Abstract
In the crystal structure of the title compound, C6H9N2 +·C6H4NO3 −·C6H5NO3, ions and molecules are connected via intermolecular N—H⋯O, N—H⋯N, O—H⋯O and C—H⋯O hydrogen bonds into a three-dimensional network.
Related literature
For background to the development of ferroelectric pure organic or inorganic compounds, see: Haertling et al. (1999 ▶); Homes et al. (2001 ▶). For our recent reports on the synthesis of a variety of compounds which have potential piezoelectric and ferroelectric properties, see: Fu et al. (2009 ▶); Hang et al. (2009 ▶).
Experimental
Crystal data
C6H9N2 +·C6H4NO3 −·C6H5NO3
M r = 386.36
Triclinic,
a = 6.3666 (13) Å
b = 7.4451 (15) Å
c = 21.262 (4) Å
α = 92.41 (3)°
β = 95.56 (3)°
γ = 113.99 (3)°
V = 912.8 (3) Å3
Z = 2
Mo Kα radiation
μ = 0.11 mm−1
T = 293 K
0.20 × 0.20 × 0.20 mm
Data collection
Rigaku Mercury2 diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.825, T max = 1.000
9547 measured reflections
4182 independent reflections
2896 reflections with I > 2σ(I)
R int = 0.034
Refinement
R[F 2 > 2σ(F 2)] = 0.054
wR(F 2) = 0.140
S = 1.05
4182 reflections
253 parameters
H-atom parameters constrained
Δρmax = 0.16 e Å−3
Δρmin = −0.25 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810021902/jh2162sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810021902/jh2162Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—H1A⋯O2i | 0.89 | 2.09 | 2.952 (2) | 162 |
| N1—H1B⋯O3ii | 0.89 | 1.87 | 2.753 (2) | 169 |
| N1—H1C⋯N2iii | 0.89 | 2.16 | 2.866 (2) | 136 |
| O4—H4A⋯O3 | 0.96 | 1.58 | 2.5385 (19) | 173 |
| C1—H1D⋯O5iv | 0.93 | 2.52 | 3.229 (3) | 133 |
| C2—H2A⋯O6v | 0.93 | 2.58 | 3.327 (3) | 138 |
| C8—H10A⋯O4iii | 0.93 | 2.54 | 3.462 (3) | 169 |
Symmetry codes: (i)
; (ii)
; (iii)
; (iv)
; (v)
.
Acknowledgments
The authors are grateful to the starter fund of Southeast University for financial support to buy the X-ray diffractometer.
supplementary crystallographic information
Comment
At present, much attention in ferroelectric material field is focused on developing ferroelectric pure organic or inorganic compounds (Haertling et al. 1999; Homes et al. 2001). Recently we have reported the synthesis of a variety of compounds (Fu et al., 2009; Hang et al., 2009), which have potential piezoelectric and ferroelectric properties. In order to find more dielectric ferroelectric materials, we investigate the physical properties of the title compound(Fig. 1). The dielectric constant of the title compound as a function of temperature indicates that the permittivity is basically temperature-independent (dielectric constant equaling to 2.8 to 4.6), suggesting that this compound should be not a real ferroelectrics or there may be no distinct phase transition occurred within the measured temperature range. Similarly, below the melting point (399 K) of the compound, the dielectric constant as a function of temperature also goes smoothly, and there is no dielectric anomaly observed (dielectric constant equaling to 2.8 to 4.6).Herein, we report the synthesis and crystal structure of the title compound.
The molecular structure of the title compound is shown in Fig. 1. There are one 4-nitrophenolate anion, an substituted ammonium cation and a neutral 4-nitrophenol molecule in the asymmetric unit. Molecules of the title compound have normal geometric parameters. The bond lengths and angles are within their normal ranges. All pyridine rings are, of course, planar. As can be seen from the packing diagram (Fig. 2), molecules are connected via intermolecular C—H···O and O—H···N hydrogen bonds to form a three dimensional network. Dipole–dipole and van der Waals interactions are effective in the molecular packing.
Experimental
4-nitrophenol (2.085 g, 0.015 mol) was added slowly to a solution of pyridin-3-ylmethanamine (1.62 g, 0.015 mol) in methanol.After several days, the title compound was formed and recrystallized from solution to afford colourless prismatic crystals suitable for X-ray analysis.
Refinement
H atoms were positioned geometrically and refined using a riding model, with C—H(aromatic) = 0.93 and 0.97 (methylene) Å, N—H = 0.89 Å and O—H = 0.97 Å and with Uiso(H) = 1.3–1.5Ueq(C, N, O).
Figures
Fig. 1.
Perspective structure of the title compound, showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
The crystal packing of the title compound viewed along the a axis showing the hydrogen bondings network. Some of the H atoms have been ommitted for clarity.
Crystal data
| C6H9N2+·C6H4NO3−·C6H5nO3 | Z = 2 |
| Mr = 386.36 | F(000) = 404 |
| Triclinic, P1 | Dx = 1.406 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 6.3666 (13) Å | Cell parameters from 4182 reflections |
| b = 7.4451 (15) Å | θ = 2.6–27.5° |
| c = 21.262 (4) Å | µ = 0.11 mm−1 |
| α = 92.41 (3)° | T = 293 K |
| β = 95.56 (3)° | Prism, colorless |
| γ = 113.99 (3)° | 0.20 × 0.20 × 0.20 mm |
| V = 912.8 (3) Å3 |
Data collection
| Rigaku Mercury2 diffractometer | 4182 independent reflections |
| Radiation source: fine-focus sealed tube | 2896 reflections with I > 2σ(I) |
| graphite | Rint = 0.034 |
| Detector resolution: 13.6612 pixels mm-1 | θmax = 27.5°, θmin = 3.0° |
| CCD_Profile_fitting scans | h = −8→8 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −9→9 |
| Tmin = 0.825, Tmax = 1.000 | l = −27→27 |
| 9547 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)] = 0.054 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.140 | H-atom parameters constrained |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0576P)2 + 0.2125P] where P = (Fo2 + 2Fc2)/3 |
| 4182 reflections | (Δ/σ)max < 0.001 |
| 253 parameters | Δρmax = 0.16 e Å−3 |
| 0 restraints | Δρmin = −0.25 e Å−3 |
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 | ||
| O3 | 0.3538 (2) | 0.0490 (2) | 0.19323 (6) | 0.0471 (3) | |
| O4 | 0.7520 (2) | 0.0641 (2) | 0.23068 (6) | 0.0490 (4) | |
| H4A | 0.6012 | 0.0634 | 0.2194 | 0.074* | |
| C10 | 0.2665 (3) | 0.2431 (3) | 0.01944 (8) | 0.0389 (4) | |
| N3 | 0.2243 (3) | 0.2980 (2) | −0.04283 (8) | 0.0481 (4) | |
| C7 | 0.3307 (3) | 0.1152 (3) | 0.13814 (8) | 0.0369 (4) | |
| O2 | 0.3528 (3) | 0.2970 (2) | −0.08282 (7) | 0.0609 (4) | |
| O1 | 0.0584 (3) | 0.3409 (3) | −0.05577 (7) | 0.0687 (5) | |
| C9 | 0.1125 (3) | 0.2297 (3) | 0.06264 (9) | 0.0442 (5) | |
| H9A | −0.0114 | 0.2633 | 0.0522 | 0.053* | |
| C8 | 0.1442 (3) | 0.1664 (3) | 0.12100 (9) | 0.0438 (4) | |
| H10A | 0.0403 | 0.1572 | 0.1499 | 0.053* | |
| C13 | 0.8177 (3) | 0.1128 (3) | 0.29326 (8) | 0.0388 (4) | |
| C12 | 0.4868 (3) | 0.1361 (3) | 0.09345 (9) | 0.0445 (5) | |
| H12A | 0.6144 | 0.1074 | 0.1040 | 0.053* | |
| C11 | 0.4552 (3) | 0.1978 (3) | 0.03479 (9) | 0.0445 (5) | |
| H11A | 0.5589 | 0.2091 | 0.0057 | 0.053* | |
| C18 | 0.6884 (3) | 0.1667 (3) | 0.33310 (9) | 0.0488 (5) | |
| H18A | 0.5513 | 0.1731 | 0.3165 | 0.059* | |
| C16 | 0.9669 (4) | 0.2016 (3) | 0.42097 (9) | 0.0523 (5) | |
| C14 | 1.0262 (3) | 0.1105 (3) | 0.31834 (9) | 0.0476 (5) | |
| H14A | 1.1167 | 0.0798 | 0.2917 | 0.057* | |
| C15 | 1.0994 (4) | 0.1534 (3) | 0.38222 (10) | 0.0530 (5) | |
| H15A | 1.2379 | 0.1497 | 0.3991 | 0.064* | |
| C17 | 0.7627 (4) | 0.2106 (3) | 0.39719 (10) | 0.0570 (6) | |
| H17A | 0.6761 | 0.2459 | 0.4240 | 0.068* | |
| O5 | 1.2363 (4) | 0.2523 (5) | 0.50752 (9) | 0.1289 (10) | |
| O6 | 0.9263 (4) | 0.2807 (4) | 0.52407 (9) | 0.1112 (8) | |
| N4 | 1.0492 (5) | 0.2488 (4) | 0.48875 (10) | 0.0792 (7) | |
| N1 | −0.0537 (3) | 0.7260 (2) | 0.20070 (7) | 0.0414 (4) | |
| H1A | −0.1686 | 0.7006 | 0.1696 | 0.062* | |
| H1B | 0.0690 | 0.8325 | 0.1935 | 0.062* | |
| H1C | −0.0989 | 0.7476 | 0.2375 | 0.062* | |
| N2 | 0.5902 (3) | 0.6209 (3) | 0.28249 (8) | 0.0502 (4) | |
| C1 | 0.5678 (4) | 0.6498 (3) | 0.34345 (9) | 0.0485 (5) | |
| H1D | 0.6919 | 0.6693 | 0.3739 | 0.058* | |
| C4 | 0.2013 (3) | 0.5896 (3) | 0.25514 (9) | 0.0398 (4) | |
| C5 | 0.4074 (3) | 0.5913 (3) | 0.24015 (9) | 0.0466 (5) | |
| H5A | 0.4205 | 0.5703 | 0.1975 | 0.056* | |
| C3 | 0.1849 (3) | 0.6229 (3) | 0.31859 (9) | 0.0469 (5) | |
| H3A | 0.0499 | 0.6254 | 0.3309 | 0.056* | |
| C6 | 0.0087 (4) | 0.5549 (3) | 0.20322 (10) | 0.0491 (5) | |
| H6A | 0.0559 | 0.5305 | 0.1628 | 0.059* | |
| H6C | −0.1262 | 0.4384 | 0.2101 | 0.059* | |
| C2 | 0.3695 (3) | 0.6522 (3) | 0.36331 (9) | 0.0490 (5) | |
| H2A | 0.3605 | 0.6733 | 0.4062 | 0.059* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O3 | 0.0441 (8) | 0.0624 (9) | 0.0358 (7) | 0.0228 (7) | 0.0022 (6) | 0.0128 (6) |
| O4 | 0.0430 (8) | 0.0695 (9) | 0.0332 (7) | 0.0231 (7) | −0.0002 (6) | 0.0017 (6) |
| C10 | 0.0433 (10) | 0.0396 (10) | 0.0295 (9) | 0.0146 (8) | −0.0031 (7) | 0.0008 (7) |
| N3 | 0.0561 (11) | 0.0485 (10) | 0.0345 (9) | 0.0185 (8) | −0.0034 (8) | 0.0026 (7) |
| C7 | 0.0358 (9) | 0.0402 (10) | 0.0305 (9) | 0.0128 (8) | −0.0018 (7) | 0.0015 (7) |
| O2 | 0.0672 (10) | 0.0792 (11) | 0.0352 (8) | 0.0280 (8) | 0.0083 (7) | 0.0124 (7) |
| O1 | 0.0807 (12) | 0.0936 (12) | 0.0480 (9) | 0.0546 (10) | −0.0054 (8) | 0.0147 (8) |
| C9 | 0.0437 (11) | 0.0536 (11) | 0.0404 (10) | 0.0265 (9) | −0.0004 (8) | 0.0038 (9) |
| C8 | 0.0433 (11) | 0.0561 (12) | 0.0370 (10) | 0.0249 (9) | 0.0074 (8) | 0.0044 (9) |
| C13 | 0.0389 (10) | 0.0422 (10) | 0.0324 (9) | 0.0143 (8) | 0.0020 (7) | 0.0050 (8) |
| C12 | 0.0398 (10) | 0.0605 (12) | 0.0386 (10) | 0.0267 (9) | 0.0014 (8) | 0.0068 (9) |
| C11 | 0.0412 (10) | 0.0563 (12) | 0.0360 (10) | 0.0198 (9) | 0.0059 (8) | 0.0037 (8) |
| C18 | 0.0410 (11) | 0.0651 (13) | 0.0432 (11) | 0.0253 (10) | 0.0035 (8) | 0.0031 (9) |
| C16 | 0.0573 (13) | 0.0654 (13) | 0.0322 (10) | 0.0250 (11) | −0.0012 (9) | 0.0009 (9) |
| C14 | 0.0441 (11) | 0.0602 (12) | 0.0420 (11) | 0.0264 (10) | 0.0024 (8) | −0.0029 (9) |
| C15 | 0.0458 (12) | 0.0689 (14) | 0.0451 (12) | 0.0283 (11) | −0.0090 (9) | −0.0022 (10) |
| C17 | 0.0527 (13) | 0.0778 (15) | 0.0436 (12) | 0.0291 (12) | 0.0128 (9) | −0.0005 (11) |
| O5 | 0.1125 (19) | 0.228 (3) | 0.0508 (12) | 0.088 (2) | −0.0332 (12) | −0.0189 (14) |
| O6 | 0.1272 (19) | 0.172 (2) | 0.0420 (10) | 0.0706 (18) | 0.0152 (11) | −0.0083 (12) |
| N4 | 0.0898 (17) | 0.1082 (18) | 0.0373 (11) | 0.0416 (14) | −0.0021 (11) | −0.0018 (11) |
| N1 | 0.0396 (9) | 0.0564 (10) | 0.0309 (8) | 0.0226 (8) | 0.0024 (6) | 0.0071 (7) |
| N2 | 0.0444 (10) | 0.0676 (11) | 0.0412 (9) | 0.0260 (9) | 0.0038 (7) | 0.0050 (8) |
| C1 | 0.0471 (11) | 0.0589 (12) | 0.0383 (11) | 0.0217 (10) | −0.0015 (8) | 0.0085 (9) |
| C4 | 0.0421 (10) | 0.0377 (10) | 0.0379 (10) | 0.0159 (8) | −0.0004 (8) | 0.0047 (8) |
| C5 | 0.0499 (12) | 0.0566 (12) | 0.0343 (10) | 0.0232 (10) | 0.0043 (8) | 0.0016 (9) |
| C3 | 0.0431 (11) | 0.0576 (12) | 0.0430 (11) | 0.0232 (10) | 0.0075 (8) | 0.0076 (9) |
| C6 | 0.0529 (12) | 0.0454 (11) | 0.0462 (12) | 0.0212 (10) | −0.0091 (9) | −0.0012 (9) |
| C2 | 0.0507 (12) | 0.0643 (13) | 0.0329 (10) | 0.0235 (10) | 0.0088 (8) | 0.0081 (9) |
Geometric parameters (Å, °)
| O3—C7 | 1.308 (2) | C14—C15 | 1.373 (3) |
| O4—C13 | 1.344 (2) | C14—H14A | 0.9300 |
| O4—H4A | 0.9646 | C15—H15A | 0.9300 |
| C10—C9 | 1.385 (3) | C17—H17A | 0.9300 |
| C10—C11 | 1.387 (3) | O5—N4 | 1.209 (3) |
| C10—N3 | 1.435 (2) | O6—N4 | 1.218 (3) |
| N3—O1 | 1.232 (2) | N1—C6 | 1.482 (2) |
| N3—O2 | 1.238 (2) | N1—H1A | 0.8900 |
| C7—C8 | 1.409 (3) | N1—H1B | 0.8900 |
| C7—C12 | 1.409 (3) | N1—H1C | 0.8900 |
| C9—C8 | 1.371 (3) | N2—C1 | 1.336 (3) |
| C9—H9A | 0.9300 | N2—C5 | 1.336 (3) |
| C8—H10A | 0.9300 | C1—C2 | 1.376 (3) |
| C13—C14 | 1.389 (3) | C1—H1D | 0.9300 |
| C13—C18 | 1.389 (3) | C4—C5 | 1.375 (3) |
| C12—C11 | 1.372 (3) | C4—C3 | 1.383 (3) |
| C12—H12A | 0.9300 | C4—C6 | 1.498 (3) |
| C11—H11A | 0.9300 | C5—H5A | 0.9300 |
| C18—C17 | 1.378 (3) | C3—C2 | 1.375 (3) |
| C18—H18A | 0.9300 | C3—H3A | 0.9300 |
| C16—C15 | 1.370 (3) | C6—H6A | 0.9700 |
| C16—C17 | 1.377 (3) | C6—H6C | 0.9700 |
| C16—N4 | 1.462 (3) | C2—H2A | 0.9300 |
| C13—O4—H4A | 110.0 | C14—C15—H15A | 120.3 |
| C9—C10—C11 | 121.06 (17) | C16—C17—C18 | 119.14 (19) |
| C9—C10—N3 | 119.04 (17) | C16—C17—H17A | 120.4 |
| C11—C10—N3 | 119.86 (18) | C18—C17—H17A | 120.4 |
| O1—N3—O2 | 121.47 (17) | O5—N4—O6 | 122.7 (2) |
| O1—N3—C10 | 119.44 (17) | O5—N4—C16 | 118.4 (2) |
| O2—N3—C10 | 119.07 (17) | O6—N4—C16 | 119.0 (2) |
| O3—C7—C8 | 120.54 (17) | C6—N1—H1A | 109.5 |
| O3—C7—C12 | 122.14 (16) | C6—N1—H1B | 109.5 |
| C8—C7—C12 | 117.31 (16) | H1A—N1—H1B | 109.5 |
| C8—C9—C10 | 119.43 (17) | C6—N1—H1C | 109.5 |
| C8—C9—H9A | 120.3 | H1A—N1—H1C | 109.5 |
| C10—C9—H9A | 120.3 | H1B—N1—H1C | 109.5 |
| C9—C8—C7 | 121.42 (18) | C1—N2—C5 | 116.81 (18) |
| C9—C8—H10A | 119.3 | N2—C1—C2 | 123.07 (19) |
| C7—C8—H10A | 119.3 | N2—C1—H1D | 118.5 |
| O4—C13—C14 | 117.63 (17) | C2—C1—H1D | 118.5 |
| O4—C13—C18 | 123.06 (17) | C5—C4—C3 | 117.13 (18) |
| C14—C13—C18 | 119.31 (17) | C5—C4—C6 | 119.56 (18) |
| C11—C12—C7 | 121.54 (17) | C3—C4—C6 | 123.31 (18) |
| C11—C12—H12A | 119.2 | N2—C5—C4 | 124.60 (18) |
| C7—C12—H12A | 119.2 | N2—C5—H5A | 117.7 |
| C12—C11—C10 | 119.20 (18) | C4—C5—H5A | 117.7 |
| C12—C11—H11A | 120.4 | C2—C3—C4 | 119.60 (19) |
| C10—C11—H11A | 120.4 | C2—C3—H3A | 120.2 |
| C17—C18—C13 | 120.22 (19) | C4—C3—H3A | 120.2 |
| C17—C18—H18A | 119.9 | N1—C6—C4 | 111.67 (16) |
| C13—C18—H18A | 119.9 | N1—C6—H6A | 109.3 |
| C15—C16—C17 | 121.48 (19) | C4—C6—H6A | 109.3 |
| C15—C16—N4 | 118.6 (2) | N1—C6—H6C | 109.3 |
| C17—C16—N4 | 119.9 (2) | C4—C6—H6C | 109.3 |
| C15—C14—C13 | 120.36 (19) | H6A—C6—H6C | 107.9 |
| C15—C14—H14A | 119.8 | C3—C2—C1 | 118.79 (19) |
| C13—C14—H14A | 119.8 | C3—C2—H2A | 120.6 |
| C16—C15—C14 | 119.43 (19) | C1—C2—H2A | 120.6 |
| C16—C15—H15A | 120.3 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H1A···O2i | 0.89 | 2.09 | 2.952 (2) | 162 |
| N1—H1B···O3ii | 0.89 | 1.87 | 2.753 (2) | 169 |
| N1—H1C···N2iii | 0.89 | 2.16 | 2.866 (2) | 136 |
| O4—H4A···O3 | 0.96 | 1.58 | 2.5385 (19) | 173 |
| C1—H1D···O5iv | 0.93 | 2.52 | 3.229 (3) | 133 |
| C2—H2A···O6v | 0.93 | 2.58 | 3.327 (3) | 138 |
| C8—H10A···O4iii | 0.93 | 2.54 | 3.462 (3) | 169 |
Symmetry codes: (i) −x, −y+1, −z; (ii) x, y+1, z; (iii) x−1, y, z; (iv) −x+2, −y+1, −z+1; (v) −x+1, −y+1, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: JH2162).
References
- Fu, D. W., Ge, J. Z., Dai, J., Ye, H. Y. & Qu, Z. R. (2009). Inorg. Chem. Commun.12, 994–997.
- Haertling, G. H. (1999). J. Am. Ceram. Soc.82, 797–810.
- Hang, T., Fu, D. W., Ye, Q. & Xiong, R. G. (2009). Cryst. Growth Des.5, 2026–2029.
- Homes, C. C., Vogt, T., Shapiro, S. M., Wakimoto, S. & Ramirez, A. P. (2001). Science, 293, 673–676. [DOI] [PubMed]
- Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
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/S1600536810021902/jh2162sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810021902/jh2162Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


