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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jul 22;65(Pt 8):m979. doi: 10.1107/S1600536809028360

catena-Poly[[[tetra­aqua­manganese(II)]-μ-4,4′-bipyridine] bis­(3-hydroxy­cinnamate) dihydrate]

Zhi-Wei Tang a, Jun-Dan Fu a, Long-Ping Jiang a, Yi-Hang Wen a,*
PMCID: PMC2977154  PMID: 21583422

Abstract

The title compound, {[Mn(C10H8N2)(H2O)4](C9H7O3)2·2H2O}n, was obtained by the hydro­thermal reaction of manganese chloride with mixed 3-hydroxy­lcinnamic acid (H2 L) and 4,4′-bipyridine (4,4′-bipy) ligands. The structure contains [Mn(C10H8N2)(H2O)4]2+ cations with the MnII atoms lying on a centres of inversion and bridged into a linear chain along the a axis by 4,4′-bipy ligands, surrounded by HL anions and uncoordinated water mol­ecules. Extensive O—H⋯O hydrogen-bonding and weak π–π inter­actions [centroid–centroid distance = 3.7572  (3) Å] between the constituents lead to the formation of a three-dimensional supra­molecular network.

Related literature

For potential applications of compounds with supramolecular architectures, see: Niu et al. (2008); Xue et al. (2007); Ye et al. (2005); Zhang et al. (2009). For the synthesis of supra­molecular coordination compounds containing 4-pyridyl and carboxyl­ate groups, see: Feng et al. (2008); He et al. (2007); Li et al. (2008).graphic file with name e-65-0m979-scheme1.jpg

Experimental

Crystal data

  • [Mn(C10H8N2)(H2O)4](C9H7O3)2·2H2O

  • M r = 645.51

  • Monoclinic, Inline graphic

  • a = 11.6620 (12) Å

  • b = 11.2726 (13) Å

  • c = 11.6238 (13) Å

  • β = 96.520 (9)°

  • V = 1518.2 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.50 mm−1

  • T = 296 K

  • 0.21 × 0.14 × 0.07 mm

Data collection

  • Bruker APEXII area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.92, T max = 0.97

  • 13208 measured reflections

  • 3513 independent reflections

  • 2293 reflections with I > 2σ(I)

  • R int = 0.060

Refinement

  • R[F 2 > 2σ(F 2)] = 0.044

  • wR(F 2) = 0.118

  • S = 1.04

  • 3513 reflections

  • 217 parameters

  • 10 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.21 e Å−3

  • Δρmin = −0.31 e Å−3

Data collection: APEX2 (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT; 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/S1600536809028360/at2846sup1.cif

e-65-0m979-sup1.cif (19.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028360/at2846Isup2.hkl

e-65-0m979-Isup2.hkl (172.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O3W—H3WA⋯O2i 0.832 (16) 1.912 (18) 2.738 (2) 171 (3)
O1W—H1WA⋯O1ii 0.833 (17) 1.888 (17) 2.719 (2) 174 (3)
O2W—H2WA⋯O3Wiii 0.815 (17) 2.024 (17) 2.838 (3) 176 (3)
O3W—H3WB⋯O2iv 0.842 (16) 1.902 (18) 2.741 (2) 174 (3)
O2W—H2WB⋯O1v 0.832 (16) 1.878 (16) 2.702 (2) 171 (3)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic; (iii) Inline graphic; (iv) Inline graphic; (v) Inline graphic.

supplementary crystallographic information

Comment

The construction of supramolecular architectures based on metal and organic building blocks is currently of great interest for their aesthetic architectures and potential functions such as adsorption, ion exchange, magnetic and luminescent materials (Niu et al., 2008; Xue et al., 2007; Ye et al., 2005; Zhang et al., 2009). Recently, we are interested in the synthesis of novel supramolecular coordination compounds which contain not only 4-pyridyl but also carboxylate groups in the crystal structure (He et al., 2007; Feng et al., 2008; Li et al., 2008). Here we report the crystal structure of the title compound, [Mn(C10H8N2)(H2O)4]2.2(C9H7O3).2H2O, (I).

The present X-ray single-crystal diffraction study reveals that (I) is a new coordination polymer involving Mn2+ and 3-hydroxycinnamate anions, as shown in Fig. 1. The MnII is hexacoordinated in an octahedral manner by four water molecules in the equatorial plane and two N atoms in the axial positions from two 4,4'-bipyridine molecules. The bond lengths of Mn—N and Mn—O are 2.2863 (17) Å and in the range 2.1641 (15)—2.1675 (17) Å, respectively. As shown in Fig. 2, the linear cationic chains, 3-Hydroxycinnamate anions and lattice water molecules are linked together through a series of O—H···O bonds with the hydrogen bonds lengths in the range of 2.702 (2)—2.838 (3) Å and bond angles between 171 (3) and 176 (3) °. The extensive hydrogen bonds together with the weak π-π interactions between hca- anions and 4,4'-bipyridine (the centroid-to-centroid distance is 3.7572 Å) stabilize the crystal structure, forming a three-dimensional network.

Experimental

MnCl2.4H2O (0.0973 g, 0.5 mmol), 3-hydroxycinnamic acid (0.1619 g, 1 mmol), NaOH (0.0405 g, 1 mmol), 4,4'-bipy (0.1562 g, 1 mmol) and H2O-ethanol (4:1, 15 mL) was sealed in a 25 ml stainless-steel reactor with a Telflon liner and was heated at 433 K for 3 d, then the reactor was cooled slowly to room temperature. The solution was filtered, giving yellow single crystals suitable for X-ray analysis in yield 30%.

Refinement

The carbon-bound H-atoms were positioned geometrically and included in the refinement using a riding model [C—H 0.93 Å Uiso(H) = 1.2Ueq(C)]. The water and hydroxyl H atoms were located from different maps, and their positions were refined isotropically, with O—H distances fixed by Owater—H = 0.85 (2) Å, Ohydroxyl—H = 0.96 (2) Å and H—H = 1.30 (2) Å, their displacement parameters were set to 1.5Ueq(Owater) and 1.2Ueq(Ohydroxyl).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level and H atoms have been omitted for clarity. [Symmetry codes: (i) 2 - x, 1 - y, -1 - z; (ii) 3 - x, 1 - y, 1 - z; (iii) -1 + x, y, z]

Fig. 2.

Fig. 2.

Packing diagram showing hydrogen bonds as dashed lines. All H atoms have been omitted for clarity.

Crystal data

[Mn(C10H8N2)(H2O)4](C9H7O3)2·2H2O F(000) = 674
Mr = 645.51 Dx = 1.412 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 1488 reflections
a = 11.6620 (12) Å θ = 1.8–27.7°
b = 11.2726 (13) Å µ = 0.50 mm1
c = 11.6238 (13) Å T = 296 K
β = 96.520 (9)° Block, yellow
V = 1518.2 (3) Å3 0.21 × 0.14 × 0.07 mm
Z = 2

Data collection

Bruker APEXII area-detector diffractometer 3513 independent reflections
Radiation source: fine-focus sealed tube 2293 reflections with I > 2σ(I)
graphite Rint = 0.060
ω scans θmax = 27.7°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −15→14
Tmin = 0.92, Tmax = 0.97 k = −14→14
13208 measured reflections l = −15→15

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)] = 0.044 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.118 H atoms treated by a mixture of independent and constrained refinement
S = 1.04 w = 1/[σ2(Fo2) + (0.0535P)2 + 0.0147P] where P = (Fo2 + 2Fc2)/3
3513 reflections (Δ/σ)max < 0.001
217 parameters Δρmax = 0.21 e Å3
10 restraints Δρmin = −0.31 e Å3

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
Mn1 1.0000 0.5000 −0.5000 0.02932 (15)
C1 1.24961 (19) 0.5744 (2) −0.5720 (2) 0.0384 (6)
H1A 1.2060 0.6305 −0.6164 0.046*
C2 1.36718 (19) 0.5795 (2) −0.5695 (2) 0.0383 (6)
H2A 1.4008 0.6376 −0.6116 0.046*
C3 1.43615 (18) 0.4985 (2) −0.50437 (18) 0.0316 (5)
C4 1.3781 (2) 0.4144 (3) −0.4478 (3) 0.0657 (9)
H4A 1.4193 0.3561 −0.4042 0.079*
C5 1.2599 (2) 0.4158 (3) −0.4553 (3) 0.0652 (9)
H5A 1.2239 0.3575 −0.4156 0.078*
C6 0.3636 (2) 0.6015 (2) −0.1614 (2) 0.0479 (6)
C7 0.2912 (2) 0.6654 (3) −0.2419 (2) 0.0529 (7)
H7A 0.2115 0.6598 −0.2423 0.063*
C8 0.3368 (2) 0.7364 (3) −0.3205 (2) 0.0519 (7)
H8A 0.2881 0.7802 −0.3734 0.062*
C9 0.4546 (2) 0.7436 (2) −0.3218 (2) 0.0479 (7)
H9A 0.4849 0.7928 −0.3751 0.057*
C10 0.5288 (2) 0.6779 (2) −0.2439 (2) 0.0397 (6)
C11 0.4815 (2) 0.6072 (2) −0.1637 (2) 0.0454 (6)
H11A 0.5299 0.5630 −0.1108 0.055*
C12 0.6538 (2) 0.6860 (2) −0.2478 (2) 0.0403 (6)
H12A 0.6795 0.7441 −0.2956 0.048*
C13 0.7334 (2) 0.6189 (2) −0.1900 (2) 0.0425 (6)
H13A 0.7098 0.5621 −0.1397 0.051*
C14 0.8572 (2) 0.6292 (2) −0.20085 (19) 0.0377 (6)
N1 1.19366 (15) 0.49461 (16) −0.51532 (16) 0.0353 (4)
O1 0.89468 (15) 0.71680 (16) −0.25223 (15) 0.0487 (5)
O1W 1.02880 (17) 0.43379 (17) −0.32434 (13) 0.0502 (5)
H1WA 1.049 (3) 0.3672 (17) −0.298 (3) 0.075*
H1WB 1.004 (3) 0.472 (2) −0.272 (2) 0.075*
O2 0.92237 (14) 0.54517 (16) −0.15829 (14) 0.0443 (4)
O2W 0.98772 (18) 0.31913 (16) −0.56349 (17) 0.0531 (5)
H2WA 0.955 (3) 0.260 (2) −0.542 (3) 0.080*
H2WB 1.022 (3) 0.300 (3) −0.620 (2) 0.080*
O3 0.32335 (17) 0.5320 (2) −0.0786 (2) 0.0769 (7)
H3 0.2485 (18) 0.551 (3) −0.074 (3) 0.092*
O3W 0.11487 (15) 0.61016 (17) −0.01468 (16) 0.0480 (5)
H3WA 0.110 (2) 0.566 (2) 0.0420 (18) 0.072*
H3WB 0.058 (2) 0.593 (3) −0.0630 (19) 0.072*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Mn1 0.0232 (3) 0.0318 (3) 0.0335 (2) 0.0007 (2) 0.00570 (18) 0.0012 (2)
C1 0.0256 (13) 0.0441 (15) 0.0449 (13) 0.0012 (10) 0.0012 (10) 0.0104 (11)
C2 0.0261 (13) 0.0458 (15) 0.0431 (12) −0.0034 (10) 0.0039 (10) 0.0140 (11)
C3 0.0237 (11) 0.0340 (12) 0.0377 (11) 0.0004 (10) 0.0063 (9) 0.0002 (10)
C4 0.0266 (15) 0.066 (2) 0.106 (2) 0.0109 (13) 0.0130 (14) 0.0522 (18)
C5 0.0276 (15) 0.064 (2) 0.106 (2) 0.0062 (13) 0.0183 (15) 0.0493 (18)
C6 0.0354 (15) 0.0512 (17) 0.0569 (15) 0.0013 (12) 0.0047 (12) −0.0016 (13)
C7 0.0354 (15) 0.066 (2) 0.0553 (16) 0.0066 (13) −0.0035 (12) −0.0148 (14)
C8 0.0446 (17) 0.0655 (19) 0.0433 (14) 0.0151 (14) −0.0059 (12) −0.0087 (13)
C9 0.0500 (18) 0.0548 (17) 0.0384 (13) 0.0082 (13) 0.0030 (12) −0.0054 (12)
C10 0.0356 (14) 0.0437 (15) 0.0393 (12) 0.0037 (11) 0.0018 (10) −0.0100 (11)
C11 0.0318 (14) 0.0513 (16) 0.0526 (15) 0.0061 (12) 0.0019 (11) 0.0024 (12)
C12 0.0404 (15) 0.0417 (15) 0.0396 (12) 0.0002 (12) 0.0080 (11) −0.0057 (11)
C13 0.0372 (14) 0.0433 (15) 0.0485 (14) −0.0013 (11) 0.0106 (11) 0.0009 (12)
C14 0.0373 (14) 0.0422 (14) 0.0347 (12) −0.0033 (11) 0.0082 (10) −0.0094 (11)
N1 0.0240 (10) 0.0362 (11) 0.0467 (10) 0.0030 (9) 0.0089 (8) 0.0047 (9)
O1 0.0520 (11) 0.0422 (11) 0.0552 (10) −0.0082 (9) 0.0199 (9) −0.0059 (8)
O1W 0.0615 (13) 0.0542 (12) 0.0363 (9) 0.0249 (10) 0.0118 (8) 0.0075 (8)
O2 0.0343 (10) 0.0513 (11) 0.0481 (9) 0.0056 (8) 0.0079 (8) −0.0013 (8)
O2W 0.0644 (13) 0.0367 (10) 0.0639 (12) −0.0111 (9) 0.0321 (10) −0.0091 (9)
O3 0.0394 (12) 0.0962 (17) 0.0977 (16) 0.0068 (12) 0.0190 (12) 0.0337 (14)
O3W 0.0375 (11) 0.0509 (12) 0.0554 (11) −0.0055 (9) 0.0040 (8) 0.0011 (9)

Geometric parameters (Å, °)

Mn1—O1W 2.1641 (15) C7—H7A 0.9300
Mn1—O1Wi 2.1641 (15) C8—C9 1.378 (4)
Mn1—O2Wi 2.1675 (17) C8—H8A 0.9300
Mn1—O2W 2.1675 (17) C9—C10 1.393 (3)
Mn1—N1i 2.2863 (17) C9—H9A 0.9300
Mn1—N1 2.2863 (17) C10—C11 1.388 (3)
C1—N1 1.329 (3) C10—C12 1.466 (3)
C1—C2 1.369 (3) C11—H11A 0.9300
C1—H1A 0.9300 C12—C13 1.320 (3)
C2—C3 1.385 (3) C12—H12A 0.9300
C2—H2A 0.9300 C13—C14 1.468 (3)
C3—C4 1.375 (3) C13—H13A 0.9300
C3—C3ii 1.482 (4) C14—O1 1.258 (3)
C4—C5 1.371 (3) C14—O2 1.278 (3)
C4—H4A 0.9300 O1W—H1WA 0.833 (17)
C5—N1 1.323 (3) O1W—H1WB 0.825 (16)
C5—H5A 0.9300 O2W—H2WA 0.815 (17)
C6—O3 1.364 (3) O2W—H2WB 0.832 (16)
C6—C11 1.380 (3) O3—H3 0.908 (18)
C6—C7 1.388 (4) O3W—H3WA 0.832 (16)
C7—C8 1.368 (4) O3W—H3WB 0.842 (16)
O1W—Mn1—O1Wi 180.00 (10) C8—C7—H7A 120.0
O1W—Mn1—O2Wi 90.34 (8) C6—C7—H7A 120.0
O1Wi—Mn1—O2Wi 89.66 (8) C7—C8—C9 120.4 (3)
O1W—Mn1—O2W 89.66 (8) C7—C8—H8A 119.8
O1Wi—Mn1—O2W 90.34 (8) C9—C8—H8A 119.8
O2Wi—Mn1—O2W 180.00 (10) C8—C9—C10 120.6 (3)
O1W—Mn1—N1i 89.11 (7) C8—C9—H9A 119.7
O1Wi—Mn1—N1i 90.89 (7) C10—C9—H9A 119.7
O2Wi—Mn1—N1i 88.63 (7) C11—C10—C9 118.5 (2)
O2W—Mn1—N1i 91.37 (7) C11—C10—C12 121.9 (2)
O1W—Mn1—N1 90.89 (7) C9—C10—C12 119.6 (2)
O1Wi—Mn1—N1 89.11 (7) C6—C11—C10 120.8 (2)
O2Wi—Mn1—N1 91.37 (7) C6—C11—H11A 119.6
O2W—Mn1—N1 88.63 (7) C10—C11—H11A 119.6
N1i—Mn1—N1 180.0 C13—C12—C10 126.4 (2)
N1—C1—C2 124.4 (2) C13—C12—H12A 116.8
N1—C1—H1A 117.8 C10—C12—H12A 116.8
C2—C1—H1A 117.8 C12—C13—C14 123.6 (2)
C1—C2—C3 120.1 (2) C12—C13—H13A 118.2
C1—C2—H2A 119.9 C14—C13—H13A 118.2
C3—C2—H2A 119.9 O1—C14—O2 122.8 (2)
C4—C3—C2 115.4 (2) O1—C14—C13 120.0 (2)
C4—C3—C3ii 122.0 (3) O2—C14—C13 117.1 (2)
C2—C3—C3ii 122.6 (2) C5—N1—C1 115.2 (2)
C5—C4—C3 120.5 (2) C5—N1—Mn1 119.98 (15)
C5—C4—H4A 119.7 C1—N1—Mn1 124.44 (15)
C3—C4—H4A 119.7 Mn1—O1W—H1WA 132 (2)
N1—C5—C4 124.3 (2) Mn1—O1W—H1WB 119 (2)
N1—C5—H5A 117.8 H1WA—O1W—H1WB 108 (2)
C4—C5—H5A 117.8 Mn1—O2W—H2WA 133 (2)
O3—C6—C11 117.6 (2) Mn1—O2W—H2WB 119 (2)
O3—C6—C7 122.8 (2) H2WA—O2W—H2WB 108 (2)
C11—C6—C7 119.6 (3) C6—O3—H3 108 (2)
C8—C7—C6 120.1 (3) H3WA—O3W—H3WB 105 (2)
N1—C1—C2—C3 −0.3 (4) C9—C10—C12—C13 −171.1 (2)
C1—C2—C3—C4 1.7 (4) C10—C12—C13—C14 177.8 (2)
C1—C2—C3—C3ii −178.3 (3) C12—C13—C14—O1 11.9 (4)
C2—C3—C4—C5 −1.6 (4) C12—C13—C14—O2 −166.8 (2)
C3ii—C3—C4—C5 178.3 (3) C4—C5—N1—C1 1.2 (4)
C3—C4—C5—N1 0.2 (5) C4—C5—N1—Mn1 −171.9 (3)
O3—C6—C7—C8 178.0 (3) C2—C1—N1—C5 −1.2 (4)
C11—C6—C7—C8 −2.1 (4) C2—C1—N1—Mn1 171.64 (19)
C6—C7—C8—C9 1.1 (4) O1W—Mn1—N1—C5 29.3 (2)
C7—C8—C9—C10 0.6 (4) O1Wi—Mn1—N1—C5 −150.7 (2)
C8—C9—C10—C11 −1.4 (3) O2Wi—Mn1—N1—C5 119.6 (2)
C8—C9—C10—C12 179.3 (2) O2W—Mn1—N1—C5 −60.4 (2)
O3—C6—C11—C10 −178.7 (2) O1W—Mn1—N1—C1 −143.18 (19)
C7—C6—C11—C10 1.4 (4) O1Wi—Mn1—N1—C1 36.82 (19)
C9—C10—C11—C6 0.4 (4) O2Wi—Mn1—N1—C1 −52.81 (19)
C12—C10—C11—C6 179.6 (2) O2W—Mn1—N1—C1 127.19 (19)
C11—C10—C12—C13 9.7 (4)

Symmetry codes: (i) −x+2, −y+1, −z−1; (ii) −x+3, −y+1, −z−1.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O3W—H3WA···O2iii 0.83 (2) 1.91 (2) 2.738 (2) 171 (3)
O1W—H1WA···O1iv 0.83 (2) 1.89 (2) 2.719 (2) 174 (3)
O2W—H2WA···O3Wv 0.82 (2) 2.02 (2) 2.838 (3) 176 (3)
O3W—H3WB···O2vi 0.84 (2) 1.90 (2) 2.741 (2) 174 (3)
O2W—H2WB···O1i 0.83 (2) 1.88 (2) 2.702 (2) 171 (3)

Symmetry codes: (iii) −x+1, −y+1, −z; (iv) −x+2, y−1/2, −z−1/2; (v) −x+1, y−1/2, −z−1/2; (vi) x−1, y, z; (i) −x+2, −y+1, −z−1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: AT2846).

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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/S1600536809028360/at2846sup1.cif

e-65-0m979-sup1.cif (19.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809028360/at2846Isup2.hkl

e-65-0m979-Isup2.hkl (172.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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