research communications
An unusual two-dimensional MOF formed from NiII, thiophene-2,5-dicarboxylate and trans-1,2-bis(pyridin-4-yl)ethylene
aDepartment of Chemistry, KU Leuven, Biomolecular Architecture, Celestijnenlaan 200F, Leuven (Heverlee), B-3001, Belgium
*Correspondence e-mail: [email protected]
A new NiII MOF, poly[[sesqui[μ-trans-1,2-bis(pyridin-4-yl)ethylene](μ-thiophene-2,5-dicarboxylato)nickel(II)] dimethylformamide 0.205-solvate], {[Ni(C6H3O4S)(C12H10N2)1.5].0.205C3H7NO}n, was obtained under solvothermal conditions and its structure was determined by single-crystal X-ray diffraction. The structure reveals that Ni nodes are bridged by thiophene-2,5-dicarboxylate (HT) and trans-1,2-bis(pyridin-4-yl)ethylene (Bpe) to generate an unusual two-dimensional layered framework, and the overall crystal is formed by an interlocked stacking of these layers. Topological simplification classifies the framework as a non-interpenetrated 3-nodal (2,2,5)-connected net, in which the Ni-containing node acts as the higher-connected vertex and the two organic ligands serve as 2-connected linkers propagating the connectivity within the layer. The experimental powder X-ray diffraction (PXRD) pattern is in good agreement with that simulated from the single-crystal structure, further confirming that the powder sample is consistent with the single-crystal model and exhibits good phase purity.
Keywords: crystal structure; metal-organic framework; nickel; thiophene-2,5-dicarboxylate; trans-1,2-bis(pyridin-4-yl)ethylene.
CCDC reference: 2534227
1. Chemical context
Metal–organic frameworks (MOFs) continue to attract strong interest in crystal engineering owing to their high structural tunability and rich topological diversity (Furukawa et al., 2013
). This diversity arises primarily from the wide range of coordination numbers and geometries accessible to metal nodes (or clusters), together with the adjustable connectivity, length and conformation of organic linkers (O'Keeffe & Yaghi, 2012
). As a result, MOFs can display varied dimensionalities and connectivity patterns, often accompanied by key structural features such as porosity, layered packing and interpenetration. In this context, mixed-ligand strategies provide an efficient route to modulate connectivity and spatial extension by combining complementary coordinating groups, thereby expanding the diversity and accessibility of framework architectures and underlying topologies (Yin et al., 2015
).
Within the widely used combination of dicarboxylate and N-donor linker construction method, thiophene-2,5-dicarboxylate (HT) exhibits distinctive features. The thiophene core introduces a sulfur-containing heteroaromatic, π-conjugated motif, so that, in addition to providing robust carboxylate bridges, it may influence interlayer packing and framework dimensionality through π–π interactions and other weak supramolecular contacts (Thuéry & Harrowfield, 2022
; Zheng et al., 2008
). Meanwhile, the linear N-donor ligand trans-1,2-bis(pyridin-4-yl)ethylene (Bpe) is rigid and offers a relatively long spacer length; its terminal pyridyl N atoms impart well-defined directional coordination and it is therefore frequently employed as a `pillar' to tune metal–metal separations, promote layered architectures, and regulate the underlying topology (Wu et al., 2019
; Zhang et al., 2012
). Accordingly, the synergistic assembly of HT and Bpe provides a suitable platform for constructing frameworks with characteristic layered motifs and topological features.
On this basis, a new NiII MOF, Ni-HT-Bpe, was obtained under solvothermal conditions and its structure was determined by single-crystal X-ray diffraction. Notably, the framework adopts a thick parallel polycatenated 2D entangled architecture, which belongs to a comparatively rare subclass among entangled 2D coordination networks (ca. 9.2% overall in an extended ring net (ERN)-based statistical survey; Alexandrov et al., 2017
). Moreover, closely related systems based on the same (or very similar) linker combinations more commonly form twofold interpenetrated 3D frameworks (Jia et al., 2024
; Alamgir et al., 2021
; Sen et al., 2013
), highlighting an unusual structure–composition relationship for Ni-HT-Bpe.
2. Structural commentary
The Ni-HT-Bpe structure crystallizes in the triclinic P with one Ni ion, one thiophene-2,5-dicarboxylate and one and a half trans-1,2-bis(pyridin-4-yl)ethylene in the asymmetric unit (Fig. 1
). The asymmetric unit also contains a dimethylformamide (DMF) molecule with an occupancy of 0.205 (7) close to the inversion center at 1/2,1/2,1/2 generating a second DMF. The second Bpe half is generated by inversion symmetry. The other Bpe molecule is partly disordered (atoms N2, C13–C18) over two positions with occupancies of 0.544 (17) and 0.456 (17).
| Figure 1 Asymmetric unit of the title compound Ni-HT-Bpe showing the atom labelling and 30% probability ellipsoids. Only the major component of the disordered trans-1,2-bis(pyridin-4-yl)ethylene is shown and the partial dimethylformamide molecule has been removed for clarity. |
The Ni ion is octahedrally coordinated by three N atoms from Bpe [atoms N1, N2 and N3(x, y, −1 + z)] and three O atoms from HT [atoms O1, O3(x, 1 + y, z) and O4(x, 1 + y, z)] (Table 1
). This results in chain formation in three directions: in the c-axis direction by interactions with N2 and N3, close to the a-axis direction by interactions with N1, and in the b-axis direction by interactions with O1, O3 and O4 (Table 1
, Fig. 2
). Oxygen atom O2 does not interact with the Ni ion, but forms a hydrogen bond with the neighbouring Bpe pyridyl ring (atom H8, see Table 2
). Oxygen atoms O3 and O4 also show hydrogen bonds with the other Bpe molecule (atoms H21 and H19A, respectively, see Table 2
).
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|
| Figure 2 Packing diagram of Ni-HT-Bpe. Hydrogen atoms and DMF molecules are omitted for clarity. |
The DMF molecule is positioned close to the disordered Bpe part and one of the methyl groups interacts with it through a C—H⋯π interaction (Table 2
). In addition, a C=O⋯π interaction is observed with a neighbouring (N1,C17–C11) ring. Two additional C—H⋯π interactions are listed in Table 2
.
A void-space representation was generated using Mercury (Macrae et al., 2020
) for the solvent-free structural model (Fig. 3
). The plot highlights the presence of internal cavities within the unit cell, which appear as discrete void regions rather than a clearly continuous channel system. A quantitative porosity analysis was carried out using Zeo++ (Willems et al., 2012
) in high-accuracy mode using the solvent-free CIF. The framework exhibits a substantial geometric void volume of 454.2 Å3 per corresponding to a void fraction of 0.372. However, the probe-accessible volume and accessible surface area are both zero for a probe radius of 1.86 Å (approximate the kinetic size of N2) indicating that the pore apertures are too small to be accessible to N2 under this probe condition.
| Figure 3 Visualization of the voids in the crystal packing of Ni-HT-Bpe using Mercury (Macrae et al., 2020 |
The structure reveals that Ni nodes are bridged by HT and Bpe to generate an unusual two-dimensional layered framework, and the overall crystal is formed by an interlocked stacking of these layers. Topological simplification classifies the framework as a non-interpenetrated 3-nodal (2,2,5)-connected net, in which the Ni-containing node acts as the higher-connected vertex and the two organic ligands serve as 2-connected linkers propagating the connectivity within the layer. The experimental powder X-ray diffraction (PXRD) pattern is in good agreement with that simulated from the single-crystal structure, further confirming that the powder sample is consistent with the single-crystal model and exhibits good phase purity.
The connectivity of Ni-HT-Bpe was analyzed by a topological simplification in which the coordination framework is reduced to its underlying net (Fig. 4
; Blatov et al., 2014
). The structure forms 2D layers parallel to (100), and only one structural group is present, indicating that the framework is non-interpenetrated. In the reduced representation, the layer can be described as a 3-nodal (2,2,5)-connected net. The metal-containing node (originating from the Ni coordination environment) acts as the higher-connected vertex, while both organic linkers function as 2-connected spacers that propagate the network within the layer. The resulting topology is 22,5-c net with stoichiometry (2-c)4(2-c)(5-c)2.
| Figure 4 Topological analysis of Ni-HT-Bpe: (a) 3 × 3 × 3 unit cells of the framework; (b) 3 × 3 × 3 unit cells view of the corresponding simplified net; (c) representation of a single two-dimensional layer [parallel to (100)]. |
3. Database survey
A search of the Cambridge Structural Database (CSD, version 6.01, November 2025; Groom et al., 2016
) for thiophene-2,5-dicarboxylate resulted in 868 hits with 27 containing an O⋯Ni interaction of which 20 are present in the MOF subset. A search for 1,2-bis(pyridin-4-yl)ethylene yielded 2868 hits with 123 showing an N⋯Ni interaction of which 97 hits belong to the MOF subset.
Two structures are worthwhile to mention due to the presence of very similar building units. Refcode LICNER (Han et al., 2007
) refers to a Ni polymer containing thiophene-2,5-dicarboxylate (tda) and 1,3-di-pyridin-4-ylpropane (bpp). Each Ni ion is six-coordinated by four O atoms (two from two independent tda and two aqua O atoms) and two N atoms from two bpp ligands. A 2D grid-type bilayer formed through intermolecular O—H⋯O interactions is running parallel to the (001) plane.
The asymmetric unit of the second one, KIFBOT (Lu et al., 2018
), contains one Ni atom, one thiophene-2,5-dicarboxylate anion (tdc), one 2,2′-dimethyl-4,4′-bipyridine ligand (dmbpy) and one μ2-O atom. The Ni ion is six-coordinated by three carboxylate O atoms from three different tda, two N atoms from two different dmbpy and one μ2-O atom. A dimeric Ni unit [Ni2(COO)4(μ2-OH)] acts as secondary building unit (SBU) and neighbouring SBUs are connected by tdc ligands to form 2D grids, which extend into a 3D framework by dmbpy pillars.
4. Synthesis and crystallization
The reaction scheme to synthesize the title compound is given in Fig. 5
.
| | Figure 5 Reaction scheme for the synthesis of Ni-HT-Bpe. |
Ni(NO3)2·6H2O (29 mg, 0.10 mmol), thiophene-2,5-dicarboxylic acid (HT; 15.6 mg, 0.10 mmol) and trans-1,2-bis(pyridin-4-yl)ethylene (Bpe; 27 mg, 0.15 mmol) were placed in a 25 mL Teflon-lined stainless-steel autoclave, and DMF/EtOH/H2O (10 mL) was added. The mixture was sonicated for 5 min and then stirred at room temperature for 10 min to give a homogeneous suspension. The vessel was sealed and heated at 368K for 4 days and then cooled to room temperature at a rate of 6 K h−1. Green block-shaped crystals and needle-like crystals of Ni-HT-Bpe were obtained. For powder preparation, the as-synthesized product was collected by filtration, washed with DMF (3 × 10 mL) followed by EtOH (3 × 10 mL), and dried in a vacuum oven at 353K overnight to afford Ni-HT-Bpe as green powder (54 mg, 75% yield based on Bpe).
The phase purity of the powder sample was assessed by powder X-ray diffraction (PXRD). Powder X-ray diffraction data were collected on a PANalytical Empyrean diffractometer (Malvern Panalytical) in transmission geometry over the 2θ range 1.3–45°, using a PIXcel3D hybrid pixel detector and Cu Kα radiation (Kα1, λ = 1.5406 Å; Kα2, λ = 1.5444 Å). The experimental PXRD pattern matches well with the peak positions in the pattern simulated from the single-crystal X-ray structure using Mercury (Macrae et al., 2020
), confirming that the crystalline powder material is consistent with the single-crystal model (Fig. 6
). Noticeable discrepancies in relative intensities are observed. As the sample contains both needle-shaped and block-like crystals (Fig. 7
), these discrepancies can be attributed mainly to preferred orientation effects arising from the strongly anisotropic, needle-shaped crystallites (and their intergrown bundles) present in the bulk sample, whereas the simulated pattern assumes an ideal randomly oriented powder.
| Figure 6 Experimental (top) and simulated (bottom) PXRD patterns of Ni-HT-Bpe. The experimental pattern was recorded using Cu Kα radiation, and the simulated pattern was calculated using Mercury (Macrae et al., 2020 |
| Figure 7 Optical micrographs of needle-like and block-like crystals in the as-synthesized sample (bright-field); panel (c) was acquired under crossed polarizers. |
5. Refinement
Crystal data, data collection and structure details are summarized in Table 3
. Part of trans-1,2-bis(pyridyl)ethylene (atoms N2, C13-C18) was disordered over two positions with occupancies of 0.544 (17) and 0.456 (17). The DMF molecule with refined occupancy 0.205 (7) was subject to DFIX, FLAT, RIGU and ISOR restraints to maintain the expected geometry.
|
Supporting information
CCDC reference: 2534227
contains datablock I. DOI: https://doi.org/10.1107/S2056989026002276/vu2018sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989026002276/vu2018Isup2.hkl
| [Ni(C6H3O4S)(C12H10N2)1.5]·0.205C3H7NO | Z = 2 |
| Mr = 517.08 | F(000) = 532 |
| Triclinic, P1 | Dx = 1.407 Mg m−3 |
| a = 9.7666 (4) Å | Cu Kα radiation, λ = 1.54178 Å |
| b = 9.8999 (4) Å | Cell parameters from 8971 reflections |
| c = 13.5669 (6) Å | θ = 5.6–72.4° |
| α = 98.092 (2)° | µ = 2.26 mm−1 |
| β = 96.235 (2)° | T = 273 K |
| γ = 107.823 (2)° | Block, clear light green |
| V = 1220.25 (9) Å3 | 0.15 × 0.13 × 0.12 mm |
| Bruker D8 Venture diffractometer | 3940 reflections with I > 2σ(I) |
| Detector resolution: 7.9 pixels mm-1 | Rint = 0.058 |
| φ and ω scans | θmax = 73.0°, θmin = 5.6° |
| Absorption correction: multi-scan (SADABS; Krause et al., 2015) | h = −10→12 |
| Tmin = 0.487, Tmax = 0.754 | k = −12→12 |
| 16259 measured reflections | l = −16→16 |
| 4801 independent reflections |
| Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
| Least-squares matrix: full | H-atom parameters constrained |
| R[F2 > 2σ(F2)] = 0.066 | w = 1/[σ2(Fo2) + (0.0753P)2 + 2.321P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.185 | (Δ/σ)max < 0.001 |
| S = 1.04 | Δρmax = 0.43 e Å−3 |
| 4801 reflections | Δρmin = −0.60 e Å−3 |
| 411 parameters | Extinction correction: SHELXL-2016/4 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| 77 restraints | Extinction coefficient: 0.0106 (15) |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
| x | y | z | Uiso*/Ueq | Occ. (<1) | |
| Ni1 | 0.69283 (7) | 0.86205 (6) | 0.22629 (4) | 0.0380 (3) | |
| S1 | 0.75169 (11) | 0.38941 (11) | 0.23040 (9) | 0.0504 (3) | |
| O1 | 0.7559 (3) | 0.6858 (3) | 0.2229 (2) | 0.0504 (7) | |
| O2 | 0.9965 (4) | 0.7930 (3) | 0.2616 (3) | 0.0727 (10) | |
| O3 | 0.6566 (3) | 0.0670 (3) | 0.2320 (2) | 0.0470 (6) | |
| O4 | 0.8783 (3) | 0.0550 (3) | 0.2622 (2) | 0.0459 (6) | |
| N1 | 0.4762 (4) | 0.7301 (4) | 0.1770 (2) | 0.0458 (8) | |
| N3 | 0.7129 (4) | 0.8640 (3) | 1.0730 (2) | 0.0423 (7) | |
| C1 | 0.8847 (5) | 0.6871 (4) | 0.2486 (3) | 0.0485 (9) | |
| C2 | 0.8999 (5) | 0.5449 (4) | 0.2600 (4) | 0.0516 (10) | |
| C3 | 1.0229 (5) | 0.5158 (5) | 0.2889 (5) | 0.0751 (16) | |
| H3 | 1.114325 | 0.585919 | 0.307182 | 0.090* | |
| C4 | 0.9981 (5) | 0.3673 (5) | 0.2886 (5) | 0.0744 (16) | |
| H4 | 1.071606 | 0.329647 | 0.306474 | 0.089* | |
| C5 | 0.8571 (5) | 0.2859 (4) | 0.2596 (4) | 0.0518 (10) | |
| C6 | 0.7934 (4) | 0.1281 (4) | 0.2508 (3) | 0.0434 (8) | |
| C7 | 0.3659 (5) | 0.7815 (5) | 0.1773 (3) | 0.0537 (10) | |
| H7 | 0.382073 | 0.872090 | 0.215811 | 0.064* | |
| C8 | 0.2282 (5) | 0.7078 (6) | 0.1236 (4) | 0.0649 (12) | |
| H8 | 0.154093 | 0.748213 | 0.126837 | 0.078* | |
| C9 | 0.2014 (5) | 0.5726 (5) | 0.0647 (4) | 0.0607 (12) | |
| C10 | 0.3152 (6) | 0.5201 (6) | 0.0651 (5) | 0.0744 (15) | |
| H10 | 0.302092 | 0.430102 | 0.026884 | 0.089* | |
| C11 | 0.4482 (5) | 0.5981 (5) | 0.1210 (4) | 0.0604 (12) | |
| H11 | 0.522886 | 0.558289 | 0.120386 | 0.072* | |
| C12 | 0.0596 (5) | 0.4845 (6) | 0.0014 (4) | 0.0686 (13) | |
| H12 | 0.056538 | 0.399799 | −0.039758 | 0.082* | |
| N2a | 0.6832 (11) | 0.8719 (19) | 0.3816 (7) | 0.049 (6) | 0.544 (17) |
| C13a | 0.5639 (11) | 0.877 (2) | 0.4220 (7) | 0.074 (4) | 0.544 (17) |
| H13a | 0.484307 | 0.881302 | 0.379870 | 0.089* | 0.544 (17) |
| C14a | 0.5542 (11) | 0.876 (2) | 0.5208 (6) | 0.080 (5) | 0.544 (17) |
| H14a | 0.465101 | 0.865300 | 0.542590 | 0.096* | 0.544 (17) |
| C15a | 0.6735 (16) | 0.889 (2) | 0.5887 (9) | 0.051 (4) | 0.544 (17) |
| C16a | 0.8002 (12) | 0.8912 (16) | 0.5493 (8) | 0.050 (3) | 0.544 (17) |
| H16a | 0.883435 | 0.894223 | 0.591251 | 0.060* | 0.544 (17) |
| C17a | 0.8004 (13) | 0.8888 (16) | 0.4472 (9) | 0.053 (3) | 0.544 (17) |
| H17a | 0.888120 | 0.899723 | 0.423208 | 0.064* | 0.544 (17) |
| C18a | 0.660 (2) | 0.879 (2) | 0.6943 (10) | 0.051 (5) | 0.544 (17) |
| H18a | 0.568903 | 0.867991 | 0.712312 | 0.062* | 0.544 (17) |
| N12b | 0.6761 (16) | 0.867 (2) | 0.3781 (12) | 0.059 (9) | 0.456 (17) |
| C113b | 0.5687 (17) | 0.762 (2) | 0.4074 (8) | 0.094 (7) | 0.456 (17) |
| H113b | 0.498886 | 0.693813 | 0.357604 | 0.113* | 0.456 (17) |
| C114b | 0.5589 (17) | 0.752 (2) | 0.5057 (8) | 0.092 (7) | 0.456 (17) |
| H114b | 0.479659 | 0.682122 | 0.521112 | 0.111* | 0.456 (17) |
| C115b | 0.6630 (16) | 0.841 (2) | 0.5816 (9) | 0.043 (4) | 0.456 (17) |
| C116b | 0.779 (2) | 0.9444 (17) | 0.5532 (10) | 0.064 (4) | 0.456 (17) |
| H116b | 0.851599 | 1.011918 | 0.601356 | 0.076* | 0.456 (17) |
| C117b | 0.7812 (19) | 0.9422 (19) | 0.4510 (10) | 0.063 (5) | 0.456 (17) |
| H117b | 0.865749 | 1.000082 | 0.432854 | 0.076* | 0.456 (17) |
| C118b | 0.653 (3) | 0.832 (3) | 0.6879 (11) | 0.054 (6) | 0.456 (17) |
| H118b | 0.561079 | 0.786706 | 0.702699 | 0.065* | 0.456 (17) |
| C19 | 0.7642 (5) | 0.8832 (5) | 0.7661 (3) | 0.0506 (10) | |
| H19a | 0.856178 | 0.892861 | 0.749447 | 0.061* | 0.544 (17) |
| H19Ab | 0.857626 | 0.926208 | 0.752932 | 0.061* | 0.456 (17) |
| C20 | 0.7444 (4) | 0.8739 (5) | 0.8704 (3) | 0.0468 (9) | |
| C21 | 0.6174 (5) | 0.8778 (5) | 0.9068 (3) | 0.0517 (10) | |
| H21 | 0.539662 | 0.883691 | 0.863557 | 0.062* | |
| C22 | 0.6070 (5) | 0.8729 (5) | 1.0051 (3) | 0.0512 (10) | |
| H22 | 0.520791 | 0.875931 | 1.026875 | 0.061* | |
| C23 | 0.8363 (4) | 0.8605 (4) | 1.0386 (3) | 0.0462 (9) | |
| H23 | 0.912659 | 0.855557 | 1.083746 | 0.055* | |
| C24 | 0.8546 (5) | 0.8638 (5) | 0.9401 (3) | 0.0486 (9) | |
| H24 | 0.941229 | 0.859288 | 0.919813 | 0.058* | |
| C25 | 0.532 (4) | 0.489 (3) | 0.613 (3) | 0.115 (10) | 0.205 (7) |
| H25 | 0.469078 | 0.488621 | 0.659763 | 0.138* | 0.205 (7) |
| O5 | 0.653 (4) | 0.486 (4) | 0.638 (3) | 0.158 (12) | 0.205 (7) |
| N4 | 0.488 (4) | 0.494 (4) | 0.517 (3) | 0.120 (9) | 0.205 (7) |
| C26 | 0.339 (4) | 0.500 (5) | 0.496 (4) | 0.124 (11) | 0.205 (7) |
| H26A | 0.285901 | 0.468594 | 0.548200 | 0.186* | 0.205 (7) |
| H26B | 0.290252 | 0.438990 | 0.432179 | 0.186* | 0.205 (7) |
| H26C | 0.343390 | 0.597964 | 0.492258 | 0.186* | 0.205 (7) |
| C27 | 0.571 (6) | 0.498 (6) | 0.434 (4) | 0.147 (15) | 0.205 (7) |
| H27A | 0.519568 | 0.419088 | 0.380124 | 0.221* | 0.205 (7) |
| H27B | 0.664506 | 0.490555 | 0.457324 | 0.221* | 0.205 (7) |
| H27C | 0.584640 | 0.587607 | 0.410528 | 0.221* | 0.205 (7) |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Ni1 | 0.0410 (4) | 0.0368 (4) | 0.0366 (4) | 0.0120 (3) | 0.0031 (2) | 0.0118 (2) |
| S1 | 0.0459 (6) | 0.0397 (5) | 0.0669 (7) | 0.0161 (4) | 0.0007 (4) | 0.0156 (4) |
| O1 | 0.0501 (16) | 0.0438 (15) | 0.0586 (17) | 0.0175 (12) | 0.0002 (13) | 0.0154 (12) |
| O2 | 0.0541 (19) | 0.0419 (17) | 0.122 (3) | 0.0139 (15) | 0.0082 (19) | 0.0239 (18) |
| O3 | 0.0405 (15) | 0.0428 (14) | 0.0574 (16) | 0.0143 (12) | 0.0012 (12) | 0.0118 (12) |
| O4 | 0.0429 (14) | 0.0370 (13) | 0.0607 (17) | 0.0163 (11) | 0.0027 (12) | 0.0152 (12) |
| N1 | 0.0434 (17) | 0.0473 (18) | 0.0438 (17) | 0.0093 (14) | 0.0025 (14) | 0.0148 (14) |
| N3 | 0.0473 (18) | 0.0440 (17) | 0.0391 (16) | 0.0176 (14) | 0.0055 (13) | 0.0139 (13) |
| C1 | 0.053 (2) | 0.041 (2) | 0.053 (2) | 0.0175 (18) | 0.0045 (18) | 0.0138 (17) |
| C2 | 0.051 (2) | 0.041 (2) | 0.066 (3) | 0.0169 (18) | 0.0047 (19) | 0.0168 (18) |
| C3 | 0.049 (3) | 0.043 (2) | 0.129 (5) | 0.011 (2) | −0.005 (3) | 0.027 (3) |
| C4 | 0.052 (3) | 0.044 (2) | 0.127 (5) | 0.019 (2) | −0.005 (3) | 0.024 (3) |
| C5 | 0.049 (2) | 0.036 (2) | 0.072 (3) | 0.0162 (17) | 0.004 (2) | 0.0154 (18) |
| C6 | 0.045 (2) | 0.0387 (19) | 0.047 (2) | 0.0141 (16) | 0.0049 (16) | 0.0112 (16) |
| C7 | 0.048 (2) | 0.060 (3) | 0.049 (2) | 0.015 (2) | 0.0038 (18) | 0.0068 (19) |
| C8 | 0.048 (2) | 0.077 (3) | 0.070 (3) | 0.021 (2) | 0.004 (2) | 0.018 (3) |
| C9 | 0.055 (3) | 0.059 (3) | 0.055 (3) | 0.006 (2) | −0.007 (2) | 0.008 (2) |
| C10 | 0.062 (3) | 0.057 (3) | 0.089 (4) | 0.012 (2) | −0.010 (3) | −0.001 (3) |
| C11 | 0.049 (2) | 0.045 (2) | 0.076 (3) | 0.0095 (19) | −0.006 (2) | 0.002 (2) |
| C12 | 0.055 (3) | 0.066 (3) | 0.075 (3) | 0.014 (2) | −0.003 (2) | 0.004 (2) |
| N2a | 0.038 (9) | 0.088 (12) | 0.020 (6) | 0.021 (7) | 0.006 (5) | 0.004 (6) |
| C13a | 0.059 (6) | 0.134 (13) | 0.042 (5) | 0.047 (7) | 0.005 (4) | 0.022 (6) |
| C14a | 0.051 (5) | 0.158 (15) | 0.042 (5) | 0.047 (7) | 0.013 (4) | 0.023 (6) |
| C15a | 0.055 (7) | 0.056 (11) | 0.038 (5) | 0.017 (6) | 0.002 (4) | 0.007 (5) |
| C16a | 0.044 (5) | 0.072 (8) | 0.039 (5) | 0.024 (5) | 0.005 (3) | 0.016 (5) |
| C17a | 0.044 (5) | 0.075 (9) | 0.044 (5) | 0.022 (5) | 0.008 (4) | 0.019 (5) |
| C18a | 0.048 (7) | 0.062 (12) | 0.047 (6) | 0.022 (7) | 0.011 (4) | 0.010 (5) |
| N12b | 0.060 (15) | 0.046 (10) | 0.068 (14) | 0.009 (8) | 0.001 (10) | 0.028 (8) |
| C113b | 0.082 (9) | 0.111 (14) | 0.041 (6) | −0.032 (9) | −0.007 (6) | 0.016 (7) |
| C114b | 0.082 (9) | 0.108 (14) | 0.047 (6) | −0.027 (9) | −0.006 (6) | 0.027 (7) |
| C115b | 0.048 (7) | 0.050 (11) | 0.030 (6) | 0.012 (5) | 0.006 (4) | 0.011 (5) |
| C116b | 0.071 (10) | 0.063 (9) | 0.044 (6) | 0.008 (7) | −0.002 (6) | 0.009 (6) |
| C117b | 0.058 (8) | 0.075 (11) | 0.046 (7) | 0.001 (7) | 0.011 (6) | 0.021 (7) |
| C118b | 0.062 (8) | 0.064 (15) | 0.031 (6) | 0.007 (9) | 0.009 (5) | 0.017 (6) |
| C19 | 0.052 (2) | 0.064 (3) | 0.038 (2) | 0.020 (2) | 0.0086 (17) | 0.0131 (18) |
| C20 | 0.048 (2) | 0.052 (2) | 0.040 (2) | 0.0163 (18) | 0.0068 (16) | 0.0120 (17) |
| C21 | 0.049 (2) | 0.070 (3) | 0.042 (2) | 0.025 (2) | 0.0068 (17) | 0.0194 (19) |
| C22 | 0.049 (2) | 0.069 (3) | 0.045 (2) | 0.027 (2) | 0.0090 (17) | 0.0205 (19) |
| C23 | 0.044 (2) | 0.051 (2) | 0.043 (2) | 0.0150 (17) | 0.0024 (16) | 0.0128 (17) |
| C24 | 0.047 (2) | 0.058 (2) | 0.042 (2) | 0.0177 (19) | 0.0074 (17) | 0.0123 (18) |
| C25 | 0.121 (12) | 0.103 (14) | 0.120 (12) | 0.033 (9) | 0.022 (8) | 0.019 (9) |
| O5 | 0.135 (14) | 0.16 (2) | 0.167 (19) | 0.046 (14) | 0.010 (12) | 0.026 (15) |
| N4 | 0.125 (12) | 0.109 (13) | 0.118 (11) | 0.028 (9) | 0.024 (7) | 0.013 (9) |
| C26 | 0.134 (14) | 0.103 (19) | 0.124 (19) | 0.027 (15) | 0.008 (12) | 0.020 (16) |
| C27 | 0.16 (2) | 0.14 (2) | 0.139 (18) | 0.033 (16) | 0.046 (16) | 0.030 (16) |
| Ni1—O1 | 2.017 (3) | C14a—H14a | 0.9300 |
| Ni1—O3i | 2.156 (3) | C14a—C15a | 1.364 (13) |
| Ni1—O4i | 2.144 (3) | C15a—C16a | 1.396 (14) |
| Ni1—N1 | 2.094 (3) | C15a—C18a | 1.467 (11) |
| Ni1—N3ii | 2.112 (3) | C16a—H16a | 0.9300 |
| Ni1—C6i | 2.472 (4) | C16a—C17a | 1.383 (11) |
| Ni1—N2 | 2.109 (9) | C17a—H17a | 0.9300 |
| Ni1—N12b | 2.079 (15) | C18a—H18a | 0.9300 |
| S1—C2 | 1.721 (4) | C18a—C19 | 1.31 (2) |
| S1—C5 | 1.714 (4) | N12b—C113b | 1.371 (14) |
| O1—C1 | 1.264 (5) | N12b—C117b | 1.300 (14) |
| O2—C1 | 1.236 (5) | C113b—H113b | 0.9300 |
| O3—Ni1iii | 2.156 (3) | C113b—C114b | 1.363 (12) |
| O3—C6 | 1.266 (5) | C114b—H114b | 0.9300 |
| O4—Ni1iii | 2.144 (3) | C114b—C115b | 1.359 (14) |
| O4—C6 | 1.268 (5) | C115b—C116b | 1.401 (14) |
| N1—C7 | 1.325 (6) | C115b—C118b | 1.470 (11) |
| N1—C11 | 1.347 (6) | C116b—H116b | 0.9300 |
| N3—Ni1iv | 2.112 (3) | C116b—C117b | 1.387 (13) |
| N3—C22 | 1.341 (5) | C117b—H117b | 0.9300 |
| N3—C23 | 1.347 (5) | C118b—H118b | 0.9300 |
| C1—C2 | 1.488 (5) | C118b—C19 | 1.35 (2) |
| C2—C3 | 1.349 (6) | C19—H19a | 0.9300 |
| C3—H3 | 0.9300 | C19—H19Ab | 0.9300 |
| C3—C4 | 1.414 (6) | C19—C20 | 1.461 (5) |
| C4—H4 | 0.9300 | C20—C21 | 1.393 (6) |
| C4—C5 | 1.347 (6) | C20—C24 | 1.391 (6) |
| C5—C6 | 1.476 (5) | C21—H21 | 0.9300 |
| C6—Ni1iii | 2.472 (4) | C21—C22 | 1.355 (6) |
| C7—H7 | 0.9300 | C22—H22 | 0.9300 |
| C7—C8 | 1.381 (6) | C23—H23 | 0.9300 |
| C8—H8 | 0.9300 | C23—C24 | 1.370 (5) |
| C8—C9 | 1.393 (7) | C24—H24 | 0.9300 |
| C9—C10 | 1.363 (7) | C25—H25 | 0.9300 |
| C9—C12 | 1.486 (6) | C25—O5 | 1.213 (19) |
| C10—H10 | 0.9300 | C25—N4 | 1.34 (2) |
| C10—C11 | 1.366 (7) | N4—C26 | 1.47 (2) |
| C11—H11 | 0.9300 | N4—C27 | 1.46 (2) |
| C12—C12v | 1.290 (10) | C26—H26A | 0.9600 |
| C12—H12 | 0.9300 | C26—H26B | 0.9600 |
| N2a—C13a | 1.352 (8) | C26—H26C | 0.9600 |
| N2a—C17a | 1.323 (8) | C27—H27A | 0.9600 |
| C13a—H13a | 0.9300 | C27—H27B | 0.9600 |
| C13a—C14a | 1.355 (11) | C27—H27C | 0.9600 |
| O1—Ni1—O3i | 172.16 (11) | N2a—C13a—H13a | 118.3 |
| O1—Ni1—O4i | 110.62 (11) | N2a—C13a—C14a | 123.4 (8) |
| O1—Ni1—N1 | 90.21 (13) | C14a—C13a—H13a | 118.3 |
| O1—Ni1—N3ii | 91.18 (12) | C13a—C14a—H14a | 119.6 |
| O1—Ni1—C6i | 141.40 (13) | C13a—C14a—C15a | 120.8 (9) |
| O1—Ni1—N2a | 90.2 (5) | C15a—C14a—H14a | 119.6 |
| O1—Ni1—N12b | 90.1 (5) | C14a—C15a—C16a | 116.4 (10) |
| O3i—Ni1—C6i | 30.80 (12) | C14a—C15a—C18a | 120.5 (13) |
| O4i—Ni1—O3i | 61.62 (10) | C16a—C15a—C18a | 122.4 (13) |
| O4i—Ni1—C6i | 30.85 (11) | C15a—C16a—H16a | 120.4 |
| N1—Ni1—O3i | 97.44 (12) | C17a—C16a—C15a | 119.1 (9) |
| N1—Ni1—O4i | 158.61 (12) | C17a—C16a—H16a | 120.4 |
| N1—Ni1—N3ii | 87.44 (13) | N2a—C17a—C16a | 123.9 (10) |
| N1—Ni1—C6i | 127.99 (13) | N2a—C17a—H17a | 118.1 |
| N1—Ni1—N2a | 95.7 (3) | C16a—C17a—H17a | 118.1 |
| N3ii—Ni1—O3i | 87.47 (12) | C15a—C18a—H18a | 116.6 |
| N3ii—Ni1—O4i | 87.32 (12) | C19—C18a—C15a | 126.8 (16) |
| N3ii—Ni1—C6i | 85.91 (13) | C19—C18a—H18a | 116.6 |
| N2a—Ni1—O3i | 90.7 (5) | C113b—N12b—Ni1 | 120.4 (11) |
| N2a—Ni1—O4i | 89.2 (4) | C117b—N12b—Ni1 | 123.5 (10) |
| N2a—Ni1—N3ii | 176.6 (4) | C117b—N12b—C113b | 113.9 (12) |
| N2a—Ni1—C6i | 91.0 (5) | N12b—C113b—H113b | 118.3 |
| N12b—Ni1—O3i | 91.1 (5) | C114b—C113b—N12b | 123.4 (11) |
| N12b—Ni1—O4i | 91.1 (4) | C114b—C113b—H113b | 118.3 |
| N12b—Ni1—N1 | 93.8 (4) | C113b—C114b—H114b | 119.5 |
| N12b—Ni1—N3ii | 178.3 (5) | C115b—C114b—C113b | 121.0 (11) |
| N12b—Ni1—C6i | 92.4 (5) | C115b—C114b—H114b | 119.5 |
| C5—S1—C2 | 91.8 (2) | C114b—C115b—C116b | 116.6 (11) |
| C1—O1—Ni1 | 125.3 (3) | C114b—C115b—C118b | 121.4 (14) |
| C6—O3—Ni1iii | 88.5 (2) | C116b—C115b—C118b | 122.0 (13) |
| C6—O4—Ni1iii | 89.0 (2) | C115b—C116b—H116b | 121.1 |
| C7—N1—Ni1 | 122.3 (3) | C117b—C116b—C115b | 117.9 (12) |
| C7—N1—C11 | 116.5 (4) | C117b—C116b—H116b | 121.1 |
| C11—N1—Ni1 | 119.3 (3) | N12b—C117b—C116b | 126.0 (13) |
| C22—N3—Ni1iv | 122.7 (3) | N12b—C117b—H117b | 117.0 |
| C22—N3—C23 | 116.0 (3) | C116b—C117b—H117b | 117.0 |
| C23—N3—Ni1iv | 121.2 (3) | C115b—C118b—H118b | 116.9 |
| O1—C1—C2 | 115.4 (4) | C19—C118b—C115b | 126.3 (19) |
| O2—C1—O1 | 126.2 (4) | C19—C118b—H118b | 116.9 |
| O2—C1—C2 | 118.3 (4) | C18a—C19—H19a | 117.9 |
| C1—C2—S1 | 121.0 (3) | C18a—C19—C20 | 124.2 (8) |
| C3—C2—S1 | 111.0 (3) | C118b—C19—H19Ab | 118.5 |
| C3—C2—C1 | 127.9 (4) | C118b—C19—C20 | 123.0 (9) |
| C2—C3—H3 | 123.6 | C20—C19—H19a | 117.9 |
| C2—C3—C4 | 112.9 (4) | C20—C19—H19Ab | 118.5 |
| C4—C3—H3 | 123.6 | C21—C20—C19 | 122.8 (4) |
| C3—C4—H4 | 123.4 | C24—C20—C19 | 121.2 (4) |
| C5—C4—C3 | 113.1 (4) | C24—C20—C21 | 116.0 (4) |
| C5—C4—H4 | 123.4 | C20—C21—H21 | 119.9 |
| C4—C5—S1 | 111.2 (3) | C22—C21—C20 | 120.1 (4) |
| C4—C5—C6 | 127.3 (4) | C22—C21—H21 | 119.9 |
| C6—C5—S1 | 121.4 (3) | N3—C22—C21 | 124.3 (4) |
| O3—C6—Ni1iii | 60.67 (19) | N3—C22—H22 | 117.8 |
| O3—C6—O4 | 120.7 (3) | C21—C22—H22 | 117.8 |
| O3—C6—C5 | 120.6 (3) | N3—C23—H23 | 118.5 |
| O4—C6—Ni1iii | 60.12 (19) | N3—C23—C24 | 123.1 (4) |
| O4—C6—C5 | 118.7 (4) | C24—C23—H23 | 118.5 |
| C5—C6—Ni1iii | 176.5 (3) | C20—C24—H24 | 119.8 |
| N1—C7—H7 | 118.2 | C23—C24—C20 | 120.5 (4) |
| N1—C7—C8 | 123.5 (4) | C23—C24—H24 | 119.8 |
| C8—C7—H7 | 118.2 | O5—C25—H25 | 120.0 |
| C7—C8—H8 | 120.3 | O5—C25—N4 | 120 (4) |
| C7—C8—C9 | 119.4 (5) | N4—C25—H25 | 120.0 |
| C9—C8—H8 | 120.3 | C25—N4—C26 | 115 (3) |
| C8—C9—C12 | 124.6 (5) | C25—N4—C27 | 127 (4) |
| C10—C9—C8 | 116.7 (4) | C27—N4—C26 | 118 (4) |
| C10—C9—C12 | 118.7 (5) | N4—C26—H26A | 109.5 |
| C9—C10—H10 | 119.6 | N4—C26—H26B | 109.5 |
| C9—C10—C11 | 120.8 (5) | N4—C26—H26C | 109.5 |
| C11—C10—H10 | 119.6 | H26A—C26—H26B | 109.5 |
| N1—C11—C10 | 123.1 (5) | H26A—C26—H26C | 109.5 |
| N1—C11—H11 | 118.4 | H26B—C26—H26C | 109.5 |
| C10—C11—H11 | 118.4 | N4—C27—H27A | 109.5 |
| C9—C12—H12 | 117.2 | N4—C27—H27B | 109.5 |
| C12v—C12—C9 | 125.6 (7) | N4—C27—H27C | 109.5 |
| C12v—C12—H12 | 117.2 | H27A—C27—H27B | 109.5 |
| C13a—N2a—Ni1 | 123.1 (8) | H27A—C27—H27C | 109.5 |
| C17a—N2a—Ni1 | 121.1 (7) | H27B—C27—H27C | 109.5 |
| C17a—N2a—C13a | 115.5 (9) | ||
| Ni1—O1—C1—O2 | −14.6 (7) | C10—C9—C12—C12v | 175.1 (8) |
| Ni1—O1—C1—C2 | 167.8 (3) | C11—N1—C7—C8 | −0.5 (7) |
| Ni1iii—O3—C6—O4 | −3.5 (4) | C12—C9—C10—C11 | 179.0 (5) |
| Ni1iii—O3—C6—C5 | 176.2 (4) | N2a—C13a—C14a—C15a | 9 (3) |
| Ni1iii—O4—C6—O3 | 3.6 (4) | C13a—N2a—C17a—C16a | 9 (2) |
| Ni1iii—O4—C6—C5 | −176.2 (4) | C13a—C14a—C15a—C16a | −5 (3) |
| Ni1—N1—C7—C8 | 163.5 (4) | C13a—C14a—C15a—C18a | −176.3 (15) |
| Ni1—N1—C11—C10 | −163.1 (4) | C14a—C15a—C16a—C17a | 4 (2) |
| Ni1iv—N3—C22—C21 | 178.4 (4) | C14a—C15a—C18a—C19 | 176.7 (16) |
| Ni1iv—N3—C23—C24 | −179.0 (3) | C15a—C16a—C17a—N2a | −6 (2) |
| Ni1—N2a—C13a—C14a | 176.4 (12) | C15a—C18a—C19—C20 | 179.3 (13) |
| Ni1—N2a—C17a—C16a | −177.7 (11) | C16a—C15a—C18a—C19 | 6 (3) |
| Ni1—N12b—C113b—C114b | 174.4 (16) | C17a—N2a—C13a—C14a | −10 (2) |
| Ni1—N12b—C117b—C116b | −176.8 (14) | C18a—C15a—C16a—C17a | 174.6 (14) |
| S1—C2—C3—C4 | −0.7 (7) | C18a—C19—C20—C21 | −8.4 (13) |
| S1—C5—C6—O3 | −7.8 (6) | C18a—C19—C20—C24 | 173.0 (11) |
| S1—C5—C6—O4 | 172.0 (3) | N12b—C113b—C114b—C115b | −5 (3) |
| O1—C1—C2—S1 | 4.6 (6) | C113b—N12b—C117b—C116b | −13 (3) |
| O1—C1—C2—C3 | −178.1 (5) | C113b—C114b—C115b—C116b | 1 (3) |
| O2—C1—C2—S1 | −173.2 (4) | C113b—C114b—C115b—C118b | 180 (2) |
| O2—C1—C2—C3 | 4.1 (8) | C114b—C115b—C116b—C117b | −3 (3) |
| N1—C7—C8—C9 | −0.6 (8) | C114b—C115b—C118b—C19 | 160 (2) |
| N3—C23—C24—C20 | 1.2 (7) | C115b—C116b—C117b—N12b | 10 (3) |
| C1—C2—C3—C4 | −178.2 (5) | C115b—C118b—C19—C20 | 177.9 (16) |
| C2—S1—C5—C4 | −1.1 (5) | C116b—C115b—C118b—C19 | −21 (3) |
| C2—S1—C5—C6 | 179.7 (4) | C117b—N12b—C113b—C114b | 10 (3) |
| C2—C3—C4—C5 | −0.1 (8) | C118b—C115b—C116b—C117b | 178.2 (19) |
| C3—C4—C5—S1 | 0.9 (7) | C118b—C19—C20—C21 | −31.1 (15) |
| C3—C4—C5—C6 | 180.0 (5) | C118b—C19—C20—C24 | 150.4 (14) |
| C4—C5—C6—O3 | 173.2 (5) | C19—C20—C21—C22 | −178.1 (4) |
| C4—C5—C6—O4 | −7.1 (8) | C19—C20—C24—C23 | 177.6 (4) |
| C5—S1—C2—C1 | 178.7 (4) | C20—C21—C22—N3 | −0.2 (7) |
| C5—S1—C2—C3 | 1.0 (5) | C21—C20—C24—C23 | −1.0 (6) |
| C7—N1—C11—C10 | 1.3 (7) | C22—N3—C23—C24 | −0.8 (6) |
| C7—C8—C9—C10 | 0.9 (8) | C23—N3—C22—C21 | 0.3 (7) |
| C7—C8—C9—C12 | −178.2 (5) | C24—C20—C21—C22 | 0.5 (7) |
| C8—C9—C10—C11 | −0.1 (8) | O5—C25—N4—C26 | −179 (3) |
| C8—C9—C12—C12v | −5.8 (11) | O5—C25—N4—C27 | −1 (3) |
| C9—C10—C11—N1 | −1.1 (9) |
| Symmetry codes: (i) x, y+1, z; (ii) x, y, z−1; (iii) x, y−1, z; (iv) x, y, z+1; (v) −x, −y+1, −z. |
| Cg1, Cg2 and Cg3 are the centroids of rings (N2A,C13A–C17A), (N3,C20–C24) and (N1,C7–C11), respectively. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C8—H8···O2vi | 0.93 | 2.59 | 3.314 (7) | 135 |
| C19—H19A···O4vii | 0.93 | 2.51 | 3.430 (6) | 169 |
| C21—H21···O3viii | 0.93 | 2.41 | 3.331 (6) | 171 |
| C27—H27C···Cg1 | 0.96 | 2.78 | 3.57 (6) | 140 |
| C10—H10···Cg2viii | 0.93 | 2.88 | 3.696 (6) | 147 |
| C22—H22···Cg3iv | 0.93 | 2.93 | 3.534 (5) | 124 |
| Symmetry codes: (iv) x, y, z+1; (vi) x−1, y, z; (vii) −x+2, −y+1, −z+1; (viii) −x+1, −y+1, −z+1. |
Acknowledgements
CR and XJ acknowledge the China Scholarship Council (CSC) for doctoral fellowships. We thank Professor Tatjana N. Parac-Vogt and Professor Wim Dehaen for access to powder X-ray diffraction facilities and laboratory resources for synthesis. We thank Dongjing Hong (Anhui Normal University, China) for providing access to the X-ray diffractometer. We acknowledge the use of the DIRAC computer cluster (Department of Chemistry, KU Leuven) for computational resources.
References
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