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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Jan 4;64(Pt 2):o370. doi: 10.1107/S1600536807066615

4,4-Bis(4-methyl­phenyl­sulfan­yl)-1,1-diphenyl-2-aza­buta-1,3-diene

Rodolphe Kinghat a, Hamid Boudiba a, Abderrahim Khatyr a, Michael Knorr a, Marek M Kubicki b,*
PMCID: PMC2960289  PMID: 21201402

Abstract

In the title compound, C29H25NS2, both the Cl atoms of the aza­diene precursor 4,4-dichloro-1,1-diphenyl-2-aza­buta-1,3-diene are replaced by two vicinal S-p-tolyl substituents attached to the terminal C atom of a π-conjugated 2-aza­butadiene array. The aza­diene chain is planar to within 0.01 Å. One of the phenyl rings seems to be slightly π-conjugated with the aza­diene core [dihedral angle 5.1 (2)°].

Related literature

Some related structures of alkoxo- (Jacquot et al., 2000), cyano- (Jacquot-Rousseau et al., 2002) and iPrS-substituted (Jacquot-Rousseau et al., 2005) 4,4-dichloro-1,1-diphenyl-2-aza­buta-1,3-dienes (Jacquot et al., 1999) have been reported. For related literature, see: Tanimoto et al. (1976); Truce & Boudakian (1956).graphic file with name e-64-0o370-scheme1.jpg

Experimental

Crystal data

  • C29H25NS2

  • M r = 451.66

  • Triclinic, Inline graphic

  • a = 6.9340 (10) Å

  • b = 12.3009 (2) Å

  • c = 14.4247 (3) Å

  • α = 101.7371 (8)°

  • β = 98.2522 (7)°

  • γ = 93.0400 (10)°

  • V = 1187.90 (4) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.24 mm−1

  • T = 120 (2) K

  • 0.2 × 0.12 × 0.08 mm

Data collection

  • Nonius KappaCCD diffractometer

  • Absorption correction: none

  • 7710 measured reflections

  • 5329 independent reflections

  • 4695 reflections with I > 2σ(I)

  • R int = 0.019

Refinement

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.089

  • S = 1.04

  • 5329 reflections

  • 317 parameters

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

  • Δρmax = 0.27 e Å−3

  • Δρmin = −0.24 e Å−3

Data collection: KappaCCD Server Software (Nonius, 1997); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: DENZO (Otwinowski & Minor, 1997) and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536807066615/gw2031sup1.cif

e-64-0o370-sup1.cif (19.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066615/gw2031Isup2.hkl

e-64-0o370-Isup2.hkl (255.6KB, hkl)

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

Acknowledgments

CNRS is acknowledged for financial support

supplementary crystallographic information

Comment

The investigations of Truce and Boudakian on the reactivity of 1,1-dichloroethylene (1) towards an excess of sodium p-toluenethiolate have shown that this reaction affords exclusively cis-1,2-bis-(p-tolylmercapto) ethane (2). The intermediacy of an alkyne species ArSCCH has been suggested to rationalize this interesting rearrangement reaction which implies some addition–elimination sequences (Truce & Boudakian, 1956). Another research group has later confirmed these findings (Tanimoto et al., 1976) (Fig. 2). In the context of our interest in developing novel π-conjugated dithioether compounds as ligands for coordination chemistry, we have recently reported on the synthesis and crystal structure of [(i-PrS)2C=C(H)—N=CPh2] (4a), obtained by reaction of an excess of sodium i-propylthiolate with 4,4-dichloro-1,1-diphenyl-2-azabuta-1,3-diene (3) in DMF as solvent (Jacquot-Rousseau et al., 2005). In the light of the results mentioned above, we were intrigued whether the reaction of (3) (Jacquot et al., 1999) with sodium p-toluenethiolate would lead to [(p-tolylS)2C=C(H)—N=CPh2] (4 b) or to an rearranged product bearing the two –S-p-tolyl substituents on two different carbon atoms, similar to the case of olefin (2) (Fig. 3).

The molecular structure of (4 b) is shown in Fig. 1. The transoid conformation of the azabutadiene chain found in precursor (3) and in the S-i-propyl derivative (4a) is also observed in the crystal structure of (4 b). In contrast to compound (2), both the S-p-tolyl substituents are attached to the same C(3) atom.

One may expect that one of the two phenyl groups bound to C(1) makes part of the phenyl/azadiene chain π-conjugation. In fact, a dihedral angle between C10–C15 phenyl plane and that of azadiene chain C1—N—C2—C3 is equal only to 5.1 (2)°. Note that these dihedral angles amount to 28.7 (1)° in precursor (3) and 38.8 (3)° in (4a). An obvious question arises: the reported values of dihedral angles are due to the electronic structures of compounds (3) and (4) or to the packing in the crystals? This problem requires some calculations on the electronic structure of (4 b) and will be separately treated elsewhere.

Experimental

4,4-Dichloro-1,1-diphenyl-2-azabuta-1,3-diene (3) (1.1 mmol) was stirred with an excess of 4-toluenethiolate (8 mmol) in dry DMF (10 ml). The reaction mixture was kept at room temperature for 8 h, then poured into water (100 ml) and extracted with diethyl ether (150 ml). The organic solution was washed three times with water, dried over anhydrous sodium sulfate and evaporated. The crude residue was recristallized from ethanol (75% yield). 1H NMR: δ = 2.30 p.p.m. (s, 3H, Ar—CH3); 2.33 p.p.m. (s, 3H, Ar—CH3);), 6.99–7.02 p.p.m. (m, 8H, phenyl) 7.10 p.p.m. (s, 1H, C=CH), 7.23–7.28 p.p.m. (m, 10H, Ar—H).

Refinement

The hydrogen H(2) bound to the carbon C(2) of the azadienic chain as well as those of p-methyl groups (C22 and C29) were located from difference Fourier map and isotropically refined. Other aromatic H atoms were included in calculated positions and treated in a riding model with isotropic displacement parameters set to 1.2 times those of carbon atoms bearing them.

Figures

Fig. 1.

Fig. 1.

View of (4 b) with ellipsoids at the 30% probability level.

Fig. 2.

Fig. 2.

p-S-tolyl substitution on 1,1-dichloroethylene.

Fig. 3.

Fig. 3.

p-S-tolyl substitution on an azadienic chain.

Crystal data

C29H25NS2 Z = 2
Mr = 451.66 F000 = 476
Triclinic, P1 Dx = 1.263 Mg m3
Hall symbol: -P 1 Melting point: 382 K
a = 6.9340 (10) Å Mo Kα radiation λ = 0.71073 Å
b = 12.3009 (2) Å Cell parameters from 3954 reflections
c = 14.4247 (3) Å θ = 1.0–27.5º
α = 101.7371 (8)º µ = 0.24 mm1
β = 98.2522 (7)º T = 120 (2) K
γ = 93.0400 (10)º Irregular, yellow
V = 1187.90 (4) Å3 0.2 × 0.12 × 0.08 mm

Data collection

Nonius KappaCCD diffractometer 4695 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.019
Monochromator: graphite θmax = 27.4º
T = 120(2) K θmin = 1.5º
CCD scans h = −8→8
Absorption correction: none k = −12→15
7710 measured reflections l = −18→18
5329 independent reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.034 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.089   w = 1/[σ2(Fo2) + (0.0329P)2 + 0.5208P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.001
5329 reflections Δρmax = 0.27 e Å3
317 parameters Δρmin = −0.24 e Å3
Primary atom site location: structure-invariant direct methods Extinction correction: none

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 0.22781 (5) 0.37867 (3) 0.35024 (2) 0.02290 (9)
S2 0.43297 (4) 0.52776 (3) 0.23783 (2) 0.02161 (9)
N 0.48657 (16) 0.21771 (9) 0.26950 (8) 0.0221 (2)
C1 0.58163 (18) 0.13424 (11) 0.23639 (9) 0.0204 (3)
C2 0.50043 (19) 0.31661 (11) 0.23787 (10) 0.0227 (3)
C3 0.39300 (18) 0.40002 (11) 0.27163 (9) 0.0200 (3)
C4 0.71038 (19) 0.13495 (10) 0.16171 (9) 0.0206 (3)
C5 0.6304 (2) 0.12895 (14) 0.06658 (11) 0.0328 (3)
H5 0.4953 0.1238 0.0489 0.039*
C6 0.7506 (3) 0.13066 (16) −0.00219 (12) 0.0415 (4)
H6 0.6960 0.1270 −0.0656 0.050*
C7 0.9508 (2) 0.13778 (14) 0.02340 (12) 0.0364 (4)
H7 1.0312 0.1378 −0.0230 0.044*
C8 1.0317 (2) 0.14488 (13) 0.11728 (12) 0.0350 (3)
H8 1.1670 0.1506 0.1345 0.042*
C9 0.9128 (2) 0.14354 (12) 0.18644 (11) 0.0287 (3)
H9 0.9686 0.1484 0.2499 0.034*
C10 0.56071 (18) 0.03303 (11) 0.27658 (9) 0.0207 (3)
C11 0.6700 (2) −0.05758 (11) 0.25308 (10) 0.0250 (3)
H11 0.7553 −0.0568 0.2089 0.030*
C12 0.6528 (2) −0.14933 (12) 0.29507 (11) 0.0293 (3)
H12 0.7284 −0.2087 0.2799 0.035*
C13 0.5238 (2) −0.15238 (12) 0.35923 (11) 0.0285 (3)
H13 0.5126 −0.2136 0.3874 0.034*
C14 0.4112 (2) −0.06400 (13) 0.38151 (12) 0.0322 (3)
H14 0.3228 −0.0664 0.4240 0.039*
C15 0.4296 (2) 0.02781 (12) 0.34092 (11) 0.0290 (3)
H15 0.3537 0.0869 0.3566 0.035*
C16 0.19592 (18) 0.55484 (11) 0.18701 (9) 0.0200 (3)
C17 0.05190 (19) 0.47143 (11) 0.13858 (10) 0.0231 (3)
H17 0.0744 0.3969 0.1344 0.028*
C18 −0.1256 (2) 0.50030 (12) 0.09652 (10) 0.0258 (3)
H18 −0.2222 0.4443 0.0652 0.031*
C19 −0.1623 (2) 0.61123 (12) 0.10010 (10) 0.0249 (3)
C20 −0.0167 (2) 0.69289 (12) 0.14901 (10) 0.0269 (3)
H20 −0.0387 0.7675 0.1528 0.032*
C21 0.1609 (2) 0.66593 (11) 0.19237 (10) 0.0255 (3)
H21 0.2563 0.7221 0.2249 0.031*
C22 −0.3522 (2) 0.64249 (15) 0.05100 (12) 0.0328 (3)
C23 0.16434 (19) 0.51460 (10) 0.39797 (9) 0.0195 (3)
C24 −0.02989 (19) 0.53814 (11) 0.38031 (9) 0.0217 (3)
H24 −0.1223 0.4848 0.3408 0.026*
C25 −0.08547 (19) 0.64104 (11) 0.42158 (10) 0.0233 (3)
H25 −0.2158 0.6559 0.4098 0.028*
C26 0.0502 (2) 0.72288 (11) 0.48054 (9) 0.0222 (3)
C27 0.2438 (2) 0.69758 (11) 0.49862 (9) 0.0231 (3)
H27 0.3362 0.7509 0.5383 0.028*
C28 0.30109 (19) 0.59443 (11) 0.45858 (9) 0.0218 (3)
H28 0.4305 0.5786 0.4721 0.026*
C29 −0.0105 (3) 0.83537 (13) 0.52391 (12) 0.0316 (3)
H2 0.587 (2) 0.3271 (13) 0.1916 (11) 0.023 (4)*
H221 −0.460 (3) 0.6112 (18) 0.0711 (16) 0.060 (6)*
H222 −0.370 (3) 0.6152 (19) −0.0180 (18) 0.065 (7)*
H223 −0.357 (3) 0.722 (2) 0.0618 (17) 0.075 (7)*
H291 −0.049 (3) 0.8755 (17) 0.4753 (15) 0.050 (5)*
H292 0.094 (3) 0.8815 (18) 0.5682 (15) 0.055 (6)*
H293 −0.120 (3) 0.8270 (19) 0.5548 (16) 0.066 (7)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.02781 (18) 0.01708 (16) 0.02706 (18) 0.00498 (12) 0.01078 (13) 0.00695 (13)
S2 0.01964 (16) 0.02080 (17) 0.02704 (18) 0.00391 (12) 0.00537 (12) 0.00951 (13)
N 0.0233 (5) 0.0201 (5) 0.0235 (6) 0.0061 (4) 0.0038 (4) 0.0045 (4)
C1 0.0199 (6) 0.0198 (6) 0.0200 (6) 0.0040 (5) 0.0010 (5) 0.0021 (5)
C2 0.0229 (6) 0.0226 (6) 0.0235 (7) 0.0053 (5) 0.0042 (5) 0.0059 (5)
C3 0.0207 (6) 0.0193 (6) 0.0206 (6) 0.0035 (5) 0.0028 (5) 0.0056 (5)
C4 0.0235 (6) 0.0162 (6) 0.0228 (6) 0.0048 (5) 0.0053 (5) 0.0037 (5)
C5 0.0273 (7) 0.0471 (9) 0.0257 (7) 0.0121 (6) 0.0035 (6) 0.0095 (7)
C6 0.0454 (9) 0.0584 (11) 0.0255 (8) 0.0162 (8) 0.0095 (7) 0.0144 (7)
C7 0.0398 (9) 0.0389 (9) 0.0375 (9) 0.0084 (7) 0.0209 (7) 0.0126 (7)
C8 0.0250 (7) 0.0377 (8) 0.0433 (9) −0.0011 (6) 0.0105 (6) 0.0080 (7)
C9 0.0258 (7) 0.0311 (7) 0.0268 (7) −0.0012 (6) 0.0014 (6) 0.0035 (6)
C10 0.0217 (6) 0.0198 (6) 0.0197 (6) 0.0033 (5) 0.0022 (5) 0.0023 (5)
C11 0.0285 (7) 0.0229 (7) 0.0259 (7) 0.0064 (5) 0.0090 (5) 0.0056 (5)
C12 0.0346 (8) 0.0218 (7) 0.0345 (8) 0.0089 (6) 0.0100 (6) 0.0077 (6)
C13 0.0342 (7) 0.0225 (7) 0.0306 (8) 0.0016 (6) 0.0057 (6) 0.0095 (6)
C14 0.0349 (8) 0.0300 (8) 0.0360 (8) 0.0042 (6) 0.0166 (6) 0.0093 (6)
C15 0.0305 (7) 0.0251 (7) 0.0351 (8) 0.0092 (6) 0.0137 (6) 0.0070 (6)
C16 0.0212 (6) 0.0232 (6) 0.0190 (6) 0.0062 (5) 0.0068 (5) 0.0087 (5)
C17 0.0270 (7) 0.0213 (6) 0.0227 (7) 0.0051 (5) 0.0055 (5) 0.0064 (5)
C18 0.0252 (7) 0.0292 (7) 0.0233 (7) 0.0024 (5) 0.0025 (5) 0.0072 (6)
C19 0.0240 (7) 0.0330 (7) 0.0224 (7) 0.0093 (5) 0.0078 (5) 0.0123 (6)
C20 0.0304 (7) 0.0232 (7) 0.0320 (8) 0.0095 (5) 0.0087 (6) 0.0131 (6)
C21 0.0260 (7) 0.0218 (7) 0.0300 (7) 0.0026 (5) 0.0052 (6) 0.0079 (5)
C22 0.0273 (8) 0.0437 (9) 0.0318 (8) 0.0108 (7) 0.0044 (6) 0.0166 (7)
C23 0.0243 (6) 0.0185 (6) 0.0183 (6) 0.0044 (5) 0.0066 (5) 0.0070 (5)
C24 0.0220 (6) 0.0224 (6) 0.0209 (6) 0.0011 (5) 0.0037 (5) 0.0049 (5)
C25 0.0212 (6) 0.0270 (7) 0.0244 (7) 0.0069 (5) 0.0068 (5) 0.0084 (5)
C26 0.0287 (7) 0.0217 (6) 0.0188 (6) 0.0058 (5) 0.0088 (5) 0.0057 (5)
C27 0.0269 (7) 0.0222 (6) 0.0196 (6) 0.0000 (5) 0.0025 (5) 0.0047 (5)
C28 0.0205 (6) 0.0243 (6) 0.0226 (6) 0.0040 (5) 0.0031 (5) 0.0092 (5)
C29 0.0381 (8) 0.0249 (7) 0.0323 (8) 0.0083 (6) 0.0112 (7) 0.0021 (6)

Geometric parameters (Å, °)

S1—C3 1.7689 (13) C14—H14 0.9300
S1—C23 1.7776 (13) C15—H15 0.9300
S2—C3 1.7572 (13) C16—C21 1.3892 (19)
S2—C16 1.7781 (13) C16—C17 1.3919 (19)
N—C1 1.2959 (17) C17—C18 1.3890 (19)
N—C2 1.3869 (17) C17—H17 0.9300
C1—C10 1.4851 (18) C18—C19 1.393 (2)
C1—C4 1.4955 (18) C18—H18 0.9300
C2—C3 1.3515 (18) C19—C20 1.388 (2)
C2—H2 0.983 (15) C19—C22 1.5098 (19)
C4—C9 1.3904 (19) C20—C21 1.3873 (19)
C4—C5 1.3902 (19) C20—H20 0.9300
C5—C6 1.387 (2) C21—H21 0.9300
C5—H5 0.9300 C22—H221 0.93 (2)
C6—C7 1.378 (2) C22—H222 0.97 (2)
C6—H6 0.9300 C22—H223 0.96 (3)
C7—C8 1.373 (2) C23—C24 1.3912 (18)
C7—H7 0.9300 C23—C28 1.3936 (18)
C8—C9 1.385 (2) C24—C25 1.3843 (19)
C8—H8 0.9300 C24—H24 0.9300
C9—H9 0.9300 C25—C26 1.3941 (19)
C10—C11 1.3934 (18) C25—H25 0.9300
C10—C15 1.3974 (19) C26—C27 1.3942 (19)
C11—C12 1.3927 (19) C26—C29 1.5062 (19)
C11—H11 0.9300 C27—C28 1.3864 (19)
C12—C13 1.381 (2) C27—H27 0.9300
C12—H12 0.9300 C28—H28 0.9300
C13—C14 1.384 (2) C29—H291 0.95 (2)
C13—H13 0.9300 C29—H292 0.97 (2)
C14—C15 1.382 (2) C29—H293 0.95 (2)
C3—S1—C23 104.31 (6) C21—C16—C17 119.68 (12)
C3—S2—C16 103.68 (6) C21—C16—S2 116.76 (10)
C1—N—C2 121.26 (12) C17—C16—S2 123.46 (10)
N—C1—C10 117.10 (12) C18—C17—C16 119.57 (12)
N—C1—C4 123.91 (12) C18—C17—H17 120.2
C10—C1—C4 118.98 (11) C16—C17—H17 120.2
C3—C2—N 119.27 (12) C17—C18—C19 121.53 (13)
C3—C2—H2 119.6 (9) C17—C18—H18 119.2
N—C2—H2 121.2 (9) C19—C18—H18 119.2
C2—C3—S2 117.32 (10) C20—C19—C18 117.82 (12)
C2—C3—S1 119.54 (10) C20—C19—C22 120.64 (13)
S2—C3—S1 123.10 (8) C18—C19—C22 121.53 (14)
C9—C4—C5 118.69 (13) C21—C20—C19 121.59 (13)
C9—C4—C1 120.58 (12) C21—C20—H20 119.2
C5—C4—C1 120.73 (12) C19—C20—H20 119.2
C6—C5—C4 120.46 (14) C20—C21—C16 119.80 (13)
C6—C5—H5 119.8 C20—C21—H21 120.1
C4—C5—H5 119.8 C16—C21—H21 120.1
C7—C6—C5 120.06 (15) C19—C22—H221 111.6 (13)
C7—C6—H6 120.0 C19—C22—H222 111.9 (13)
C5—C6—H6 120.0 H221—C22—H222 105.5 (18)
C8—C7—C6 120.05 (14) C19—C22—H223 111.4 (14)
C8—C7—H7 120.0 H221—C22—H223 109.5 (19)
C6—C7—H7 120.0 H222—C22—H223 106.6 (19)
C7—C8—C9 120.25 (14) C24—C23—C28 119.57 (12)
C7—C8—H8 119.9 C24—C23—S1 118.78 (10)
C9—C8—H8 119.9 C28—C23—S1 121.44 (10)
C8—C9—C4 120.48 (14) C25—C24—C23 119.96 (12)
C8—C9—H9 119.8 C25—C24—H24 120.0
C4—C9—H9 119.8 C23—C24—H24 120.0
C11—C10—C15 118.28 (12) C24—C25—C26 121.25 (12)
C11—C10—C1 122.05 (12) C24—C25—H25 119.4
C15—C10—C1 119.66 (12) C26—C25—H25 119.4
C12—C11—C10 120.62 (13) C27—C26—C25 118.15 (12)
C12—C11—H11 119.7 C27—C26—C29 120.85 (13)
C10—C11—H11 119.7 C25—C26—C29 121.01 (13)
C13—C12—C11 120.18 (13) C28—C27—C26 121.20 (12)
C13—C12—H12 119.9 C28—C27—H27 119.4
C11—C12—H12 119.9 C26—C27—H27 119.4
C12—C13—C14 119.75 (13) C27—C28—C23 119.84 (12)
C12—C13—H13 120.1 C27—C28—H28 120.1
C14—C13—H13 120.1 C23—C28—H28 120.1
C15—C14—C13 120.26 (14) C26—C29—H291 110.6 (12)
C15—C14—H14 119.9 C26—C29—H292 112.6 (13)
C13—C14—H14 119.9 H291—C29—H292 106.3 (17)
C14—C15—C10 120.89 (13) C26—C29—H293 110.2 (14)
C14—C15—H15 119.6 H291—C29—H293 106.8 (18)
C10—C15—H15 119.6 H292—C29—H293 110.1 (18)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: GW2031).

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/S1600536807066615/gw2031sup1.cif

e-64-0o370-sup1.cif (19.7KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536807066615/gw2031Isup2.hkl

e-64-0o370-Isup2.hkl (255.6KB, hkl)

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


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