Abstract
In the title compound, C18H17ClO2S, the dihedral angle between the mean planes of the benzofuran ring system and the methylphenyl ring is 14.50 (4)°. The centroid–centroid distances between the benzene and the methylphenyl rings are 3.827 (2) and 3.741 (2) Å, while the centroid–centroid distance between the furan and methylphenyl rings is 3.843 (2) Å. These distances indicate π–π interactions; on the other hand, the interplanar angles between the benzene and methylphenyl rings, and between the furan and methylphenyl rings are 13.89 (4) and 15.53 (4)°, respectively. In the crystal, the molecules stack along the a-axis direction.
Related literature
For background information about related compounds and their crystal structures, see Choi et al. (2010a
▶,b
▶). For π–π stacking in metal complexes with aromatic nitrogen ligands, see: Janiak (2000 ▶).
Experimental
Crystal data
C18H17ClO2S
M r = 332.83
Triclinic,
a = 7.3638 (5) Å
b = 10.2524 (6) Å
c = 11.8335 (7) Å
α = 68.949 (3)°
β = 89.362 (3)°
γ = 71.460 (3)°
V = 785.11 (8) Å3
Z = 2
Mo Kα radiation
μ = 0.38 mm−1
T = 173 K
0.46 × 0.37 × 0.33 mm
Data collection
Bruker SMART APEXII CCD diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.691, T max = 0.746
13937 measured reflections
3759 independent reflections
3348 reflections with I > 2σ(I)
R int = 0.031
Refinement
R[F 2 > 2σ(F 2)] = 0.034
wR(F 2) = 0.100
S = 1.06
3759 reflections
203 parameters
H-atom parameters constrained
Δρmax = 0.31 e Å−3
Δρmin = −0.29 e Å−3
Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; 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 ▶) and DIAMOND (Brandenburg, 1998 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) I. DOI: 10.1107/S1600536814005601/fb2296sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814005601/fb2296Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536814005601/fb2296Isup3.cml
CCDC reference: 991267
Additional supporting information: crystallographic information; 3D view; checkCIF report
supplementary crystallographic information
1. Comment
As a part of our ongoing study of 5-chloro-3-ethylsulfinyl-7-methyl-1-benzofuran derivatives which contain 4-fluorophenyl and 4 iodophenyl substituents in the 2-position (Choi et al. (2010a,b) for the F and I-compound, respectively), we report the crystal structure of the title compound.
In the title molecule (Fig. 1), the benzofuran unit is essentially planar, with the mean deviation from the least-squares plane defined by the nine constituent atoms which equals to 0.016 (1) Å. The 4-methylphenyl ring is also essentially planar, with the mean deviation of 0.004 (1) Å from the least-squares plane defined by the six core-ring atoms. The dihedral angle between the benzofuran ring system and the core of the 4-methylphenyl rings is 14.50 (4)°.
Let the centroid names Cg1, Cg2 and Cg3 be assigned to the benzene ring (C2–C7), the furan ring (C1/C2/C7/O1/C8) and the core of 4-methylphenyl ring (C10–C15), respectively: The centroid–centroid separations of Cg1···Cg3i, Cg1···Cg3ii and Cg2···Cg3i are 3.827 (2), 3.741 (2) and 3.843 (2) Å, respectively. (The symmetry codes are: (i) -x + 1, -y + 1, -z + 1; (ii) -x, -y + 1, -z + 1.)
The interplanar angles between the benzene and the core of 4-methylphenyl ring and between the furan and the core of 4-methylphenyl ring equal to 13.89 (4) and 15.53 (4)°, respectively. These angles are quite large for the rings being in π-electron···π-electron interactions as it follows from the study by Janiak (2000) who investigated π–π stacking in metal complexes with aromatic nitrogen ligands. According to Fig. 8 of Janiak's study, the interplanar angles between the rings that are involved in π-electron···π-electron interactions are less than 10° in overwhelming majority of cases.
2. Experimental
3-Chloroperoxybenzoic acid (77%, 224 mg, 1.0 mmol) was added in small portions to the stirred solution of 5-chloro-3-ethylsulfanyl-7-methyl-2-(4-methylphenyl)-1-benzofuran (285 mg, 0.9 mmol) in dichloromethane (30 ml) at 273 K. The mixture was washed with saturated sodium hydrogen carbonate solution after having been stirred at room temperature for 4h. The organic layer was separated, dried over magnesium sulfate, filtered and concentrated at reduced pressure.
The residue was purified by column chromatography (hexane–ethyl acetate, 1:1v/v) to afford the title compound as a colourless solid [yield 71%, m.p. 392–393 K; Rf = 0.56 (hexane–ethyl acetate, 1:1 v/v)]. Single crystals suitable for X-ray diffraction were prepared by slow evaporation of the 5% solution of the title compound in acetone at room temperature. The average crystal size was approximately 1.1 × 1.3 × 0.8 mm. (The measured crystal was cut from a large one.) The crystals are soluble in polar solvents.
3. Refinement
All the hydrogen atoms were observed in the difference electron density map. However, they were situated into the idealized positions and refined using a riding-model approximation. The used constraints: C—H = 0.95 Å for aryl, 0.98 Å for methyl and for 0.99 Å for methylene H atoms. Uiso(H) = 1.2Ueq(C) for aryl and methylene, while 1.5Ueq(C) for the methyl H atoms. The positions of methyl hydrogens were optimized using the SHELXL-97's command AFIX 137 (Sheldrick, 2008).
Figures
Fig. 1.
The title molecule with the atom numbering scheme. The displacement ellipsoids are drawn at the 50% probability level. The hydrogen atoms are presented as small spheres of arbitrary radius.
Fig. 2.
A view of possible π···π interactions (dotted lines) in the crystal structure of the title compound. The H-atoms have been omitted for clarity. [Symmetry codes: (i) -x + 1, -y + 1, -z + 1; (ii) -x, -y + 1, -z + 1.]
Crystal data
| C18H17ClO2S | Z = 2 |
| Mr = 332.83 | F(000) = 348 |
| Triclinic, P1 | Dx = 1.408 Mg m−3 |
| Hall symbol: -P 1 | Melting point = 392–393 K |
| a = 7.3638 (5) Å | Mo Kα radiation, λ = 0.71073 Å |
| b = 10.2524 (6) Å | Cell parameters from 8286 reflections |
| c = 11.8335 (7) Å | θ = 2.3–28.4° |
| α = 68.949 (3)° | µ = 0.38 mm−1 |
| β = 89.362 (3)° | T = 173 K |
| γ = 71.460 (3)° | Block, colourless |
| V = 785.11 (8) Å3 | 0.46 × 0.37 × 0.33 mm |
Data collection
| Bruker SMART APEXII CCD diffractometer | 3759 independent reflections |
| Radiation source: rotating anode | 3348 reflections with I > 2σ(I) |
| Graphite multilayer monochromator | Rint = 0.031 |
| Detector resolution: 10.0 pixels mm-1 | θmax = 28.0°, θmin = 2.3° |
| φ and ω scans | h = −9→9 |
| Absorption correction: multi-scan (SADABS; Bruker, 2009) | k = −13→13 |
| Tmin = 0.691, Tmax = 0.746 | l = −15→15 |
| 13937 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.034 | H-atom parameters constrained |
| wR(F2) = 0.100 | w = 1/[σ2(Fo2) + (0.0517P)2 + 0.2412P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.06 | (Δ/σ)max < 0.001 |
| 3759 reflections | Δρmax = 0.31 e Å−3 |
| 203 parameters | Δρmin = −0.29 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.006 (2) |
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. |
| 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 > 2sigma(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 | ||
| Cl1 | 0.02297 (6) | 0.70926 (4) | −0.07104 (3) | 0.03932 (13) | |
| S1 | 0.36271 (5) | 0.19161 (4) | 0.40911 (3) | 0.02784 (11) | |
| O1 | 0.19351 (14) | 0.58273 (10) | 0.44275 (8) | 0.0265 (2) | |
| O2 | 0.21419 (17) | 0.18248 (12) | 0.32973 (11) | 0.0411 (3) | |
| C1 | 0.29375 (19) | 0.37881 (14) | 0.39556 (12) | 0.0251 (3) | |
| C2 | 0.20899 (19) | 0.50599 (14) | 0.28375 (12) | 0.0248 (3) | |
| C3 | 0.1735 (2) | 0.52797 (15) | 0.16126 (13) | 0.0279 (3) | |
| H3 | 0.2128 | 0.4481 | 0.1335 | 0.033* | |
| C4 | 0.0781 (2) | 0.67216 (16) | 0.08294 (13) | 0.0290 (3) | |
| C5 | 0.0153 (2) | 0.79189 (15) | 0.12135 (13) | 0.0298 (3) | |
| H5 | −0.0515 | 0.8884 | 0.0634 | 0.036* | |
| C7 | 0.14795 (19) | 0.62695 (15) | 0.31933 (12) | 0.0251 (3) | |
| C6 | 0.0489 (2) | 0.77201 (15) | 0.24256 (13) | 0.0273 (3) | |
| C8 | 0.28210 (19) | 0.43087 (14) | 0.48790 (12) | 0.0249 (3) | |
| C9 | −0.0186 (2) | 0.89610 (16) | 0.28858 (15) | 0.0343 (3) | |
| H9A | −0.1057 | 0.9849 | 0.2243 | 0.052* | |
| H9B | 0.0929 | 0.9177 | 0.3116 | 0.052* | |
| H9C | −0.0870 | 0.8668 | 0.3599 | 0.052* | |
| C10 | 0.3426 (2) | 0.36521 (15) | 0.61893 (12) | 0.0262 (3) | |
| C11 | 0.2685 (2) | 0.44896 (16) | 0.69082 (13) | 0.0299 (3) | |
| H11 | 0.1763 | 0.5457 | 0.6543 | 0.036* | |
| C12 | 0.3291 (2) | 0.39130 (18) | 0.81450 (14) | 0.0343 (3) | |
| H12 | 0.2787 | 0.4499 | 0.8615 | 0.041* | |
| C13 | 0.4619 (2) | 0.24959 (18) | 0.87129 (13) | 0.0339 (3) | |
| C14 | 0.5333 (2) | 0.16600 (17) | 0.80041 (14) | 0.0338 (3) | |
| H14 | 0.6229 | 0.0683 | 0.8379 | 0.041* | |
| C15 | 0.4761 (2) | 0.22262 (16) | 0.67607 (13) | 0.0297 (3) | |
| H15 | 0.5282 | 0.1639 | 0.6294 | 0.036* | |
| C16 | 0.5257 (3) | 0.1898 (2) | 1.00639 (14) | 0.0458 (4) | |
| H16A | 0.6069 | 0.0852 | 1.0331 | 0.069* | |
| H16B | 0.4121 | 0.1986 | 1.0509 | 0.069* | |
| H16C | 0.5994 | 0.2468 | 1.0229 | 0.069* | |
| C17 | 0.5744 (2) | 0.18473 (17) | 0.32871 (14) | 0.0336 (3) | |
| H17A | 0.6062 | 0.1004 | 0.3012 | 0.040* | |
| H17B | 0.5467 | 0.2772 | 0.2556 | 0.040* | |
| C18 | 0.7460 (2) | 0.16692 (17) | 0.40993 (15) | 0.0363 (3) | |
| H18A | 0.7127 | 0.2480 | 0.4401 | 0.054* | |
| H18B | 0.8561 | 0.1696 | 0.3630 | 0.054* | |
| H18C | 0.7798 | 0.0717 | 0.4791 | 0.054* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl1 | 0.0511 (3) | 0.0362 (2) | 0.02820 (19) | −0.01466 (18) | −0.00402 (16) | −0.00909 (15) |
| S1 | 0.0307 (2) | 0.02136 (17) | 0.03107 (19) | −0.00773 (14) | 0.00090 (14) | −0.01020 (13) |
| O1 | 0.0277 (5) | 0.0223 (5) | 0.0278 (5) | −0.0054 (4) | 0.0023 (4) | −0.0101 (4) |
| O2 | 0.0422 (7) | 0.0359 (6) | 0.0484 (7) | −0.0158 (5) | −0.0071 (5) | −0.0166 (5) |
| C1 | 0.0235 (6) | 0.0218 (6) | 0.0280 (6) | −0.0057 (5) | 0.0031 (5) | −0.0089 (5) |
| C2 | 0.0210 (6) | 0.0230 (6) | 0.0296 (7) | −0.0065 (5) | 0.0029 (5) | −0.0098 (5) |
| C3 | 0.0274 (7) | 0.0263 (6) | 0.0304 (7) | −0.0080 (5) | 0.0016 (5) | −0.0119 (5) |
| C4 | 0.0283 (7) | 0.0304 (7) | 0.0275 (7) | −0.0106 (6) | −0.0006 (5) | −0.0092 (5) |
| C5 | 0.0274 (7) | 0.0240 (6) | 0.0334 (7) | −0.0067 (5) | −0.0010 (6) | −0.0070 (5) |
| C7 | 0.0225 (6) | 0.0241 (6) | 0.0280 (6) | −0.0068 (5) | 0.0017 (5) | −0.0100 (5) |
| C6 | 0.0226 (6) | 0.0236 (6) | 0.0338 (7) | −0.0059 (5) | 0.0019 (5) | −0.0103 (5) |
| C8 | 0.0222 (6) | 0.0216 (6) | 0.0304 (7) | −0.0068 (5) | 0.0041 (5) | −0.0098 (5) |
| C9 | 0.0339 (8) | 0.0237 (7) | 0.0410 (8) | −0.0028 (6) | 0.0020 (6) | −0.0130 (6) |
| C10 | 0.0258 (7) | 0.0275 (6) | 0.0275 (6) | −0.0121 (5) | 0.0056 (5) | −0.0102 (5) |
| C11 | 0.0320 (7) | 0.0292 (7) | 0.0318 (7) | −0.0132 (6) | 0.0080 (6) | −0.0129 (6) |
| C12 | 0.0398 (8) | 0.0396 (8) | 0.0318 (7) | −0.0199 (7) | 0.0115 (6) | −0.0173 (6) |
| C13 | 0.0327 (8) | 0.0441 (8) | 0.0278 (7) | −0.0205 (7) | 0.0064 (6) | −0.0104 (6) |
| C14 | 0.0294 (7) | 0.0340 (7) | 0.0315 (7) | −0.0097 (6) | 0.0021 (6) | −0.0058 (6) |
| C15 | 0.0270 (7) | 0.0313 (7) | 0.0304 (7) | −0.0088 (6) | 0.0042 (5) | −0.0121 (6) |
| C16 | 0.0473 (10) | 0.0616 (11) | 0.0283 (8) | −0.0238 (9) | 0.0054 (7) | −0.0117 (7) |
| C17 | 0.0341 (8) | 0.0309 (7) | 0.0331 (7) | −0.0029 (6) | 0.0056 (6) | −0.0160 (6) |
| C18 | 0.0332 (8) | 0.0325 (7) | 0.0451 (9) | −0.0107 (6) | 0.0082 (6) | −0.0172 (7) |
Geometric parameters (Å, º)
| Cl1—C4 | 1.7465 (15) | C10—C15 | 1.397 (2) |
| S1—O2 | 1.4962 (12) | C10—C11 | 1.4054 (19) |
| S1—C1 | 1.7686 (13) | C11—C12 | 1.384 (2) |
| S1—C17 | 1.8129 (16) | C11—H11 | 0.9500 |
| O1—C7 | 1.3746 (16) | C12—C13 | 1.389 (2) |
| O1—C8 | 1.3782 (15) | C12—H12 | 0.9500 |
| C1—C8 | 1.3689 (19) | C13—C14 | 1.391 (2) |
| C1—C2 | 1.4498 (18) | C13—C16 | 1.510 (2) |
| C2—C7 | 1.3905 (18) | C14—C15 | 1.387 (2) |
| C2—C3 | 1.3988 (19) | C14—H14 | 0.9500 |
| C3—C4 | 1.3811 (19) | C15—H15 | 0.9500 |
| C3—H3 | 0.9500 | C16—H16A | 0.9800 |
| C4—C5 | 1.401 (2) | C16—H16B | 0.9800 |
| C5—C6 | 1.388 (2) | C16—H16C | 0.9800 |
| C5—H5 | 0.9500 | C17—C18 | 1.519 (2) |
| C7—C6 | 1.3868 (18) | C17—H17A | 0.9900 |
| C6—C9 | 1.5006 (19) | C17—H17B | 0.9900 |
| C8—C10 | 1.4597 (19) | C18—H18A | 0.9800 |
| C9—H9A | 0.9800 | C18—H18B | 0.9800 |
| C9—H9B | 0.9800 | C18—H18C | 0.9800 |
| C9—H9C | 0.9800 | ||
| O2—S1—C1 | 106.72 (6) | C15—C10—C8 | 122.50 (13) |
| O2—S1—C17 | 106.62 (7) | C11—C10—C8 | 119.29 (12) |
| C1—S1—C17 | 98.27 (7) | C12—C11—C10 | 120.40 (14) |
| C7—O1—C8 | 107.00 (10) | C12—C11—H11 | 119.8 |
| C8—C1—C2 | 107.17 (12) | C10—C11—H11 | 119.8 |
| C8—C1—S1 | 127.41 (10) | C11—C12—C13 | 121.40 (14) |
| C2—C1—S1 | 124.75 (10) | C11—C12—H12 | 119.3 |
| C7—C2—C3 | 119.38 (12) | C13—C12—H12 | 119.3 |
| C7—C2—C1 | 104.93 (12) | C12—C13—C14 | 118.17 (14) |
| C3—C2—C1 | 135.63 (13) | C12—C13—C16 | 120.22 (15) |
| C4—C3—C2 | 116.30 (13) | C14—C13—C16 | 121.61 (15) |
| C4—C3—H3 | 121.8 | C15—C14—C13 | 121.24 (14) |
| C2—C3—H3 | 121.8 | C15—C14—H14 | 119.4 |
| C3—C4—C5 | 123.25 (13) | C13—C14—H14 | 119.4 |
| C3—C4—Cl1 | 119.41 (11) | C14—C15—C10 | 120.58 (14) |
| C5—C4—Cl1 | 117.29 (11) | C14—C15—H15 | 119.7 |
| C6—C5—C4 | 121.19 (13) | C10—C15—H15 | 119.7 |
| C6—C5—H5 | 119.4 | C13—C16—H16A | 109.5 |
| C4—C5—H5 | 119.4 | C13—C16—H16B | 109.5 |
| O1—C7—C6 | 124.11 (12) | H16A—C16—H16B | 109.5 |
| O1—C7—C2 | 110.69 (11) | C13—C16—H16C | 109.5 |
| C6—C7—C2 | 125.17 (13) | H16A—C16—H16C | 109.5 |
| C7—C6—C5 | 114.68 (12) | H16B—C16—H16C | 109.5 |
| C7—C6—C9 | 122.11 (13) | C18—C17—S1 | 111.08 (10) |
| C5—C6—C9 | 123.20 (13) | C18—C17—H17A | 109.4 |
| C1—C8—O1 | 110.19 (12) | S1—C17—H17A | 109.4 |
| C1—C8—C10 | 135.60 (12) | C18—C17—H17B | 109.4 |
| O1—C8—C10 | 114.20 (11) | S1—C17—H17B | 109.4 |
| C6—C9—H9A | 109.5 | H17A—C17—H17B | 108.0 |
| C6—C9—H9B | 109.5 | C17—C18—H18A | 109.5 |
| H9A—C9—H9B | 109.5 | C17—C18—H18B | 109.5 |
| C6—C9—H9C | 109.5 | H18A—C18—H18B | 109.5 |
| H9A—C9—H9C | 109.5 | C17—C18—H18C | 109.5 |
| H9B—C9—H9C | 109.5 | H18A—C18—H18C | 109.5 |
| C15—C10—C11 | 118.19 (13) | H18B—C18—H18C | 109.5 |
| O2—S1—C1—C8 | 131.72 (13) | C4—C5—C6—C7 | 0.2 (2) |
| C17—S1—C1—C8 | −118.07 (13) | C4—C5—C6—C9 | −178.83 (14) |
| O2—S1—C1—C2 | −37.66 (13) | C2—C1—C8—O1 | 0.68 (15) |
| C17—S1—C1—C2 | 72.54 (13) | S1—C1—C8—O1 | −170.20 (10) |
| C8—C1—C2—C7 | −1.27 (15) | C2—C1—C8—C10 | −178.15 (15) |
| S1—C1—C2—C7 | 169.92 (10) | S1—C1—C8—C10 | 11.0 (2) |
| C8—C1—C2—C3 | −178.44 (15) | C7—O1—C8—C1 | 0.20 (14) |
| S1—C1—C2—C3 | −7.3 (2) | C7—O1—C8—C10 | 179.30 (11) |
| C7—C2—C3—C4 | 0.1 (2) | C1—C8—C10—C15 | 15.7 (2) |
| C1—C2—C3—C4 | 176.96 (15) | O1—C8—C10—C15 | −163.06 (12) |
| C2—C3—C4—C5 | −1.2 (2) | C1—C8—C10—C11 | −165.94 (15) |
| C2—C3—C4—Cl1 | −178.57 (10) | O1—C8—C10—C11 | 15.27 (18) |
| C3—C4—C5—C6 | 1.0 (2) | C15—C10—C11—C12 | 0.8 (2) |
| Cl1—C4—C5—C6 | 178.51 (11) | C8—C10—C11—C12 | −177.59 (13) |
| C8—O1—C7—C6 | 176.97 (13) | C10—C11—C12—C13 | −0.8 (2) |
| C8—O1—C7—C2 | −1.06 (14) | C11—C12—C13—C14 | 0.0 (2) |
| C3—C2—C7—O1 | 179.17 (11) | C11—C12—C13—C16 | 179.84 (14) |
| C1—C2—C7—O1 | 1.44 (15) | C12—C13—C14—C15 | 0.9 (2) |
| C3—C2—C7—C6 | 1.2 (2) | C16—C13—C14—C15 | −179.02 (14) |
| C1—C2—C7—C6 | −176.57 (13) | C13—C14—C15—C10 | −0.8 (2) |
| O1—C7—C6—C5 | −179.01 (12) | C11—C10—C15—C14 | 0.0 (2) |
| C2—C7—C6—C5 | −1.3 (2) | C8—C10—C15—C14 | 178.34 (13) |
| O1—C7—C6—C9 | 0.0 (2) | O2—S1—C17—C18 | −170.38 (10) |
| C2—C7—C6—C9 | 177.75 (13) | C1—S1—C17—C18 | 79.34 (11) |
Footnotes
Supporting information for this paper is available from the IUCr electronic archives (Reference: FB2296).
References
- Brandenburg, K. (1998). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Bruker (2009). APEX2, SADABS and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- Choi, H. D., Seo, P. J., Son, B. W. & Lee, U. (2010a). Acta Cryst. E66, o886. [DOI] [PMC free article] [PubMed]
- Choi, H. D., Seo, P. J., Son, B. W. & Lee, U. (2010b). Acta Cryst. E66, o2277. [DOI] [PMC free article] [PubMed]
- Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
- Janiak, C. (2000). J. Chem. Soc. Dalton Trans. pp. 3885–3896.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [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. DOI: 10.1107/S1600536814005601/fb2296sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814005601/fb2296Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536814005601/fb2296Isup3.cml
CCDC reference: 991267
Additional supporting information: crystallographic information; 3D view; checkCIF report


