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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Aug 17;67(Pt 9):o2340. doi: 10.1107/S1600536811032247

2-{Hy­droxy[1-(4-meth­oxy­phen­yl)-4-oxo-3-phenyl­azetidin-2-yl]meth­yl}acrylonitrile

C M Sai Prasanna a, K Sethusankar b,*, R Rajesh c, R Raghunathan c
PMCID: PMC3200613  PMID: 22058961

Abstract

In the title compound, C20H18N2O3, the β-lactam ring is essentially planar, having a maximum deviation of 0.0291 (15) Å for the N atom, and perpendicular to the phenyl ring [dihedral angle = 85.55 (11)°]. The carbonitrile side chain is almost linear, the C—C—N angle being 176.8 (2)°. The crystal packing is stabilized by inter­molecular O—H⋯O and C—H⋯O inter­actions.

Related literature

For uses of acrylonitrile derivatives, see: Ambrosi et al. (1994). For the pharmacological properties of β-lactam derivatives, see: Brakhage (1998). For related structures, see: Sundaresan et al. (2008); Kamala et al. (2008). For related geometrical parameters, see: Nizam Mohideen et al. (2007).graphic file with name e-67-o2340-scheme1.jpg

Experimental

Crystal data

  • C20H18N2O3

  • M r = 334.36

  • Monoclinic, Inline graphic

  • a = 9.9694 (3) Å

  • b = 19.8196 (6) Å

  • c = 9.6013 (3) Å

  • β = 112.718 (1)°

  • V = 1749.93 (9) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 295 K

  • 0.30 × 0.20 × 0.20 mm

Data collection

  • Bruker Kappa APEXII CCD diffractometer

  • 10596 measured reflections

  • 4368 independent reflections

  • 3621 reflections with I > 2σ(I)

  • R int = 0.019

Refinement

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.100

  • S = 1.01

  • 4368 reflections

  • 228 parameters

  • 2 restraints

  • H-atom parameters constrained

  • Δρmax = 0.16 e Å−3

  • Δρmin = −0.15 e Å−3

Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); 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 (Farrugia, 1997); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811032247/rk2289sup1.cif

e-67-o2340-sup1.cif (19.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811032247/rk2289Isup2.hkl

e-67-o2340-Isup2.hkl (209.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811032247/rk2289Isup3.cml

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—H3⋯O1i 0.82 1.90 2.716 (2) 172
C9—H9⋯O2ii 0.98 2.50 3.467 (2) 169

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

Acknowledgments

CMS and KS thank Dr Babu Varghese, SAIF, IIT, Chennai, India, for the X-ray intensity data collection and Dr V. Murugan, Head of the Department of Physics, for providing facilities in the department to carry out this work.

supplementary crystallographic information

Comment

Acrylonitriles are useful intermediates in organic synthesis and are capable of undergoing many useful organic transformations (Ambrosi et al., 1994), for example, into pyrazole, isoxazole and pyrimidine derivatives. β-Lactams are one of the best known and most extensively studied class of compounds due to their biological activities. The most commonly used β-lactam antibiotics for the therapy of infectious diseases are penicillin and cephalosporin (Brakhage, 1998). X-ray analysis confirms the molecular structure and atom connectivity as illustrated in Fig. 1.

In the title compound C20H18N2O3, due to conjugation in the C19═C18–C20≡N2 moiety, the bond length between C18 and C20 (1.429 (3)Å) shows a significant shortening (Nizam Mohideen et al., 2007). The β-lactam ring is essentially planar and the keto O1 atom deviates from this mean plane by -0.1095 (13)°. The methoxy phenyl (C11-C15) and the phenyl rings (C1-C6) form dihedral angles of 15.66 (10)° and 85.55 (11)°, respectively, with the β-lactam ring. The sum of the angles around N1 atom of the β-lactam ring system accounts for 359.5 (3)° which is in accordance with sp2 hybridization. The phenyl ring and methoxy phenyl ring are cis related with respect to the β-lactam ring.

The bond angles at C18 deviate significantly from regular trigonal geometry. The bond angle around C20, in the chains of atoms C18/C20/N2, is 176.8 (2)° and thus the carbonitrile side chain is almost linear. The torsion angle of -112.87 (19)° for C7–C17–C18═C19 indicates a deviation of the β-lactam ring from the plane of the olefinic double bond. The methoxy group is slightly twisted from the plane of the phenyl ring (C10-C15) to which it is attached as evidenced by the torsion angle C14-C13-O2-C16 of 7.8 (2)°. The interplanar angle between the phenyl (C1-C6) and methoxy phenyl group (C10-C15) is 81.04 (9)°. The title compound exhibits structural similarities with the already reported related structures (Sundaresan et al., 2008, Kamala et al., 2008).

The crystal packing is stabilized by O–H···O and C–H···O hydrogen bonds via O3–H3···O1i and C9–H9···O2ii intermolecular interactions, viewed down the a axis. Symmetry codes: (i) x, -y, z+1/2; (ii) x+1, y, z. The packing view of the title compound is shown in Fig. 2.

Experimental

To the reaction mixture of 1-(4-methoxyphenyl)-4-oxo-3-phenylazetidine-2-carbaldehyde (1 mmol) with acrylonitrile (2 mmol), a catalytic quantity of 1,4-diazabicyclo[2.2.2]octane (10-15 mol %) was added. The reaction mixture was left standing at room temperature in a stoppered sample flask. The progress of the reaction was monitored by TLC over a period of several days. After a period of 10 days, the TLC revealed the presence of a product. The reaction mixture was dissolved in ethyl acetate and washed with aqueous HCl solution (0.25 M) and water followed by brine solution. The organic layer was separated and dried over sodium sulfate. Filtering and evaporation of the organic solvent was done under reduced pressure. The product was separated by flash column chromatography using hexane and ethyl acetate as an eluent (1:9) to give colourless solid. The product was dissolved in chloroform and heated for two minutes. The resulting solution was subjected to crystallization by slow evaporation of the solvent resulting in single crystals suitable for XRD studies.

Refinement

The hydrogen atoms were placed in calculated positions with C–H = 0.93Å to 0.98Å, O–H = 0.82Å and refined in the riding model with fixed isotropic displacement parameters: Uiso(H) = 1.2Ueq(C) for aromatic, methylene, methine groups, Uiso(H) = 1.5Ueq(C) for methyl group and Uiso(H) = 1.5Ueq(O) for hydroxy groups.

The 1876 Friedel pairs were merged ('MERG 2' instruction in SHELXL refinement).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound with the atom numbering scheme. Displacement ellipsoids are drawn at 30% probability level. H atoms are presented as a small spheres of arbitrary radius.

Fig. 2.

Fig. 2.

Packing arrangement of the title compound in the unit cell as viewed down the a axis. The O–H···O and C–H···O intermolecular interactions indicated by dashed lines.

Crystal data

C20H18N2O3 F(000) = 704
Mr = 334.36 Dx = 1.269 Mg m3
Monoclinic, Cc Mo Kα radiation, λ = 0.71073 Å
Hall symbol: C -2yc Cell parameters from 4368 reflections
a = 9.9694 (3) Å θ = 2.4–29.7°
b = 19.8196 (6) Å µ = 0.09 mm1
c = 9.6013 (3) Å T = 295 K
β = 112.718 (1)° Block, colourless
V = 1749.93 (9) Å3 0.30 × 0.20 × 0.20 mm
Z = 4

Data collection

Bruker Kappa APEXII CCD diffractometer 3621 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tube Rint = 0.019
graphite θmax = 29.7°, θmin = 2.4°
ω and φ scans h = −13→13
10596 measured reflections k = −25→27
4368 independent reflections l = −11→13

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)] = 0.038 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100 H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.0577P)2 + 0.1723P] where P = (Fo2 + 2Fc2)/3
4368 reflections (Δ/σ)max < 0.001
228 parameters Δρmax = 0.16 e Å3
2 restraints Δρmin = −0.15 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 > 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 0.6009 (3) 0.19499 (12) 0.1527 (3) 0.0809 (7)
H1 0.6877 0.2116 0.1515 0.097*
C2 0.6025 (2) 0.15799 (11) 0.2755 (3) 0.0630 (5)
H2 0.6902 0.1499 0.3558 0.076*
C3 0.47523 (17) 0.13317 (8) 0.27943 (17) 0.0401 (3)
C4 0.3470 (2) 0.14539 (10) 0.1573 (2) 0.0579 (5)
H4 0.2599 0.1284 0.1570 0.069*
C5 0.3470 (3) 0.18264 (12) 0.0352 (2) 0.0779 (7)
H5 0.2600 0.1908 −0.0461 0.093*
C6 0.4739 (3) 0.20732 (11) 0.0336 (3) 0.0746 (7)
H6 0.4737 0.2324 −0.0482 0.089*
C7 0.38921 (15) 0.13134 (7) 0.50213 (17) 0.0340 (3)
H7 0.3452 0.1742 0.4561 0.041*
C8 0.36425 (16) 0.03948 (7) 0.39009 (16) 0.0379 (3)
C9 0.47470 (16) 0.09626 (7) 0.41628 (17) 0.0362 (3)
H9 0.5727 0.0827 0.4844 0.043*
C10 0.16463 (15) 0.06120 (7) 0.49049 (16) 0.0359 (3)
C11 0.10281 (17) 0.11362 (8) 0.5408 (2) 0.0443 (4)
H11 0.1396 0.1571 0.5466 0.053*
C12 −0.01237 (18) 0.10169 (8) 0.5822 (2) 0.0471 (4)
H12 −0.0528 0.1371 0.6165 0.057*
C13 −0.06861 (16) 0.03725 (8) 0.57319 (18) 0.0414 (3)
C14 −0.00915 (17) −0.01503 (8) 0.51980 (19) 0.0425 (4)
H14 −0.0471 −0.0584 0.5123 0.051*
C15 0.10649 (17) −0.00288 (8) 0.47766 (18) 0.0410 (3)
H15 0.1452 −0.0379 0.4406 0.049*
C16 −0.2330 (2) −0.03522 (11) 0.6291 (3) 0.0599 (5)
H16A −0.2710 −0.0556 0.5308 0.090*
H16B −0.3083 −0.0327 0.6680 0.090*
H16C −0.1540 −0.0620 0.6957 0.090*
C17 0.47215 (16) 0.13644 (8) 0.67345 (17) 0.0391 (3)
H17 0.4046 0.1492 0.7208 0.047*
C18 0.58853 (18) 0.19031 (8) 0.70558 (18) 0.0433 (4)
C19 0.7295 (2) 0.17793 (11) 0.7631 (2) 0.0607 (5)
H19A 0.7953 0.2131 0.7778 0.073*
H19B 0.7629 0.1341 0.7890 0.073*
C20 0.5348 (2) 0.25736 (10) 0.6650 (3) 0.0602 (5)
N1 0.28665 (13) 0.07467 (6) 0.45591 (15) 0.0381 (3)
N2 0.4860 (3) 0.30955 (10) 0.6326 (4) 0.1008 (8)
O1 0.34670 (14) −0.01631 (6) 0.33461 (15) 0.0505 (3)
O2 −0.18217 (13) 0.03094 (6) 0.61854 (16) 0.0557 (3)
O3 0.53772 (13) 0.07510 (6) 0.73290 (14) 0.0525 (3)
H3 0.4856 0.0542 0.7661 0.079*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0945 (18) 0.0779 (15) 0.098 (2) −0.0164 (13) 0.0673 (17) 0.0082 (13)
C2 0.0580 (11) 0.0681 (11) 0.0739 (13) −0.0036 (9) 0.0375 (10) 0.0104 (10)
C3 0.0488 (8) 0.0364 (7) 0.0431 (8) 0.0012 (6) 0.0268 (7) −0.0027 (6)
C4 0.0618 (10) 0.0669 (11) 0.0434 (10) −0.0110 (9) 0.0186 (8) 0.0037 (8)
C5 0.1023 (18) 0.0790 (15) 0.0425 (11) −0.0110 (13) 0.0172 (11) 0.0081 (10)
C6 0.129 (2) 0.0563 (12) 0.0573 (12) −0.0166 (12) 0.0570 (14) −0.0006 (9)
C7 0.0361 (7) 0.0303 (6) 0.0398 (7) −0.0006 (5) 0.0192 (6) −0.0018 (5)
C8 0.0429 (8) 0.0365 (7) 0.0377 (8) 0.0052 (6) 0.0193 (7) 0.0000 (6)
C9 0.0379 (7) 0.0364 (7) 0.0381 (7) 0.0036 (5) 0.0186 (6) −0.0004 (5)
C10 0.0334 (7) 0.0358 (7) 0.0390 (7) 0.0036 (6) 0.0146 (6) −0.0007 (6)
C11 0.0438 (8) 0.0321 (7) 0.0628 (11) 0.0002 (6) 0.0271 (7) −0.0025 (7)
C12 0.0438 (8) 0.0399 (8) 0.0655 (11) 0.0089 (7) 0.0298 (8) 0.0003 (7)
C13 0.0322 (7) 0.0448 (8) 0.0474 (9) 0.0027 (6) 0.0155 (6) 0.0056 (6)
C14 0.0415 (8) 0.0352 (8) 0.0521 (9) −0.0046 (6) 0.0195 (7) −0.0016 (6)
C15 0.0432 (8) 0.0359 (7) 0.0442 (8) 0.0009 (6) 0.0171 (7) −0.0056 (6)
C16 0.0520 (10) 0.0602 (11) 0.0747 (14) −0.0111 (8) 0.0324 (10) 0.0041 (9)
C17 0.0426 (8) 0.0425 (8) 0.0381 (8) −0.0011 (6) 0.0221 (6) −0.0006 (6)
C18 0.0497 (9) 0.0449 (9) 0.0386 (8) −0.0053 (7) 0.0206 (7) −0.0064 (6)
C19 0.0509 (10) 0.0615 (11) 0.0645 (12) −0.0068 (9) 0.0166 (9) −0.0034 (9)
C20 0.0520 (10) 0.0496 (11) 0.0780 (13) −0.0107 (8) 0.0239 (9) −0.0131 (9)
N1 0.0395 (6) 0.0323 (6) 0.0473 (7) −0.0010 (5) 0.0221 (5) −0.0062 (5)
N2 0.0825 (14) 0.0460 (11) 0.161 (3) −0.0015 (9) 0.0328 (14) −0.0037 (12)
O1 0.0618 (7) 0.0393 (6) 0.0584 (7) −0.0014 (5) 0.0321 (6) −0.0114 (5)
O2 0.0462 (7) 0.0517 (7) 0.0801 (9) 0.0010 (5) 0.0364 (6) 0.0068 (6)
O3 0.0558 (7) 0.0535 (7) 0.0536 (7) 0.0034 (5) 0.0271 (6) 0.0171 (5)

Geometric parameters (Å, °)

C1—C6 1.361 (4) C11—C12 1.373 (2)
C1—C2 1.383 (3) C11—H11 0.9300
C1—H1 0.9300 C12—C13 1.384 (2)
C2—C3 1.375 (2) C12—H12 0.9300
C2—H2 0.9300 C13—O2 1.367 (2)
C3—C4 1.382 (2) C13—C14 1.387 (2)
C3—C9 1.506 (2) C14—C15 1.382 (2)
C4—C5 1.385 (3) C14—H14 0.9300
C4—H4 0.9300 C15—H15 0.9300
C5—C6 1.361 (4) C16—O2 1.423 (2)
C5—H5 0.9300 C16—H16A 0.9600
C6—H6 0.9300 C16—H16B 0.9600
C7—N1 1.4675 (18) C16—H16C 0.9600
C7—C17 1.533 (2) C17—O3 1.3938 (19)
C7—C9 1.559 (2) C17—C18 1.518 (2)
C7—H7 0.9800 C17—H17 0.9800
C8—O1 1.2105 (18) C18—C19 1.319 (3)
C8—N1 1.3645 (19) C18—C20 1.429 (3)
C8—C9 1.526 (2) C19—H19A 0.9300
C9—H9 0.9800 C19—H19B 0.9300
C10—C15 1.382 (2) C20—N2 1.134 (3)
C10—C11 1.387 (2) O3—H3 0.8200
C10—N1 1.4047 (19)
C6—C1—C2 120.8 (2) C10—C11—H11 119.8
C6—C1—H1 119.6 C11—C12—C13 120.30 (14)
C2—C1—H1 119.6 C11—C12—H12 119.8
C3—C2—C1 120.4 (2) C13—C12—H12 119.8
C3—C2—H2 119.8 O2—C13—C12 115.46 (14)
C1—C2—H2 119.8 O2—C13—C14 125.06 (14)
C2—C3—C4 118.34 (16) C12—C13—C14 119.48 (14)
C2—C3—C9 120.81 (15) C15—C14—C13 120.13 (14)
C4—C3—C9 120.79 (14) C15—C14—H14 119.9
C3—C4—C5 120.60 (19) C13—C14—H14 119.9
C3—C4—H4 119.7 C10—C15—C14 120.17 (14)
C5—C4—H4 119.7 C10—C15—H15 119.9
C6—C5—C4 120.3 (2) C14—C15—H15 119.9
C6—C5—H5 119.8 O2—C16—H16A 109.5
C4—C5—H5 119.8 O2—C16—H16B 109.5
C1—C6—C5 119.6 (2) H16A—C16—H16B 109.5
C1—C6—H6 120.2 O2—C16—H16C 109.5
C5—C6—H6 120.2 H16A—C16—H16C 109.5
N1—C7—C17 113.52 (12) H16B—C16—H16C 109.5
N1—C7—C9 87.60 (10) O3—C17—C18 109.23 (12)
C17—C7—C9 114.72 (12) O3—C17—C7 110.82 (13)
N1—C7—H7 112.9 C18—C17—C7 108.52 (12)
C17—C7—H7 112.9 O3—C17—H17 109.4
C9—C7—H7 112.9 C18—C17—H17 109.4
O1—C8—N1 131.25 (14) C7—C17—H17 109.4
O1—C8—C9 135.95 (14) C19—C18—C20 120.90 (16)
N1—C8—C9 92.80 (11) C19—C18—C17 124.13 (16)
C3—C9—C8 117.38 (13) C20—C18—C17 114.94 (15)
C3—C9—C7 115.56 (12) C18—C19—H19A 120.0
C8—C9—C7 84.78 (11) C18—C19—H19B 120.0
C3—C9—H9 112.2 H19A—C19—H19B 120.0
C8—C9—H9 112.2 N2—C20—C18 176.8 (2)
C7—C9—H9 112.2 C8—N1—C10 135.24 (12)
C15—C10—C11 119.48 (14) C8—N1—C7 94.46 (11)
C15—C10—N1 121.69 (13) C10—N1—C7 129.77 (11)
C11—C10—N1 118.83 (13) C13—O2—C16 117.93 (14)
C12—C11—C10 120.40 (14) C17—O3—H3 109.5
C12—C11—H11 119.8
C6—C1—C2—C3 −0.2 (4) C12—C13—C14—C15 0.7 (2)
C1—C2—C3—C4 0.9 (3) C11—C10—C15—C14 −2.3 (2)
C1—C2—C3—C9 −176.48 (18) N1—C10—C15—C14 176.76 (14)
C2—C3—C4—C5 −1.0 (3) C13—C14—C15—C10 0.9 (2)
C9—C3—C4—C5 176.35 (18) N1—C7—C17—O3 52.33 (16)
C3—C4—C5—C6 0.5 (3) C9—C7—C17—O3 −46.30 (16)
C2—C1—C6—C5 −0.3 (4) N1—C7—C17—C18 172.26 (12)
C4—C5—C6—C1 0.2 (4) C9—C7—C17—C18 73.64 (15)
C2—C3—C9—C8 −146.86 (16) O3—C17—C18—C19 8.0 (2)
C4—C3—C9—C8 35.9 (2) C7—C17—C18—C19 −112.87 (19)
C2—C3—C9—C7 115.42 (18) O3—C17—C18—C20 −173.48 (15)
C4—C3—C9—C7 −61.8 (2) C7—C17—C18—C20 65.61 (19)
O1—C8—C9—C3 68.9 (2) O1—C8—N1—C10 2.8 (3)
N1—C8—C9—C3 −111.64 (14) C9—C8—N1—C10 −176.66 (16)
O1—C8—C9—C7 −174.95 (18) O1—C8—N1—C7 174.71 (17)
N1—C8—C9—C7 4.50 (11) C9—C8—N1—C7 −4.78 (12)
N1—C7—C9—C3 113.74 (13) C15—C10—N1—C8 9.6 (3)
C17—C7—C9—C3 −131.40 (14) C11—C10—N1—C8 −171.31 (17)
N1—C7—C9—C8 −4.18 (11) C15—C10—N1—C7 −159.80 (15)
C17—C7—C9—C8 110.68 (13) C11—C10—N1—C7 19.2 (2)
C15—C10—C11—C12 2.1 (2) C17—C7—N1—C8 −111.32 (13)
N1—C10—C11—C12 −177.01 (15) C9—C7—N1—C8 4.67 (12)
C10—C11—C12—C13 −0.4 (3) C17—C7—N1—C10 61.25 (19)
C11—C12—C13—O2 179.40 (16) C9—C7—N1—C10 177.24 (14)
C11—C12—C13—C14 −1.0 (3) C12—C13—O2—C16 −172.56 (17)
O2—C13—C14—C15 −179.66 (15) C14—C13—O2—C16 7.8 (2)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O3—H3···O1i 0.82 1.90 2.716 (2) 172
C9—H9···O2ii 0.98 2.50 3.467 (2) 169

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RK2289).

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) global, I. DOI: 10.1107/S1600536811032247/rk2289sup1.cif

e-67-o2340-sup1.cif (19.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811032247/rk2289Isup2.hkl

e-67-o2340-Isup2.hkl (209.7KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811032247/rk2289Isup3.cml

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


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