Abstract
In the crystal structure of the title compound, [V(C12H17N2O)O2], the vanadium(V) centre is five-coordinate in a distorted square-pyramidal environment. The three atoms of the deprotonated Schiff base and a double-bonded O atom comprise the basal plane. N—H⋯O hydrogen bonds lead to a zigzag chain structure parallel to [001].
Related literature
For general background, see: Carter-Franklin et al. (2003 ▶); Eady (2003 ▶); Evangelou (2002 ▶); Mendz (1991 ▶); Mokry & Carrano (1993 ▶); Parekh et al. (2006 ▶); Rehder et al. (2002 ▶, 2003 ▶); Shahzadi et al. (2007 ▶). For related structures, see: Kwiatkowski et al. (2003 ▶, 2007 ▶); Rao et al. (1981 ▶). For synthesis, see: Kwiatkowski et al. (2003 ▶). For the calculation of square-pyramidal geometries, see: Holmes (1984 ▶).
Experimental
Crystal data
[V(C12H17N2O)O2]
M r = 288.22
Orthorhombic,
a = 11.1198 (6) Å
b = 15.7408 (8) Å
c = 7.6448 (3) Å
V = 1338.10 (11) Å3
Z = 4
Mo Kα radiation
μ = 0.74 mm−1
T = 295 (2) K
0.20 × 0.04 × 0.04 mm
Data collection
Oxford Diffraction Ruby CCD diffractometer
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008 ▶) T min = 0.941, T max = 0.964
11574 measured reflections
2126 independent reflections
1387 reflections with I > 2σ(I)
R int = 0.071
Refinement
R[F 2 > 2σ(F 2)] = 0.029
wR(F 2) = 0.051
S = 0.83
2126 reflections
167 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.19 e Å−3
Δρmin = −0.16 e Å−3
Absolute structure: Flack (1983 ▶), 849 Friedel pairs
Flack parameter: 0.23 (2)
Data collection: CrysAlis CCD (Oxford Diffraction, 2008 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2008 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEPII (Johnson, 1976 ▶); software used to prepare material for publication: SHELXL97 and PLATON (Spek, 2003 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808042839/ng2526sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808042839/ng2526Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N11—H11A⋯O14i | 0.90 | 2.08 | 2.942 (4) | 159 |
| N11—H11B⋯O15ii | 0.90 | 2.29 | 3.173 (4) | 168 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This scientific work has been supported by Funds for Science in Years 2007–2009 as a research project (N N204 0355 33 and DS/8210–4–0086–9).
supplementary crystallographic information
Comment
Vanadium(IV) and (V) complexes with Schiff bases are excellent model compounds for some biological enzymes, viz.: haloperoxidases (Carter-Franklin et al., 2003; Rehder et al., 2003), phosphomutases (Mendz, 1991) and nitrogenases (Eady, 2003). Their various pharmocological properties also has been reported, especially as an antidiabetes (Rehder et al., 2002), anticancer (Evangelou, 2002), antifungal and antibacterial (Parekh et al., 2006; Shahzadi et al., 2007) agents.
The crystal structure of (I) consists of monomeric complex molecules (Fig. 1) with a distorted square pyramidal geometry about vanadium with O15 at the apex. By the use of the dihedral angle method and the unit bond lengths, it was estimated that the structure is displaced by 76.1% along the Berry coordinate from the ideal trigonal bipyramidal (0%) toward the ideal square pyramidal (100%) geometry (Holmes, 1984). In contrast to this structure, the similar monomeric complex, but derived from 4,6-dimetoxysalicylaldehyde (Kwiatkowski et al., 2003), reveals a distorted trigonal bipyramidal environment with the degree of the distortion of 41.2% along the Berry coordinate. The vanadium atom is displaced from the mean plane passing through the four basal atoms, N8, N11, O13 and O14, by ca 0.51 (1) Å towards O15. The bond lengths V12—N8 of 2.171 (3) Å, V12—N11 of 2.118 (2) Å, V12—O13 of 1.883 (2) Å, V12—O14 of 1.635 (2) Å, V12—O15 of 1.615 (2) Å and the O=V=O angle of 109.9° are similar to the values in other cis-VO2+ complexes (Mokry & Carrano, 1993; Kwiatkowski et al., 2003; Kwiatkowski et al., 2007). The six-membered chelate ring (V12, O13, C1, C2, C7, N8) is concluded to be an envelope on V12 atom. The ring puckering analysis shows that the five-membered chelate ring defined by V12, N11, C10, C9, N8 atoms adopts a twisted conformation on C10 and N11 atoms, with P = 282.7 (2)° and Tau(M) = 49.9 (2)° for reference bond V12—N8 (Rao et al., 1981).
The crystal structure of the monomeric complex (I) is stabilized by the C—H···O, N—H···O hydrogen bonds and C—H···π interactions. Hydrogen bonds between dioxidovanadium oxygen atoms and nitrogen and carbon atoms of neighbouring molecules result in formation of infinite chains and closed loops, extending in the a direction (Tables 1 and 2, Fig. 2).
Experimental
The complex (I) were obtained in a template/complexation reactions analogous to those described for preparation of dioxidovanadium(V) complexes with Schiff base ligands (Kwiatkowski et al., 2003). A solution of 1 mmol of 2-methyl-1,2-diaminopropane in 10 ml of absolute ethanol was added under stirring to a freshly filtered solution of vanadium(V) oxytriethoxide (1 mmol) in 50 ml of absolute EtOH producing a yellow suspension of the intermediate. 2-Acetylphenol (1 mmol) dissolved in absolute EtOH was added to the aforementioned suspension. After refluxing (70 ml) of the resulting mixture for 2 h and its cooling to room temperature the separated solids were filtered off, washed several times with EtOH and dried over molecular sieves.
Refinement
All H atoms were positioned geometrically and refined using a riding model, with C–H distances of 0.93–0.97Å and with Uiso(H) = 1.2Ueq(C) (C–H = 0.96Å and Uiso(H) = 1.5Ueq(C) for the methyl group) and with N–H distances of 0.90Å and with Uiso(H) = 1.2Ueq(C).
Figures
Fig. 1.
The molecular structure of the title complex (I), with displacement ellipsoids drawn at the 25% probability level and H atoms are shown as small spheres of arbitrary radius.
Fig. 2.
The arrangement of the molecules of (I) in the crystal structure viewed approximately along a axis. The C—H···O and N—H···O hydrogen bonds are represented by dashed lines and the C—H···π interactions are represented by dotted lines.
Crystal data
| [V(C12H17N2O)O2] | F(000) = 600 |
| Mr = 288.22 | Dx = 1.431 Mg m−3 |
| Orthorhombic, Pna21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2c -2n | Cell parameters from 2126 reflections |
| a = 11.1198 (6) Å | θ = 3.2–25.1° |
| b = 15.7408 (8) Å | µ = 0.74 mm−1 |
| c = 7.6448 (3) Å | T = 295 K |
| V = 1338.10 (11) Å3 | Needle, white |
| Z = 4 | 0.2 × 0.04 × 0.04 mm |
Data collection
| Oxford Diffraction Ruby CCD diffractometer | 2126 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 1387 reflections with I > 2σ(I) |
| graphite | Rint = 0.071 |
| Detector resolution: 10.4002 pixels mm-1 | θmax = 25.1°, θmin = 3.2° |
| ω scans | h = −12→13 |
| Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2008) | k = −18→18 |
| Tmin = 0.941, Tmax = 0.964 | l = −9→7 |
| 11574 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.029 | H-atom parameters constrained |
| wR(F2) = 0.051 | w = 1/[σ2(Fo2) + (0.0211P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 0.83 | (Δ/σ)max < 0.001 |
| 2126 reflections | Δρmax = 0.19 e Å−3 |
| 167 parameters | Δρmin = −0.16 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 849 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.23 (2) |
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 takeninto account individually in the estimation of e.s.d.'s in distances, anglesand torsion angles; correlations between e.s.d.'s in cell parameters are onlyused 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 andgoodness of fit S are based on F2, conventional R-factors R are basedon F, with F set to zero for negative F2. The threshold expression ofF2 > σ(F2) is used only for calculating R-factors(gt) etc. and isnot relevant to the choice of reflections for refinement. R-factors basedon 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 | 0.3317 (3) | 0.3973 (2) | 0.5333 (4) | 0.0380 (8) | |
| C2 | 0.2695 (3) | 0.37563 (19) | 0.6865 (4) | 0.0354 (8) | |
| C3 | 0.3314 (3) | 0.37812 (17) | 0.8474 (6) | 0.0512 (8) | |
| H3A | 0.2903 | 0.3651 | 0.9499 | 0.061* | |
| C4 | 0.4498 (3) | 0.3992 (2) | 0.8561 (6) | 0.0560 (10) | |
| H4A | 0.4887 | 0.4012 | 0.9637 | 0.067* | |
| C5 | 0.5121 (3) | 0.4175 (2) | 0.7045 (6) | 0.0602 (11) | |
| H5A | 0.5931 | 0.4319 | 0.7101 | 0.072* | |
| C6 | 0.4544 (3) | 0.4145 (2) | 0.5448 (5) | 0.0510 (10) | |
| H6A | 0.4982 | 0.4240 | 0.4431 | 0.061* | |
| C7 | 0.1437 (3) | 0.34815 (19) | 0.6801 (4) | 0.0399 (8) | |
| N8 | 0.0753 (2) | 0.36544 (15) | 0.5463 (3) | 0.0378 (7) | |
| C9 | −0.0510 (3) | 0.3371 (2) | 0.5463 (4) | 0.0422 (9) | |
| H9A | −0.0956 | 0.3677 | 0.6353 | 0.051* | |
| H9B | −0.0549 | 0.2770 | 0.5733 | 0.051* | |
| C10 | −0.1063 (3) | 0.3534 (2) | 0.3683 (4) | 0.0407 (9) | |
| N11 | −0.06106 (19) | 0.44045 (15) | 0.3205 (5) | 0.0408 (6) | |
| H11A | −0.0946 | 0.4790 | 0.3925 | 0.049* | |
| H11B | −0.0844 | 0.4528 | 0.2107 | 0.049* | |
| V12 | 0.12859 (4) | 0.45059 (3) | 0.33674 (6) | 0.03758 (15) | |
| O13 | 0.27910 (18) | 0.39910 (13) | 0.3758 (3) | 0.0456 (6) | |
| O14 | 0.1359 (2) | 0.45725 (14) | 0.1236 (2) | 0.0467 (6) | |
| O15 | 0.1372 (2) | 0.54432 (13) | 0.4218 (2) | 0.0483 (6) | |
| C26 | 0.0950 (3) | 0.29854 (18) | 0.8337 (6) | 0.0592 (9) | |
| H26A | 0.0162 | 0.2776 | 0.8060 | 0.089* | |
| H26B | 0.0905 | 0.3349 | 0.9343 | 0.089* | |
| H26C | 0.1474 | 0.2516 | 0.8584 | 0.089* | |
| C27 | −0.0620 (3) | 0.2904 (2) | 0.2305 (5) | 0.0536 (9) | |
| H27A | 0.0243 | 0.2886 | 0.2320 | 0.080* | |
| H27B | −0.0890 | 0.3081 | 0.1170 | 0.080* | |
| H27C | −0.0933 | 0.2349 | 0.2559 | 0.080* | |
| C28 | −0.2434 (3) | 0.3536 (2) | 0.3770 (5) | 0.0699 (12) | |
| H28A | −0.2697 | 0.3960 | 0.4587 | 0.105* | |
| H28B | −0.2713 | 0.2988 | 0.4143 | 0.105* | |
| H28C | −0.2756 | 0.3661 | 0.2633 | 0.105* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.039 (2) | 0.0260 (19) | 0.049 (2) | 0.0093 (17) | 0.0054 (19) | 0.0025 (17) |
| C2 | 0.041 (2) | 0.0303 (19) | 0.035 (2) | 0.0077 (17) | 0.0034 (17) | −0.0038 (16) |
| C3 | 0.064 (2) | 0.0462 (19) | 0.043 (2) | 0.0081 (17) | 0.007 (3) | 0.005 (3) |
| C4 | 0.058 (3) | 0.056 (2) | 0.054 (3) | 0.0082 (19) | −0.009 (3) | −0.016 (3) |
| C5 | 0.039 (2) | 0.053 (3) | 0.089 (3) | −0.0058 (19) | −0.002 (3) | −0.005 (2) |
| C6 | 0.050 (3) | 0.051 (2) | 0.052 (2) | 0.001 (2) | 0.009 (2) | 0.003 (2) |
| C7 | 0.056 (2) | 0.0311 (19) | 0.033 (2) | 0.0004 (19) | 0.0127 (18) | −0.0038 (14) |
| N8 | 0.0384 (19) | 0.0394 (17) | 0.0355 (16) | 0.0009 (14) | 0.0112 (14) | −0.0026 (14) |
| C9 | 0.053 (3) | 0.039 (2) | 0.0346 (19) | −0.0049 (19) | 0.0174 (18) | −0.0038 (17) |
| C10 | 0.038 (2) | 0.0445 (19) | 0.040 (2) | −0.0079 (17) | 0.0074 (17) | −0.0095 (18) |
| N11 | 0.0423 (14) | 0.0400 (14) | 0.0400 (13) | 0.0048 (13) | −0.0037 (18) | −0.0058 (18) |
| V12 | 0.0404 (3) | 0.0357 (3) | 0.0366 (3) | 0.0011 (3) | 0.0062 (4) | 0.0047 (4) |
| O13 | 0.0417 (13) | 0.0517 (14) | 0.0434 (17) | 0.0064 (10) | 0.0104 (11) | 0.0074 (12) |
| O14 | 0.0508 (14) | 0.0579 (14) | 0.0315 (11) | 0.0065 (16) | 0.0078 (11) | 0.0070 (11) |
| O15 | 0.0559 (16) | 0.0353 (13) | 0.0538 (12) | −0.0029 (13) | 0.0005 (11) | −0.0044 (11) |
| C26 | 0.082 (3) | 0.0554 (19) | 0.0399 (16) | −0.0127 (18) | 0.015 (3) | 0.005 (3) |
| C27 | 0.067 (2) | 0.047 (2) | 0.0469 (18) | −0.008 (2) | 0.013 (2) | −0.007 (2) |
| C28 | 0.046 (2) | 0.085 (3) | 0.078 (3) | −0.017 (2) | 0.004 (2) | −0.004 (3) |
Geometric parameters (Å, °)
| C1—O13 | 1.339 (4) | C10—N11 | 1.504 (4) |
| C1—C6 | 1.393 (5) | C10—C28 | 1.527 (4) |
| C1—C2 | 1.402 (4) | C10—C27 | 1.529 (4) |
| C2—C3 | 1.410 (5) | N11—V12 | 2.118 (2) |
| C2—C7 | 1.465 (4) | N11—H11A | 0.9000 |
| C3—C4 | 1.359 (4) | N11—H11B | 0.9000 |
| C3—H3A | 0.9300 | V12—O15 | 1.6151 (19) |
| C4—C5 | 1.380 (5) | V12—O14 | 1.6352 (18) |
| C4—H4A | 0.9300 | V12—O13 | 1.883 (2) |
| C5—C6 | 1.380 (4) | C26—H26A | 0.9600 |
| C5—H5A | 0.9300 | C26—H26B | 0.9600 |
| C6—H6A | 0.9300 | C26—H26C | 0.9600 |
| C7—N8 | 1.304 (4) | C27—H27A | 0.9600 |
| C7—C26 | 1.510 (4) | C27—H27B | 0.9600 |
| N8—C9 | 1.473 (4) | C27—H27C | 0.9600 |
| N8—V12 | 2.171 (3) | C28—H28A | 0.9600 |
| C9—C10 | 1.515 (4) | C28—H28B | 0.9600 |
| C9—H9A | 0.9700 | C28—H28C | 0.9600 |
| C9—H9B | 0.9700 | ||
| O13—C1—C6 | 118.7 (3) | C10—N11—V12 | 112.76 (17) |
| O13—C1—C2 | 122.7 (3) | C10—N11—H11A | 109.0 |
| C6—C1—C2 | 118.5 (3) | V12—N11—H11A | 109.0 |
| C1—C2—C3 | 118.7 (3) | C10—N11—H11B | 109.0 |
| C1—C2—C7 | 121.0 (3) | V12—N11—H11B | 109.0 |
| C3—C2—C7 | 120.2 (3) | H11A—N11—H11B | 107.8 |
| C4—C3—C2 | 121.5 (4) | O15—V12—O14 | 109.85 (10) |
| C4—C3—H3A | 119.2 | O15—V12—O13 | 106.06 (11) |
| C2—C3—H3A | 119.2 | O14—V12—O13 | 98.12 (10) |
| C3—C4—C5 | 119.7 (4) | O15—V12—N11 | 98.71 (11) |
| C3—C4—H4A | 120.1 | O14—V12—N11 | 89.77 (13) |
| C5—C4—H4A | 120.1 | O13—V12—N11 | 149.49 (10) |
| C6—C5—C4 | 120.1 (4) | O15—V12—N8 | 106.46 (9) |
| C6—C5—H5A | 119.9 | O14—V12—N8 | 142.05 (11) |
| C4—C5—H5A | 119.9 | O13—V12—N8 | 81.94 (9) |
| C5—C6—C1 | 121.2 (3) | N11—V12—N8 | 74.05 (12) |
| C5—C6—H6A | 119.4 | C1—O13—V12 | 122.65 (18) |
| C1—C6—H6A | 119.4 | C7—C26—H26A | 109.5 |
| N8—C7—C2 | 121.4 (3) | C7—C26—H26B | 109.5 |
| N8—C7—C26 | 120.6 (3) | H26A—C26—H26B | 109.5 |
| C2—C7—C26 | 118.0 (3) | C7—C26—H26C | 109.5 |
| C7—N8—C9 | 119.5 (3) | H26A—C26—H26C | 109.5 |
| C7—N8—V12 | 123.3 (2) | H26B—C26—H26C | 109.5 |
| C9—N8—V12 | 116.56 (19) | C10—C27—H27A | 109.5 |
| N8—C9—C10 | 109.6 (2) | C10—C27—H27B | 109.5 |
| N8—C9—H9A | 109.8 | H27A—C27—H27B | 109.5 |
| C10—C9—H9A | 109.8 | C10—C27—H27C | 109.5 |
| N8—C9—H9B | 109.8 | H27A—C27—H27C | 109.5 |
| C10—C9—H9B | 109.8 | H27B—C27—H27C | 109.5 |
| H9A—C9—H9B | 108.2 | C10—C28—H28A | 109.5 |
| N11—C10—C9 | 103.7 (3) | C10—C28—H28B | 109.5 |
| N11—C10—C28 | 110.0 (2) | H28A—C28—H28B | 109.5 |
| C9—C10—C28 | 111.5 (3) | C10—C28—H28C | 109.5 |
| N11—C10—C27 | 108.4 (3) | H28A—C28—H28C | 109.5 |
| C9—C10—C27 | 112.2 (3) | H28B—C28—H28C | 109.5 |
| C28—C10—C27 | 110.7 (3) | ||
| O13—C1—C2—C3 | −178.0 (3) | N8—C9—C10—C27 | 74.2 (3) |
| C6—C1—C2—C3 | 4.6 (4) | C9—C10—N11—V12 | 53.3 (3) |
| O13—C1—C2—C7 | 4.0 (4) | C28—C10—N11—V12 | 172.7 (2) |
| C6—C1—C2—C7 | −173.4 (3) | C27—C10—N11—V12 | −66.2 (3) |
| C1—C2—C3—C4 | −1.5 (4) | C10—N11—V12—O15 | −139.7 (2) |
| C7—C2—C3—C4 | 176.6 (3) | C10—N11—V12—O14 | 110.2 (3) |
| C2—C3—C4—C5 | −0.9 (5) | C10—N11—V12—O13 | 4.5 (4) |
| C3—C4—C5—C6 | 0.0 (5) | C10—N11—V12—N8 | −35.0 (2) |
| C4—C5—C6—C1 | 3.4 (6) | C7—N8—V12—O15 | −66.8 (3) |
| O13—C1—C6—C5 | 176.9 (3) | C9—N8—V12—O15 | 103.9 (2) |
| C2—C1—C6—C5 | −5.6 (5) | C7—N8—V12—O14 | 130.5 (2) |
| C1—C2—C7—N8 | −20.0 (4) | C9—N8—V12—O14 | −58.7 (3) |
| C3—C2—C7—N8 | 162.0 (3) | C7—N8—V12—O13 | 37.6 (2) |
| C1—C2—C7—C26 | 159.8 (3) | C9—N8—V12—O13 | −151.6 (2) |
| C3—C2—C7—C26 | −18.2 (4) | C7—N8—V12—N11 | −161.4 (3) |
| C2—C7—N8—C9 | −179.5 (3) | C9—N8—V12—N11 | 9.3 (2) |
| C26—C7—N8—C9 | 0.8 (4) | C6—C1—O13—V12 | −136.7 (2) |
| C2—C7—N8—V12 | −9.0 (4) | C2—C1—O13—V12 | 45.9 (4) |
| C26—C7—N8—V12 | 171.2 (2) | O15—V12—O13—C1 | 50.2 (2) |
| C7—N8—C9—C10 | −172.0 (3) | O14—V12—O13—C1 | 163.6 (2) |
| V12—N8—C9—C10 | 16.9 (3) | N11—V12—O13—C1 | −92.8 (3) |
| N8—C9—C10—N11 | −42.6 (3) | N8—V12—O13—C1 | −54.7 (2) |
| N8—C9—C10—C28 | −161.0 (3) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N11—H11A···O14i | 0.90 | 2.08 | 2.942 (4) | 159 |
| N11—H11B···O15ii | 0.90 | 2.29 | 3.173 (4) | 168 |
| C26—H26B···O14iii | 0.96 | 2.46 | 3.370 (4) | 158 |
Symmetry codes: (i) −x, −y+1, z+1/2; (ii) −x, −y+1, z−1/2; (iii) x, y, z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2526).
References
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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/S1600536808042839/ng2526sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536808042839/ng2526Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


