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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 4;67(Pt 7):o1561. doi: 10.1107/S1600536811019465

N-[7-Eth­oxy-1-(prop-2-en-1-yl)-1H-indazol-4-yl]-4-methyl­benzene­sulfonamide

Najat Abbassi a, El Mostapha Rakib a,*, Hafid Zouihri b
PMCID: PMC3151999  PMID: 21836974

Abstract

In the title compound, C19H21N3O3S, the C—SO2—NH—C torsion angle is 103.72 (11)°. The almost planar indazole ring [r.m.s. deviation = 0.0202 (14) Å] is twisted away from the methyl­benzene ring by 76.87 (7)°. The vinyl group is disordered over two orientations with site occupancies of 0.622 (10) and 0.378 (10). The S atom has a distorted tetra­hedral geometry [maximum deviation: O—S—O = 119.18 (11)°]. An intra­molecular C—H⋯O hydrogen bond occurs. In the crystal, two mol­ecules are linked about a center of inversion by pairs of N—H⋯O hydrogen bonds, generating a dimer. C—H⋯π inter­actions are also observed.

Related literature

For a related structure, see: Abbassi et al. (2011b ). For the biological activity of sulfonamides, see: Soledade et al. (2006); Lee & Lee (2002). For the synthesis of 7-eth­oxy-N-alkyl­indazole derivatives, see: Abbassi et al. (2011a ).graphic file with name e-67-o1561-scheme1.jpg

Experimental

Crystal data

  • C19H21N3O3S

  • M r = 371.45

  • Triclinic, Inline graphic

  • a = 8.2208 (3) Å

  • b = 10.4985 (4) Å

  • c = 11.9655 (5) Å

  • α = 108.814 (2)°

  • β = 92.346 (2)°

  • γ = 107.500 (2)°

  • V = 921.33 (6) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.20 mm−1

  • T = 296 K

  • 0.32 × 0.17 × 0.12 mm

Data collection

  • Bruker APEXII CCD detector diffractometer

  • 23139 measured reflections

  • 3629 independent reflections

  • 3281 reflections with I > 2σ(I)

  • R int = 0.023

Refinement

  • R[F 2 > 2σ(F 2)] = 0.042

  • wR(F 2) = 0.118

  • S = 1.08

  • 3629 reflections

  • 259 parameters

  • 6 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.39 e Å−3

  • Δρmin = −0.32 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811019465/ng5164sup1.cif

e-67-o1561-sup1.cif (19.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811019465/ng5164Isup2.hkl

e-67-o1561-Isup2.hkl (177.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811019465/ng5164Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

Cg1 is the centroid of the C7–C12 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3⋯O3i 0.86 (2) 2.15 (2) 3.002 (2) 171 (2)
C14—H14B⋯O1 0.97 2.35 2.974 (2) 121
C19—H19CCg1ii 0.96 2.87 3.622 (2) 136

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors thank the Unit of Support for Technical and Scientific Research (UATRS, CNRST) for the X-ray measurements.

supplementary crystallographic information

Comment

Various sulfonamides are widely used as anti-hypertensive [Soledade et al., 2006; Lee & Lee, 2002]. In a former paper, we reported the crystal structure of N-(7-ethoxy-1H-indazol-4-yl)-4-methylbenzenesulfonamide [Abbassi et al., 2011b]. In this communication, the crystal structure of N-[7-ethoxy-1-(prop-2-en-1-yl)-1H-indazol-4-yl]-4-methylbenzenesulfonamide is reported.

The title heterocyclic compound, C19H21N3O3S, is a new synthetic molecule whish is bent at the S atom with an C—SO~2~—NH—C torsion angle of 103.72 (11)°. The indazol planar ring [r.m.s. deviation: 0.0202 (14) Å] is twisted away from the methylbenzene ring by 76.87 (7)°. The vinyl group is disordered over two positions with site occupancies of 0.622 (10) and 0.378 (10). The S atom has a distorted tetrahedral geometry [maximum deviation: O—S—O = 119.17 (10)°].

In the crystal structure, the molecules are linked by N—H···O hydrogen bonds together with weak C—H···O interactions. There also exist C—H···Cg contacts between the methyl groups of the methylbenzene and the indazol rings. The crystal structure is further stabilized by intermolecular π–π stacking interactions [centroid–centroid distances = 3.6673 (9)–3.8109 (10) A °].

Experimental

A mixture of 1-allyl-4-nitro-1H-indazole [Abbassi et al., 2011a] (1.22 mmol) and anhydrous SnCl2 (1.1 g, 6.1 mmol) in 25 mL of absolute ethanol was heated at 60 °C for 2 h. After reduction, the starting material disappeared, and the solution was allowed to cool down. The pH was made slightly basic (pH 7–8) by addition of 5% aqueous potassium bicarbonate before extraction with ethyl acetate. The organic phase was washed with brine and dried over magnesium sulfate. The solvent was removed to afford the amine, which was immediately dissolved in pyridine (5 ml) and then reacted with 4-methylbenzenesulfonyl chloride (0.26 g, 1.25 mmol) at room temperature for 24 h. After the reaction mixture was concentrated in vacuo, the resulting residue was purified by flash chromatography (eluted with Ethyl acetate: Hexane 1:9).

Refinement

The H atoms bound to C were positioned geometrically and constrained to ride on their parent atoms [C—H distances are 0.93Å for CH groups with Uiso(H) = 1.2 Ueq(C), and 0.97 Å for CH3 groups, and the N3—H3 atoms were refined with restraints (dN–H = 0.86 (2) Å) and then were treated as riding in the last cycles of refinement. The vinyl group is disordered over two positions with site occupancies of 0.622 (10) and 0.378 (10), the corresponding C—C and C==C distances in the major and minor conformers were refined with distance restraints of: 1.54 (2) Å and 1.35 (2) Å, respectively.

Figures

Fig. 1.

Fig. 1.

Molecular view of the title compound showing the atom-labeling scheme. Displacement ellipsoids are drawn at the 30% probability level. H atoms are represented as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

Partial packing view showing the chain formed by N—H···O. H atoms not involved in hydrogen bonds have been omitted for clarity.

Crystal data

C19H21N3O3S Z = 2
Mr = 371.45 F(000) = 392
Triclinic, P1 Dx = 1.339 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.2208 (3) Å Cell parameters from 341 reflections
b = 10.4985 (4) Å θ = 2.5–27.9°
c = 11.9655 (5) Å µ = 0.20 mm1
α = 108.814 (2)° T = 296 K
β = 92.346 (2)° Prism, colourless
γ = 107.500 (2)° 0.32 × 0.17 × 0.12 mm
V = 921.33 (6) Å3

Data collection

Bruker APEXII CCD detector diffractometer 3281 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.023
graphite θmax = 26.0°, θmin = 2.2°
ω and φ scans h = −10→9
23139 measured reflections k = −12→12
3629 independent reflections l = −14→14

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)] = 0.042 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118 H atoms treated by a mixture of independent and constrained refinement
S = 1.08 w = 1/[σ2(Fo2) + (0.053P)2 + 0.4364P] where P = (Fo2 + 2Fc2)/3
3629 reflections (Δ/σ)max < 0.001
259 parameters Δρmax = 0.39 e Å3
6 restraints Δρmin = −0.32 e Å3

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 Occ. (<1)
C1 −0.1369 (3) 0.4744 (3) 0.2566 (2) 0.0518 (6)
C10 0.4698 (3) 0.9705 (2) 0.33160 (18) 0.0362 (4)
C11 0.5617 (2) 0.8894 (2) 0.36197 (17) 0.0345 (4)
C12 0.4804 (3) 0.7709 (2) 0.39361 (17) 0.0346 (4)
C13 0.6165 (3) 0.7239 (3) 0.4207 (2) 0.0444 (5)
C14 0.8737 (3) 1.0072 (3) 0.3443 (2) 0.0574 (7)
C15 0.4773 (4) 1.1700 (3) 0.2738 (3) 0.0595 (7)
C16 0.4069 (5) 1.1104 (4) 0.1447 (3) 0.0873 (10)
C17A 0.8898 (7) 0.9302 (9) 0.2134 (5) 0.0553 (16) 0.622 (10)
C17B 0.9147 (12) 1.0054 (12) 0.2270 (8) 0.057 (3) 0.378 (10)
C18A 0.8938 (10) 0.9902 (9) 0.1303 (6) 0.101 (3) 0.622 (10)
C18B 0.8493 (13) 0.8767 (12) 0.1399 (10) 0.079 (4) 0.378 (10)
C19 −0.3856 (5) 0.3527 (4) −0.0543 (3) 0.0891 (11)
C2 −0.2614 (4) 0.4503 (3) 0.1640 (2) 0.0587 (7)
C3 −0.2476 (4) 0.3819 (3) 0.0462 (2) 0.0596 (7)
C4 −0.1046 (4) 0.3413 (3) 0.0237 (2) 0.0697 (8)
C5 0.0215 (4) 0.3650 (3) 0.1146 (2) 0.0595 (7)
C6 0.0038 (3) 0.4302 (2) 0.2315 (2) 0.0422 (5)
C7 0.3012 (3) 0.7306 (2) 0.39635 (17) 0.0348 (4)
C8 0.2116 (3) 0.8081 (2) 0.36507 (19) 0.0395 (5)
C9 0.2950 (3) 0.9261 (2) 0.3323 (2) 0.0408 (5)
H1 −0.1478 0.5201 0.3352 0.062*
H13 0.6020 0.6459 0.4448 0.053*
H14A 0.9800 1.0318 0.3969 0.069*
H14B 0.8479 1.0937 0.3523 0.069*
H15A 0.5564 1.2664 0.2933 0.071*
H15B 0.3835 1.1747 0.3199 0.071*
H16A 0.4981 1.0999 0.0987 0.131*
H16B 0.3571 1.1738 0.1251 0.131*
H16C 0.3198 1.0189 0.1266 0.131*
H17A 0.8970 0.8388 0.1918 0.066* 0.622 (10)
H17B 0.9807 1.0864 0.2132 0.069* 0.378 (10)
H18A 0.8868 1.0814 0.1503 0.121* 0.622 (10)
H18B 0.9036 0.9407 0.0523 0.121* 0.622 (10)
H18C 0.7840 0.7984 0.1577 0.095* 0.378 (10)
H18D 0.8694 0.8659 0.0620 0.095* 0.378 (10)
H19A −0.3360 0.3474 −0.1263 0.134*
H19B −0.4341 0.4283 −0.0346 0.134*
H19C −0.4746 0.2638 −0.0662 0.134*
H2 −0.3559 0.4805 0.1810 0.070*
H3 0.146 (3) 0.630 (3) 0.484 (2) 0.049*
H4 −0.0927 0.2968 −0.0549 0.084*
H5 0.1176 0.3372 0.0973 0.071*
H8 0.0931 0.7822 0.3655 0.047*
H9 0.2298 0.9753 0.3105 0.049*
N1 0.7663 (2) 0.8046 (2) 0.40729 (19) 0.0497 (5)
N2 0.7338 (2) 0.9065 (2) 0.37229 (17) 0.0424 (4)
N3 0.2190 (2) 0.61730 (19) 0.43869 (17) 0.0405 (4)
O1 0.5640 (2) 1.08767 (18) 0.30610 (17) 0.0553 (4)
O2 0.3035 (2) 0.42371 (19) 0.29865 (18) 0.0590 (5)
O3 0.0727 (2) 0.37090 (18) 0.41924 (17) 0.0571 (5)
S1 0.15828 (7) 0.45175 (6) 0.34923 (5) 0.04300 (19)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0504 (13) 0.0580 (14) 0.0400 (12) 0.0181 (11) 0.0053 (10) 0.0081 (10)
C10 0.0355 (10) 0.0370 (10) 0.0364 (10) 0.0126 (8) 0.0059 (8) 0.0128 (8)
C11 0.0286 (9) 0.0394 (10) 0.0318 (9) 0.0119 (8) 0.0019 (7) 0.0076 (8)
C12 0.0331 (10) 0.0369 (10) 0.0316 (9) 0.0140 (8) 0.0005 (8) 0.0076 (8)
C13 0.0416 (12) 0.0485 (12) 0.0483 (12) 0.0224 (10) 0.0022 (9) 0.0177 (10)
C14 0.0285 (11) 0.0816 (18) 0.0628 (15) 0.0110 (11) 0.0078 (10) 0.0330 (14)
C15 0.0690 (17) 0.0516 (14) 0.0642 (16) 0.0189 (13) 0.0112 (13) 0.0293 (13)
C16 0.105 (3) 0.093 (3) 0.071 (2) 0.032 (2) 0.0053 (19) 0.0394 (19)
C17A 0.038 (2) 0.072 (4) 0.064 (4) 0.016 (3) 0.014 (2) 0.037 (4)
C17B 0.059 (5) 0.059 (5) 0.073 (6) 0.024 (5) 0.023 (4) 0.043 (5)
C18A 0.117 (6) 0.114 (6) 0.070 (4) 0.022 (4) 0.018 (3) 0.044 (4)
C18B 0.074 (6) 0.114 (9) 0.049 (5) 0.037 (6) 0.013 (5) 0.021 (6)
C19 0.099 (3) 0.098 (3) 0.0555 (17) 0.038 (2) −0.0175 (17) 0.0068 (17)
C2 0.0527 (14) 0.0640 (16) 0.0520 (14) 0.0207 (12) 0.0015 (11) 0.0103 (12)
C3 0.0698 (17) 0.0534 (14) 0.0446 (13) 0.0157 (13) −0.0038 (12) 0.0089 (11)
C4 0.088 (2) 0.0736 (19) 0.0408 (13) 0.0338 (17) 0.0084 (13) 0.0049 (13)
C5 0.0667 (17) 0.0604 (16) 0.0495 (14) 0.0285 (13) 0.0133 (12) 0.0093 (12)
C6 0.0446 (12) 0.0341 (10) 0.0426 (11) 0.0087 (9) 0.0063 (9) 0.0107 (9)
C7 0.0329 (10) 0.0345 (10) 0.0337 (10) 0.0099 (8) 0.0028 (8) 0.0090 (8)
C8 0.0285 (10) 0.0442 (11) 0.0453 (11) 0.0129 (8) 0.0052 (8) 0.0146 (9)
C9 0.0354 (11) 0.0448 (11) 0.0488 (12) 0.0200 (9) 0.0048 (9) 0.0190 (10)
N1 0.0374 (10) 0.0607 (12) 0.0561 (12) 0.0245 (9) 0.0037 (8) 0.0201 (10)
N2 0.0287 (9) 0.0521 (11) 0.0468 (10) 0.0156 (8) 0.0046 (7) 0.0160 (8)
N3 0.0408 (10) 0.0393 (10) 0.0401 (10) 0.0109 (8) 0.0068 (8) 0.0144 (8)
O1 0.0415 (9) 0.0510 (10) 0.0749 (12) 0.0130 (7) 0.0121 (8) 0.0259 (9)
O2 0.0538 (10) 0.0526 (10) 0.0732 (12) 0.0269 (8) 0.0122 (9) 0.0164 (9)
O3 0.0664 (11) 0.0446 (9) 0.0658 (11) 0.0143 (8) 0.0097 (9) 0.0303 (8)
S1 0.0451 (3) 0.0360 (3) 0.0494 (3) 0.0139 (2) 0.0067 (2) 0.0166 (2)

Geometric parameters (Å, °)

C1—H1 0.9300 C18B—C17B 1.345 (12)
C1—C2 1.382 (4) C19—H19C 0.9600
C10—O1 1.376 (3) C19—H19B 0.9600
C10—C9 1.372 (3) C19—H19A 0.9600
C11—C10 1.412 (3) C2—H2 0.9300
C11—C12 1.401 (3) C2—C3 1.388 (4)
C11—N2 1.366 (3) C3—C19 1.506 (4)
C12—C13 1.417 (3) C3—C4 1.374 (4)
C13—H13 0.9300 C4—H4 0.9300
C13—N1 1.317 (3) C5—H5 0.9300
C14—H14B 0.9700 C5—C4 1.378 (4)
C14—H14A 0.9700 C6—C1 1.381 (3)
C14—C17A 1.546 (7) C6—C5 1.380 (3)
C14—C17B 1.453 (8) C7—N3 1.436 (3)
C15—H15B 0.9700 C7—C12 1.410 (3)
C15—H15A 0.9700 C7—C8 1.370 (3)
C15—C16 1.483 (4) C8—H8 0.9300
C16—H16C 0.9600 C8—C9 1.408 (3)
C16—H16B 0.9600 C9—H9 0.9300
C16—H16A 0.9600 N2—C14 1.443 (3)
C17A—H17A 0.9300 N2—N1 1.358 (3)
C17A—C18A 1.335 (8) N3—H3 0.84 (3)
C17B—H17B 0.9300 O1—C15 1.403 (3)
C18A—H18B 0.9300 S1—C6 1.767 (2)
C18A—H18A 0.9300 S1—N3 1.6280 (19)
C18B—H18D 0.9300 S1—O3 1.4369 (17)
C18B—H18C 0.9300 S1—O2 1.4260 (18)
C2—C1—H1 120.3 C17A—C18A—H18B 120.0
C6—C1—H1 120.3 C17A—C18A—H18A 120.0
C6—C1—C2 119.5 (2) H18C—C18B—H18D 120.0
O1—C10—C11 117.06 (18) C17B—C18B—H18D 120.0
C9—C10—C11 116.67 (19) C17B—C18B—H18C 120.0
C9—C10—O1 126.26 (19) C3—C2—H2 119.5
C12—C11—C10 122.13 (18) C1—C2—H2 119.5
N2—C11—C10 131.2 (2) C1—C2—C3 121.1 (3)
N2—C11—C12 106.64 (18) C2—C3—C19 120.9 (3)
C7—C12—C13 136.1 (2) C4—C3—C19 120.9 (3)
C11—C12—C13 104.30 (18) C4—C3—C2 118.2 (3)
C11—C12—C7 119.59 (18) C5—C4—H4 119.1
C12—C13—H13 124.3 C3—C4—H4 119.1
N1—C13—H13 124.3 C3—C4—C5 121.7 (3)
N1—C13—C12 111.4 (2) C6—C5—H5 120.3
H14A—C14—H14B 108.8 C4—C5—H5 120.3
C17A—C14—H14B 110.7 C4—C5—C6 119.4 (3)
C17B—C14—H14B 86.7 C1—C6—S1 120.01 (17)
N2—C14—H14B 110.7 C5—C6—S1 119.80 (19)
C17A—C14—H14A 110.7 C5—C6—C1 120.2 (2)
C17B—C14—H14A 108.8 C12—C7—N3 120.09 (18)
N2—C14—H14A 110.7 C8—C7—N3 121.55 (18)
C17B—C14—C17A 27.3 (3) C8—C7—C12 118.23 (19)
N2—C14—C17A 105.1 (3) C9—C8—H8 119.3
N2—C14—C17B 127.8 (5) C7—C8—H8 119.3
H15A—C15—H15B 107.9 C7—C8—C9 121.47 (19)
C16—C15—H15B 109.2 C8—C9—H9 119.1
O1—C15—H15B 109.2 C10—C9—H9 119.1
C16—C15—H15A 109.2 C10—C9—C8 121.89 (19)
O1—C15—H15A 109.2 C13—N1—N2 106.45 (17)
O1—C15—C16 112.1 (3) C11—N2—C14 129.6 (2)
H16B—C16—H16C 109.5 N1—N2—C14 119.12 (19)
H16A—C16—H16C 109.5 N1—N2—C11 111.18 (18)
C15—C16—H16C 109.5 S1—N3—H3 110.4 (19)
H16A—C16—H16B 109.5 C7—N3—H3 116.7 (18)
C15—C16—H16B 109.5 C7—N3—S1 120.46 (15)
C15—C16—H16A 109.5 C10—O1—C15 118.87 (19)
C14—C17A—H17A 118.9 N3—S1—C6 107.93 (10)
C18A—C17A—H17A 118.9 O3—S1—C6 108.09 (11)
C18A—C17A—C14 122.3 (7) O2—S1—C6 107.73 (11)
C14—C17B—H17B 122.8 O3—S1—N3 104.80 (10)
C18B—C17B—H17B 122.8 O2—S1—N3 108.66 (11)
C18B—C17B—C14 114.3 (9) O2—S1—O3 119.18 (11)
H18A—C18A—H18B 120.0

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the C7–C12 ring.
D—H···A D—H H···A D···A D—H···A
N3—H3···O3i 0.86 (2) 2.15 (2) 3.002 (2) 171 (2)
C5—H5···O2 0.93 2.53 2.908 (3) 104
C14—H14B···O1 0.97 2.35 2.974 (2) 121
C19—H19C···Cg1ii 0.96 2.87 3.622 (2) 136

Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x, −y+1, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5164).

References

  1. Abbassi, N., Rakib, E. M., Hannioui, A., Alaoui, M., Benchidmi, M., Essassi, E. M. & Geffken, D. (2011a). Heterocycles, 83, 891–900.
  2. Abbassi, N., Rakib, E. M. & Zouihri, H. (2011b). Acta Cryst. E67, o1354. [DOI] [PMC free article] [PubMed]
  3. Bruker (2005). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Lee, J. S. & Lee, C. H. (2002). Bull. Korean Chem. Soc. 23, 167–169.
  5. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  6. Soledade, M., Pedras, C. & Jha, M. (2006). Bioorg. Med. Chem. 14, 4958–4979. [DOI] [PubMed]
  7. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  8. 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 datablock(s) I, global. DOI: 10.1107/S1600536811019465/ng5164sup1.cif

e-67-o1561-sup1.cif (19.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811019465/ng5164Isup2.hkl

e-67-o1561-Isup2.hkl (177.9KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811019465/ng5164Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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