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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Oct 20;68(Pt 11):m1368. doi: 10.1107/S1600536812042456

Potassium N-bromo-2,4-dichloro­benzene­sulfonamidate sesquihydrate

B Thimme Gowda a,*, Sabine Foro b, H S Spandana a
PMCID: PMC3515121  PMID: 23284348

Abstract

The asymmetric unit of the title salt, K+·C6H3BrCl2NO2S·1.5H2O, contains one K+ cation, one N-bromo-2,4-dichlorobenzenesulfonamidate anion, one water molecule in general position and one water molecule located on a twofold rotation axis. The K+ cation is hepta-coordinated by three water O atoms and four sulfonyl O atoms from three symmetry-related N-bromo-2,4-dichloro­benzene­sulfonamide anions. The S=N distance of 1.575 (3) Å is consistent with that of a double bond. In the crystal, the anions are linked by O—H⋯Br and O—H⋯N hydrogen bonds into layers parallel to the ac plane.

Related literature  

For preparation of N-haloaryl­sulfonamides, see: Gowda & Mahadevappa (1983). For studies of the effect of substituents on the structures of N-haloaryl­sulfonamides, see: George et al. (2000); Gowda et al. (2007, 2011a ,b ); Olmstead & Power (1986).graphic file with name e-68-m1368-scheme1.jpg

Experimental  

Crystal data  

  • K+·C6H3BrCl2NO2S·1.5H2O

  • M r = 740.18

  • Monoclinic, Inline graphic

  • a = 12.5263 (7) Å

  • b = 6.7638 (4) Å

  • c = 29.703 (2) Å

  • β = 98.352 (5)°

  • V = 2489.9 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 4.22 mm−1

  • T = 293 K

  • 0.32 × 0.32 × 0.28 mm

Data collection  

  • Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector

  • Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) T min = 0.345, T max = 0.384

  • 4960 measured reflections

  • 2535 independent reflections

  • 2204 reflections with I > 2σ(I)

  • R int = 0.014

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.037

  • wR(F 2) = 0.093

  • S = 1.09

  • 2535 reflections

  • 150 parameters

  • 3 restraints

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

  • Δρmax = 0.76 e Å−3

  • Δρmin = −0.65 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2009); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2009); 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: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812042456/nc2295sup1.cif

e-68-m1368-sup1.cif (23KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042456/nc2295Isup2.hkl

e-68-m1368-Isup2.hkl (124.6KB, hkl)

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

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

D—H⋯A D—H H⋯A DA D—H⋯A
O3—H31⋯Br1i 0.80 (2) 2.78 (2) 3.550 (3) 160 (4)
O3—H32⋯N1 0.81 (2) 2.15 (3) 2.917 (4) 158 (5)
O4—H41⋯N1ii 0.82 (2) 2.16 (2) 2.957 (3) 165 (5)

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

Acknowledgments

BTG thanks the University Grants Commission, Government of India, New Delhi, for a one-time grant to Faculty/Professors under UGC–BSR.

supplementary crystallographic information

Comment

The present work was undertaken in order to explore the effect of replacing sodium ion by potassium ion on the solid state structures of metal salts of N-haloarylsulfonamidates (Gowda et al., 2007, 2011a,b). As part of this work, the structure of potassium N-bromo-2,4-dichlorobenzenesulfonamidate sesquihydrate (I) has been determined (Fig. 1). The structure of (I) resembles those of potassium N-bromo-2-chlorobenzenesulfonamidate sesquihydrate (II) (Gowda et al., 2011a), potassium N-bromo-4-chlorobenzenesulfonamidate sesquihydrate (III) (Gowda et al., 2011b), sodium N-bromo-2,4-dichlorobenzenesulfonamidate sesquihydrate (IV) (Gowda et al., 2007) and other sodium N-chloro-arylsulfonamidates (George et al., 2000; Olmstead & Power, 1986).

In the title compound, K+ ion is hepta coordinated by three O atoms from water molecules and four sulfonyl O atoms of three different N-bromo-2,4-dichlorobenzenesulfonamide anions. The replacement of Na+ by K+ changes co-ordination from hexa to hepta in the structure (Gowda et al., 2007) and other parameters.

The S—N distance of 1.575 (3) Å is consistent with a S—N double bond and is in agreement with the observed values of 1.582 (4) Å in (II), 1.584 (6) Å in (III) and 1.590 (6) Å in (IV).

The asymmetric unit of (I) consists of one potassium cation, one N-bromo-2,4-dichlorobenzenesulfonamidate anion and one water molecule in general position and and one water molecule located on a twofold rotation axis.

In the crystal structure the anions are linked by intermolecular O—H···Br and O—H···N hydrogen bonding into layers, that are parallel to the ac plane (Fig. 2 and Table 1).

Experimental

The title compound was prepared by a method similar to the one described by Gowda & Mahadevappa (Gowda & Mahadevappa, 1983). 2 g of 2,4-dichlorobenzenesulfonamide was dissolved with stirring in 40 ml of 5M KOH at room temperature. The resultant solution was cooled in ice and 4 ml of liquid bromine was added drop wise with constant stirring. The resultant potassium salt of N-bromo-2,4-dichlorobenzenesulfonamide was filtered under suction, washed quickly with a minimum quantity of ice cold water. The purity of the compound was checked by determining its melting point (203–205° C) and estimating, iodometrically, the amount of active bromine present in it. It was further characterized from its infrared spectrum.

Prism like yellow single crystals of the title compound used in the X-ray diffraction studies were obtained from its aqueous solution at room temperature.

Refinement

H atoms bonded to C were positioned with idealized geometry using a riding model with the aromatic C—H = 0.93 Å. The H atoms bound to O atoms were located in difference map and later restrained to O—H = 0.82 (2) Å. All H atoms were refined with isotropic displacement parameters set at 1.2 Ueq of the parent atom.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound, showing the atom labelling scheme for the asymmetric unit and extended to show the coordination geometry for the K+. The displacement ellipsoids are drawn at the 50% probability level. The H atoms are represented as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

Molecular packing of the title compound with hydrogen bonding shown as dashed lines.

Crystal data

K+·C6H3BrCl2NO2S·1.5H2O F(000) = 1448
Mr = 740.18 Dx = 1.975 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2yc Cell parameters from 2489 reflections
a = 12.5263 (7) Å θ = 3.0–27.7°
b = 6.7638 (4) Å µ = 4.22 mm1
c = 29.703 (2) Å T = 293 K
β = 98.352 (5)° Prism, yellow
V = 2489.9 (3) Å3 0.32 × 0.32 × 0.28 mm
Z = 4

Data collection

Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector 2535 independent reflections
Radiation source: fine-focus sealed tube 2204 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.014
Rotation method data acquisition using ω scans. θmax = 26.4°, θmin = 3.3°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009) h = −15→13
Tmin = 0.345, Tmax = 0.384 k = −8→5
4960 measured reflections l = −37→22

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)] = 0.037 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.093 H atoms treated by a mixture of independent and constrained refinement
S = 1.09 w = 1/[σ2(Fo2) + (0.0429P)2 + 8.3581P] where P = (Fo2 + 2Fc2)/3
2535 reflections (Δ/σ)max = 0.001
150 parameters Δρmax = 0.76 e Å3
3 restraints Δρmin = −0.65 e Å3

Special details

Experimental. Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
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
C1 0.0780 (3) 0.4566 (5) 0.11591 (11) 0.0271 (7)
C2 0.1438 (3) 0.3775 (5) 0.08637 (12) 0.0317 (7)
C3 0.1538 (3) 0.4716 (6) 0.04598 (12) 0.0392 (9)
H3 0.1980 0.4192 0.0264 0.047*
C4 0.0974 (3) 0.6446 (6) 0.03496 (13) 0.0426 (9)
C5 0.0320 (3) 0.7248 (6) 0.06337 (14) 0.0447 (9)
H5 −0.0056 0.8413 0.0556 0.054*
C6 0.0228 (3) 0.6302 (5) 0.10361 (13) 0.0367 (8)
H6 −0.0214 0.6841 0.1230 0.044*
Br1 −0.11245 (3) 0.10625 (6) 0.130655 (14) 0.04440 (14)
Cl1 0.21550 (9) 0.15999 (15) 0.09788 (4) 0.0485 (3)
Cl2 0.10726 (10) 0.7571 (2) −0.01671 (4) 0.0650 (4)
K1 0.34306 (6) 0.13766 (12) 0.23492 (3) 0.0366 (2)
N1 0.0277 (2) 0.1274 (4) 0.16389 (10) 0.0319 (6)
O1 0.1712 (2) 0.3416 (4) 0.19584 (8) 0.0386 (6)
O2 −0.0093 (2) 0.4804 (4) 0.18845 (8) 0.0383 (6)
O3 0.2037 (2) −0.1486 (4) 0.19206 (10) 0.0426 (6)
H31 0.234 (3) −0.195 (7) 0.1725 (12) 0.051*
H32 0.155 (3) −0.088 (6) 0.1774 (14) 0.051*
O4 0.5000 0.4277 (6) 0.2500 0.0471 (10)
H41 0.490 (4) 0.502 (6) 0.2710 (11) 0.056*
S1 0.06429 (7) 0.34987 (12) 0.16983 (3) 0.02745 (19)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0271 (16) 0.0256 (16) 0.0280 (16) −0.0039 (13) 0.0014 (12) −0.0003 (13)
C2 0.0261 (16) 0.0319 (18) 0.0371 (18) −0.0031 (14) 0.0042 (14) 0.0000 (15)
C3 0.0350 (19) 0.048 (2) 0.0364 (19) −0.0108 (17) 0.0109 (15) −0.0008 (17)
C4 0.040 (2) 0.048 (2) 0.038 (2) −0.0161 (18) −0.0006 (16) 0.0113 (17)
C5 0.047 (2) 0.036 (2) 0.050 (2) 0.0043 (18) 0.0016 (18) 0.0116 (18)
C6 0.0359 (19) 0.0322 (18) 0.041 (2) 0.0040 (15) 0.0036 (15) 0.0029 (15)
Br1 0.0342 (2) 0.0494 (3) 0.0498 (2) −0.00725 (17) 0.00672 (16) −0.01193 (18)
Cl1 0.0484 (6) 0.0376 (5) 0.0645 (7) 0.0110 (4) 0.0250 (5) 0.0029 (5)
Cl2 0.0592 (7) 0.0857 (9) 0.0483 (6) −0.0170 (6) 0.0024 (5) 0.0322 (6)
K1 0.0312 (4) 0.0354 (4) 0.0423 (4) 0.0051 (3) 0.0021 (3) −0.0034 (3)
N1 0.0307 (15) 0.0279 (15) 0.0373 (16) 0.0006 (12) 0.0060 (12) 0.0047 (12)
O1 0.0373 (14) 0.0399 (14) 0.0353 (14) 0.0026 (11) −0.0064 (11) 0.0010 (11)
O2 0.0444 (15) 0.0387 (14) 0.0339 (13) 0.0094 (12) 0.0130 (11) −0.0046 (11)
O3 0.0475 (17) 0.0380 (15) 0.0434 (16) 0.0052 (12) 0.0099 (13) 0.0004 (12)
O4 0.073 (3) 0.031 (2) 0.041 (2) 0.000 0.022 (2) 0.000
S1 0.0302 (4) 0.0260 (4) 0.0260 (4) 0.0028 (3) 0.0033 (3) 0.0000 (3)

Geometric parameters (Å, º)

C1—C6 1.384 (5) K1—O3 2.788 (3)
C1—C2 1.395 (5) K1—O1iii 2.895 (3)
C1—S1 1.787 (3) K1—O2iii 3.045 (3)
C2—C3 1.380 (5) K1—S1iii 3.4910 (12)
C2—Cl1 1.732 (4) N1—S1 1.575 (3)
C3—C4 1.381 (6) O1—S1 1.447 (3)
C3—H3 0.9300 O1—K1ii 2.895 (3)
C4—C5 1.370 (6) O2—S1 1.443 (3)
C4—Cl2 1.734 (4) O2—K1iv 2.683 (2)
C5—C6 1.375 (5) O2—K1ii 3.045 (3)
C5—H5 0.9300 O3—K1iii 2.740 (3)
C6—H6 0.9300 O3—H31 0.802 (19)
Br1—N1 1.890 (3) O3—H32 0.808 (19)
K1—O1 2.675 (3) O4—K1v 2.767 (3)
K1—O2i 2.683 (2) O4—H41 0.820 (19)
K1—O3ii 2.740 (3) S1—K1ii 3.4910 (12)
K1—O4 2.767 (3)
C6—C1—C2 118.5 (3) O3—K1—K1v 130.38 (6)
C6—C1—S1 118.0 (3) O1iii—K1—K1v 90.06 (6)
C2—C1—S1 123.4 (3) O2iii—K1—K1v 43.27 (5)
C3—C2—C1 120.4 (3) S1iii—K1—K1v 66.97 (2)
C3—C2—Cl1 117.0 (3) O1—K1—K1iii 94.01 (7)
C1—C2—Cl1 122.6 (3) O2i—K1—K1iii 103.41 (6)
C2—C3—C4 119.3 (4) O3ii—K1—K1iii 93.78 (7)
C2—C3—H3 120.4 O4—K1—K1iii 157.36 (5)
C4—C3—H3 120.4 O3—K1—K1iii 38.92 (6)
C5—C4—C3 121.4 (4) O1iii—K1—K1iii 38.01 (5)
C5—C4—Cl2 119.8 (3) O2iii—K1—K1iii 84.35 (5)
C3—C4—Cl2 118.8 (3) S1iii—K1—K1iii 61.08 (2)
C4—C5—C6 118.9 (4) K1v—K1—K1iii 120.90 (2)
C4—C5—H5 120.5 O1—K1—K1ii 41.78 (6)
C6—C5—H5 120.5 O2i—K1—K1ii 149.20 (6)
C5—C6—C1 121.5 (4) O3ii—K1—K1ii 39.74 (6)
C5—C6—H6 119.2 O4—K1—K1ii 78.55 (6)
C1—C6—H6 119.2 O3—K1—K1ii 108.70 (7)
O1—K1—O2i 123.54 (8) O1iii—K1—K1ii 107.85 (6)
O1—K1—O3ii 79.66 (9) O2iii—K1—K1ii 117.01 (6)
O2i—K1—O3ii 149.20 (9) S1iii—K1—K1ii 113.48 (3)
O1—K1—O4 102.28 (8) K1v—K1—K1ii 120.90 (2)
O2i—K1—O4 80.66 (7) K1iii—K1—K1ii 104.55 (3)
O3ii—K1—O4 74.11 (7) S1—N1—Br1 111.33 (16)
O1—K1—O3 75.45 (8) S1—O1—K1 151.14 (16)
O2i—K1—O3 85.56 (9) S1—O1—K1ii 101.80 (13)
O3ii—K1—O3 122.44 (5) K1—O1—K1ii 100.21 (8)
O4—K1—O3 161.68 (7) S1—O2—K1iv 165.01 (16)
O1—K1—O1iii 122.42 (5) S1—O2—K1ii 95.45 (12)
O2i—K1—O1iii 102.09 (8) K1iv—O2—K1ii 85.68 (7)
O3ii—K1—O1iii 76.13 (8) K1iii—O3—K1 101.34 (10)
O4—K1—O1iii 119.42 (6) K1iii—O3—H31 123 (4)
O3—K1—O1iii 75.21 (8) K1—O3—H31 106 (4)
O1—K1—O2iii 157.55 (8) K1iii—O3—H32 117 (4)
O2i—K1—O2iii 78.37 (9) K1—O3—H32 106 (3)
O3ii—K1—O2iii 78.12 (8) H31—O3—H32 102 (5)
O4—K1—O2iii 74.58 (7) K1—O4—K1v 89.71 (12)
O3—K1—O2iii 114.43 (8) K1—O4—H41 112 (3)
O1iii—K1—O2iii 48.19 (7) K1v—O4—H41 119 (3)
O1—K1—S1iii 142.27 (7) O2—S1—O1 114.34 (16)
O2i—K1—S1iii 91.31 (6) O2—S1—N1 115.83 (16)
O3ii—K1—S1iii 74.74 (7) O1—S1—N1 104.73 (16)
O4—K1—S1iii 96.86 (5) O2—S1—C1 104.25 (15)
O3—K1—S1iii 95.47 (7) O1—S1—C1 107.00 (16)
O1iii—K1—S1iii 23.94 (5) N1—S1—C1 110.46 (16)
O2iii—K1—S1iii 24.30 (5) O2—S1—K1ii 60.25 (11)
O1—K1—K1v 145.05 (6) O1—S1—K1ii 54.26 (11)
O2i—K1—K1v 51.05 (6) N1—S1—K1ii 132.87 (12)
O3ii—K1—K1v 98.18 (7) C1—S1—K1ii 115.93 (11)
O4—K1—K1v 45.15 (6)
C6—C1—C2—C3 0.3 (5) S1iii—K1—O3—K1iii 26.89 (8)
S1—C1—C2—C3 −177.6 (3) K1v—K1—O3—K1iii 91.14 (10)
C6—C1—C2—Cl1 −179.3 (3) K1ii—K1—O3—K1iii −90.17 (8)
S1—C1—C2—Cl1 2.9 (4) O1—K1—O4—K1v −165.19 (7)
C1—C2—C3—C4 −0.3 (5) O2i—K1—O4—K1v −42.70 (6)
Cl1—C2—C3—C4 179.3 (3) O3ii—K1—O4—K1v 119.46 (7)
C2—C3—C4—C5 0.1 (6) O3—K1—O4—K1v −84.4 (3)
C2—C3—C4—Cl2 −178.0 (3) O1iii—K1—O4—K1v 55.99 (7)
C3—C4—C5—C6 0.0 (6) O2iii—K1—O4—K1v 37.71 (5)
Cl2—C4—C5—C6 178.1 (3) S1iii—K1—O4—K1v 47.51 (2)
C4—C5—C6—C1 −0.1 (6) K1iii—K1—O4—K1v 59.77 (14)
C2—C1—C6—C5 −0.1 (5) K1ii—K1—O4—K1v 160.16 (4)
S1—C1—C6—C5 177.9 (3) K1iv—O2—S1—O1 −89.2 (6)
O2i—K1—O1—S1 77.2 (4) K1ii—O2—S1—O1 4.50 (17)
O3ii—K1—O1—S1 −124.9 (3) K1iv—O2—S1—N1 32.8 (7)
O4—K1—O1—S1 164.0 (3) K1ii—O2—S1—N1 126.44 (14)
O3—K1—O1—S1 2.7 (3) K1iv—O2—S1—C1 154.3 (6)
O1iii—K1—O1—S1 −58.8 (3) K1ii—O2—S1—C1 −111.99 (12)
O2iii—K1—O1—S1 −116.7 (3) K1iv—O2—S1—K1ii −93.7 (6)
S1iii—K1—O1—S1 −77.2 (4) K1—O1—S1—O2 134.2 (3)
K1v—K1—O1—S1 145.6 (3) K1ii—O1—S1—O2 −4.81 (18)
K1iii—K1—O1—S1 −31.8 (3) K1—O1—S1—N1 6.3 (4)
K1ii—K1—O1—S1 −139.2 (4) K1ii—O1—S1—N1 −132.65 (13)
O2i—K1—O1—K1ii −143.58 (9) K1—O1—S1—C1 −111.0 (3)
O3ii—K1—O1—K1ii 14.32 (8) K1ii—O1—S1—C1 110.07 (14)
O4—K1—O1—K1ii −56.74 (8) K1—O1—S1—K1ii 139.0 (4)
O3—K1—O1—K1ii 141.96 (10) Br1—N1—S1—O2 52.7 (2)
O1iii—K1—O1—K1ii 80.46 (13) Br1—N1—S1—O1 179.61 (16)
O2iii—K1—O1—K1ii 22.6 (2) Br1—N1—S1—C1 −65.5 (2)
S1iii—K1—O1—K1ii 62.01 (13) Br1—N1—S1—K1ii 125.06 (12)
K1v—K1—O1—K1ii −75.18 (13) C6—C1—S1—O2 1.3 (3)
K1iii—K1—O1—K1ii 107.44 (7) C2—C1—S1—O2 179.2 (3)
O1—K1—O3—K1iii −115.86 (10) C6—C1—S1—O1 −120.2 (3)
O2i—K1—O3—K1iii 117.79 (9) C2—C1—S1—O1 57.7 (3)
O3ii—K1—O3—K1iii −48.49 (13) C6—C1—S1—N1 126.4 (3)
O4—K1—O3—K1iii 159.0 (2) C2—C1—S1—N1 −55.8 (3)
O1iii—K1—O3—K1iii 14.03 (8) C6—C1—S1—K1ii −62.2 (3)
O2iii—K1—O3—K1iii 42.71 (11) C2—C1—S1—K1ii 115.6 (3)

Symmetry codes: (i) x+1/2, y−1/2, z; (ii) −x+1/2, y+1/2, −z+1/2; (iii) −x+1/2, y−1/2, −z+1/2; (iv) x−1/2, y+1/2, z; (v) −x+1, y, −z+1/2.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
O3—H31···Br1i 0.80 (2) 2.78 (2) 3.550 (3) 160 (4)
O3—H32···N1 0.81 (2) 2.15 (3) 2.917 (4) 158 (5)
O4—H41···N1ii 0.82 (2) 2.16 (2) 2.957 (3) 165 (5)

Symmetry codes: (i) x+1/2, y−1/2, z; (ii) −x+1/2, y+1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NC2295).

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 datablock(s) I, global. DOI: 10.1107/S1600536812042456/nc2295sup1.cif

e-68-m1368-sup1.cif (23KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042456/nc2295Isup2.hkl

e-68-m1368-Isup2.hkl (124.6KB, hkl)

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


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