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COMMUNICATIONS
ISSN: 2056-9890

Crystal structure, Hirshfeld 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

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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]

Edited by A. Briceno, Venezuelan Institute of Scientific Research, Venezuela (Received 20 August 2025; accepted 2 October 2025; online 7 October 2025)

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 asymmetric unit. 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.

1. Chemical context

3d-Metal complexes featuring tridentate bis­azole­pyridine ligands constitute a versatile class of coordination compounds with applications in biochemistry (Fares et al. 2020View full citation), catalysis (Wei et al., 2015View full citation) and mol­ecular magnetism (Halcrow 2024View full citation). 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.

[Scheme 1]

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., 2007View full citation; Bonhommeau et al., 2012View full citation; Piñeiro-López et al., 2018View full citation), 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 asymmetric unit. 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[link]). 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, 2004View full citation). 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., 2015View full citation). The values indicate a pseudo-octa­hedral coordination environment [for an ideal octa­hedron Σ = Θ = CShM(Oh) = 0].

[Figure 1]
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, Mathematical equation − z; (ii) Mathematical equation + x, Mathematical equation + y, Mathematical equation − z; (iii) 1 − x, y, Mathematical equation − z; (iv) Mathematical equation − x, −Mathematical equation + y, z; (v) Mathematical equation + x, −Mathematical equation + y, Mathematical equation − z; (vi) Mathematical equation + x, Mathematical equation − y, 1 − z; (vii) 1 − x, 1 − y, 1 − z; (viii) 1 − x, y, Mathematical equation − z.

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[link]). Weak inter­molecular C—H(pz, py)⋯N/C(pz, trz) inter­actions, ranging from 3.189 (2) to 3.695 (2) Å (Table 1[link]), 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[link].

Table 1
Hydrogen-bond and short contact geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O2—H2A⋯N5 0.85 (3) 1.89 (2) 2.750 (2) 178 (3)
C1—H1⋯N6i 0.95 2.27 3.189 (2) 163
C3—H3⋯O2ii 0.95 2.29 3.208 (2) 161
C5—H5⋯O2ii 0.95 2.46 3.386 (2) 164
C5—H5⋯N5ii 0.95 1.90 3.463 (2) 129
C7—H7⋯C1iii 0.95 2.63 3.537 (2) 159
C19—H19A⋯N2iv 0.97 2.74 3.491 (2) 133
C19—H19A⋯C3iv 0.97 2.89 3.695 (2) 140
C6⋯C3v 3.482 (2)
C7⋯C3v 3.498 (2)
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation; (v) Mathematical equation.
[Figure 2]
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[link]ac). 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]
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., 2021View full citation), 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[link]ac). 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]
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., 2016View full citation) 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., 2017View full citation), BEJQOA (Seredyuk et al., 2022View full citation), BOWRIR (Senthil Kumar et al., 2020View full citation) and XODCEB (Shiga et al., 2019View full citation). Table 2[link] 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.

Table 2
Computed distortion indices (Å, °) for the title compound and for similar complexes reported in the literature.

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

5. Synthesis and crystallization

The synthesis of the title compound followed the protocol reported for a similar complex (Seredyuk et al., 2022View full citation). 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 refinement details are summarized in Table 3[link]. 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)].

Table 3
Experimental details

Crystal data
Chemical formula [Fe(C18H11N6O)2]·2CH4O
Mr 774.59
Crystal system, space group Orthorhombic, Pbcn
Temperature (K) 100
a, b, c (Å) 12.64747 (16), 10.56703 (12), 26.4991 (4)
V3) 3541.51 (8)
Z 4
Radiation type Cu Kα
μ (mm−1) 3.92
Crystal size (mm) 0.2 × 0.10 × 0.02
 
Data collection
Diffractometer Rigaku R-AXIS Spider
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2024View full citation)
Tmin, Tmax 0.534, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 14149, 3464, 3112
Rint 0.035
(sin θ/λ)max−1) 0.632
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.037, 0.097, 1.05
No. of reflections 3464
No. of parameters 267
H-atom treatment H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.38, −0.30
Computer programs: CrysAlis PRO (Rigaku OD, 2024View full citation), OLEX2.solve 1.5 (Bourhis et al., 2015View full citation), SHELXL2018/3 (Sheldrick, 2015View full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

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 top
Crystal data top
[Fe(C18H11N6O)2]·2CH4ODx = 1.453 Mg m3
Mr = 774.59Cu Kα radiation, λ = 1.54184 Å
Orthorhombic, PbcnCell parameters from 1992 reflections
a = 12.64747 (16) Åθ = 2.6–21.9°
b = 10.56703 (12) ŵ = 3.92 mm1
c = 26.4991 (4) ÅT = 100 K
V = 3541.51 (8) Å3Plate, clear dark red
Z = 40.2 × 0.1 × 0.02 mm
F(000) = 1600
Data collection top
Rigaku R-AXIS Spider
diffractometer
3464 independent reflections
Radiation source: sealed X-ray tube3112 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.035
ω scansθmax = 77.0°, θmin = 3.3°
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2024)
h = 1415
Tmin = 0.534, Tmax = 1.000k = 1012
14149 measured reflectionsl = 3231
Refinement top
Refinement on F2Primary atom site location: iterative
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.037H 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 reflectionsΔρmax = 0.38 e Å3
267 parametersΔρmin = 0.30 e Å3
0 restraints
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*/Ueq
Fe10.5000000.71753 (3)0.2500000.01699 (12)
N20.60321 (11)0.88309 (13)0.18316 (5)0.0211 (3)
N50.51474 (11)0.50739 (14)0.33332 (6)0.0212 (3)
N10.50229 (10)0.84881 (14)0.19681 (6)0.0201 (3)
N60.69158 (11)0.47812 (14)0.32708 (6)0.0248 (3)
O20.33165 (11)0.58628 (13)0.37969 (6)0.0337 (3)
H2A0.388 (2)0.560 (3)0.3652 (11)0.051*
C100.60031 (14)0.44450 (16)0.34999 (7)0.0234 (4)
N40.55298 (11)0.58772 (13)0.29740 (5)0.0200 (3)
O10.76510 (15)0.11184 (16)0.45227 (8)0.0592 (5)
N30.64849 (12)0.72535 (13)0.23605 (6)0.0192 (3)
C30.60208 (15)0.97836 (16)0.14857 (7)0.0252 (4)
H30.6617381.0181590.1336460.028 (5)*
C10.43939 (14)0.92266 (16)0.16998 (7)0.0231 (4)
H10.3643430.9200880.1711410.018 (5)*
C90.65775 (14)0.56733 (16)0.29510 (7)0.0219 (4)
C140.59610 (19)0.17309 (18)0.46954 (7)0.0370 (5)
C150.50599 (18)0.2460 (2)0.46065 (8)0.0368 (5)
H150.4448130.2363060.4810860.034 (6)*
C110.59762 (15)0.34926 (16)0.39076 (7)0.0255 (4)
C40.68561 (14)0.81295 (16)0.20461 (6)0.0209 (3)
C80.71692 (14)0.64890 (16)0.26088 (7)0.0216 (4)
C20.49829 (14)1.00533 (19)0.13958 (7)0.0264 (4)
H20.4712931.0676680.1171930.035 (6)*
C130.68376 (18)0.19108 (19)0.43879 (8)0.0375 (5)
C50.79190 (14)0.83074 (17)0.19502 (7)0.0249 (4)
H50.8160120.8942040.1723860.035 (6)*
C60.86160 (14)0.75147 (18)0.22005 (8)0.0279 (4)
H60.9354550.7598170.2144140.028 (5)*
C120.68793 (17)0.27699 (18)0.39928 (9)0.0349 (5)
H120.7494200.2860940.3790180.035 (6)*
C190.3624 (2)0.6729 (2)0.41714 (9)0.0448 (6)
H19A0.4088980.7370420.4022920.068 (9)*
H19B0.4002470.6280010.4439980.064 (9)*
H19C0.2995440.7139420.4312450.071 (10)*
C70.82468 (16)0.65977 (19)0.25333 (7)0.0273 (4)
H70.8726010.6056580.2705520.029 (5)*
C160.50739 (16)0.33329 (19)0.42130 (8)0.0303 (4)
H160.4462880.3830660.4149090.031 (6)*
C180.6261 (3)0.0745 (2)0.50447 (9)0.0503 (7)
H180.5839480.0393180.5306060.066 (9)*
C170.7255 (3)0.0429 (2)0.49248 (11)0.0611 (8)
H170.7648010.0202370.5097700.073 (10)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Fe10.0157 (2)0.0172 (2)0.0181 (2)0.0000.00027 (13)0.000
N20.0203 (7)0.0218 (7)0.0213 (7)0.0000 (6)0.0010 (6)0.0024 (6)
N50.0224 (7)0.0200 (7)0.0212 (7)0.0031 (6)0.0002 (6)0.0033 (6)
N10.0184 (7)0.0204 (7)0.0214 (7)0.0004 (5)0.0001 (5)0.0016 (6)
N60.0224 (7)0.0235 (7)0.0286 (8)0.0000 (6)0.0013 (6)0.0059 (6)
O20.0288 (7)0.0369 (7)0.0354 (8)0.0025 (6)0.0023 (6)0.0099 (6)
C100.0232 (9)0.0212 (8)0.0258 (9)0.0024 (7)0.0018 (7)0.0017 (7)
N40.0183 (7)0.0194 (7)0.0222 (7)0.0020 (5)0.0005 (5)0.0014 (6)
O10.0574 (11)0.0473 (9)0.0729 (12)0.0010 (8)0.0213 (9)0.0316 (9)
N30.0193 (7)0.0188 (7)0.0195 (7)0.0009 (6)0.0001 (6)0.0003 (5)
C30.0303 (9)0.0224 (8)0.0229 (9)0.0005 (7)0.0014 (7)0.0047 (7)
C10.0230 (9)0.0233 (8)0.0230 (8)0.0041 (7)0.0019 (7)0.0016 (7)
C90.0211 (8)0.0211 (8)0.0234 (8)0.0002 (7)0.0014 (7)0.0028 (7)
C140.0639 (15)0.0252 (9)0.0218 (9)0.0096 (10)0.0079 (9)0.0020 (7)
C150.0570 (15)0.0290 (10)0.0243 (10)0.0052 (9)0.0058 (9)0.0013 (8)
C110.0314 (10)0.0217 (8)0.0234 (9)0.0050 (7)0.0053 (7)0.0025 (7)
C40.0227 (9)0.0207 (8)0.0193 (8)0.0009 (7)0.0007 (7)0.0009 (6)
C80.0210 (8)0.0209 (8)0.0230 (8)0.0014 (7)0.0014 (7)0.0011 (7)
C20.0309 (10)0.0257 (9)0.0228 (9)0.0052 (7)0.0017 (7)0.0028 (7)
C130.0442 (12)0.0278 (9)0.0405 (12)0.0042 (9)0.0168 (10)0.0085 (9)
C50.0234 (9)0.0254 (9)0.0261 (9)0.0028 (7)0.0020 (7)0.0049 (7)
C60.0177 (9)0.0313 (9)0.0347 (10)0.0005 (8)0.0014 (7)0.0048 (8)
C120.0333 (11)0.0309 (10)0.0405 (12)0.0056 (8)0.0070 (9)0.0119 (9)
C190.0680 (16)0.0340 (11)0.0325 (11)0.0132 (11)0.0105 (11)0.0067 (9)
C70.0219 (9)0.0280 (9)0.0320 (10)0.0019 (8)0.0016 (7)0.0064 (8)
C160.0409 (11)0.0245 (9)0.0254 (10)0.0021 (8)0.0026 (8)0.0021 (8)
C180.088 (2)0.0333 (12)0.0300 (11)0.0088 (13)0.0149 (12)0.0091 (9)
C170.084 (2)0.0421 (13)0.0570 (16)0.0069 (14)0.0303 (15)0.0262 (12)
Geometric parameters (Å, º) top
Fe1—N1i1.9778 (15)C9—C81.458 (2)
Fe1—N11.9778 (15)C14—C151.396 (3)
Fe1—N41.9770 (14)C14—C131.389 (3)
Fe1—N4i1.9770 (14)C14—C181.444 (3)
Fe1—N3i1.9158 (15)C15—H150.9500
Fe1—N31.9158 (15)C15—C161.392 (3)
N2—N11.375 (2)C11—C121.392 (3)
N2—C31.362 (2)C11—C161.409 (3)
N2—C41.399 (2)C4—C51.381 (2)
N5—C101.345 (2)C8—C71.382 (3)
N5—N41.364 (2)C2—H20.9500
N1—C11.322 (2)C13—C121.387 (3)
N6—C101.352 (2)C5—H50.9500
N6—C91.338 (2)C5—C61.385 (3)
O2—H2A0.85 (3)C6—H60.9500
O2—C191.405 (3)C6—C71.391 (3)
C10—C111.477 (2)C12—H120.9500
N4—C91.344 (2)C19—H19A0.9800
O1—C131.374 (3)C19—H19B0.9800
O1—C171.384 (3)C19—H19C0.9800
N3—C41.331 (2)C7—H70.9500
N3—C81.354 (2)C16—H160.9500
C3—H30.9500C18—H180.9500
C3—C21.364 (3)C18—C171.339 (4)
C1—H10.9500C17—H170.9500
C1—C21.403 (3)
N1i—Fe1—N190.92 (9)C14—C15—H15120.6
N4i—Fe1—N192.23 (6)C16—C15—C14118.8 (2)
N4—Fe1—N1i92.23 (6)C16—C15—H15120.6
N4—Fe1—N1159.14 (6)C12—C11—C10118.26 (17)
N4i—Fe1—N1i159.14 (5)C12—C11—C16120.36 (18)
N4—Fe1—N4i92.13 (8)C16—C11—C10121.36 (17)
N3i—Fe1—N1i79.51 (6)N3—C4—N2111.09 (15)
N3—Fe1—N179.51 (6)N3—C4—C5123.59 (16)
N3—Fe1—N1i96.99 (6)C5—C4—N2125.31 (16)
N3i—Fe1—N196.98 (6)N3—C8—C9109.07 (15)
N3i—Fe1—N4i79.64 (6)N3—C8—C7120.68 (16)
N3i—Fe1—N4103.86 (6)C7—C8—C9130.18 (17)
N3—Fe1—N479.64 (6)C3—C2—C1106.30 (16)
N3—Fe1—N4i103.86 (6)C3—C2—H2126.8
N3—Fe1—N3i175.06 (8)C1—C2—H2126.8
N1—N2—C4116.41 (14)O1—C13—C14111.21 (19)
C3—N2—N1111.23 (14)O1—C13—C12124.5 (2)
C3—N2—C4132.29 (15)C12—C13—C14124.3 (2)
C10—N5—N4104.56 (13)C4—C5—H5121.7
N2—N1—Fe1112.69 (10)C4—C5—C6116.69 (16)
C1—N1—Fe1142.05 (12)C6—C5—H5121.7
C1—N1—N2105.17 (14)C5—C6—H6119.6
C9—N6—C10101.33 (14)C5—C6—C7120.74 (17)
C19—O2—H2A107.2 (19)C7—C6—H6119.6
N5—C10—N6114.20 (15)C11—C12—H12121.6
N5—C10—C11123.95 (16)C13—C12—C11116.8 (2)
N6—C10—C11121.82 (16)C13—C12—H12121.6
N5—N4—Fe1139.02 (11)O2—C19—H19A109.5
C9—N4—Fe1114.63 (11)O2—C19—H19B109.5
C9—N4—N5106.35 (13)O2—C19—H19C109.5
C13—O1—C17104.5 (2)H19A—C19—H19B109.5
C4—N3—Fe1119.77 (12)H19A—C19—H19C109.5
C4—N3—C8119.57 (15)H19B—C19—H19C109.5
C8—N3—Fe1120.46 (12)C8—C7—C6118.72 (17)
N2—C3—H3126.8C8—C7—H7120.6
N2—C3—C2106.38 (16)C6—C7—H7120.6
C2—C3—H3126.8C15—C16—C11121.32 (19)
N1—C1—H1124.5C15—C16—H16119.3
N1—C1—C2110.91 (16)C11—C16—H16119.3
C2—C1—H1124.5C14—C18—H18127.0
N6—C9—N4113.56 (15)C17—C18—C14105.9 (2)
N6—C9—C8130.27 (16)C17—C18—H18127.0
N4—C9—C8116.07 (15)O1—C17—H17123.5
C15—C14—C18136.1 (2)C18—C17—O1113.0 (2)
C13—C14—C15118.49 (18)C18—C17—H17123.5
C13—C14—C18105.4 (2)
Fe1—N1—C1—C2175.25 (15)N3—C8—C7—C60.5 (3)
Fe1—N4—C9—N6179.26 (12)C3—N2—N1—Fe1176.63 (11)
Fe1—N4—C9—C83.9 (2)C3—N2—N1—C10.66 (19)
Fe1—N3—C4—N24.37 (19)C3—N2—C4—N3177.97 (17)
Fe1—N3—C4—C5175.56 (14)C3—N2—C4—C52.1 (3)
Fe1—N3—C8—C91.54 (19)C9—N6—C10—N50.5 (2)
Fe1—N3—C8—C7175.82 (14)C9—N6—C10—C11177.82 (16)
N2—N1—C1—C20.70 (19)C9—C8—C7—C6176.21 (18)
N2—C3—C2—C10.1 (2)C14—C15—C16—C110.3 (3)
N2—C4—C5—C6179.99 (17)C14—C13—C12—C110.3 (3)
N5—C10—C11—C12170.28 (18)C14—C18—C17—O10.1 (3)
N5—C10—C11—C1611.3 (3)C15—C14—C13—O1179.64 (19)
N5—N4—C9—N60.3 (2)C15—C14—C13—C120.3 (3)
N5—N4—C9—C8176.53 (14)C15—C14—C18—C17179.4 (3)
N1—N2—C3—C20.4 (2)C4—N2—N1—Fe16.09 (18)
N1—N2—C4—N31.4 (2)C4—N2—N1—C1176.61 (14)
N1—N2—C4—C5178.66 (17)C4—N2—C3—C2176.33 (18)
N1—C1—C2—C30.5 (2)C4—N3—C8—C9176.42 (15)
N6—C10—C11—C1211.6 (3)C4—N3—C8—C70.9 (3)
N6—C10—C11—C16166.86 (18)C4—C5—C6—C70.5 (3)
N6—C9—C8—N3179.67 (17)C8—N3—C4—N2179.28 (14)
N6—C9—C8—C72.6 (3)C8—N3—C4—C50.6 (3)
C10—N5—N4—Fe1179.40 (14)C13—O1—C17—C180.1 (3)
C10—N5—N4—C90.06 (18)C13—C14—C15—C160.3 (3)
C10—N6—C9—N40.5 (2)C13—C14—C18—C170.2 (3)
C10—N6—C9—C8175.77 (18)C5—C6—C7—C80.2 (3)
C10—C11—C12—C13178.16 (17)C12—C11—C16—C150.3 (3)
C10—C11—C16—C15178.12 (18)C16—C11—C12—C130.3 (3)
N4—N5—C10—N60.4 (2)C18—C14—C15—C16178.8 (2)
N4—N5—C10—C11177.92 (16)C18—C14—C13—O10.3 (2)
N4—C9—C8—N33.5 (2)C18—C14—C13—C12179.1 (2)
N4—C9—C8—C7173.51 (19)C17—O1—C13—C140.2 (3)
O1—C13—C12—C11179.6 (2)C17—O1—C13—C12179.1 (2)
N3—C4—C5—C60.1 (3)
Symmetry code: (i) x+1, y, z+1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O2—H2A···N50.85 (3)1.89 (2)2.750 (2)178 (3)
C1—H1···N6ii0.952.273.189 (2)163
C3—H3···O2iii0.952.293.208 (2)161
C5—H5···O2iii0.952.463.386 (2)164
C5—H5···N5iii0.951.903.463 (2)129
C7—H7···C1iv0.952.633.537 (2)159
C19—H19A···N2i0.972.743.491 (2)133
C19—H19A···C3i0.972.893.695 (2)140
C6···C3v3.482 (2)
C7···C3v3.498 (2)
Symmetry codes: (i) x+1, y, z+1/2; (ii) x1/2, y+1/2, z+1/2; (iii) x+1/2, y+1/2, z+1/2; (iv) x+1/2, y1/2, z+1/2; (v) x+3/2, y1/2, z.
Computed distortion indices (Å, °) for the title compound and for similar complexes reported in the literature. top
CSD Refcodeazol 1/azol 2<Fe—N>ΣΘCShM(Oh)
Title compound1,2,4-triazole/pyrazole1.95790.9315.22.300
BEJQOA1,2,4-triazole/pyrazole1.94687.5308.92.163
ABUFOVbenzimidazole/benzimidazole1.93780.1262.71.753
BOWRIRtetrazole/pyrazole1.93489.7287.42.043
XODCEBbenzimidazole/pyrazole1.95087.5276.61.925
 

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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