research communications\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

An unusual two-dimensional MOF formed from NiII, thio­phene-2,5-di­carboxyl­ate and trans-1,2-bis­­(pyridin-4-yl)ethyl­ene

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aDepartment of Chemistry, KU Leuven, Biomolecular Architecture, Celestijnenlaan 200F, Leuven (Heverlee), B-3001, Belgium
*Correspondence e-mail: [email protected]

Edited by F. Di Salvo, University of Buenos Aires, Argentina (Received 12 January 2026; accepted 2 March 2026; online 5 March 2026)

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.

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., 2013View full citation). 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, 2012View full citation). 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., 2015View full citation).

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 ππ inter­actions and other weak supra­molecular contacts (Thuéry & Harrowfield, 2022View full citation; Zheng et al., 2008View full citation). 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., 2019View full citation; Zhang et al., 2012View full citation). 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., 2017View full citation). Moreover, closely related systems based on the same (or very similar) linker combinations more commonly form twofold inter­penetrated 3D frameworks (Jia et al., 2024View full citation; Alamgir et al., 2021View full citation; Sen et al., 2013View full citation), highlighting an unusual structure–composition relationship for Ni-HT-Bpe.

[Scheme 1]

2. Structural commentary

The Ni-HT-Bpe structure crystallizes in the triclinic space group PMathematical equation 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[link]). 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]
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[link]). 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[link], Fig. 2[link]). 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[link]). Oxygen atoms O3 and O4 also show hydrogen bonds with the other Bpe mol­ecule (atoms H21 and H19A, respectively, see Table 2[link]).

Table 1
Selected bond lengths (Å)

Ni1—O1 2.017 (3) Ni1—N1 2.094 (3)
Ni1—O3i 2.156 (3) Ni1—N3ii 2.112 (3)
Ni1—O4i 2.144 (3) Ni1—N2 2.109 (9)
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.

Table 2
Hydrogen-bond geometry (Å, °)

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 DA D—H⋯A
C8—H8⋯O2iii 0.93 2.59 3.314 (7) 135
C19—H19A⋯O4iv 0.93 2.51 3.430 (6) 169
C21—H21⋯O3v 0.93 2.41 3.331 (6) 171
C27—H27CCg1 0.96 2.78 3.57 (6) 140
C10—H10⋯Cg2v 0.93 2.88 3.696 (6) 147
C22—H22⋯Cg3vi 0.93 2.93 3.534 (5) 124
Symmetry codes: (iii) Mathematical equation; (iv) Mathematical equation; (v) Mathematical equation; (vi) Mathematical equation.
[Figure 2]
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[link]). 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[link].

A void-space representation was generated using Mercury (Macrae et al., 2020View full citation) for the solvent-free structural model (Fig. 3[link]). 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., 2012View full citation) in high-accuracy mode using the solvent-free CIF. The framework exhibits a substantial geometric void volume of 454.2 Å3 per unit cell, 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]
Figure 3
Visualization of the voids in the crystal packing of Ni-HT-Bpe using Mercury (Macrae et al., 2020View full citation).

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[link]; Blatov et al., 2014View full citation). 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]
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., 2016View full citation) 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., 2007View full citation) 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., 2018View full citation), 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[link].

[Figure 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., 2020View full citation), confirming that the crystalline powder material is consistent with the single-crystal model (Fig. 6[link]). Noticeable discrepancies in relative intensities are observed. As the sample contains both needle-shaped and block-like crystals (Fig. 7[link]), 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]
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., 2020View full citation) based on the single-crystal structure.
[Figure 7]
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 refinement details are summarized in Table 3[link]. 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.

Table 3
Experimental details

Crystal data
Chemical formula [Ni(C6H3O4S)(C12H10N2)1.5]·0.205C3H7NO
Mr 517.08
Crystal system, space group Triclinic, PMathematical equation
Temperature (K) 273
a, b, c (Å) 9.7666 (4), 9.8999 (4), 13.5669 (6)
α, β, γ (°) 98.092 (2), 96.235 (2), 107.823 (2)
V3) 1220.25 (9)
Z 2
Radiation type Cu Kα
μ (mm−1) 2.26
Crystal size (mm) 0.15 × 0.13 × 0.12
 
Data collection
Diffractometer Bruker D8 Venture
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.487, 0.754
No. of measured, independent and observed [I > 2σ(I)] reflections 16259, 4801, 3940
Rint 0.058
(sin θ/λ)max−1) 0.620
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.066, 0.185, 1.04
No. of reflections 4801
No. of parameters 411
No. of restraints 77
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.43, −0.60
Computer programs: SAINT (Bruker, 2015View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2016/4 (Sheldrick, 2015bView full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

Poly[[sesqui[µ-trans-1,2-bis(pyridin-4-yl)ethylene](µ-thiophene-2,5-dicarboxylato)nickel(II)] dimethylformamide 0.205-solvate] top
Crystal data top
[Ni(C6H3O4S)(C12H10N2)1.5]·0.205C3H7NOZ = 2
Mr = 517.08F(000) = 532
Triclinic, P1Dx = 1.407 Mg m3
a = 9.7666 (4) ÅCu Kα radiation, λ = 1.54178 Å
b = 9.8999 (4) ÅCell parameters from 8971 reflections
c = 13.5669 (6) Åθ = 5.6–72.4°
α = 98.092 (2)°µ = 2.26 mm1
β = 96.235 (2)°T = 273 K
γ = 107.823 (2)°Block, clear light green
V = 1220.25 (9) Å30.15 × 0.13 × 0.12 mm
Data collection top
Bruker D8 Venture
diffractometer
3940 reflections with I > 2σ(I)
Detector resolution: 7.9 pixels mm-1Rint = 0.058
φ and ω scansθmax = 73.0°, θmin = 5.6°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1012
Tmin = 0.487, Tmax = 0.754k = 1212
16259 measured reflectionsl = 1616
4801 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-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 = 1.04Δρmax = 0.43 e Å3
4801 reflectionsΔρmin = 0.60 e Å3
411 parametersExtinction correction: SHELXL-2016/4 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
77 restraintsExtinction coefficient: 0.0106 (15)
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Ni10.69283 (7)0.86205 (6)0.22629 (4)0.0380 (3)
S10.75169 (11)0.38941 (11)0.23040 (9)0.0504 (3)
O10.7559 (3)0.6858 (3)0.2229 (2)0.0504 (7)
O20.9965 (4)0.7930 (3)0.2616 (3)0.0727 (10)
O30.6566 (3)0.0670 (3)0.2320 (2)0.0470 (6)
O40.8783 (3)0.0550 (3)0.2622 (2)0.0459 (6)
N10.4762 (4)0.7301 (4)0.1770 (2)0.0458 (8)
N30.7129 (4)0.8640 (3)1.0730 (2)0.0423 (7)
C10.8847 (5)0.6871 (4)0.2486 (3)0.0485 (9)
C20.8999 (5)0.5449 (4)0.2600 (4)0.0516 (10)
C31.0229 (5)0.5158 (5)0.2889 (5)0.0751 (16)
H31.1143250.5859190.3071820.090*
C40.9981 (5)0.3673 (5)0.2886 (5)0.0744 (16)
H41.0716060.3296470.3064740.089*
C50.8571 (5)0.2859 (4)0.2596 (4)0.0518 (10)
C60.7934 (4)0.1281 (4)0.2508 (3)0.0434 (8)
C70.3659 (5)0.7815 (5)0.1773 (3)0.0537 (10)
H70.3820730.8720900.2158110.064*
C80.2282 (5)0.7078 (6)0.1236 (4)0.0649 (12)
H80.1540930.7482130.1268370.078*
C90.2014 (5)0.5726 (5)0.0647 (4)0.0607 (12)
C100.3152 (6)0.5201 (6)0.0651 (5)0.0744 (15)
H100.3020920.4301020.0268840.089*
C110.4482 (5)0.5981 (5)0.1210 (4)0.0604 (12)
H110.5228860.5582890.1203860.072*
C120.0596 (5)0.4845 (6)0.0014 (4)0.0686 (13)
H120.0565380.3997990.0397580.082*
N2a0.6832 (11)0.8719 (19)0.3816 (7)0.049 (6)0.544 (17)
C13a0.5639 (11)0.877 (2)0.4220 (7)0.074 (4)0.544 (17)
H13a0.4843070.8813020.3798700.089*0.544 (17)
C14a0.5542 (11)0.876 (2)0.5208 (6)0.080 (5)0.544 (17)
H14a0.4651010.8653000.5425900.096*0.544 (17)
C15a0.6735 (16)0.889 (2)0.5887 (9)0.051 (4)0.544 (17)
C16a0.8002 (12)0.8912 (16)0.5493 (8)0.050 (3)0.544 (17)
H16a0.8834350.8942230.5912510.060*0.544 (17)
C17a0.8004 (13)0.8888 (16)0.4472 (9)0.053 (3)0.544 (17)
H17a0.8881200.8997230.4232080.064*0.544 (17)
C18a0.660 (2)0.879 (2)0.6943 (10)0.051 (5)0.544 (17)
H18a0.5689030.8679910.7123120.062*0.544 (17)
N12b0.6761 (16)0.867 (2)0.3781 (12)0.059 (9)0.456 (17)
C113b0.5687 (17)0.762 (2)0.4074 (8)0.094 (7)0.456 (17)
H113b0.4988860.6938130.3576040.113*0.456 (17)
C114b0.5589 (17)0.752 (2)0.5057 (8)0.092 (7)0.456 (17)
H114b0.4796590.6821220.5211120.111*0.456 (17)
C115b0.6630 (16)0.841 (2)0.5816 (9)0.043 (4)0.456 (17)
C116b0.779 (2)0.9444 (17)0.5532 (10)0.064 (4)0.456 (17)
H116b0.8515991.0119180.6013560.076*0.456 (17)
C117b0.7812 (19)0.9422 (19)0.4510 (10)0.063 (5)0.456 (17)
H117b0.8657491.0000820.4328540.076*0.456 (17)
C118b0.653 (3)0.832 (3)0.6879 (11)0.054 (6)0.456 (17)
H118b0.5610790.7867060.7026990.065*0.456 (17)
C190.7642 (5)0.8832 (5)0.7661 (3)0.0506 (10)
H19a0.8561780.8928610.7494470.061*0.544 (17)
H19Ab0.8576260.9262080.7529320.061*0.456 (17)
C200.7444 (4)0.8739 (5)0.8704 (3)0.0468 (9)
C210.6174 (5)0.8778 (5)0.9068 (3)0.0517 (10)
H210.5396620.8836910.8635570.062*
C220.6070 (5)0.8729 (5)1.0051 (3)0.0512 (10)
H220.5207910.8759311.0268750.061*
C230.8363 (4)0.8605 (4)1.0386 (3)0.0462 (9)
H230.9126590.8555571.0837460.055*
C240.8546 (5)0.8638 (5)0.9401 (3)0.0486 (9)
H240.9412290.8592880.9198130.058*
C250.532 (4)0.489 (3)0.613 (3)0.115 (10)0.205 (7)
H250.4690780.4886210.6597630.138*0.205 (7)
O50.653 (4)0.486 (4)0.638 (3)0.158 (12)0.205 (7)
N40.488 (4)0.494 (4)0.517 (3)0.120 (9)0.205 (7)
C260.339 (4)0.500 (5)0.496 (4)0.124 (11)0.205 (7)
H26A0.2859010.4685940.5482000.186*0.205 (7)
H26B0.2902520.4389900.4321790.186*0.205 (7)
H26C0.3433900.5979640.4922580.186*0.205 (7)
C270.571 (6)0.498 (6)0.434 (4)0.147 (15)0.205 (7)
H27A0.5195680.4190880.3801240.221*0.205 (7)
H27B0.6645060.4905550.4573240.221*0.205 (7)
H27C0.5846400.5876070.4105280.221*0.205 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ni10.0410 (4)0.0368 (4)0.0366 (4)0.0120 (3)0.0031 (2)0.0118 (2)
S10.0459 (6)0.0397 (5)0.0669 (7)0.0161 (4)0.0007 (4)0.0156 (4)
O10.0501 (16)0.0438 (15)0.0586 (17)0.0175 (12)0.0002 (13)0.0154 (12)
O20.0541 (19)0.0419 (17)0.122 (3)0.0139 (15)0.0082 (19)0.0239 (18)
O30.0405 (15)0.0428 (14)0.0574 (16)0.0143 (12)0.0012 (12)0.0118 (12)
O40.0429 (14)0.0370 (13)0.0607 (17)0.0163 (11)0.0027 (12)0.0152 (12)
N10.0434 (17)0.0473 (18)0.0438 (17)0.0093 (14)0.0025 (14)0.0148 (14)
N30.0473 (18)0.0440 (17)0.0391 (16)0.0176 (14)0.0055 (13)0.0139 (13)
C10.053 (2)0.041 (2)0.053 (2)0.0175 (18)0.0045 (18)0.0138 (17)
C20.051 (2)0.041 (2)0.066 (3)0.0169 (18)0.0047 (19)0.0168 (18)
C30.049 (3)0.043 (2)0.129 (5)0.011 (2)0.005 (3)0.027 (3)
C40.052 (3)0.044 (2)0.127 (5)0.019 (2)0.005 (3)0.024 (3)
C50.049 (2)0.036 (2)0.072 (3)0.0162 (17)0.004 (2)0.0154 (18)
C60.045 (2)0.0387 (19)0.047 (2)0.0141 (16)0.0049 (16)0.0112 (16)
C70.048 (2)0.060 (3)0.049 (2)0.015 (2)0.0038 (18)0.0068 (19)
C80.048 (2)0.077 (3)0.070 (3)0.021 (2)0.004 (2)0.018 (3)
C90.055 (3)0.059 (3)0.055 (3)0.006 (2)0.007 (2)0.008 (2)
C100.062 (3)0.057 (3)0.089 (4)0.012 (2)0.010 (3)0.001 (3)
C110.049 (2)0.045 (2)0.076 (3)0.0095 (19)0.006 (2)0.002 (2)
C120.055 (3)0.066 (3)0.075 (3)0.014 (2)0.003 (2)0.004 (2)
N2a0.038 (9)0.088 (12)0.020 (6)0.021 (7)0.006 (5)0.004 (6)
C13a0.059 (6)0.134 (13)0.042 (5)0.047 (7)0.005 (4)0.022 (6)
C14a0.051 (5)0.158 (15)0.042 (5)0.047 (7)0.013 (4)0.023 (6)
C15a0.055 (7)0.056 (11)0.038 (5)0.017 (6)0.002 (4)0.007 (5)
C16a0.044 (5)0.072 (8)0.039 (5)0.024 (5)0.005 (3)0.016 (5)
C17a0.044 (5)0.075 (9)0.044 (5)0.022 (5)0.008 (4)0.019 (5)
C18a0.048 (7)0.062 (12)0.047 (6)0.022 (7)0.011 (4)0.010 (5)
N12b0.060 (15)0.046 (10)0.068 (14)0.009 (8)0.001 (10)0.028 (8)
C113b0.082 (9)0.111 (14)0.041 (6)0.032 (9)0.007 (6)0.016 (7)
C114b0.082 (9)0.108 (14)0.047 (6)0.027 (9)0.006 (6)0.027 (7)
C115b0.048 (7)0.050 (11)0.030 (6)0.012 (5)0.006 (4)0.011 (5)
C116b0.071 (10)0.063 (9)0.044 (6)0.008 (7)0.002 (6)0.009 (6)
C117b0.058 (8)0.075 (11)0.046 (7)0.001 (7)0.011 (6)0.021 (7)
C118b0.062 (8)0.064 (15)0.031 (6)0.007 (9)0.009 (5)0.017 (6)
C190.052 (2)0.064 (3)0.038 (2)0.020 (2)0.0086 (17)0.0131 (18)
C200.048 (2)0.052 (2)0.040 (2)0.0163 (18)0.0068 (16)0.0120 (17)
C210.049 (2)0.070 (3)0.042 (2)0.025 (2)0.0068 (17)0.0194 (19)
C220.049 (2)0.069 (3)0.045 (2)0.027 (2)0.0090 (17)0.0205 (19)
C230.044 (2)0.051 (2)0.043 (2)0.0150 (17)0.0024 (16)0.0128 (17)
C240.047 (2)0.058 (2)0.042 (2)0.0177 (19)0.0074 (17)0.0123 (18)
C250.121 (12)0.103 (14)0.120 (12)0.033 (9)0.022 (8)0.019 (9)
O50.135 (14)0.16 (2)0.167 (19)0.046 (14)0.010 (12)0.026 (15)
N40.125 (12)0.109 (13)0.118 (11)0.028 (9)0.024 (7)0.013 (9)
C260.134 (14)0.103 (19)0.124 (19)0.027 (15)0.008 (12)0.020 (16)
C270.16 (2)0.14 (2)0.139 (18)0.033 (16)0.046 (16)0.030 (16)
Geometric parameters (Å, º) top
Ni1—O12.017 (3)C14a—H14a0.9300
Ni1—O3i2.156 (3)C14a—C15a1.364 (13)
Ni1—O4i2.144 (3)C15a—C16a1.396 (14)
Ni1—N12.094 (3)C15a—C18a1.467 (11)
Ni1—N3ii2.112 (3)C16a—H16a0.9300
Ni1—C6i2.472 (4)C16a—C17a1.383 (11)
Ni1—N22.109 (9)C17a—H17a0.9300
Ni1—N12b2.079 (15)C18a—H18a0.9300
S1—C21.721 (4)C18a—C191.31 (2)
S1—C51.714 (4)N12b—C113b1.371 (14)
O1—C11.264 (5)N12b—C117b1.300 (14)
O2—C11.236 (5)C113b—H113b0.9300
O3—Ni1iii2.156 (3)C113b—C114b1.363 (12)
O3—C61.266 (5)C114b—H114b0.9300
O4—Ni1iii2.144 (3)C114b—C115b1.359 (14)
O4—C61.268 (5)C115b—C116b1.401 (14)
N1—C71.325 (6)C115b—C118b1.470 (11)
N1—C111.347 (6)C116b—H116b0.9300
N3—Ni1iv2.112 (3)C116b—C117b1.387 (13)
N3—C221.341 (5)C117b—H117b0.9300
N3—C231.347 (5)C118b—H118b0.9300
C1—C21.488 (5)C118b—C191.35 (2)
C2—C31.349 (6)C19—H19a0.9300
C3—H30.9300C19—H19Ab0.9300
C3—C41.414 (6)C19—C201.461 (5)
C4—H40.9300C20—C211.393 (6)
C4—C51.347 (6)C20—C241.391 (6)
C5—C61.476 (5)C21—H210.9300
C6—Ni1iii2.472 (4)C21—C221.355 (6)
C7—H70.9300C22—H220.9300
C7—C81.381 (6)C23—H230.9300
C8—H80.9300C23—C241.370 (5)
C8—C91.393 (7)C24—H240.9300
C9—C101.363 (7)C25—H250.9300
C9—C121.486 (6)C25—O51.213 (19)
C10—H100.9300C25—N41.34 (2)
C10—C111.366 (7)N4—C261.47 (2)
C11—H110.9300N4—C271.46 (2)
C12—C12v1.290 (10)C26—H26A0.9600
C12—H120.9300C26—H26B0.9600
N2a—C13a1.352 (8)C26—H26C0.9600
N2a—C17a1.323 (8)C27—H27A0.9600
C13a—H13a0.9300C27—H27B0.9600
C13a—C14a1.355 (11)C27—H27C0.9600
O1—Ni1—O3i172.16 (11)N2a—C13a—H13a118.3
O1—Ni1—O4i110.62 (11)N2a—C13a—C14a123.4 (8)
O1—Ni1—N190.21 (13)C14a—C13a—H13a118.3
O1—Ni1—N3ii91.18 (12)C13a—C14a—H14a119.6
O1—Ni1—C6i141.40 (13)C13a—C14a—C15a120.8 (9)
O1—Ni1—N2a90.2 (5)C15a—C14a—H14a119.6
O1—Ni1—N12b90.1 (5)C14a—C15a—C16a116.4 (10)
O3i—Ni1—C6i30.80 (12)C14a—C15a—C18a120.5 (13)
O4i—Ni1—O3i61.62 (10)C16a—C15a—C18a122.4 (13)
O4i—Ni1—C6i30.85 (11)C15a—C16a—H16a120.4
N1—Ni1—O3i97.44 (12)C17a—C16a—C15a119.1 (9)
N1—Ni1—O4i158.61 (12)C17a—C16a—H16a120.4
N1—Ni1—N3ii87.44 (13)N2a—C17a—C16a123.9 (10)
N1—Ni1—C6i127.99 (13)N2a—C17a—H17a118.1
N1—Ni1—N2a95.7 (3)C16a—C17a—H17a118.1
N3ii—Ni1—O3i87.47 (12)C15a—C18a—H18a116.6
N3ii—Ni1—O4i87.32 (12)C19—C18a—C15a126.8 (16)
N3ii—Ni1—C6i85.91 (13)C19—C18a—H18a116.6
N2a—Ni1—O3i90.7 (5)C113b—N12b—Ni1120.4 (11)
N2a—Ni1—O4i89.2 (4)C117b—N12b—Ni1123.5 (10)
N2a—Ni1—N3ii176.6 (4)C117b—N12b—C113b113.9 (12)
N2a—Ni1—C6i91.0 (5)N12b—C113b—H113b118.3
N12b—Ni1—O3i91.1 (5)C114b—C113b—N12b123.4 (11)
N12b—Ni1—O4i91.1 (4)C114b—C113b—H113b118.3
N12b—Ni1—N193.8 (4)C113b—C114b—H114b119.5
N12b—Ni1—N3ii178.3 (5)C115b—C114b—C113b121.0 (11)
N12b—Ni1—C6i92.4 (5)C115b—C114b—H114b119.5
C5—S1—C291.8 (2)C114b—C115b—C116b116.6 (11)
C1—O1—Ni1125.3 (3)C114b—C115b—C118b121.4 (14)
C6—O3—Ni1iii88.5 (2)C116b—C115b—C118b122.0 (13)
C6—O4—Ni1iii89.0 (2)C115b—C116b—H116b121.1
C7—N1—Ni1122.3 (3)C117b—C116b—C115b117.9 (12)
C7—N1—C11116.5 (4)C117b—C116b—H116b121.1
C11—N1—Ni1119.3 (3)N12b—C117b—C116b126.0 (13)
C22—N3—Ni1iv122.7 (3)N12b—C117b—H117b117.0
C22—N3—C23116.0 (3)C116b—C117b—H117b117.0
C23—N3—Ni1iv121.2 (3)C115b—C118b—H118b116.9
O1—C1—C2115.4 (4)C19—C118b—C115b126.3 (19)
O2—C1—O1126.2 (4)C19—C118b—H118b116.9
O2—C1—C2118.3 (4)C18a—C19—H19a117.9
C1—C2—S1121.0 (3)C18a—C19—C20124.2 (8)
C3—C2—S1111.0 (3)C118b—C19—H19Ab118.5
C3—C2—C1127.9 (4)C118b—C19—C20123.0 (9)
C2—C3—H3123.6C20—C19—H19a117.9
C2—C3—C4112.9 (4)C20—C19—H19Ab118.5
C4—C3—H3123.6C21—C20—C19122.8 (4)
C3—C4—H4123.4C24—C20—C19121.2 (4)
C5—C4—C3113.1 (4)C24—C20—C21116.0 (4)
C5—C4—H4123.4C20—C21—H21119.9
C4—C5—S1111.2 (3)C22—C21—C20120.1 (4)
C4—C5—C6127.3 (4)C22—C21—H21119.9
C6—C5—S1121.4 (3)N3—C22—C21124.3 (4)
O3—C6—Ni1iii60.67 (19)N3—C22—H22117.8
O3—C6—O4120.7 (3)C21—C22—H22117.8
O3—C6—C5120.6 (3)N3—C23—H23118.5
O4—C6—Ni1iii60.12 (19)N3—C23—C24123.1 (4)
O4—C6—C5118.7 (4)C24—C23—H23118.5
C5—C6—Ni1iii176.5 (3)C20—C24—H24119.8
N1—C7—H7118.2C23—C24—C20120.5 (4)
N1—C7—C8123.5 (4)C23—C24—H24119.8
C8—C7—H7118.2O5—C25—H25120.0
C7—C8—H8120.3O5—C25—N4120 (4)
C7—C8—C9119.4 (5)N4—C25—H25120.0
C9—C8—H8120.3C25—N4—C26115 (3)
C8—C9—C12124.6 (5)C25—N4—C27127 (4)
C10—C9—C8116.7 (4)C27—N4—C26118 (4)
C10—C9—C12118.7 (5)N4—C26—H26A109.5
C9—C10—H10119.6N4—C26—H26B109.5
C9—C10—C11120.8 (5)N4—C26—H26C109.5
C11—C10—H10119.6H26A—C26—H26B109.5
N1—C11—C10123.1 (5)H26A—C26—H26C109.5
N1—C11—H11118.4H26B—C26—H26C109.5
C10—C11—H11118.4N4—C27—H27A109.5
C9—C12—H12117.2N4—C27—H27B109.5
C12v—C12—C9125.6 (7)N4—C27—H27C109.5
C12v—C12—H12117.2H27A—C27—H27B109.5
C13a—N2a—Ni1123.1 (8)H27A—C27—H27C109.5
C17a—N2a—Ni1121.1 (7)H27B—C27—H27C109.5
C17a—N2a—C13a115.5 (9)
Ni1—O1—C1—O214.6 (7)C10—C9—C12—C12v175.1 (8)
Ni1—O1—C1—C2167.8 (3)C11—N1—C7—C80.5 (7)
Ni1iii—O3—C6—O43.5 (4)C12—C9—C10—C11179.0 (5)
Ni1iii—O3—C6—C5176.2 (4)N2a—C13a—C14a—C15a9 (3)
Ni1iii—O4—C6—O33.6 (4)C13a—N2a—C17a—C16a9 (2)
Ni1iii—O4—C6—C5176.2 (4)C13a—C14a—C15a—C16a5 (3)
Ni1—N1—C7—C8163.5 (4)C13a—C14a—C15a—C18a176.3 (15)
Ni1—N1—C11—C10163.1 (4)C14a—C15a—C16a—C17a4 (2)
Ni1iv—N3—C22—C21178.4 (4)C14a—C15a—C18a—C19176.7 (16)
Ni1iv—N3—C23—C24179.0 (3)C15a—C16a—C17a—N2a6 (2)
Ni1—N2a—C13a—C14a176.4 (12)C15a—C18a—C19—C20179.3 (13)
Ni1—N2a—C17a—C16a177.7 (11)C16a—C15a—C18a—C196 (3)
Ni1—N12b—C113b—C114b174.4 (16)C17a—N2a—C13a—C14a10 (2)
Ni1—N12b—C117b—C116b176.8 (14)C18a—C15a—C16a—C17a174.6 (14)
S1—C2—C3—C40.7 (7)C18a—C19—C20—C218.4 (13)
S1—C5—C6—O37.8 (6)C18a—C19—C20—C24173.0 (11)
S1—C5—C6—O4172.0 (3)N12b—C113b—C114b—C115b5 (3)
O1—C1—C2—S14.6 (6)C113b—N12b—C117b—C116b13 (3)
O1—C1—C2—C3178.1 (5)C113b—C114b—C115b—C116b1 (3)
O2—C1—C2—S1173.2 (4)C113b—C114b—C115b—C118b180 (2)
O2—C1—C2—C34.1 (8)C114b—C115b—C116b—C117b3 (3)
N1—C7—C8—C90.6 (8)C114b—C115b—C118b—C19160 (2)
N3—C23—C24—C201.2 (7)C115b—C116b—C117b—N12b10 (3)
C1—C2—C3—C4178.2 (5)C115b—C118b—C19—C20177.9 (16)
C2—S1—C5—C41.1 (5)C116b—C115b—C118b—C1921 (3)
C2—S1—C5—C6179.7 (4)C117b—N12b—C113b—C114b10 (3)
C2—C3—C4—C50.1 (8)C118b—C115b—C116b—C117b178.2 (19)
C3—C4—C5—S10.9 (7)C118b—C19—C20—C2131.1 (15)
C3—C4—C5—C6180.0 (5)C118b—C19—C20—C24150.4 (14)
C4—C5—C6—O3173.2 (5)C19—C20—C21—C22178.1 (4)
C4—C5—C6—O47.1 (8)C19—C20—C24—C23177.6 (4)
C5—S1—C2—C1178.7 (4)C20—C21—C22—N30.2 (7)
C5—S1—C2—C31.0 (5)C21—C20—C24—C231.0 (6)
C7—N1—C11—C101.3 (7)C22—N3—C23—C240.8 (6)
C7—C8—C9—C100.9 (8)C23—N3—C22—C210.3 (7)
C7—C8—C9—C12178.2 (5)C24—C20—C21—C220.5 (7)
C8—C9—C10—C110.1 (8)O5—C25—N4—C26179 (3)
C8—C9—C12—C12v5.8 (11)O5—C25—N4—C271 (3)
C9—C10—C11—N11.1 (9)
Symmetry codes: (i) x, y+1, z; (ii) x, y, z1; (iii) x, y1, z; (iv) x, y, z+1; (v) x, y+1, z.
Hydrogen-bond geometry (Å, º) top
Cg1, Cg2 and Cg3 are the centroids of rings (N2A,C13A–C17A), (N3,C20–C24) and (N1,C7–C11), respectively.
D—H···AD—HH···AD···AD—H···A
C8—H8···O2vi0.932.593.314 (7)135
C19—H19A···O4vii0.932.513.430 (6)169
C21—H21···O3viii0.932.413.331 (6)171
C27—H27C···Cg10.962.783.57 (6)140
C10—H10···Cg2viii0.932.883.696 (6)147
C22—H22···Cg3iv0.932.933.534 (5)124
Symmetry codes: (iv) x, y, z+1; (vi) x1, 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.

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