
Acta Cryst. (2013). E69, m132 [ doi:10.1107/S1600536813002985 ]
The crystal structure of the title compound, (C12H12N2)(C12H11N2)[Mo(CN)8]·4H2O, consists of 4,4'-(ethene-1,2-diyl)dipyridinium and 4-[2-(pyridin-4-yl)ethenyl]pyridinium cations disordered over the same site, an [Mo(CN)8]3- anion and four water molecules of crystallization. The eight-coordinate [Mo(CN)8]3- unit exhibits a slightly distorted square-antiprismatic geometry. In the structure, the cations (crystallographic symmetry, 2) and anions (crystallographic symmetry, 222) are arranged alternately by N-H
O and O-H
N hydrogen bonds, forming layers parallel to the bc plane. These layers are further linked through O-H
N hydrogen bonds, generating a three-dimensional supramolecular network.
Single crystals of the title compound were prepared at room temperature by slow diffusion of a CH3CN/H2O (1:1 v/v) solution containing both CeIII(NO3)3.6H2O (0.05 mmol) and dpe (0.15 mmol) in a CH3CN/H2O (1:1 v/v) solution of [HN(n-C4H9)3]3[MoV(CN)8].4H2O (0.05 mmol). After four weeks, dark-blue rod-like crystals were obtained.
All non-H atoms were refined anisotropically. The (C)H atoms were calculated at idealized positions and included in the refinement in a riding mode. The (N)H and (O)H atoms of water molecules were located from a difference Fourier map and refined as riding [N—H = 0.89 Å, U(H) = 1.2Ueq(N); O—H = 0.85 Å, U(H) = 1.5Ueq(O)], with the occupancy factor of the N-bound H atoms set to. 0.75
Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004; 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: SHELXTL (Sheldrick, 2008).
| (C12H12N2)(C12H11N2)[Mo(CN)8]·4H2O | F(000) = 1524 |
| Mr = 743.63 | Dx = 1.567 Mg m−3 |
| Orthorhombic, Ccca | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2b 2bc | Cell parameters from 6602 reflections |
| a = 12.403 (3) Å | θ = 3.4–29.0° |
| b = 16.534 (3) Å | µ = 0.48 mm−1 |
| c = 15.370 (3) Å | T = 291 K |
| V = 3151.8 (11) Å3 | Rod, dark blue |
| Z = 4 | 0.18 × 0.15 × 0.13 mm |
| Bruker SMART APEXII diffractometer | 1442 independent reflections |
| Radiation source: fine-focus sealed tube | 1388 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.016 |
| phi and ω scans | θmax = 25.3°, θmin = 3.4° |
| Absorption correction: multi-scan (SADABS; Bruker, 2004) | h = −14→14 |
| Tmin = 0.919, Tmax = 0.941 | k = −15→19 |
| 6789 measured reflections | l = −18→16 |
| 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)] = 0.021 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.052 | H-atom parameters constrained |
| S = 1.09 | w = 1/[σ2(Fo2) + (0.0237P)2 + 4.1639P] where P = (Fo2 + 2Fc2)/3 |
| 1442 reflections | (Δ/σ)max < 0.001 |
| 112 parameters | Δρmax = 0.28 e Å−3 |
| 0 restraints | Δρmin = −0.31 e Å−3 |
| (C12H12N2)(C12H11N2)[Mo(CN)8]·4H2O | V = 3151.8 (11) Å3 |
| Mr = 743.63 | Z = 4 |
| Orthorhombic, Ccca | Mo Kα radiation |
| a = 12.403 (3) Å | µ = 0.48 mm−1 |
| b = 16.534 (3) Å | T = 291 K |
| c = 15.370 (3) Å | 0.18 × 0.15 × 0.13 mm |
| Bruker SMART APEXII diffractometer | 1442 independent reflections |
| Absorption correction: multi-scan (SADABS; Bruker, 2004) | 1388 reflections with I > 2σ(I) |
| Tmin = 0.919, Tmax = 0.941 | Rint = 0.016 |
| 6789 measured reflections | θmax = 25.3° |
| R[F2 > 2σ(F2)] = 0.021 | H-atom parameters constrained |
| wR(F2) = 0.052 | Δρmax = 0.28 e Å−3 |
| S = 1.09 | Δρmin = −0.31 e Å−3 |
| 1442 reflections | Absolute structure: ? |
| 112 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
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. |
| x | y | z | Uiso*/Ueq | Occ. (<1) | |
| Mo1 | 0.0000 | 0.2500 | 0.2500 | 0.01026 (10) | |
| O1 | 0.65008 (10) | −0.07739 (7) | −0.07004 (7) | 0.0222 (3) | |
| H1A | 0.7081 | −0.0819 | −0.0991 | 0.033* | |
| H1B | 0.6515 | −0.1156 | −0.0330 | 0.033* | |
| N1 | −0.15776 (12) | 0.39926 (8) | 0.18061 (8) | 0.0217 (3) | |
| N2 | −0.12604 (11) | 0.18087 (8) | 0.07447 (9) | 0.0214 (3) | |
| N3 | 0.61502 (11) | 0.04861 (9) | 0.04165 (9) | 0.0222 (3) | |
| H3X | 0.6177 | 0.0114 | −0.0001 | 0.027* | 0.75 |
| C1 | −0.10315 (12) | 0.34816 (9) | 0.20714 (9) | 0.0153 (3) | |
| C2 | −0.08556 (13) | 0.20481 (9) | 0.13705 (10) | 0.0153 (3) | |
| C3 | 0.61146 (13) | 0.12818 (10) | 0.02559 (10) | 0.0226 (4) | |
| H3 | 0.6063 | 0.1466 | −0.0314 | 0.027* | |
| C4 | 0.61534 (13) | 0.18237 (10) | 0.09245 (10) | 0.0197 (3) | |
| H4 | 0.6125 | 0.2375 | 0.0809 | 0.024* | |
| C5 | 0.62366 (12) | 0.15508 (9) | 0.17825 (10) | 0.0171 (3) | |
| C6 | 0.62332 (13) | 0.07142 (10) | 0.19249 (11) | 0.0212 (4) | |
| H6 | 0.6258 | 0.0511 | 0.2489 | 0.025* | |
| C7 | 0.61929 (14) | 0.01956 (10) | 0.12305 (11) | 0.0239 (4) | |
| H7 | 0.6195 | −0.0360 | 0.1324 | 0.029* | |
| C8 | 0.62950 (13) | 0.20979 (10) | 0.25268 (10) | 0.0177 (3) | |
| H8 | 0.6335 | 0.1868 | 0.3078 | 0.021* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Mo1 | 0.01259 (15) | 0.00997 (14) | 0.00822 (14) | 0.000 | 0.000 | 0.000 |
| O1 | 0.0281 (6) | 0.0209 (6) | 0.0175 (6) | 0.0004 (5) | 0.0046 (5) | −0.0005 (5) |
| N1 | 0.0279 (8) | 0.0213 (7) | 0.0158 (7) | 0.0060 (6) | −0.0014 (6) | −0.0007 (6) |
| N2 | 0.0263 (8) | 0.0205 (7) | 0.0175 (7) | −0.0032 (6) | −0.0032 (6) | −0.0003 (6) |
| N3 | 0.0209 (7) | 0.0244 (8) | 0.0213 (7) | 0.0016 (6) | 0.0000 (6) | −0.0098 (6) |
| C1 | 0.0185 (8) | 0.0168 (8) | 0.0107 (7) | −0.0012 (6) | 0.0010 (6) | −0.0029 (6) |
| C2 | 0.0168 (8) | 0.0125 (8) | 0.0166 (8) | −0.0007 (6) | 0.0011 (7) | 0.0027 (6) |
| C3 | 0.0219 (8) | 0.0295 (10) | 0.0164 (8) | 0.0023 (7) | 0.0000 (7) | −0.0004 (7) |
| C4 | 0.0222 (8) | 0.0181 (8) | 0.0188 (8) | 0.0018 (6) | 0.0005 (7) | 0.0007 (6) |
| C5 | 0.0141 (7) | 0.0187 (8) | 0.0186 (8) | 0.0013 (6) | 0.0003 (6) | −0.0010 (6) |
| C6 | 0.0253 (9) | 0.0193 (8) | 0.0190 (8) | 0.0005 (7) | −0.0006 (7) | 0.0013 (6) |
| C7 | 0.0255 (9) | 0.0182 (9) | 0.0281 (9) | 0.0005 (7) | −0.0011 (8) | −0.0028 (7) |
| C8 | 0.0184 (8) | 0.0199 (8) | 0.0149 (8) | 0.0019 (7) | −0.0011 (6) | 0.0002 (6) |
| Mo1—C2 | 2.1674 (16) | N3—C7 | 1.341 (2) |
| Mo1—C2i | 2.1674 (16) | N3—H3X | 0.8896 |
| Mo1—C2ii | 2.1674 (16) | C3—C4 | 1.364 (2) |
| Mo1—C2iii | 2.1674 (16) | C3—H3 | 0.9300 |
| Mo1—C1i | 2.1690 (16) | C4—C5 | 1.398 (2) |
| Mo1—C1iii | 2.1690 (16) | C4—H4 | 0.9300 |
| Mo1—C1 | 2.1690 (16) | C5—C6 | 1.400 (2) |
| Mo1—C1ii | 2.1690 (16) | C5—C8 | 1.460 (2) |
| O1—H1A | 0.8501 | C6—C7 | 1.370 (2) |
| O1—H1B | 0.8505 | C6—H6 | 0.9300 |
| N1—C1 | 1.157 (2) | C7—H7 | 0.9300 |
| N2—C2 | 1.155 (2) | C8—C8i | 1.332 (3) |
| N3—C3 | 1.339 (2) | C8—H8 | 0.9300 |
| C2—Mo1—C2i | 121.37 (8) | C1iii—Mo1—C1ii | 107.72 (8) |
| C2—Mo1—C2ii | 73.57 (8) | C1—Mo1—C1ii | 144.64 (8) |
| C2i—Mo1—C2ii | 139.67 (8) | H1A—O1—H1B | 105.6 |
| C2—Mo1—C2iii | 139.67 (8) | C3—N3—C7 | 121.66 (14) |
| C2i—Mo1—C2iii | 73.57 (8) | C3—N3—H3X | 123.2 |
| C2ii—Mo1—C2iii | 121.37 (8) | C7—N3—H3X | 115.1 |
| C2—Mo1—C1i | 72.33 (5) | N1—C1—Mo1 | 177.01 (13) |
| C2i—Mo1—C1i | 74.09 (6) | N2—C2—Mo1 | 176.36 (14) |
| C2ii—Mo1—C1i | 142.18 (5) | N3—C3—C4 | 120.35 (15) |
| C2iii—Mo1—C1i | 77.74 (6) | N3—C3—H3 | 119.8 |
| C2—Mo1—C1iii | 142.18 (5) | C4—C3—H3 | 119.8 |
| C2i—Mo1—C1iii | 77.74 (6) | C3—C4—C5 | 120.08 (15) |
| C2ii—Mo1—C1iii | 72.33 (5) | C3—C4—H4 | 120.0 |
| C2iii—Mo1—C1iii | 74.09 (6) | C5—C4—H4 | 120.0 |
| C1i—Mo1—C1iii | 144.64 (8) | C4—C5—C6 | 117.78 (14) |
| C2—Mo1—C1 | 74.09 (6) | C4—C5—C8 | 122.88 (14) |
| C2i—Mo1—C1 | 72.33 (5) | C6—C5—C8 | 119.32 (14) |
| C2ii—Mo1—C1 | 77.74 (6) | C7—C6—C5 | 119.78 (15) |
| C2iii—Mo1—C1 | 142.18 (5) | C7—C6—H6 | 120.1 |
| C1i—Mo1—C1 | 107.72 (8) | C5—C6—H6 | 120.1 |
| C1iii—Mo1—C1 | 83.12 (8) | N3—C7—C6 | 120.27 (15) |
| C2—Mo1—C1ii | 77.74 (6) | N3—C7—H7 | 119.9 |
| C2i—Mo1—C1ii | 142.18 (5) | C6—C7—H7 | 119.9 |
| C2ii—Mo1—C1ii | 74.09 (6) | C8i—C8—C5 | 124.74 (18) |
| C2iii—Mo1—C1ii | 72.33 (5) | C8i—C8—H8 | 117.6 |
| C1i—Mo1—C1ii | 83.12 (8) | C5—C8—H8 | 117.6 |
| Symmetry codes: (i) x, −y+1/2, −z+1/2; (ii) −x, −y+1/2, z; (iii) −x, y, −z+1/2. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1A···N1iv | 0.85 | 2.11 | 2.9524 (19) | 174 |
| O1—H1B···N2v | 0.85 | 2.00 | 2.8195 (18) | 162 |
| N3—H3X···O1 | 0.89 | 1.86 | 2.7342 (17) | 166 |
| Symmetry codes: (iv) x+1, y−1/2, −z; (v) −x+1/2, −y, z. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O1—H1A···N1i | 0.85 | 2.11 | 2.9524 (19) | 173.9 |
| O1—H1B···N2ii | 0.85 | 2.00 | 2.8195 (18) | 162.0 |
| N3—H3X···O1 | 0.89 | 1.86 | 2.7342 (17) | 165.7 |
| Symmetry codes: (i) x+1, y−1/2, −z; (ii) −x+1/2, −y, z. |
Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany.
Bruker (2004). APEX2, SAINT and SADABS. Bruker AXS Inc., Madison,Wisconsin, USA.
Liu, W.-Y., Zhou, H. & Yuan, A.-H. (2008). Acta Cryst. E64, m1151.
Nowicka, B., Korzeniak, T., Stefańczyk, O., Pinkowicz, D., Chorąży, S., Podgajny, R. & Sieklucka, B. (2012). Coord. Chem. Rev. 256, 1946–1971.
Prins, F., Pasca, E., de Jongh, L. J., Kooijman, H., Spek, A. L. & Tanase, S. (2007). Angew. Chem. Int. Ed. 46, 6081–6084.
Qian, S.-Y., Liu, W.-Y. & Yuan, A.-H. (2009). Acta Cryst. E65, m1031–m1032.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Sieklucka, B., Podgajny, R., Korzeniak, T., Nowicka, B., Pinkowicz, D. & Kozieł, M. (2011). Eur. J. Inorg. Chem. pp. 305–326.
Tanase, S., de Jongh, L. J., Prins, F. & Evangelisti, M. (2008). ChemPhysChem, 9, 1975–1978.
Zhou, H.-C., Long, J. F. & Yaghi, O. M. (2012). Chem. Rev. 112, 673–674.
In the past few years, much attention has been put into the design and construction of multi-functional materials (Zhou et al., 2012). Octacyanometallates [M(CN)8]n- (M = Mo, W; n = 3, 4) with flexible coordination modes and lower symmetries have been aggressively studied recently (Nowicka et al., 2012), because these building blocks can adopt various geometries, e.g., square antiprismatic, dodecahedral or bicapped trigonal prismatic, depending on the external environments. The combination of the [M(CN)8]n- precusors and the second metal centers has produced various dimensional molecular structures and the resulting materials have displayed intriguing properties (Sieklucka et al., 2011). However, the development of octacyano- and lanthanide-based assemblies has been somewhat hampered by the tendency of the lanthanide ions to adopt higher coordination numbers, their ability to easily adapt to a given environment, and in the absence of design strategies for 4f-4d/5d networks. Recently, we used [MoV(CN)8]3- as building block to react with the lanthanide ion Ce3+ and dpe ligand (dpe = 1,2-di(pyridin-4-yl)ethylene), in order to obtain new octacyanide-based 4f/4 d compound with open structure. Unfortunately, a new ion-pair compound without Ce3+ ions was isolated. The asymmetric unit of the title compound contains 4,4'-ethene-1,2-diyldipyridinium, [H2dpe]2+, and 4-(2-(pyridin-4-yl)ethenyl)pyridinium, [Hdpe]+, cations, one [Mo(CN)8]3- anion, and four crystallized water molecules (Fig. 1). Both the [H2dpe]2+ and [Hdpe]+ cations are disordered over the same site. The eight-coordinated [Mo(CN)8] unit exhibits a distorted slightly square antiprismatic geometry, typical of octacyanometalates (Prins et al., 2007; Tanase et al., 2008). The average distances of Mo1—C and C—N bonds are 2.1682 and 1.156 Å, respectively, while the Mo1—CN bonds are almost linear with the maximum deviation from linearity of 3.8°.
In the structure, [H2dpe]2+ cation, [Hdpe]+ cation and [Mo(CN)8]3- unit are arranged alternatively through N3—H3X···O1 and O1—H1B···N2v (symmetric code: (v) -x + 1/2, -y, z) hydrogen bonds (Table 1) to generate a two-dimensional layer. These layers are further interlinked through O1—H1A···N1iv (symmetric code: (iv) x + 1, y - 1/2, -z) hydrogen bonds, forming a three-dimensional supramolecular network (Fig. 2). This structural feature has also been observed in related octacyanide-based compounds (C10H10N4)(C10H9N4)[M(CN)8].nH2O (M = Mo, W) (Qian et al., 2009; Liu et al., 2008).