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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 4;67(Pt 1):m25. doi: 10.1107/S1600536810043655

{2-[(Dimethyl­amino)­meth­yl]phen­yl}bis­(4-methyl­phen­yl)bis­muthane

Masatoshi Kawahata a, Shuji Yasuike b,, Izumi Kinebuchi b, Kentaro Yamaguchi a, Jyoji Kurita b,*
PMCID: PMC3050329  PMID: 21522549

Abstract

The title compound, [Bi(C7H7)2(C9H12N)], was obtained by treating chlorodi(p-tol­yl)bis­muthane with o-lithio-N,N-dimethyl­benzyl­amine. An intra­molecular Bi⋯N nonbonding inter­action is observed in the distorted trigonal triaryl­bis­muth coordination of the title compound.

Related literature

For a review of the applications and structural chemistry of organobismuth compounds, see: Matano & Ikegami (2001); Silvestru et al. (1999). For related structural reports, see: Suzuki et al. (1993); Tokunaga et al. (2000a ,b ); Okajima et al. (2002).graphic file with name e-67-00m25-scheme1.jpg

Experimental

Crystal data

  • [Bi(C7H7)2(C9H12N)]

  • M r = 525.43

  • Monoclinic, Inline graphic

  • a = 6.0991 (12) Å

  • b = 19.630 (4) Å

  • c = 8.3699 (16) Å

  • β = 93.073 (2)°

  • V = 1000.6 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 8.81 mm−1

  • T = 100 K

  • 0.20 × 0.08 × 0.01 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.272, T max = 0.917

  • 4908 measured reflections

  • 3626 independent reflections

  • 3410 reflections with I > 2σ(I)

  • R int = 0.016

Refinement

  • R[F 2 > 2σ(F 2)] = 0.019

  • wR(F 2) = 0.037

  • S = 1.00

  • 3626 reflections

  • 231 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.86 e Å−3

  • Δρmin = −0.59 e Å−3

  • Absolute structure: Flack (1983), with 1544 Friedel pairs

  • Flack parameter: 0.412 (7)

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: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810043655/si2298sup1.cif

e-67-00m25-sup1.cif (18.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810043655/si2298Isup2.hkl

e-67-00m25-Isup2.hkl (174.2KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

C1—Bi1 2.291 (5)
C8—Bi1 2.265 (5)
C15—Bi1 2.267 (5)
N1—Bi1 2.902 (4)
C1—Bi1—C8 96.07 (16)
C1—Bi1—C15 90.74 (16)
C1—Bi1—N1 157.55 (14)
C8—Bi1—C15 94.85 (17)
C8—Bi1—N1 81.26 (14)
C15—Bi1—N1 67.43 (13)

Acknowledgments

This work was supported by a Grant-in Aid for Scientific Research (C) (to JK), and by the ‘Academic Frontier’ Project for Private Universities from the Ministry of Education, Culture, Sports, Science and Technology of Japan (to SY). Financial support was also provided by the Specific Research Fund of Hokuriku University. All are gratefully acknowledged.

supplementary crystallographic information

Comment

Interest in the chemistry of organobisumuth(III) compounds has increased in recent years, due to the potential reagents and catalysts in organic synthesis as well as biological activity (Matano & Ikegami, 2001). Among these, the structural chemistry of bismuth compounds, including intramolecular interaction between bismuth and heteroatoms, has been widely reported in a review (Silvestru et al. 1999). On the other hand, we have recently reported the synthesis and structure of various organoantimony(III) compounds, such as 1-[8-(N,N-dimethylaminomethyl)naphthyl]bis(4-methylphenyl)stibane (Tokunaga et al., 2000a), [2-(N,N-dimethylaminomethyl)phenyl]bis(4-methylphenyl)stibane (Tokunaga et al., 2000b), and Sb(S)-[2-(S)-(N,N-dimethylaminomethyl)phenyl](1-naphthyl)(4-methylphenyl)stibane (Okajima et al., 2002), bearing the CH2NMe2 moiety adjacent to the Sb atom as a pendant arm. X-ray crystal analyses of these compounds revealed the presence of intramolecular coordination between the Sb and N atoms. Here we report the synthesis and structure of the title compound, in which the central Sb atom of the [2-(N,N-dimethylaminomethyl)phenyl]bis(4-methylphenyl)stibane is replaced with Bi atom. The molecular structure and atom-numbering of the title compound are shown in Fig. 1. Selected geometric parameters are presented in Table 1. The analysis revealed that the Bi and three C (C1, C8, and C15) atoms exhibit a distorted trigonal-pyramidal arrangement with the Bi atom being far from the basal three-carbon plane (1.220 (3) Å). In addition, an intramolecular coordination between the Bi and N atoms is observed; the distance between the Bi and N atoms is 2.902 (4) Å, which corresponds to 74% of the sum of the van der Waals radii of both elements (3.94 Å) and accords with 131% of the covalent bond length (2.22 Å). It should be noted that the bond angle for C1—Bi1—N1 [157.55 (14)°] is significantly larger than those for C8—Bi1—N1 [81.26 (14)°] and C15—Bi1—N1 [67.43 (13)°], and the bond distance between Bi1 and C1 [2.291 (5) Å] is obviously longer than those for Bi1–C8 [2.265 (5) Å] and C15 [2.267 (5) Å]. The results imply that the central Bi atom is distorted equatorial vacant trigonal bipyramidal configuration with the N1 of the pendant arm and the C1 of the tolyl group being apical positions, similar to the geometry of chloro[2-(N,N-dimethylaminomethyl)phenyl](4-methylphenyl)bismuthane (Suzuki et al., 1993). These results showed that the title compound is a hypervalent compound with 10-Bi-4 system, by analogy with the 10-Sb-4 system of the organoantimony compounds (Tokunaga et al., 2000a,b; Okajima et al., 2002).

Experimental

The title compound was synthesized as follows: To a solution of N,N-dimethylbenzylamine (1.89 g, 14.0 mmol) in ether (25 ml) was added n-butyllithium (1.65 M in hexane, 10.2 ml, 16.8 mmol) at 273 K under an argon atmosphere, and the mixture was stirred for 24 h at room temperature. To this solution was added a suspension of chlorobis(4-methylphenyl)bismuthane [prepared by the redistribution reaction on the treatment of tris(4-methylphenyl)bismuthane (2.31 g, 4.8 mmol) and trichlorobismuthane (756 mg, 2.4 mmol) in ether (20 ml) at room temperature for 2 h] over 10 min at 273 K, and the mixture was stirred for 24 h at the same temperature. The mixture was quenched with water (100 ml) and diluted with CH2Cl2 (100 ml), and insoluble substances were removed by filtration. The organic layer was separated and the aqueous layer was extracted with CH2Cl2 (50 ml). The combined organic layer was washed with brine, dried and evaporated in vacuo. Purification of the residue by recrystallization from CH3CN gave 2-(N,N-dimethylaminomethyl)phenylbis(4-methylphenyl)bismuthane as colourless prisms (2.0 g, 53% yield; m.p. 372–374 K; 1H NMR (CDCl3): δ 1.98 (s, 6H), 2.30 (s, 6H), 3.40 (s, 2H), 7.14 (d, J = 7.3 Hz, 4H), 7.16 (m, 1H), 7.25 (m, 2H), 7.62 (d, J = 7.3 Hz, 4H), 7.80 (d, J = 6.9 Hz, 1H); 13C NMR (CDCl3): δ 21.5 (q), 44.5 (q), 67.1 (t), 127.2 (d), 129.3 (d), 129.6 (d), 130.8 (d), 136.5 (s), 137.7 (d), 139.6 (d), 145.1 (s), 155.9 (s), 158.5 (s); analysis calculated for C23H26BiN: C 52.58, H 4.99, N 2.67%; found: C 52.57, H 4.92, N 2.63%.

Refinement

The H atoms were positioned geometrically (C—H = 0.93–0.96 Å) and were included in the refinement in the riding model approximation, with Uiso(H) = xUeq(C, N), where x = 1.5 for methyl and x = 1.2 for all other H atoms. The crystal studied was a twin with the refined BASF ratio of 0.412 (7)/0.588 (7). The Flack parameter = 0.412 (7) was refined in the full matrix least-squares process using the TWIN/BASF option.

Figures

Fig. 1.

Fig. 1.

View of the title compound with the atom numbering scheme. The thermal ellipsoids are drawn at the 50% probability level. H atoms are shown as small spheres of arbitrary radii.

Crystal data

[Bi(C7H7)2(C9H12N)] F(000) = 508
Mr = 525.43 Dx = 1.744 Mg m3
Monoclinic, P21 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P2yb Cell parameters from 3137 reflections
a = 6.0991 (12) Å θ = 2.4–26.9°
b = 19.630 (4) Å µ = 8.81 mm1
c = 8.3699 (16) Å T = 100 K
β = 93.073 (2)° Prismatic, colourless
V = 1000.6 (3) Å3 0.20 × 0.08 × 0.01 mm
Z = 2

Data collection

Bruker APEXII CCD area-detector diffractometer 3626 independent reflections
Radiation source: fine-focus sealed tube 3410 reflections with I > 2σ(I)
graphite Rint = 0.016
φ and ω scans θmax = 27.0°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −7→7
Tmin = 0.272, Tmax = 0.917 k = −22→24
4908 measured reflections l = −10→5

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.019 H-atom parameters constrained
wR(F2) = 0.037 w = 1/[σ2(Fo2) + (0.0116P)2] where P = (Fo2 + 2Fc2)/3
S = 1.00 (Δ/σ)max = 0.001
3626 reflections Δρmax = 0.86 e Å3
231 parameters Δρmin = −0.59 e Å3
1 restraint Absolute structure: Flack (1983), with 1544 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.412 (7)

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
C1 0.6751 (8) 0.6439 (2) 0.4839 (6) 0.0163 (10)
C2 0.8412 (8) 0.6254 (3) 0.5966 (6) 0.0230 (12)
C3 0.8193 (8) 0.5693 (3) 0.6955 (6) 0.0232 (12)
C4 0.6268 (8) 0.5298 (2) 0.6864 (6) 0.0204 (11)
C5 0.4595 (8) 0.5495 (2) 0.5785 (6) 0.0216 (11)
C6 0.4845 (8) 0.6055 (2) 0.4787 (6) 0.0199 (11)
C7 0.6102 (9) 0.4657 (2) 0.7843 (6) 0.0261 (12)
C8 0.9474 (8) 0.7916 (2) 0.4269 (6) 0.0169 (11)
C9 0.8880 (8) 0.8577 (2) 0.4634 (6) 0.0181 (11)
C10 1.0307 (8) 0.9002 (2) 0.5535 (6) 0.0185 (11)
C11 1.2387 (8) 0.8775 (2) 0.6077 (6) 0.0158 (10)
C12 1.2973 (8) 0.8115 (2) 0.5681 (6) 0.0190 (11)
C13 1.1561 (8) 0.7696 (2) 0.4794 (6) 0.0176 (11)
C14 1.3902 (8) 0.9223 (2) 0.7087 (6) 0.0240 (12)
C15 0.9686 (7) 0.6605 (2) 0.1743 (5) 0.0134 (10)
C16 0.9732 (8) 0.5895 (2) 0.2016 (6) 0.0197 (11)
C17 1.1305 (9) 0.5485 (3) 0.1324 (6) 0.0248 (12)
C18 1.2779 (9) 0.5775 (3) 0.0349 (7) 0.0286 (13)
C19 1.2694 (8) 0.6474 (3) 0.0021 (6) 0.0220 (11)
C20 1.1185 (18) 0.6885 (5) 0.0734 (12) 0.019 (2)
C21 1.1160 (17) 0.7642 (5) 0.0378 (11) 0.0148 (19)
C22 0.9016 (9) 0.8666 (2) 0.0186 (6) 0.0234 (12)
C23 0.7809 (8) 0.7669 (2) −0.1263 (6) 0.0248 (12)
N1 0.8969 (6) 0.79253 (18) 0.0204 (5) 0.0154 (9)
Bi1 0.70642 (2) 0.72364 (2) 0.286635 (16) 0.01465 (4)
H2 0.9692 0.6512 0.6057 0.028*
H3 0.9333 0.5577 0.7687 0.028*
H5 0.3285 0.5251 0.5724 0.026*
H6 0.3698 0.6174 0.4065 0.024*
H7A 0.6739 0.4284 0.7290 0.039*
H7B 0.4586 0.4560 0.8001 0.039*
H7C 0.6874 0.4719 0.8863 0.039*
H9 0.7511 0.8741 0.4273 0.022*
H10 0.9866 0.9442 0.5778 0.022*
H12 1.4351 0.7952 0.6022 0.023*
H13 1.2011 0.7258 0.4542 0.021*
H14A 1.3614 0.9164 0.8195 0.036*
H14B 1.3662 0.9691 0.6790 0.036*
H14C 1.5398 0.9102 0.6922 0.036*
H16 0.8711 0.5698 0.2661 0.024*
H17 1.1347 0.5019 0.1524 0.030*
H18 1.3842 0.5506 −0.0097 0.034*
H19 1.3657 0.6663 −0.0680 0.026*
H21A 1.1975 0.7878 0.1237 0.018*
H21B 1.1904 0.7721 −0.0600 0.018*
H22A 0.9813 0.8819 −0.0705 0.035*
H22B 0.9724 0.8829 0.1163 0.035*
H22C 0.7541 0.8837 0.0086 0.035*
H23A 0.8557 0.7820 −0.2180 0.037*
H23B 0.6332 0.7840 −0.1326 0.037*
H23C 0.7782 0.7180 −0.1241 0.037*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.019 (3) 0.015 (2) 0.015 (3) 0.001 (2) 0.003 (2) 0.000 (2)
C2 0.019 (3) 0.030 (3) 0.019 (3) −0.007 (2) 0.002 (2) −0.002 (2)
C3 0.024 (3) 0.028 (3) 0.018 (3) 0.005 (2) −0.002 (2) 0.004 (2)
C4 0.021 (3) 0.022 (3) 0.018 (3) 0.004 (2) 0.007 (2) 0.001 (2)
C5 0.018 (3) 0.021 (3) 0.027 (3) −0.006 (2) 0.007 (2) 0.001 (2)
C6 0.017 (3) 0.019 (3) 0.024 (3) 0.004 (2) −0.001 (2) 0.002 (2)
C7 0.034 (3) 0.018 (3) 0.026 (3) 0.002 (2) 0.009 (3) 0.002 (2)
C8 0.020 (3) 0.014 (2) 0.017 (3) −0.0034 (19) 0.004 (2) −0.0005 (19)
C9 0.020 (3) 0.015 (2) 0.019 (3) 0.002 (2) −0.001 (2) 0.001 (2)
C10 0.027 (3) 0.014 (2) 0.016 (3) 0.001 (2) 0.007 (2) 0.000 (2)
C11 0.020 (3) 0.016 (2) 0.011 (3) −0.005 (2) 0.002 (2) 0.0015 (19)
C12 0.017 (3) 0.021 (3) 0.019 (3) 0.003 (2) −0.001 (2) 0.002 (2)
C13 0.022 (3) 0.015 (2) 0.016 (3) 0.000 (2) 0.004 (2) −0.0033 (19)
C14 0.025 (3) 0.023 (3) 0.024 (3) −0.005 (2) 0.004 (2) −0.006 (2)
C15 0.013 (2) 0.015 (2) 0.013 (3) 0.0007 (19) 0.001 (2) −0.0001 (19)
C16 0.026 (3) 0.017 (3) 0.015 (3) −0.004 (2) −0.004 (2) −0.002 (2)
C17 0.031 (3) 0.017 (3) 0.026 (3) 0.003 (2) −0.005 (3) −0.003 (2)
C18 0.025 (3) 0.031 (3) 0.030 (3) 0.006 (2) 0.001 (3) −0.011 (2)
C19 0.021 (3) 0.026 (3) 0.019 (3) −0.006 (2) 0.002 (2) −0.002 (2)
C20 0.017 (4) 0.020 (4) 0.020 (5) 0.000 (3) −0.012 (3) −0.004 (3)
C21 0.013 (4) 0.017 (4) 0.015 (4) 0.000 (3) 0.007 (3) −0.001 (3)
C22 0.032 (3) 0.019 (3) 0.019 (3) −0.001 (2) 0.004 (2) 0.006 (2)
C23 0.027 (3) 0.025 (3) 0.022 (3) 0.004 (2) 0.001 (2) 0.006 (2)
N1 0.013 (2) 0.016 (2) 0.017 (2) −0.0011 (16) 0.0037 (17) 0.0023 (16)
Bi1 0.01336 (7) 0.01541 (7) 0.01517 (7) 0.0000 (2) 0.00051 (5) −0.0003 (2)

Geometric parameters (Å, °)

C1—C6 1.384 (6) C14—H14A 0.9600
C1—C2 1.394 (6) C14—H14B 0.9600
C1—Bi1 2.291 (5) C14—H14C 0.9600
C2—C3 1.389 (7) C15—C20 1.391 (12)
C2—H2 0.9300 C15—C16 1.412 (6)
C3—C4 1.405 (7) C15—Bi1 2.267 (5)
C3—H3 0.9300 C16—C17 1.401 (7)
C4—C5 1.381 (7) C16—H16 0.9300
C4—C7 1.509 (7) C17—C18 1.370 (7)
C5—C6 1.394 (7) C17—H17 0.9300
C5—H5 0.9300 C18—C19 1.400 (7)
C6—H6 0.9300 C18—H18 0.9300
C7—H7A 0.9600 C19—C20 1.383 (11)
C7—H7B 0.9600 C19—H19 0.9300
C7—H7C 0.9600 C20—C21 1.515 (7)
C8—C9 1.386 (6) C21—N1 1.448 (10)
C8—C13 1.393 (6) C21—H21A 0.9700
C8—Bi1 2.265 (5) C21—H21B 0.9700
C9—C10 1.397 (6) C22—N1 1.454 (6)
C9—H9 0.9300 C22—H22A 0.9600
C10—C11 1.397 (6) C22—H22B 0.9600
C10—H10 0.9300 C22—H22C 0.9600
C11—C12 1.388 (6) C23—N1 1.473 (6)
C11—C14 1.503 (6) C23—H23A 0.9600
C12—C13 1.379 (6) C23—H23B 0.9600
C12—H12 0.9300 C23—H23C 0.9600
C13—H13 0.9300 N1—Bi1 2.902 (4)
C6—C1—C2 117.3 (4) C20—C15—C16 118.7 (6)
C6—C1—Bi1 116.8 (3) C20—C15—Bi1 122.5 (5)
C2—C1—Bi1 125.4 (4) C16—C15—Bi1 118.8 (4)
C3—C2—C1 121.3 (5) C17—C16—C15 120.5 (5)
C3—C2—H2 119.4 C17—C16—H16 119.7
C1—C2—H2 119.4 C15—C16—H16 119.7
C2—C3—C4 120.8 (5) C18—C17—C16 119.6 (5)
C2—C3—H3 119.6 C18—C17—H17 120.2
C4—C3—H3 119.6 C16—C17—H17 120.2
C5—C4—C3 117.9 (5) C17—C18—C19 120.3 (5)
C5—C4—C7 121.3 (5) C17—C18—H18 119.8
C3—C4—C7 120.7 (4) C19—C18—H18 119.8
C4—C5—C6 120.7 (5) C20—C19—C18 120.4 (6)
C4—C5—H5 119.6 C20—C19—H19 119.8
C6—C5—H5 119.6 C18—C19—H19 119.8
C1—C6—C5 122.0 (4) C19—C20—C15 120.4 (8)
C1—C6—H6 119.0 C19—C20—C21 119.1 (11)
C5—C6—H6 119.0 C15—C20—C21 120.5 (10)
C4—C7—H7A 109.5 N1—C21—C20 113.4 (10)
C4—C7—H7B 109.5 N1—C21—H21A 108.9
H7A—C7—H7B 109.5 C20—C21—H21A 108.9
C4—C7—H7C 109.5 N1—C21—H21B 108.9
H7A—C7—H7C 109.5 C20—C21—H21B 108.9
H7B—C7—H7C 109.5 H21A—C21—H21B 107.7
C9—C8—C13 117.8 (4) N1—C22—H22A 109.5
C9—C8—Bi1 119.7 (3) N1—C22—H22B 109.5
C13—C8—Bi1 122.5 (3) H22A—C22—H22B 109.5
C8—C9—C10 121.0 (4) N1—C22—H22C 109.5
C8—C9—H9 119.5 H22A—C22—H22C 109.5
C10—C9—H9 119.5 H22B—C22—H22C 109.5
C9—C10—C11 120.9 (4) N1—C23—H23A 109.5
C9—C10—H10 119.6 N1—C23—H23B 109.5
C11—C10—H10 119.6 H23A—C23—H23B 109.5
C12—C11—C10 117.4 (4) N1—C23—H23C 109.5
C12—C11—C14 121.5 (4) H23A—C23—H23C 109.5
C10—C11—C14 121.0 (4) H23B—C23—H23C 109.5
C13—C12—C11 121.6 (4) C21—N1—C22 111.6 (5)
C13—C12—H12 119.2 C21—N1—C23 110.6 (5)
C11—C12—H12 119.2 C22—N1—C23 110.0 (4)
C12—C13—C8 121.3 (4) C21—N1—Bi1 98.6 (4)
C12—C13—H13 119.4 C22—N1—Bi1 118.9 (3)
C8—C13—H13 119.4 C23—N1—Bi1 106.7 (3)
C11—C14—H14A 109.5 C1—Bi1—C8 96.07 (16)
C11—C14—H14B 109.5 C1—Bi1—C15 90.74 (16)
H14A—C14—H14B 109.5 C1—Bi1—N1 157.55 (14)
C11—C14—H14C 109.5 C8—Bi1—C15 94.85 (17)
H14A—C14—H14C 109.5 C8—Bi1—N1 81.26 (14)
H14B—C14—H14C 109.5 C15—Bi1—N1 67.43 (13)

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SI2298).

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 I, global. DOI: 10.1107/S1600536810043655/si2298sup1.cif

e-67-00m25-sup1.cif (18.8KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810043655/si2298Isup2.hkl

e-67-00m25-Isup2.hkl (174.2KB, hkl)

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


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