Abstract
The asymmetric unit of the crystal structure of the title compound, [Cd2Cl4(C5H8N2)3]n, contains two CdII cations, three 1-ethyl-1H-imidazole ligands, and four Cl− anions. The two CdII atoms have quite different coordination environments: one is octahedrally coordinated by four Cl atoms and two N atoms from two 1-ethyl-1H-imidazole ligands, and the second is in a severely distorted fivefold coordination by four Cl atoms and one N atom from a 1-ethyl-1H-imidazole ligand. Adjacent CdII cations are interconnected alternately by pairs of chloride bridges, generating an infinite step-like chain along the a axis. One ethyl group of the 1-ethyl-1H-imidazole ligand is disordered over two sets of sites with a 0.668 (13):0.332 (13) site-occupancy ratio.
Related literature
For general background to compounds with organic framework structures and with ferroelectric properties, see: Ye et al. (2009 ▶); Zhang et al. (2009 ▶).
Experimental
Crystal data
[Cd2Cl4(C5H8N2)3]
M r = 655.02
Monoclinic,
a = 15.227 (3) Å
b = 8.8651 (18) Å
c = 18.069 (4) Å
β = 110.34 (3)°
V = 2286.9 (8) Å3
Z = 4
Mo Kα radiation
μ = 2.34 mm−1
T = 293 K
0.30 × 0.25 × 0.20 mm
Data collection
Rigaku SCXmini diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.501, T max = 0.626
23098 measured reflections
5241 independent reflections
4674 reflections with I > 2σ(I)
R int = 0.027
Refinement
R[F 2 > 2σ(F 2)] = 0.028
wR(F 2) = 0.059
S = 1.17
5241 reflections
251 parameters
33 restraints
H-atom parameters constrained
Δρmax = 0.51 e Å−3
Δρmin = −0.78 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND (Brandenburg & Putz, 1999 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S160053681104894X/vn2017sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681104894X/vn2017Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| Cd1—N1 | 2.250 (2) |
| Cd1—N3 | 2.267 (2) |
| Cd1—Cl1 | 2.6259 (11) |
| Cd1—Cl1i | 2.6995 (8) |
| Cd1—Cl2 | 2.7203 (8) |
| Cd1—Cl3 | 2.8930 (12) |
| Cd2—N5 | 2.227 (2) |
| Cd2—Cl3 | 2.4713 (8) |
| Cd2—Cl4 | 2.5120 (8) |
| Cd2—Cl2 | 2.6340 (11) |
| Cd2—Cl4ii | 2.7526 (11) |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors are grateful to the starter fund of Southeast University for financial support to buy the X-ray diffractometer.
supplementary crystallographic information
Comment
The title compound, [C15H24Cd2Cl4N6], (I), was prepared from 1-ethyl-1H-imidazole and cadmium(II) chloride in N,N-dimethylformamide. The X-ray crystal structure of the title complex at 298 K (Fig. 1) shows a novel infinite one-dimensional coordination chain along the a axis (Fig. 2). There are two types of Cd atoms with different coordination environments: Cd(1) is coordinated by two 2-ethyl imidazole ligands and four bridging Cl atoms, and Cd(2) is in severely distorted pentahedral coordination by four bridging Cl atoms, and one 2-ethyl imidazole ligand.
In order to examine possible structure phase transitions of compound (I), we measured its temperature-dependent dielectric constant. Large dielectric anomalies usually indicate structural changes such as paraelectric-to-ferroelectric phase transitions. Unfortunately, the dielectric constant of compound (I) goes smoothly in the temperature range 93–273 K, suggesting the absence of distinct phase transitions (Ye et al., 2009; Zhang et al., 2009).
Experimental
A mixture of CdCl2 (2.27 g, 10 mmol) and 2-ethyl imidazole (1.82 g, 20 mmol) in water was stirred for several minutes at room temperature, to which was then added 10 ml N,N-dimethylformamide. Colourless block-shaped crystals suitable for X-ray diffraction analysis were obtained by slow evaporation of the solution at room temperature over 2 weeks.
Refinement
Positional parameters of all H atoms except for H1A, H1B and H1C were calculated geometrically and the H atoms were set to ride the C atoms to which they are bonded, with Uiso(H) = 1.2 Uiso(C) and 1.5Uiso(C) for methyl H atoms. The positional parameters of the H atoms (C1) were refined freely. And in the last stage of the refinement, they were restrained with the C—H = 0.96 (2)Å with Uiso(H)=1.5Uiso(C).
Figures
Fig. 1.
: Labeling scheme of (I). Thermal displacement ellipsoids depicted at 50% probability.
Fig. 2.
: Packing diagram of the title compound.
Crystal data
| [Cd2Cl4(C5H8N2)3] | F(000) = 1280 |
| Mr = 655.02 | Dx = 1.893 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 5246 reflections |
| a = 15.227 (3) Å | θ = 2.8–27.5° |
| b = 8.8651 (18) Å | µ = 2.34 mm−1 |
| c = 18.069 (4) Å | T = 293 K |
| β = 110.34 (3)° | Block, colourless |
| V = 2286.9 (8) Å3 | 0.30 × 0.25 × 0.20 mm |
| Z = 4 |
Data collection
| Rigaku SCXmini diffractometer | 4674 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.027 |
| graphite | θmax = 27.5°, θmin = 3.0° |
| ω scans | h = −19→19 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −11→11 |
| Tmin = 0.501, Tmax = 0.626 | l = −23→23 |
| 23098 measured reflections | 2 standard reflections every 150 reflections |
| 5241 independent reflections | intensity decay: none |
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)] = 0.028 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.059 | H-atom parameters constrained |
| S = 1.17 | w = 1/[σ2(Fo2) + (0.0209P)2 + 1.5151P] where P = (Fo2 + 2Fc2)/3 |
| 5241 reflections | (Δ/σ)max = 0.002 |
| 251 parameters | Δρmax = 0.51 e Å−3 |
| 33 restraints | Δρmin = −0.78 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 | Occ. (<1) | |
| C1 | 0.2535 (3) | 0.3210 (4) | 0.7812 (2) | 0.0622 (10) | |
| H1A | 0.2185 | 0.2300 | 0.7790 | 0.093* | |
| H1C | 0.3122 | 0.2969 | 0.7754 | 0.093* | |
| H1B | 0.2185 | 0.3873 | 0.7394 | 0.093* | |
| C2A | 0.2704 (3) | 0.3936 (4) | 0.8556 (2) | 0.042 (3) | 0.332 (13) |
| H2A | 0.3278 | 0.3539 | 0.8935 | 0.050* | 0.332 (13) |
| H2B | 0.2197 | 0.3693 | 0.8744 | 0.050* | 0.332 (13) |
| C2B | 0.2259 (6) | 0.4184 (8) | 0.8346 (5) | 0.066 (2) | 0.668 (13) |
| H2C | 0.2360 | 0.3650 | 0.8837 | 0.079* | 0.668 (13) |
| H2D | 0.1595 | 0.4400 | 0.8112 | 0.079* | 0.668 (13) |
| C3 | 0.2872 (2) | 0.6581 (4) | 0.79499 (18) | 0.0450 (7) | |
| H3A | 0.2728 | 0.6360 | 0.7418 | 0.054* | |
| C4 | 0.3207 (2) | 0.7902 (3) | 0.83155 (17) | 0.0398 (7) | |
| H4A | 0.3333 | 0.8755 | 0.8070 | 0.048* | |
| C5 | 0.3075 (2) | 0.6412 (3) | 0.91979 (18) | 0.0417 (7) | |
| H5A | 0.3090 | 0.6020 | 0.9680 | 0.050* | |
| C6 | 0.5076 (3) | 1.5520 (6) | 1.2355 (2) | 0.0877 (16) | |
| H6A | 0.5458 | 1.6406 | 1.2514 | 0.132* | |
| H6B | 0.5439 | 1.4645 | 1.2586 | 0.132* | |
| H6C | 0.4550 | 1.5595 | 1.2530 | 0.132* | |
| C7 | 0.4739 (2) | 1.5390 (4) | 1.1487 (2) | 0.0498 (8) | |
| H7A | 0.4385 | 1.6288 | 1.1258 | 0.060* | |
| H7B | 0.5273 | 1.5335 | 1.1313 | 0.060* | |
| C8 | 0.3308 (2) | 1.3745 (3) | 1.12864 (19) | 0.0428 (7) | |
| H8A | 0.2998 | 1.4343 | 1.1540 | 0.051* | |
| C9 | 0.3018 (2) | 1.2413 (3) | 1.09349 (19) | 0.0421 (7) | |
| H9A | 0.2465 | 1.1928 | 1.0906 | 0.050* | |
| C10 | 0.43245 (19) | 1.2905 (3) | 1.08022 (17) | 0.0374 (7) | |
| H10A | 0.4858 | 1.2833 | 1.0665 | 0.045* | |
| C11 | −0.0447 (3) | 0.3094 (4) | 0.7616 (2) | 0.0550 (9) | |
| H11A | −0.0935 | 0.2562 | 0.7217 | 0.083* | |
| H11B | 0.0016 | 0.2388 | 0.7921 | 0.083* | |
| H11C | −0.0160 | 0.3805 | 0.7369 | 0.083* | |
| C12 | −0.0856 (2) | 0.3921 (4) | 0.81485 (19) | 0.0451 (7) | |
| H12A | −0.1335 | 0.4613 | 0.7836 | 0.054* | |
| H12B | −0.1152 | 0.3200 | 0.8391 | 0.054* | |
| C13 | 0.0617 (2) | 0.4182 (3) | 0.93522 (18) | 0.0396 (7) | |
| H13A | 0.0771 | 0.3166 | 0.9441 | 0.048* | |
| C14 | 0.10997 (19) | 0.5361 (3) | 0.97753 (17) | 0.0365 (6) | |
| H14A | 0.1649 | 0.5291 | 1.0211 | 0.044* | |
| C15 | −0.00935 (19) | 0.6269 (3) | 0.88567 (16) | 0.0336 (6) | |
| H15A | −0.0530 | 0.6937 | 0.8533 | 0.040* | |
| N1 | 0.36568 (15) | 1.1879 (3) | 1.06256 (14) | 0.0337 (5) | |
| N2 | 0.41452 (16) | 1.4056 (3) | 1.12006 (14) | 0.0339 (5) | |
| N3 | 0.33331 (15) | 0.7790 (3) | 0.91045 (13) | 0.0334 (5) | |
| N4 | 0.2787 (2) | 0.5636 (3) | 0.85209 (16) | 0.0463 (6) | |
| N5 | 0.06491 (15) | 0.6681 (2) | 0.94594 (13) | 0.0321 (5) | |
| N6 | −0.01384 (16) | 0.4769 (3) | 0.87701 (14) | 0.0339 (5) | |
| Cd1 | 0.369012 (13) | 0.97139 (2) | 0.998629 (12) | 0.03133 (6) | |
| Cd2 | 0.109824 (13) | 0.90222 (2) | 0.986382 (12) | 0.02988 (6) | |
| Cl1 | 0.53919 (5) | 0.88774 (8) | 1.08530 (4) | 0.03651 (15) | |
| Cl2 | 0.27753 (4) | 0.82083 (8) | 1.08130 (4) | 0.03515 (15) | |
| Cl3 | 0.17898 (5) | 1.05852 (8) | 0.90744 (4) | 0.03683 (15) | |
| Cl4 | 0.06876 (5) | 1.00365 (9) | 1.10005 (4) | 0.03945 (16) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.084 (3) | 0.043 (2) | 0.057 (2) | −0.0094 (19) | 0.021 (2) | −0.0090 (17) |
| C2A | 0.058 (7) | 0.018 (4) | 0.054 (6) | −0.007 (4) | 0.024 (5) | −0.003 (4) |
| C2B | 0.077 (5) | 0.055 (4) | 0.087 (5) | −0.031 (3) | 0.053 (4) | −0.030 (3) |
| C3 | 0.0518 (18) | 0.0498 (18) | 0.0333 (15) | 0.0009 (15) | 0.0147 (14) | −0.0061 (14) |
| C4 | 0.0474 (17) | 0.0365 (16) | 0.0372 (16) | 0.0016 (13) | 0.0167 (14) | 0.0028 (13) |
| C5 | 0.0579 (19) | 0.0358 (16) | 0.0404 (16) | −0.0077 (14) | 0.0283 (15) | −0.0069 (13) |
| C6 | 0.082 (3) | 0.118 (4) | 0.072 (3) | −0.053 (3) | 0.037 (2) | −0.048 (3) |
| C7 | 0.0517 (19) | 0.0323 (16) | 0.064 (2) | −0.0108 (14) | 0.0185 (17) | −0.0093 (15) |
| C8 | 0.0355 (15) | 0.0426 (18) | 0.0537 (19) | 0.0034 (13) | 0.0200 (14) | −0.0109 (14) |
| C9 | 0.0312 (15) | 0.0424 (17) | 0.0555 (19) | −0.0057 (13) | 0.0188 (14) | −0.0137 (15) |
| C10 | 0.0304 (14) | 0.0373 (16) | 0.0479 (17) | −0.0011 (12) | 0.0178 (13) | −0.0074 (13) |
| C11 | 0.062 (2) | 0.058 (2) | 0.0451 (19) | −0.0062 (17) | 0.0177 (17) | −0.0156 (16) |
| C12 | 0.0444 (17) | 0.0395 (17) | 0.0491 (18) | −0.0096 (14) | 0.0131 (15) | −0.0090 (14) |
| C13 | 0.0464 (17) | 0.0247 (14) | 0.0499 (18) | 0.0041 (12) | 0.0195 (15) | 0.0022 (13) |
| C14 | 0.0339 (14) | 0.0331 (15) | 0.0413 (15) | 0.0063 (12) | 0.0116 (13) | 0.0026 (13) |
| C15 | 0.0373 (15) | 0.0268 (14) | 0.0361 (15) | 0.0006 (11) | 0.0119 (12) | 0.0023 (11) |
| N1 | 0.0282 (11) | 0.0316 (13) | 0.0418 (13) | −0.0014 (9) | 0.0129 (10) | −0.0061 (10) |
| N2 | 0.0337 (12) | 0.0286 (12) | 0.0377 (13) | −0.0014 (10) | 0.0102 (10) | −0.0036 (10) |
| N3 | 0.0328 (12) | 0.0329 (12) | 0.0357 (13) | −0.0032 (10) | 0.0135 (10) | −0.0038 (10) |
| N4 | 0.0614 (17) | 0.0392 (14) | 0.0496 (15) | −0.0139 (12) | 0.0336 (14) | −0.0150 (12) |
| N5 | 0.0347 (12) | 0.0251 (11) | 0.0375 (12) | 0.0001 (9) | 0.0137 (10) | −0.0004 (10) |
| N6 | 0.0382 (13) | 0.0267 (12) | 0.0389 (13) | −0.0028 (10) | 0.0161 (11) | −0.0040 (10) |
| Cd1 | 0.02946 (11) | 0.02810 (11) | 0.03840 (12) | −0.00269 (8) | 0.01428 (9) | −0.00548 (8) |
| Cd2 | 0.02865 (10) | 0.02620 (10) | 0.03691 (11) | −0.00126 (8) | 0.01409 (8) | −0.00228 (8) |
| Cl1 | 0.0308 (3) | 0.0377 (4) | 0.0418 (4) | −0.0001 (3) | 0.0136 (3) | 0.0090 (3) |
| Cl2 | 0.0298 (3) | 0.0415 (4) | 0.0343 (3) | 0.0030 (3) | 0.0114 (3) | 0.0043 (3) |
| Cl3 | 0.0335 (3) | 0.0341 (3) | 0.0436 (4) | −0.0006 (3) | 0.0143 (3) | 0.0083 (3) |
| Cl4 | 0.0342 (3) | 0.0471 (4) | 0.0354 (4) | 0.0105 (3) | 0.0099 (3) | −0.0062 (3) |
Geometric parameters (Å, °)
| C1—C2A | 1.4306 | C10—N1 | 1.318 (3) |
| C1—C2B | 1.460 (7) | C10—N2 | 1.331 (4) |
| C1—H1A | 0.9600 | C10—H10A | 0.9300 |
| C1—H1C | 0.9600 | C11—C12 | 1.506 (4) |
| C1—H1B | 0.9600 | C11—H11A | 0.9600 |
| C2A—N4 | 1.515 (4) | C11—H11B | 0.9600 |
| C2A—H2A | 0.9700 | C11—H11C | 0.9600 |
| C2A—H2B | 0.9700 | C12—N6 | 1.472 (4) |
| C2B—N4 | 1.492 (6) | C12—H12A | 0.9700 |
| C2B—H2C | 0.9700 | C12—H12B | 0.9700 |
| C2B—H2D | 0.9700 | C13—C14 | 1.351 (4) |
| C3—C4 | 1.354 (4) | C13—N6 | 1.364 (4) |
| C3—N4 | 1.370 (4) | C13—H13A | 0.9300 |
| C3—H3A | 0.9300 | C14—N5 | 1.377 (4) |
| C4—N3 | 1.374 (4) | C14—H14A | 0.9300 |
| C4—H4A | 0.9300 | C15—N5 | 1.320 (3) |
| C5—N3 | 1.313 (4) | C15—N6 | 1.338 (3) |
| C5—N4 | 1.338 (4) | C15—H15A | 0.9300 |
| C5—H5A | 0.9300 | Cd1—N1 | 2.250 (2) |
| C6—C7 | 1.475 (5) | Cd1—N3 | 2.267 (2) |
| C6—H6A | 0.9600 | Cd2—N5 | 2.227 (2) |
| C6—H6B | 0.9600 | Cd1—Cl1 | 2.6259 (11) |
| C6—H6C | 0.9600 | Cd1—Cl1i | 2.6995 (8) |
| C7—N2 | 1.469 (4) | Cd1—Cl2 | 2.7203 (8) |
| C7—H7A | 0.9700 | Cd1—Cl3 | 2.8930 (12) |
| C7—H7B | 0.9700 | Cd2—Cl3 | 2.4713 (8) |
| C8—C9 | 1.341 (4) | Cd2—Cl4 | 2.5120 (8) |
| C8—N2 | 1.365 (4) | Cd2—Cl2 | 2.6340 (11) |
| C8—H8A | 0.9300 | Cd2—Cl4ii | 2.7526 (11) |
| C9—N1 | 1.364 (3) | Cd1—Cl1i | 2.6995 (8) |
| C9—H9A | 0.9300 | Cd2—Cl4ii | 2.7526 (11) |
| C2A—C1—C2B | 27.5 (4) | C11—C12—H12B | 109.2 |
| C2A—C1—H1A | 109.5 | H12A—C12—H12B | 107.9 |
| C2B—C1—H1A | 104.0 | C14—C13—N6 | 106.7 (2) |
| C2A—C1—H1C | 109.5 | C14—C13—H13A | 126.6 |
| C2B—C1—H1C | 134.2 | N6—C13—H13A | 126.6 |
| H1A—C1—H1C | 109.5 | C13—C14—N5 | 109.2 (3) |
| C2A—C1—H1B | 109.5 | C13—C14—H14A | 125.4 |
| C2B—C1—H1B | 87.1 | N5—C14—H14A | 125.4 |
| H1A—C1—H1B | 109.5 | N5—C15—N6 | 111.5 (2) |
| H1C—C1—H1B | 109.5 | N5—C15—H15A | 124.3 |
| C1—C2A—N4 | 113.50 (16) | N6—C15—H15A | 124.3 |
| C1—C2A—H2A | 108.9 | C10—N1—C9 | 105.1 (2) |
| N4—C2A—H2A | 108.9 | C10—N1—Cd1 | 124.04 (18) |
| C1—C2A—H2B | 108.9 | C9—N1—Cd1 | 130.79 (19) |
| N4—C2A—H2B | 108.9 | C10—N2—C8 | 106.4 (2) |
| H2A—C2A—H2B | 107.7 | C10—N2—C7 | 126.3 (3) |
| C1—C2B—N4 | 113.2 (5) | C8—N2—C7 | 127.3 (3) |
| C1—C2B—H2C | 108.9 | C5—N3—C4 | 105.1 (2) |
| N4—C2B—H2C | 108.9 | C5—N3—Cd1 | 128.25 (19) |
| C1—C2B—H2D | 108.9 | C4—N3—Cd1 | 126.01 (19) |
| N4—C2B—H2D | 108.9 | C5—N4—C3 | 106.7 (3) |
| H2C—C2B—H2D | 107.8 | C5—N4—C2B | 128.2 (4) |
| C4—C3—N4 | 106.2 (3) | C3—N4—C2B | 123.6 (4) |
| C4—C3—H3A | 126.9 | C5—N4—C2A | 118.6 (3) |
| N4—C3—H3A | 126.9 | C3—N4—C2A | 132.1 (3) |
| C3—C4—N3 | 109.7 (3) | C2B—N4—C2A | 26.4 (4) |
| C3—C4—H4A | 125.2 | C15—N5—C14 | 105.5 (2) |
| N3—C4—H4A | 125.2 | C15—N5—Cd2 | 127.30 (18) |
| N3—C5—N4 | 112.3 (3) | C14—N5—Cd2 | 127.19 (19) |
| N3—C5—H5A | 123.9 | C15—N6—C13 | 107.1 (2) |
| N4—C5—H5A | 123.9 | C15—N6—C12 | 126.2 (2) |
| C7—C6—H6A | 109.5 | C13—N6—C12 | 126.6 (2) |
| C7—C6—H6B | 109.5 | N1—Cd1—N3 | 163.71 (8) |
| H6A—C6—H6B | 109.5 | N1—Cd1—Cl1 | 97.38 (6) |
| C7—C6—H6C | 109.5 | N3—Cd1—Cl1 | 98.78 (6) |
| H6A—C6—H6C | 109.5 | N1—Cd1—Cl1i | 90.14 (6) |
| H6B—C6—H6C | 109.5 | N3—Cd1—Cl1i | 89.86 (6) |
| N2—C7—C6 | 112.5 (3) | Cl1—Cd1—Cl1i | 82.49 (3) |
| N2—C7—H7A | 109.1 | N1—Cd1—Cl2 | 91.68 (6) |
| C6—C7—H7A | 109.1 | N3—Cd1—Cl2 | 88.48 (6) |
| N2—C7—H7B | 109.1 | Cl1—Cd1—Cl2 | 96.98 (3) |
| C6—C7—H7B | 109.1 | Cl1i—Cd1—Cl2 | 178.16 (2) |
| H7A—C7—H7B | 107.8 | N1—Cd1—Cl3 | 82.42 (6) |
| C9—C8—N2 | 106.9 (3) | N3—Cd1—Cl3 | 81.52 (6) |
| C9—C8—H8A | 126.6 | Cl1—Cd1—Cl3 | 177.86 (2) |
| N2—C8—H8A | 126.6 | Cl1i—Cd1—Cl3 | 99.63 (3) |
| C8—C9—N1 | 109.6 (3) | Cl2—Cd1—Cl3 | 80.91 (3) |
| C8—C9—H9A | 125.2 | N5—Cd2—Cl3 | 118.48 (6) |
| N1—C9—H9A | 125.2 | N5—Cd2—Cl4 | 117.80 (6) |
| N1—C10—N2 | 112.0 (2) | Cl3—Cd2—Cl4 | 123.25 (3) |
| N1—C10—H10A | 124.0 | N5—Cd2—Cl2 | 94.36 (6) |
| N2—C10—H10A | 124.0 | Cl3—Cd2—Cl2 | 91.04 (3) |
| C12—C11—H11A | 109.5 | Cl4—Cd2—Cl2 | 91.50 (3) |
| C12—C11—H11B | 109.5 | N5—Cd2—Cl4ii | 88.06 (6) |
| H11A—C11—H11B | 109.5 | Cl3—Cd2—Cl4ii | 92.16 (3) |
| C12—C11—H11C | 109.5 | Cl4—Cd2—Cl4ii | 82.98 (3) |
| H11A—C11—H11C | 109.5 | Cl2—Cd2—Cl4ii | 174.48 (2) |
| H11B—C11—H11C | 109.5 | Cd1—Cl1—Cd1i | 97.51 (3) |
| N6—C12—C11 | 111.9 (3) | Cd2—Cl2—Cd1 | 94.22 (3) |
| N6—C12—H12A | 109.2 | Cd2—Cl3—Cd1 | 93.68 (3) |
| C11—C12—H12A | 109.2 | Cd2—Cl4—Cd2ii | 97.02 (3) |
| N6—C12—H12B | 109.2 |
Symmetry codes: (i) −x+1, −y+2, −z+2; (ii) −x, −y+2, −z+2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: VN2017).
References
- Brandenburg, K. & Putz, H. (1999). DIAMOND. Crystal Impact GbR, Bonn, Germany.
- Rigaku (2005). CrystalClear. Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Ye, H. Y., Fu, D. W., Zhang, Y., Zhang, W., Xiong, R. G. & Huang, S. P. (2009). J. Am. Chem. Soc. 131, 42–43. [DOI] [PubMed]
- Zhang, W., Cheng, L. Z., Xiong, R. G., Nakamura, T. & Huang, S. P. (2009). J. Am. Chem. Soc. 131, 12544–12545. [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 datablock(s) I, global. DOI: 10.1107/S160053681104894X/vn2017sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681104894X/vn2017Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


