Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102014026/ta1385sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S0108270102014026/ta1385Isup2.hkl |
Since K3[Fe(CN)6] has a tendency to decompose on heating and irradiation, the synthesis was performed at room temperature and crystallization in the dark. A solution of K3[Fe(CN)6] (65.8 mg, 0.2 mmol) in water (5 ml) was added to an aqueous solution (5 ml) of YCl3·6H2O (60.7 mg, 0.2 mmol) and caprolactam (90.4 mg, 0.8 mmol). The mixture was filtered and slowly evaporated to generate yellow single crystals of (I) (yield 30%).
The coordinates of the H atoms of the water molecules were found from difference Fourier maps and normalized to have an O—H distance of 0.85 Å. H atoms bound to C and N atoms were also visible in difference maps, and were placed using the HFIX commands in SHELXL97 (Sheldrick, 1997) and refined as riding atoms, with C—H distances of 0.96–0.97 Å and N—H distances of 0.86 Å. During the refinement, there was a high peak (2.0 e Å3) in the vicinity of C5 (1.2 Å), indicating the presence of a degree of disorder about the C atom. A treatment of disorder was applied, and the refinement gave occupancies for C5 and C5' of 0.82 and 0.18, respectively.
Cyano-bridged Prussian Blue complexes have been widely studied in the past. Recently, a growing trend in this field has been to prepare lanthanoid-transition-metal complexes because of their fascinating applications as catalysts (Amer & Alper, 1989) and semi-permeable solid membranes to desalinate seawater (Mullica & Sappenfield, 1991), as well as precursors of electroceramic materials (Sadaoka et al., 1996), and chemical sensor materials and oxide fuel cells (Minh, 1993). The most attractive property of lanthanoid-transition-metal complexes is their magnetism. A series of cyano-bridged three-dimensional lanthanoid hexacyanometallates, [LnM(CN)6].nH2O (M is FeIII or CrIII, n = 4 or 5), were synthesized and ferrimagnetic ordering was observed in 1976 (Hulliger & Landolt, 1976). Very recently, many analogous Prussian Blue 4f-3 d complexes with interesting zero- and three-dimensional structures have been synthesized by incorporating betaine (Yan et al., 2001), 2,2'-bipyrimidine (Ma et al., 2001), 2,2'-dipyridyl-N,N'-dioxide (Gao et al., 1999), dimethylformamide (Kou et al., 1998; Kou, Gao & Jin, 2001; Kou, Gao, Sun & Zhang, 2001; Combs et al., 2000; Figuerola et al., 2001), dimethylsulfoxide (Yang et al., 2001), urea (Kou, Gao, Li et al., 2002) and pyrrolidone (Kou, Gao & Wang, 2002; Sun et al., 2002) as organic ligands.
Caprolactam (capro) has been shown to act as a useful ligand in the construction of 4f-3 d complexes, for example, one-dimensional [Ga(capro)2(H2O)4Cr(CN)6]·H2O Should the first metal be Gd not Ga? (Kou, Gao, Li et al., 2002). Bearing in mind that the introduction of larger numbers of ligands always leads to lower-dimensional complexes, we tried to prepare an Y-capro-Fe complex with a molar ratio for Y:capro of 1:4. Unexpectedly, however, we obtained the title cyano-bridged bimetallic dimeric complex, (I). \sch
As shown in Fig. 1, the Y atom in (I) is seven-coordinate with approximately pentagonal-bipyramidal stereochemistry, with water molecules O3 and O3i [symmetry code: (i) -x, y, 1/2 - z] defining the apical positions. Of the five ligands in the equatorial positions, one is the N-bound µ-CN, and flanking this are two O-bound caprolactam moieties, which are markedly inclined towards the bridged ferricyanide moiety such that they partially envelop it. Water molecules occupy the other two equatorial positions. The two monodentate caprolactam molecules are in cis positions, with O1—Y—O1i 159.24 (10)°. The Y—N4—C4—Fe—C1—N1 sequence of atoms lies on a crystallographic twofold axis. To our knowledge, this perfectly linear cyano-bridging linkage has never previously been observed in other cyano-bridged complexes.
The Y—Owater bond lengths (Y—O2, Y—O3) are a little longer than that of Y—Ocapro (Y—O1) (Table 1). The Y—N4 bond length is a little shorter than that of the Gd—N bonds in [Ga(capro)2(H2O)4Cr(CN)6]·H2O Should the first metal be Gd not Ga? (2.505 and 2.501 Å; Kou, Gao, Li et al., 2002), which may be due to the difference in the radii of the two lanthanoid ions.
The geometry of the [Fe(CN)6]3- ion is approximately octahedral, with Fe—C bond distances in the range 1.930 (3)–1.937 (3) Å and C—Fe—C angles in the range 89.09 (8)–90.91 (8)°. The average C≡N bond length of 1.143 Å is in accord with the sum of the triple-bond radii of C and N atoms (0.603 and 0.55 Å, respectively; Reference?). The Fe—C—N bonds are almost linear and range from 178.1 (3) to 180.0° Please clarify - only two values in the CIF, the second of which is 179.2 (2)°.
Data collection: SMART (Bruker, 2000); cell refinement: SMART; data reduction: SAINT (Bruker, 2000); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2002); software used to prepare material for publication: SHELXL97.
Fig. 1. A view of (I) with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level. The suffix A denotes atoms at (?) Please provide missing symmetry code. |
[FeY(C6H11NO)2(CN)6(H2O)4] | F(000) = 1228 |
Mr = 599.26 | Dx = 1.508 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 4518 reflections |
a = 14.006 (3) Å | θ = 2.4–32.0° |
b = 12.951 (3) Å | µ = 2.78 mm−1 |
c = 15.011 (3) Å | T = 293 K |
β = 104.15 (3)° | Block, yellow |
V = 2640.3 (10) Å3 | 0.30 × 0.26 × 0.18 mm |
Z = 4 |
Make Model CCD area-detector diffractometer | 4853 independent reflections |
Radiation source: fine-focus sealed tube | 3691 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.038 |
Detector resolution: 15 × 15 microns pixels mm-1 | θmax = 33.5°, θmin = 2.2° |
φ and ω scans | h = −19→20 |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | k = −16→19 |
Tmin = 0.445, Tmax = 0.606 | l = −22→13 |
12364 measured reflections |
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)] = 0.044 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.087 | H-atom parameters constrained |
S = 1.06 | w = 1/[σ2(Fo2) + (0.0132P)2 + 5.7178P] where P = (Fo2 + 2Fc2)/3 |
4853 reflections | (Δ/σ)max = 0.002 |
161 parameters | Δρmax = 0.81 e Å−3 |
4 restraints | Δρmin = −0.55 e Å−3 |
[FeY(C6H11NO)2(CN)6(H2O)4] | V = 2640.3 (10) Å3 |
Mr = 599.26 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 14.006 (3) Å | µ = 2.78 mm−1 |
b = 12.951 (3) Å | T = 293 K |
c = 15.011 (3) Å | 0.30 × 0.26 × 0.18 mm |
β = 104.15 (3)° |
Make Model CCD area-detector diffractometer | 4853 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2000) | 3691 reflections with I > 2σ(I) |
Tmin = 0.445, Tmax = 0.606 | Rint = 0.038 |
12364 measured reflections |
R[F2 > 2σ(F2)] = 0.044 | 4 restraints |
wR(F2) = 0.087 | H-atom parameters constrained |
S = 1.06 | Δρmax = 0.81 e Å−3 |
4853 reflections | Δρmin = −0.55 e Å−3 |
161 parameters |
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) | |
Y | 0.0000 | 0.77158 (2) | 0.2500 | 0.02047 (8) | |
Fe | 0.0000 | 1.19406 (3) | 0.2500 | 0.01897 (10) | |
O1 | 0.12658 (14) | 0.80234 (15) | 0.36757 (14) | 0.0413 (5) | |
O2 | 0.09388 (15) | 0.62302 (15) | 0.24751 (18) | 0.0571 (7) | |
H21 | 0.1527 | 0.6183 | 0.2419 | 0.069* | |
H20 | 0.0822 | 0.5597 | 0.2553 | 0.069* | |
O3 | −0.09493 (15) | 0.80271 (17) | 0.35407 (14) | 0.0463 (5) | |
H30 | −0.1511 | 0.7738 | 0.3407 | 0.056* | |
H31 | −0.0658 | 0.8119 | 0.4103 | 0.056* | |
N1 | 0.0000 | 1.4318 (2) | 0.2500 | 0.0479 (9) | |
N2 | 0.0225 (2) | 1.1874 (2) | 0.45933 (18) | 0.0539 (7) | |
N3 | 0.22582 (18) | 1.1919 (2) | 0.2837 (2) | 0.0479 (6) | |
N4 | 0.0000 | 0.9570 (2) | 0.2500 | 0.0425 (8) | |
N5 | 0.1558 (2) | 0.9120 (2) | 0.4853 (2) | 0.0605 (8) | |
H5A | 0.0943 | 0.9075 | 0.4840 | 0.073* | |
C1 | 0.0000 | 1.3433 (3) | 0.2500 | 0.0306 (7) | |
C2 | 0.01371 (18) | 1.1917 (2) | 0.38158 (19) | 0.0314 (5) | |
C3 | 0.14200 (18) | 1.19343 (18) | 0.27128 (18) | 0.0285 (5) | |
C4 | 0.0000 | 1.0450 (3) | 0.2500 | 0.0295 (7) | |
C5 | 0.2920 (3) | 0.8568 (3) | 0.4244 (3) | 0.0507 (13) | 0.824 (10) |
H5B | 0.3263 | 0.8257 | 0.4813 | 0.061* | 0.824 (10) |
H5C | 0.3006 | 0.8128 | 0.3755 | 0.061* | 0.824 (10) |
C5' | 0.2475 (9) | 0.9120 (14) | 0.3679 (8) | 0.0507 (13) | 0.176 (10) |
H5'A | 0.2660 | 0.8580 | 0.3316 | 0.061* | 0.176 (10) |
H5'B | 0.2093 | 0.9609 | 0.3258 | 0.061* | 0.176 (10) |
C6 | 0.3386 (3) | 0.9559 (4) | 0.4163 (4) | 0.0925 (16) | |
H6A | 0.3594 | 0.9929 | 0.3690 | 0.111* | 0.176 (10) |
H6B | 0.3855 | 0.9012 | 0.4346 | 0.111* | 0.176 (10) |
H6C | 0.2956 | 0.9922 | 0.3655 | 0.111* | 0.824 (10) |
H6D | 0.3999 | 0.9430 | 0.3991 | 0.111* | 0.824 (10) |
C7 | 0.3590 (3) | 1.0280 (3) | 0.4956 (3) | 0.0793 (13) | |
H7A | 0.3888 | 1.0900 | 0.4781 | 0.095* | |
H7B | 0.4070 | 0.9961 | 0.5457 | 0.095* | |
C8 | 0.2714 (4) | 1.0590 (4) | 0.5303 (4) | 0.0952 (17) | |
H8A | 0.2940 | 1.1043 | 0.5827 | 0.114* | |
H8B | 0.2275 | 1.0989 | 0.4827 | 0.114* | |
C9 | 0.2150 (3) | 0.9768 (4) | 0.5574 (3) | 0.0839 (14) | |
H9A | 0.1714 | 1.0073 | 0.5913 | 0.101* | |
H9B | 0.2604 | 0.9323 | 0.5997 | 0.101* | |
C10 | 0.1851 (2) | 0.8600 (2) | 0.4224 (2) | 0.0444 (7) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Y | 0.02200 (14) | 0.01577 (14) | 0.02371 (15) | 0.000 | 0.00572 (11) | 0.000 |
Fe | 0.0189 (2) | 0.0149 (2) | 0.0240 (2) | 0.000 | 0.00688 (17) | 0.000 |
O1 | 0.0365 (11) | 0.0409 (11) | 0.0392 (11) | −0.0055 (8) | −0.0044 (9) | −0.0054 (8) |
O2 | 0.0365 (11) | 0.0215 (9) | 0.124 (2) | 0.0016 (8) | 0.0396 (13) | −0.0001 (11) |
O3 | 0.0361 (11) | 0.0717 (15) | 0.0348 (11) | −0.0177 (10) | 0.0158 (9) | −0.0194 (10) |
N1 | 0.061 (2) | 0.0219 (16) | 0.062 (3) | 0.000 | 0.0188 (19) | 0.000 |
N2 | 0.0506 (16) | 0.082 (2) | 0.0309 (13) | −0.0053 (14) | 0.0141 (12) | −0.0024 (13) |
N3 | 0.0271 (12) | 0.0602 (16) | 0.0576 (17) | 0.0007 (11) | 0.0127 (11) | 0.0081 (13) |
N4 | 0.053 (2) | 0.0181 (14) | 0.056 (2) | 0.000 | 0.0123 (17) | 0.000 |
N5 | 0.0412 (15) | 0.082 (2) | 0.0624 (19) | −0.0184 (14) | 0.0215 (13) | −0.0323 (16) |
C1 | 0.0330 (18) | 0.0220 (16) | 0.039 (2) | 0.000 | 0.0126 (15) | 0.000 |
C2 | 0.0266 (12) | 0.0360 (13) | 0.0327 (14) | −0.0019 (10) | 0.0092 (10) | −0.0021 (11) |
C3 | 0.0260 (12) | 0.0266 (11) | 0.0338 (13) | −0.0014 (9) | 0.0094 (10) | 0.0017 (10) |
C4 | 0.0320 (18) | 0.0219 (15) | 0.0346 (19) | 0.000 | 0.0079 (14) | 0.000 |
C5 | 0.037 (2) | 0.055 (3) | 0.061 (3) | −0.0021 (16) | 0.0136 (18) | −0.0164 (19) |
C5' | 0.037 (2) | 0.055 (3) | 0.061 (3) | −0.0021 (16) | 0.0136 (18) | −0.0164 (19) |
C6 | 0.075 (3) | 0.104 (4) | 0.117 (4) | −0.036 (3) | 0.058 (3) | −0.033 (3) |
C7 | 0.058 (2) | 0.070 (3) | 0.111 (4) | −0.028 (2) | 0.022 (2) | −0.025 (3) |
C8 | 0.085 (3) | 0.083 (3) | 0.120 (4) | −0.021 (3) | 0.028 (3) | −0.055 (3) |
C9 | 0.087 (3) | 0.103 (3) | 0.071 (3) | −0.028 (3) | 0.038 (2) | −0.052 (3) |
C10 | 0.0351 (15) | 0.0492 (18) | 0.0472 (18) | −0.0095 (12) | 0.0069 (13) | −0.0121 (14) |
Y—O1i | 2.211 (2) | N5—C9 | 1.458 (4) |
Y—O1 | 2.211 (2) | N5—H5A | 0.8600 |
Y—O2 | 2.3359 (19) | C5—C6 | 1.458 (5) |
Y—O3 | 2.321 (2) | C5—C10 | 1.491 (4) |
Y—O3i | 2.321 (2) | C5—H5B | 0.9600 |
Y—O2i | 2.3359 (19) | C5—H5C | 0.9599 |
Y—N4 | 2.401 (3) | C5'—C6 | 1.422 (9) |
Fe—C1 | 1.933 (3) | C5'—C10 | 1.496 (9) |
Fe—C2 | 1.937 (3) | C5'—H5'A | 0.9599 |
Fe—C3i | 1.936 (2) | C5'—H5'B | 0.9600 |
Fe—C3 | 1.936 (2) | C6—C7 | 1.484 (6) |
Fe—C4 | 1.930 (3) | C6—H6A | 0.9600 |
Fe—C2i | 1.937 (3) | C6—H6B | 0.9600 |
O1—C10 | 1.256 (3) | C6—H6C | 0.9700 |
O2—H21 | 0.8500 | C6—H6D | 0.9700 |
O2—H20 | 0.8499 | C7—C8 | 1.501 (6) |
O3—H30 | 0.8495 | C7—H7A | 0.9700 |
O3—H31 | 0.8512 | C7—H7B | 0.9700 |
N1—C1 | 1.146 (4) | C8—C9 | 1.442 (6) |
N2—C2 | 1.145 (4) | C8—H8A | 0.9700 |
N3—C3 | 1.143 (3) | C8—H8B | 0.9700 |
N4—C4 | 1.140 (5) | C9—H9A | 0.9700 |
N5—C10 | 1.304 (4) | C9—H9B | 0.9700 |
O1i—Y—O1 | 159.24 (10) | C6—C5—C10 | 116.2 (3) |
O1i—Y—O3 | 91.52 (8) | C6—C5—H5B | 107.9 |
O1—Y—O2 | 79.43 (8) | C10—C5—H5B | 108.1 |
O1—Y—O3 | 84.89 (8) | C6—C5—H5C | 108.4 |
O3—Y—O2 | 124.84 (8) | C10—C5—H5C | 108.3 |
O1—Y—O2i | 118.71 (8) | H5B—C5—H5C | 107.6 |
O1—Y—O3i | 91.52 (8) | C6—C5'—C10 | 118.1 (8) |
O3—Y—O2i | 73.44 (8) | C6—C5'—H5'A | 104.4 |
O2i—Y—O2 | 69.09 (10) | C10—C5'—H5'A | 104.9 |
O3i—Y—O3 | 159.99 (11) | C6—C5'—H5'B | 111.0 |
O1i—Y—O2 | 118.71 (8) | C10—C5'—H5'B | 110.5 |
O3i—Y—O2 | 73.44 (8) | H5'A—C5'—H5'B | 106.9 |
O1i—Y—O3i | 84.89 (8) | C5'—C6—C7 | 129.4 (8) |
O1i—Y—O2i | 79.43 (8) | C5—C6—C7 | 119.3 (4) |
O3i—Y—O2i | 124.84 (8) | C5'—C6—H6A | 102.6 |
O1i—Y—N4 | 79.62 (5) | C7—C6—H6A | 104.2 |
O1—Y—N4 | 79.62 (5) | C5'—C6—H6B | 108.5 |
O2—Y—N4 | 145.46 (5) | C7—C6—H6B | 104.5 |
O3—Y—N4 | 80.00 (5) | H6A—C6—H6B | 105.6 |
O3i—Y—N4 | 80.00 (5) | C5—C6—H6C | 106.7 |
O2i—Y—N4 | 145.46 (5) | C7—C6—H6C | 106.7 |
C1—Fe—C2 | 90.91 (8) | C5—C6—H6D | 108.3 |
C1—Fe—C3 | 90.24 (7) | C7—C6—H6D | 108.2 |
C3—Fe—C2 | 89.43 (11) | H6C—C6—H6D | 107.0 |
C4—Fe—C2 | 89.09 (8) | C6—C7—C8 | 115.6 (3) |
C4—Fe—C3 | 89.76 (7) | C6—C7—H7A | 108.4 |
C2i—Fe—C2 | 178.17 (16) | C8—C7—H7A | 108.4 |
C3i—Fe—C3 | 179.52 (14) | C6—C7—H7B | 108.4 |
C4—Fe—C3i | 89.76 (7) | C8—C7—H7B | 108.4 |
C1—Fe—C3i | 90.24 (7) | H7A—C7—H7B | 107.4 |
C4—Fe—C2i | 89.09 (8) | C9—C8—C7 | 116.8 (4) |
C1—Fe—C2i | 90.91 (8) | C9—C8—H8A | 108.1 |
C3i—Fe—C2i | 89.43 (11) | C7—C8—H8A | 108.1 |
C3—Fe—C2i | 90.57 (11) | C9—C8—H8B | 108.1 |
C3i—Fe—C2 | 90.57 (11) | C7—C8—H8B | 108.1 |
C10—O1—Y | 153.9 (2) | H8A—C8—H8B | 107.3 |
Y—O2—H21 | 128.5 | C8—C9—N5 | 117.8 (4) |
Y—O2—H20 | 131.6 | C8—C9—H9A | 107.9 |
H21—O2—H20 | 99.7 | N5—C9—H9A | 107.9 |
Y—O3—H30 | 114.5 | C8—C9—H9B | 107.9 |
Y—O3—H31 | 118.5 | N5—C9—H9B | 107.9 |
H30—O3—H31 | 119.1 | H9A—C9—H9B | 107.2 |
C10—N5—C9 | 127.8 (3) | O1—C10—N5 | 120.8 (3) |
C10—N5—H5A | 116.1 | O1—C10—C5 | 119.2 (3) |
C9—N5—H5A | 116.1 | N5—C10—C5 | 119.4 (3) |
N2—C2—Fe | 178.1 (3) | O1—C10—C5' | 106.5 (5) |
N3—C3—Fe | 179.2 (2) | N5—C10—C5' | 119.5 (7) |
Symmetry code: (i) −x, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H21···N3ii | 0.85 | 2.07 | 2.823 (3) | 148 |
O2—H20···N1iii | 0.85 | 2.01 | 2.809 (3) | 157 |
O3—H30···N3iv | 0.85 | 2.03 | 2.861 (3) | 167 |
O3—H31···N2v | 0.85 | 1.90 | 2.739 (3) | 168 |
N5—H5A···N2v | 0.86 | 2.36 | 3.098 (4) | 144 |
Symmetry codes: (ii) −x+1/2, y−1/2, −z+1/2; (iii) x, y−1, z; (iv) x−1/2, y−1/2, z; (v) −x, −y+2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | [FeY(C6H11NO)2(CN)6(H2O)4] |
Mr | 599.26 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 293 |
a, b, c (Å) | 14.006 (3), 12.951 (3), 15.011 (3) |
β (°) | 104.15 (3) |
V (Å3) | 2640.3 (10) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 2.78 |
Crystal size (mm) | 0.30 × 0.26 × 0.18 |
Data collection | |
Diffractometer | Make Model CCD area-detector |
Absorption correction | Multi-scan (SADABS; Bruker, 2000) |
Tmin, Tmax | 0.445, 0.606 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 12364, 4853, 3691 |
Rint | 0.038 |
(sin θ/λ)max (Å−1) | 0.776 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.044, 0.087, 1.06 |
No. of reflections | 4853 |
No. of parameters | 161 |
No. of restraints | 4 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.81, −0.55 |
Computer programs: SMART (Bruker, 2000), SMART, SAINT (Bruker, 2000), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2002), SHELXL97.
Y—O1 | 2.211 (2) | Fe—C3 | 1.936 (2) |
Y—O2 | 2.3359 (19) | Fe—C4 | 1.930 (3) |
Y—O3 | 2.321 (2) | N1—C1 | 1.146 (4) |
Y—N4 | 2.401 (3) | N2—C2 | 1.145 (4) |
Fe—C1 | 1.933 (3) | N3—C3 | 1.143 (3) |
Fe—C2 | 1.937 (3) | N4—C4 | 1.140 (5) |
O1i—Y—O1 | 159.24 (10) | O3—Y—N4 | 80.00 (5) |
O1—Y—O2 | 79.43 (8) | C1—Fe—C2 | 90.91 (8) |
O1—Y—O3 | 84.89 (8) | C1—Fe—C3 | 90.24 (7) |
O3—Y—O2 | 124.84 (8) | C3—Fe—C2 | 89.43 (11) |
O1—Y—O2i | 118.71 (8) | C4—Fe—C2 | 89.09 (8) |
O1—Y—O3i | 91.52 (8) | C4—Fe—C3 | 89.76 (7) |
O3—Y—O2i | 73.44 (8) | C2i—Fe—C2 | 178.17 (16) |
O2i—Y—O2 | 69.09 (10) | C3i—Fe—C3 | 179.52 (14) |
O3i—Y—O3 | 159.99 (11) | C10—O1—Y | 153.9 (2) |
O1—Y—N4 | 79.62 (5) | N2—C2—Fe | 178.1 (3) |
O2—Y—N4 | 145.46 (5) | N3—C3—Fe | 179.2 (2) |
Symmetry code: (i) −x, y, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O2—H21···N3ii | 0.85 | 2.07 | 2.823 (3) | 148 |
O2—H20···N1iii | 0.85 | 2.01 | 2.809 (3) | 157 |
O3—H30···N3iv | 0.85 | 2.03 | 2.861 (3) | 167 |
O3—H31···N2v | 0.85 | 1.90 | 2.739 (3) | 168 |
N5—H5A···N2v | 0.86 | 2.36 | 3.098 (4) | 144 |
Symmetry codes: (ii) −x+1/2, y−1/2, −z+1/2; (iii) x, y−1, z; (iv) x−1/2, y−1/2, z; (v) −x, −y+2, −z+1. |
Cyano-bridged Prussian Blue complexes have been widely studied in the past. Recently, a growing trend in this field has been to prepare lanthanoid-transition-metal complexes because of their fascinating applications as catalysts (Amer & Alper, 1989) and semi-permeable solid membranes to desalinate seawater (Mullica & Sappenfield, 1991), as well as precursors of electroceramic materials (Sadaoka et al., 1996), and chemical sensor materials and oxide fuel cells (Minh, 1993). The most attractive property of lanthanoid-transition-metal complexes is their magnetism. A series of cyano-bridged three-dimensional lanthanoid hexacyanometallates, [LnM(CN)6].nH2O (M is FeIII or CrIII, n = 4 or 5), were synthesized and ferrimagnetic ordering was observed in 1976 (Hulliger & Landolt, 1976). Very recently, many analogous Prussian Blue 4f-3 d complexes with interesting zero- and three-dimensional structures have been synthesized by incorporating betaine (Yan et al., 2001), 2,2'-bipyrimidine (Ma et al., 2001), 2,2'-dipyridyl-N,N'-dioxide (Gao et al., 1999), dimethylformamide (Kou et al., 1998; Kou, Gao & Jin, 2001; Kou, Gao, Sun & Zhang, 2001; Combs et al., 2000; Figuerola et al., 2001), dimethylsulfoxide (Yang et al., 2001), urea (Kou, Gao, Li et al., 2002) and pyrrolidone (Kou, Gao & Wang, 2002; Sun et al., 2002) as organic ligands.
Caprolactam (capro) has been shown to act as a useful ligand in the construction of 4f-3 d complexes, for example, one-dimensional [Ga(capro)2(H2O)4Cr(CN)6]·H2O Should the first metal be Gd not Ga? (Kou, Gao, Li et al., 2002). Bearing in mind that the introduction of larger numbers of ligands always leads to lower-dimensional complexes, we tried to prepare an Y-capro-Fe complex with a molar ratio for Y:capro of 1:4. Unexpectedly, however, we obtained the title cyano-bridged bimetallic dimeric complex, (I). \sch
As shown in Fig. 1, the Y atom in (I) is seven-coordinate with approximately pentagonal-bipyramidal stereochemistry, with water molecules O3 and O3i [symmetry code: (i) -x, y, 1/2 - z] defining the apical positions. Of the five ligands in the equatorial positions, one is the N-bound µ-CN, and flanking this are two O-bound caprolactam moieties, which are markedly inclined towards the bridged ferricyanide moiety such that they partially envelop it. Water molecules occupy the other two equatorial positions. The two monodentate caprolactam molecules are in cis positions, with O1—Y—O1i 159.24 (10)°. The Y—N4—C4—Fe—C1—N1 sequence of atoms lies on a crystallographic twofold axis. To our knowledge, this perfectly linear cyano-bridging linkage has never previously been observed in other cyano-bridged complexes.
The Y—Owater bond lengths (Y—O2, Y—O3) are a little longer than that of Y—Ocapro (Y—O1) (Table 1). The Y—N4 bond length is a little shorter than that of the Gd—N bonds in [Ga(capro)2(H2O)4Cr(CN)6]·H2O Should the first metal be Gd not Ga? (2.505 and 2.501 Å; Kou, Gao, Li et al., 2002), which may be due to the difference in the radii of the two lanthanoid ions.
The geometry of the [Fe(CN)6]3- ion is approximately octahedral, with Fe—C bond distances in the range 1.930 (3)–1.937 (3) Å and C—Fe—C angles in the range 89.09 (8)–90.91 (8)°. The average C≡N bond length of 1.143 Å is in accord with the sum of the triple-bond radii of C and N atoms (0.603 and 0.55 Å, respectively; Reference?). The Fe—C—N bonds are almost linear and range from 178.1 (3) to 180.0° Please clarify - only two values in the CIF, the second of which is 179.2 (2)°.