Abstract
In the mixed-valence CuI/CuII coordination polymer, [Cu2Cl3(C20H14N4)]n, the two Cu atoms are bridged to a pair of Cl atoms across a centre of inversion. The monovalent metal atoms is coordinated by a pyridine N atom as well as by three Cl atoms in a tetrahedral CuNCl3 geometry. The divalent metal atom is N,N′,N′′-chelated by the heterocycle, and it exists in a square-pyramidal CuN3Cl2 geometry; the apical site is occupied by the second bridging Cl atom. The bridging modes of the Cl atoms and the heterocycle give rise to the formation of a layered arrangement parallel to (001).
Related literature
For related structures, see: Hou et al. (2005 ▶); Zhang et al. (2007 ▶)
Experimental
Crystal data
[Cu2Cl3(C20H14N4)]
M r = 543.78
Triclinic,
a = 8.1389 (8) Å
b = 9.8161 (10) Å
c = 12.4823 (13) Å
α = 79.512 (2)°
β = 85.036 (2)°
γ = 88.202 (2)°
V = 976.78 (17) Å3
Z = 2
Mo Kα radiation
μ = 2.60 mm−1
T = 294 K
0.15 × 0.12 × 0.10 mm
Data collection
Bruker SMART diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.694, T max = 0.771
7840 measured reflections
3778 independent reflections
3391 reflections with I > 2σ(I)
R int = 0.014
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.072
S = 1.06
3778 reflections
262 parameters
H-atom parameters constrained
Δρmax = 0.40 e Å−3
Δρmin = −0.34 e Å−3
Data collection: SMART (Bruker, 1998 ▶); cell refinement: SAINT (Bruker, 1998 ▶); 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 datablocks I, global. DOI: 10.1107/S1600536811014759/ng5143sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014759/ng5143Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
supplementary crystallographic information
Comment
Terpyridine and its derivatives have been receiving rapidly increasing attention recently not only because of their versatility as building blocks in supramolecular assembles, but also due to the interesting electronic, photonic and magnetic properties of their transition metal complexes.
4'-(4-Pyridyl)-2,2':6'2''-terpyridine(pyterpy) belongs to this group of ligands and has usually been used to construct a great variety of structurally interesting entities, such as ribbon-type coordination polymers (Hou et al., 2005) and self-catenated networks (Zhang et al., 2007).
The structure of the title compound (I) is shown in Fig. 1. Single-crystal X-ray diffraction shows that the asymmetric unit contains two Cu crystallographically nonequivalent atoms. The Cu1 atom has a distorted square-pyramidal coordination formed by three N atoms of tridentate 4'-(4-pyridyl)-2,2':6'2''-terpyridine (pyterpy) ligand and two Cl atoms. The Cu2 atom is coordinated by one N atom from the pendent monodentate pyridine of pyterpy as well as by three Cl atoms, conferring a tetrahedral coordination geometry. The two terpy ligands in a transoid arrangement link Cu1 and Cu2 atoms, to form a mixed-valence tetrameric M4L4 rectangular unit with a separation of 11.017 Å, which is smaller than those in reported ribbon-type compounds, and then linked by a Cu2Cl2 cluster, leading to the formation of an infinite 1-D coordination polymer (Fig. 2).
Experimental
The mixture of CuCl (0.020 g, 0.2 mmol), 4'-(4-pyridyl)-2,2':6'2''-terpyridine (pyterpy) (0.062 g, 0.1 mmol), and acetonitrile (6 ml) were placed and sealed in a 15 ml Teflon-lined stainless steel reactor and heated to 180 °C for 72 h, then cooled down to room temperature at a rate of 2 °C/ 20 min. Single crystals suitable for X-ray diffraction were obtained in the form of black bars in ca 20% yield.
Refinement
H atoms were positioned geometrically and refined using a riding model, with C—H = 0.93 Å (aromatic) and Uiso(H) = 1.2Ueq(C)
Figures
Fig. 1.
The asymmetric unit of the title compound.
Fig. 2.
The 1-D zigzag chain structure of the title compoud.
Crystal data
| [Cu2Cl3(C20H14N4)] | Z = 2 |
| Mr = 543.78 | F(000) = 542 |
| Triclinic, P1 | Dx = 1.849 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 8.1389 (8) Å | Cell parameters from 1056 reflections |
| b = 9.8161 (10) Å | θ = 2.4–26.0° |
| c = 12.4823 (13) Å | µ = 2.60 mm−1 |
| α = 79.512 (2)° | T = 294 K |
| β = 85.036 (2)° | Block, black |
| γ = 88.202 (2)° | 0.15 × 0.12 × 0.10 mm |
| V = 976.78 (17) Å3 |
Data collection
| Bruker SMART diffractometer | 3778 independent reflections |
| Radiation source: fine-focus sealed tube | 3391 reflections with I > 2σ(I) |
| graphite | Rint = 0.014 |
| φ and ω scans | θmax = 26.0°, θmin = 2.1° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −10→9 |
| Tmin = 0.694, Tmax = 0.771 | k = −12→12 |
| 7840 measured reflections | l = −15→15 |
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)] = 0.027 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.072 | H-atom parameters constrained |
| S = 1.06 | w = 1/[σ2(Fo2) + (0.0383P)2 + 0.3983P] where P = (Fo2 + 2Fc2)/3 |
| 3778 reflections | (Δ/σ)max = 0.002 |
| 262 parameters | Δρmax = 0.40 e Å−3 |
| 0 restraints | Δρmin = −0.34 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 | ||
| Cu1 | 1.55686 (3) | 0.36696 (3) | −0.35707 (2) | 0.02849 (9) | |
| Cu2 | 1.49349 (3) | 0.14312 (3) | −0.05428 (3) | 0.04087 (10) | |
| Cl1 | 1.36557 (7) | −0.05058 (6) | −0.10452 (5) | 0.03600 (14) | |
| Cl3 | 1.68201 (7) | 0.25884 (6) | −0.18347 (5) | 0.03968 (15) | |
| Cl2 | 1.73952 (7) | 0.30031 (7) | −0.48213 (5) | 0.04485 (16) | |
| C16 | 0.4539 (2) | 0.3584 (2) | 0.30399 (17) | 0.0271 (4) | |
| N2 | 0.6324 (2) | 0.54582 (18) | 0.28869 (14) | 0.0266 (4) | |
| N4 | 1.2937 (2) | 0.24557 (19) | 0.00438 (16) | 0.0332 (4) | |
| N3 | 0.3521 (2) | 0.43980 (19) | 0.35802 (14) | 0.0299 (4) | |
| N1 | 0.6210 (2) | 0.77686 (18) | 0.35354 (14) | 0.0288 (4) | |
| C11 | 1.3087 (3) | 0.3651 (2) | 0.03817 (19) | 0.0333 (5) | |
| H11 | 1.4103 | 0.4084 | 0.0239 | 0.040* | |
| C15 | 0.6150 (2) | 0.4212 (2) | 0.26284 (17) | 0.0265 (4) | |
| C14 | 0.7417 (2) | 0.3610 (2) | 0.20518 (17) | 0.0282 (4) | |
| H14 | 0.7274 | 0.2755 | 0.1854 | 0.034* | |
| C9 | 1.0297 (2) | 0.3681 (2) | 0.11560 (17) | 0.0273 (4) | |
| C8 | 0.8918 (2) | 0.4302 (2) | 0.17696 (17) | 0.0260 (4) | |
| C6 | 0.7742 (2) | 0.6135 (2) | 0.26509 (17) | 0.0270 (4) | |
| C7 | 0.9077 (2) | 0.5576 (2) | 0.20962 (17) | 0.0286 (4) | |
| H7 | 1.0068 | 0.6047 | 0.1944 | 0.034* | |
| C10 | 1.1832 (3) | 0.4291 (2) | 0.09312 (19) | 0.0324 (5) | |
| H10 | 1.2014 | 0.5126 | 0.1150 | 0.039* | |
| C1 | 0.6025 (3) | 0.8956 (2) | 0.39099 (19) | 0.0355 (5) | |
| H1 | 0.5002 | 0.9170 | 0.4237 | 0.043* | |
| C3 | 0.8787 (3) | 0.9570 (3) | 0.3336 (2) | 0.0464 (6) | |
| H3 | 0.9655 | 1.0182 | 0.3272 | 0.056* | |
| C18 | 0.2576 (3) | 0.1787 (3) | 0.3369 (2) | 0.0415 (6) | |
| H18 | 0.2260 | 0.0904 | 0.3308 | 0.050* | |
| C4 | 0.9006 (3) | 0.8347 (2) | 0.2933 (2) | 0.0404 (6) | |
| H4 | 1.0018 | 0.8122 | 0.2598 | 0.049* | |
| C5 | 0.7688 (3) | 0.7472 (2) | 0.30392 (17) | 0.0286 (4) | |
| C17 | 0.4102 (3) | 0.2284 (2) | 0.29147 (19) | 0.0335 (5) | |
| H17 | 0.4816 | 0.1749 | 0.2532 | 0.040* | |
| C2 | 0.7283 (3) | 0.9875 (3) | 0.3832 (2) | 0.0411 (6) | |
| H2 | 0.7120 | 1.0691 | 0.4109 | 0.049* | |
| C13 | 1.0125 (3) | 0.2455 (3) | 0.0776 (2) | 0.0465 (7) | |
| H13 | 0.9113 | 0.2014 | 0.0886 | 0.056* | |
| C20 | 0.2040 (3) | 0.3911 (3) | 0.40001 (19) | 0.0368 (5) | |
| H20 | 0.1330 | 0.4468 | 0.4364 | 0.044* | |
| C19 | 0.1529 (3) | 0.2610 (3) | 0.3913 (2) | 0.0420 (6) | |
| H19 | 0.0496 | 0.2296 | 0.4216 | 0.050* | |
| C12 | 1.1452 (3) | 0.1887 (3) | 0.0232 (2) | 0.0480 (7) | |
| H12 | 1.1300 | 0.1065 | −0.0014 | 0.058* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.02035 (14) | 0.03193 (16) | 0.03487 (16) | 0.00211 (10) | 0.00583 (10) | −0.01466 (11) |
| Cu2 | 0.02869 (16) | 0.04265 (18) | 0.0509 (2) | 0.00035 (12) | 0.01106 (13) | −0.01440 (14) |
| Cl1 | 0.0362 (3) | 0.0355 (3) | 0.0399 (3) | −0.0021 (2) | −0.0025 (2) | −0.0165 (2) |
| Cl3 | 0.0261 (3) | 0.0494 (3) | 0.0401 (3) | −0.0083 (2) | 0.0011 (2) | 0.0003 (3) |
| Cl2 | 0.0350 (3) | 0.0568 (4) | 0.0461 (3) | 0.0020 (3) | 0.0134 (2) | −0.0265 (3) |
| C16 | 0.0199 (10) | 0.0300 (11) | 0.0308 (11) | 0.0016 (8) | 0.0031 (8) | −0.0069 (9) |
| N2 | 0.0191 (8) | 0.0270 (9) | 0.0340 (9) | 0.0018 (7) | 0.0035 (7) | −0.0092 (7) |
| N4 | 0.0229 (9) | 0.0345 (10) | 0.0428 (11) | 0.0016 (7) | 0.0081 (8) | −0.0140 (8) |
| N3 | 0.0234 (9) | 0.0323 (10) | 0.0334 (10) | 0.0012 (7) | 0.0061 (7) | −0.0085 (8) |
| N1 | 0.0244 (9) | 0.0311 (9) | 0.0335 (9) | 0.0033 (7) | −0.0003 (7) | −0.0143 (8) |
| C11 | 0.0208 (10) | 0.0339 (12) | 0.0455 (13) | −0.0020 (9) | 0.0067 (9) | −0.0120 (10) |
| C15 | 0.0211 (10) | 0.0263 (10) | 0.0319 (11) | 0.0001 (8) | 0.0028 (8) | −0.0073 (8) |
| C14 | 0.0228 (10) | 0.0270 (10) | 0.0359 (11) | −0.0002 (8) | 0.0051 (8) | −0.0121 (9) |
| C9 | 0.0217 (10) | 0.0289 (11) | 0.0315 (11) | 0.0030 (8) | 0.0033 (8) | −0.0092 (9) |
| C8 | 0.0211 (10) | 0.0285 (11) | 0.0291 (10) | 0.0023 (8) | 0.0016 (8) | −0.0094 (8) |
| C6 | 0.0203 (10) | 0.0284 (11) | 0.0331 (11) | 0.0024 (8) | 0.0015 (8) | −0.0099 (9) |
| C7 | 0.0199 (10) | 0.0309 (11) | 0.0365 (12) | −0.0011 (8) | 0.0035 (8) | −0.0125 (9) |
| C10 | 0.0235 (11) | 0.0306 (11) | 0.0452 (13) | −0.0013 (9) | 0.0034 (9) | −0.0149 (10) |
| C1 | 0.0316 (12) | 0.0363 (12) | 0.0416 (13) | 0.0062 (10) | 0.0012 (10) | −0.0184 (10) |
| C3 | 0.0365 (13) | 0.0401 (14) | 0.0682 (18) | −0.0090 (11) | −0.0012 (12) | −0.0244 (13) |
| C18 | 0.0294 (12) | 0.0366 (13) | 0.0583 (16) | −0.0068 (10) | 0.0024 (11) | −0.0096 (11) |
| C4 | 0.0261 (11) | 0.0393 (13) | 0.0595 (15) | −0.0017 (10) | 0.0031 (10) | −0.0213 (12) |
| C5 | 0.0238 (10) | 0.0294 (11) | 0.0342 (11) | 0.0038 (8) | −0.0005 (8) | −0.0117 (9) |
| C17 | 0.0232 (11) | 0.0334 (12) | 0.0444 (13) | −0.0002 (9) | 0.0043 (9) | −0.0115 (10) |
| C2 | 0.0433 (14) | 0.0348 (13) | 0.0504 (14) | 0.0015 (10) | −0.0019 (11) | −0.0231 (11) |
| C13 | 0.0246 (11) | 0.0452 (14) | 0.0749 (18) | −0.0108 (10) | 0.0186 (11) | −0.0334 (13) |
| C20 | 0.0240 (11) | 0.0434 (13) | 0.0411 (13) | 0.0019 (10) | 0.0092 (9) | −0.0087 (10) |
| C19 | 0.0225 (11) | 0.0462 (14) | 0.0538 (15) | −0.0075 (10) | 0.0082 (10) | −0.0044 (12) |
| C12 | 0.0326 (13) | 0.0413 (14) | 0.0762 (19) | −0.0075 (11) | 0.0179 (12) | −0.0361 (13) |
Geometric parameters (Å, °)
| Cu1—N2i | 1.9466 (16) | C14—H14 | 0.9300 |
| Cu1—N1i | 2.0455 (18) | C9—C10 | 1.387 (3) |
| Cu1—N3i | 2.0557 (18) | C9—C13 | 1.387 (3) |
| Cu1—Cl2 | 2.2325 (6) | C9—C8 | 1.483 (3) |
| Cu1—Cl3 | 2.5172 (6) | C8—C7 | 1.397 (3) |
| Cu2—N4 | 2.0374 (18) | C6—C7 | 1.390 (3) |
| Cu2—Cl3 | 2.2933 (6) | C6—C5 | 1.478 (3) |
| Cu2—Cl1ii | 2.3964 (7) | C7—H7 | 0.9300 |
| Cu2—Cl1 | 2.4007 (6) | C10—H10 | 0.9300 |
| Cu2—Cu2ii | 2.8917 (7) | C1—C2 | 1.371 (3) |
| Cl1—Cu2ii | 2.3964 (7) | C1—H1 | 0.9300 |
| C16—N3 | 1.355 (3) | C3—C2 | 1.373 (3) |
| C16—C17 | 1.375 (3) | C3—C4 | 1.385 (3) |
| C16—C15 | 1.477 (3) | C3—H3 | 0.9300 |
| N2—C6 | 1.333 (3) | C18—C19 | 1.377 (3) |
| N2—C15 | 1.335 (3) | C18—C17 | 1.385 (3) |
| N2—Cu1i | 1.9466 (16) | C18—H18 | 0.9300 |
| N4—C11 | 1.330 (3) | C4—C5 | 1.377 (3) |
| N4—C12 | 1.332 (3) | C4—H4 | 0.9300 |
| N3—C20 | 1.339 (3) | C17—H17 | 0.9300 |
| N3—Cu1i | 2.0557 (18) | C2—H2 | 0.9300 |
| N1—C1 | 1.332 (3) | C13—C12 | 1.382 (3) |
| N1—C5 | 1.353 (3) | C13—H13 | 0.9300 |
| N1—Cu1i | 2.0455 (18) | C20—C19 | 1.381 (3) |
| C11—C10 | 1.380 (3) | C20—H20 | 0.9300 |
| C11—H11 | 0.9300 | C19—H19 | 0.9300 |
| C15—C14 | 1.385 (3) | C12—H12 | 0.9300 |
| C14—C8 | 1.403 (3) | ||
| N2i—Cu1—N1i | 78.97 (7) | C10—C9—C8 | 121.92 (19) |
| N2i—Cu1—N3i | 79.19 (7) | C13—C9—C8 | 121.8 (2) |
| N1i—Cu1—N3i | 156.19 (7) | C7—C8—C14 | 118.17 (18) |
| N2i—Cu1—Cl2 | 162.20 (6) | C7—C8—C9 | 121.33 (19) |
| N1i—Cu1—Cl2 | 99.27 (5) | C14—C8—C9 | 120.49 (19) |
| N3i—Cu1—Cl2 | 98.61 (5) | N2—C6—C7 | 120.70 (19) |
| N2i—Cu1—Cl3 | 96.91 (5) | N2—C6—C5 | 112.78 (17) |
| N1i—Cu1—Cl3 | 97.93 (5) | C7—C6—C5 | 126.51 (19) |
| N3i—Cu1—Cl3 | 93.99 (5) | C6—C7—C8 | 119.42 (19) |
| Cl2—Cu1—Cl3 | 100.87 (2) | C6—C7—H7 | 120.3 |
| N4—Cu2—Cl3 | 120.37 (6) | C8—C7—H7 | 120.3 |
| N4—Cu2—Cl1ii | 104.34 (6) | C11—C10—C9 | 119.6 (2) |
| Cl3—Cu2—Cl1ii | 107.93 (2) | C11—C10—H10 | 120.2 |
| N4—Cu2—Cl1 | 101.32 (6) | C9—C10—H10 | 120.2 |
| Cl3—Cu2—Cl1 | 115.66 (2) | N1—C1—C2 | 122.6 (2) |
| Cl1ii—Cu2—Cl1 | 105.86 (2) | N1—C1—H1 | 118.7 |
| N4—Cu2—Cu2ii | 111.61 (6) | C2—C1—H1 | 118.7 |
| Cl3—Cu2—Cu2ii | 127.92 (2) | C2—C3—C4 | 119.6 (2) |
| Cl1ii—Cu2—Cu2ii | 52.998 (16) | C2—C3—H3 | 120.2 |
| Cl1—Cu2—Cu2ii | 52.861 (18) | C4—C3—H3 | 120.2 |
| Cu2ii—Cl1—Cu2 | 74.14 (2) | C19—C18—C17 | 119.5 (2) |
| Cu2—Cl3—Cu1 | 112.90 (2) | C19—C18—H18 | 120.2 |
| N3—C16—C17 | 122.26 (19) | C17—C18—H18 | 120.2 |
| N3—C16—C15 | 113.85 (18) | C5—C4—C3 | 118.4 (2) |
| C17—C16—C15 | 123.88 (18) | C5—C4—H4 | 120.8 |
| C6—N2—C15 | 121.47 (17) | C3—C4—H4 | 120.8 |
| C6—N2—Cu1i | 119.54 (14) | N1—C5—C4 | 121.9 (2) |
| C15—N2—Cu1i | 118.95 (14) | N1—C5—C6 | 113.76 (18) |
| C11—N4—C12 | 116.29 (19) | C4—C5—C6 | 124.37 (19) |
| C11—N4—Cu2 | 121.51 (15) | C16—C17—C18 | 118.6 (2) |
| C12—N4—Cu2 | 121.71 (15) | C16—C17—H17 | 120.7 |
| C20—N3—C16 | 118.36 (19) | C18—C17—H17 | 120.7 |
| C20—N3—Cu1i | 127.42 (15) | C1—C2—C3 | 118.8 (2) |
| C16—N3—Cu1i | 114.11 (14) | C1—C2—H2 | 120.6 |
| C1—N1—C5 | 118.65 (19) | C3—C2—H2 | 120.6 |
| C1—N1—Cu1i | 126.56 (15) | C12—C13—C9 | 120.2 (2) |
| C5—N1—Cu1i | 114.75 (14) | C12—C13—H13 | 119.9 |
| N4—C11—C10 | 124.2 (2) | C9—C13—H13 | 119.9 |
| N4—C11—H11 | 117.9 | N3—C20—C19 | 122.4 (2) |
| C10—C11—H11 | 117.9 | N3—C20—H20 | 118.8 |
| N2—C15—C14 | 120.84 (19) | C19—C20—H20 | 118.8 |
| N2—C15—C16 | 113.24 (17) | C18—C19—C20 | 118.9 (2) |
| C14—C15—C16 | 125.90 (19) | C18—C19—H19 | 120.6 |
| C15—C14—C8 | 119.30 (19) | C20—C19—H19 | 120.6 |
| C15—C14—H14 | 120.4 | N4—C12—C13 | 123.4 (2) |
| C8—C14—H14 | 120.4 | N4—C12—H12 | 118.3 |
| C10—C9—C13 | 116.26 (19) | C13—C12—H12 | 118.3 |
Symmetry codes: (i) −x+2, −y+1, −z; (ii) −x+3, −y, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5143).
References
- Bruker (1998). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- Hou, L., Li, D., Shi, W.-J., Yin, Y.-G. & Ng, S. W. (2005). Inorg. Chem. 44, 7825–7832. [DOI] [PubMed]
- Sheldrick, G. M. (1996). University of Göttingen, Germany.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Zhang, S.-S., Zhan, S.-Z., Li, M., Peng, R. & Li, D. (2007). Inorg. Chem. 46, 4365–4367. [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/S1600536811014759/ng5143sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014759/ng5143Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


