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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Apr 8;65(Pt 5):m487–m488. doi: 10.1107/S1600536809011982

Tetra­aqua­bis(3,5-di-4-pyridyl-1,2,4-triazolato-κN)cobalt(II) dihydrate

Lin Yi Dong a,*
PMCID: PMC2977553  PMID: 21583739

Abstract

The CoII atom in the title compound, [Co(C12H8N5)2(H2O)4]·2H2O, lies on a center of inversion and is bonded to two N-heterocycles and to four water mol­ecules in a slightly distorted octahedral coordination. The coordinated and lattice water mol­ecules inter­act with the N-heterocycles through O—H⋯N hydrogen bonds, generating a three-dimensional supra­molecular architecture.

Related literature

For magnetic studies of transition metal complexes with 1,2,4-triazole derivatives, see: Haasnoot (2000). For the potential applications of complexes containing substituted 1,2,4-triazole ligands with spin-crossover properties in mol­ecular-based memory devices, displays and optical switches, see: Kahn & Martinez (1998). For 3,5-di(4-pyridine)-1,2,4-triazole, see: Zhang et al. (2006); Sreenivasulu & Vittal (2004). For the structure of water, see: Tajkhorshid et al. (2002). For the synthesis, see: Basu & Dutta (1964). For a trinuclear water cluster, see: König (1944).graphic file with name e-65-0m487-scheme1.jpg

Experimental

Crystal data

  • [Co(C12H8N5)2(H2O)4]·2H2O

  • M r = 611.49

  • Monoclinic, Inline graphic

  • a = 7.3660 (15) Å

  • b = 15.654 (3) Å

  • c = 11.857 (2) Å

  • β = 107.34 (3)°

  • V = 1305.1 (5) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.72 mm−1

  • T = 293 K

  • 0.40 × 0.20 × 0.12 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.842, T max = 0.917

  • 11054 measured reflections

  • 2423 independent reflections

  • 2009 reflections with I > 2σ(I)

  • R int = 0.065

Refinement

  • R[F 2 > 2σ(F 2)] = 0.054

  • wR(F 2) = 0.108

  • S = 1.07

  • 2420 reflections

  • 243 parameters

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

  • Δρmax = 0.29 e Å−3

  • Δρmin = −0.41 e Å−3

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT; program(s) used to solve structure: SHELXL97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 1999); software used to prepare material for publication: publCIF (Westrip, 2009).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809011982/ng2566sup1.cif

e-65-0m487-sup1.cif (18.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809011982/ng2566Isup2.hkl

e-65-0m487-Isup2.hkl (118.9KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

Co1—O1 2.100 (2)
Co1—O2 2.126 (2)
Co1—N1 2.134 (3)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
O1—H1A⋯N3ii 0.851 (10) 2.42 (3) 3.070 (4) 134 (3)
O1—H1A⋯N4ii 0.851 (10) 1.966 (12) 2.803 (4) 167 (4)
O1—H1B⋯O3iii 0.852 (10) 1.99 (2) 2.791 (4) 155 (3)
O2—H2A⋯O3 0.851 (10) 1.973 (14) 2.801 (4) 164 (3)
O2—H2B⋯N3iv 0.850 (10) 1.973 (19) 2.792 (4) 161 (5)
O2—H2B⋯N4iv 0.850 (10) 2.60 (4) 3.220 (4) 130 (4)
O3—H3A⋯N2v 0.852 (10) 2.077 (12) 2.926 (4) 174 (4)
O3—H3B⋯N5vi 0.849 (10) 1.950 (14) 2.786 (4) 168 (5)

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

supplementary crystallographic information

Comment

Transition metal complexes with 1,2,4-triazole derivatives as ligands are of great interest as they are the subject of magnetic studies (Haasnoot, 2000). Some complexes containing substituted 1,2,4-triazole ligands have spin-crossover properties, which could be used in molecular-based memory devices, displays and optical switches (Kahn & Martinez, 1998). The ligand 3,5-di(4-pyridine)-1,2,4-triazole (L) is of special interest as it contains multi-dentate donor atoms and shows diverse coordination modes.. Especially only a few examples about the coordinaiton chemistry of L are reported. Some unusual coordination modes of L also have been reported forming interesting supramolecular isomerism systems (Zhang et al., 2006). On the other hand, water is quite important for our common life (Tajkhorshid et al., 2002). It has been the focus of intense research interests for their unusual properties in biological system and also plays an important role in biological self-assembly processes (Sreenivasulu & Vittal, 2004).

In this work, we synthesized a new compound [Co(L)2(H2O)4](H2O)2 (I) (L = 3,5-di(4-pyridine)-1,2,4-triazole). 1 is composed of one cobalt(II) cation, two L ligand, four coordinated and two lattice water molecules. The cobalt(II) cation is six-coordinated in the octahedral geometry. The equatorial site of Cobalt cation is occupied by four aqua molecules while the axial site is occupied by two nitrogen atoms of two mono-dentate L ligands. The mono-dentate coordination mode of L is different from previously reported di-, tri- or tetra-dentate coordination modes of L.

O1, O2 from coordination water molecules and O3 from lattice water molecules generate strong intermolecular hydrogen bondings and construct trinuclear water clusters, in which O3 acts as the hydrogen acceptors and O1, O2 act as hydrogen bonding donors. The hydrogen-bonding distances are 2.791 (4) Å (O1—H1B···O3) and 2.801 (4) Å(O2—H2A···O3), respectively. The average O···O distance is 2.796 (4) Å, which is similar to that(2.75 Å) in the structure of ice (König, 1944).

strong N—H···O hydrogen bonds generated from water molecules and nitrogen atoms of pyridine or triazole groups are also observed rusulting in the three-dimensional supramolecular network(Table 2). π-π stacking interactions between two neighboring triazole groups further consolidating the architecture centroid-centroid distance 3.677 (4) Å]

Perspective drawing with the atomic numbering scheme is illustrated in figure 1. Selected geometric parameters (Å, °) for 1 are listed in table 1. Selected hydrogen-bonding geometric parameters (Å, °) for 1 are listed in table 2. The trinuclear water clusters, corresponding N—H···O hydrogen bonds and π-π stacking are shown in figure 2. The three-dimensional supramolecular packing architecture of (I) is shown in figure 3.

Experimental

The ligand was prepared according to the previous literature (Basu & Dutta, (1964)). [Co(L)2(H2O)4](H2O) (1) (L = 3,5-di(4-pyridine)-1,2,4-triazole) was prepared under the hydrotheraml conditions. [Co(ClO4)2].6H2O (0.2 mmol), L (0.2 mmol) and 18 ml water was added to a 25 ml reaction vessel. the reaction vessel was then sealed and subsequently placed in an oven for 140 h at 160°C. well shaped red block crystals were obtained and washed with ethanol.

Refinement

The carbon-bound H atoms were positioned geometrically and were allowed to ride on their parent C atoms. The water H atoms were located from a difference density map and were refined with distance restraints of O—H = 0.85±0.01 Å.

Figures

Fig. 1.

Fig. 1.

The molecular structure and atom-labeling scheme of (I).

Fig. 2.

Fig. 2.

The trinuclear water clusters stabling the packing structure of 1.

Crystal data

[Co(C12H8N5)2(H2O)4]·2(H2O) F(000) = 634
Mr = 611.49 Dx = 1.556 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 556 reflections
a = 7.3660 (15) Å θ = 1.5–25.5°
b = 15.654 (3) Å µ = 0.72 mm1
c = 11.857 (2) Å T = 293 K
β = 107.34 (3)° Block, red
V = 1305.1 (5) Å3 0.40 × 0.20 × 0.12 mm
Z = 2

Data collection

Bruker SMART CCD area-detector diffractometer 2423 independent reflections
Radiation source: fine-focus sealed tube 2009 reflections with I > 2σ(I)
graphite Rint = 0.065
φ and ω scans θmax = 25.5°, θmin = 3.2°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −8→8
Tmin = 0.842, Tmax = 0.917 k = −18→18
11054 measured reflections l = −14→14

Refinement

Refinement on F2 0 restraints
Least-squares matrix: full H atoms treated by a mixture of independent and constrained refinement
R[F2 > 2σ(F2)] = 0.054 w = 1/[σ2(Fo2) + (0.0298P)2 + 0.2298P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.108 (Δ/σ)max < 0.001
S = 1.07 Δρmax = 0.29 e Å3
2420 reflections Δρmin = −0.41 e Å3
243 parameters

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
C1 0.3827 (5) 0.6826 (2) −0.0776 (3) 0.0306 (8)
C2 0.3536 (5) 0.7690 (2) −0.0713 (3) 0.0299 (8)
C3 0.3919 (4) 0.80864 (19) 0.0377 (3) 0.0218 (7)
C4 0.4634 (5) 0.7565 (2) 0.1360 (3) 0.0290 (8)
C5 0.4886 (5) 0.6711 (2) 0.1224 (3) 0.0294 (8)
C6 0.3518 (5) 0.8987 (2) 0.0514 (3) 0.0229 (7)
C7 0.2496 (5) 1.02433 (19) 0.0220 (3) 0.0241 (7)
C8 0.1690 (5) 1.1049 (2) −0.0324 (3) 0.0244 (7)
C9 0.1117 (5) 1.1170 (2) −0.1528 (3) 0.0330 (9)
C10 0.0440 (6) 1.1952 (2) −0.1990 (3) 0.0368 (9)
C11 0.0861 (6) 1.2510 (3) −0.0181 (4) 0.0450 (11)
C12 0.1540 (6) 1.1751 (2) 0.0357 (4) 0.0403 (10)
Co1 0.5000 0.5000 0.0000 0.02203 (19)
H1 0.363 (5) 0.657 (2) −0.147 (3) 0.033 (10)*
H2 0.313 (5) 0.799 (3) −0.138 (3) 0.046 (12)*
H4 0.495 (5) 0.781 (2) 0.209 (3) 0.034 (10)*
H5 0.532 (5) 0.637 (2) 0.187 (3) 0.036 (10)*
H9 0.118 (5) 1.075 (2) −0.199 (3) 0.028 (10)*
H10 0.013 (6) 1.203 (3) −0.278 (4) 0.052 (13)*
H11 0.078 (6) 1.299 (3) 0.026 (4) 0.057 (13)*
H12 0.188 (6) 1.170 (3) 0.116 (4) 0.051 (12)*
H1A 0.261 (5) 0.484 (3) −0.2116 (18) 0.069 (16)*
H2A 0.276 (4) 0.5057 (16) 0.135 (3) 0.031 (10)*
H3A 0.163 (5) 0.571 (2) 0.2816 (10) 0.041 (12)*
H1B 0.143 (3) 0.475 (3) −0.140 (3) 0.077 (17)*
H2B 0.416 (6) 0.446 (3) 0.1861 (19) 0.084 (18)*
H3B 0.081 (6) 0.6269 (11) 0.194 (4) 0.069 (16)*
N1 0.4483 (4) 0.63277 (16) 0.0175 (2) 0.0262 (6)
N2 0.2624 (4) 0.95193 (16) −0.0378 (2) 0.0229 (6)
N3 0.3929 (4) 0.93481 (17) 0.1575 (2) 0.0295 (7)
N4 0.3253 (4) 1.01645 (17) 0.1389 (2) 0.0308 (7)
N5 0.0298 (4) 1.26290 (18) −0.1346 (3) 0.0371 (8)
O1 0.2504 (3) 0.49368 (17) −0.1431 (2) 0.0334 (6)
O2 0.3487 (4) 0.46767 (16) 0.1212 (2) 0.0302 (6)
O3 0.1157 (4) 0.57516 (16) 0.2069 (2) 0.0329 (6)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.047 (2) 0.0220 (18) 0.0201 (18) 0.0038 (16) 0.0054 (16) −0.0033 (15)
C2 0.044 (2) 0.0184 (17) 0.0245 (19) 0.0057 (15) 0.0057 (16) 0.0020 (15)
C3 0.0241 (18) 0.0184 (16) 0.0231 (17) 0.0017 (13) 0.0074 (14) −0.0003 (13)
C4 0.043 (2) 0.0239 (18) 0.0188 (18) 0.0052 (16) 0.0075 (16) −0.0032 (15)
C5 0.043 (2) 0.0200 (18) 0.0232 (19) 0.0050 (15) 0.0065 (16) 0.0043 (14)
C6 0.0277 (18) 0.0182 (16) 0.0224 (17) −0.0006 (14) 0.0066 (14) 0.0000 (13)
C7 0.0297 (18) 0.0194 (17) 0.0227 (17) −0.0001 (13) 0.0072 (14) 0.0002 (13)
C8 0.0247 (18) 0.0211 (17) 0.0269 (18) −0.0023 (14) 0.0067 (14) −0.0009 (14)
C9 0.044 (2) 0.0231 (19) 0.028 (2) 0.0046 (16) 0.0043 (17) −0.0031 (16)
C10 0.044 (2) 0.033 (2) 0.027 (2) 0.0034 (17) 0.0023 (18) 0.0073 (17)
C11 0.067 (3) 0.024 (2) 0.045 (3) 0.013 (2) 0.017 (2) −0.0019 (18)
C12 0.065 (3) 0.027 (2) 0.028 (2) 0.0129 (18) 0.011 (2) 0.0002 (16)
Co1 0.0282 (4) 0.0162 (3) 0.0206 (3) 0.0025 (3) 0.0055 (2) 0.0004 (3)
N1 0.0358 (17) 0.0170 (14) 0.0251 (15) 0.0032 (12) 0.0081 (12) −0.0001 (11)
N2 0.0283 (15) 0.0154 (14) 0.0241 (15) 0.0011 (11) 0.0063 (12) −0.0011 (11)
N3 0.0398 (18) 0.0213 (15) 0.0255 (16) 0.0099 (13) 0.0065 (13) 0.0017 (12)
N4 0.0461 (18) 0.0213 (16) 0.0221 (15) 0.0069 (13) 0.0057 (13) −0.0013 (11)
N5 0.044 (2) 0.0223 (16) 0.044 (2) 0.0079 (14) 0.0115 (16) 0.0055 (14)
O1 0.0312 (14) 0.0408 (15) 0.0264 (14) −0.0029 (13) 0.0058 (10) −0.0009 (12)
O2 0.0346 (15) 0.0295 (13) 0.0296 (14) 0.0062 (11) 0.0142 (12) 0.0021 (11)
O3 0.0436 (16) 0.0239 (14) 0.0286 (15) 0.0017 (12) 0.0067 (12) 0.0018 (11)

Geometric parameters (Å, °)

C1—N1 1.337 (4) C10—N5 1.328 (5)
C1—C2 1.376 (5) C10—H10 0.90 (4)
C1—H1 0.89 (4) C11—N5 1.331 (5)
C2—C3 1.385 (5) C11—C12 1.370 (5)
C2—H2 0.89 (4) C11—H11 0.93 (4)
C3—C4 1.392 (5) C12—H12 0.92 (4)
C3—C6 1.459 (4) Co1—O1i 2.100 (2)
C4—C5 1.365 (5) Co1—O1 2.100 (2)
C4—H4 0.91 (4) Co1—O2i 2.126 (2)
C5—N1 1.332 (4) Co1—O2 2.126 (2)
C5—H5 0.91 (4) Co1—N1i 2.134 (3)
C6—N3 1.329 (4) Co1—N1 2.134 (3)
C6—N2 1.354 (4) N3—N4 1.365 (4)
C7—N4 1.336 (4) O1—H1A 0.851 (10)
C7—N2 1.355 (4) O1—H1B 0.852 (10)
C7—C8 1.459 (4) O2—H2A 0.851 (10)
C8—C9 1.377 (5) O2—H2B 0.850 (10)
C8—C12 1.387 (5) O3—H3A 0.852 (10)
C9—C10 1.373 (5) O3—H3B 0.849 (10)
C9—H9 0.87 (4)
N1—C1—C2 123.4 (3) C11—C12—C8 119.8 (4)
N1—C1—H1 116 (2) C11—C12—H12 121 (3)
C2—C1—H1 121 (2) C8—C12—H12 120 (3)
C1—C2—C3 120.0 (3) O1i—Co1—O1 180.0
C1—C2—H2 119 (3) O1i—Co1—O2i 91.47 (10)
C3—C2—H2 121 (3) O1—Co1—O2i 88.53 (10)
C2—C3—C4 116.1 (3) O1i—Co1—O2 88.53 (10)
C2—C3—C6 123.0 (3) O1—Co1—O2 91.47 (10)
C4—C3—C6 120.8 (3) O2i—Co1—O2 180.0
C5—C4—C3 120.4 (3) O1i—Co1—N1i 89.19 (10)
C5—C4—H4 122 (2) O1—Co1—N1i 90.81 (10)
C3—C4—H4 118 (2) O2i—Co1—N1i 91.23 (10)
N1—C5—C4 123.5 (3) O2—Co1—N1i 88.77 (10)
N1—C5—H5 116 (2) O1i—Co1—N1 90.81 (10)
C4—C5—H5 120 (2) O1—Co1—N1 89.19 (10)
N3—C6—N2 113.4 (3) O2i—Co1—N1 88.77 (10)
N3—C6—C3 121.3 (3) O2—Co1—N1 91.23 (10)
N2—C6—C3 125.1 (3) N1i—Co1—N1 180.0
N4—C7—N2 113.1 (3) C5—N1—C1 116.7 (3)
N4—C7—C8 121.8 (3) C5—N1—Co1 122.2 (2)
N2—C7—C8 125.0 (3) C1—N1—Co1 121.0 (2)
C9—C8—C12 116.1 (3) C6—N2—C7 101.5 (3)
C9—C8—C7 122.5 (3) C6—N3—N4 106.0 (2)
C12—C8—C7 121.3 (3) C7—N4—N3 105.8 (2)
C10—C9—C8 120.0 (3) C10—N5—C11 115.6 (3)
C10—C9—H9 120 (2) Co1—O1—H1A 118 (3)
C8—C9—H9 120 (2) Co1—O1—H1B 126 (3)
N5—C10—C9 124.3 (4) H1A—O1—H1B 109.1 (17)
N5—C10—H10 117 (3) Co1—O2—H2A 117 (2)
C9—C10—H10 119 (3) Co1—O2—H2B 115 (3)
N5—C11—C12 124.2 (4) H2A—O2—H2B 109.4 (15)
N5—C11—H11 115 (3) H3A—O3—H3B 106 (4)
C12—C11—H11 121 (3)
N1—C1—C2—C3 −0.3 (6) C2—C1—N1—Co1 −177.5 (3)
C1—C2—C3—C4 1.4 (5) O1i—Co1—N1—C5 −36.4 (3)
C1—C2—C3—C6 −175.5 (3) O1—Co1—N1—C5 143.6 (3)
C2—C3—C4—C5 −1.3 (5) O2i—Co1—N1—C5 −127.9 (3)
C6—C3—C4—C5 175.6 (3) O2—Co1—N1—C5 52.1 (3)
C3—C4—C5—N1 0.1 (6) N1i—Co1—N1—C5 −122 (27)
C2—C3—C6—N3 −179.1 (3) O1i—Co1—N1—C1 140.0 (3)
C4—C3—C6—N3 4.2 (5) O1—Co1—N1—C1 −40.0 (3)
C2—C3—C6—N2 4.7 (5) O2i—Co1—N1—C1 48.5 (3)
C4—C3—C6—N2 −172.0 (3) O2—Co1—N1—C1 −131.5 (3)
N4—C7—C8—C9 171.9 (3) N1i—Co1—N1—C1 55 (27)
N2—C7—C8—C9 −5.8 (5) N3—C6—N2—C7 −0.6 (4)
N4—C7—C8—C12 −5.0 (5) C3—C6—N2—C7 175.9 (3)
N2—C7—C8—C12 177.3 (3) N4—C7—N2—C6 0.0 (4)
C12—C8—C9—C10 −0.2 (6) C8—C7—N2—C6 177.9 (3)
C7—C8—C9—C10 −177.4 (3) N2—C6—N3—N4 0.8 (4)
C8—C9—C10—N5 0.5 (6) C3—C6—N3—N4 −175.7 (3)
N5—C11—C12—C8 0.6 (7) N2—C7—N4—N3 0.5 (4)
C9—C8—C12—C11 −0.3 (6) C8—C7—N4—N3 −177.5 (3)
C7—C8—C12—C11 176.9 (4) C6—N3—N4—C7 −0.8 (4)
C4—C5—N1—C1 1.1 (5) C9—C10—N5—C11 −0.2 (6)
C4—C5—N1—Co1 177.6 (3) C12—C11—N5—C10 −0.3 (6)
C2—C1—N1—C5 −1.0 (5)

Symmetry codes: (i) −x+1, −y+1, −z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1—H1A···N3ii 0.85 (1) 2.42 (3) 3.070 (4) 134 (3)
O1—H1A···N4ii 0.85 (1) 1.97 (1) 2.803 (4) 167 (4)
O1—H1B···O3iii 0.85 (1) 1.99 (2) 2.791 (4) 155 (3)
O2—H2A···O3 0.85 (1) 1.97 (1) 2.801 (4) 164 (3)
O2—H2B···N3iv 0.85 (1) 1.97 (2) 2.792 (4) 161 (5)
O2—H2B···N4iv 0.85 (1) 2.60 (4) 3.220 (4) 130 (4)
O3—H3A···N2v 0.85 (1) 2.08 (1) 2.926 (4) 174 (4)
O3—H3B···N5vi 0.85 (1) 1.95 (1) 2.786 (4) 168 (5)

Symmetry codes: (ii) x, −y+3/2, z−1/2; (iii) −x, −y+1, −z; (iv) −x+1, y−1/2, −z+1/2; (v) x, −y+3/2, z+1/2; (vi) −x, −y+2, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2566).

References

  1. Basu, U. P. & Dutta, S. (1964). J. Org. Chem.30, 3562–3564. [DOI] [PubMed]
  2. Brandenburg, K. (1999). DIAMOND Crystal Impact GbR, Bonn, Germany.
  3. Bruker (1997). SAINT and SMART Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Haasnoot, J. G. (2000). Coord. Chem. Rev.200–202, 131–185.
  5. Kahn, O. & Martinez, C. J. (1998). Science, 279, 44–48.
  6. König, H. A. Z. (1944). Z. Kristallogr.105, 279–286.
  7. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  8. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  9. Sreenivasulu, B. & Vittal, J. J. (2004). Angew. Chem. Int. Ed.43, 5769–5772. [DOI] [PubMed]
  10. Tajkhorshid, E., Nollert, P., Jensen, M., Miercke, L. J. W., Connell, J. O., Stroud, R. M. & Schulten, K. (2002). Science, 296, 525–530. [DOI] [PubMed]
  11. Westrip (2009). publCIF In preparation.
  12. Zhang, J. P., Lin, Y. Y., Huang, X. C. & Chen, X. M. (2006). Cryst. Growth Des.6, 519–523.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809011982/ng2566sup1.cif

e-65-0m487-sup1.cif (18.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809011982/ng2566Isup2.hkl

e-65-0m487-Isup2.hkl (118.9KB, hkl)

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


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