Abstract
In the title complex, [CuCl2(C17H11N3O2)2], the CuII ion is located on an inversion center. It exhibits a distorted octahedral coordination geometry defined by two chloride anions at trans sites and four 3-pyridyl N atoms at equatorial sites from two (6-nicotinoyl-2-pyridyl)(3-pyridyl)methanone ligands. The (6-nicotinoyl-2-pyridyl)(3-pyridyl)methanone ligand can be viewed as having two pendant 3-pyridyl rings attached to a central pyridyl skeleton via separate carbonyl bridges, acting in a κ2 N,N′-chelating mode with its 3-pyridyl N atoms bound to the CuII ion. The pendant 3-pyridyl rings make a dihedral angle of 80.76 (5)°. In the crystal, molecules are linked through intermolecular C—H⋯π and C—H⋯O interactions, forming a three-dimentional framework.
Related literature
For transition metal complexes with di-pyrid-2-yl ketone, see: Papaefstathiou & Perlepes (2002 ▶); Efthymiou et al. (2006 ▶). For the crystal structure of an analogous CuII complex, see: Wan et al. (2008 ▶). For C—H⋯π interactions, see: Umezawa et al. (1998 ▶).
Experimental
Crystal data
[CuCl2(C17H11N3O2)2]
M r = 713.02
Monoclinic,
a = 18.728 (3) Å
b = 11.8971 (18) Å
c = 16.695 (3) Å
β = 121.522 (3)°
V = 3170.9 (8) Å3
Z = 4
Mo Kα radiation
μ = 0.91 mm−1
T = 293 K
0.40 × 0.30 × 0.30 mm
Data collection
Bruker APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2007 ▶) T min = 0.848, T max = 1.000
11215 measured reflections
3937 independent reflections
3361 reflections with I > 2σ(I)
R int = 0.020
Refinement
R[F 2 > 2σ(F 2)] = 0.029
wR(F 2) = 0.084
S = 1.04
3937 reflections
215 parameters
H-atom parameters constrained
Δρmax = 0.25 e Å−3
Δρmin = −0.21 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: APEX2 and SAINT (Bruker, 2007 ▶); 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 and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811017685/zq2102sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811017685/zq2102Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the C13–C17,N3 ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C13—H13A⋯O1i | 0.93 | 2.61 | 3.418 (2) | 146 |
| C2—H2A⋯Cg1ii | 0.93 | 2.73 | 3.621 (3) | 162 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors are grateful for financial support from the Science and Technology program, Beijing Municipal Education Commission.
supplementary crystallographic information
Comment
Di-pyridin-2-yl-methanone (di-pyrid-2-yl ketone, DPK), (C5H4N)2CO, is an extraordinarily versatile ligand among the thousands of basic building blocks that have been used in coordination chemistry and materials science (Papaefstathiou & Perlepes, 2002; Efthymiou et al., 2006). Herein, we report the mononuclear CuII complex with the oligo-pyridyl ketone ligand (6-nicotinoyl-2-pyridyl)(3-pyridyl)methanone (abbreviated as L), a member of the pyridinylmethanone family.
In the crystal structure of the title complex, the center CuII adopts an octahedral coordination geometry with two chlorido depositing in trans to each other, and two 2,6-pyridinediylbis(3-pyridinyl)methanone ligands bound to the ion by four 3-pyridyl N atoms (Fig. 1). The Cu1—N3 and Cu1—Cl1 bond lengths equal 2.0412 (12) Å and 2.3087 (4) Å, respectively, while the Cu-N1 exhibits weak bonding with the Cu-N1 distance of 2.615 (1) Å. The latter Cu—N bonds are remarkably longer than that (about 2.03 Å) in the similar complex Cu(L)2(BF4)2 (Wan et al. 2008). The pendant 3-pyridyl rings exhibit a dihedral angle of 80.76 (5)°. The mononuclear complex units link each other through the intermolecular C2—H2A···π and C13—H13A···O1ii interactions to form a three-dimentional framework, as shown in Fig. 2. For the C—H···π interaction (Umezawa et al. 1998), the C2···Cg1 distance (where Cg1 is the centroid of the ring containing N3i; i: -x+1, -y, 0.5-z) is 3.621 (3) Å, and the C2—H2A···Cg1 angle is 161.8° . For the C—H···O interaction, the C13···O1ii distance is 3.418 (2) Å, and the C13—H13A···O1ii angle is 146.2° (ii: x+0.5, y-0.5, z).
Experimental
The (6-nicotinoyl-2-pyridyl)(3-pyridyl)methanone ligand was obtained following the reaction procedure as reported in literature (Wan et al., 2008). Reaction of (6-nicotinoyl-2-pyridyl)(3-pyridyl)methanone (29 mg, 0.1 mmol) with CuCl2 (7 mg, 0.05 mmol) in acetonitrile formed trans-[Cu(C17H11N3O2)2Cl2] as a blue solution, which was left stand in air for four days to obtain block-like crystals (yield 13.1mg, 61%).
Refinement
The hydrogen atoms were placed in idealized positions and allowed to ride on the relevant carbon atoms, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C).
Figures
Fig. 1.
The atom-numbering scheme of the title complex (symmetry code: (i) -x+1.5, -y+0.5, -z+1.5) with red-dashed lines indicating weak Cu1-N1 bonding. Displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity.
Fig. 2.
View of the crystal packing of the title compound.
Crystal data
| [CuCl2(C17H11N3O2)2] | Z = 4 |
| Mr = 713.02 | F(000) = 1452 |
| Monoclinic, C2/c | Dx = 1.494 Mg m−3 |
| Hall symbol: -C 2yc | Mo Kα radiation, λ = 0.71073 Å |
| a = 18.728 (3) Å | µ = 0.91 mm−1 |
| b = 11.8971 (18) Å | T = 293 K |
| c = 16.695 (3) Å | Block, blue |
| β = 121.522 (3)° | 0.40 × 0.30 × 0.30 mm |
| V = 3170.9 (8) Å3 |
Data collection
| Bruker APEXII CCD area-detector diffractometer | 3937 independent reflections |
| Radiation source: fine-focus sealed tube | 3361 reflections with I > 2σ(I) |
| graphite | Rint = 0.020 |
| ω scans | θmax = 28.3°, θmin = 2.1° |
| Absorption correction: multi-scan (SADABS; Bruker, 2007) | h = −24→24 |
| Tmin = 0.848, Tmax = 1.000 | k = −15→15 |
| 11215 measured reflections | l = −19→22 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.029 | H-atom parameters constrained |
| wR(F2) = 0.084 | w = 1/[σ2(Fo2) + (0.0423P)2 + 2.1803P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.04 | (Δ/σ)max = 0.001 |
| 3937 reflections | Δρmax = 0.25 e Å−3 |
| 215 parameters | Δρmin = −0.21 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.00079 (17) |
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 | ||
| Cu1 | 0.7500 | 0.2500 | 0.5000 | 0.03142 (9) | |
| Cl1 | 0.69747 (3) | 0.11938 (3) | 0.38011 (3) | 0.03905 (11) | |
| O2 | 0.77486 (11) | 0.74717 (10) | 0.35782 (15) | 0.0670 (5) | |
| C12 | 0.73237 (11) | 0.67642 (13) | 0.36615 (13) | 0.0423 (4) | |
| C1 | 0.45389 (14) | 0.2790 (2) | 0.33217 (19) | 0.0666 (6) | |
| H1A | 0.4120 | 0.2267 | 0.2971 | 0.080* | |
| C2 | 0.43565 (12) | 0.39132 (18) | 0.32729 (16) | 0.0588 (5) | |
| H2A | 0.3811 | 0.4166 | 0.2878 | 0.071* | |
| C3 | 0.49909 (10) | 0.46676 (15) | 0.38157 (12) | 0.0404 (4) | |
| C4 | 0.57867 (10) | 0.42349 (14) | 0.44252 (12) | 0.0386 (3) | |
| H4A | 0.6207 | 0.4729 | 0.4830 | 0.046* | |
| N1 | 0.59789 (9) | 0.31499 (12) | 0.44589 (11) | 0.0464 (3) | |
| C5 | 0.53567 (13) | 0.24547 (15) | 0.39018 (18) | 0.0571 (5) | |
| H5A | 0.5483 | 0.1698 | 0.3905 | 0.069* | |
| C6 | 0.47982 (11) | 0.58898 (16) | 0.37172 (13) | 0.0453 (4) | |
| O1 | 0.41059 (9) | 0.62239 (13) | 0.35012 (13) | 0.0676 (4) | |
| C7 | 0.54433 (11) | 0.67304 (14) | 0.38234 (13) | 0.0432 (4) | |
| C8 | 0.53320 (14) | 0.78598 (18) | 0.39550 (17) | 0.0602 (5) | |
| H8A | 0.4891 | 0.8084 | 0.4023 | 0.072* | |
| C9 | 0.58907 (15) | 0.86377 (16) | 0.39825 (18) | 0.0657 (6) | |
| H9A | 0.5826 | 0.9397 | 0.4062 | 0.079* | |
| C10 | 0.65408 (13) | 0.82833 (15) | 0.38923 (14) | 0.0520 (5) | |
| H10A | 0.6924 | 0.8795 | 0.3908 | 0.062* | |
| C11 | 0.66154 (11) | 0.71359 (13) | 0.37759 (12) | 0.0394 (4) | |
| N2 | 0.60753 (9) | 0.63678 (11) | 0.37358 (10) | 0.0378 (3) | |
| N3 | 0.76337 (8) | 0.36519 (10) | 0.41813 (9) | 0.0300 (3) | |
| C14 | 0.74131 (10) | 0.47290 (12) | 0.41611 (11) | 0.0314 (3) | |
| H14A | 0.7177 | 0.4935 | 0.4510 | 0.038* | |
| C15 | 0.75214 (10) | 0.55503 (12) | 0.36437 (11) | 0.0338 (3) | |
| C16 | 0.78887 (11) | 0.52392 (15) | 0.31374 (12) | 0.0419 (4) | |
| H16A | 0.7983 | 0.5770 | 0.2794 | 0.050* | |
| C17 | 0.81099 (11) | 0.41376 (15) | 0.31523 (13) | 0.0431 (4) | |
| H17A | 0.8353 | 0.3914 | 0.2815 | 0.052* | |
| C13 | 0.79703 (10) | 0.33587 (14) | 0.36711 (11) | 0.0368 (3) | |
| H13A | 0.8113 | 0.2611 | 0.3667 | 0.044* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.04854 (17) | 0.01975 (13) | 0.03224 (15) | −0.00100 (10) | 0.02548 (13) | 0.00062 (9) |
| Cl1 | 0.0554 (2) | 0.02824 (18) | 0.0347 (2) | −0.00295 (15) | 0.02439 (18) | −0.00262 (14) |
| O2 | 0.0755 (10) | 0.0343 (7) | 0.1049 (14) | −0.0040 (6) | 0.0566 (10) | 0.0174 (7) |
| C12 | 0.0487 (9) | 0.0296 (7) | 0.0459 (9) | −0.0008 (7) | 0.0230 (8) | 0.0109 (7) |
| C1 | 0.0446 (11) | 0.0549 (12) | 0.0815 (16) | −0.0138 (9) | 0.0198 (11) | −0.0136 (11) |
| C2 | 0.0344 (9) | 0.0595 (12) | 0.0661 (13) | 0.0007 (8) | 0.0149 (9) | −0.0019 (10) |
| C3 | 0.0366 (8) | 0.0426 (9) | 0.0436 (9) | 0.0033 (7) | 0.0221 (7) | 0.0027 (7) |
| C4 | 0.0371 (8) | 0.0365 (8) | 0.0390 (8) | −0.0007 (6) | 0.0177 (7) | 0.0016 (6) |
| N1 | 0.0412 (8) | 0.0358 (7) | 0.0534 (9) | 0.0007 (6) | 0.0186 (7) | 0.0041 (6) |
| C5 | 0.0498 (11) | 0.0376 (10) | 0.0752 (15) | −0.0054 (8) | 0.0266 (11) | −0.0042 (9) |
| C6 | 0.0433 (9) | 0.0466 (9) | 0.0468 (10) | 0.0112 (8) | 0.0242 (8) | 0.0031 (8) |
| O1 | 0.0517 (8) | 0.0637 (9) | 0.0945 (12) | 0.0184 (7) | 0.0432 (9) | 0.0034 (8) |
| C7 | 0.0444 (9) | 0.0361 (8) | 0.0428 (9) | 0.0093 (7) | 0.0185 (8) | 0.0022 (7) |
| C8 | 0.0609 (13) | 0.0440 (10) | 0.0716 (14) | 0.0169 (9) | 0.0318 (11) | −0.0033 (10) |
| C9 | 0.0750 (15) | 0.0305 (9) | 0.0796 (15) | 0.0102 (9) | 0.0320 (13) | −0.0070 (9) |
| C10 | 0.0630 (12) | 0.0273 (8) | 0.0548 (11) | −0.0004 (8) | 0.0233 (10) | 0.0011 (7) |
| C11 | 0.0489 (9) | 0.0264 (7) | 0.0365 (8) | 0.0033 (6) | 0.0178 (7) | 0.0052 (6) |
| N2 | 0.0430 (7) | 0.0279 (6) | 0.0397 (7) | 0.0055 (5) | 0.0196 (6) | 0.0041 (5) |
| N3 | 0.0373 (7) | 0.0248 (5) | 0.0326 (6) | 0.0011 (5) | 0.0214 (6) | 0.0023 (5) |
| C14 | 0.0374 (7) | 0.0264 (7) | 0.0343 (7) | 0.0021 (6) | 0.0213 (6) | 0.0036 (6) |
| C15 | 0.0366 (8) | 0.0284 (7) | 0.0352 (8) | −0.0024 (6) | 0.0179 (6) | 0.0052 (6) |
| C16 | 0.0462 (9) | 0.0437 (9) | 0.0407 (9) | −0.0072 (7) | 0.0262 (8) | 0.0073 (7) |
| C17 | 0.0491 (10) | 0.0495 (9) | 0.0438 (9) | −0.0021 (8) | 0.0335 (8) | −0.0011 (7) |
| C13 | 0.0428 (9) | 0.0332 (7) | 0.0394 (8) | 0.0019 (6) | 0.0251 (7) | −0.0011 (6) |
Geometric parameters (Å, °)
| Cu1—N3 | 2.0412 (12) | C7—N2 | 1.338 (2) |
| Cu1—N3i | 2.0412 (12) | C7—C8 | 1.395 (3) |
| Cu1—Cl1 | 2.3087 (4) | C8—C9 | 1.380 (3) |
| Cu1—Cl1i | 2.3087 (4) | C8—H8A | 0.9300 |
| O2—C12 | 1.215 (2) | C9—C10 | 1.369 (3) |
| C12—C15 | 1.495 (2) | C9—H9A | 0.9300 |
| C12—C11 | 1.502 (3) | C10—C11 | 1.396 (2) |
| C1—C2 | 1.371 (3) | C10—H10A | 0.9300 |
| C1—C5 | 1.376 (3) | C11—N2 | 1.339 (2) |
| C1—H1A | 0.9300 | N3—C14 | 1.3415 (18) |
| C2—C3 | 1.383 (3) | N3—C13 | 1.3438 (19) |
| C2—H2A | 0.9300 | C14—C15 | 1.3875 (19) |
| C3—C4 | 1.391 (2) | C14—H14A | 0.9300 |
| C3—C6 | 1.487 (2) | C15—C16 | 1.390 (2) |
| C4—N1 | 1.333 (2) | C16—C17 | 1.371 (2) |
| C4—H4A | 0.9300 | C16—H16A | 0.9300 |
| N1—C5 | 1.332 (2) | C17—C13 | 1.383 (2) |
| C5—H5A | 0.9300 | C17—H17A | 0.9300 |
| C6—O1 | 1.217 (2) | C13—H13A | 0.9300 |
| C6—C7 | 1.506 (3) | ||
| N3—Cu1—N3i | 180.0 | C9—C8—C7 | 118.57 (19) |
| N3—Cu1—Cl1 | 90.99 (4) | C9—C8—H8A | 120.7 |
| N3i—Cu1—Cl1 | 89.01 (4) | C7—C8—H8A | 120.7 |
| N3—Cu1—Cl1i | 89.01 (4) | C10—C9—C8 | 119.50 (18) |
| N3i—Cu1—Cl1i | 90.99 (4) | C10—C9—H9A | 120.2 |
| Cl1—Cu1—Cl1i | 180.0 | C8—C9—H9A | 120.2 |
| O2—C12—C15 | 118.88 (17) | C9—C10—C11 | 118.42 (19) |
| O2—C12—C11 | 119.02 (16) | C9—C10—H10A | 120.8 |
| C15—C12—C11 | 122.10 (14) | C11—C10—H10A | 120.8 |
| C2—C1—C5 | 118.40 (19) | N2—C11—C10 | 123.12 (17) |
| C2—C1—H1A | 120.8 | N2—C11—C12 | 119.14 (14) |
| C5—C1—H1A | 120.8 | C10—C11—C12 | 117.71 (16) |
| C1—C2—C3 | 119.45 (18) | C7—N2—C11 | 117.58 (14) |
| C1—C2—H2A | 120.3 | C14—N3—C13 | 118.19 (13) |
| C3—C2—H2A | 120.3 | C14—N3—Cu1 | 120.94 (10) |
| C2—C3—C4 | 117.64 (17) | C13—N3—Cu1 | 120.84 (10) |
| C2—C3—C6 | 119.12 (16) | N3—C14—C15 | 123.02 (14) |
| C4—C3—C6 | 123.23 (16) | N3—C14—H14A | 118.5 |
| N1—C4—C3 | 123.46 (16) | C15—C14—H14A | 118.5 |
| N1—C4—H4A | 118.3 | C14—C15—C16 | 118.09 (14) |
| C3—C4—H4A | 118.3 | C14—C15—C12 | 123.33 (14) |
| C5—N1—C4 | 116.97 (16) | C16—C15—C12 | 118.41 (14) |
| N1—C5—C1 | 123.86 (18) | C17—C16—C15 | 118.97 (14) |
| N1—C5—H5A | 118.1 | C17—C16—H16A | 120.5 |
| C1—C5—H5A | 118.1 | C15—C16—H16A | 120.5 |
| O1—C6—C3 | 120.78 (18) | C16—C17—C13 | 119.84 (15) |
| O1—C6—C7 | 118.89 (17) | C16—C17—H17A | 120.1 |
| C3—C6—C7 | 120.22 (15) | C13—C17—H17A | 120.1 |
| N2—C7—C8 | 122.80 (18) | N3—C13—C17 | 121.86 (15) |
| N2—C7—C6 | 118.31 (15) | N3—C13—H13A | 119.1 |
| C8—C7—C6 | 118.79 (17) | C17—C13—H13A | 119.1 |
| C5—C1—C2—C3 | −1.2 (4) | O2—C12—C11—C10 | −7.4 (3) |
| C1—C2—C3—C4 | −2.9 (3) | C15—C12—C11—C10 | 172.79 (16) |
| C1—C2—C3—C6 | 176.4 (2) | C8—C7—N2—C11 | −0.2 (3) |
| C2—C3—C4—N1 | 5.2 (3) | C6—C7—N2—C11 | 176.08 (15) |
| C6—C3—C4—N1 | −174.07 (17) | C10—C11—N2—C7 | −0.8 (3) |
| C3—C4—N1—C5 | −3.0 (3) | C12—C11—N2—C7 | −178.81 (15) |
| C4—N1—C5—C1 | −1.6 (3) | Cl1—Cu1—N3—C14 | 136.92 (12) |
| C2—C1—C5—N1 | 3.7 (4) | Cl1i—Cu1—N3—C14 | −43.08 (12) |
| C2—C3—C6—O1 | 30.2 (3) | Cl1—Cu1—N3—C13 | −45.23 (12) |
| C4—C3—C6—O1 | −150.5 (2) | Cl1i—Cu1—N3—C13 | 134.77 (12) |
| C2—C3—C6—C7 | −145.85 (19) | C13—N3—C14—C15 | −0.4 (2) |
| C4—C3—C6—C7 | 33.5 (3) | Cu1—N3—C14—C15 | 177.50 (11) |
| O1—C6—C7—N2 | −157.20 (19) | N3—C14—C15—C16 | −1.1 (2) |
| C3—C6—C7—N2 | 18.9 (3) | N3—C14—C15—C12 | −176.31 (15) |
| O1—C6—C7—C8 | 19.2 (3) | O2—C12—C15—C14 | 146.67 (19) |
| C3—C6—C7—C8 | −164.64 (18) | C11—C12—C15—C14 | −33.5 (2) |
| N2—C7—C8—C9 | 1.0 (3) | O2—C12—C15—C16 | −28.5 (3) |
| C6—C7—C8—C9 | −175.3 (2) | C11—C12—C15—C16 | 151.27 (16) |
| C7—C8—C9—C10 | −0.8 (4) | C14—C15—C16—C17 | 1.5 (2) |
| C8—C9—C10—C11 | −0.1 (3) | C12—C15—C16—C17 | 176.90 (16) |
| C9—C10—C11—N2 | 0.9 (3) | C15—C16—C17—C13 | −0.4 (3) |
| C9—C10—C11—C12 | 178.98 (19) | C14—N3—C13—C17 | 1.6 (2) |
| O2—C12—C11—N2 | 170.73 (18) | Cu1—N3—C13—C17 | −176.35 (13) |
| C15—C12—C11—N2 | −9.1 (2) | C16—C17—C13—N3 | −1.2 (3) |
Symmetry codes: (i) −x+3/2, −y+1/2, −z+1.
Hydrogen-bond geometry (Å, °)
| Cg1 is the centroid of the C13–C17,N3 ring. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C13—H13A···O1ii | 0.93 | 2.61 | 3.418 (2) | 146 |
| C2—H2A···Cg1iii | 0.93 | 2.73 | 3.621 (3) | 162 |
Symmetry codes: (ii) x+1/2, y−1/2, z; (iii) −x+1, y, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZQ2102).
References
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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/S1600536811017685/zq2102sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811017685/zq2102Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


