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The nine-coordinate SmIII cation in [Sm{O2CCH(OH)CH(OH)CO2}{O2CCH(OH)CH(OH)CO2H}(OH2)3], or [Sm(C4H4O6)(C4H5O6)(H2O)3]n, is located on a crystallographic twofold axis. The coordination geometry is capped square-antiprismatic and is defined by four O atoms derived from carboxyl­ate/carboxyl­ic acid groups, two hydroxyl O atoms and three water mol­ecules. The SmIII atoms are linked by the tartrate ligands into layers, which are connected via O—H...O hydrogen bonds involving the carboxyl­ate and hydroxyl O atoms, and water mol­ecules.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802007420/tk6058sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802007420/tk6058Isup2.hkl
Contains datablock I

CCDC reference: 185758

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.011 Å
  • H-atom completeness 94%
  • R factor = 0.028
  • wR factor = 0.072
  • Data-to-parameter ratio = 10.9

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry

General Notes

FORMU_01 There is a discrepancy between the atom counts in the _chemical_formula_sum and the formula from the _atom_site* data. Atom count from _chemical_formula_sum:C8 H15 O15 Sm1 Atom count from the _atom_site data: C8 H14 O15 Sm1 CELLZ_01 From the CIF: _cell_formula_units_Z 4 From the CIF: _chemical_formula_sum C8 H15 O15 Sm TEST: Compare cell contents of formula and atom_site data atom Z*formula cif sites diff C 32.00 32.00 0.00 H 60.00 56.00 4.00 O 60.00 60.00 0.00 Sm 4.00 4.00 0.00 Difference between formula and atom_site contents detected. WARNING: H atoms missing from atom site list. Is this intentional? REFLT_03 From the CIF: _diffrn_reflns_theta_max 25.00 From the CIF: _reflns_number_total 1205 Count of symmetry unique reflns 810 Completeness (_total/calc) 148.77% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 395 Fraction of Friedel pairs measured 0.488 Are heavy atom types Z>Si present yes WARNING: Large fraction of Friedel related reflns may be needed to determine absolute structure

Comment top

Owing to their enormous variety of intriguing structural topologies, chemists have devoted great effort to the research of novel chiral coordination materials. Recently, the crystal engineering strategy has been utilized in the construction of metal–organic coordination polymers by using asymmetric bridging ligands as building blocks (Rowan & Nolte, 1998; Amabilino & Stoddart, 1995; Piguet et al., 1997; Biradha et al., 1999). The higher coordination numbers of lanthanide ions and the inherent flexibility of their coordination geometries might lead to some unprecedented topological architectures (Long et al., 2000, 2001; Pan et al., 2000). We are currently interested in pursuing synthetic strategies by using lanthanide ions as nodes in the construction of chiral polymeric frameworks. Tartaric acid, which has six O atoms as potential donors, is a rather versatile ligand for the synthesis of chiral polymeric complexes containing lanthanide cations. To date, only two tartrate-bridged lanthanide complexes have been reported (Hawthorne et al., 1983; Starynowicz & Meyer, 2000). As part of our investigations of polycarboxylic acid-bridged chiral polymeric complexes, the title complex [Sm(C4H4O6)(C4H5O6)(H2O)3]n, (I), was prepared and obtained as colorless crystals.

The title compound comprises two-dimensional chiral sheets that are built up by connecting the SmIII cations with its neighbors through bridging tartrate ligands. The crystal structure and the coordination modes of tartrate ligands are similar to the previously reported ErIV complex [Er{O2CCH(OH)CH(OH)CO2}2(OH2)3] (Hawthorne et al., 1983). The molecular structure has twofold symmetry so that the asymmetric unit comprises half an Sm cation, one tartrate anion and 1.5 water molecules. Atoms Sm and O8, of a coordinated water molecule, lie on the symmetry axis. This implies some disorder in the structure in that the non-coordinating carboxylate residue (containing the O5 and O6 atoms) is protonated 50% of the time. For the tartrate ligand, the hydroxyl O3 atom and atom O2 of the coordinating carboxylate group chelates a Sm atom. Atom O1 bridges a symmetry-related Sm atom. Four carboxylate O atoms, two hydroxyl O atoms and three water molecules form a distorted monocapped square-antiprismatic coordination sphere (Fig. 1). The mean Sm—Ocarboxylate distance of 2.378 (5) Å is about 0.173 Å shorter than the average length of the Sm—Ohydroxyl bond. The Sm—Owater bond lengths are in the range 2.463 (6)–2.732 (15) Å, with the longer bond involving the water molecule lying on the symmetry axis. Each tartrate ligand acts as a bridging ligand connecting two Sm atoms into a two-dimensional chiral structure (Fig. 2). The layers are linked together through a complicated hydrogen-bonding scheme involving the water ligands, hydroxyl O atoms and the carboxylate O atoms. Thus, a three-dimensional framework is produced (Fig. 3), in which the mean O—H···O hydrogen-bonding distance is 2.745 (9) Å.

Experimental top

The pH of a mixture of SmCl3 (5.0 mmol) (prepared from Sm2O3 dissolved in 35% HCl) and L-tartaric acid (1.50 g, 10.0 mmol) in H2O (60 ml) was adjusted to 1.66 with 10% HCl under vigorous stirring. Colorless crystals of the title compound were isolated after three weeks.

Refinement top

H atoms were included as riding. Disorder is evident in the structure in that the crystallographically independent tartrate anion is protonated at the O5 and O6 carboxyl O atoms 50% of the time.

Computing details top

Data collection: SMART (Siemens, 1996); cell refinement: SAINT (Siemens, 1994); data reduction: SMART and SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Siemens, 1994); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. A perspective view of the locally expanded unit for (I). Displacement ellipsoids are drawn at the 30% probability level [symmetry codes: (i) y, x, 1 - z; (ii) x, -1 + y, z; (iii) -1 + y, x, 1 - z].
[Figure 2] Fig. 2. A view down the c axis, showing the extended lamellar structure of (I). For clarity, H atoms had been omitted.
[Figure 3] Fig. 3. Cell-packing diagram viewed down the b axis. Hydrogen bonding is indicated by dashed lines.
Poly[triaqua(µ-hydrogen tartrato)(µ-tartrato)samarium(III)] top
Crystal data top
[Sm(C4H4O6)(C4H5O6)(H2O)3]Dx = 2.429 Mg m3
Mr = 501.55Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P41212Cell parameters from 207 reflections
a = 6.1030 (3) Åθ = 2.2–25.0°
c = 36.826 (2) ŵ = 4.37 mm1
V = 1371.6 (1) Å3T = 293 K
Z = 4Rhombus, colorless
F(000) = 9800.42 × 0.40 × 0.30 mm
Data collection top
Siemens SMART CCD
diffractometer
1205 independent reflections
Radiation source: fine-focus sealed tube1185 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.025
ϕ and ω scansθmax = 25.0°, θmin = 2.2°
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
h = 63
Tmin = 0.172, Tmax = 0.269k = 76
3367 measured reflectionsl = 2743
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.028 w = 1/[σ2(Fo2) + (0.0139P)2 + 15.128P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.072(Δ/σ)max < 0.001
S = 1.00Δρmax = 0.77 e Å3
1205 reflectionsΔρmin = 1.01 e Å3
111 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0024 (3)
Primary atom site location: structure-invariant direct methodsAbsolute structure: (Flack, 1983)
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.00 (4)
Crystal data top
[Sm(C4H4O6)(C4H5O6)(H2O)3]Z = 4
Mr = 501.55Mo Kα radiation
Tetragonal, P41212µ = 4.37 mm1
a = 6.1030 (3) ÅT = 293 K
c = 36.826 (2) Å0.42 × 0.40 × 0.30 mm
V = 1371.6 (1) Å3
Data collection top
Siemens SMART CCD
diffractometer
1205 independent reflections
Absorption correction: empirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
1185 reflections with I > 2σ(I)
Tmin = 0.172, Tmax = 0.269Rint = 0.025
3367 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.028H-atom parameters constrained
wR(F2) = 0.072 w = 1/[σ2(Fo2) + (0.0139P)2 + 15.128P]
where P = (Fo2 + 2Fc2)/3
S = 1.00Δρmax = 0.77 e Å3
1205 reflectionsΔρmin = 1.01 e Å3
111 parametersAbsolute structure: (Flack, 1983)
0 restraintsAbsolute structure parameter: 0.00 (4)
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*/Ueq
Sm0.67900 (6)0.67900 (6)0.50000.02227 (18)
O10.7814 (10)1.3751 (8)0.46290 (16)0.0356 (14)
O20.7024 (10)1.0631 (8)0.49160 (11)0.0307 (12)
O30.8359 (9)0.8150 (9)0.43987 (11)0.0262 (9)
H3B0.80700.73960.42210.039*
O41.2103 (10)1.1054 (9)0.43712 (18)0.0424 (16)
H4A1.31641.17360.42940.059*
O50.9239 (12)1.0527 (12)0.35287 (17)0.0530 (17)
O61.2365 (10)0.8974 (10)0.37169 (16)0.0439 (16)
O70.3777 (9)0.6976 (12)0.45559 (15)0.0497 (17)
H7A0.29510.59330.45860.060*
H7B0.37250.80840.43950.060*
O80.3625 (17)0.3625 (17)0.50000.110 (5)
H8A0.24180.41980.50230.165*
C10.7672 (11)1.1692 (12)0.46480 (19)0.0256 (16)
C20.8230 (14)1.0406 (11)0.4303 (2)0.0255 (15)
H2A0.70261.05910.41300.031*
C31.0342 (13)1.1277 (12)0.4127 (2)0.034 (2)
H3A1.01381.28430.40790.041*
C41.0745 (14)1.0133 (13)0.3764 (3)0.038 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Sm0.0238 (2)0.0238 (2)0.0191 (2)0.0050 (2)0.00144 (18)0.00144 (18)
O10.038 (3)0.021 (3)0.048 (3)0.001 (2)0.022 (3)0.002 (2)
O20.056 (3)0.025 (3)0.011 (2)0.003 (2)0.008 (2)0.0032 (19)
O30.032 (3)0.020 (2)0.027 (2)0.002 (2)0.003 (2)0.004 (2)
O40.028 (3)0.040 (3)0.059 (4)0.010 (3)0.006 (3)0.016 (3)
O50.060 (5)0.048 (4)0.051 (4)0.021 (3)0.001 (4)0.001 (3)
O60.051 (4)0.043 (3)0.038 (3)0.016 (3)0.011 (3)0.004 (3)
O70.033 (3)0.077 (5)0.039 (3)0.017 (3)0.007 (2)0.010 (3)
O80.094 (7)0.094 (7)0.142 (12)0.021 (8)0.010 (8)0.010 (8)
C10.022 (3)0.023 (4)0.032 (4)0.005 (3)0.005 (3)0.009 (3)
C20.025 (4)0.020 (3)0.031 (4)0.003 (3)0.002 (4)0.000 (3)
C30.036 (4)0.021 (4)0.044 (5)0.002 (3)0.015 (4)0.002 (3)
C40.046 (5)0.029 (4)0.039 (4)0.003 (4)0.016 (4)0.002 (3)
Geometric parameters (Å, º) top
Sm—O2i2.369 (5)O3—H3B0.8200
Sm—O22.369 (5)O4—C31.407 (10)
Sm—O1ii2.387 (5)O4—H4A0.8200
Sm—O1iii2.387 (5)O5—C41.285 (11)
Sm—O7i2.463 (6)O6—C41.228 (9)
Sm—O72.463 (6)O7—H7A0.8200
Sm—O3i2.551 (4)O7—H7B0.8999
Sm—O32.551 (4)O8—H8A0.8200
Sm—O82.732 (15)C1—C21.531 (10)
O1—C11.261 (9)C2—C31.537 (10)
O1—Smiv2.387 (5)C2—H2A0.9800
O2—C11.245 (8)C3—C41.529 (12)
O3—C21.423 (9)C3—H3A0.9800
O2i—Sm—O284.1 (3)O7i—Sm—O860.3 (2)
O2i—Sm—O1ii132.7 (2)O7—Sm—O860.3 (2)
O2—Sm—O1ii82.1 (2)O3i—Sm—O8119.7 (1)
O2i—Sm—O1iii82.1 (2)O3—Sm—O8119.7 (1)
O2—Sm—O1iii132.7 (2)C1—O1—Smiv136.4 (5)
O1ii—Sm—O1iii137.3 (3)C1—O2—Sm129.6 (5)
O2i—Sm—O7i85.0 (2)C2—O3—Sm120.6 (4)
O2—Sm—O7i145.3 (2)C2—O3—H3B109.5
O1ii—Sm—O7i81.4 (2)Sm—O3—H3B115.5
O1iii—Sm—O7i77.8 (2)C3—O4—H4A109.5
O2i—Sm—O7145.3 (2)Sm—O7—H7A109.5
O2—Sm—O785.0 (2)Sm—O7—H7B119.9
O1ii—Sm—O777.8 (2)H7A—O7—H7B130.6
O1iii—Sm—O781.4 (2)Sm—O8—H8A109.5
O7i—Sm—O7120.6 (3)O2—C1—O1125.7 (7)
O2i—Sm—O3i62.7 (2)O2—C1—C2117.5 (6)
O2—Sm—O3i73.9 (2)O1—C1—C2116.7 (6)
O1ii—Sm—O3i70.0 (2)O3—C2—C1107.7 (6)
O1iii—Sm—O3i134.7 (2)O3—C2—C3113.1 (6)
O7i—Sm—O3i71.9 (2)C1—C2—C3111.0 (6)
O7—Sm—O3i143.3 (2)O3—C2—H2A108.3
O2i—Sm—O373.9 (2)C1—C2—H2A108.3
O2—Sm—O362.7 (2)C3—C2—H2A108.3
O1ii—Sm—O3134.7 (2)O4—C3—C4113.0 (6)
O1iii—Sm—O370.0 (2)O4—C3—C2109.7 (6)
O7i—Sm—O3143.3 (2)C4—C3—C2110.2 (6)
O7—Sm—O371.9 (2)O4—C3—H3A107.9
O3i—Sm—O3120.6 (2)C4—C3—H3A107.9
O2i—Sm—O8137.9 (2)C2—C3—H3A107.9
O2—Sm—O8137.9 (2)O6—C4—O5126.1 (8)
O1ii—Sm—O868.6 (1)O6—C4—C3121.1 (8)
O1iii—Sm—O868.6 (1)O5—C4—C3112.9 (7)
Symmetry codes: (i) y, x, z+1; (ii) y1, x, z+1; (iii) x, y1, z; (iv) x, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H3B···O6v0.821.872.681 (7)173
O4—H4A···O5vi0.822.152.867 (9)146
O7—H7A···O80.822.122.621 (11)120
O7—H7B···O4vii0.902.072.775 (10)135
O8—H8A···O2ii0.822.052.782 (6)148
Symmetry codes: (ii) y1, x, z+1; (v) x1/2, y+3/2, z+3/4; (vi) x+1/2, y+5/2, z+3/4; (vii) x1, y, z.

Experimental details

Crystal data
Chemical formula[Sm(C4H4O6)(C4H5O6)(H2O)3]
Mr501.55
Crystal system, space groupTetragonal, P41212
Temperature (K)293
a, c (Å)6.1030 (3), 36.826 (2)
V3)1371.6 (1)
Z4
Radiation typeMo Kα
µ (mm1)4.37
Crystal size (mm)0.42 × 0.40 × 0.30
Data collection
DiffractometerSiemens SMART CCD
diffractometer
Absorption correctionEmpirical (using intensity measurements)
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.172, 0.269
No. of measured, independent and
observed [I > 2σ(I)] reflections
3367, 1205, 1185
Rint0.025
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.028, 0.072, 1.00
No. of reflections1205
No. of parameters111
H-atom treatmentH-atom parameters constrained
w = 1/[σ2(Fo2) + (0.0139P)2 + 15.128P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)0.77, 1.01
Absolute structure(Flack, 1983)
Absolute structure parameter0.00 (4)

Computer programs: SMART (Siemens, 1996), SAINT (Siemens, 1994), SMART and SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Siemens, 1994), SHELXL97.

Selected geometric parameters (Å, º) top
Sm—O22.369 (5)Sm—O32.551 (4)
Sm—O1i2.387 (5)Sm—O82.732 (15)
Sm—O72.463 (6)
O2—Sm—O1ii82.1 (2)O2—Sm—O362.7 (2)
O2—Sm—O1i132.7 (2)O1ii—Sm—O3134.7 (2)
O2—Sm—O7iii145.3 (2)O1i—Sm—O370.0 (2)
O2—Sm—O785.0 (2)O7—Sm—O371.9 (2)
O1ii—Sm—O777.8 (2)O3iii—Sm—O3120.6 (2)
O1i—Sm—O781.4 (2)O2—Sm—O8137.9 (2)
O7iii—Sm—O7120.6 (3)O1i—Sm—O868.6 (1)
O2—Sm—O3iii73.9 (2)O7—Sm—O860.3 (2)
O7—Sm—O3iii143.3 (2)O3—Sm—O8119.7 (1)
Symmetry codes: (i) x, y1, z; (ii) y1, x, z+1; (iii) y, x, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O3—H3B···O6iv0.821.872.681 (7)173
O4—H4A···O5v0.822.152.867 (9)146
O7—H7A···O80.822.122.621 (11)120
O7—H7B···O4vi0.902.072.775 (10)135
O8—H8A···O2ii0.822.052.782 (6)148
Symmetry codes: (ii) y1, x, z+1; (iv) x1/2, y+3/2, z+3/4; (v) x+1/2, y+5/2, z+3/4; (vi) x1, y, z.
 

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