research communications
accessHirshfeld surface and energy framework analysis of bis{3-(benzofuran-6-yl)-5-[6-(1H-pyrazol-1-yl)pyridin-2-yl]-1H-1,2,4-triazol-1-ido}iron(II) methanol disolvate
aDepartment of Chemistry, Taras Shevchenko National University of Kyiv, Volodymyrska Street 64, Kyiv, 01601, Ukraine, bDepartment of Inorganic Polymers, "Petru Poni" Institute of Macromolecular, Chemistry, Romanian Academy of Science, Aleea Grigore Ghica Voda 41-A, Iasi, 700487, Romania, and cInstitute of Organic Chemistry, National Academy of Sciences of Ukraine, 5 Academik Kukhar Street, 02094, Kyiv, Ukraine
*Correspondence e-mail: [email protected]
The title compound, [Fe(C18H11N6O)2]·2CH3OH, crystallizes in the orthorhombic space group Pbcn (No. 60) with half of the complex molecule and a methanol molecule in the In the complex, the two tridentate 3-(benzofuran-6-yl)-5-[6-(1H-pyrazol-1-yl)pyridin-2-yl]-4H-1,2,4-triazol ligands meridionally bind to the central FeII ion through the N atoms of the heterocyclic groups, forming a pseudo-octahedral coordination sphere. In the crystal, C—H(pz)⋯π(ph) and C—H⋯N/C/O interactions consolidate the structure. Energy framework analysis at the B3LYP/6–31 G(d,p) theory level was performed to quantify the interaction energies in the crystal.
CCDC reference: 2492851
1. Chemical context
3d-Metal complexes featuring tridentate bisazolepyridine ligands constitute a versatile class of coordination compounds with applications in biochemistry (Fares et al. 2020
), catalysis (Wei et al., 2015
) and molecular magnetism (Halcrow 2024
). For ligands with asymmetric architectures, where one azole moiety bears a protonated nitrogen heteroatom, deprotonation can balance the charge of the central metal ion, yielding neutral complexes. In this case, the peripheral substituents on the neutral complexes influence intermolecular interactions, which in turn affect the connectivity, binding energy, crystal packing, and the coordination environment of the central ion.
Given the prominence of bisazolepyridines as ligands in the FeII spin-crossover domain, and motivated by our longstanding interest in complexes of 3d-metals with N-heterocyclic ligands (Seredyuk et al., 2007
; Bonhommeau et al., 2012
; Piñeiro-López et al., 2018
), herein we report a new neutral low-spin complex based on the asymmetric ligand 3-(benzofuran-6-yl)-5-[6-(1H-pyrazol-1-yl)pyridin-2-yl]-4H-1,2,4-triazol. This study details the synthesis and crystal structure of the title compound, incorporating benzofuran groups to tune intermolecular interactions.
2. Structural commentary
The title compound, [Fe(C18H11N6O)2]·2CH3OH, crystallizes in the orthorhombic space group Pbcn (No. 60) with half of the complex molecule and a methanol molecule in the In the complex, the two ligands meridionally bind to the central FeII ion, which lies on a twofold rotation axis through the N atoms of the heterocyclic groups, forming a pseudo-octahedral coordination sphere. The benzofuran group of the ligand is rotated by 16.2 (2)° relative to the almost planar pyrazole-pyridine-triazole (pz-py-trz) fragment (r.m.s. deviation = 0.055 Å). The methanol molecule forms hydrogen bonds with the trz rings (Fig. 1
). The central Fe ion has a distorted octahedral N6 coordination environment formed by the nitrogen donor atoms of the tridentate ligands. The average bond length iron–nitrogen (<Fe—N>) of 1.957 (2) Å and the volume of the [FeN6] coordination polyhedron of 9.64 Å3 are small and afor the low-spin state of the central ion (Gütlich & Goodwin, 2004
). The average trigonal distortion parameters Σ = Σ112(|90 − ϕi|), where ϕi is the angle N—Fe—N′, and Θ = Σ124(|60 − θi|), where θi is the angle generated by superposition of two opposite faces of an octahedron, are 90.9 and 315.2°, respectively. The calculated continuous shape measure [CShM(Oh)] value relative to the ideal octahedral symmetry is 2.300 (Kershaw Cook et al., 2015
). The values indicate a pseudo-octahedral coordination environment [for an ideal octahedron Σ = Θ = CShM(Oh) = 0].
| Figure 1 The molecular structure in the asymmetric unit of the title compound and contact atoms with displacement ellipsoids drawn at the 40% probability level. The second ligand is shown in wireframe style for clarity. The strong O—H⋯N (red) and weak C—H⋯N/C/O/π (green) hydrogen bonds are shown with the nearest neighbours. Symmetry codes: (i) 1 − x, 1 + y, |
3. Supramolecular features
In the crystal, the molecules interlock by inserting the narrower end of one into the wider end of another, and interact through weak C—H(pz)⋯π(ph) intermolecular contacts between the pyrazole and phenyl groups [the H2/C2⋯Cg(ph) distance is 2.550 (2)/3.489 (2) Å]. The formed supramolecular chains extend along the b-axis direction with a stacking periodicity of 10.5670 (1) Å (Fig. 2
). Weak intermolecular C—H(pz, py)⋯N/C(pz, trz) interactions, ranging from 3.189 (2) to 3.695 (2) Å (Table 1
), connect neighbouring chains into layers propagating in the ab plane. The voids between the layers are occupied by methanol molecules, which also participate in the bonding within separate layers. The methanol molecules form a strong O—H⋯N5 hydrogen bond with the deprotonated trz groups and weak C—H⋯O hydrogen bonds with the pz and py groups of the ligand. A complete list of selected intermolecular interactions is provided in Table 1
.
|
| Figure 2 (a) A fragment of supramolecular column formed by stacking of molecules along the b axis; (b) Supramolecular layers formed by stacking of the supramolecular columns in the ab plane (for a better representation, each column has a different colour). Hydrogen atoms, except those in pz-groups participating in C–H⋯Cg(π) interactions, are omitted for clarity; (c) Stacking of the layers along the b axis direction with the methanol molecules in the voids. Hydrogen atoms are omitted for clarity. |
Hirshfeld surface analysis was conducted for the complex to gain a deeper understanding of the interactions. These interactions are visualized as red (dnorm< vdW radii), white (dnorm= vdW radii), and blue (dnorm> vdW radii) spots on the dnorm surface for the compound along with fingerprint plots mapped with dnorm (where dnorm= di+ de) and decomposed to the separate contributions (Fig. 3
a–c). At 39.9%, the largest contribution to the overall crystal packing is from H⋯H interactions, which are located in the middle region of the fingerprint plot. H⋯C contacts contribute 29.8%, and H⋯O 7.7%, resulting in pairs of characteristic wings. The H⋯N contacts, represented by a pair of sharp spikes in the fingerprint plot, make a 13.2% contribution to the surface.
| Figure 3 (a) A projection of dnorm mapped on the Hirshfeld surface identifying contact points or areas for intermolecular interactions on the molecule; (b) decomposition of the projection dnorm into the specific intermolecular interactions; (c) decomposition of the two-dimensional fingerprint plot into specific interactions. |
The energy framework (Spackman et al., 2021
), was calculated based on the wave function at the B3LYP/6-31G(d,p) theory level. This framework includes components such as electrostatic (Eele), polarization (Epol), repulsion (Erep), and dispersion (Edis) interactions. The latter dominate the contributions, underscoring their primary role for neutral molecules in the crystal structure. The total energy diagram (Etot) overlaid with a fragment of the crystal structure is built using cylindrical bonds between centroids of molecules, where the radii are proportional to the relative interaction strengths (Fig. 4
a–c). The overall topology of the energy framework mirrors the interaction patterns both within and between layers, as outlined earlier. Quantitatively, the Etot for intrachain interactions is −50.1 kJ mol−1, while interchain interactions reach values as low as −81.8 kJ mol−1. Interlayer interactions, in contrast, have an energy as low as −12.2 kJ mol−1. The figure also shows colour-coding of the interactions around a central reference molecule, along with a table of the individual contributions to Etot.
| Figure 4 (a) The calculated energy frameworks, showing the total energy diagrams (Etot); (b) decomposition of the energy framework into the part corresponding to the intralayer interactions and (c) interlayer interactions. In the table, the corresponding colour-coded energy values Etot are provided, including their Eele, Epol, Edis, and Erep components. Tube size is set at 100 scale. |
4. Database survey
A search of the Cambridge Structural Database (CSD, Version 5.42, last update April 2025; Groom et al., 2016
) reveals several low-spin neutral FeII complexes based on asymmetric bisazolpyridines. The selected representative compound for different pairs of azol-azol substituents are ABUFOV (Rajnák et al., 2017
), BEJQOA (Seredyuk et al., 2022
), BOWRIR (Senthil Kumar et al., 2020
) and XODCEB (Shiga et al., 2019
). Table 2
collates some key structural parameters of the complexes. Compared to the title compound, the surveyed complexes generally do not bear voluminous substituents and exhibit lower coordination sphere distortion parameters, suggesting that the bulky benzofuran group, rigidly linked to the donor groups in the present ligand, likely induces greater deviation from an ideal octahedral geometry. This observation underscores the significant influence of peripheral substituents on the structural properties of such complexes.
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5. Synthesis and crystallization
The synthesis of the title compound followed the protocol reported for a similar complex (Seredyuk et al., 2022
). It was produced by a layering technique in a standard test tube. The layering sequence was as follows: the bottom layer contained a solution of [Fe(L2)](BF4)2 prepared by dissolving L = 3-(benzofuran-6-yl)-5-[6-(1H-pyrazol-1-yl)pyridin-2-yl]-4H-1,2,4-triazol (100 mg, 0.304 mmol) and Fe(BF4)2·6H2O (51 mg, 0.152 mmol) in boiling acetone, to which chloroform (5 ml) was then added. The middle layer was a methanol–chloroform mixture (1:10; 10 ml), which was covered by a layer of methanol (10 ml), to which 100 µl of NEt3 was added dropwise. The tube was sealed, and dark-red plate-like single crystals appeared after 3–4 weeks (yield ca. 80%). Elemental analysis calculated for C38H30FeN12O4: C, 58.92; H, 3.90; N, 21.70. Found: C, 59.14; H, 3.97; N, 22.05.
6. Refinement
Crystal data, data collection and structure details are summarized in Table 3
. The hydrogen atom H2A was refined freely, other H atoms were refined as riding [C—H = 0.95–0.98 Å with Uiso(H) = 1.2–1.5Ueq(C)].
|
Supporting information
CCDC reference: 2492851
contains datablock I. DOI: https://doi.org/10.1107/S2056989025008655/zn2044sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989025008655/zn2044Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989025008655/zn2044Isup3.cdx
| [Fe(C18H11N6O)2]·2CH4O | Dx = 1.453 Mg m−3 |
| Mr = 774.59 | Cu Kα radiation, λ = 1.54184 Å |
| Orthorhombic, Pbcn | Cell parameters from 1992 reflections |
| a = 12.64747 (16) Å | θ = 2.6–21.9° |
| b = 10.56703 (12) Å | µ = 3.92 mm−1 |
| c = 26.4991 (4) Å | T = 100 K |
| V = 3541.51 (8) Å3 | Plate, clear dark red |
| Z = 4 | 0.2 × 0.1 × 0.02 mm |
| F(000) = 1600 |
| Rigaku R-AXIS Spider diffractometer | 3464 independent reflections |
| Radiation source: sealed X-ray tube | 3112 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.035 |
| ω scans | θmax = 77.0°, θmin = 3.3° |
| Absorption correction: multi-scan (CrysAlisPro; Rigaku OD, 2024) | h = −14→15 |
| Tmin = 0.534, Tmax = 1.000 | k = −10→12 |
| 14149 measured reflections | l = −32→31 |
| Refinement on F2 | Primary atom site location: iterative |
| Least-squares matrix: full | Hydrogen site location: mixed |
| R[F2 > 2σ(F2)] = 0.037 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.097 | w = 1/[σ2(Fo2) + (0.0512P)2 + 1.8481P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.001 |
| 3464 reflections | Δρmax = 0.38 e Å−3 |
| 267 parameters | Δρmin = −0.30 e Å−3 |
| 0 restraints |
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 | ||
| Fe1 | 0.500000 | 0.71753 (3) | 0.250000 | 0.01699 (12) | |
| N2 | 0.60321 (11) | 0.88309 (13) | 0.18316 (5) | 0.0211 (3) | |
| N5 | 0.51474 (11) | 0.50739 (14) | 0.33332 (6) | 0.0212 (3) | |
| N1 | 0.50229 (10) | 0.84881 (14) | 0.19681 (6) | 0.0201 (3) | |
| N6 | 0.69158 (11) | 0.47812 (14) | 0.32708 (6) | 0.0248 (3) | |
| O2 | 0.33165 (11) | 0.58628 (13) | 0.37969 (6) | 0.0337 (3) | |
| H2A | 0.388 (2) | 0.560 (3) | 0.3652 (11) | 0.051* | |
| C10 | 0.60031 (14) | 0.44450 (16) | 0.34999 (7) | 0.0234 (4) | |
| N4 | 0.55298 (11) | 0.58772 (13) | 0.29740 (5) | 0.0200 (3) | |
| O1 | 0.76510 (15) | 0.11184 (16) | 0.45227 (8) | 0.0592 (5) | |
| N3 | 0.64849 (12) | 0.72535 (13) | 0.23605 (6) | 0.0192 (3) | |
| C3 | 0.60208 (15) | 0.97836 (16) | 0.14857 (7) | 0.0252 (4) | |
| H3 | 0.661738 | 1.018159 | 0.133646 | 0.028 (5)* | |
| C1 | 0.43939 (14) | 0.92266 (16) | 0.16998 (7) | 0.0231 (4) | |
| H1 | 0.364343 | 0.920088 | 0.171141 | 0.018 (5)* | |
| C9 | 0.65775 (14) | 0.56733 (16) | 0.29510 (7) | 0.0219 (4) | |
| C14 | 0.59610 (19) | 0.17309 (18) | 0.46954 (7) | 0.0370 (5) | |
| C15 | 0.50599 (18) | 0.2460 (2) | 0.46065 (8) | 0.0368 (5) | |
| H15 | 0.444813 | 0.236306 | 0.481086 | 0.034 (6)* | |
| C11 | 0.59762 (15) | 0.34926 (16) | 0.39076 (7) | 0.0255 (4) | |
| C4 | 0.68561 (14) | 0.81295 (16) | 0.20461 (6) | 0.0209 (3) | |
| C8 | 0.71692 (14) | 0.64890 (16) | 0.26088 (7) | 0.0216 (4) | |
| C2 | 0.49829 (14) | 1.00533 (19) | 0.13958 (7) | 0.0264 (4) | |
| H2 | 0.471293 | 1.067668 | 0.117193 | 0.035 (6)* | |
| C13 | 0.68376 (18) | 0.19108 (19) | 0.43879 (8) | 0.0375 (5) | |
| C5 | 0.79190 (14) | 0.83074 (17) | 0.19502 (7) | 0.0249 (4) | |
| H5 | 0.816012 | 0.894204 | 0.172386 | 0.035 (6)* | |
| C6 | 0.86160 (14) | 0.75147 (18) | 0.22005 (8) | 0.0279 (4) | |
| H6 | 0.935455 | 0.759817 | 0.214414 | 0.028 (5)* | |
| C12 | 0.68793 (17) | 0.27699 (18) | 0.39928 (9) | 0.0349 (5) | |
| H12 | 0.749420 | 0.286094 | 0.379018 | 0.035 (6)* | |
| C19 | 0.3624 (2) | 0.6729 (2) | 0.41714 (9) | 0.0448 (6) | |
| H19A | 0.408898 | 0.737042 | 0.402292 | 0.068 (9)* | |
| H19B | 0.400247 | 0.628001 | 0.443998 | 0.064 (9)* | |
| H19C | 0.299544 | 0.713942 | 0.431245 | 0.071 (10)* | |
| C7 | 0.82468 (16) | 0.65977 (19) | 0.25333 (7) | 0.0273 (4) | |
| H7 | 0.872601 | 0.605658 | 0.270552 | 0.029 (5)* | |
| C16 | 0.50739 (16) | 0.33329 (19) | 0.42130 (8) | 0.0303 (4) | |
| H16 | 0.446288 | 0.383066 | 0.414909 | 0.031 (6)* | |
| C18 | 0.6261 (3) | 0.0745 (2) | 0.50447 (9) | 0.0503 (7) | |
| H18 | 0.583948 | 0.039318 | 0.530606 | 0.066 (9)* | |
| C17 | 0.7255 (3) | 0.0429 (2) | 0.49248 (11) | 0.0611 (8) | |
| H17 | 0.764801 | −0.020237 | 0.509770 | 0.073 (10)* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Fe1 | 0.0157 (2) | 0.0172 (2) | 0.0181 (2) | 0.000 | −0.00027 (13) | 0.000 |
| N2 | 0.0203 (7) | 0.0218 (7) | 0.0213 (7) | 0.0000 (6) | 0.0010 (6) | 0.0024 (6) |
| N5 | 0.0224 (7) | 0.0200 (7) | 0.0212 (7) | −0.0031 (6) | 0.0002 (6) | 0.0033 (6) |
| N1 | 0.0184 (7) | 0.0204 (7) | 0.0214 (7) | 0.0004 (5) | 0.0001 (5) | −0.0016 (6) |
| N6 | 0.0224 (7) | 0.0235 (7) | 0.0286 (8) | 0.0000 (6) | −0.0013 (6) | 0.0059 (6) |
| O2 | 0.0288 (7) | 0.0369 (7) | 0.0354 (8) | −0.0025 (6) | 0.0023 (6) | −0.0099 (6) |
| C10 | 0.0232 (9) | 0.0212 (8) | 0.0258 (9) | −0.0024 (7) | −0.0018 (7) | 0.0017 (7) |
| N4 | 0.0183 (7) | 0.0194 (7) | 0.0222 (7) | −0.0020 (5) | −0.0005 (5) | 0.0014 (6) |
| O1 | 0.0574 (11) | 0.0473 (9) | 0.0729 (12) | 0.0010 (8) | −0.0213 (9) | 0.0316 (9) |
| N3 | 0.0193 (7) | 0.0188 (7) | 0.0195 (7) | −0.0009 (6) | −0.0001 (6) | 0.0003 (5) |
| C3 | 0.0303 (9) | 0.0224 (8) | 0.0229 (9) | 0.0005 (7) | 0.0014 (7) | 0.0047 (7) |
| C1 | 0.0230 (9) | 0.0233 (8) | 0.0230 (8) | 0.0041 (7) | −0.0019 (7) | −0.0016 (7) |
| C9 | 0.0211 (8) | 0.0211 (8) | 0.0234 (8) | 0.0002 (7) | −0.0014 (7) | 0.0028 (7) |
| C14 | 0.0639 (15) | 0.0252 (9) | 0.0218 (9) | −0.0096 (10) | −0.0079 (9) | 0.0020 (7) |
| C15 | 0.0570 (15) | 0.0290 (10) | 0.0243 (10) | −0.0052 (9) | 0.0058 (9) | 0.0013 (8) |
| C11 | 0.0314 (10) | 0.0217 (8) | 0.0234 (9) | −0.0050 (7) | −0.0053 (7) | 0.0025 (7) |
| C4 | 0.0227 (9) | 0.0207 (8) | 0.0193 (8) | 0.0009 (7) | −0.0007 (7) | 0.0009 (6) |
| C8 | 0.0210 (8) | 0.0209 (8) | 0.0230 (8) | 0.0014 (7) | −0.0014 (7) | 0.0011 (7) |
| C2 | 0.0309 (10) | 0.0257 (9) | 0.0228 (9) | 0.0052 (7) | −0.0017 (7) | 0.0028 (7) |
| C13 | 0.0442 (12) | 0.0278 (9) | 0.0405 (12) | −0.0042 (9) | −0.0168 (10) | 0.0085 (9) |
| C5 | 0.0234 (9) | 0.0254 (9) | 0.0261 (9) | −0.0028 (7) | 0.0020 (7) | 0.0049 (7) |
| C6 | 0.0177 (9) | 0.0313 (9) | 0.0347 (10) | −0.0005 (8) | 0.0014 (7) | 0.0048 (8) |
| C12 | 0.0333 (11) | 0.0309 (10) | 0.0405 (12) | −0.0056 (8) | −0.0070 (9) | 0.0119 (9) |
| C19 | 0.0680 (16) | 0.0340 (11) | 0.0325 (11) | −0.0132 (11) | 0.0105 (11) | −0.0067 (9) |
| C7 | 0.0219 (9) | 0.0280 (9) | 0.0320 (10) | 0.0019 (8) | −0.0016 (7) | 0.0064 (8) |
| C16 | 0.0409 (11) | 0.0245 (9) | 0.0254 (10) | −0.0021 (8) | 0.0026 (8) | 0.0021 (8) |
| C18 | 0.088 (2) | 0.0333 (12) | 0.0300 (11) | −0.0088 (13) | −0.0149 (12) | 0.0091 (9) |
| C17 | 0.084 (2) | 0.0421 (13) | 0.0570 (16) | −0.0069 (14) | −0.0303 (15) | 0.0262 (12) |
| Fe1—N1i | 1.9778 (15) | C9—C8 | 1.458 (2) |
| Fe1—N1 | 1.9778 (15) | C14—C15 | 1.396 (3) |
| Fe1—N4 | 1.9770 (14) | C14—C13 | 1.389 (3) |
| Fe1—N4i | 1.9770 (14) | C14—C18 | 1.444 (3) |
| Fe1—N3i | 1.9158 (15) | C15—H15 | 0.9500 |
| Fe1—N3 | 1.9158 (15) | C15—C16 | 1.392 (3) |
| N2—N1 | 1.375 (2) | C11—C12 | 1.392 (3) |
| N2—C3 | 1.362 (2) | C11—C16 | 1.409 (3) |
| N2—C4 | 1.399 (2) | C4—C5 | 1.381 (2) |
| N5—C10 | 1.345 (2) | C8—C7 | 1.382 (3) |
| N5—N4 | 1.364 (2) | C2—H2 | 0.9500 |
| N1—C1 | 1.322 (2) | C13—C12 | 1.387 (3) |
| N6—C10 | 1.352 (2) | C5—H5 | 0.9500 |
| N6—C9 | 1.338 (2) | C5—C6 | 1.385 (3) |
| O2—H2A | 0.85 (3) | C6—H6 | 0.9500 |
| O2—C19 | 1.405 (3) | C6—C7 | 1.391 (3) |
| C10—C11 | 1.477 (2) | C12—H12 | 0.9500 |
| N4—C9 | 1.344 (2) | C19—H19A | 0.9800 |
| O1—C13 | 1.374 (3) | C19—H19B | 0.9800 |
| O1—C17 | 1.384 (3) | C19—H19C | 0.9800 |
| N3—C4 | 1.331 (2) | C7—H7 | 0.9500 |
| N3—C8 | 1.354 (2) | C16—H16 | 0.9500 |
| C3—H3 | 0.9500 | C18—H18 | 0.9500 |
| C3—C2 | 1.364 (3) | C18—C17 | 1.339 (4) |
| C1—H1 | 0.9500 | C17—H17 | 0.9500 |
| C1—C2 | 1.403 (3) | ||
| N1i—Fe1—N1 | 90.92 (9) | C14—C15—H15 | 120.6 |
| N4i—Fe1—N1 | 92.23 (6) | C16—C15—C14 | 118.8 (2) |
| N4—Fe1—N1i | 92.23 (6) | C16—C15—H15 | 120.6 |
| N4—Fe1—N1 | 159.14 (6) | C12—C11—C10 | 118.26 (17) |
| N4i—Fe1—N1i | 159.14 (5) | C12—C11—C16 | 120.36 (18) |
| N4—Fe1—N4i | 92.13 (8) | C16—C11—C10 | 121.36 (17) |
| N3i—Fe1—N1i | 79.51 (6) | N3—C4—N2 | 111.09 (15) |
| N3—Fe1—N1 | 79.51 (6) | N3—C4—C5 | 123.59 (16) |
| N3—Fe1—N1i | 96.99 (6) | C5—C4—N2 | 125.31 (16) |
| N3i—Fe1—N1 | 96.98 (6) | N3—C8—C9 | 109.07 (15) |
| N3i—Fe1—N4i | 79.64 (6) | N3—C8—C7 | 120.68 (16) |
| N3i—Fe1—N4 | 103.86 (6) | C7—C8—C9 | 130.18 (17) |
| N3—Fe1—N4 | 79.64 (6) | C3—C2—C1 | 106.30 (16) |
| N3—Fe1—N4i | 103.86 (6) | C3—C2—H2 | 126.8 |
| N3—Fe1—N3i | 175.06 (8) | C1—C2—H2 | 126.8 |
| N1—N2—C4 | 116.41 (14) | O1—C13—C14 | 111.21 (19) |
| C3—N2—N1 | 111.23 (14) | O1—C13—C12 | 124.5 (2) |
| C3—N2—C4 | 132.29 (15) | C12—C13—C14 | 124.3 (2) |
| C10—N5—N4 | 104.56 (13) | C4—C5—H5 | 121.7 |
| N2—N1—Fe1 | 112.69 (10) | C4—C5—C6 | 116.69 (16) |
| C1—N1—Fe1 | 142.05 (12) | C6—C5—H5 | 121.7 |
| C1—N1—N2 | 105.17 (14) | C5—C6—H6 | 119.6 |
| C9—N6—C10 | 101.33 (14) | C5—C6—C7 | 120.74 (17) |
| C19—O2—H2A | 107.2 (19) | C7—C6—H6 | 119.6 |
| N5—C10—N6 | 114.20 (15) | C11—C12—H12 | 121.6 |
| N5—C10—C11 | 123.95 (16) | C13—C12—C11 | 116.8 (2) |
| N6—C10—C11 | 121.82 (16) | C13—C12—H12 | 121.6 |
| N5—N4—Fe1 | 139.02 (11) | O2—C19—H19A | 109.5 |
| C9—N4—Fe1 | 114.63 (11) | O2—C19—H19B | 109.5 |
| C9—N4—N5 | 106.35 (13) | O2—C19—H19C | 109.5 |
| C13—O1—C17 | 104.5 (2) | H19A—C19—H19B | 109.5 |
| C4—N3—Fe1 | 119.77 (12) | H19A—C19—H19C | 109.5 |
| C4—N3—C8 | 119.57 (15) | H19B—C19—H19C | 109.5 |
| C8—N3—Fe1 | 120.46 (12) | C8—C7—C6 | 118.72 (17) |
| N2—C3—H3 | 126.8 | C8—C7—H7 | 120.6 |
| N2—C3—C2 | 106.38 (16) | C6—C7—H7 | 120.6 |
| C2—C3—H3 | 126.8 | C15—C16—C11 | 121.32 (19) |
| N1—C1—H1 | 124.5 | C15—C16—H16 | 119.3 |
| N1—C1—C2 | 110.91 (16) | C11—C16—H16 | 119.3 |
| C2—C1—H1 | 124.5 | C14—C18—H18 | 127.0 |
| N6—C9—N4 | 113.56 (15) | C17—C18—C14 | 105.9 (2) |
| N6—C9—C8 | 130.27 (16) | C17—C18—H18 | 127.0 |
| N4—C9—C8 | 116.07 (15) | O1—C17—H17 | 123.5 |
| C15—C14—C18 | 136.1 (2) | C18—C17—O1 | 113.0 (2) |
| C13—C14—C15 | 118.49 (18) | C18—C17—H17 | 123.5 |
| C13—C14—C18 | 105.4 (2) | ||
| Fe1—N1—C1—C2 | 175.25 (15) | N3—C8—C7—C6 | 0.5 (3) |
| Fe1—N4—C9—N6 | −179.26 (12) | C3—N2—N1—Fe1 | −176.63 (11) |
| Fe1—N4—C9—C8 | 3.9 (2) | C3—N2—N1—C1 | 0.66 (19) |
| Fe1—N3—C4—N2 | −4.37 (19) | C3—N2—C4—N3 | −177.97 (17) |
| Fe1—N3—C4—C5 | 175.56 (14) | C3—N2—C4—C5 | 2.1 (3) |
| Fe1—N3—C8—C9 | 1.54 (19) | C9—N6—C10—N5 | 0.5 (2) |
| Fe1—N3—C8—C7 | −175.82 (14) | C9—N6—C10—C11 | −177.82 (16) |
| N2—N1—C1—C2 | −0.70 (19) | C9—C8—C7—C6 | −176.21 (18) |
| N2—C3—C2—C1 | −0.1 (2) | C14—C15—C16—C11 | −0.3 (3) |
| N2—C4—C5—C6 | 179.99 (17) | C14—C13—C12—C11 | 0.3 (3) |
| N5—C10—C11—C12 | 170.28 (18) | C14—C18—C17—O1 | −0.1 (3) |
| N5—C10—C11—C16 | −11.3 (3) | C15—C14—C13—O1 | −179.64 (19) |
| N5—N4—C9—N6 | 0.3 (2) | C15—C14—C13—C12 | −0.3 (3) |
| N5—N4—C9—C8 | −176.53 (14) | C15—C14—C18—C17 | 179.4 (3) |
| N1—N2—C3—C2 | −0.4 (2) | C4—N2—N1—Fe1 | 6.09 (18) |
| N1—N2—C4—N3 | −1.4 (2) | C4—N2—N1—C1 | −176.61 (14) |
| N1—N2—C4—C5 | 178.66 (17) | C4—N2—C3—C2 | 176.33 (18) |
| N1—C1—C2—C3 | 0.5 (2) | C4—N3—C8—C9 | 176.42 (15) |
| N6—C10—C11—C12 | −11.6 (3) | C4—N3—C8—C7 | −0.9 (3) |
| N6—C10—C11—C16 | 166.86 (18) | C4—C5—C6—C7 | −0.5 (3) |
| N6—C9—C8—N3 | −179.67 (17) | C8—N3—C4—N2 | −179.28 (14) |
| N6—C9—C8—C7 | −2.6 (3) | C8—N3—C4—C5 | 0.6 (3) |
| C10—N5—N4—Fe1 | 179.40 (14) | C13—O1—C17—C18 | −0.1 (3) |
| C10—N5—N4—C9 | 0.06 (18) | C13—C14—C15—C16 | 0.3 (3) |
| C10—N6—C9—N4 | −0.5 (2) | C13—C14—C18—C17 | 0.2 (3) |
| C10—N6—C9—C8 | 175.77 (18) | C5—C6—C7—C8 | 0.2 (3) |
| C10—C11—C12—C13 | 178.16 (17) | C12—C11—C16—C15 | 0.3 (3) |
| C10—C11—C16—C15 | −178.12 (18) | C16—C11—C12—C13 | −0.3 (3) |
| N4—N5—C10—N6 | −0.4 (2) | C18—C14—C15—C16 | −178.8 (2) |
| N4—N5—C10—C11 | 177.92 (16) | C18—C14—C13—O1 | −0.3 (2) |
| N4—C9—C8—N3 | −3.5 (2) | C18—C14—C13—C12 | 179.1 (2) |
| N4—C9—C8—C7 | 173.51 (19) | C17—O1—C13—C14 | 0.2 (3) |
| O1—C13—C12—C11 | 179.6 (2) | C17—O1—C13—C12 | −179.1 (2) |
| N3—C4—C5—C6 | 0.1 (3) |
| Symmetry code: (i) −x+1, y, −z+1/2. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O2—H2A···N5 | 0.85 (3) | 1.89 (2) | 2.750 (2) | 178 (3) |
| C1—H1···N6ii | 0.95 | 2.27 | 3.189 (2) | 163 |
| C3—H3···O2iii | 0.95 | 2.29 | 3.208 (2) | 161 |
| C5—H5···O2iii | 0.95 | 2.46 | 3.386 (2) | 164 |
| C5—H5···N5iii | 0.95 | 1.90 | 3.463 (2) | 129 |
| C7—H7···C1iv | 0.95 | 2.63 | 3.537 (2) | 159 |
| C19—H19A···N2i | 0.97 | 2.74 | 3.491 (2) | 133 |
| C19—H19A···C3i | 0.97 | 2.89 | 3.695 (2) | 140 |
| C6···C3v | – | – | 3.482 (2) | – |
| C7···C3v | – | – | 3.498 (2) | – |
| Symmetry codes: (i) −x+1, y, −z+1/2; (ii) x−1/2, y+1/2, −z+1/2; (iii) x+1/2, y+1/2, −z+1/2; (iv) x+1/2, y−1/2, −z+1/2; (v) −x+3/2, y−1/2, z. |
| CSD Refcode | azol 1/azol 2 | <Fe—N> | Σ | Θ | CShM(Oh) |
| Title compound | 1,2,4-triazole/pyrazole | 1.957 | 90.9 | 315.2 | 2.300 |
| BEJQOA | 1,2,4-triazole/pyrazole | 1.946 | 87.5 | 308.9 | 2.163 |
| ABUFOV | benzimidazole/benzimidazole | 1.937 | 80.1 | 262.7 | 1.753 |
| BOWRIR | tetrazole/pyrazole | 1.934 | 89.7 | 287.4 | 2.043 |
| XODCEB | benzimidazole/pyrazole | 1.950 | 87.5 | 276.6 | 1.925 |
Acknowledgements
The authors are grateful to the FAIRE programme provided by the Cambridge Crystallographic Data Centre (CCDC) for the opportunity to use the Cambridge Structural Database (CSD) and associated software. Author contributions are as follows: conceptualization, MS; methodology, KZ; formal analysis, IOF; synthesis, IT; single-crystal measurements, SS; writing (original draft), IT and MS; writing (review and editing), KZ and VMA; visualization and calculations, OVO; funding acquisition, MS and KZ.
Funding information
Funding for this research was provided by: Ministry of Education and Science of Ukraine (grant for the perspective development of the scientific direction "Mathematical sciences and natural sciences" at the Taras Shevchenko National University of Kyiv).
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