19) | C32—H32A | 0.9600 |
| P1—C11 | 1.790 (8) | C32—H32B | 0.9600 |
| P1—C12 | 1.821 (4) | C32—H32C | 0.9600 |
| P1—C12i | 1.821 (4) | C33—H33A | 0.9600 |
| P2—C21 | 1.812 (6) | C33—H33B | 0.9600 |
| P2—C22 | 1.816 (5) | C33—H33C | 0.9600 |
| P2—C22i | 1.816 (5) | C1S—C2S | 1.3900 |
| P3—C31 | 1.808 (5) | C1S—C6S | 1.3900 |
| P3—C32 | 1.813 (4) | C1S—H1SA | 0.9300 |
| P3—C33 | 1.831 (5) | C2S—C3S | 1.3900 |
| C11—H11A | 0.9600 | C2S—H2SA | 0.9300 |
| C11—H11B | 0.9598 | C3S—C4S | 1.3900 |
| C12—H12A | 0.9600 | C3S—H3SA | 0.9300 |
| C12—H12B | 0.9600 | C4S—C5S | 1.3900 |
| C12—H12C | 0.9600 | C4S—H4SA | 0.9300 |
| C21—H21A | 0.9600 | C5S—C6S | 1.3900 |
| C21—H21B | 0.9599 | C5S—H5SA | 0.9300 |
| C22—H22A | 0.9600 | C6S—H6SA | 0.9300 |
| P1—Ru1—P2 | 97.07 (8) | H21A—C21—H21B | 109.5 |
| P1—Ru1—P3i | 91.52 (4) | P2—C22—H22A | 109.5 |
| P2—Ru1—P3i | 97.45 (4) | P2—C22—H22B | 109.5 |
| P1—Ru1—P3 | 91.52 (4) | H22A—C22—H22B | 109.5 |
| P2—Ru1—P3 | 97.45 (4) | P2—C22—H22C | 109.5 |
| P3i—Ru1—P3 | 164.31 (8) | H22A—C22—H22C | 109.5 |
| P1—Ru1—Cl1 | 94.79 (8) | H22B—C22—H22C | 109.5 |
| P2—Ru1—Cl1 | 168.14 (7) | P3—C31—H31A | 109.5 |
| P3i—Ru1—Cl1 | 82.20 (4) | P3—C31—H31B | 109.5 |
| P3—Ru1—Cl1 | 82.20 (4) | H31A—C31—H31B | 109.5 |
| P1—Ru1—Cl2 | 179.01 (9) | P3—C31—H31C | 109.5 |
| P2—Ru1—Cl2 | 81.94 (7) | H31A—C31—H31C | 109.5 |
| P3i—Ru1—Cl2 | 88.61 (4) | H31B—C31—H31C | 109.5 |
| P3—Ru1—Cl2 | 88.61 (4) | P3—C32—H32A | 109.5 |
| Cl1—Ru1—Cl2 | 86.20 (7) | P3—C32—H32B | 109.5 |
| C11—P1—C12 | 100.2 (2) | H32A—C32—H32B | 109.5 |
| C11—P1—C12i | 100.2 (2) | P3—C32—H32C | 109.5 |
| C12—P1—C12i | 98.0 (3) | H32A—C32—H32C | 109.5 |
| C11—P1—Ru1 | 115.2 (2) | H32B—C32—H32C | 109.5 |
| C12—P1—Ru1 | 119.71 (17) | P3—C33—H33A | 109.5 |
| C12i—P1—Ru1 | 119.71 (17) | P3—C33—H33B | 109.5 |
| C21—P2—C22 | 98.3 (2) | H33A—C33—H33B | 109.5 |
| C21—P2—C22i | 98.3 (2) | P3—C33—H33C | 109.5 |
| C22—P2—C22i | 98.3 (4) | H33A—C33—H33C | 109.5 |
| C21—P2—Ru1 | 124.3 (3) | H33B—C33—H33C | 109.5 |
| C22—P2—Ru1 | 116.5 (2) | C2S—C1S—C6S | 120.0 |
| C22i—P2—Ru1 | 116.5 (2) | C2S—C1S—H1SA | 120.0 |
| C31—P3—C32 | 99.3 (3) | C6S—C1S—H1SA | 120.0 |
| C31—P3—C33 | 98.1 (3) | C3S—C2S—C1S | 120.0 |
| C32—P3—C33 | 99.9 (2) | C3S—C2S—H2SA | 120.0 |
| C31—P3—Ru1 | 115.93 (18) | C1S—C2S—H2SA | 120.0 |
| C32—P3—Ru1 | 113.76 (17) | C2S—C3S—C4S | 120.0 |
| C33—P3—Ru1 | 125.57 (19) | C2S—C3S—H3SA | 120.0 |
| P1—C11—H11A | 110.1 | C4S—C3S—H3SA | 120.0 |
| P1—C11—H11B | 109.1 | C3S—C4S—C5S | 120.0 |
| H11A—C11—H11B | 109.5 | C3S—C4S—H4SA | 120.0 |
| P1—C12—H12A | 109.5 | C5S—C4S—H4SA | 120.0 |
| P1—C12—H12B | 109.5 | C6S—C5S—C4S | 120.0 |
| H12A—C12—H12B | 109.5 | C6S—C5S—H5SA | 120.0 |
| P1—C12—H12C | 109.5 | C4S—C5S—H5SA | 120.0 |
| H12A—C12—H12C | 109.5 | C5S—C6S—C1S | 120.0 |
| H12B—C12—H12C | 109.5 | C5S—C6S—H6SA | 120.0 |
| P2—C21—H21A | 110.1 | C1S—C6S—H6SA | 120.0 |
| P2—C21—H21B | 109.1 |
Symmetry codes: (i) x, −y+1/2, z.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C4S—H4SA···Cl2i | 0.93 | 2.83 | 3.710 (5) | 159. |
Symmetry codes: i.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2431).
References
- Csok, Z., Gandum, C., Rissanen, K., Tuzi, A. & Rodrigues, J. (2007). J. Organomet. Chem. 692, 5263–5271.
- Gotzig, J., Werner, R. & Werner, H. (1985). J. Organomet. Chem. 290, 99–114.
- Hartwig, J. F., Bergman, R. G. & Andersen, R. A. (1991). Organometallics, 10, 3344–3362.
- Hirano, M., Togashi, S., Ito, M., Sakaguchi, Y., Komine, N. & Komiya, S. (2010). Organometallics, 29, 3146–3159.
- Joo, F., Kannisto, M., Katho, A., Reibenspies, J., Daigle, D. & Darensbourg, D. (1994). Inorg. Chem. 33, 200–208.
- Kohlmann, W. & Werner, H. (1993). Z. Naturforsch. Teil B, 48, 1499–1511.
- Oxford Diffraction (2008). CrysAlis CCD and CrysAlis RED Oxford Diffraction Ltd, Yarnton, England.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810049706/wm2431sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810049706/wm2431Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


