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

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COMMUNICATIONS
ISSN: 2056-9890

Synthesis, crystal structure, Hirshfeld surface analysis, and energy framework of bis­­{3-(4-bromo­phen­yl)-5-[6-(1H-pyrazol-1-yl)pyridin-2-yl]-4H-1,2,4-triazol-4-ido}nickel(II) methanol disolvate and comparison with its chloro-substituted analogue

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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 cChemBioCenter, Kyiv National Taras Shevchenko University, Kyiv 02094, 61 Winston Churchill Street, Ukraine
*Correspondence e-mail: [email protected]

Edited by F. F. Ferreira, Universidade Federal do ABC, Brazil (Received 28 July 2025; accepted 20 August 2025; online 5 September 2025)

The unit cell of the title compound, [Ni(C16H10BrN6)2]·2CH3OH, contains a neutral complex and two methanol mol­ecules. The NiII ion adopts a pseudo­octa­hedral geometry, coordinated by two tridentate ligands via pyrazole, pyridine, and triazole N atoms. The average Ni—N bond length is 2.097 (4) Å. In the crystal, mol­ecules form supra­molecular chains through weak C–H⋯π inter­actions and further assemble into diperiodic layers via C—H⋯N/C inter­actions. Hirshfeld surface analysis shows H⋯H (32.1%), H⋯C/C⋯H (27.3%), H⋯N/N⋯H (14.9%), and H⋯Br/Br⋯H (14.6%) contacts. Inter­action energies were evaluated using HF/3–21 G energy frameworks analysis. Structural parameters were compared to those of the chloro-containing analogue, and the effect of substituent variation was discussed.

1. Chemical context

A significant category of coordination compounds comprises 3d-metal complexes coordinated with tridentate bis­azole­pyridine ligands (Halcrow et al., 2019View full citation; Suryadevara et al., 2022View full citation), which have been employed in diverse applications including catalysis (Xing et al., 2014View full citation; Wei et al., 2015View full citation) and mol­ecular magnetism (Suryadevara et al., 2022View full citation). Recently, we reported an NiII complex incorporating an asymmetric deprotonated chloro-substituted ligand, 3-(4-chloro­phen­yl)-5-[6-pyrazol­yl(2-pyrid­yl)]-1H-1,2,4-triazole (KULRIW; Znovjyak et al., 2024View full citation).

[Scheme 1]

In this study, we describe the synthesis and crystal structure determination of a new complex (1) featuring a bromo-substituted ligand, 3-(4-bromo­phen­yl)-5-(6-pyrazol­yl(2-pyrid­yl))-1H-1,2,4-triazole. Comprehensive structural analyses were performed and the resulting calculated parameters were compared with those of the chloro-derivative (2).

2. Structural commentary

The two tridentate ligands span meridional and perpendicular coordination sites on the octa­hedron, forming a mol­ecule with a compact coordination part and pending diverging 4-bromo­phenyl groups. The pendant group is tilted by 26.6 (2)° relative to the nearly planar pyrazole-pyridine-triazole (pz-py-trz) fragment (r.m.s. deviation = 0.074 Å). A methanol mol­ecule forms an O—H⋯N5 hydrogen bond with the triazole ring of the ligand (Table 1[link], Fig. 1[link]). The central Ni ion adopts a distorted octa­hedral N6 coordination sphere, formed by nitro­gen atoms from two tridentate ligands, with an average Ni—N bond length of 2.097 (4) Å. The [NiN6] coordination polyhedron has a volume of 11.616 Å3. The trigonal distortion parameters are Σ = 119.3° (Σ = Σ112(|90 – φi|), where φi is the N—Ni—N′ angle; Drew et al., 1995View full citation) and Θ = 386.9° (Θ = Σ124(|60 – θi|), where θi is the angle from superposed opposite octa­hedral faces; Chang et al., 1990View full citation), indicating deviation from ideal octa­hedral geometry (Σ = Θ = 0). The continuous shape measure [CShM(Oh)] relative to ideal octa­hedral symmetry is 3.702 (Kershaw Cook et al., 2015View full citation). Compared to 2, compound 1 shows marginally higher distortion indices, reflecting the effect of varying pendant substituents (Table 2[link]).

Table 1
Hydrogen-bond geometry (Å, °)

Cg is the centroid of the C11–C16 ring.

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3⋯O1i 0.95 2.35 3.269 (8) 162
C5—H5⋯O1i 0.95 2.48 3.413 (7) 167
C1—H1⋯N6ii 0.95 2.30 3.238 (6) 171
C7—H7⋯C1iii 0.95 2.71 3.615 (7) 161
O1—H1A⋯N5 0.73 (6) 2.08 (6) 2.798 (6) 168 (6)
C2—H2⋯Cgiv 0.95 2.69 3.542 (6) 140
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.

Table 2
Computed distortion indices for the title compound and for similar complexes reported in the literature

CSD refcode <M—N> (Å) Σ (°) Θ (°) CShM(Oh)
1 2.097 119.3 386.9 3.70
2_(KULRIW) 2.095 119.4 387.3 3.71
YOCFAZ 2.088a 120.8a 397.6a 3.65a
ZOCKOT 2.086 121.0 375.9 3.78
ZOTVIP 2.110 124.9 382.4 3.55
Note: (a) averaged value.
[Figure 1]
Figure 1
The mol­ecular structure in the asymmetric unit of the title compound and contact atoms with displacement ellipsoids drawn at the 50% probability level. The strong O—H⋯N (red) and weak C—H⋯N/C/O/Cg (cyan) hydrogen bonds are shown with the nearest neighbors. Symmetry codes: (i) 1 − x, 1 + y, Mathematical equation − z; (ii) Mathematical equation + x, Mathematical equation + y, Mathematical equation − z; (iii) Mathematical equation + x, −Mathematical equation + y, Mathematical equation − z.

3. Supra­molecular features

The title compound exhibits a packing similar to 2, with adjacent mol­ecules inter­locked and inter­acting via weak off-center non-perpendicular (73.0° angle) C—H(pz)⋯π(ph) contact between the pyrazole and phenyl groups [H2/C2⋯Cg(ph) = 2.686 (1)/3.542 (6) Å]. The formed one-dimensional chains extend along the b-axis direction with a periodicity of 10.1729 (4) Å (Fig. 2[link]a), and are linked into corrugated layers in the ab plane by weak C—H(pz, py)⋯N/C(pz, trz) inter­actions [3.238 (6)–3.746 (7) Å; Fig. 2[link]b]. The layers stack without inter­actions below the van der Waals radii, while methanol mol­ecules occupy the inter­layer voids and connect them through weak O⋯H—C(pz,py) inter­actions (Fig. 2[link]c). Table 1[link] provides a summary of all inter­molecular inter­actions. Compared to 2, the overall packing remains similar, with minor differences in the values of inter­molecular contacts, which can be compared using Hirshfeld surface analysis.

[Figure 2]
Figure 2
(a) A fragment of a monoperiodic supra­molecular column formed by stacking of mol­ecules along the b axis, with C—H⋯Cg contacts indicated by red dashed lines; (b) supra­molecular diperiodic layers formed by stacking supra­molecular columns in the ab plane. The C—H⋯N/C contacts between chains are indicated by black dashed cylinders. For a better representation, each column has a different color; (c) stacking of the diperiodic layers along the c axis with the methanol mol­ecules in the voids.

4. Hirshfeld surface and two-dimensional fingerprint plots

A Hirshfeld surface analysis was conducted and two-dimensional fingerprint plots were generated using CrystalExplorer 21.5 (Spackman et al., 2021View full citation), with a standard resolution for the three-dimensional dnorm surfaces plotted over a fixed color scale ranging from −0.6304 (red) to 1.6516 (blue) a.u. Red spots indicate short contacts and negative dnorm values on the surface, which correspond to the inter­actions described above. A projection of dnorm mapped over the Hirshfeld surfaces is presented in Fig. 3[link]a. The two-dimensional fingerprint plots, along with their relative contributions to the Hirshfeld surface mapped over dnorm, are shown in Fig. 4[link]a. H⋯H inter­actions account for the largest contribution to the overall crystal packing at 32.1%, and are situated in the middle region of the fingerprint plot. H⋯C/C⋯H contacts contribute 27.3%, while H⋯N/N⋯H contacts, seen as a pair of sharp spikes, represent a 14.9% contribution to the surface. Inter­actions of H⋯Br/Br⋯H make up 14.6%, forming pairs of characteristic wings. This is greater than the H⋯Cl/Cl⋯H inter­action in 2, while other contributions are smaller due to the larger van der Waals radius of Br compared to Cl (1.85 vs 1.75 Å; Bondi, 1964View full citation) and the corresponding relative contribution to the surface area of the mol­ecule. In Fig. 4[link]b, the percentage contribution of contacts to the Hirshfeld surface for the two compounds is compared. In Fig. 4[link]c, the different inter­actions are plotted onto the Hirshfeld surface. The electrostatic potential energy calculated using the HF/3-21G basis is shown in Fig. 3[link]b. The negative charge is localized on the trz-ph moiety and the Br atom of the complex mol­ecule, whereas the pz-py moieties exhibit relatively positive charges, supporting the stacking of mol­ecules into columns and the arrangement of these columns into diperiodic two-dimensional layers.

[Figure 3]
Figure 3
(a) A projection of dnorm mapped on Hirshfeld surfaces, showing the inter­molecular inter­actions within the mol­ecule. Red/blue and white areas represent regions where contacts are shorter/larger than the sum and close to the sum of the van der Waals radii, respectively. (b) Electrostatic potential for the title compound mapped on the Hirshfeld surface. Red/blue and white areas represent regions where the charge is negative/positive or close to zero.
[Figure 4]
Figure 4
(a) Decomposition of the two-dimensional fingerprint plot of 1 into specific inter­actions and (b) comparison with those in 2; (c) a projection of dnorm mapped on the Hirshfeld surfaces, showing the inter­molecular inter­actions within the mol­ecule. Red/blue and white areas represent regions where contacts are shorter/larger than the sum and close to the sum of the van der Waals radii, respectively.

5. Energy framework analysis

The energy framework (Spackman et al., 2021View full citation), calculated at the HF/3-21G level, includes electrostatic (Eele), polarization (Epol), dispersion (Edis), repulsion (Erep) components and total energy (Etot). Cylindrical radii are scaled to the relative strength. Dispersion forces dominate in the crystal of neutral mol­ecules, and the framework topology reflects the described intra- and inter­layer inter­actions. Calculated Etot values are −49.7 kJ mol−1 (intra­chain), down to −96.5 kJ mol−1 (inter­chain), and −27.0 kJ mol−1 (inter­layer). Color-coded inter­action mappings and detailed energy contributions within 3.8 Å of a central mol­ecule are summarized in Fig. 5[link]ac. Fig. 5[link]d presents a bar plot comparing the Etot values of 1 and 2. Despite identical mol­ecular structures and packing arrangements, variations in the size and electronegativity of halogen substituents account for the differing strengths of inter­molecular inter­actions in the two compounds. Consequently, interactions within a supramol­ecular layer are stronger in 1, whereas the inter­layer inter­actions are comparatively weaker.

[Figure 5]
Figure 5
(a) The calculated energy frameworks, showing the total energy diagrams (Etot), (b) decomposition of the energy framework into the part corresponding to the inter­actions within a supra­molecular layer and (c) inter­layer inter­actions. In the table, the corresponding color-coded energy values Etot are provided, including their Eele, Epol, Edis, and Erep components. Tube size is set at 100 scale, the blue color corresponds to the attractive inter­actions, yellow to the repulsive inter­actions; (d) Comparative plots of the absolute Etot values for 1 and 2. The color-coding of the bars corresponds to the symmetry operations in the table above. The asterisks distinguish the energy bars corresponding to the intra­layer inter­actions.

6. Database survey

A search of the Cambridge Structural Database (CSD, Version 5.42; Groom et al., 2016View full citation) identifies neutral Ni complexes with tridentate bis­azolpyridine ligands containing deprotonable azole groups, such as YOCFAZ (Yuan et al., 2014View full citation), ZOCKOT (Xing et al., 2014View full citation), and ZOTVIP (Wei et al., 2015View full citation). Table 2[link] summarizes the structural parameters of these complexes along with complex 2 (KULRIW).

7. Synthesis and crystallization

The ligand was synthesized by a modified procedure reported earlier (Seredyuk et al., 2022View full citation), and the synthesis of the title complex followed the method of 2 (Znovjyak et al., 2024View full citation). All chemicals were purchased from commercial suppliers and used without further purification (Merck, Enamine Ltd.).

3-(4-Bromo­phen­yl)-5-(6-pyrazol­yl(2-pyrid­yl))-1H-1,2,4-tri­a­zole (L). A Schlenk flask with an inert atmosphere was charged with 6-(1H-pyrazol-1-yl)pyridin-2-ylboronic acid, (1.00 g, 5.3 mmol), 5-iodo-3-(4-bromo­phen­yl)-1-(tetra­hydro-2H-pyran-2-yl)-1H-1,2,4-triazole (2.09 g, 4.8 mmol), [Pd(PPh3)4] (0.61 g, 0.53 mmol) and Na2CO3 (1.65 g, 15.6 mmol). Degassed 1,4-dioxane (20 mL) and degassed water (10 mL) were added, and the reaction mixture was heated to 373 K under vigorous stirring for 16 h. After filtering through a Celite pad, to the obtained solution HClaq (37%, 5 ml) was added dropwise and the obtained solution was stirred for 10 min. Thereafter the pH of the solution was brought to neutral with an aqueous solution of NaOH (10%). The resulting suspension was evaporated to dryness and resuspended in water, and the precipitate was collected by filtration, washed with water and recrystallized from chloro­form-acetone (1:1). After drying in vacuo, the final compound was isolated as an analytically pure white crystalline powder. Yield: 1.02 g, 57%. Elemental analysis calculated for C16H11BrN6: C, 52.34; H, 3.02; N, 22.89. Found: C, 52.12; H, 3.11; N, 22.62. 1H NMR (300 MHz, 298 K, DMSO-d6): δ (ppm) 14.90 (1H, s, trzH), 9.16 (1H, s, pzH), 8.12–7.96 (5H, m, phH/pyH), 7.83 (1H, s, pzH), 7.64 (2H, d, J = 8.4 Hz, phH), 6.62 (1H, s, pzH). 13C NMR (75 MHz, DMSO-d6): δ (ppm) 161.5, 154.5, 150.9, 144.7, 143.0, 141.4, 132.1, 130.7, 128.7, 128.3, 122.9, 118.8, 113.1, 108.7.

Complex 1 was produced by a layering technique in a standard test tube. The layering sequence was as follows: the bottom layer contained a solution of [Ni(L2)](ClO4)2 prepared by dissolving L (101 mg, 0.274 mmol) and Ni(ClO4)2·6H2O (50 mg, 0.137 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 5 drops of NEt3 were added. The tube was sealed, and light violet plate-like single crystals appeared after 2 weeks (yield ca. 65%). Elemental analysis calculated for C34H28Br2N12NiO2: C, 47.75; H, 3.30; N, 19.65. Found: C, 47.52; H, 3.41; N, 19.73.

8. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. H atoms were refined as riding [C—H = 0.95–0.98 Å with Uiso(H) = 1.2–1.5Ueq(C)]. The hydrogen atom H1A was refined freely.

Table 3
Experimental details

Crystal data
Chemical formula [Ni(C16H10BrN6)2]·2CH4O
Mr 855.21
Crystal system, space group Orthorhombic, Pbcn
Temperature (K) 200
a, b, c (Å) 12.8038 (8), 10.1729 (4), 27.9377 (14)
V3) 3638.9 (3)
Z 4
Radiation type Mo Kα
μ (mm−1) 2.78
Crystal size (mm) 0.3 × 0.2 × 0.03
 
Data collection
Diffractometer Xcalibur, Eos
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 11620, 3218, 2074
Rint 0.064
(sin θ/λ)max−1) 0.595
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.061, 0.134, 1.04
No. of reflections 3218
No. of parameters 236
H-atom treatment H atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3) 0.74, −0.81
Computer programs: CrysAlis PRO 1.171.43.124 (Rigaku OD, 2024View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL2018/3 (Sheldrick, 2015bView full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

Bis{3-(4-bromophenyl)-5-[6-(1H-pyrazol-1-yl)pyridin-2-yl]-4H-1,2,4-triazol-4-ido}nickel(II) methanol disolvate top
Crystal data top
[Ni(C16H10BrN6)2]·2CH4ODx = 1.561 Mg m3
Mr = 855.21Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, PbcnCell parameters from 1992 reflections
a = 12.8038 (8) Åθ = 2.6–21.9°
b = 10.1729 (4) ŵ = 2.78 mm1
c = 27.9377 (14) ÅT = 200 K
V = 3638.9 (3) Å3Plate, clear colourless
Z = 40.3 × 0.2 × 0.03 mm
F(000) = 1720
Data collection top
Xcalibur, Eos
diffractometer
3218 independent reflections
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source2074 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.064
Detector resolution: 16.1593 pixels mm-1θmax = 25.0°, θmin = 2.2°
ω scansh = 815
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2024)
k = 1212
Tmin = 0.534, Tmax = 1.000l = 3323
11620 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.061H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.134 w = 1/[σ2(Fo2) + (0.042P)2 + 6.2503P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
3218 reflectionsΔρmax = 0.74 e Å3
236 parametersΔρmin = 0.81 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
Br10.66307 (8)0.02071 (7)0.48878 (3)0.0797 (4)
Ni10.5000000.70049 (8)0.7500000.0216 (2)
N10.5117 (3)0.8456 (4)0.80613 (15)0.0256 (10)
N20.6139 (3)0.8692 (4)0.81923 (16)0.0248 (10)
N30.6556 (3)0.7082 (4)0.76558 (14)0.0219 (10)
N40.5627 (3)0.5623 (4)0.70264 (15)0.0231 (10)
N50.5333 (3)0.4789 (4)0.66679 (15)0.0251 (10)
N60.7063 (3)0.4515 (4)0.67934 (16)0.0259 (10)
C10.4561 (4)0.9206 (5)0.83493 (19)0.0301 (13)
H10.3819860.9258040.8344320.036*
C20.5201 (5)0.9917 (5)0.8664 (2)0.0390 (16)
H20.4982671.0514860.8905260.047*
C30.6200 (5)0.9572 (5)0.8552 (2)0.0335 (14)
H30.6819980.9889520.8698870.040*
C40.6923 (4)0.7938 (5)0.79686 (18)0.0241 (12)
C50.7978 (4)0.8087 (5)0.80651 (19)0.0325 (14)
H50.8223500.8719580.8288590.039*
C60.8649 (4)0.7276 (5)0.7822 (2)0.0377 (15)
H60.9380190.7353620.7873770.045*
C70.8278 (4)0.6343 (5)0.7501 (2)0.0349 (14)
H70.8744700.5770530.7338450.042*
C80.7215 (4)0.6267 (5)0.74235 (18)0.0237 (12)
C90.6658 (4)0.5433 (5)0.70830 (18)0.0237 (12)
C100.6212 (4)0.4151 (5)0.65395 (19)0.0260 (13)
C110.6278 (4)0.3207 (5)0.61459 (19)0.0275 (13)
C120.7116 (5)0.2340 (5)0.6123 (2)0.0380 (15)
H120.7621480.2353640.6371920.046*
C130.7239 (5)0.1457 (6)0.5749 (2)0.0470 (17)
H130.7822990.0881340.5737190.056*
C140.6488 (5)0.1440 (5)0.5396 (2)0.0403 (16)
C150.5639 (5)0.2259 (5)0.5405 (2)0.0414 (16)
H150.5131850.2227180.5156510.050*
C160.5530 (5)0.3147 (5)0.57862 (19)0.0345 (14)
H160.4940190.3712280.5798500.041*
O10.3537 (4)0.5660 (5)0.61938 (19)0.0542 (14)
H1A0.397 (5)0.548 (6)0.635 (2)0.05 (2)*
C170.3843 (6)0.6447 (6)0.5808 (3)0.070 (2)
H17A0.4048250.5885620.5539080.105*
H17B0.4435640.6995910.5903980.105*
H17C0.3258550.7009400.5711410.105*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.1213 (9)0.0692 (5)0.0486 (5)0.0147 (5)0.0015 (5)0.0307 (4)
Ni10.0135 (5)0.0257 (5)0.0254 (5)0.0000.0008 (5)0.000
N10.016 (3)0.031 (2)0.030 (2)0.001 (2)0.006 (2)0.0002 (19)
N20.014 (2)0.028 (2)0.032 (3)0.0003 (19)0.002 (2)0.005 (2)
N30.016 (2)0.022 (2)0.028 (2)0.0013 (19)0.001 (2)0.0033 (18)
N40.018 (3)0.026 (2)0.025 (2)0.0010 (19)0.001 (2)0.0036 (18)
N50.019 (3)0.030 (2)0.026 (2)0.003 (2)0.000 (2)0.0039 (19)
N60.017 (2)0.028 (2)0.033 (3)0.0011 (19)0.003 (2)0.0058 (19)
C10.022 (3)0.037 (3)0.031 (3)0.005 (3)0.002 (3)0.001 (2)
C20.037 (4)0.045 (4)0.035 (3)0.010 (3)0.006 (3)0.013 (3)
C30.027 (3)0.037 (3)0.036 (3)0.000 (3)0.006 (3)0.015 (3)
C40.019 (3)0.023 (3)0.030 (3)0.003 (2)0.004 (3)0.002 (2)
C50.024 (3)0.041 (3)0.032 (3)0.002 (3)0.006 (3)0.014 (3)
C60.016 (3)0.050 (4)0.047 (4)0.001 (3)0.007 (3)0.010 (3)
C70.018 (3)0.044 (3)0.043 (4)0.003 (3)0.001 (3)0.015 (3)
C80.019 (3)0.029 (3)0.023 (3)0.001 (2)0.000 (3)0.000 (2)
C90.015 (3)0.029 (3)0.027 (3)0.002 (2)0.002 (3)0.000 (2)
C100.025 (3)0.025 (3)0.028 (3)0.005 (2)0.001 (3)0.001 (2)
C110.029 (3)0.027 (3)0.026 (3)0.003 (2)0.004 (3)0.001 (2)
C120.039 (4)0.041 (3)0.033 (3)0.003 (3)0.007 (3)0.008 (3)
C130.050 (5)0.046 (4)0.045 (4)0.014 (3)0.006 (4)0.006 (3)
C140.062 (5)0.028 (3)0.031 (3)0.002 (3)0.006 (4)0.006 (2)
C150.053 (4)0.042 (4)0.028 (3)0.005 (3)0.004 (3)0.003 (3)
C160.037 (4)0.029 (3)0.038 (3)0.001 (3)0.003 (3)0.002 (3)
O10.032 (3)0.073 (3)0.058 (3)0.004 (3)0.009 (3)0.026 (3)
C170.094 (7)0.054 (4)0.063 (5)0.014 (4)0.021 (5)0.015 (4)
Geometric parameters (Å, º) top
Br1—C141.903 (5)C5—H50.9500
Ni1—N1i2.159 (4)C5—C61.372 (7)
Ni1—N12.159 (4)C6—H60.9500
Ni1—N32.041 (4)C6—C71.390 (7)
Ni1—N3i2.041 (4)C7—H70.9500
Ni1—N4i2.091 (4)C7—C81.380 (7)
Ni1—N42.091 (4)C8—C91.461 (7)
N1—N21.380 (5)C10—C111.462 (7)
N1—C11.318 (6)C11—C121.390 (7)
N2—C31.347 (6)C11—C161.389 (7)
N2—C41.409 (6)C12—H120.9500
N3—C41.320 (6)C12—C131.386 (8)
N3—C81.349 (6)C13—H130.9500
N4—N51.366 (5)C13—C141.378 (8)
N4—C91.344 (6)C14—C151.370 (8)
N5—C101.348 (6)C15—H150.9500
N6—C91.339 (6)C15—C161.404 (7)
N6—C101.352 (6)C16—H160.9500
C1—H10.9500O1—H1A0.73 (6)
C1—C21.403 (7)O1—C171.398 (8)
C2—H20.9500C17—H17A0.9800
C2—C31.364 (7)C17—H17B0.9800
C3—H30.9500C17—H17C0.9800
C4—C51.386 (7)
N1—Ni1—N1i93.7 (2)C6—C5—C4116.7 (5)
N3—Ni1—N1i101.33 (16)C6—C5—H5121.7
N3i—Ni1—N1101.33 (16)C5—C6—H6119.5
N3i—Ni1—N1i75.58 (16)C5—C6—C7121.0 (5)
N3—Ni1—N175.58 (16)C7—C6—H6119.5
N3i—Ni1—N3175.6 (2)C6—C7—H7120.8
N3—Ni1—N477.64 (16)C8—C7—C6118.5 (5)
N3i—Ni1—N4105.42 (16)C8—C7—H7120.8
N3i—Ni1—N4i77.64 (16)N3—C8—C7120.4 (5)
N3—Ni1—N4i105.42 (16)N3—C8—C9111.5 (5)
N4i—Ni1—N1i153.21 (16)C7—C8—C9128.0 (5)
N4—Ni1—N1153.21 (16)N4—C9—C8118.2 (4)
N4—Ni1—N1i91.54 (16)N6—C9—N4114.2 (4)
N4i—Ni1—N191.54 (16)N6—C9—C8127.6 (5)
N4i—Ni1—N495.5 (2)N5—C10—N6113.6 (4)
N2—N1—Ni1112.2 (3)N5—C10—C11124.4 (5)
C1—N1—Ni1143.3 (4)N6—C10—C11121.9 (5)
C1—N1—N2104.5 (4)C12—C11—C10119.7 (5)
N1—N2—C4117.6 (4)C16—C11—C10122.2 (5)
C3—N2—N1111.6 (4)C16—C11—C12118.1 (5)
C3—N2—C4130.6 (5)C11—C12—H12118.9
C4—N3—Ni1120.9 (3)C13—C12—C11122.2 (6)
C4—N3—C8120.2 (4)C13—C12—H12118.9
C8—N3—Ni1118.9 (3)C12—C13—H13121.1
N5—N4—Ni1140.9 (3)C14—C13—C12117.9 (6)
C9—N4—Ni1113.6 (3)C14—C13—H13121.1
C9—N4—N5105.5 (4)C13—C14—Br1118.4 (5)
C10—N5—N4105.3 (4)C15—C14—Br1119.3 (5)
C9—N6—C10101.3 (4)C15—C14—C13122.3 (5)
N1—C1—H1124.3C14—C15—H15120.6
N1—C1—C2111.4 (5)C14—C15—C16118.9 (6)
C2—C1—H1124.3C16—C15—H15120.6
C1—C2—H2127.1C11—C16—C15120.6 (5)
C3—C2—C1105.8 (5)C11—C16—H16119.7
C3—C2—H2127.1C15—C16—H16119.7
N2—C3—C2106.7 (5)C17—O1—H1A112 (5)
N2—C3—H3126.6O1—C17—H17A109.5
C2—C3—H3126.6O1—C17—H17B109.5
N3—C4—N2113.6 (4)O1—C17—H17C109.5
N3—C4—C5123.2 (5)H17A—C17—H17B109.5
C5—C4—N2123.2 (5)H17A—C17—H17C109.5
C4—C5—H5121.7H17B—C17—H17C109.5
Br1—C14—C15—C16178.8 (4)C1—N1—N2—C4175.0 (4)
Ni1—N1—N2—C3178.2 (3)C1—C2—C3—N20.6 (6)
Ni1—N1—N2—C43.0 (5)C3—N2—C4—N3174.0 (5)
Ni1—N1—C1—C2176.8 (4)C3—N2—C4—C56.4 (9)
Ni1—N3—C4—N23.7 (6)C4—N2—C3—C2173.9 (5)
Ni1—N3—C4—C5175.9 (4)C4—N3—C8—C71.7 (7)
Ni1—N3—C8—C7176.4 (4)C4—N3—C8—C9178.1 (4)
Ni1—N3—C8—C90.1 (5)C4—C5—C6—C70.9 (9)
Ni1—N4—N5—C10177.8 (4)C5—C6—C7—C81.4 (9)
Ni1—N4—C9—N6177.7 (3)C6—C7—C8—N30.1 (8)
Ni1—N4—C9—C85.4 (6)C6—C7—C8—C9175.6 (5)
N1—N2—C3—C20.5 (6)C7—C8—C9—N4172.4 (5)
N1—N2—C4—N30.2 (6)C7—C8—C9—N64.0 (9)
N1—N2—C4—C5179.4 (5)C8—N3—C4—N2178.2 (4)
N1—C1—C2—C30.5 (7)C8—N3—C4—C52.2 (8)
N2—N1—C1—C20.2 (6)C9—N4—N5—C100.6 (5)
N2—C4—C5—C6179.5 (5)C9—N6—C10—N50.8 (6)
N3—C4—C5—C60.9 (8)C9—N6—C10—C11175.8 (5)
N3—C8—C9—N43.6 (6)C10—N6—C9—N41.2 (6)
N3—C8—C9—N6180.0 (5)C10—N6—C9—C8175.3 (5)
N4—N5—C10—N60.1 (6)C10—C11—C12—C13177.6 (5)
N4—N5—C10—C11176.4 (4)C10—C11—C16—C15177.7 (5)
N5—N4—C9—N61.2 (6)C11—C12—C13—C141.0 (9)
N5—N4—C9—C8175.7 (4)C12—C11—C16—C151.7 (8)
N5—C10—C11—C12162.1 (5)C12—C13—C14—Br1178.7 (4)
N5—C10—C11—C1618.4 (8)C12—C13—C14—C150.1 (9)
N6—C10—C11—C1221.6 (8)C13—C14—C15—C160.0 (9)
N6—C10—C11—C16157.8 (5)C14—C15—C16—C110.9 (8)
C1—N1—N2—C30.2 (6)C16—C11—C12—C131.8 (9)
Symmetry code: (i) x+1, y, z+3/2.
Hydrogen-bond geometry (Å, º) top
Cg is the centroid of the C11–C16 ring.
D—H···AD—HH···AD···AD—H···A
C3—H3···O1ii0.952.353.269 (8)162
C5—H5···O1ii0.952.483.413 (7)167
C1—H1···N6iii0.952.303.238 (6)171
C7—H7···C1iv0.952.713.615 (7)161
O1—H1A···N50.73 (6)2.08 (6)2.798 (6)168 (6)
C2—H2···Cgv0.952.693.542 (6)140
Symmetry codes: (ii) x+1/2, y+1/2, z+3/2; (iii) x1/2, y+1/2, z+3/2; (iv) x+1/2, y1/2, z+3/2; (v) x+1, y+1, z+3/2.
Computed distortion indices for the title compound and for similar complexes reported in the literature top
CSD refcode<M—N> (Å)Σ (°)Θ (°)CShM(Oh)
12.097119.3386.93.70
2_(KULRIW)2.095119.4387.33.71
YOCFAZ2.088a120.8a397.6a3.65a
ZOCKOT2.086121.0375.93.78
ZOTVIP2.110124.9382.43.55
Note: (a) averaged value.
Hydrogen-bond geometry (Å, °) top
D–H···AD–HH···AD···AD–H···A
C3–H3···O1i0.952.353.268 (7)162
C5–H5···O1i0.952.483.410 (7)167
C1–H1···N6ii0.952.303.238 (6)171
C7–H7···C1ii0.952.713.615 (7)161
O1–H1A···N50.73 (6)2.08 (6)2.798 (6)168 (6)
Symmetry codes: (i) 1/2 + x, 1/2 + y, 1.5 - z; (ii) 1/2 + x, -1/2 + y, 1.5 - z

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, KZ and MS; methodology, KZ; formal analysis, SON; synthesis, SOM; single-crystal measurements, SS; writing (original draft), MS; writing (review and editing of the manuscript), OT, MS; visualization and calculations, KZ, YSM; funding acquisition, MS.

Funding information

Funding for this research was provided by: grants from the Ministry of Education and Science of Ukraine (grant No. 24BF037-03).

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