Abstract
In the title salt, (C12H20N2)[CuCl4], the CuII atom occupies a general position in a flattened tetrahedral environment by Cl ligands, characterized by Cl—Cu—Cl angles of 134.04 (3) and 137.18 (4)°. The six-membered piperazinediium ring adopts a chair conformation. The organic cation and inorganic anion interact through N—H⋯Cl and C—H⋯Cl hydrogen bonds, forming a three-dimensional network.
Related literature
For general background to the properties of tetrahalidocuprate(II) compounds, see: Solomon et al. (1992 ▶); Kim et al. (2001 ▶); Panja et al. (2005 ▶); Lee et al. (2004 ▶); Turnbull et al. (2005 ▶); Shapiro et al. (2007 ▶). For general background to the geometry of the tetrahalidocuprate(II) species, see: Halvorson et al. (1990 ▶). For puckering parameters, see: Cremer & Pople (1975 ▶).
Experimental
Crystal data
(C12H20N2)[CuCl4]
M r = 397.64
Triclinic,
a = 7.1986 (15) Å
b = 7.7611 (11) Å
c = 15.635 (4) Å
α = 77.035 (16)°
β = 79.311 (19)°
γ = 81.845 (14)°
V = 831.9 (3) Å3
Z = 2
Ag Kα radiation
λ = 0.56087 Å
μ = 1.01 mm−1
T = 293 K
0.25 × 0.20 × 0.15 mm
Data collection
Nonius MACH-3 diffractometer
Absorption correction: part of the refinement model (ΔF) (Walker & Stuart, 1983 ▶) T min = 0.786, T max = 0.863
9228 measured reflections
8079 independent reflections
4600 reflections with I > 2σ(I)
R int = 0.020
2 standard reflections every 120 min intensity decay: 7%
Refinement
R[F 2 > 2σ(F 2)] = 0.050
wR(F 2) = 0.129
S = 1.00
8079 reflections
172 parameters
H-atom parameters constrained
Δρmax = 0.87 e Å−3
Δρmin = −0.68 e Å−3
Data collection: CAD-4 EXPRESS (Enraf–Nonius, 1994 ▶); cell refinement: CAD-4 EXPRESS; data reduction: XCAD4 (Harms & Wocadlo, 1996 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012 ▶); software used to prepare material for publication: WinGX (Farrugia, 2012 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536813021454/ru2053sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813021454/ru2053Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1⋯Cl3i | 0.91 | 2.48 | 3.1610 (18) | 132 |
| N2—H2A⋯Cl2ii | 0.90 | 2.35 | 3.144 (2) | 147 |
| N2—H2B⋯Cl1iii | 0.90 | 2.30 | 3.152 (2) | 159 |
| N2—H2B⋯Cl2iii | 0.90 | 2.80 | 3.271 (2) | 114 |
| C2—H2D⋯Cl1i | 0.97 | 2.74 | 3.666 (3) | 159 |
| C3—H3B⋯Cl1iv | 0.97 | 2.78 | 3.585 (2) | 141 |
| C4—H4B⋯Cl4ii | 0.97 | 2.66 | 3.616 (2) | 168 |
| C6—H6⋯Cl4ii | 0.93 | 2.71 | 3.572 (2) | 154 |
| C12—H12C⋯Cl3i | 0.96 | 2.71 | 3.568 (3) | 149 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
.
Acknowledgments
This work was supported by the Tunisian Ministry of HEScR.
supplementary crystallographic information
1. Comment
Cuprates are chemical compounds in which copper forms complex anions where the overall charge is negative. In such complexes, the ligands are generally cyanides, hydroxides or halides. Due to their important properties, the cuprates still constitute a research axis in many laboratories (Solomon et al., 1992; Kim et al., 2001; Lee et al., 2004; Panja et al., 2005; Turnbull et al., 2005; Shapiro et al., 2007). We report here synthesis and crystal structure of a new cuprate, (C12H20N2)[CuCl4] (I). Crystal structure of (I) gives another illustration of this type of material. The asymmetric unit within the unit cell is build of one tetrahedral [CuCl4]2- anion and one 1-(2,3-dimethylphenyl)piperazine-1,4-diium cation (Fig. 1). The copper(II) anion exhibits a coordination geometry intermediate between tetrahedral and square–planar. However we can tell that the configuration adopted by this anion is a flattened tetrahedral where the two trans bond angles, Cl(1)—Cu—Cl(4) = 137.18 (4)° and Cl(2)—Cu—Cl(3) = 134.04 (3)°, are very near to the minimum of the potential curve describing the angular deformation of isolated [CuCl4]2- anion (θ min = 135.95°) (Halvorson et al., 1990). The phenyl ring (C5—C10) of 1-(2,3-dimethylphenyl)piperazine-1,4-diium is planar with an r.m.s. deviation of 0.0111. The 6-membered piperazinium ring adopts a chair conformation, with puckering parameters (Cremer & Pople, 1975) QT = 0.581 (2) Å, θ = 5.3 (2)° and φ = 328 (3)°. The dihedral angle between the piperazine (N1–N2/C1–C4) ring and the benzene (C5–C10) ring is 65.41 (7) °. In the crystal, neighboring molecules are linked by N—H···Cl and C—H···Cl hydrogen bonds, forming a three-dimensional network (Figure 2).
2. Experimental
To an aqueous solution (10 ml) of HCl (0.2M) was added 1-(2,3-dimethylphenyl)piperazine (0.19 g, 1 mmol). To the obtained solution, a blue aqueous solution (10 ml) of CuCl2.6H2O (0.170 g, 1 mmol) was added slowly with stirring. The resulting solution was submitted to a slow evaporation at room temperature until the formation of yellow crystals of the title compound.
3. Refinement
H atoms were placed in their calculated positions and then refined using the riding model with atom-H lengths of 0.93 Å (CH), 0.97 Å (CH2), 0.96 Å (CH3), 0.91 Å (NH) and 0.90 Å (NH3). Uiso were set to 1.2 (CH, CH2), 1.5 (CH3) or 1.20 (NH) times Ueq of the parent atom.
Figures
Fig. 1.
The molecular structure of (I) with 50% probability displacement ellipsoids. Dashed lines indicate C—H···Cl.
Fig. 2.
Perspective view of the three-dimensional network of (I), showing the intermolecular hydrogen bonds (dashed solid lines) interactions.
Crystal data
| (C12H20N2)[CuCl4] | Z = 2 |
| Mr = 397.64 | F(000) = 406 |
| Triclinic, P1 | Dx = 1.588 Mg m−3 |
| Hall symbol: -P 1 | Ag Kα radiation, λ = 0.56087 Å |
| a = 7.1986 (15) Å | Cell parameters from 25 reflections |
| b = 7.7611 (11) Å | θ = 9.0–10.7° |
| c = 15.635 (4) Å | µ = 1.01 mm−1 |
| α = 77.035 (16)° | T = 293 K |
| β = 79.311 (19)° | Prism, yellow |
| γ = 81.845 (14)° | 0.25 × 0.20 × 0.15 mm |
| V = 831.9 (3) Å3 |
Data collection
| Nonius MACH-3 diffractometer | 4600 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.020 |
| Graphite monochromator | θmax = 28.0°, θmin = 2.1° |
| non–profiled ω scans | h = −12→11 |
| Absorption correction: part of the refinement model (ΔF) (Walker & Stuart, 1983) | k = −12→12 |
| Tmin = 0.786, Tmax = 0.863 | l = −26→2 |
| 9228 measured reflections | 2 standard reflections every 120 min |
| 8079 independent reflections | intensity decay: 7% |
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)] = 0.050 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.129 | H-atom parameters constrained |
| S = 1.00 | w = 1/[σ2(Fo2) + (0.0614P)2 + 0.0435P] where P = (Fo2 + 2Fc2)/3 |
| 8079 reflections | (Δ/σ)max < 0.001 |
| 172 parameters | Δρmax = 0.87 e Å−3 |
| 0 restraints | Δρmin = −0.68 e Å−3 |
| 0 constraints |
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 | 0.28980 (4) | 0.31174 (4) | 0.166012 (19) | 0.03259 (8) | |
| Cl3 | 0.56150 (8) | 0.21183 (7) | 0.22023 (4) | 0.03825 (13) | |
| Cl2 | 0.20878 (9) | 0.53035 (8) | 0.05406 (4) | 0.04152 (14) | |
| Cl1 | 0.27357 (11) | 0.07141 (8) | 0.10849 (5) | 0.04717 (16) | |
| Cl4 | 0.13588 (11) | 0.43179 (10) | 0.27862 (5) | 0.05472 (19) | |
| N1 | 0.6470 (2) | 0.7932 (2) | 0.25996 (11) | 0.0256 (3) | |
| H1 | 0.5611 | 0.8853 | 0.2411 | 0.031* | |
| C5 | 0.6198 (3) | 0.7639 (3) | 0.35900 (14) | 0.0287 (4) | |
| C10 | 0.4411 (3) | 0.8116 (3) | 0.40409 (15) | 0.0307 (4) | |
| C4 | 0.8414 (3) | 0.8412 (3) | 0.21292 (15) | 0.0298 (4) | |
| H4A | 0.8718 | 0.9435 | 0.2317 | 0.036* | |
| H4B | 0.9365 | 0.7426 | 0.2283 | 0.036* | |
| N2 | 0.7973 (3) | 0.7293 (3) | 0.08360 (13) | 0.0342 (4) | |
| H2A | 0.8894 | 0.6389 | 0.0928 | 0.041* | |
| H2B | 0.7938 | 0.7594 | 0.0248 | 0.041* | |
| C9 | 0.4213 (3) | 0.7840 (3) | 0.49714 (16) | 0.0342 (5) | |
| C1 | 0.6039 (3) | 0.6330 (3) | 0.23052 (15) | 0.0337 (4) | |
| H1A | 0.4785 | 0.6019 | 0.2598 | 0.040* | |
| H1B | 0.6956 | 0.5328 | 0.2479 | 0.040* | |
| C2 | 0.6112 (3) | 0.6693 (3) | 0.13116 (16) | 0.0359 (5) | |
| H2C | 0.5914 | 0.5621 | 0.1135 | 0.043* | |
| H2D | 0.5098 | 0.7603 | 0.1146 | 0.043* | |
| C6 | 0.7721 (3) | 0.6850 (3) | 0.40122 (16) | 0.0365 (5) | |
| H6 | 0.8884 | 0.6514 | 0.3688 | 0.044* | |
| C3 | 0.8434 (3) | 0.8834 (3) | 0.11406 (15) | 0.0337 (4) | |
| H3A | 0.7513 | 0.9847 | 0.0988 | 0.040* | |
| H3B | 0.9680 | 0.9148 | 0.0839 | 0.040* | |
| C7 | 0.7467 (4) | 0.6570 (4) | 0.49343 (17) | 0.0436 (6) | |
| H7 | 0.8462 | 0.6033 | 0.5238 | 0.052* | |
| C8 | 0.5736 (4) | 0.7093 (3) | 0.53963 (17) | 0.0420 (5) | |
| H8 | 0.5590 | 0.6937 | 0.6012 | 0.050* | |
| C11 | 0.2342 (4) | 0.8368 (4) | 0.55160 (19) | 0.0506 (7) | |
| H70 | 0.2526 | 0.8319 | 0.6114 | 0.076* | |
| H72 | 0.1441 | 0.7564 | 0.5520 | 0.076* | |
| H71 | 0.1871 | 0.9556 | 0.5260 | 0.076* | |
| C12 | 0.2729 (3) | 0.8866 (4) | 0.35844 (18) | 0.0450 (6) | |
| H12A | 0.1645 | 0.9099 | 0.4019 | 0.067* | |
| H12B | 0.2459 | 0.8026 | 0.3269 | 0.067* | |
| H12C | 0.3005 | 0.9953 | 0.3173 | 0.067* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.03341 (14) | 0.03084 (14) | 0.03585 (16) | 0.00481 (10) | −0.01015 (11) | −0.01292 (11) |
| Cl3 | 0.0377 (3) | 0.0295 (2) | 0.0513 (3) | 0.0060 (2) | −0.0183 (2) | −0.0128 (2) |
| Cl2 | 0.0450 (3) | 0.0395 (3) | 0.0405 (3) | 0.0100 (2) | −0.0159 (3) | −0.0105 (2) |
| Cl1 | 0.0676 (4) | 0.0333 (3) | 0.0480 (4) | −0.0068 (3) | −0.0224 (3) | −0.0121 (3) |
| Cl4 | 0.0545 (4) | 0.0622 (4) | 0.0416 (3) | 0.0228 (3) | −0.0035 (3) | −0.0199 (3) |
| N1 | 0.0264 (8) | 0.0238 (7) | 0.0260 (8) | 0.0000 (6) | −0.0036 (6) | −0.0058 (6) |
| C5 | 0.0346 (10) | 0.0263 (9) | 0.0254 (9) | −0.0014 (7) | −0.0033 (8) | −0.0081 (7) |
| C10 | 0.0313 (10) | 0.0303 (10) | 0.0301 (10) | −0.0023 (8) | −0.0025 (8) | −0.0078 (8) |
| C4 | 0.0278 (9) | 0.0309 (10) | 0.0312 (10) | −0.0033 (7) | −0.0045 (8) | −0.0072 (8) |
| N2 | 0.0353 (9) | 0.0381 (10) | 0.0304 (9) | 0.0012 (7) | −0.0043 (8) | −0.0129 (8) |
| C9 | 0.0373 (11) | 0.0330 (10) | 0.0309 (11) | −0.0076 (9) | 0.0033 (9) | −0.0082 (9) |
| C1 | 0.0394 (11) | 0.0300 (10) | 0.0345 (11) | −0.0097 (8) | −0.0031 (9) | −0.0109 (9) |
| C2 | 0.0376 (11) | 0.0412 (12) | 0.0325 (11) | −0.0069 (9) | −0.0060 (9) | −0.0130 (9) |
| C6 | 0.0361 (11) | 0.0398 (12) | 0.0335 (11) | 0.0076 (9) | −0.0078 (9) | −0.0123 (9) |
| C3 | 0.0345 (11) | 0.0351 (11) | 0.0314 (11) | −0.0086 (9) | −0.0004 (9) | −0.0072 (9) |
| C7 | 0.0475 (14) | 0.0492 (14) | 0.0334 (12) | 0.0070 (11) | −0.0133 (11) | −0.0090 (11) |
| C8 | 0.0550 (15) | 0.0419 (13) | 0.0290 (11) | −0.0022 (11) | −0.0065 (10) | −0.0092 (10) |
| C11 | 0.0481 (15) | 0.0613 (17) | 0.0385 (14) | −0.0070 (13) | 0.0094 (12) | −0.0145 (13) |
| C12 | 0.0295 (11) | 0.0605 (16) | 0.0396 (13) | −0.0013 (11) | −0.0021 (10) | −0.0040 (12) |
Geometric parameters (Å, º)
| Cu1—Cl4 | 2.2170 (9) | C9—C11 | 1.510 (3) |
| Cu1—Cl3 | 2.2439 (8) | C1—C2 | 1.508 (3) |
| Cu1—Cl2 | 2.2467 (8) | C1—H1A | 0.9700 |
| Cu1—Cl1 | 2.2704 (7) | C1—H1B | 0.9700 |
| N1—C5 | 1.493 (3) | C2—H2C | 0.9700 |
| N1—C1 | 1.507 (3) | C2—H2D | 0.9700 |
| N1—C4 | 1.511 (3) | C6—C7 | 1.390 (3) |
| N1—H1 | 0.9100 | C6—H6 | 0.9300 |
| C5—C6 | 1.382 (3) | C3—H3A | 0.9700 |
| C5—C10 | 1.391 (3) | C3—H3B | 0.9700 |
| C10—C9 | 1.405 (3) | C7—C8 | 1.376 (4) |
| C10—C12 | 1.499 (3) | C7—H7 | 0.9300 |
| C4—C3 | 1.504 (3) | C8—H8 | 0.9300 |
| C4—H4A | 0.9700 | C11—H70 | 0.9600 |
| C4—H4B | 0.9700 | C11—H72 | 0.9600 |
| N2—C3 | 1.481 (3) | C11—H71 | 0.9600 |
| N2—C2 | 1.488 (3) | C12—H12A | 0.9600 |
| N2—H2A | 0.9000 | C12—H12B | 0.9600 |
| N2—H2B | 0.9000 | C12—H12C | 0.9600 |
| C9—C8 | 1.377 (4) | ||
| Cl4—Cu1—Cl3 | 97.87 (3) | N1—C1—H1B | 109.4 |
| Cl4—Cu1—Cl2 | 98.37 (3) | C2—C1—H1B | 109.4 |
| Cl3—Cu1—Cl2 | 134.04 (3) | H1A—C1—H1B | 108.0 |
| Cl4—Cu1—Cl1 | 137.18 (4) | N2—C2—C1 | 111.22 (19) |
| Cl3—Cu1—Cl1 | 96.67 (3) | N2—C2—H2C | 109.4 |
| Cl2—Cu1—Cl1 | 99.83 (3) | C1—C2—H2C | 109.4 |
| C5—N1—C1 | 111.00 (16) | N2—C2—H2D | 109.4 |
| C5—N1—C4 | 115.08 (16) | C1—C2—H2D | 109.4 |
| C1—N1—C4 | 108.77 (16) | H2C—C2—H2D | 108.0 |
| C5—N1—H1 | 107.2 | C5—C6—C7 | 118.2 (2) |
| C1—N1—H1 | 107.2 | C5—C6—H6 | 120.9 |
| C4—N1—H1 | 107.2 | C7—C6—H6 | 120.9 |
| C6—C5—C10 | 123.4 (2) | N2—C3—C4 | 110.92 (18) |
| C6—C5—N1 | 118.13 (19) | N2—C3—H3A | 109.5 |
| C10—C5—N1 | 118.40 (19) | C4—C3—H3A | 109.5 |
| C5—C10—C9 | 116.8 (2) | N2—C3—H3B | 109.5 |
| C5—C10—C12 | 123.3 (2) | C4—C3—H3B | 109.5 |
| C9—C10—C12 | 119.9 (2) | H3A—C3—H3B | 108.0 |
| C3—C4—N1 | 109.47 (17) | C8—C7—C6 | 119.7 (2) |
| C3—C4—H4A | 109.8 | C8—C7—H7 | 120.1 |
| N1—C4—H4A | 109.8 | C6—C7—H7 | 120.1 |
| C3—C4—H4B | 109.8 | C7—C8—C9 | 121.7 (2) |
| N1—C4—H4B | 109.8 | C7—C8—H8 | 119.1 |
| H4A—C4—H4B | 108.2 | C9—C8—H8 | 119.1 |
| C3—N2—C2 | 111.79 (17) | C9—C11—H70 | 109.5 |
| C3—N2—H2A | 109.3 | C9—C11—H72 | 109.5 |
| C2—N2—H2A | 109.3 | H70—C11—H72 | 109.5 |
| C3—N2—H2B | 109.3 | C9—C11—H71 | 109.5 |
| C2—N2—H2B | 109.3 | H70—C11—H71 | 109.5 |
| H2A—N2—H2B | 107.9 | H72—C11—H71 | 109.5 |
| C8—C9—C10 | 120.1 (2) | C10—C12—H12A | 109.5 |
| C8—C9—C11 | 119.2 (2) | C10—C12—H12B | 109.5 |
| C10—C9—C11 | 120.6 (2) | H12A—C12—H12B | 109.5 |
| N1—C1—C2 | 111.01 (18) | C10—C12—H12C | 109.5 |
| N1—C1—H1A | 109.4 | H12A—C12—H12C | 109.5 |
| C2—C1—H1A | 109.4 | H12B—C12—H12C | 109.5 |
| C1—N1—C5—C6 | 88.3 (2) | C12—C10—C9—C11 | −2.8 (4) |
| C4—N1—C5—C6 | −35.8 (3) | C5—N1—C1—C2 | 174.05 (18) |
| C1—N1—C5—C10 | −89.5 (2) | C4—N1—C1—C2 | −58.4 (2) |
| C4—N1—C5—C10 | 146.48 (19) | C3—N2—C2—C1 | −53.9 (3) |
| C6—C5—C10—C9 | 3.1 (3) | N1—C1—C2—N2 | 55.3 (3) |
| N1—C5—C10—C9 | −179.34 (19) | C10—C5—C6—C7 | −2.1 (4) |
| C6—C5—C10—C12 | −176.0 (2) | N1—C5—C6—C7 | −179.7 (2) |
| N1—C5—C10—C12 | 1.6 (3) | C2—N2—C3—C4 | 56.3 (2) |
| C5—N1—C4—C3 | −174.74 (17) | N1—C4—C3—N2 | −59.4 (2) |
| C1—N1—C4—C3 | 60.0 (2) | C5—C6—C7—C8 | −0.5 (4) |
| C5—C10—C9—C8 | −1.4 (3) | C6—C7—C8—C9 | 2.1 (4) |
| C12—C10—C9—C8 | 177.7 (2) | C10—C9—C8—C7 | −1.1 (4) |
| C5—C10—C9—C11 | 178.2 (2) | C11—C9—C8—C7 | 179.3 (3) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1···Cl3i | 0.91 | 2.48 | 3.1610 (18) | 132 |
| N2—H2A···Cl2ii | 0.90 | 2.35 | 3.144 (2) | 147 |
| N2—H2B···Cl1iii | 0.90 | 2.30 | 3.152 (2) | 159 |
| N2—H2B···Cl2iii | 0.90 | 2.80 | 3.271 (2) | 114 |
| C2—H2D···Cl1i | 0.97 | 2.74 | 3.666 (3) | 159 |
| C3—H3B···Cl1iv | 0.97 | 2.78 | 3.585 (2) | 141 |
| C4—H4B···Cl4ii | 0.97 | 2.66 | 3.616 (2) | 168 |
| C6—H6···Cl4ii | 0.93 | 2.71 | 3.572 (2) | 154 |
| C12—H12C···Cl3i | 0.96 | 2.71 | 3.568 (3) | 149 |
Symmetry codes: (i) x, y+1, z; (ii) x+1, y, z; (iii) −x+1, −y+1, −z; (iv) x+1, y+1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RU2053).
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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 datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S1600536813021454/ru2053sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813021454/ru2053Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


