Abstract
In the title thiourea derivative, C16H17N3OS, the hydroxy- and methyl-substituted benzene rings form dihedral angles of 9.62 (12) and 55.69 (6)°, respectively, with the central CN3S chromophore (r.m.s. deviation = 0.0117 Å). An intramolecular O—H⋯N hydrogen bond ensures the coplanarity of the central atoms. The H atoms of the NH groups are syn and the conformation about the N=C double bond [1.295 (4) Å] is E. In the crystal, helical supramolecular chains sustained primarily by N—H⋯S hydrogen bonds are found. Additional stabilization is provided by C—H⋯π and π–π [ring centroid(hydroxybenzene)⋯ring centroid(methylbenzene) = 3.8524 (18) Å] interactions.
Related literature
For pharmaceutical applications of thioruea derivatives, see: Venkatachalam et al. (2004 ▶); Bruce et al. (2007 ▶). For related thiourea structures, see: Normaya et al. (2011 ▶); Salam et al. (2011 ▶); Dzulkifli et al. (2011 ▶).
Experimental
Crystal data
C16H17N3OS
M r = 299.39
Monoclinic,
a = 14.6966 (8) Å
b = 7.3586 (4) Å
c = 14.0926 (8) Å
β = 94.358 (5)°
V = 1519.66 (15) Å3
Z = 4
Mo Kα radiation
μ = 0.22 mm−1
T = 100 K
0.30 × 0.10 × 0.05 mm
Data collection
Agilent Supernova Dual diffractometer with an Atlas detector
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010 ▶) T min = 0.419, T max = 1.000
7614 measured reflections
3375 independent reflections
2094 reflections with I > 2σ(I)
R int = 0.066
Refinement
R[F 2 > 2σ(F 2)] = 0.060
wR(F 2) = 0.174
S = 1.00
3375 reflections
201 parameters
3 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.34 e Å−3
Δρmin = −0.34 e Å−3
Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811013729/hg5025sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013729/hg5025Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the C10–C15 ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| O1—H1o⋯N1 | 0.84 (1) | 1.81 (2) | 2.551 (3) | 145 (3) |
| N2—H2n⋯S1i | 0.88 (1) | 2.51 (2) | 3.323 (2) | 154 (3) |
| N3—H3n⋯S1i | 0.88 (1) | 2.49 (2) | 3.286 (3) | 151 (2) |
| C8—H8b⋯Cg1i | 0.98 | 2.59 | 3.501 (3) | 155 |
Symmetry code: (i)
.
Acknowledgments
This work was financially supported by the Ministry of Science Technology and Innovation (MOSTI) under a research grant (No. 06–01-09-SF0046). The authors would like to thank Universiti Malaysia Sarawak (UNIMAS) for the facilities to carry out the research work. The authors also thank the University of Malaya for support of the crystallographic facility.
supplementary crystallographic information
Comment
In continuation of structural investigations into the conformation and hydrogen bonding patterns in thiourea derivatives (Normaya et al. 2011; Salam et al., 2011; Dzulkifli et al., 2011), and also motivated by their pharmacological potential (Venkatachalam et al. 2004; Bruce et al., 2007), the title compound, (I), was investigated.
With respect to the planar (r.m.s. = 0.0117 Å) central CN3S chromophore in (I), Fig. 1, the OH– and Me-benzene rings are twisted as seen in the respective dihedral angles of 9.62 (12) and 55.69 (6) °. The almost co-planarity of the central atoms is ascribed to the formation of an intramolecular hydroxyl-O—H···N-imine hydrogen bond, Table 1. The H atoms of the NH groups are syn, and the conformation about the N1═C7 double bond [1.295 (4) Å] is E. The syn arrangement in (I) contrast the anti arrangement often seen in such derivatives but is readily explained in terms of the intramolecular O—H···N-imine hydrogen bond in (I) by contrast to the normally observed intramolecular N—H···N-imine hydrogen bond (Normaya et al. 2011; Salam et al., 2011; Dzulkifli et al., 2011).
Helical supramolecular chains along the b axis dominate the crystal packing, Fig. 2 and Table 1. These arise as a result of the thione-S interacting with both N—H atoms of a neighbouring molecule thereby forming six-membered hydrogen bond mediated rings. Chains are stabilized by C—H..π, Table 1, and π–π [ring centroid(C1···C6)···ring centroid(C10···C15)i = 3.8524 (18) Å, dihedral angle = 2.37 (15) ° for i: 1 - x, -1/2 + y, 1/2 - z] interactions, Fig. 3.
Experimental
2-Methylphenylisothiocyanate (0.746 g, 5 mmol) and hydrazine hydrate (0.253 g, 5 mmol), each dissolved in 10 ml e thanol, were mixed with constant stirring. The stirring was continued for 30 min and the white product formed was washed with ethanol and dried in vacuo. A solution of the isolated 2-methylphenylthiosemicarbazide (0.540 g, 3 mmol) in 10 ml me thanol was then refluxed with a methanolic solution of 2-hydroxyacetophenone (0.408 g, 3 mmol) for 5 h after adding 1–2 drops of glacial acetic acid. On cooling, the solution to room temperature, a light-yellow powder separated and washed with methanol. The powder was recrystallized from methanol and dried in vacuo over silica gel. (M.pt. 451–453 K. Yield 0.740 g (78%). Elemental analysis: Calc. for C16H17N3OS: C, 64.21; H, 5.73; N, 14.04%. Found: C, 64.17; H, 5.67; N, 14.01%. FT—IR (KBr, cm-1) νmax: 3175 (m, OH), 3000 (s, NH), 1583 (w, C═N), 943 (m, N—N), 1371, 861 (w, C═S).
Refinement
Carbon-bound H-atoms were placed in calculated positions (C–H = 0.98 to 1.00 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2–1.5Ueq(C). The O– and N-bound H-atoms were located in a difference Fourier map and were refined with distance restraints of O—H = 0.84±0.01 Å and N—H 0.88±0.01 Å, and with Uiso(H) = yUeq(parent atom) for y = 1.5 (O) and 1.2 (N).
Figures
Fig. 1.
The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.
Fig. 2.
A view of the helical supramolecular chain aligned along the b axis in (I). The N—H···S hydrogen bonds are shown as orange dashed lines. Further stabilization to the chain is provided by C—H···π and π–π interactions, shown as blue and purple dashed lines, respectively.
Fig. 3.
A view in projection down the c axis of the crystal packing in (I) showing the staking of layers comprising the helical supramolecular chains shown in Fig. 2. The O—H···O and N—H···S hydrogen bonds (orange), and C—H···π (blue) and π–π (purple) interactions are shown as dashed lines.
Crystal data
| C16H17N3OS | F(000) = 632 |
| Mr = 299.39 | Dx = 1.309 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 1905 reflections |
| a = 14.6966 (8) Å | θ = 2.8–29.3° |
| b = 7.3586 (4) Å | µ = 0.22 mm−1 |
| c = 14.0926 (8) Å | T = 100 K |
| β = 94.358 (5)° | Prism, light-yellow |
| V = 1519.66 (15) Å3 | 0.30 × 0.10 × 0.05 mm |
| Z = 4 |
Data collection
| Agilent Supernova Dual diffractometer with an Atlas detector | 3375 independent reflections |
| Radiation source: SuperNova (Mo) X-ray Source | 2094 reflections with I > 2σ(I) |
| Mirror | Rint = 0.066 |
| Detector resolution: 10.4041 pixels mm-1 | θmax = 27.5°, θmin = 2.8° |
| ω scans | h = −14→19 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −9→7 |
| Tmin = 0.419, Tmax = 1.000 | l = −18→15 |
| 7614 measured 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)] = 0.060 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.174 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.00 | w = 1/[σ2(Fo2) + (0.0769P)2] where P = (Fo2 + 2Fc2)/3 |
| 3375 reflections | (Δ/σ)max < 0.001 |
| 201 parameters | Δρmax = 0.34 e Å−3 |
| 3 restraints | Δρmin = −0.34 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 | ||
| S1 | 0.46230 (5) | 0.24817 (10) | 0.38597 (5) | 0.0188 (2) | |
| O1 | 0.21619 (14) | 0.2307 (3) | 0.31997 (15) | 0.0250 (5) | |
| H1O | 0.2693 (11) | 0.261 (4) | 0.308 (2) | 0.038* | |
| N1 | 0.33770 (15) | 0.3710 (3) | 0.22261 (17) | 0.0182 (6) | |
| N2 | 0.42781 (16) | 0.4196 (3) | 0.21980 (18) | 0.0190 (6) | |
| H2N | 0.4433 (19) | 0.497 (3) | 0.1764 (16) | 0.023* | |
| N3 | 0.57409 (16) | 0.4362 (3) | 0.27942 (17) | 0.0197 (6) | |
| H3N | 0.5801 (19) | 0.496 (4) | 0.2259 (13) | 0.024* | |
| C1 | 0.1592 (2) | 0.2588 (4) | 0.2410 (2) | 0.0229 (7) | |
| C2 | 0.0685 (2) | 0.2066 (5) | 0.2458 (3) | 0.0309 (8) | |
| H2 | 0.0496 | 0.1544 | 0.3027 | 0.037* | |
| C3 | 0.0062 (2) | 0.2298 (5) | 0.1692 (3) | 0.0331 (9) | |
| H3A | −0.0553 | 0.1927 | 0.1732 | 0.040* | |
| C4 | 0.0327 (2) | 0.3073 (5) | 0.0857 (3) | 0.0320 (8) | |
| H4 | −0.0104 | 0.3236 | 0.0327 | 0.038* | |
| C5 | 0.1220 (2) | 0.3603 (4) | 0.0806 (2) | 0.0260 (8) | |
| H5A | 0.1396 | 0.4142 | 0.0236 | 0.031* | |
| C6 | 0.18777 (19) | 0.3372 (4) | 0.1568 (2) | 0.0200 (7) | |
| C7 | 0.28345 (19) | 0.3879 (4) | 0.1464 (2) | 0.0189 (7) | |
| C8 | 0.3131 (2) | 0.4548 (4) | 0.0530 (2) | 0.0229 (7) | |
| H8A | 0.3795 | 0.4432 | 0.0525 | 0.034* | |
| H8B | 0.2957 | 0.5827 | 0.0445 | 0.034* | |
| H8C | 0.2834 | 0.3824 | 0.0012 | 0.034* | |
| C9 | 0.48965 (19) | 0.3751 (4) | 0.2920 (2) | 0.0174 (7) | |
| C10 | 0.65424 (19) | 0.4166 (4) | 0.3422 (2) | 0.0172 (7) | |
| C11 | 0.6563 (2) | 0.4776 (4) | 0.4351 (2) | 0.0201 (7) | |
| H11 | 0.6024 | 0.5242 | 0.4592 | 0.024* | |
| C12 | 0.7355 (2) | 0.4712 (4) | 0.4928 (2) | 0.0252 (7) | |
| H12A | 0.7364 | 0.5112 | 0.5570 | 0.030* | |
| C13 | 0.8147 (2) | 0.4057 (4) | 0.4568 (2) | 0.0253 (7) | |
| H13 | 0.8703 | 0.4035 | 0.4960 | 0.030* | |
| C14 | 0.8128 (2) | 0.3441 (4) | 0.3647 (2) | 0.0231 (7) | |
| H14 | 0.8671 | 0.2974 | 0.3414 | 0.028* | |
| C15 | 0.73287 (19) | 0.3485 (4) | 0.3047 (2) | 0.0195 (7) | |
| C16 | 0.7318 (2) | 0.2841 (4) | 0.2034 (2) | 0.0260 (8) | |
| H16A | 0.7815 | 0.1969 | 0.1974 | 0.039* | |
| H16B | 0.7401 | 0.3882 | 0.1615 | 0.039* | |
| H16C | 0.6733 | 0.2253 | 0.1851 | 0.039* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0225 (4) | 0.0163 (4) | 0.0179 (4) | −0.0009 (3) | 0.0039 (3) | −0.0001 (3) |
| O1 | 0.0214 (11) | 0.0291 (13) | 0.0247 (13) | −0.0029 (10) | 0.0027 (10) | −0.0005 (10) |
| N1 | 0.0150 (12) | 0.0148 (13) | 0.0247 (15) | −0.0010 (10) | 0.0019 (10) | −0.0010 (11) |
| N2 | 0.0179 (13) | 0.0166 (14) | 0.0222 (15) | −0.0023 (10) | 0.0002 (11) | 0.0044 (11) |
| N3 | 0.0187 (13) | 0.0205 (14) | 0.0199 (15) | −0.0006 (11) | 0.0016 (11) | 0.0052 (11) |
| C1 | 0.0245 (16) | 0.0172 (16) | 0.0269 (18) | 0.0046 (13) | 0.0018 (13) | −0.0085 (14) |
| C2 | 0.0234 (17) | 0.030 (2) | 0.040 (2) | −0.0028 (14) | 0.0098 (15) | −0.0020 (16) |
| C3 | 0.0198 (17) | 0.031 (2) | 0.049 (2) | −0.0018 (14) | 0.0039 (16) | −0.0077 (17) |
| C4 | 0.0248 (18) | 0.0298 (19) | 0.040 (2) | 0.0018 (15) | −0.0039 (15) | 0.0006 (17) |
| C5 | 0.0242 (17) | 0.0207 (17) | 0.032 (2) | 0.0010 (14) | −0.0026 (14) | −0.0014 (15) |
| C6 | 0.0174 (15) | 0.0158 (16) | 0.0266 (18) | −0.0010 (12) | 0.0003 (13) | −0.0037 (13) |
| C7 | 0.0209 (15) | 0.0104 (15) | 0.0250 (18) | 0.0038 (12) | 0.0004 (13) | −0.0030 (13) |
| C8 | 0.0248 (16) | 0.0192 (17) | 0.0247 (18) | −0.0002 (13) | 0.0021 (13) | −0.0036 (14) |
| C9 | 0.0180 (15) | 0.0151 (15) | 0.0197 (16) | 0.0034 (12) | 0.0045 (12) | −0.0028 (13) |
| C10 | 0.0185 (15) | 0.0126 (15) | 0.0205 (17) | −0.0006 (12) | 0.0014 (12) | 0.0014 (12) |
| C11 | 0.0272 (16) | 0.0095 (14) | 0.0239 (18) | 0.0015 (13) | 0.0045 (13) | −0.0009 (13) |
| C12 | 0.0354 (19) | 0.0158 (16) | 0.0235 (18) | −0.0033 (14) | −0.0037 (14) | 0.0013 (14) |
| C13 | 0.0249 (17) | 0.0192 (17) | 0.030 (2) | −0.0021 (13) | −0.0091 (14) | 0.0055 (14) |
| C14 | 0.0171 (15) | 0.0183 (16) | 0.034 (2) | 0.0001 (13) | 0.0034 (13) | 0.0026 (15) |
| C15 | 0.0262 (16) | 0.0132 (15) | 0.0200 (17) | −0.0058 (13) | 0.0063 (13) | −0.0003 (13) |
| C16 | 0.0275 (17) | 0.0240 (18) | 0.0276 (19) | −0.0018 (14) | 0.0094 (14) | −0.0020 (14) |
Geometric parameters (Å, °)
| S1—C9 | 1.694 (3) | C6—C7 | 1.473 (4) |
| O1—C1 | 1.357 (4) | C7—C8 | 1.500 (4) |
| O1—H1O | 0.842 (10) | C8—H8A | 0.9800 |
| N1—C7 | 1.295 (4) | C8—H8B | 0.9800 |
| N1—N2 | 1.375 (3) | C8—H8C | 0.9800 |
| N2—C9 | 1.352 (4) | C10—C11 | 1.383 (4) |
| N2—H2N | 0.880 (10) | C10—C15 | 1.400 (4) |
| N3—C9 | 1.344 (3) | C11—C12 | 1.369 (4) |
| N3—C10 | 1.426 (4) | C11—H11 | 0.9500 |
| N3—H3N | 0.882 (10) | C12—C13 | 1.391 (4) |
| C1—C2 | 1.394 (4) | C12—H12A | 0.9500 |
| C1—C6 | 1.411 (4) | C13—C14 | 1.373 (4) |
| C2—C3 | 1.372 (5) | C13—H13 | 0.9500 |
| C2—H2 | 0.9500 | C14—C15 | 1.395 (4) |
| C3—C4 | 1.390 (5) | C14—H14 | 0.9500 |
| C3—H3A | 0.9500 | C15—C16 | 1.503 (4) |
| C4—C5 | 1.376 (4) | C16—H16A | 0.9800 |
| C4—H4 | 0.9500 | C16—H16B | 0.9800 |
| C5—C6 | 1.400 (4) | C16—H16C | 0.9800 |
| C5—H5A | 0.9500 | ||
| C1—O1—H1O | 108 (2) | H8A—C8—H8B | 109.5 |
| C7—N1—N2 | 119.0 (2) | C7—C8—H8C | 109.5 |
| C9—N2—N1 | 120.6 (2) | H8A—C8—H8C | 109.5 |
| C9—N2—H2N | 119 (2) | H8B—C8—H8C | 109.5 |
| N1—N2—H2N | 119.3 (19) | N3—C9—N2 | 113.2 (2) |
| C9—N3—C10 | 127.7 (2) | N3—C9—S1 | 124.3 (2) |
| C9—N3—H3N | 115.6 (19) | N2—C9—S1 | 122.4 (2) |
| C10—N3—H3N | 116.7 (19) | C11—C10—C15 | 121.0 (3) |
| O1—C1—C2 | 116.8 (3) | C11—C10—N3 | 120.9 (3) |
| O1—C1—C6 | 123.2 (3) | C15—C10—N3 | 117.9 (3) |
| C2—C1—C6 | 120.0 (3) | C12—C11—C10 | 120.5 (3) |
| C3—C2—C1 | 120.8 (3) | C12—C11—H11 | 119.7 |
| C3—C2—H2 | 119.6 | C10—C11—H11 | 119.7 |
| C1—C2—H2 | 119.6 | C11—C12—C13 | 119.5 (3) |
| C2—C3—C4 | 120.2 (3) | C11—C12—H12A | 120.2 |
| C2—C3—H3A | 119.9 | C13—C12—H12A | 120.2 |
| C4—C3—H3A | 119.9 | C14—C13—C12 | 120.1 (3) |
| C5—C4—C3 | 119.4 (3) | C14—C13—H13 | 120.0 |
| C5—C4—H4 | 120.3 | C12—C13—H13 | 120.0 |
| C3—C4—H4 | 120.3 | C13—C14—C15 | 121.5 (3) |
| C4—C5—C6 | 122.1 (3) | C13—C14—H14 | 119.3 |
| C4—C5—H5A | 119.0 | C15—C14—H14 | 119.3 |
| C6—C5—H5A | 119.0 | C14—C15—C10 | 117.4 (3) |
| C5—C6—C1 | 117.6 (3) | C14—C15—C16 | 121.1 (3) |
| C5—C6—C7 | 120.1 (3) | C10—C15—C16 | 121.5 (3) |
| C1—C6—C7 | 122.3 (3) | C15—C16—H16A | 109.5 |
| N1—C7—C6 | 115.1 (3) | C15—C16—H16B | 109.5 |
| N1—C7—C8 | 123.9 (3) | H16A—C16—H16B | 109.5 |
| C6—C7—C8 | 120.9 (3) | C15—C16—H16C | 109.5 |
| C7—C8—H8A | 109.5 | H16A—C16—H16C | 109.5 |
| C7—C8—H8B | 109.5 | H16B—C16—H16C | 109.5 |
| C7—N1—N2—C9 | −168.5 (3) | C10—N3—C9—N2 | 178.6 (3) |
| O1—C1—C2—C3 | −179.9 (3) | C10—N3—C9—S1 | −3.6 (4) |
| C6—C1—C2—C3 | 0.3 (5) | N1—N2—C9—N3 | −178.5 (2) |
| C1—C2—C3—C4 | −0.5 (5) | N1—N2—C9—S1 | 3.7 (4) |
| C2—C3—C4—C5 | 0.1 (5) | C9—N3—C10—C11 | −56.4 (4) |
| C3—C4—C5—C6 | 0.6 (5) | C9—N3—C10—C15 | 129.0 (3) |
| C4—C5—C6—C1 | −0.8 (5) | C15—C10—C11—C12 | −0.5 (4) |
| C4—C5—C6—C7 | 177.0 (3) | N3—C10—C11—C12 | −174.9 (3) |
| O1—C1—C6—C5 | −179.4 (3) | C10—C11—C12—C13 | 1.1 (4) |
| C2—C1—C6—C5 | 0.3 (4) | C11—C12—C13—C14 | −1.5 (5) |
| O1—C1—C6—C7 | 2.8 (5) | C12—C13—C14—C15 | 1.2 (5) |
| C2—C1—C6—C7 | −177.4 (3) | C13—C14—C15—C10 | −0.6 (4) |
| N2—N1—C7—C6 | −178.4 (2) | C13—C14—C15—C16 | 178.8 (3) |
| N2—N1—C7—C8 | 1.2 (4) | C11—C10—C15—C14 | 0.2 (4) |
| C5—C6—C7—N1 | 176.2 (3) | N3—C10—C15—C14 | 174.8 (3) |
| C1—C6—C7—N1 | −6.1 (4) | C11—C10—C15—C16 | −179.2 (3) |
| C5—C6—C7—C8 | −3.4 (4) | N3—C10—C15—C16 | −4.6 (4) |
| C1—C6—C7—C8 | 174.3 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1o···N1 | 0.842 (10) | 1.81 (2) | 2.551 (3) | 145 (3) |
| N2—H2n···S1i | 0.880 (10) | 2.508 (16) | 3.323 (2) | 154 (3) |
| N3—H3n···S1i | 0.882 (10) | 2.485 (17) | 3.286 (3) | 151 (2) |
| C8—H8b···Cg1i | 0.98 | 2.59 | 3.501 (3) | 155 |
Symmetry codes: (i) −x+1, y+1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5025).
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 datablocks global, I. DOI: 10.1107/S1600536811013729/hg5025sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811013729/hg5025Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



