Abstract
The whole molecule of the title complex, [Pd(C15H21N2S2)2], is generated by twofold rotational symmetry. The palladium(II) atom exhibits a square-planar coordination geometry, and is located on the crystallographic twofold axis that induces a cis configuration of the N,S chelating ligands. In the crystal, molecules stack along the c-axis direction and there are no significant intermolecular interactions present. The structure was refined as an inversion twin with a final BASF parameter of 0.34 (2).
Keywords: crystal structure, palladium(II) complex, cis-ligand configuration
Related literature
For the crystal structures of the free Schiff base ligand and of its NiII complex, see: Howlader et al. (2015a
▸,b
▸). For similar bis(dithiocarbazato)Pd complexes with a cis configuration of the azomethine N and thiolate S atoms, see: Ali et al. (2002 ▸); Liu et al. (2011 ▸); Duan et al. (1998 ▸); Tampouris et al. (2007 ▸). For complexes with a trans configuration, see: Khaledi & Mohd Ali (2011 ▸); Tampouris et al. (2007 ▸); Tarafder et al. (2010 ▸).
Experimental
Crystal data
[Pd(C15H21N2S2)2]
M r = 693.32
Monoclinic,
a = 18.3559 (11) Å
b = 9.6747 (5) Å
c = 10.3368 (6) Å
β = 116.810 (2)°
V = 1638.37 (16) Å3
Z = 2
Cu Kα radiation
μ = 7.14 mm−1
T = 173 K
0.25 × 0.16 × 0.11 mm
Data collection
Rigaku R-AXIS RAPID diffractometer
Absorption correction: multi-scan (ABSCOR; Rigaku, 1995 ▸) T min = 0.268, T max = 0.507
9318 measured reflections
2710 independent reflections
2121 reflections with I > 2σ(I)
R int = 0.120
Refinement
R[F 2 > 2σ(F 2)] = 0.091
wR(F 2) = 0.225
S = 1.03
2710 reflections
180 parameters
1 restraint
H-atom parameters constrained
Δρmax = 2.07 e Å−3
Δρmin = −1.32 e Å−3
Absolute structure: Flack (1983 ▸), 1218 Friedel pairs
Absolute structure parameter: 0.34 (2)
Data collection: RAPID-AUTO (Rigaku, 2010 ▸); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; program(s) used to solve structure: SIR92 (Altomare et al., 1994 ▸); program(s) used to refine structure: SHELXL97 (Sheldrick, 2015 ▸); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012 ▸); software used to prepare material for publication: PLATON (Spek, 2009 ▸) and publCIF (Westrip, 2010 ▸).
Supplementary Material
Crystal structure: contains datablock(s) Global, I. DOI: 10.1107/S2056989015002236/su5071sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015002236/su5071Isup2.hkl
x y z . DOI: 10.1107/S2056989015002236/su5071fig1.tif
A view of the molecular structure of the title complex, with atom labelling (symmetry code: (i) −x + 1, y, −z). Displacement ellipsoids are drawn at the 50% probability level.
b . DOI: 10.1107/S2056989015002236/su5071fig2.tif
Crystal packing of the title complex viewed along the b axis.
CCDC reference: 1046981
Additional supporting information: crystallographic information; 3D view; checkCIF report
Acknowledgments
MBHH and MSB are grateful to the Department of Chemistry, Rajshahi University, for the provision of laboratory facilities. MCS acknowledges the Department of Applied Chemistry, Toyama University, for providing funds for single-crystal X-ray analyses.
supplementary crystallographic information
S1. Synthesis and crystallization
A solution of PdCl2 (0.044 g, 0.25 mmol, 25 mL methanol) was added to a solution of the ligand, S-hexyl (E)-3-(4-methylbenzylidene)dithiocarbazate (0.147 g, 0.5 mmol, 10 mL methanol). The resulting mixture was stirred at room temperature for 3 h. An orange red precipitate was formed, filtered off, washed with methanol and dried in vacuo over anhydrous CaCl2. Orange red single crystals, suitable for X-ray diffraction, of the compound were obtained by slow evaporation from a mixture of chloroform and acetonitrile (1:1) after 5 days (m.p.: 433 K).
S2. Refinement
Crystal data, data collection and structure refinement details are summarized in Table 1. All H atoms were fixed geometrically (C—H = 0.95 - 0.99 Å) and refined as riding, with Uiso(H) =1.2 Ueq(C). The rather high R factor is affected by the small crystal dimensions and consequently by low diffraction at high θ angles. The collected data were cut at a resolution of 0.85 Å. The structure was refined as an inversion twin with a final BASF parameter = 0.34 (2).
S3. Comment
In the crystal of the title complex, Fig. 1, the PdII atom resides on a crystallographic twofold rotational axis and the two chelating Schiff base ligands, in their deprotonated imino thiolate form, coordinate the metal center via the azomithine nitrogen atom, N1 and thiolate sulfur atom, S1 in a cis-planar configuration (Fig. 1). However, the donor atoms are not coplanar as observed for the corresponding nickel derivative (Howlader et al., 2015b), but the square planar geometry presents a slight tetrahedral distortion with displacement of atoms N1 and S1 of ± 0.121 (14) and ∓ 0.134 (6) Å, respectively, from the coordination mean plane. The Pd1–S1 and Pd1—N1 coordination bond distances are of 2.264 (4) and 2.154 (12) Å, respectively, with an N1—Pd1—S1 chelating angle of 83.2 (3)°. These values are in agreement with those observed in similar Pd-bis(dithiocarbazato) complexes, either with a cis configuration (Ali et al., 2002; Liu, et al., 2011; Duan et al., 1998; Tampouris et al., 2007) or with a trans configuration (Khaledi et al., 2011; Tampouris et al., 2007; Tarafder et al., 2010). It is worth noting that the E conformation about the imine bond N1═C8 [= 1.207 (17) Å; torsion angle N2—N1—C8—C5 = 172.1 (14)°] is different to that observed in the nickel derivative mentioned above, viz.1.2 (7)°. This allows an approach between the rings of the methylbenzylidene moieties, with a centroid-to-centroid distance of 4.114 (8) Å, indicating a very weak π-π interaction.
In the crystal, there are no significant intermolecular interactions present. The molecules pack along the c axis direction (Fig. 2).
Figures
Fig. 1.
A view of the molecular structure of the title complex, with atom labelling (symmetry code: (i) -x + 1, y, -z). Displacement ellipsoids are drawn at the 50% probability level.
Fig. 2.

Crystal packing of the title complex viewed along the b axis.
Crystal data
| [Pd(C15H21N2S2)2] | Z = 2 |
| Mr = 693.32 | F(000) = 720 |
| Monoclinic, C2 | Dx = 1.405 Mg m−3 |
| Hall symbol: C 2y | Cu Kα radiation, λ = 1.54187 Å |
| a = 18.3559 (11) Å | θ = 4.8–67.0° |
| b = 9.6747 (5) Å | µ = 7.14 mm−1 |
| c = 10.3368 (6) Å | T = 173 K |
| β = 116.810 (2)° | Prism, orange |
| V = 1638.37 (16) Å3 | 0.25 × 0.16 × 0.11 mm |
Data collection
| Rigaku R-AXIS RAPID diffractometer | 2710 independent reflections |
| Radiation source: fine-focus sealed tube | 2121 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.120 |
| Detector resolution: 10.000 pixels mm-1 | θmax = 65.1°, θmin = 4.8° |
| ω scans | h = −21→21 |
| Absorption correction: multi-scan (ABSCOR; Rigaku, 1995) | k = −11→11 |
| Tmin = 0.268, Tmax = 0.507 | l = −12→12 |
| 9318 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)] = 0.091 | H-atom parameters constrained |
| wR(F2) = 0.225 | w = 1/[σ2(Fo2) + (0.1251P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.03 | (Δ/σ)max < 0.001 |
| 2710 reflections | Δρmax = 2.07 e Å−3 |
| 180 parameters | Δρmin = −1.31 e Å−3 |
| 1 restraint | Absolute structure: Flack (1983), 1218 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Absolute structure parameter: 0.34 (2) |
Special details
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
| Pd1 | 0.5000 | 0.5495 | 0.0000 | 0.0607 (4) | |
| S1 | 0.4807 (3) | 0.3802 (4) | 0.1325 (5) | 0.0725 (11) | |
| S2 | 0.4003 (2) | 0.3956 (4) | 0.3156 (4) | 0.0726 (9) | |
| N1 | 0.4949 (7) | 0.6818 (12) | 0.1634 (13) | 0.060 (3) | |
| N2 | 0.4526 (9) | 0.6244 (17) | 0.2347 (16) | 0.071 (4) | |
| C1 | 0.7185 (10) | 1.1510 (17) | 0.0408 (17) | 0.087 (4) | |
| H1A | 0.7670 | 1.1034 | 0.0465 | 0.130* | |
| H1B | 0.7353 | 1.2327 | 0.1036 | 0.130* | |
| H1C | 0.6839 | 1.1796 | −0.0594 | 0.130* | |
| C2 | 0.6712 (6) | 1.0545 (19) | 0.0900 (11) | 0.063 (3) | |
| C3 | 0.6745 (8) | 0.9122 (16) | 0.0758 (15) | 0.072 (4) | |
| H3 | 0.7083 | 0.8746 | 0.0369 | 0.086* | |
| C4 | 0.6290 (7) | 0.8236 (13) | 0.1178 (14) | 0.062 (3) | |
| H4 | 0.6339 | 0.7262 | 0.1124 | 0.075* | |
| C5 | 0.5759 (7) | 0.8797 (13) | 0.1679 (13) | 0.061 (3) | |
| C6 | 0.5741 (8) | 1.0255 (14) | 0.1841 (14) | 0.070 (4) | |
| H6 | 0.5412 | 1.0656 | 0.2234 | 0.084* | |
| C7 | 0.6196 (8) | 1.1052 (14) | 0.1431 (14) | 0.071 (3) | |
| H7 | 0.6161 | 1.2025 | 0.1509 | 0.085* | |
| C8 | 0.5215 (8) | 0.7962 (12) | 0.2045 (14) | 0.062 (3) | |
| H8 | 0.5048 | 0.8378 | 0.2700 | 0.074* | |
| C9 | 0.4449 (11) | 0.4926 (16) | 0.2274 (18) | 0.059 (4) | |
| C10 | 0.3742 (9) | 0.529 (2) | 0.4125 (15) | 0.080 (5) | |
| H10A | 0.4242 | 0.5722 | 0.4885 | 0.096* | |
| H10B | 0.3406 | 0.6025 | 0.3449 | 0.096* | |
| C11 | 0.3247 (9) | 0.4534 (18) | 0.4821 (16) | 0.081 (4) | |
| H11A | 0.2809 | 0.3981 | 0.4062 | 0.097* | |
| H11B | 0.3617 | 0.3886 | 0.5571 | 0.097* | |
| C12 | 0.2885 (8) | 0.545 (2) | 0.5472 (14) | 0.081 (3) | |
| H12A | 0.2580 | 0.6183 | 0.4765 | 0.097* | |
| H12B | 0.3327 | 0.5904 | 0.6324 | 0.097* | |
| C13 | 0.2311 (9) | 0.4735 (19) | 0.5952 (19) | 0.091 (5) | |
| H13A | 0.1951 | 0.4112 | 0.5161 | 0.109* | |
| H13B | 0.2642 | 0.4148 | 0.6800 | 0.109* | |
| C14 | 0.1813 (12) | 0.559 (3) | 0.632 (2) | 0.133 (7) | |
| H14A | 0.1500 | 0.6224 | 0.5504 | 0.160* | |
| H14B | 0.2165 | 0.6168 | 0.7170 | 0.160* | |
| C15 | 0.1205 (10) | 0.475 (2) | 0.670 (2) | 0.110 (6) | |
| H15A | 0.0888 | 0.5391 | 0.6982 | 0.165* | |
| H15B | 0.1512 | 0.4118 | 0.7499 | 0.165* | |
| H15C | 0.0835 | 0.4224 | 0.5845 | 0.165* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Pd1 | 0.0664 (7) | 0.0506 (7) | 0.0761 (7) | 0.000 | 0.0419 (5) | 0.000 |
| S1 | 0.093 (3) | 0.051 (2) | 0.095 (3) | 0.001 (2) | 0.062 (2) | 0.004 (2) |
| S2 | 0.084 (2) | 0.059 (2) | 0.092 (2) | −0.0072 (17) | 0.0542 (19) | 0.0009 (17) |
| N1 | 0.055 (6) | 0.057 (7) | 0.076 (7) | −0.011 (5) | 0.037 (6) | 0.006 (5) |
| N2 | 0.067 (8) | 0.072 (9) | 0.091 (9) | −0.027 (7) | 0.050 (7) | −0.017 (7) |
| C1 | 0.081 (9) | 0.094 (12) | 0.096 (11) | −0.013 (8) | 0.048 (9) | 0.004 (8) |
| C2 | 0.063 (6) | 0.054 (7) | 0.073 (6) | 0.014 (9) | 0.032 (5) | −0.003 (9) |
| C3 | 0.063 (8) | 0.084 (11) | 0.086 (9) | 0.003 (7) | 0.048 (7) | −0.002 (7) |
| C4 | 0.058 (6) | 0.048 (7) | 0.082 (8) | 0.003 (5) | 0.034 (6) | 0.003 (6) |
| C5 | 0.060 (7) | 0.052 (7) | 0.076 (8) | 0.000 (6) | 0.036 (6) | 0.001 (5) |
| C6 | 0.076 (7) | 0.053 (10) | 0.093 (8) | 0.001 (7) | 0.048 (7) | −0.005 (6) |
| C7 | 0.074 (8) | 0.055 (8) | 0.080 (9) | −0.004 (6) | 0.032 (7) | 0.011 (6) |
| C8 | 0.079 (8) | 0.030 (6) | 0.096 (9) | 0.006 (6) | 0.057 (7) | 0.005 (6) |
| C9 | 0.068 (9) | 0.052 (9) | 0.063 (9) | −0.004 (7) | 0.034 (7) | 0.000 (6) |
| C10 | 0.085 (8) | 0.090 (14) | 0.081 (8) | −0.017 (10) | 0.053 (7) | 0.007 (9) |
| C11 | 0.084 (9) | 0.083 (11) | 0.086 (10) | −0.009 (8) | 0.048 (8) | 0.002 (8) |
| C12 | 0.084 (7) | 0.088 (9) | 0.081 (7) | −0.019 (12) | 0.047 (6) | −0.019 (12) |
| C13 | 0.082 (10) | 0.104 (12) | 0.109 (12) | 0.010 (9) | 0.063 (9) | 0.002 (9) |
| C14 | 0.162 (16) | 0.118 (16) | 0.150 (15) | 0.043 (19) | 0.098 (14) | −0.003 (17) |
| C15 | 0.106 (12) | 0.112 (14) | 0.160 (17) | −0.024 (10) | 0.102 (13) | −0.010 (11) |
Geometric parameters (Å, º)
| Pd1—N1 | 2.154 (12) | C6—C7 | 1.337 (16) |
| Pd1—N1i | 2.154 (12) | C6—H6 | 0.9500 |
| Pd1—S1 | 2.264 (4) | C7—H7 | 0.9500 |
| Pd1—S1i | 2.264 (4) | C8—H8 | 0.9500 |
| S1—C9 | 1.777 (17) | C10—C11 | 1.573 (19) |
| S2—C9 | 1.747 (16) | C10—H10A | 0.9900 |
| S2—C10 | 1.829 (18) | C10—H10B | 0.9900 |
| N1—C8 | 1.208 (16) | C11—C12 | 1.44 (2) |
| N1—N2 | 1.404 (17) | C11—H11A | 0.9900 |
| N2—C9 | 1.282 (15) | C11—H11B | 0.9900 |
| C1—C2 | 1.511 (19) | C12—C13 | 1.52 (2) |
| C1—H1A | 0.9800 | C12—H12A | 0.9900 |
| C1—H1B | 0.9800 | C12—H12B | 0.9900 |
| C1—H1C | 0.9800 | C13—C14 | 1.41 (2) |
| C2—C7 | 1.381 (16) | C13—H13A | 0.9900 |
| C2—C3 | 1.39 (2) | C13—H13B | 0.9900 |
| C3—C4 | 1.397 (18) | C14—C15 | 1.56 (3) |
| C3—H3 | 0.9500 | C14—H14A | 0.9900 |
| C4—C5 | 1.403 (16) | C14—H14B | 0.9900 |
| C4—H4 | 0.9500 | C15—H15A | 0.9800 |
| C5—C6 | 1.423 (17) | C15—H15B | 0.9800 |
| C5—C8 | 1.460 (16) | C15—H15C | 0.9800 |
| N1—Pd1—N1i | 107.1 (6) | N2—C9—S2 | 124.7 (15) |
| N1—Pd1—S1 | 83.2 (3) | N2—C9—S1 | 125.6 (15) |
| N1i—Pd1—S1 | 168.1 (3) | S2—C9—S1 | 109.6 (9) |
| N1—Pd1—S1i | 168.1 (3) | C11—C10—S2 | 105.5 (13) |
| N1i—Pd1—S1i | 83.2 (3) | C11—C10—H10A | 110.6 |
| S1—Pd1—S1i | 87.3 (2) | S2—C10—H10A | 110.6 |
| C9—S1—Pd1 | 95.1 (5) | C11—C10—H10B | 110.6 |
| C9—S2—C10 | 101.8 (7) | S2—C10—H10B | 110.6 |
| C8—N1—N2 | 114.2 (12) | H10A—C10—H10B | 108.8 |
| C8—N1—Pd1 | 131.8 (10) | C12—C11—C10 | 114.0 (15) |
| N2—N1—Pd1 | 114.0 (9) | C12—C11—H11A | 108.7 |
| C9—N2—N1 | 115.8 (16) | C10—C11—H11A | 108.7 |
| C2—C1—H1A | 109.5 | C12—C11—H11B | 108.7 |
| C2—C1—H1B | 109.5 | C10—C11—H11B | 108.7 |
| H1A—C1—H1B | 109.5 | H11A—C11—H11B | 107.6 |
| C2—C1—H1C | 109.5 | C11—C12—C13 | 113.9 (18) |
| H1A—C1—H1C | 109.5 | C11—C12—H12A | 108.8 |
| H1B—C1—H1C | 109.5 | C13—C12—H12A | 108.8 |
| C7—C2—C3 | 117.7 (14) | C11—C12—H12B | 108.8 |
| C7—C2—C1 | 121.0 (16) | C13—C12—H12B | 108.8 |
| C3—C2—C1 | 121.2 (12) | H12A—C12—H12B | 107.7 |
| C2—C3—C4 | 120.9 (12) | C14—C13—C12 | 116.7 (19) |
| C2—C3—H3 | 119.5 | C14—C13—H13A | 108.1 |
| C4—C3—H3 | 119.5 | C12—C13—H13A | 108.1 |
| C3—C4—C5 | 119.4 (12) | C14—C13—H13B | 108.1 |
| C3—C4—H4 | 120.3 | C12—C13—H13B | 108.1 |
| C5—C4—H4 | 120.3 | H13A—C13—H13B | 107.3 |
| C4—C5—C6 | 118.9 (11) | C13—C14—C15 | 112 (2) |
| C4—C5—C8 | 123.5 (11) | C13—C14—H14A | 109.1 |
| C6—C5—C8 | 117.6 (11) | C15—C14—H14A | 109.1 |
| C7—C6—C5 | 118.9 (12) | C13—C14—H14B | 109.1 |
| C7—C6—H6 | 120.5 | C15—C14—H14B | 109.1 |
| C5—C6—H6 | 120.5 | H14A—C14—H14B | 107.8 |
| C6—C7—C2 | 124.0 (14) | C14—C15—H15A | 109.5 |
| C6—C7—H7 | 118.0 | C14—C15—H15B | 109.5 |
| C2—C7—H7 | 118.0 | H15A—C15—H15B | 109.5 |
| N1—C8—C5 | 129.2 (12) | C14—C15—H15C | 109.5 |
| N1—C8—H8 | 115.4 | H15A—C15—H15C | 109.5 |
| C5—C8—H8 | 115.4 | H15B—C15—H15C | 109.5 |
Symmetry code: (i) −x+1, y, −z.
Footnotes
Supporting information for this paper is available from the IUCr electronic archives (Reference: SU5071).
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 datablock(s) Global, I. DOI: 10.1107/S2056989015002236/su5071sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989015002236/su5071Isup2.hkl
x y z . DOI: 10.1107/S2056989015002236/su5071fig1.tif
A view of the molecular structure of the title complex, with atom labelling (symmetry code: (i) −x + 1, y, −z). Displacement ellipsoids are drawn at the 50% probability level.
b . DOI: 10.1107/S2056989015002236/su5071fig2.tif
Crystal packing of the title complex viewed along the b axis.
CCDC reference: 1046981
Additional supporting information: crystallographic information; 3D view; checkCIF report

