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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Dec 16;66(Pt 1):o152–o153. doi: 10.1107/S1600536809053367

7-Chloro-4-[(E)-N′-(4-fluoro­benzyl­idene)hydrazin­yl]quinoline monohydrate

Marcus V N de Souza a, R Alan Howie b, Edward R T Tiekink c,*, James L Wardell d,, Solange M S V Wardell e
PMCID: PMC2980273  PMID: 21580042

Abstract

The mol­ecule of the title hydrate, C16H11ClFN3·H2O, is slightly twisted, as indicated by the dihedral angle of 9.55 (10)° formed between the quinoline ring system and the benzene ring. The conformation about the C=N double bond is E, and the amine-H atom is oriented towards the quinoline residue. In the crystal structure, the water mol­ecule accepts an N—H⋯O and makes two O—H⋯Nquinoline hydrogen bonds, generating a two-dimensional array in the ab plane, which is further stabilized by C—H⋯O inter­actions. The most significant contacts between layers are of the type C—H⋯F.

Related literature

For background information on the pharmacological activity of quinoline derivatives, see: Elslager et al. (1969); Font et al. (1997); Kaminsky & Meltzer (1968); Musiol et al. (2006); Nakamura et al. (1999); Palmer et al. (1993); Ridley (2002); Sloboda et al. (1991); Tanenbaum & Tuffanelli (1980); Warshakoon et al. (2006). For recent studies into quinoline-based anti-malarials, see: Andrade et al. (2007); Cunico et al. (2006); da Silva et al. (2003); de Souza et al. (2005). For crystallographic studies on mol­ecules related to the title compound, see: Kaiser et al. (2009); de Souza et al. (2009); de Ferreira et al. (2009). For the synthesis, see: Pellerano et al. (1976).graphic file with name e-66-0o152-scheme1.jpg

Experimental

Crystal data

  • C16H11ClFN3·H2O

  • M r = 317.74

  • Monoclinic, Inline graphic

  • a = 3.7795 (2) Å

  • b = 15.4188 (11) Å

  • c = 24.8576 (16) Å

  • β = 90.286 (4)°

  • V = 1448.57 (16) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.28 mm−1

  • T = 120 K

  • 0.90 × 0.04 × 0.04 mm

Data collection

  • Nonius KappaCCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2007) T min = 0.614, T max = 0.746

  • 19494 measured reflections

  • 3291 independent reflections

  • 2009 reflections with I > 2σ(I)

  • R int = 0.098

Refinement

  • R[F 2 > 2σ(F 2)] = 0.059

  • wR(F 2) = 0.131

  • S = 1.04

  • 3291 reflections

  • 205 parameters

  • 3 restraints

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

  • Δρmax = 0.33 e Å−3

  • Δρmin = −0.37 e Å−3

Data collection: COLLECT (Hooft, 1998); cell refinement: DENZO (Otwinowski & Minor, 1997) and COLLECT; data reduction: DENZO and COLLECT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2006); software used to prepare material for publication: publCIF (Westrip, 2009).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809053367/lh2970sup1.cif

e-66-0o152-sup1.cif (19.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809053367/lh2970Isup2.hkl

e-66-0o152-Isup2.hkl (158.2KB, 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
O1w—H1w⋯N1i 0.84 (2) 2.28 (2) 2.999 (3) 144 (2)
O1w—H2w⋯N1ii 0.85 (2) 1.93 (2) 2.761 (3) 166 (3)
N2—H2n⋯O1wiii 0.88 2.01 2.865 (3) 165
C5—H5⋯O1wiii 0.95 2.45 3.379 (3) 164
C10—H10⋯O1wiii 0.95 2.50 3.302 (3) 142
C1—H1⋯F1iv 0.95 2.56 3.399 (3) 147
C6—H6⋯F1v 0.95 2.56 3.477 (3) 161

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic.

Acknowledgments

The use of the EPSRC X-ray crystallographic service at the University of Southampton, England and the valuable assistance of the staff there is gratefully acknowledged. JLW acknowledges support from CAPES (Brazil).

supplementary crystallographic information

Comment

The title compound, crystallized as a hydrate, (I), was prepared as part of continuing studies designed to develop antimalarial compounds based on the quinoline nucleus (Andrade et al., 2007; Cunico et al., 2006; da Silva et al., 2003; de Souza et al., 2005). The systematic examination of quinoline derivatives comes about owing to the fact that the majority of antimalarial agents, including chloroquine (Tanenbaum & Tuffanelli, 1980), mefloquine (Palmer et al., 1993), primaquine (Elslager et al., 1969) and amodiaquine (Ridley, 2002), have a quinoline ring substructure, the mainstay of malaria chemotherapy for much of the past 40 years (Font et al., 1997; Kaminsky & Meltzer, 1968; Musiol et al., 2006; Nakamura et al., 1999; Sloboda et al., 1991; Warshakoon et al., 2006). Allied with these investigations are structural studies aimed at elucidating systematic structural trends in these molecules (Kaiser et al. 2009; de Souza et al. 2009; de Ferreira et al. 2009).

The molecule in (I), Fig. 1, features an effectively planar quinoline residue (maximum deviations of 0.018 (2) Å for atom C4 and -0.025 (2) Å for atom C2) which forms a dihedral angle of 9.55 (10) ° with the C11–C16 benzene ring. Twists in the molecule are evident about the N2–C3 and C10–C11 bonds as seen in the values of the N3–N2–C3–C2 and N3–C10–C11—C12 torsion angles of 6.9 (4) and -6.6 (4) °, respectively. As observed in related systems, the amine-H is orientated over the quinoline residue (Kaiser et al. 2009; de Souza et al. 2009; de Ferreira et al., 2009). The conformation about the N3═C10 double bond is E. The molecule crystallizes as a hydrate and the latter species is pivotal in stabilizing the crystal structure. Thus, the water-H atoms form donor O–H···N hydrogen bonds to quinoline-N atoms derived from two molecules. At the same time, the water-O atom accepts a N–H···O hydrogen bond from the amine-N2 of another molecule. Thus, the water molecule provides links between three molecules, leading to the formation of a 2-D array, Fig. 2 and Table 1. The resultant layer in the ab plane is further stabilized by C–H···O interactions, Table 1, and weak π···π contacts [ring centroid(N1,C1—C4,C9)···ring centroid(C4–C9)i = 3.7070 (14) Å, dihedral angle = 1.45 (11) ° for i: -1 + x, y, z]. Layers stack along the c direction with the most significant contacts between layers being of the type C–H···F whereby the fluoride is bifurcated, Table 1 and Fig. 3.

Experimental

A solution of 7-chloro-4-hydrazinoquinoline (0.20 g, 1.0 mmol) and 4-fluorobenzaldehyde (0.15 g, 1.2 mmol) in EtOH (5 ml) was maintained at room temperature overnight and rotary evaporated. The solid residue, was washed with cold Et2O (3 x 10 ml) and recrystallized from EtOH m.pt. 518–519 K, lit. value 518 K (Pellerano et al., 1976), yield 74%. The sample for the X-ray study was slowly grown from moist EtOH and was found to be the monohydrate. 1H NMR (400 MHz, DMSO-d6) δ: 7.28–7.32 (3H, m), 7.54 (1H, d, J = 8.4 Hz), 7.84–7.88 (3H, m), 8.34–8.40 (3H, m), 11.3 (1H, br.s, NH). MS/ESI: [M+. - H]: 298. IR νmax (cm-1; KBr disc): 3232 (N–H), 1585 (C═N), 817 (C–F).

Refinement

The amine- and C-bound H atoms were geometrically placed (N–H = 0.88 Å and C–H = 0.95 Å) and refined as riding with Uiso(H) = 1.2Ueq(C). The water-bound H atoms were located from a difference map and refined (O–H = 0.84 (1) Å) with Uiso(H) = 1.5Ueq(O).

Figures

Fig. 1.

Fig. 1.

The molecular structure of both components comprising the asymmetric unit of (I) showing the atom-labelling scheme and displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

A view of the 2-D supramolecular array in (I) showing the O–H···N and N–H···O hydrogen bonds as orange and blue dashed lines, respectively. Colour code: Cl, cyan; F, pink; O, red; N, blue; C, grey; and H, green.

Fig. 3.

Fig. 3.

A view in projection along the a axis of the unit-cell contents in (I) showing the stacking of layers along the c direction. The O–H···N and N–H···O hydrogen bonds are shown as orange and blue dashed lines, respectively, and the C–H···F contacts are represented by pink dashed lines. One of the 2-D arrays, as shown in Fig. 2, has been highlighted in space-filling mode. Colour code: Cl, cyan; F, pink; O, red; N, blue; C, grey; and H, green.

Crystal data

C16H11ClFN3·H2O F(000) = 656
Mr = 317.74 Dx = 1.457 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 13530 reflections
a = 3.7795 (2) Å θ = 2.9–27.5°
b = 15.4188 (11) Å µ = 0.28 mm1
c = 24.8576 (16) Å T = 120 K
β = 90.286 (4)° Needle, colourless
V = 1448.57 (16) Å3 0.90 × 0.04 × 0.04 mm
Z = 4

Data collection

Enraf–Nonius KappaCCD area-detector diffractometer 3291 independent reflections
Radiation source: Enraf Nonius FR591 rotating anode 2009 reflections with I > 2σ(I)
10 cm confocal mirrors Rint = 0.098
Detector resolution: 9.091 pixels mm-1 θmax = 27.5°, θmin = 3.1°
φ and ω scans h = −4→4
Absorption correction: multi-scan (SADABS; Sheldrick, 2007) k = −20→19
Tmin = 0.614, Tmax = 0.746 l = −32→32
19494 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)] = 0.059 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.131 H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0463P)2 + 0.5902P] where P = (Fo2 + 2Fc2)/3
3291 reflections (Δ/σ)max < 0.001
205 parameters Δρmax = 0.33 e Å3
3 restraints Δρmin = −0.37 e Å3

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
Cl1 0.85154 (18) −0.01273 (5) 0.43677 (3) 0.0319 (2)
F1 0.1997 (4) 0.22958 (11) −0.11624 (6) 0.0367 (5)
N1 0.3942 (5) −0.13713 (14) 0.26095 (9) 0.0214 (5)
N2 0.6585 (5) 0.08516 (14) 0.17189 (8) 0.0221 (5)
H2N 0.7847 0.1268 0.1867 0.027*
N3 0.5476 (5) 0.09163 (15) 0.11914 (8) 0.0212 (5)
C1 0.3270 (7) −0.12969 (18) 0.20855 (11) 0.0225 (6)
H1 0.2176 −0.1776 0.1911 0.027*
C2 0.4043 (6) −0.05737 (18) 0.17733 (10) 0.0210 (6)
H2 0.3436 −0.0566 0.1402 0.025*
C3 0.5701 (6) 0.01357 (17) 0.20052 (10) 0.0178 (6)
C4 0.6457 (6) 0.01003 (16) 0.25750 (10) 0.0176 (6)
C5 0.8024 (6) 0.07868 (18) 0.28696 (11) 0.0210 (6)
H5 0.8680 0.1303 0.2687 0.025*
C6 0.8613 (6) 0.07213 (18) 0.34118 (10) 0.0220 (6)
H6 0.9655 0.1189 0.3605 0.026*
C7 0.7663 (7) −0.00432 (18) 0.36790 (11) 0.0218 (6)
C8 0.6151 (6) −0.07217 (18) 0.34132 (10) 0.0214 (6)
H8 0.5531 −0.1233 0.3604 0.026*
C9 0.5501 (6) −0.06654 (16) 0.28533 (10) 0.0179 (6)
C10 0.6205 (7) 0.16293 (18) 0.09495 (11) 0.0219 (6)
H10 0.7507 0.2064 0.1136 0.026*
C11 0.5085 (7) 0.17884 (18) 0.03962 (11) 0.0216 (6)
C12 0.3483 (7) 0.11448 (18) 0.00825 (11) 0.0231 (6)
H12 0.3087 0.0586 0.0232 0.028*
C13 0.2471 (7) 0.13101 (18) −0.04411 (11) 0.0237 (6)
H13 0.1409 0.0871 −0.0656 0.028*
C14 0.3041 (7) 0.21294 (19) −0.06453 (11) 0.0256 (7)
C15 0.4572 (7) 0.27824 (19) −0.03525 (11) 0.0269 (7)
H15 0.4911 0.3342 −0.0504 0.032*
C16 0.5614 (7) 0.26028 (18) 0.01715 (11) 0.0232 (6)
H16 0.6708 0.3044 0.0380 0.028*
O1W 0.0566 (5) 0.23633 (12) 0.20098 (8) 0.0287 (5)
H1W 0.262 (3) 0.2503 (17) 0.2111 (12) 0.043*
H2W −0.086 (5) 0.2775 (13) 0.2069 (12) 0.043*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl1 0.0381 (4) 0.0386 (5) 0.0191 (4) −0.0007 (3) −0.0065 (3) −0.0001 (3)
F1 0.0475 (10) 0.0422 (11) 0.0205 (9) 0.0086 (8) −0.0082 (8) 0.0037 (8)
N1 0.0218 (12) 0.0225 (13) 0.0200 (13) 0.0000 (10) −0.0006 (9) −0.0006 (10)
N2 0.0269 (12) 0.0218 (13) 0.0177 (12) −0.0046 (10) −0.0046 (9) 0.0001 (10)
N3 0.0219 (12) 0.0265 (14) 0.0153 (12) 0.0018 (10) −0.0022 (9) 0.0005 (10)
C1 0.0185 (14) 0.0204 (16) 0.0286 (17) 0.0005 (11) −0.0024 (12) −0.0026 (13)
C2 0.0204 (14) 0.0270 (16) 0.0156 (14) 0.0007 (12) −0.0052 (11) −0.0005 (12)
C3 0.0150 (13) 0.0189 (15) 0.0195 (14) 0.0014 (11) −0.0008 (10) −0.0011 (12)
C4 0.0151 (13) 0.0168 (14) 0.0209 (14) 0.0033 (11) −0.0002 (10) −0.0018 (12)
C5 0.0204 (14) 0.0189 (15) 0.0237 (15) 0.0012 (11) 0.0001 (11) −0.0018 (12)
C6 0.0242 (15) 0.0210 (16) 0.0208 (15) −0.0003 (12) −0.0035 (11) −0.0059 (12)
C7 0.0204 (14) 0.0276 (17) 0.0175 (14) 0.0030 (12) −0.0016 (11) −0.0034 (12)
C8 0.0198 (14) 0.0223 (16) 0.0220 (15) 0.0050 (12) −0.0007 (11) 0.0046 (12)
C9 0.0154 (13) 0.0149 (14) 0.0233 (15) 0.0003 (11) −0.0026 (10) −0.0030 (12)
C10 0.0222 (15) 0.0215 (16) 0.0221 (16) 0.0019 (12) 0.0000 (11) −0.0046 (13)
C11 0.0185 (14) 0.0253 (16) 0.0209 (15) 0.0030 (12) 0.0004 (11) 0.0010 (12)
C12 0.0261 (15) 0.0194 (15) 0.0238 (16) −0.0004 (12) 0.0010 (12) −0.0001 (12)
C13 0.0240 (15) 0.0241 (16) 0.0229 (16) 0.0009 (12) −0.0018 (12) −0.0045 (13)
C14 0.0273 (15) 0.0350 (18) 0.0145 (14) 0.0051 (13) −0.0025 (11) 0.0012 (13)
C15 0.0265 (15) 0.0256 (17) 0.0287 (17) 0.0025 (13) −0.0004 (12) 0.0043 (13)
C16 0.0244 (15) 0.0240 (16) 0.0213 (15) −0.0016 (12) −0.0012 (11) −0.0037 (13)
O1W 0.0255 (11) 0.0227 (11) 0.0377 (13) −0.0003 (9) −0.0020 (9) −0.0045 (9)

Geometric parameters (Å, °)

Cl1—C7 1.745 (3) C6—H6 0.9500
F1—C14 1.367 (3) C7—C8 1.362 (4)
N1—C1 1.331 (3) C8—C9 1.414 (3)
N1—C9 1.377 (3) C8—H8 0.9500
N2—C3 1.356 (3) C10—C11 1.458 (4)
N2—N3 1.378 (3) C10—H10 0.9500
N2—H2N 0.8800 C11—C16 1.389 (4)
N3—C10 1.284 (3) C11—C12 1.398 (4)
C1—C2 1.390 (4) C12—C13 1.379 (4)
C1—H1 0.9500 C12—H12 0.9500
C2—C3 1.385 (4) C13—C14 1.379 (4)
C2—H2 0.9500 C13—H13 0.9500
C3—C4 1.445 (3) C14—C15 1.369 (4)
C4—C5 1.415 (4) C15—C16 1.387 (4)
C4—C9 1.416 (4) C15—H15 0.9500
C5—C6 1.369 (3) C16—H16 0.9500
C5—H5 0.9500 O1W—H1W 0.841 (10)
C6—C7 1.401 (4) O1W—H2W 0.845 (10)
C1—N1—C9 116.2 (2) C7—C8—H8 120.0
C3—N2—N3 118.9 (2) C9—C8—H8 120.0
C3—N2—H2N 120.5 N1—C9—C8 117.2 (2)
N3—N2—H2N 120.5 N1—C9—C4 123.6 (2)
C10—N3—N2 116.3 (2) C8—C9—C4 119.2 (2)
N1—C1—C2 125.2 (3) N3—C10—C11 121.6 (2)
N1—C1—H1 117.4 N3—C10—H10 119.2
C2—C1—H1 117.4 C11—C10—H10 119.2
C3—C2—C1 119.8 (2) C16—C11—C12 118.7 (2)
C3—C2—H2 120.1 C16—C11—C10 119.3 (2)
C1—C2—H2 120.1 C12—C11—C10 122.0 (3)
N2—C3—C2 122.4 (2) C13—C12—C11 120.8 (3)
N2—C3—C4 119.8 (2) C13—C12—H12 119.6
C2—C3—C4 117.7 (2) C11—C12—H12 119.6
C5—C4—C9 118.5 (2) C12—C13—C14 118.3 (3)
C5—C4—C3 124.0 (2) C12—C13—H13 120.9
C9—C4—C3 117.4 (2) C14—C13—H13 120.9
C6—C5—C4 121.3 (3) F1—C14—C15 118.8 (3)
C6—C5—H5 119.3 F1—C14—C13 118.3 (2)
C4—C5—H5 119.3 C15—C14—C13 123.0 (3)
C5—C6—C7 119.2 (2) C14—C15—C16 118.0 (3)
C5—C6—H6 120.4 C14—C15—H15 121.0
C7—C6—H6 120.4 C16—C15—H15 121.0
C8—C7—C6 121.6 (2) C15—C16—C11 121.2 (3)
C8—C7—Cl1 119.6 (2) C15—C16—H16 119.4
C6—C7—Cl1 118.8 (2) C11—C16—H16 119.4
C7—C8—C9 120.0 (2) H1W—O1W—H2W 110.0 (16)
C3—N2—N3—C10 176.0 (2) C7—C8—C9—N1 −179.5 (2)
C9—N1—C1—C2 0.5 (4) C7—C8—C9—C4 0.3 (4)
N1—C1—C2—C3 1.3 (4) C5—C4—C9—N1 179.6 (2)
N3—N2—C3—C2 6.9 (4) C3—C4—C9—N1 0.7 (4)
N3—N2—C3—C4 −172.4 (2) C5—C4—C9—C8 −0.2 (3)
C1—C2—C3—N2 178.6 (2) C3—C4—C9—C8 −179.1 (2)
C1—C2—C3—C4 −2.0 (4) N2—N3—C10—C11 −178.2 (2)
N2—C3—C4—C5 1.6 (4) N3—C10—C11—C16 173.3 (2)
C2—C3—C4—C5 −177.7 (2) N3—C10—C11—C12 −6.6 (4)
N2—C3—C4—C9 −179.5 (2) C16—C11—C12—C13 0.5 (4)
C2—C3—C4—C9 1.1 (3) C10—C11—C12—C13 −179.5 (2)
C9—C4—C5—C6 −0.1 (4) C11—C12—C13—C14 −0.8 (4)
C3—C4—C5—C6 178.7 (2) C12—C13—C14—F1 −179.2 (2)
C4—C5—C6—C7 0.4 (4) C12—C13—C14—C15 0.2 (4)
C5—C6—C7—C8 −0.3 (4) F1—C14—C15—C16 180.0 (2)
C5—C6—C7—Cl1 178.65 (19) C13—C14—C15—C16 0.5 (4)
C6—C7—C8—C9 0.0 (4) C14—C15—C16—C11 −0.8 (4)
Cl1—C7—C8—C9 −178.98 (18) C12—C11—C16—C15 0.2 (4)
C1—N1—C9—C8 178.3 (2) C10—C11—C16—C15 −179.7 (2)
C1—N1—C9—C4 −1.5 (4)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1w—H1w···N1i 0.843 (16) 2.28 (2) 2.999 (3) 144 (2)
O1w—H2w···N1ii 0.85 (2) 1.93 (2) 2.761 (3) 166 (3)
N2—H2n···O1wiii 0.88 2.01 2.865 (3) 165
C5—H5···O1wiii 0.95 2.45 3.379 (3) 164
C10—H10···O1wiii 0.95 2.50 3.302 (3) 142
C1—H1···F1iv 0.95 2.56 3.399 (3) 147
C6—H6···F1v 0.95 2.56 3.477 (3) 161

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH2970).

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/S1600536809053367/lh2970sup1.cif

e-66-0o152-sup1.cif (19.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809053367/lh2970Isup2.hkl

e-66-0o152-Isup2.hkl (158.2KB, hkl)

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


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