In the title compound, the CuI atom is coordinated by two S atoms and two I atoms in a distorted tetrahedral mode.
Keywords: crystal structure, N-acetylthiomorpholine, coordination polymer, copper(I) iodide
Abstract
The reaction of copper(I) iodide with N-acetylthiomorpholine (L, C6H11NOS) in acetonitrile results in a coordination polymer with composition [CuI(L)2]n. The CuI atom is coordinated by two S atoms and two I atoms, adopting a distorted tetrahedral environment. The μ2-bridging mode of the I atoms gives rise to chains extending parallel to [010]. C—H⋯O hydrogen-bonding interactions between the chains lead to a three-dimensional network.
Chemical context
Synthesis, structures and luminescence properties of copper(I) complexes involving CuI and thioethers as co-ligands have been studied extensively (Harvey & Knorr, 2010 ▸; Knorr et al., 2010 ▸; Henline et al., 2014 ▸). The tendency of copper(I) iodide to form aggregates often leads to short Cu—Cu bonds and intriguing diversities in the respective crystal structures (Peng et al., 2010 ▸), comprising of [CuI]n chains with split stair motifs (Moreno et al., 1995 ▸; Blake et al., 1999 ▸; Cariati et al., 2002 ▸; Näther et al., 2003 ▸; Thébault et al., 2006 ▸), zigzag chains (Munakata et al., 1997 ▸) or helical chains (Munakata et al., 1997 ▸; Kang & Anson, 1995 ▸). Most of these structures include aromatic nitrogen donor co-ligands. In this context we have studied the interaction of N-acetylthiomorpholine with CuI to investigate the coordination behaviour of the copper(I) atom with the S donor atom of the N-acetylthiomorpholine co-ligand, because both are soft atoms in the sense of the HSAB concept. Although a number of copper(I) complexes with thioether ligands are known (Knorr et al., 2010 ▸; Henline et al., 2014 ▸), to the best of our knowledge, a [CuI]n chain structure has not been reported until now. Herein, we report a copper(I) coordination polymer with a zigzag chain [CuI]n, resulting from the reaction of CuI with N-acetylthiomorpholine (L).
Structural commentary
The asymmetric unit of the title compound, [CuI(L)2]n, comprises of a copper(I) iodide moiety and two N-acetylthiomorpholine co-ligands (L A and L B) and is shown in Fig. 1 ▸. The CuI atom has a slightly distorted tetrahedral environment (Table 1 ▸). The two thiomorpholine rings have the stable chair conformation (Kang et al., 2015 ▸). The dihedral angles between acetyl CCO and thiomorpholine CNC planes are 3.9 (4) and 6.6 (2)° for L A and L B, respectively. The I atoms link neighboring CuI atoms in a μ 2 -bridging mode into polymeric zigzag chains extending parallel to [010] (Fig. 2 ▸).
Figure 1.
The asymmetric unit of the title compound, shown with displacement ellipsoids drawn at the 50% probability level. H atom are shown as small spheres of arbitrary radius.
Table 1. Selected geometric parameters (Å, °).
| Cu1—S1 | 2.3012 (6) | Cu1—I1 | 2.6221 (3) |
| Cu1—S2 | 2.3064 (6) | Cu1—I1i | 2.6476 (3) |
| S1—Cu1—S2 | 114.28 (2) | S2—Cu1—I1 | 101.246 (16) |
| S1—Cu1—I1 | 112.179 (17) | I1—Cu1—I1i | 109.949 (9) |
Symmetry code: (i)
.
Figure 2.
The polymeric chain structure in [CuI(L)2] formed through the μ2-bridging mode of the I atoms. All H atoms have been omitted for clarity.
Supramolecular features
As shown in Fig. 3 ▸, C10—H10A⋯ O1 hydrogen bonds (yellow dashed lines) between the thiomorpholine ring of L B and the carbonyl oxygen atoms of L A result in a layered network parallel to (101). Additional C12—H12B⋯O2 hydrogen bonds between methyl groups of L B ligands and carbonyl oxygen atoms of neighbouring L B ligands (red dashed lines) form cyclic centrosymmetric dimers of N-acetylthiomorpholines. The combination of the [CuI]n chains and the two types of hydrogen-bonding interactions with additional C—H⋯O interactions (Table 2 ▸) leads to a three-dimensional network.
Figure 3.
The crystal structure of [CuI(L)2] in a projection along [010]. C—H⋯O hydrogen bonds are shown as yellow and red dashed lines. H atoms not involved in intermolecular interactions have been omitted for clarity.
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C4—H4A⋯O2ii | 0.99 | 2.52 | 3.241 (3) | 129 |
| C6—H6B⋯O2ii | 0.98 | 2.47 | 3.418 (3) | 162 |
| C10—H10A⋯O1iii | 0.99 | 2.58 | 3.144 (3) | 116 |
| C12—H12B⋯O2iv | 0.98 | 2.59 | 3.372 (3) | 137 |
Symmetry codes: (ii)
; (iii)
; (iv)
.
Synthesis and crystallization
Preparation of N-acetylthiomorpholine (L)
Thiomorpholine (1.03 g, 0.010 mol) and triethylamine (1.03 g, 0.010 mol) in chloroform (20 mL) were placed in a one-neck round-bottomed flask and kept at 273 K. Then, acetic anhydride (1.02 g, 0.010 mol) was added dropwise. The reactant mixture was stirred for approximately one day. The orange liquid product was purified by using short column chromatography (silica gel, 90% n-hexane and 10% ethyl acetate, Rf = 0.28; yield 1.08 g, 74.5%). 1H NMR (300 MHz, CDCl3) / ppm: 3.860 (triplet, 2H, CH2-N), 3.719 (triplet, 2H, CH2-N), 2.614 (triplet, 2H, CH2-S), 2.597 (triplet, 2H, CH2-S), 2.086 (singlet, 3H, CH3); 13C NMR (300MHz, CDCl3) / ppm: 168.919 (C=O); 48.993, 43.972 (N—C); 27.248, 27.740 (S—C), 21.527(CH3)
Preparation of [CuI(L)2]n
An acetonitrile (2 mL) solution of L (0.08 g, 0.55 mmol) was allowed to mix with an acetonitrile (3 mL) solution of CuI (0.052 g, 0.27 mmol). The colorless precipitate was filtered and washed with diethyl ether/acetonitrile (3/1 v/v) solution (yield 0.116 g, 88.5%). Single crystals suitable for X-ray analysis were obtained by slow evaporation.
Refinement
Crystal data, data collection and structure refinement details are summarized in Table 3 ▸. All C-bound H atoms were positioned geometrically, with d(C—H) = 0.99 Å, U iso = 1.2U eq(C) for methylene, and d(C—H) = 0.98 Å, U iso = 1.5U eq(C) for methyl groups.
Table 3. Experimental details.
| Crystal data | |
| Chemical formula | [CuI(C6H11NOS)2] |
| M r | 480.87 |
| Crystal system, space group | Monoclinic, P21/n |
| Temperature (K) | 173 |
| a, b, c (Å) | 14.1513 (4), 7.6557 (2), 16.9423 (4) |
| β (°) | 113.805 (1) |
| V (Å3) | 1679.34 (8) |
| Z | 4 |
| Radiation type | Mo Kα |
| μ (mm−1) | 3.39 |
| Crystal size (mm) | 0.40 × 0.10 × 0.02 |
| Data collection | |
| Diffractometer | Bruker APEXII CCD |
| Absorption correction | Multi-scan (SADABS; Bruker, 2014 ▸) |
| T min, T max | 0.518, 0.746 |
| No. of measured, independent and observed [I > 2σ(I)] reflections | 12664, 3306, 3020 |
| R int | 0.023 |
| (sin θ/λ)max (Å−1) | 0.617 |
| Refinement | |
| R[F 2 > 2σ(F 2)], wR(F 2), S | 0.018, 0.045, 1.05 |
| No. of reflections | 3306 |
| No. of parameters | 183 |
| H-atom treatment | H-atom parameters constrained |
| Δρmax, Δρmin (e Å−3) | 0.51, −0.37 |
Supplementary Material
Crystal structure: contains datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S2056989016019794/wm5347sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989016019794/wm5347Isup2.hkl
CCDC reference: 1522053
Additional supporting information: crystallographic information; 3D view; checkCIF report
Acknowledgments
This research was supported by the Basic Science Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (No. 2015R1D1A4A01020317).
supplementary crystallographic information
Crystal data
| [CuI(C6H11NOS)2] | F(000) = 952 |
| Mr = 480.87 | Dx = 1.902 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| a = 14.1513 (4) Å | Cell parameters from 8258 reflections |
| b = 7.6557 (2) Å | θ = 2.4–27.4° |
| c = 16.9423 (4) Å | µ = 3.39 mm−1 |
| β = 113.805 (1)° | T = 173 K |
| V = 1679.34 (8) Å3 | Plate, colourless |
| Z = 4 | 0.40 × 0.10 × 0.02 mm |
Data collection
| Bruker APEXII CCD diffractometer | 3020 reflections with I > 2σ(I) |
| φ and ω scans | Rint = 0.023 |
| Absorption correction: multi-scan (SADABS; Bruker, 2014) | θmax = 26.0°, θmin = 1.6° |
| Tmin = 0.518, Tmax = 0.746 | h = −13→17 |
| 12664 measured reflections | k = −9→9 |
| 3306 independent reflections | l = −20→20 |
Refinement
| Refinement on F2 | 0 restraints |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.018 | H-atom parameters constrained |
| wR(F2) = 0.045 | w = 1/[σ2(Fo2) + (0.0221P)2 + 0.5521P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.003 |
| 3306 reflections | Δρmax = 0.51 e Å−3 |
| 183 parameters | Δρmin = −0.37 e Å−3 |
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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| Cu1 | 0.18899 (2) | 1.02851 (3) | 0.16379 (2) | 0.02035 (7) | |
| I1 | 0.22857 (2) | 1.36381 (2) | 0.18629 (2) | 0.02246 (6) | |
| S1 | 0.01447 (4) | 0.97167 (7) | 0.10384 (3) | 0.01843 (11) | |
| S2 | 0.27317 (4) | 0.95551 (7) | 0.07682 (3) | 0.01754 (11) | |
| O1 | −0.12671 (13) | 0.4134 (2) | 0.18413 (10) | 0.0306 (4) | |
| O2 | 0.55531 (13) | 0.4901 (2) | 0.13221 (10) | 0.0326 (4) | |
| N1 | −0.12119 (14) | 0.6992 (2) | 0.15212 (11) | 0.0222 (4) | |
| N2 | 0.41457 (14) | 0.6547 (2) | 0.05909 (11) | 0.0211 (4) | |
| C1 | −0.09223 (18) | 0.6587 (3) | 0.08061 (14) | 0.0261 (5) | |
| H1A | −0.1457 | 0.7049 | 0.0264 | 0.031* | |
| H1B | −0.0897 | 0.5303 | 0.0747 | 0.031* | |
| C2 | 0.01160 (17) | 0.7356 (3) | 0.09339 (15) | 0.0237 (5) | |
| H2A | 0.0279 | 0.7034 | 0.0437 | 0.028* | |
| H2B | 0.0656 | 0.6845 | 0.1459 | 0.028* | |
| C3 | −0.03090 (17) | 0.9830 (3) | 0.18944 (13) | 0.0204 (5) | |
| H3A | 0.0220 | 0.9323 | 0.2427 | 0.024* | |
| H3B | −0.0408 | 1.1068 | 0.2011 | 0.024* | |
| C4 | −0.13193 (17) | 0.8852 (3) | 0.16610 (14) | 0.0226 (5) | |
| H4A | −0.1559 | 0.8994 | 0.2131 | 0.027* | |
| H4B | −0.1849 | 0.9365 | 0.1130 | 0.027* | |
| C5 | −0.13845 (16) | 0.5668 (3) | 0.19871 (13) | 0.0227 (5) | |
| C6 | −0.1756 (2) | 0.6151 (3) | 0.26767 (15) | 0.0301 (5) | |
| H6A | −0.2461 | 0.6610 | 0.2406 | 0.045* | |
| H6B | −0.1300 | 0.7045 | 0.3054 | 0.045* | |
| H6C | −0.1748 | 0.5114 | 0.3018 | 0.045* | |
| C7 | 0.46423 (17) | 0.8128 (3) | 0.10528 (14) | 0.0241 (5) | |
| H7A | 0.4710 | 0.8983 | 0.0640 | 0.029* | |
| H7B | 0.5345 | 0.7841 | 0.1480 | 0.029* | |
| C8 | 0.40226 (17) | 0.8939 (3) | 0.15130 (14) | 0.0244 (5) | |
| H8A | 0.4389 | 0.9987 | 0.1833 | 0.029* | |
| H8B | 0.3973 | 0.8093 | 0.1937 | 0.029* | |
| C9 | 0.23472 (16) | 0.7451 (3) | 0.02483 (13) | 0.0195 (4) | |
| H9A | 0.2295 | 0.6596 | 0.0668 | 0.023* | |
| H9B | 0.1658 | 0.7552 | −0.0233 | 0.023* | |
| C10 | 0.31244 (17) | 0.6798 (3) | −0.00969 (14) | 0.0229 (5) | |
| H10A | 0.2879 | 0.5677 | −0.0403 | 0.027* | |
| H10B | 0.3172 | 0.7653 | −0.0518 | 0.027* | |
| C11 | 0.46543 (18) | 0.4999 (3) | 0.07934 (14) | 0.0234 (5) | |
| C12 | 0.4073 (2) | 0.3374 (3) | 0.03610 (18) | 0.0339 (6) | |
| H12A | 0.4529 | 0.2358 | 0.0560 | 0.051* | |
| H12B | 0.3837 | 0.3489 | −0.0266 | 0.051* | |
| H12C | 0.3475 | 0.3221 | 0.0508 | 0.051* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.02182 (15) | 0.01848 (14) | 0.02120 (14) | −0.00092 (11) | 0.00916 (12) | −0.00102 (10) |
| I1 | 0.03471 (10) | 0.01382 (8) | 0.01707 (8) | −0.00131 (6) | 0.00859 (7) | −0.00134 (5) |
| S1 | 0.0196 (3) | 0.0185 (3) | 0.0176 (2) | 0.0000 (2) | 0.0080 (2) | 0.00071 (19) |
| S2 | 0.0196 (3) | 0.0148 (2) | 0.0179 (2) | −0.0001 (2) | 0.0073 (2) | −0.00149 (19) |
| O1 | 0.0306 (9) | 0.0224 (9) | 0.0302 (9) | −0.0033 (7) | 0.0034 (7) | 0.0003 (7) |
| O2 | 0.0305 (10) | 0.0403 (10) | 0.0256 (9) | 0.0143 (8) | 0.0099 (8) | 0.0080 (7) |
| N1 | 0.0240 (10) | 0.0211 (10) | 0.0236 (9) | −0.0025 (8) | 0.0119 (8) | −0.0020 (7) |
| N2 | 0.0179 (9) | 0.0209 (10) | 0.0220 (9) | 0.0008 (7) | 0.0055 (8) | −0.0049 (7) |
| C1 | 0.0296 (13) | 0.0257 (12) | 0.0245 (12) | −0.0081 (10) | 0.0123 (10) | −0.0085 (9) |
| C2 | 0.0280 (12) | 0.0194 (11) | 0.0266 (11) | 0.0000 (10) | 0.0141 (10) | −0.0055 (9) |
| C3 | 0.0245 (12) | 0.0203 (11) | 0.0184 (10) | 0.0004 (9) | 0.0108 (9) | −0.0017 (8) |
| C4 | 0.0224 (12) | 0.0221 (12) | 0.0257 (11) | 0.0038 (9) | 0.0122 (10) | 0.0023 (9) |
| C5 | 0.0128 (11) | 0.0265 (12) | 0.0199 (11) | −0.0047 (9) | −0.0025 (9) | 0.0005 (9) |
| C6 | 0.0292 (13) | 0.0332 (14) | 0.0290 (12) | −0.0054 (11) | 0.0129 (11) | 0.0064 (10) |
| C7 | 0.0185 (11) | 0.0270 (12) | 0.0246 (11) | −0.0017 (10) | 0.0065 (9) | −0.0059 (9) |
| C8 | 0.0189 (12) | 0.0299 (12) | 0.0203 (11) | 0.0004 (10) | 0.0036 (9) | −0.0079 (9) |
| C9 | 0.0179 (11) | 0.0171 (10) | 0.0197 (10) | −0.0012 (9) | 0.0036 (9) | −0.0021 (8) |
| C10 | 0.0206 (11) | 0.0246 (11) | 0.0197 (11) | 0.0009 (9) | 0.0042 (9) | −0.0065 (9) |
| C11 | 0.0311 (13) | 0.0254 (12) | 0.0234 (11) | 0.0058 (10) | 0.0211 (11) | 0.0055 (9) |
| C12 | 0.0403 (15) | 0.0210 (12) | 0.0523 (16) | 0.0006 (11) | 0.0308 (13) | 0.0014 (11) |
Geometric parameters (Å, º)
| Cu1—S1 | 2.3012 (6) | C3—H3A | 0.9900 |
| Cu1—S2 | 2.3064 (6) | C3—H3B | 0.9900 |
| Cu1—I1 | 2.6221 (3) | C4—H4A | 0.9900 |
| Cu1—I1i | 2.6476 (3) | C4—H4B | 0.9900 |
| I1—Cu1ii | 2.6476 (3) | C5—C6 | 1.508 (3) |
| S1—C3 | 1.810 (2) | C6—H6A | 0.9800 |
| S1—C2 | 1.815 (2) | C6—H6B | 0.9800 |
| S2—C9 | 1.811 (2) | C6—H6C | 0.9800 |
| S2—C8 | 1.814 (2) | C7—C8 | 1.521 (3) |
| O1—C5 | 1.225 (3) | C7—H7A | 0.9900 |
| O2—C11 | 1.227 (3) | C7—H7B | 0.9900 |
| N1—C5 | 1.366 (3) | C8—H8A | 0.9900 |
| N1—C1 | 1.460 (3) | C8—H8B | 0.9900 |
| N1—C4 | 1.462 (3) | C9—C10 | 1.523 (3) |
| N2—C11 | 1.357 (3) | C9—H9A | 0.9900 |
| N2—C10 | 1.457 (3) | C9—H9B | 0.9900 |
| N2—C7 | 1.459 (3) | C10—H10A | 0.9900 |
| C1—C2 | 1.515 (3) | C10—H10B | 0.9900 |
| C1—H1A | 0.9900 | C11—C12 | 1.508 (3) |
| C1—H1B | 0.9900 | C12—H12A | 0.9800 |
| C2—H2A | 0.9900 | C12—H12B | 0.9800 |
| C2—H2B | 0.9900 | C12—H12C | 0.9800 |
| C3—C4 | 1.518 (3) | ||
| S1—Cu1—S2 | 114.28 (2) | O1—C5—N1 | 121.6 (2) |
| S1—Cu1—I1 | 112.179 (17) | O1—C5—C6 | 120.6 (2) |
| S2—Cu1—I1 | 101.246 (16) | N1—C5—C6 | 117.7 (2) |
| S1—Cu1—I1i | 108.190 (16) | C5—C6—H6A | 109.5 |
| S2—Cu1—I1i | 110.870 (16) | C5—C6—H6B | 109.5 |
| I1—Cu1—I1i | 109.949 (9) | H6A—C6—H6B | 109.5 |
| Cu1—I1—Cu1ii | 126.245 (8) | C5—C6—H6C | 109.5 |
| C3—S1—C2 | 97.16 (10) | H6A—C6—H6C | 109.5 |
| C3—S1—Cu1 | 107.58 (7) | H6B—C6—H6C | 109.5 |
| C2—S1—Cu1 | 102.08 (7) | N2—C7—C8 | 111.16 (18) |
| C9—S2—C8 | 97.32 (10) | N2—C7—H7A | 109.4 |
| C9—S2—Cu1 | 113.27 (7) | C8—C7—H7A | 109.4 |
| C8—S2—Cu1 | 104.68 (7) | N2—C7—H7B | 109.4 |
| C5—N1—C1 | 119.82 (18) | C8—C7—H7B | 109.4 |
| C5—N1—C4 | 125.09 (18) | H7A—C7—H7B | 108.0 |
| C1—N1—C4 | 115.07 (17) | C7—C8—S2 | 112.12 (15) |
| C11—N2—C10 | 124.83 (18) | C7—C8—H8A | 109.2 |
| C11—N2—C7 | 119.84 (18) | S2—C8—H8A | 109.2 |
| C10—N2—C7 | 115.28 (17) | C7—C8—H8B | 109.2 |
| N1—C1—C2 | 112.30 (18) | S2—C8—H8B | 109.2 |
| N1—C1—H1A | 109.1 | H8A—C8—H8B | 107.9 |
| C2—C1—H1A | 109.1 | C10—C9—S2 | 110.89 (15) |
| N1—C1—H1B | 109.1 | C10—C9—H9A | 109.5 |
| C2—C1—H1B | 109.1 | S2—C9—H9A | 109.5 |
| H1A—C1—H1B | 107.9 | C10—C9—H9B | 109.5 |
| C1—C2—S1 | 112.54 (16) | S2—C9—H9B | 109.5 |
| C1—C2—H2A | 109.1 | H9A—C9—H9B | 108.0 |
| S1—C2—H2A | 109.1 | N2—C10—C9 | 111.90 (17) |
| C1—C2—H2B | 109.1 | N2—C10—H10A | 109.2 |
| S1—C2—H2B | 109.1 | C9—C10—H10A | 109.2 |
| H2A—C2—H2B | 107.8 | N2—C10—H10B | 109.2 |
| C4—C3—S1 | 111.67 (14) | C9—C10—H10B | 109.2 |
| C4—C3—H3A | 109.3 | H10A—C10—H10B | 107.9 |
| S1—C3—H3A | 109.3 | O2—C11—N2 | 121.7 (2) |
| C4—C3—H3B | 109.3 | O2—C11—C12 | 120.4 (2) |
| S1—C3—H3B | 109.3 | N2—C11—C12 | 117.9 (2) |
| H3A—C3—H3B | 107.9 | C11—C12—H12A | 109.5 |
| N1—C4—C3 | 111.95 (18) | C11—C12—H12B | 109.5 |
| N1—C4—H4A | 109.2 | H12A—C12—H12B | 109.5 |
| C3—C4—H4A | 109.2 | C11—C12—H12C | 109.5 |
| N1—C4—H4B | 109.2 | H12A—C12—H12C | 109.5 |
| C3—C4—H4B | 109.2 | H12B—C12—H12C | 109.5 |
| H4A—C4—H4B | 107.9 | ||
| C5—N1—C1—C2 | −120.4 (2) | C11—N2—C7—C8 | −120.0 (2) |
| C4—N1—C1—C2 | 61.1 (3) | C10—N2—C7—C8 | 62.5 (2) |
| N1—C1—C2—S1 | −59.4 (2) | N2—C7—C8—S2 | −60.5 (2) |
| C3—S1—C2—C1 | 52.97 (17) | C9—S2—C8—C7 | 54.16 (18) |
| Cu1—S1—C2—C1 | 162.73 (14) | Cu1—S2—C8—C7 | 170.60 (15) |
| C2—S1—C3—C4 | −53.85 (17) | C8—S2—C9—C10 | −54.05 (16) |
| Cu1—S1—C3—C4 | −158.97 (13) | Cu1—S2—C9—C10 | −163.52 (12) |
| C5—N1—C4—C3 | 119.1 (2) | C11—N2—C10—C9 | 118.9 (2) |
| C1—N1—C4—C3 | −62.5 (2) | C7—N2—C10—C9 | −63.8 (2) |
| S1—C3—C4—N1 | 61.7 (2) | S2—C9—C10—N2 | 61.7 (2) |
| C1—N1—C5—O1 | 2.6 (3) | C10—N2—C11—O2 | 172.7 (2) |
| C4—N1—C5—O1 | −179.1 (2) | C7—N2—C11—O2 | −4.6 (3) |
| C1—N1—C5—C6 | −175.7 (2) | C10—N2—C11—C12 | −8.6 (3) |
| C4—N1—C5—C6 | 2.6 (3) | C7—N2—C11—C12 | 174.10 (19) |
Symmetry codes: (i) −x+1/2, y−1/2, −z+1/2; (ii) −x+1/2, y+1/2, −z+1/2.
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C4—H4A···O2ii | 0.99 | 2.52 | 3.241 (3) | 129 |
| C6—H6B···O2ii | 0.98 | 2.47 | 3.418 (3) | 162 |
| C10—H10A···O1iii | 0.99 | 2.58 | 3.144 (3) | 116 |
| C12—H12B···O2iv | 0.98 | 2.59 | 3.372 (3) | 137 |
Symmetry codes: (ii) −x+1/2, y+1/2, −z+1/2; (iii) −x, −y+1, −z; (iv) −x+1, −y+1, −z.
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 datablock(s) I, New_Global_Publ_Block. DOI: 10.1107/S2056989016019794/wm5347sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989016019794/wm5347Isup2.hkl
CCDC reference: 1522053
Additional supporting information: crystallographic information; 3D view; checkCIF report



