Abstract
In the title thiourea derivative, C14H20N4S, the non-ring non-H atoms are approximately planar, with an r.m.s. deviation of 0.0720 Å. The pyridine ring is twisted out of this plane and makes a dihedral angle of 16.85 (13)° with it. The mean plane passing through the cyclohexyl ring is almost normal to the central plane [dihedral angle = 69.23 (8)°]. An intramolecular N—H⋯N(imine) hydrogen bond occurs. Centrosymmetric dimers are formed in the crystal structure via pairs of N—H⋯S hydrogen bonds, and these are connected into a supramolecular chain along the a axis via C—H⋯π(pyridyl) interactions.
Related literature
For related thiourea structures, see: Tiekink (1989 ▶); Lai & Tiekink (2002 ▶); Muramulla et al. (2009 ▶).
Experimental
Crystal data
C14H20N4S
M r = 276.40
Triclinic,
a = 5.8824 (6) Å
b = 10.2410 (9) Å
c = 12.3902 (14) Å
α = 94.718 (8)°
β = 90.427 (9)°
γ = 90.979 (8)°
V = 743.74 (13) Å3
Z = 2
Mo Kα radiation
μ = 0.21 mm−1
T = 295 K
0.25 × 0.20 × 0.15 mm
Data collection
Agilent Supernova Dual diffractometer with an Atlas detector
Absorption correction: multi-scan (CrysAlis PRO; Agilent Technologies, 2010 ▶) T min = 0.842, T max = 1.000
5817 measured reflections
3292 independent reflections
2355 reflections with I > 2σ(I)
R int = 0.027
Refinement
R[F 2 > 2σ(F 2)] = 0.053
wR(F 2) = 0.151
S = 1.04
3292 reflections
181 parameters
2 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.22 e Å−3
Δρmin = −0.20 e Å−3
Data collection: CrysAlis PRO (Agilent Technologies, 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/S1600536811009317/hg5008sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009317/hg5008Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
Cg1 is the centroid of the pyridyl ring.
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1⋯N3 | 0.87 (2) | 2.16 (2) | 2.592 (3) | 111 (2) |
| N2—H2⋯S1i | 0.88 (2) | 2.73 (2) | 3.610 (2) | 174 (2) |
| C9—H9b⋯Cg1ii | 0.96 | 2.89 | 3.776 (3) | 155 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work was supported financially by the Ministry of Science, Technology and Innovation (MOSTI) under research grant No. 06-01-09-SF0046. The authors 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 long-term structural investigations of thiourea derivatives (Tiekink, 1989; Lai & Tiekink, 2002; Muramulla et al., 2009), the title compound, (I), was investigated. The atoms comprising the thiosemicarbazone backbone of the molecules, i.e. S1,N1—N3,C1,C7—C10 are co-planar (r.m.s. = 0.0720 Å). While the pyridine residue is twisted out of this plane as seen in the value of the N3—C8—C10—N4 torsion angle of 164.7 (2) °, the cyclohexyl group is almost normal to the plane; C2—C1—N1—C7 is 87.7 (3) °. The amine-N—H1 and imine-N3 atoms are directed to the same side of the molecule enabling the formation of an intramolecular N—H···N hydrogen bond, Table 1. The pyridine-N atom is directed away from the rest of the molecule and is proximate to the methyl substituent which results in the formation of a C—H···N contact, Table 1.
The crystal packing is dominated by N—H···S hydrogen bonds that lead to centrosymmetric dimers, Table 1. Dimers aligned along the a axis are connected into a supramolecular chain via C—H···π interactions involving methyl-H and the pyridyl ring. There are no specific intermolecular interactions occurring between chains, Fig. 3.
Experimental
Cyclohexyl isothiocyanate (0.706 g, 5 mmol) and hydrazine hydrate (0.250 g, 5 mmol), each dissolved in 10 ml ethanol, were mixed with constant stirring. The stirring was continued for 30 min and the white product, N(4)-cyclohexylthiosemicarbazide formed was washed with ethanol and dried. A solution of the N(4)-cyclohexylthiosemicarbazide (0.51 g, 3 mmol) in 10 ml methanol was refluxed with a methanolic solution of 2-acetylpyridine (0.363 g, 3 mmol) for 5 h after adding 1–2 drops of acetic acid. A white powder separated on cooling the solution which was filtered and washed with methanol. This was recrystallized from methanol and dried in vacuo over silica gel. (M.pt. 453–455 K; Yield 0.682 g, 76%). Elemental analysis: Calc.: C, 60.83; H, 7.29; N, 11.60%. Found: C, 60.72; H, 7.25; N, 11.57%. FT—IR (KBr, cm-1) νmax: 3329 (s, NH), 2931, 2851 (s, cyclohexyl), 1580 (w, C═N—N═C), 980 (m, N—N), 1358, 835 (w, C═ S), 657 (m, pyridine in plane).
Refinement
Carbon-bound H-atoms were placed in calculated positions (C–H = 0.93 to 0.98 Å) and were included in the refinement in the riding model approximation, with Uiso(H) set to 1.2–1.5Ueq(C). The N-bound H-atoms were located in a difference Fourier map and were refined with a distance restraint of N—H 0.88±0.01 Å, and with Uiso(H) = 1.2Ueq(N).
Figures
Fig. 1.
The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 35% probability level.
Fig. 2.
A view of the supramolecular chain aligned along the a axis in (I). The N—H···S hydrogen bonds and C—H···π contacts are shown as orange and purple dashed lines, respectively.
Fig. 3.
A view in projection down the a axis of the crystal packing in (I). The N—H···S hydrogen bonds and C—H···π contacts are shown as orange and purple dashed lines, respectively.
Crystal data
| C14H20N4S | Z = 2 |
| Mr = 276.40 | F(000) = 296 |
| Triclinic, P1 | Dx = 1.234 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 5.8824 (6) Å | Cell parameters from 2234 reflections |
| b = 10.2410 (9) Å | θ = 2.5–29.3° |
| c = 12.3902 (14) Å | µ = 0.21 mm−1 |
| α = 94.718 (8)° | T = 295 K |
| β = 90.427 (9)° | Block, colourless |
| γ = 90.979 (8)° | 0.25 × 0.20 × 0.15 mm |
| V = 743.74 (13) Å3 |
Data collection
| Agilent Supernova Dual diffractometer with an Atlas detector | 3292 independent reflections |
| Radiation source: SuperNova (Mo) X-ray Source | 2355 reflections with I > 2σ(I) |
| Mirror | Rint = 0.027 |
| Detector resolution: 10.4041 pixels mm-1 | θmax = 27.5°, θmin = 2.5° |
| ω scans | h = −7→5 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent Technologies, 2010) | k = −12→11 |
| Tmin = 0.842, Tmax = 1.000 | l = −16→15 |
| 5817 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)] = 0.053 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.151 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.04 | w = 1/[σ2(Fo2) + (0.0595P)2 + 0.2389P] where P = (Fo2 + 2Fc2)/3 |
| 3292 reflections | (Δ/σ)max < 0.001 |
| 181 parameters | Δρmax = 0.22 e Å−3 |
| 2 restraints | Δρmin = −0.20 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 | ||
| S1 | 0.98373 (10) | 0.38035 (6) | 0.62998 (5) | 0.0566 (2) | |
| N1 | 0.6028 (3) | 0.4301 (2) | 0.73985 (16) | 0.0516 (5) | |
| N2 | 0.6780 (3) | 0.56047 (19) | 0.60354 (16) | 0.0473 (5) | |
| N3 | 0.4954 (3) | 0.63316 (18) | 0.63973 (15) | 0.0443 (4) | |
| N4 | 0.2260 (4) | 0.9312 (2) | 0.61127 (19) | 0.0655 (6) | |
| C1 | 0.6423 (4) | 0.3310 (2) | 0.81548 (18) | 0.0509 (6) | |
| H1A | 0.7317 | 0.2612 | 0.7785 | 0.061* | |
| C2 | 0.7750 (5) | 0.3871 (3) | 0.9131 (2) | 0.0774 (9) | |
| H2A | 0.6945 | 0.4610 | 0.9476 | 0.093* | |
| H2B | 0.9219 | 0.4189 | 0.8903 | 0.093* | |
| C3 | 0.8102 (6) | 0.2857 (4) | 0.9947 (3) | 0.1056 (13) | |
| H3A | 0.9038 | 0.2159 | 0.9627 | 0.127* | |
| H3B | 0.8898 | 0.3264 | 1.0579 | 0.127* | |
| C4 | 0.5863 (6) | 0.2288 (4) | 1.0287 (2) | 0.0850 (10) | |
| H4A | 0.6135 | 0.1614 | 1.0776 | 0.102* | |
| H4B | 0.4981 | 0.2969 | 1.0668 | 0.102* | |
| C5 | 0.4558 (5) | 0.1713 (3) | 0.9314 (3) | 0.0797 (9) | |
| H5A | 0.3094 | 0.1388 | 0.9542 | 0.096* | |
| H5B | 0.5380 | 0.0976 | 0.8977 | 0.096* | |
| C6 | 0.4189 (5) | 0.2718 (3) | 0.8486 (2) | 0.0746 (8) | |
| H6A | 0.3421 | 0.2296 | 0.7851 | 0.090* | |
| H6B | 0.3222 | 0.3407 | 0.8796 | 0.090* | |
| C7 | 0.7428 (4) | 0.4599 (2) | 0.66113 (17) | 0.0436 (5) | |
| C8 | 0.4457 (4) | 0.7360 (2) | 0.59286 (18) | 0.0433 (5) | |
| C9 | 0.5690 (4) | 0.7871 (2) | 0.4999 (2) | 0.0575 (6) | |
| H9A | 0.5857 | 0.7177 | 0.4437 | 0.086* | |
| H9B | 0.7165 | 0.8197 | 0.5238 | 0.086* | |
| H9C | 0.4842 | 0.8567 | 0.4725 | 0.086* | |
| C10 | 0.2493 (4) | 0.8097 (2) | 0.64002 (17) | 0.0438 (5) | |
| C11 | 0.1000 (4) | 0.7543 (2) | 0.70977 (19) | 0.0516 (6) | |
| H11 | 0.1192 | 0.6689 | 0.7279 | 0.062* | |
| C12 | −0.0774 (4) | 0.8277 (3) | 0.7519 (2) | 0.0627 (7) | |
| H12 | −0.1794 | 0.7929 | 0.7993 | 0.075* | |
| C13 | −0.1011 (5) | 0.9530 (3) | 0.7227 (2) | 0.0702 (8) | |
| H13 | −0.2191 | 1.0048 | 0.7500 | 0.084* | |
| C14 | 0.0518 (5) | 1.0001 (3) | 0.6527 (3) | 0.0768 (9) | |
| H14 | 0.0339 | 1.0850 | 0.6327 | 0.092* | |
| H1 | 0.478 (3) | 0.474 (2) | 0.743 (2) | 0.065 (8)* | |
| H2 | 0.768 (4) | 0.579 (3) | 0.5503 (14) | 0.065 (8)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0544 (4) | 0.0507 (4) | 0.0685 (4) | 0.0198 (3) | 0.0197 (3) | 0.0228 (3) |
| N1 | 0.0532 (11) | 0.0492 (12) | 0.0560 (11) | 0.0178 (9) | 0.0174 (9) | 0.0209 (9) |
| N2 | 0.0480 (10) | 0.0408 (11) | 0.0557 (11) | 0.0121 (8) | 0.0150 (9) | 0.0165 (9) |
| N3 | 0.0448 (9) | 0.0368 (10) | 0.0527 (11) | 0.0086 (7) | 0.0091 (8) | 0.0101 (8) |
| N4 | 0.0693 (13) | 0.0387 (12) | 0.0918 (16) | 0.0159 (10) | 0.0248 (12) | 0.0197 (11) |
| C1 | 0.0587 (13) | 0.0454 (13) | 0.0517 (13) | 0.0179 (10) | 0.0168 (11) | 0.0172 (11) |
| C2 | 0.0801 (19) | 0.084 (2) | 0.0717 (18) | −0.0111 (16) | 0.0005 (15) | 0.0302 (16) |
| C3 | 0.101 (3) | 0.137 (3) | 0.087 (2) | −0.018 (2) | −0.0175 (19) | 0.062 (2) |
| C4 | 0.103 (2) | 0.090 (2) | 0.0679 (19) | 0.0107 (19) | 0.0187 (17) | 0.0400 (17) |
| C5 | 0.088 (2) | 0.067 (2) | 0.089 (2) | −0.0019 (16) | 0.0221 (17) | 0.0356 (17) |
| C6 | 0.0723 (18) | 0.078 (2) | 0.0778 (19) | −0.0094 (15) | 0.0030 (15) | 0.0351 (16) |
| C7 | 0.0480 (12) | 0.0358 (12) | 0.0479 (12) | 0.0066 (9) | 0.0061 (10) | 0.0085 (9) |
| C8 | 0.0479 (12) | 0.0338 (11) | 0.0495 (12) | 0.0041 (9) | 0.0055 (9) | 0.0101 (9) |
| C9 | 0.0650 (15) | 0.0477 (14) | 0.0633 (15) | 0.0124 (11) | 0.0193 (12) | 0.0206 (12) |
| C10 | 0.0480 (11) | 0.0365 (12) | 0.0479 (12) | 0.0061 (9) | 0.0031 (10) | 0.0080 (10) |
| C11 | 0.0543 (13) | 0.0455 (14) | 0.0568 (14) | 0.0105 (10) | 0.0090 (11) | 0.0120 (11) |
| C12 | 0.0603 (15) | 0.0694 (19) | 0.0594 (15) | 0.0102 (13) | 0.0161 (12) | 0.0079 (13) |
| C13 | 0.0689 (17) | 0.0608 (18) | 0.0806 (19) | 0.0243 (14) | 0.0174 (15) | −0.0027 (15) |
| C14 | 0.0823 (19) | 0.0418 (15) | 0.109 (2) | 0.0219 (13) | 0.0256 (18) | 0.0138 (15) |
Geometric parameters (Å, °)
| S1—C7 | 1.678 (2) | C4—H4A | 0.9700 |
| N1—C7 | 1.332 (3) | C4—H4B | 0.9700 |
| N1—C1 | 1.457 (3) | C5—C6 | 1.529 (4) |
| N1—H1 | 0.870 (10) | C5—H5A | 0.9700 |
| N2—C7 | 1.359 (3) | C5—H5B | 0.9700 |
| N2—N3 | 1.374 (2) | C6—H6A | 0.9700 |
| N2—H2 | 0.878 (10) | C6—H6B | 0.9700 |
| N3—C8 | 1.281 (3) | C8—C10 | 1.488 (3) |
| N4—C10 | 1.331 (3) | C8—C9 | 1.491 (3) |
| N4—C14 | 1.336 (3) | C9—H9A | 0.9600 |
| C1—C2 | 1.503 (4) | C9—H9B | 0.9600 |
| C1—C6 | 1.512 (3) | C9—H9C | 0.9600 |
| C1—H1A | 0.9800 | C10—C11 | 1.384 (3) |
| C2—C3 | 1.523 (4) | C11—C12 | 1.377 (3) |
| C2—H2A | 0.9700 | C11—H11 | 0.9300 |
| C2—H2B | 0.9700 | C12—C13 | 1.370 (4) |
| C3—C4 | 1.508 (5) | C12—H12 | 0.9300 |
| C3—H3A | 0.9700 | C13—C14 | 1.364 (4) |
| C3—H3B | 0.9700 | C13—H13 | 0.9300 |
| C4—C5 | 1.498 (5) | C14—H14 | 0.9300 |
| C7—N1—C1 | 125.56 (19) | C6—C5—H5B | 109.2 |
| C7—N1—H1 | 114.1 (18) | H5A—C5—H5B | 107.9 |
| C1—N1—H1 | 120.3 (18) | C1—C6—C5 | 111.2 (2) |
| C7—N2—N3 | 118.18 (18) | C1—C6—H6A | 109.4 |
| C7—N2—H2 | 115.9 (18) | C5—C6—H6A | 109.4 |
| N3—N2—H2 | 125.6 (18) | C1—C6—H6B | 109.4 |
| C8—N3—N2 | 119.02 (18) | C5—C6—H6B | 109.4 |
| C10—N4—C14 | 117.7 (2) | H6A—C6—H6B | 108.0 |
| N1—C1—C2 | 111.2 (2) | N1—C7—N2 | 115.73 (19) |
| N1—C1—C6 | 110.3 (2) | N1—C7—S1 | 124.18 (17) |
| C2—C1—C6 | 110.8 (2) | N2—C7—S1 | 120.08 (16) |
| N1—C1—H1A | 108.1 | N3—C8—C10 | 114.81 (19) |
| C2—C1—H1A | 108.1 | N3—C8—C9 | 126.0 (2) |
| C6—C1—H1A | 108.1 | C10—C8—C9 | 119.19 (19) |
| C1—C2—C3 | 111.7 (3) | C8—C9—H9A | 109.5 |
| C1—C2—H2A | 109.3 | C8—C9—H9B | 109.5 |
| C3—C2—H2A | 109.3 | H9A—C9—H9B | 109.5 |
| C1—C2—H2B | 109.3 | C8—C9—H9C | 109.5 |
| C3—C2—H2B | 109.3 | H9A—C9—H9C | 109.5 |
| H2A—C2—H2B | 107.9 | H9B—C9—H9C | 109.5 |
| C4—C3—C2 | 111.2 (3) | N4—C10—C11 | 122.2 (2) |
| C4—C3—H3A | 109.4 | N4—C10—C8 | 116.23 (19) |
| C2—C3—H3A | 109.4 | C11—C10—C8 | 121.5 (2) |
| C4—C3—H3B | 109.4 | C12—C11—C10 | 119.0 (2) |
| C2—C3—H3B | 109.4 | C12—C11—H11 | 120.5 |
| H3A—C3—H3B | 108.0 | C10—C11—H11 | 120.5 |
| C5—C4—C3 | 110.2 (3) | C13—C12—C11 | 118.8 (2) |
| C5—C4—H4A | 109.6 | C13—C12—H12 | 120.6 |
| C3—C4—H4A | 109.6 | C11—C12—H12 | 120.6 |
| C5—C4—H4B | 109.6 | C12—C13—C14 | 118.7 (3) |
| C3—C4—H4B | 109.6 | C12—C13—H13 | 120.7 |
| H4A—C4—H4B | 108.1 | C14—C13—H13 | 120.7 |
| C4—C5—C6 | 111.9 (3) | N4—C14—C13 | 123.6 (3) |
| C4—C5—H5A | 109.2 | N4—C14—H14 | 118.2 |
| C6—C5—H5A | 109.2 | C13—C14—H14 | 118.2 |
| C4—C5—H5B | 109.2 | ||
| C7—N2—N3—C8 | 173.2 (2) | N2—N3—C8—C10 | −178.40 (18) |
| C7—N1—C1—C2 | 87.7 (3) | N2—N3—C8—C9 | 0.0 (3) |
| C7—N1—C1—C6 | −149.0 (2) | C14—N4—C10—C11 | 0.3 (4) |
| N1—C1—C2—C3 | 178.0 (3) | C14—N4—C10—C8 | −179.7 (2) |
| C6—C1—C2—C3 | 54.9 (3) | N3—C8—C10—N4 | 164.7 (2) |
| C1—C2—C3—C4 | −56.3 (4) | C9—C8—C10—N4 | −13.9 (3) |
| C2—C3—C4—C5 | 56.3 (4) | N3—C8—C10—C11 | −15.3 (3) |
| C3—C4—C5—C6 | −56.3 (4) | C9—C8—C10—C11 | 166.1 (2) |
| N1—C1—C6—C5 | −177.8 (2) | N4—C10—C11—C12 | −0.7 (4) |
| C2—C1—C6—C5 | −54.2 (3) | C8—C10—C11—C12 | 179.3 (2) |
| C4—C5—C6—C1 | 55.7 (4) | C10—C11—C12—C13 | 0.4 (4) |
| C1—N1—C7—N2 | −176.6 (2) | C11—C12—C13—C14 | 0.2 (4) |
| C1—N1—C7—S1 | 4.3 (3) | C10—N4—C14—C13 | 0.3 (5) |
| N3—N2—C7—N1 | 8.8 (3) | C12—C13—C14—N4 | −0.6 (5) |
| N3—N2—C7—S1 | −172.17 (15) |
Hydrogen-bond geometry (Å, °)
| Cg1 is the centroid of the pyridyl ring [ok as edited?] |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1···N3 | 0.87 (2) | 2.16 (2) | 2.592 (3) | 111 (2) |
| C9—H9C···N4 | 0.96 | 2.39 | 2.822 (3) | 107 |
| N2—H2···S1i | 0.88 (2) | 2.73 (2) | 3.610 (2) | 174 (2) |
| C9—H9B···Cg1ii | 0.96 | 2.89 | 3.776 (3) | 155 |
Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) x+1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5008).
References
- Agilent Technologies (2010). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
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- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Lai, C. S. & Tiekink, E. R. T. (2002). Acta Cryst. E58, o538–o539.
- Muramulla, S., Arman, H. D., Zhao, C.-G. & Tiekink, E. R. T. (2009). Acta Cryst. E65, o3070. [DOI] [PMC free article] [PubMed]
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- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
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/S1600536811009317/hg5008sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009317/hg5008Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



