Abstract
In the title molecule, C16H15BrN2S2, the central imidazo[2,1-b]thiazole fragment is almost planar (r.m.s. deviation = 0.012 Å), and the fused 5,6,7,8-tetrahydrobenzene ring adopts an unsymmetrical half-chair conformation. The dihedral angle between the imidazo[2,1-b]thiazole and benzene planes is 18.25 (4)°. The terminal methylsulfanyl substituent lies practically within the benzene plane [the dihedral angle between the corresponding planes is 7.20 (10)°] and is turned toward the C—Br bond. In the crystal, molecules form infinite chains along [100] via secondary Br⋯N interactions [3.1861 (16) Å]. The chains are arranged at van der Waals distances.
Related literature
For applications of imidazo[2,1-b][1,3]benzothiazoles, see: Ager et al. (1988 ▶); Sanfilippo et al. (1988 ▶); Barchéchath et al. (2005 ▶); Andreani et al. (2008 ▶); Chao et al. (2009 ▶); Kumbhare et al. (2011 ▶); Chandak et al. (2013 ▶). For the crystal structures of related compounds, see: Landreau et al. (2002 ▶); Adib et al. (2008 ▶); Fun, Asik et al. (2011 ▶); Fun, Hemamalini et al. (2011 ▶); Ghabbour et al. (2012 ▶); Bunev et al. (2013 ▶, 2014 ▶).
Experimental
Crystal data
C16H15BrN2S2
M r = 379.34
Triclinic,
a = 7.3132 (3) Å
b = 7.5663 (3) Å
c = 14.4543 (7) Å
α = 95.033 (1)°
β = 97.188 (1)°
γ = 101.938 (1)°
V = 771.03 (6) Å3
Z = 2
Mo Kα radiation
μ = 2.93 mm−1
T = 120 K
0.15 × 0.10 × 0.10 mm
Data collection
Bruker APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2003 ▶) T min = 0.668, T max = 0.758
10352 measured reflections
4508 independent reflections
3927 reflections with I > 2σ(I)
R int = 0.025
Refinement
R[F 2 > 2σ(F 2)] = 0.030
wR(F 2) = 0.073
S = 1.05
4508 reflections
191 parameters
H-atom parameters constrained
Δρmax = 0.67 e Å−3
Δρmin = −0.32 e Å−3
Data collection: APEX2 (Bruker, 2005 ▶); cell refinement: SAINT (Bruker, 2001 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814008976/rk2426sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814008976/rk2426Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536814008976/rk2426Isup3.cml
CCDC reference: 998505
Additional supporting information: crystallographic information; 3D view; checkCIF report
Acknowledgments
The authors are grateful to the Ministry of Education and Science of the Russian Federation (State program No. 426).
supplementary crystallographic information
1. Comment
Imidazo[2,1–b][1,3]benzothiazole are of great interest due to their biological properties. These compounds and their derivatives demonstrate the antitumor (Andreani et al., 2008), antiallergic (Ager et al., 1988), anesthetic (Sanfilippo et al., 1988) and anti–cancer (Kumbhare et al., 2011) activities as well as the inhibition activity of apoptosis in testiculargerm cells (Chandak et al., 2013), lymphocytes (Barchéchath et al., 2005), and FMS–like tyrosine kinase–3 (FLT3) (Chao et al., 2009).
In this work, a new halogensubstituted 5,6,7,8–tetrahydrobenzo[d]imidazo[2,1–b]thiazole, C16H15BrN2S2, I, was prepared by the reaction of 5,6,7,8–tetrahydrobenzo[d]imidazo[2,1–b]thiazole with bromine at room temperature (Fig. 1), and its structure was unambiguously established by the X–ray diffraction study (Fig. 2).
In the title molecule (I) the central imidazo[2,1–b]thiazole fragment is almost planar (r.m.s. deviation = 0.012 Å), and the fused 5,6,7,8-tetrahydrobenzene ring adopts an unsymmetrical half–chair conformation (the C6 and C7 carbon atoms are out of the plane passed through the other atoms of the ring by -0.246 (2) and 0.508 (2) Å, respectively). The bond lengths and angles within the molecule of I are in a good agreement with those found in the related compounds (Landreau et al., 2002; Adib et al., 2008; Fun, Asik et al., 2011; Fun, Hemamalini et al., 2011; Ghabbour et al., 2012; Bunev et al., 2013, 2014). The dihedral angle between the imidazo[2,1–b]thiazole and benzene planes is 18.25 (4)°. The terminal methylthio substituent lies practically within the benzene plane (the dihedral angle between the corresponding planes is 7.20 (10)°) and is turned toward the C—Br bond.
In the crystal, the molecules of I form infinite chains along [100] by intermolecular secondary Br1···N1i interactions (3.1861 (16) Å) (Fig. 3). The chains are arranged at van der Waals distances. Symmetry code: (i) 1 + x, y, z.
2. Experimental
A solution of bromine (139 µL, 430.4 mg, 2.69 mmol) in dry CHCl3 (10 mL) was added to a solutions 2–(4–(methylthio)phenyl)–5,6,7,8–tetrahydrobenzo[d]imidazo[2,1–b]thiazole (808.3 mg, 2.69 mmol) in dry CHCl3 (30 mL). The reaction mixture was stirred at room temperature for 3 h. the solvent was evaporated from the reaction mixture on rotavapor. The crude product was diluted with 5% solution Na2CO3 in water (25 mL). The precipitate was filtered and crystallized from DMF. Yield is 75%. The single–crystal of the product I was obtained by slow crystallization from DMF. M.p. = 439–441 K. IR (KBr), ν/cm-1: 3131, 3073, 1580, 1523, 1501, 1337, 1144, 815, 714. 1H NMR (600 MHz, DMSO–d6, 304 K): 7.63 (d, 2H, J = 8.9), 7.54 (d, 2H, J = 8.9), 3.39–3.33 (m, 2H), 3.02–2.96 (m, 2H), 2.45 (s, 3H), 1.91–1.81 (m, 4H). Anal. Calcd for C16H15BrN2S: C, 50.66; H, 3.99. Found: C, 50.57; H, 4.08.
3. Refinement
All hydrogen atoms were placed in the calculated positions with C—H = 0.95–0.99 Å and refined in the riding model with fixed isotropic displacement parameters: Uiso(H) = 1.5Ueq(C) for the methyl group and Uiso(H) = 1.2Ueq(C) for the other groups.
Figures
Fig. 1.

The synthesis of 3-bromo-2-[4-(methylsulfanyl)phenyl]-5,6,7,8-tetrahydro-1,3-benzothiazolo[3,2-a]imidazole.
Fig. 2.

Molecular structure of I. Displacement ellipsoids are presented at the 50% probability level. H atoms are depicted as small spheres of arbitrary radius.
Fig. 3.
A portion of the crystal structure of I demonstrating the chains along [100]. The intermolecular secondary Br···N interactions are depicted by dashed lines.
Crystal data
| C16H15BrN2S2 | Z = 2 |
| Mr = 379.34 | F(000) = 384 |
| Triclinic, P1 | Dx = 1.634 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 7.3132 (3) Å | Cell parameters from 4428 reflections |
| b = 7.5663 (3) Å | θ = 2.8–32.3° |
| c = 14.4543 (7) Å | µ = 2.93 mm−1 |
| α = 95.033 (1)° | T = 120 K |
| β = 97.188 (1)° | Prism, colourless |
| γ = 101.938 (1)° | 0.15 × 0.10 × 0.10 mm |
| V = 771.03 (6) Å3 |
Data collection
| Bruker APEXII CCD diffractometer | 4508 independent reflections |
| Radiation source: fine-focus sealed tube | 3927 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.025 |
| φ and ω scans | θmax = 30.0°, θmin = 2.8° |
| Absorption correction: multi-scan (SADABS; Bruker, 2003) | h = −10→10 |
| Tmin = 0.668, Tmax = 0.758 | k = −10→10 |
| 10352 measured reflections | l = −20→20 |
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) = 0.073 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0377P)2 + 0.1351P] where P = (Fo2 + 2Fc2)/3 |
| 4508 reflections | (Δ/σ)max = 0.001 |
| 191 parameters | Δρmax = 0.67 e Å−3 |
| 0 restraints | Δρmin = −0.32 e Å−3 |
Special details
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
| Br1 | 0.52846 (2) | 0.33371 (2) | 0.103656 (13) | 0.01782 (6) | |
| S1 | 0.31673 (8) | 0.75383 (8) | 0.55165 (4) | 0.02712 (12) | |
| N1 | −0.0318 (2) | 0.3490 (2) | 0.10823 (11) | 0.0169 (3) | |
| C2 | 0.1565 (3) | 0.3866 (2) | 0.15151 (13) | 0.0150 (3) | |
| C3 | 0.2697 (2) | 0.3284 (2) | 0.09002 (13) | 0.0146 (3) | |
| N4 | 0.1494 (2) | 0.2541 (2) | 0.00724 (10) | 0.0136 (3) | |
| C4A | 0.1551 (3) | 0.1754 (2) | −0.08424 (13) | 0.0147 (3) | |
| C5 | 0.3302 (3) | 0.1399 (2) | −0.11797 (13) | 0.0159 (3) | |
| H5A | 0.3921 | 0.0696 | −0.0739 | 0.019* | |
| H5B | 0.4195 | 0.2568 | −0.1199 | 0.019* | |
| C6 | 0.2819 (3) | 0.0326 (3) | −0.21646 (14) | 0.0194 (4) | |
| H6A | 0.3978 | 0.0462 | −0.2464 | 0.023* | |
| H6B | 0.2372 | −0.0981 | −0.2106 | 0.023* | |
| C7 | 0.1308 (3) | 0.0964 (3) | −0.27918 (13) | 0.0208 (4) | |
| H7A | 0.1110 | 0.0295 | −0.3429 | 0.025* | |
| H7B | 0.1735 | 0.2276 | −0.2844 | 0.025* | |
| C8 | −0.0560 (3) | 0.0635 (3) | −0.23845 (13) | 0.0186 (4) | |
| H8A | −0.1458 | 0.1253 | −0.2726 | 0.022* | |
| H8B | −0.1133 | −0.0684 | −0.2457 | 0.022* | |
| C8A | −0.0175 (3) | 0.1366 (2) | −0.13656 (13) | 0.0154 (3) | |
| S9 | −0.19453 (6) | 0.18940 (6) | −0.07481 (3) | 0.01700 (10) | |
| C9A | −0.0272 (2) | 0.2722 (2) | 0.02379 (13) | 0.0153 (3) | |
| C10 | 0.2059 (3) | 0.4782 (2) | 0.24789 (13) | 0.0164 (3) | |
| C11 | 0.0607 (3) | 0.4836 (3) | 0.30255 (14) | 0.0191 (4) | |
| H11 | −0.0658 | 0.4267 | 0.2767 | 0.023* | |
| C12 | 0.0991 (3) | 0.5705 (3) | 0.39362 (14) | 0.0204 (4) | |
| H12 | −0.0014 | 0.5733 | 0.4291 | 0.024* | |
| C13 | 0.2850 (3) | 0.6542 (3) | 0.43388 (13) | 0.0199 (4) | |
| C14 | 0.4292 (3) | 0.6527 (3) | 0.37994 (14) | 0.0232 (4) | |
| H14 | 0.5554 | 0.7108 | 0.4058 | 0.028* | |
| C15 | 0.3898 (3) | 0.5664 (3) | 0.28802 (14) | 0.0217 (4) | |
| H15 | 0.4900 | 0.5676 | 0.2520 | 0.026* | |
| C16 | 0.5684 (3) | 0.8198 (3) | 0.58283 (16) | 0.0302 (5) | |
| H16A | 0.6001 | 0.8615 | 0.6502 | 0.045* | |
| H16B | 0.6187 | 0.9185 | 0.5472 | 0.045* | |
| H16C | 0.6242 | 0.7154 | 0.5682 | 0.045* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1 | 0.01313 (9) | 0.02030 (10) | 0.01932 (10) | 0.00599 (7) | −0.00109 (6) | −0.00219 (7) |
| S1 | 0.0271 (3) | 0.0327 (3) | 0.0173 (2) | 0.0007 (2) | 0.0029 (2) | −0.0057 (2) |
| N1 | 0.0157 (7) | 0.0163 (7) | 0.0187 (8) | 0.0026 (6) | 0.0042 (6) | 0.0015 (6) |
| C2 | 0.0154 (8) | 0.0140 (8) | 0.0158 (8) | 0.0029 (7) | 0.0033 (7) | 0.0023 (6) |
| C3 | 0.0134 (8) | 0.0155 (8) | 0.0154 (8) | 0.0051 (7) | 0.0010 (6) | 0.0008 (6) |
| N4 | 0.0109 (7) | 0.0153 (7) | 0.0145 (7) | 0.0034 (6) | 0.0011 (5) | 0.0010 (6) |
| C4A | 0.0145 (8) | 0.0121 (8) | 0.0175 (9) | 0.0030 (6) | 0.0023 (7) | 0.0016 (6) |
| C5 | 0.0140 (8) | 0.0160 (8) | 0.0186 (9) | 0.0050 (7) | 0.0036 (7) | 0.0004 (7) |
| C6 | 0.0195 (9) | 0.0217 (9) | 0.0179 (9) | 0.0083 (8) | 0.0030 (7) | −0.0010 (7) |
| C7 | 0.0221 (9) | 0.0247 (10) | 0.0159 (9) | 0.0070 (8) | 0.0025 (7) | −0.0004 (7) |
| C8 | 0.0178 (9) | 0.0193 (9) | 0.0167 (9) | 0.0036 (7) | −0.0016 (7) | −0.0013 (7) |
| C8A | 0.0136 (8) | 0.0140 (8) | 0.0182 (8) | 0.0025 (7) | 0.0028 (7) | 0.0007 (6) |
| S9 | 0.01080 (19) | 0.0210 (2) | 0.0186 (2) | 0.00355 (17) | 0.00092 (16) | 0.00057 (17) |
| C9A | 0.0119 (8) | 0.0160 (8) | 0.0186 (8) | 0.0030 (7) | 0.0033 (7) | 0.0031 (7) |
| C10 | 0.0192 (9) | 0.0129 (8) | 0.0167 (8) | 0.0027 (7) | 0.0028 (7) | 0.0010 (6) |
| C11 | 0.0176 (9) | 0.0174 (9) | 0.0208 (9) | 0.0017 (7) | 0.0021 (7) | 0.0001 (7) |
| C12 | 0.0211 (9) | 0.0208 (9) | 0.0193 (9) | 0.0037 (8) | 0.0051 (7) | 0.0010 (7) |
| C13 | 0.0252 (10) | 0.0187 (9) | 0.0145 (8) | 0.0037 (8) | 0.0019 (7) | −0.0011 (7) |
| C14 | 0.0196 (9) | 0.0252 (10) | 0.0208 (10) | −0.0006 (8) | 0.0014 (7) | −0.0028 (8) |
| C15 | 0.0205 (9) | 0.0235 (10) | 0.0194 (9) | 0.0009 (8) | 0.0063 (7) | −0.0012 (8) |
| C16 | 0.0286 (11) | 0.0311 (12) | 0.0249 (11) | −0.0003 (9) | −0.0030 (9) | −0.0030 (9) |
Geometric parameters (Å, º)
| Br1—C3 | 1.8693 (18) | C7—H7B | 0.9900 |
| S1—C13 | 1.7673 (19) | C8—C8A | 1.498 (3) |
| S1—C16 | 1.793 (2) | C8—H8A | 0.9900 |
| N1—C9A | 1.312 (2) | C8—H8B | 0.9900 |
| N1—C2 | 1.400 (2) | C8A—S9 | 1.7529 (19) |
| C2—C3 | 1.391 (2) | S9—C9A | 1.7354 (19) |
| C2—C10 | 1.467 (3) | C10—C15 | 1.399 (3) |
| C3—N4 | 1.391 (2) | C10—C11 | 1.405 (3) |
| N4—C9A | 1.374 (2) | C11—C12 | 1.387 (3) |
| N4—C4A | 1.411 (2) | C11—H11 | 0.9500 |
| C4A—C8A | 1.349 (2) | C12—C13 | 1.403 (3) |
| C4A—C5 | 1.492 (2) | C12—H12 | 0.9500 |
| C5—C6 | 1.537 (3) | C13—C14 | 1.389 (3) |
| C5—H5A | 0.9900 | C14—C15 | 1.396 (3) |
| C5—H5B | 0.9900 | C14—H14 | 0.9500 |
| C6—C7 | 1.524 (3) | C15—H15 | 0.9500 |
| C6—H6A | 0.9900 | C16—H16A | 0.9800 |
| C6—H6B | 0.9900 | C16—H16B | 0.9800 |
| C7—C8 | 1.537 (3) | C16—H16C | 0.9800 |
| C7—H7A | 0.9900 | ||
| C13—S1—C16 | 103.71 (10) | C8A—C8—H8B | 109.9 |
| C9A—N1—C2 | 104.13 (15) | C7—C8—H8B | 109.9 |
| C3—C2—N1 | 110.13 (16) | H8A—C8—H8B | 108.3 |
| C3—C2—C10 | 130.54 (17) | C4A—C8A—C8 | 124.20 (17) |
| N1—C2—C10 | 119.33 (16) | C4A—C8A—S9 | 113.31 (14) |
| C2—C3—N4 | 106.03 (15) | C8—C8A—S9 | 122.44 (13) |
| C2—C3—Br1 | 131.99 (14) | C9A—S9—C8A | 89.99 (9) |
| N4—C3—Br1 | 121.98 (13) | N1—C9A—N4 | 114.32 (16) |
| C9A—N4—C3 | 105.38 (15) | N1—C9A—S9 | 134.58 (14) |
| C9A—N4—C4A | 114.32 (15) | N4—C9A—S9 | 111.08 (13) |
| C3—N4—C4A | 140.26 (16) | C15—C10—C11 | 117.62 (17) |
| C8A—C4A—N4 | 111.27 (16) | C15—C10—C2 | 123.61 (17) |
| C8A—C4A—C5 | 124.77 (17) | C11—C10—C2 | 118.73 (17) |
| N4—C4A—C5 | 123.97 (16) | C12—C11—C10 | 121.15 (18) |
| C4A—C5—C6 | 110.25 (15) | C12—C11—H11 | 119.4 |
| C4A—C5—H5A | 109.6 | C10—C11—H11 | 119.4 |
| C6—C5—H5A | 109.6 | C11—C12—C13 | 120.61 (18) |
| C4A—C5—H5B | 109.6 | C11—C12—H12 | 119.7 |
| C6—C5—H5B | 109.6 | C13—C12—H12 | 119.7 |
| H5A—C5—H5B | 108.1 | C14—C13—C12 | 118.75 (18) |
| C7—C6—C5 | 112.55 (15) | C14—C13—S1 | 124.86 (16) |
| C7—C6—H6A | 109.1 | C12—C13—S1 | 116.38 (15) |
| C5—C6—H6A | 109.1 | C13—C14—C15 | 120.45 (19) |
| C7—C6—H6B | 109.1 | C13—C14—H14 | 119.8 |
| C5—C6—H6B | 109.1 | C15—C14—H14 | 119.8 |
| H6A—C6—H6B | 107.8 | C14—C15—C10 | 121.38 (18) |
| C6—C7—C8 | 110.44 (16) | C14—C15—H15 | 119.3 |
| C6—C7—H7A | 109.6 | C10—C15—H15 | 119.3 |
| C8—C7—H7A | 109.6 | S1—C16—H16A | 109.5 |
| C6—C7—H7B | 109.6 | S1—C16—H16B | 109.5 |
| C8—C7—H7B | 109.6 | H16A—C16—H16B | 109.5 |
| H7A—C7—H7B | 108.1 | S1—C16—H16C | 109.5 |
| C8A—C8—C7 | 109.02 (15) | H16A—C16—H16C | 109.5 |
| C8A—C8—H8A | 109.9 | H16B—C16—H16C | 109.5 |
| C7—C8—H8A | 109.9 | ||
| C9A—N1—C2—C3 | −0.4 (2) | C8—C8A—S9—C9A | −175.86 (16) |
| C9A—N1—C2—C10 | 178.60 (16) | C2—N1—C9A—N4 | 0.5 (2) |
| N1—C2—C3—N4 | 0.2 (2) | C2—N1—C9A—S9 | −178.31 (16) |
| C10—C2—C3—N4 | −178.66 (17) | C3—N4—C9A—N1 | −0.4 (2) |
| N1—C2—C3—Br1 | −178.84 (14) | C4A—N4—C9A—N1 | −178.63 (15) |
| C10—C2—C3—Br1 | 2.3 (3) | C3—N4—C9A—S9 | 178.71 (12) |
| C2—C3—N4—C9A | 0.07 (19) | C4A—N4—C9A—S9 | 0.45 (19) |
| Br1—C3—N4—C9A | 179.24 (12) | C8A—S9—C9A—N1 | 177.7 (2) |
| C2—C3—N4—C4A | 177.6 (2) | C8A—S9—C9A—N4 | −1.11 (14) |
| Br1—C3—N4—C4A | −3.2 (3) | C3—C2—C10—C15 | 17.2 (3) |
| C9A—N4—C4A—C8A | 0.7 (2) | N1—C2—C10—C15 | −161.53 (18) |
| C3—N4—C4A—C8A | −176.6 (2) | C3—C2—C10—C11 | −164.91 (19) |
| C9A—N4—C4A—C5 | −179.12 (16) | N1—C2—C10—C11 | 16.3 (3) |
| C3—N4—C4A—C5 | 3.5 (3) | C15—C10—C11—C12 | −1.1 (3) |
| C8A—C4A—C5—C6 | −6.7 (3) | C2—C10—C11—C12 | −179.12 (17) |
| N4—C4A—C5—C6 | 173.18 (16) | C10—C11—C12—C13 | −0.5 (3) |
| C4A—C5—C6—C7 | 39.6 (2) | C11—C12—C13—C14 | 1.7 (3) |
| C5—C6—C7—C8 | −63.1 (2) | C11—C12—C13—S1 | −177.96 (15) |
| C6—C7—C8—C8A | 49.1 (2) | C16—S1—C13—C14 | −6.6 (2) |
| N4—C4A—C8A—C8 | 175.79 (16) | C16—S1—C13—C12 | 173.04 (16) |
| C5—C4A—C8A—C8 | −4.3 (3) | C12—C13—C14—C15 | −1.2 (3) |
| N4—C4A—C8A—S9 | −1.6 (2) | S1—C13—C14—C15 | 178.47 (16) |
| C5—C4A—C8A—S9 | 178.26 (14) | C13—C14—C15—C10 | −0.5 (3) |
| C7—C8—C8A—C4A | −17.4 (3) | C11—C10—C15—C14 | 1.7 (3) |
| C7—C8—C8A—S9 | 159.79 (14) | C2—C10—C15—C14 | 179.55 (18) |
| C4A—C8A—S9—C9A | 1.59 (15) |
Footnotes
Supporting information for this paper is available from the IUCr electronic archives (Reference: RK2426).
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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) global, I. DOI: 10.1107/S1600536814008976/rk2426sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814008976/rk2426Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536814008976/rk2426Isup3.cml
CCDC reference: 998505
Additional supporting information: crystallographic information; 3D view; checkCIF report

