Abstract
In the cyrstal structure of the title compound, [Cu(NCS)(C18H20N2O2)]n, the CuI atom is coordinated in a distorted tetrahedral geometry by two imino N atoms from a bidentate chelating Schiff base ligand, and one N and one S atoms from two thiocyanate anions. The thiocyanate anion bridges the CuI atoms, forming a zigzag chain along [101]. The Schiff base ligand adopts an E,E configuration and the dihedral angle between the terminal benzene rings is 53.68 (8)°.
Related literature
For related copper(I) complexes with bidentate ligands, see: Amirnasr et al. (2006 ▶); Khalaji, Brad & Zhang (2008 ▶); Khalaji, Welter et al. (2008 ▶); Khalaji & Welter (2006 ▶); Zhao et al. (2008 ▶).
Experimental
Crystal data
[Cu(NCS)(C18H20N2O2)]
M r = 417.99
Monoclinic,
a = 8.1316 (3) Å
b = 23.5113 (9) Å
c = 10.1597 (4) Å
β = 107.1245 (15)°
V = 1856.27 (11) Å3
Z = 4
Mo Kα radiation
μ = 1.31 mm−1
T = 193 (1) K
0.31 × 0.17 × 0.02 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: numerical (ABSCOR; Higashi, 1995 ▶) T min = 0.771, T max = 0.974
28362 measured reflections
5395 independent reflections
4614 reflections with I > 2σ(I)
R int = 0.031
Refinement
R[F 2 > 2σ(F 2)] = 0.030
wR(F 2) = 0.076
S = 1.05
5395 reflections
235 parameters
H-atom parameters constrained
Δρmax = 0.51 e Å−3
Δρmin = −0.23 e Å−3
Data collection: PROCESS-AUTO (Rigaku/MSC, 2004 ▶); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2004 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: CrystalStructure and PLATON (Spek, 2003 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808041925/lh2744sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808041925/lh2744Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Cu1—S1 | 2.3130 (4) |
| Cu1—N1i | 1.9347 (12) |
| Cu1—N2 | 2.0917 (12) |
| Cu1—N3 | 2.0900 (13) |
Symmetry code: (i)
.
supplementary crystallographic information
Comment
Synthesis and characterization of copper(I) complexes with bidentate chelating Schiff base ligands have received much attention in recent years (Khalaji, Brad & Zhang, 2008; Khalaji, Welter et al., 2008; Zhao et al., 2008). Depending on the ligands involved, copper(I) complexes can show a wide variety of structures (Amirnasr et al., 2006; Khalaji & Welter, 2006; Khalaji, Brad & Zhang, 2008; Khalaji, Welter et al., 2008). As part of a general study of transition metal complexes with bidentate chelating Schiff base ligands (Khalaji & Welter, 2006; Khalaji, Brad & Zhang, 2008; Khalaji, Welter et al., 2008), here, we reported the synthesis and the crystal structure of the title compound, (I).
The crystal structure of the title compound, (I), is shown in Fig. 1. The Schiff base (3-MeO-ba)2en ligand chelates the CuI atom to form a five-membered ring, with N2—Cu1—N3 = 83.78 (4)°, which is in good agreement with the corresponding angles in related complexes (Khalaji & Welter, 2006; Khalaji, Brad & Zhang, 2008; Khalaji, Welter et al., 2008). The Cu—N and Cu—S distances (Table 1) are similar to those in the other copper(I) complexes. The C12—N3 and C9—N2 bond lengths of 1.2717 (18) and 1.2665 (18) Å, respectively, conform to the value for a C=N double bond, while the N2—C10 and N3—C11 bond lengths of 1.462 (2) and 1.476 (2) Å, respectively, conform to the value for a C—N single bond. These C—N lengths are comparable to the corresponding values observed in other tetrahedral copper(I) complexes with bidentate chelating Schiff base ligands (Khalaji & Welter, 2006; Khalaji, Brad & Zhang, 2008; Khalaji, Welter et al., 2008). The bidentate chelating (3-MeO-ba)2en ligand adopts an E,E configuration in this structure.
Experimental
The title compound, (I), was synthesized using a method analogous to the literature procedure (Khalaji & Welter, 2006), except that CuI was replaced with CuNCS. Single crystals suitable for data collection were obtained by slow evaporation from an acetonitrile solution at 273 K.
Refinement
H atoms were positioned geometrically (C—H = 0.95–0.99 Å) and treated as riding, with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C).
Figures
Fig. 1.
The molecular structure of the title compound with atom-labeling scheme. Displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.
A partial packing view of the title compound, (I).
Crystal data
| [Cu(NCS)(C18H20N2O2)] | F(000) = 864.00 |
| Mr = 417.99 | Dx = 1.496 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71075 Å |
| Hall symbol: -P 2yn | Cell parameters from 22727 reflections |
| a = 8.1316 (3) Å | θ = 3.1–30.0° |
| b = 23.5113 (9) Å | µ = 1.31 mm−1 |
| c = 10.1597 (4) Å | T = 193 K |
| β = 107.1245 (15)° | Platelet, yellow |
| V = 1856.27 (11) Å3 | 0.31 × 0.17 × 0.02 mm |
| Z = 4 |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 4614 reflections with I > 2σ(I) |
| Detector resolution: 10.00 pixels mm-1 | Rint = 0.031 |
| ω scans | θmax = 30.0°, θmin = 3.1° |
| Absorption correction: numerical (ABSCOR; Higashi, 1995) | h = −10→11 |
| Tmin = 0.771, Tmax = 0.974 | k = −32→32 |
| 28362 measured reflections | l = −14→12 |
| 5395 independent 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)] = 0.030 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.076 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0358P)2 + 0.7637P] where P = (Fo2 + 2Fc2)/3 |
| 5395 reflections | (Δ/σ)max = 0.001 |
| 235 parameters | Δρmax = 0.51 e Å−3 |
| 0 restraints | Δρmin = −0.23 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 | 0.42300 (2) | 0.235166 (8) | 0.471370 (18) | 0.02525 (6) | |
| S1 | 0.16168 (5) | 0.188164 (18) | 0.41646 (4) | 0.03209 (9) | |
| O1 | −0.06043 (17) | 0.34954 (5) | 0.56184 (14) | 0.0406 (3) | |
| O2 | 0.46009 (18) | 0.04893 (6) | 0.71225 (15) | 0.0472 (3) | |
| N1 | 0.01289 (17) | 0.24053 (6) | 0.16100 (13) | 0.0302 (3) | |
| N2 | 0.41448 (15) | 0.30353 (5) | 0.33778 (12) | 0.0248 (2) | |
| N3 | 0.61360 (15) | 0.20470 (5) | 0.38943 (12) | 0.0245 (2) | |
| C1 | 0.07436 (18) | 0.21886 (6) | 0.26548 (15) | 0.0255 (3) | |
| C2 | 0.3075 (2) | 0.38111 (6) | 0.44500 (16) | 0.0277 (3) | |
| C3 | 0.1706 (2) | 0.35321 (6) | 0.47169 (16) | 0.0281 (3) | |
| H3 | 0.1399 | 0.3160 | 0.4364 | 0.034* | |
| C4 | 0.0781 (2) | 0.37944 (6) | 0.55001 (15) | 0.0294 (3) | |
| C5 | 0.1271 (2) | 0.43268 (7) | 0.60751 (18) | 0.0374 (4) | |
| H5 | 0.0657 | 0.4504 | 0.6626 | 0.045* | |
| C6 | 0.2674 (3) | 0.45947 (8) | 0.5830 (2) | 0.0476 (5) | |
| H6 | 0.3037 | 0.4954 | 0.6240 | 0.057* | |
| C7 | 0.3549 (2) | 0.43480 (7) | 0.5002 (2) | 0.0411 (4) | |
| H7 | 0.4472 | 0.4545 | 0.4809 | 0.049* | |
| C8 | −0.1738 (2) | 0.37722 (8) | 0.6249 (2) | 0.0428 (4) | |
| H8A | −0.1147 | 0.3833 | 0.7228 | 0.064* | |
| H8B | −0.2757 | 0.3534 | 0.6151 | 0.064* | |
| H8C | −0.2091 | 0.4140 | 0.5800 | 0.064* | |
| C9 | 0.39553 (19) | 0.35649 (6) | 0.35092 (16) | 0.0283 (3) | |
| H9 | 0.4406 | 0.3817 | 0.2971 | 0.034* | |
| C10 | 0.4946 (2) | 0.28431 (7) | 0.23429 (15) | 0.0289 (3) | |
| H10A | 0.5255 | 0.3175 | 0.1866 | 0.035* | |
| H10B | 0.4127 | 0.2604 | 0.1649 | 0.035* | |
| C11 | 0.6547 (2) | 0.25029 (7) | 0.30428 (17) | 0.0299 (3) | |
| H11A | 0.7020 | 0.2334 | 0.2338 | 0.036* | |
| H11B | 0.7432 | 0.2758 | 0.3631 | 0.036* | |
| C12 | 0.70674 (18) | 0.16036 (6) | 0.40348 (16) | 0.0277 (3) | |
| H12 | 0.7894 | 0.1591 | 0.3541 | 0.033* | |
| C13 | 0.6977 (2) | 0.11098 (6) | 0.48926 (16) | 0.0291 (3) | |
| C14 | 0.8217 (3) | 0.06895 (8) | 0.5020 (2) | 0.0423 (4) | |
| H14 | 0.9060 | 0.0724 | 0.4547 | 0.051* | |
| C15 | 0.8215 (3) | 0.02186 (8) | 0.5846 (2) | 0.0531 (5) | |
| H15 | 0.9069 | −0.0067 | 0.5942 | 0.064* | |
| C16 | 0.6993 (3) | 0.01612 (7) | 0.6521 (2) | 0.0471 (5) | |
| H16 | 0.6997 | −0.0165 | 0.7075 | 0.056* | |
| C17 | 0.5745 (2) | 0.05804 (7) | 0.63967 (18) | 0.0359 (3) | |
| C18 | 0.5742 (2) | 0.10550 (7) | 0.55896 (17) | 0.0307 (3) | |
| H18 | 0.4900 | 0.1343 | 0.5511 | 0.037* | |
| C19 | 0.3301 (3) | 0.09082 (10) | 0.7005 (2) | 0.0532 (5) | |
| H19A | 0.3841 | 0.1279 | 0.7280 | 0.080* | |
| H19B | 0.2599 | 0.0807 | 0.7606 | 0.080* | |
| H19C | 0.2569 | 0.0927 | 0.6048 | 0.080* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.02571 (10) | 0.02875 (10) | 0.02277 (9) | −0.00058 (7) | 0.00944 (7) | 0.00156 (6) |
| S1 | 0.02396 (18) | 0.0417 (2) | 0.02944 (18) | −0.00463 (15) | 0.00609 (14) | 0.01091 (15) |
| O1 | 0.0427 (7) | 0.0376 (6) | 0.0521 (7) | −0.0008 (5) | 0.0304 (6) | −0.0038 (5) |
| O2 | 0.0445 (7) | 0.0437 (7) | 0.0519 (8) | −0.0052 (6) | 0.0118 (6) | 0.0206 (6) |
| N1 | 0.0276 (6) | 0.0381 (7) | 0.0254 (6) | −0.0013 (5) | 0.0084 (5) | −0.0009 (5) |
| N2 | 0.0246 (6) | 0.0277 (6) | 0.0243 (6) | 0.0011 (5) | 0.0103 (4) | 0.0022 (4) |
| N3 | 0.0219 (6) | 0.0267 (6) | 0.0265 (6) | −0.0017 (4) | 0.0097 (4) | −0.0012 (5) |
| C1 | 0.0207 (6) | 0.0308 (7) | 0.0267 (7) | −0.0019 (5) | 0.0094 (5) | −0.0021 (5) |
| C2 | 0.0309 (7) | 0.0231 (6) | 0.0304 (7) | 0.0032 (5) | 0.0109 (6) | 0.0021 (5) |
| C3 | 0.0325 (8) | 0.0231 (6) | 0.0310 (7) | 0.0022 (5) | 0.0127 (6) | −0.0001 (5) |
| C4 | 0.0332 (8) | 0.0288 (7) | 0.0286 (7) | 0.0039 (6) | 0.0127 (6) | 0.0026 (6) |
| C5 | 0.0460 (10) | 0.0326 (8) | 0.0382 (9) | 0.0058 (7) | 0.0193 (7) | −0.0056 (7) |
| C6 | 0.0555 (12) | 0.0295 (8) | 0.0619 (12) | −0.0046 (8) | 0.0238 (10) | −0.0167 (8) |
| C7 | 0.0429 (10) | 0.0291 (8) | 0.0558 (11) | −0.0066 (7) | 0.0218 (8) | −0.0073 (7) |
| C8 | 0.0414 (10) | 0.0485 (10) | 0.0466 (10) | 0.0115 (8) | 0.0253 (8) | 0.0059 (8) |
| C9 | 0.0289 (7) | 0.0272 (7) | 0.0308 (7) | 0.0003 (5) | 0.0122 (6) | 0.0047 (6) |
| C10 | 0.0337 (8) | 0.0311 (7) | 0.0262 (7) | 0.0027 (6) | 0.0156 (6) | 0.0025 (6) |
| C11 | 0.0282 (7) | 0.0314 (7) | 0.0349 (8) | −0.0005 (6) | 0.0170 (6) | 0.0022 (6) |
| C12 | 0.0218 (7) | 0.0315 (7) | 0.0310 (7) | −0.0002 (5) | 0.0096 (5) | −0.0033 (6) |
| C13 | 0.0280 (7) | 0.0268 (7) | 0.0300 (7) | 0.0022 (6) | 0.0048 (6) | −0.0038 (6) |
| C14 | 0.0468 (10) | 0.0380 (9) | 0.0434 (10) | 0.0151 (8) | 0.0154 (8) | −0.0034 (7) |
| C15 | 0.0703 (14) | 0.0342 (9) | 0.0539 (11) | 0.0251 (9) | 0.0167 (10) | 0.0000 (8) |
| C16 | 0.0649 (13) | 0.0244 (7) | 0.0448 (10) | 0.0057 (8) | 0.0052 (9) | 0.0040 (7) |
| C17 | 0.0369 (9) | 0.0293 (7) | 0.0363 (8) | −0.0051 (6) | 0.0026 (7) | 0.0032 (6) |
| C18 | 0.0270 (7) | 0.0266 (7) | 0.0358 (8) | 0.0002 (6) | 0.0050 (6) | 0.0030 (6) |
| C19 | 0.0392 (10) | 0.0670 (13) | 0.0561 (12) | −0.0005 (9) | 0.0183 (9) | 0.0273 (10) |
Geometric parameters (Å, °)
| Cu1—S1 | 2.3130 (4) | C14—C15 | 1.389 (2) |
| Cu1—N1i | 1.9347 (12) | C15—C16 | 1.370 (3) |
| Cu1—N2 | 2.0917 (12) | C16—C17 | 1.394 (2) |
| Cu1—N3 | 2.0900 (13) | C17—C18 | 1.384 (2) |
| S1—C1 | 1.6542 (14) | C3—H3 | 0.950 |
| O1—C4 | 1.363 (2) | C5—H5 | 0.950 |
| O1—C8 | 1.425 (2) | C6—H6 | 0.950 |
| O2—C17 | 1.364 (2) | C7—H7 | 0.950 |
| O2—C19 | 1.424 (2) | C8—H8A | 0.980 |
| N1—C1 | 1.1505 (18) | C8—H8B | 0.980 |
| N2—C9 | 1.2665 (18) | C8—H8C | 0.980 |
| N2—C10 | 1.462 (2) | C9—H9 | 0.950 |
| N3—C11 | 1.476 (2) | C10—H10A | 0.990 |
| N3—C12 | 1.2717 (18) | C10—H10B | 0.990 |
| C2—C3 | 1.386 (2) | C11—H11A | 0.990 |
| C2—C7 | 1.389 (2) | C11—H11B | 0.990 |
| C2—C9 | 1.471 (2) | C12—H12 | 0.950 |
| C3—C4 | 1.390 (2) | C14—H14 | 0.950 |
| C4—C5 | 1.389 (2) | C15—H15 | 0.950 |
| C5—C6 | 1.388 (3) | C16—H16 | 0.950 |
| C6—C7 | 1.380 (3) | C18—H18 | 0.950 |
| C10—C11 | 1.515 (2) | C19—H19A | 0.980 |
| C12—C13 | 1.467 (2) | C19—H19B | 0.980 |
| C13—C14 | 1.390 (2) | C19—H19C | 0.980 |
| C13—C18 | 1.394 (2) | ||
| S1—Cu1—N1i | 115.61 (4) | C4—C3—H3 | 119.9 |
| S1—Cu1—N2 | 110.98 (3) | C4—C5—H5 | 120.6 |
| S1—Cu1—N3 | 118.46 (3) | C6—C5—H5 | 120.6 |
| N1i—Cu1—N2 | 110.48 (5) | C5—C6—H6 | 119.4 |
| N1i—Cu1—N3 | 113.01 (5) | C7—C6—H6 | 119.4 |
| N2—Cu1—N3 | 83.78 (4) | C2—C7—H7 | 120.1 |
| Cu1—S1—C1 | 97.37 (5) | C6—C7—H7 | 120.1 |
| C4—O1—C8 | 117.71 (13) | O1—C8—H8A | 109.5 |
| C17—O2—C19 | 117.00 (15) | O1—C8—H8B | 109.5 |
| Cu1ii—N1—C1 | 169.62 (13) | O1—C8—H8C | 109.5 |
| Cu1—N2—C9 | 131.98 (11) | H8A—C8—H8B | 109.5 |
| Cu1—N2—C10 | 107.01 (8) | H8A—C8—H8C | 109.5 |
| C9—N2—C10 | 118.26 (14) | H8B—C8—H8C | 109.5 |
| Cu1—N3—C11 | 107.88 (9) | N2—C9—H9 | 118.2 |
| Cu1—N3—C12 | 136.32 (11) | C2—C9—H9 | 118.2 |
| C11—N3—C12 | 115.52 (14) | N2—C10—H10A | 109.8 |
| S1—C1—N1 | 179.41 (15) | N2—C10—H10B | 109.8 |
| C3—C2—C7 | 119.65 (17) | C11—C10—H10A | 109.8 |
| C3—C2—C9 | 120.89 (13) | C11—C10—H10B | 109.8 |
| C7—C2—C9 | 119.31 (16) | H10A—C10—H10B | 108.3 |
| C2—C3—C4 | 120.22 (13) | N3—C11—H11A | 109.6 |
| O1—C4—C3 | 114.99 (12) | N3—C11—H11B | 109.6 |
| O1—C4—C5 | 124.75 (16) | C10—C11—H11A | 109.6 |
| C3—C4—C5 | 120.26 (16) | C10—C11—H11B | 109.6 |
| C4—C5—C6 | 118.86 (18) | H11A—C11—H11B | 108.1 |
| C5—C6—C7 | 121.14 (17) | N3—C12—H12 | 117.2 |
| C2—C7—C6 | 119.77 (18) | C13—C12—H12 | 117.2 |
| N2—C9—C2 | 123.57 (15) | C13—C14—H14 | 120.2 |
| N2—C10—C11 | 109.21 (12) | C15—C14—H14 | 120.2 |
| N3—C11—C10 | 110.28 (13) | C14—C15—H15 | 119.7 |
| N3—C12—C13 | 125.68 (15) | C16—C15—H15 | 119.6 |
| C12—C13—C14 | 117.15 (16) | C15—C16—H16 | 120.0 |
| C12—C13—C18 | 123.00 (14) | C17—C16—H16 | 120.0 |
| C14—C13—C18 | 119.84 (15) | C13—C18—H18 | 120.0 |
| C13—C14—C15 | 119.6 (2) | C17—C18—H18 | 120.0 |
| C14—C15—C16 | 120.70 (19) | O2—C19—H19A | 109.5 |
| C15—C16—C17 | 120.06 (17) | O2—C19—H19B | 109.5 |
| O2—C17—C16 | 115.76 (16) | O2—C19—H19C | 109.5 |
| O2—C17—C18 | 124.37 (15) | H19A—C19—H19B | 109.5 |
| C16—C17—C18 | 119.87 (18) | H19A—C19—H19C | 109.5 |
| C13—C18—C17 | 119.96 (15) | H19B—C19—H19C | 109.5 |
| C2—C3—H3 | 119.9 | ||
| S1—Cu1—N1i—C1i | −141.8 (7) | C11—N3—C12—C13 | 176.20 (12) |
| N1i—Cu1—S1—C1 | 138.73 (7) | C12—N3—C11—C10 | 150.57 (12) |
| S1—Cu1—N2—C9 | 100.29 (12) | C3—C2—C7—C6 | 1.2 (2) |
| S1—Cu1—N2—C10 | −99.44 (8) | C7—C2—C3—C4 | 1.8 (2) |
| N2—Cu1—S1—C1 | 11.92 (7) | C3—C2—C9—N2 | −33.1 (2) |
| S1—Cu1—N3—C11 | 119.32 (7) | C9—C2—C3—C4 | −173.74 (12) |
| S1—Cu1—N3—C12 | −67.25 (13) | C7—C2—C9—N2 | 151.34 (14) |
| N3—Cu1—S1—C1 | −82.44 (6) | C9—C2—C7—C6 | 176.78 (15) |
| N1i—Cu1—N2—C9 | −29.30 (14) | C2—C3—C4—O1 | 175.86 (12) |
| N1i—Cu1—N2—C10 | 130.97 (8) | C2—C3—C4—C5 | −3.0 (2) |
| N2—Cu1—N1i—C1i | −14.7 (7) | O1—C4—C5—C6 | −177.52 (14) |
| N1i—Cu1—N3—C11 | −100.84 (9) | C3—C4—C5—C6 | 1.3 (2) |
| N1i—Cu1—N3—C12 | 72.59 (14) | C4—C5—C6—C7 | 1.7 (2) |
| N3—Cu1—N1i—C1i | 77.2 (7) | C5—C6—C7—C2 | −3.0 (2) |
| N2—Cu1—N3—C11 | 8.80 (8) | N2—C10—C11—N3 | 52.70 (16) |
| N2—Cu1—N3—C12 | −177.78 (13) | N3—C12—C13—C14 | −173.84 (14) |
| N3—Cu1—N2—C9 | −141.57 (13) | N3—C12—C13—C18 | 4.8 (2) |
| N3—Cu1—N2—C10 | 18.70 (8) | C12—C13—C14—C15 | 178.56 (15) |
| C8—O1—C4—C3 | −171.75 (13) | C12—C13—C18—C17 | −179.16 (13) |
| C8—O1—C4—C5 | 7.1 (2) | C14—C13—C18—C17 | −0.6 (2) |
| C19—O2—C17—C16 | −179.45 (15) | C18—C13—C14—C15 | −0.1 (2) |
| C19—O2—C17—C18 | 1.5 (2) | C13—C14—C15—C16 | 0.7 (2) |
| Cu1—N2—C9—C2 | −25.4 (2) | C14—C15—C16—C17 | −0.7 (2) |
| Cu1—N2—C10—C11 | −42.47 (13) | C15—C16—C17—O2 | −179.10 (15) |
| C9—N2—C10—C11 | 120.98 (14) | C15—C16—C17—C18 | −0.0 (2) |
| C10—N2—C9—C2 | 176.11 (11) | O2—C17—C18—C13 | 179.63 (14) |
| Cu1—N3—C11—C10 | −34.46 (13) | C16—C17—C18—C13 | 0.6 (2) |
| Cu1—N3—C12—C13 | 3.1 (2) |
Symmetry codes: (i) x+1/2, −y+1/2, z+1/2; (ii) x−1/2, −y+1/2, z−1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH2744).
References
- Amirnasr, M., Khalaji, A. D. & Falvello, L. R. (2006). Inorg. Chim. Acta, 359, 713–717.
- Farrugia, L. J. (1997). J. Appl. Cryst.30, 565.
- Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
- Khalaji, A. D., Brad, K. & Zhang, Y. (2008). Acta Cryst. E64, m189. [DOI] [PMC free article] [PubMed]
- Khalaji, A. D. & Welter, R. (2006). Inorg. Chim. Acta, 359, 4403–4406.
- Khalaji, A. D., Welter, R., Amirnasr, M. & Barry, A. H. (2008). Anal. Sci.24, x137–x138.
- Rigaku/MSC (2004). CrystalStructure and PROCESS-AUTO Rigaku/MSC, The Woodlands, Texas, USA.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2003). J. Appl. Cryst.36, 7–13.
- Zhao, J., Dong, W.-W., Li, D.-S. & He, Q.-F. (2008). Acta Cryst. E64, m1576. [DOI] [PMC free article] [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 global, I. DOI: 10.1107/S1600536808041925/lh2744sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808041925/lh2744Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


