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Using caprolactam as a ligand, the novel title cyano-bridged yttrium(III)-ferricyanide complex, [Y(caprolactam)2(H2O)4Fe(CN)6] or [FeY(CN)6(C6H11NO)2(H2O)4], has been synthesized and structurally characterized. The Y atom is seven-coordinate and has approximately pentagonal-bipyramidal stereochemistry, with water mol­ecules occupying apical positions. Of the five ligands in equatorial positions, one is the N-bound bridging cyano group, 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 remaining two equatorial positions. The Y-N-C-Fe-C-N sequence of atoms lies on a crystallographic twofold axis and is therefore perfectly linear, which has not been observed previously in cyano-bridged bimetallic complexes.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102014026/ta1385sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102014026/ta1385Isup2.hkl
Contains datablock I

Comment top

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 CN 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)°.

Experimental top

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%).

Refinement top

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.

Structure description top

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 CN 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)°.

Computing details top

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.

Figures top
[Figure 1] 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.
Tetraaqua-1κ4O-bis(ε-caprolactam-1κO)-µ-cyano-1:2κ2N:C-pentacyano- 2κ5C-iron(III)yttrium(III) top
Crystal data top
[FeY(C6H11NO)2(CN)6(H2O)4]F(000) = 1228
Mr = 599.26Dx = 1.508 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 4518 reflections
a = 14.006 (3) Åθ = 2.4–32.0°
b = 12.951 (3) ŵ = 2.78 mm1
c = 15.011 (3) ÅT = 293 K
β = 104.15 (3)°Block, yellow
V = 2640.3 (10) Å30.30 × 0.26 × 0.18 mm
Z = 4
Data collection top
Make Model CCD area-detector
diffractometer
4853 independent reflections
Radiation source: fine-focus sealed tube3691 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
Detector resolution: 15 × 15 microns pixels mm-1θmax = 33.5°, θmin = 2.2°
φ and ω scansh = 1920
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
k = 1619
Tmin = 0.445, Tmax = 0.606l = 2213
12364 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.087H-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 parametersΔρmax = 0.81 e Å3
4 restraintsΔρmin = 0.55 e Å3
Crystal data top
[FeY(C6H11NO)2(CN)6(H2O)4]V = 2640.3 (10) Å3
Mr = 599.26Z = 4
Monoclinic, C2/cMo Kα radiation
a = 14.006 (3) ŵ = 2.78 mm1
b = 12.951 (3) ÅT = 293 K
c = 15.011 (3) Å0.30 × 0.26 × 0.18 mm
β = 104.15 (3)°
Data collection top
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 = 0.606Rint = 0.038
12364 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0444 restraints
wR(F2) = 0.087H-atom parameters constrained
S = 1.06Δρmax = 0.81 e Å3
4853 reflectionsΔρmin = 0.55 e Å3
161 parameters
Special details top

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) top
xyzUiso*/UeqOcc. (<1)
Y0.00000.77158 (2)0.25000.02047 (8)
Fe0.00001.19406 (3)0.25000.01897 (10)
O10.12658 (14)0.80234 (15)0.36757 (14)0.0413 (5)
O20.09388 (15)0.62302 (15)0.24751 (18)0.0571 (7)
H210.15270.61830.24190.069*
H200.08220.55970.25530.069*
O30.09493 (15)0.80271 (17)0.35407 (14)0.0463 (5)
H300.15110.77380.34070.056*
H310.06580.81190.41030.056*
N10.00001.4318 (2)0.25000.0479 (9)
N20.0225 (2)1.1874 (2)0.45933 (18)0.0539 (7)
N30.22582 (18)1.1919 (2)0.2837 (2)0.0479 (6)
N40.00000.9570 (2)0.25000.0425 (8)
N50.1558 (2)0.9120 (2)0.4853 (2)0.0605 (8)
H5A0.09430.90750.48400.073*
C10.00001.3433 (3)0.25000.0306 (7)
C20.01371 (18)1.1917 (2)0.38158 (19)0.0314 (5)
C30.14200 (18)1.19343 (18)0.27128 (18)0.0285 (5)
C40.00001.0450 (3)0.25000.0295 (7)
C50.2920 (3)0.8568 (3)0.4244 (3)0.0507 (13)0.824 (10)
H5B0.32630.82570.48130.061*0.824 (10)
H5C0.30060.81280.37550.061*0.824 (10)
C5'0.2475 (9)0.9120 (14)0.3679 (8)0.0507 (13)0.176 (10)
H5'A0.26600.85800.33160.061*0.176 (10)
H5'B0.20930.96090.32580.061*0.176 (10)
C60.3386 (3)0.9559 (4)0.4163 (4)0.0925 (16)
H6A0.35940.99290.36900.111*0.176 (10)
H6B0.38550.90120.43460.111*0.176 (10)
H6C0.29560.99220.36550.111*0.824 (10)
H6D0.39990.94300.39910.111*0.824 (10)
C70.3590 (3)1.0280 (3)0.4956 (3)0.0793 (13)
H7A0.38881.09000.47810.095*
H7B0.40700.99610.54570.095*
C80.2714 (4)1.0590 (4)0.5303 (4)0.0952 (17)
H8A0.29401.10430.58270.114*
H8B0.22751.09890.48270.114*
C90.2150 (3)0.9768 (4)0.5574 (3)0.0839 (14)
H9A0.17141.00730.59130.101*
H9B0.26040.93230.59970.101*
C100.1851 (2)0.8600 (2)0.4224 (2)0.0444 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Y0.02200 (14)0.01577 (14)0.02371 (15)0.0000.00572 (11)0.000
Fe0.0189 (2)0.0149 (2)0.0240 (2)0.0000.00688 (17)0.000
O10.0365 (11)0.0409 (11)0.0392 (11)0.0055 (8)0.0044 (9)0.0054 (8)
O20.0365 (11)0.0215 (9)0.124 (2)0.0016 (8)0.0396 (13)0.0001 (11)
O30.0361 (11)0.0717 (15)0.0348 (11)0.0177 (10)0.0158 (9)0.0194 (10)
N10.061 (2)0.0219 (16)0.062 (3)0.0000.0188 (19)0.000
N20.0506 (16)0.082 (2)0.0309 (13)0.0053 (14)0.0141 (12)0.0024 (13)
N30.0271 (12)0.0602 (16)0.0576 (17)0.0007 (11)0.0127 (11)0.0081 (13)
N40.053 (2)0.0181 (14)0.056 (2)0.0000.0123 (17)0.000
N50.0412 (15)0.082 (2)0.0624 (19)0.0184 (14)0.0215 (13)0.0323 (16)
C10.0330 (18)0.0220 (16)0.039 (2)0.0000.0126 (15)0.000
C20.0266 (12)0.0360 (13)0.0327 (14)0.0019 (10)0.0092 (10)0.0021 (11)
C30.0260 (12)0.0266 (11)0.0338 (13)0.0014 (9)0.0094 (10)0.0017 (10)
C40.0320 (18)0.0219 (15)0.0346 (19)0.0000.0079 (14)0.000
C50.037 (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)
C60.075 (3)0.104 (4)0.117 (4)0.036 (3)0.058 (3)0.033 (3)
C70.058 (2)0.070 (3)0.111 (4)0.028 (2)0.022 (2)0.025 (3)
C80.085 (3)0.083 (3)0.120 (4)0.021 (3)0.028 (3)0.055 (3)
C90.087 (3)0.103 (3)0.071 (3)0.028 (3)0.038 (2)0.052 (3)
C100.0351 (15)0.0492 (18)0.0472 (18)0.0095 (12)0.0069 (13)0.0121 (14)
Geometric parameters (Å, º) top
Y—O1i2.211 (2)N5—C91.458 (4)
Y—O12.211 (2)N5—H5A0.8600
Y—O22.3359 (19)C5—C61.458 (5)
Y—O32.321 (2)C5—C101.491 (4)
Y—O3i2.321 (2)C5—H5B0.9600
Y—O2i2.3359 (19)C5—H5C0.9599
Y—N42.401 (3)C5'—C61.422 (9)
Fe—C11.933 (3)C5'—C101.496 (9)
Fe—C21.937 (3)C5'—H5'A0.9599
Fe—C3i1.936 (2)C5'—H5'B0.9600
Fe—C31.936 (2)C6—C71.484 (6)
Fe—C41.930 (3)C6—H6A0.9600
Fe—C2i1.937 (3)C6—H6B0.9600
O1—C101.256 (3)C6—H6C0.9700
O2—H210.8500C6—H6D0.9700
O2—H200.8499C7—C81.501 (6)
O3—H300.8495C7—H7A0.9700
O3—H310.8512C7—H7B0.9700
N1—C11.146 (4)C8—C91.442 (6)
N2—C21.145 (4)C8—H8A0.9700
N3—C31.143 (3)C8—H8B0.9700
N4—C41.140 (5)C9—H9A0.9700
N5—C101.304 (4)C9—H9B0.9700
O1i—Y—O1159.24 (10)C6—C5—C10116.2 (3)
O1i—Y—O391.52 (8)C6—C5—H5B107.9
O1—Y—O279.43 (8)C10—C5—H5B108.1
O1—Y—O384.89 (8)C6—C5—H5C108.4
O3—Y—O2124.84 (8)C10—C5—H5C108.3
O1—Y—O2i118.71 (8)H5B—C5—H5C107.6
O1—Y—O3i91.52 (8)C6—C5'—C10118.1 (8)
O3—Y—O2i73.44 (8)C6—C5'—H5'A104.4
O2i—Y—O269.09 (10)C10—C5'—H5'A104.9
O3i—Y—O3159.99 (11)C6—C5'—H5'B111.0
O1i—Y—O2118.71 (8)C10—C5'—H5'B110.5
O3i—Y—O273.44 (8)H5'A—C5'—H5'B106.9
O1i—Y—O3i84.89 (8)C5'—C6—C7129.4 (8)
O1i—Y—O2i79.43 (8)C5—C6—C7119.3 (4)
O3i—Y—O2i124.84 (8)C5'—C6—H6A102.6
O1i—Y—N479.62 (5)C7—C6—H6A104.2
O1—Y—N479.62 (5)C5'—C6—H6B108.5
O2—Y—N4145.46 (5)C7—C6—H6B104.5
O3—Y—N480.00 (5)H6A—C6—H6B105.6
O3i—Y—N480.00 (5)C5—C6—H6C106.7
O2i—Y—N4145.46 (5)C7—C6—H6C106.7
C1—Fe—C290.91 (8)C5—C6—H6D108.3
C1—Fe—C390.24 (7)C7—C6—H6D108.2
C3—Fe—C289.43 (11)H6C—C6—H6D107.0
C4—Fe—C289.09 (8)C6—C7—C8115.6 (3)
C4—Fe—C389.76 (7)C6—C7—H7A108.4
C2i—Fe—C2178.17 (16)C8—C7—H7A108.4
C3i—Fe—C3179.52 (14)C6—C7—H7B108.4
C4—Fe—C3i89.76 (7)C8—C7—H7B108.4
C1—Fe—C3i90.24 (7)H7A—C7—H7B107.4
C4—Fe—C2i89.09 (8)C9—C8—C7116.8 (4)
C1—Fe—C2i90.91 (8)C9—C8—H8A108.1
C3i—Fe—C2i89.43 (11)C7—C8—H8A108.1
C3—Fe—C2i90.57 (11)C9—C8—H8B108.1
C3i—Fe—C290.57 (11)C7—C8—H8B108.1
C10—O1—Y153.9 (2)H8A—C8—H8B107.3
Y—O2—H21128.5C8—C9—N5117.8 (4)
Y—O2—H20131.6C8—C9—H9A107.9
H21—O2—H2099.7N5—C9—H9A107.9
Y—O3—H30114.5C8—C9—H9B107.9
Y—O3—H31118.5N5—C9—H9B107.9
H30—O3—H31119.1H9A—C9—H9B107.2
C10—N5—C9127.8 (3)O1—C10—N5120.8 (3)
C10—N5—H5A116.1O1—C10—C5119.2 (3)
C9—N5—H5A116.1N5—C10—C5119.4 (3)
N2—C2—Fe178.1 (3)O1—C10—C5'106.5 (5)
N3—C3—Fe179.2 (2)N5—C10—C5'119.5 (7)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H21···N3ii0.852.072.823 (3)148
O2—H20···N1iii0.852.012.809 (3)157
O3—H30···N3iv0.852.032.861 (3)167
O3—H31···N2v0.851.902.739 (3)168
N5—H5A···N2v0.862.363.098 (4)144
Symmetry codes: (ii) x+1/2, y1/2, z+1/2; (iii) x, y1, z; (iv) x1/2, y1/2, z; (v) x, y+2, z+1.

Experimental details

Crystal data
Chemical formula[FeY(C6H11NO)2(CN)6(H2O)4]
Mr599.26
Crystal system, space groupMonoclinic, C2/c
Temperature (K)293
a, b, c (Å)14.006 (3), 12.951 (3), 15.011 (3)
β (°) 104.15 (3)
V3)2640.3 (10)
Z4
Radiation typeMo Kα
µ (mm1)2.78
Crystal size (mm)0.30 × 0.26 × 0.18
Data collection
DiffractometerMake Model CCD area-detector
Absorption correctionMulti-scan
(SADABS; Bruker, 2000)
Tmin, Tmax0.445, 0.606
No. of measured, independent and
observed [I > 2σ(I)] reflections
12364, 4853, 3691
Rint0.038
(sin θ/λ)max1)0.776
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.087, 1.06
No. of reflections4853
No. of parameters161
No. of restraints4
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.81, 0.55

Computer programs: SMART (Bruker, 2000), SMART, SAINT (Bruker, 2000), SHELXL97 (Sheldrick, 1997), PLATON (Spek, 2002), SHELXL97.

Selected geometric parameters (Å, º) top
Y—O12.211 (2)Fe—C31.936 (2)
Y—O22.3359 (19)Fe—C41.930 (3)
Y—O32.321 (2)N1—C11.146 (4)
Y—N42.401 (3)N2—C21.145 (4)
Fe—C11.933 (3)N3—C31.143 (3)
Fe—C21.937 (3)N4—C41.140 (5)
O1i—Y—O1159.24 (10)O3—Y—N480.00 (5)
O1—Y—O279.43 (8)C1—Fe—C290.91 (8)
O1—Y—O384.89 (8)C1—Fe—C390.24 (7)
O3—Y—O2124.84 (8)C3—Fe—C289.43 (11)
O1—Y—O2i118.71 (8)C4—Fe—C289.09 (8)
O1—Y—O3i91.52 (8)C4—Fe—C389.76 (7)
O3—Y—O2i73.44 (8)C2i—Fe—C2178.17 (16)
O2i—Y—O269.09 (10)C3i—Fe—C3179.52 (14)
O3i—Y—O3159.99 (11)C10—O1—Y153.9 (2)
O1—Y—N479.62 (5)N2—C2—Fe178.1 (3)
O2—Y—N4145.46 (5)N3—C3—Fe179.2 (2)
Symmetry code: (i) x, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H21···N3ii0.852.072.823 (3)148
O2—H20···N1iii0.852.012.809 (3)157
O3—H30···N3iv0.852.032.861 (3)167
O3—H31···N2v0.851.902.739 (3)168
N5—H5A···N2v0.862.363.098 (4)144
Symmetry codes: (ii) x+1/2, y1/2, z+1/2; (iii) x, y1, z; (iv) x1/2, y1/2, z; (v) x, y+2, z+1.
 

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