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ISSN: 2056-9890

Crystal structure and Hirshfeld surface analysis of 6-bromo-2-(penta­fluoro­phen­yl)-2,3,7,7a-tetra­hydro-3a,6-ep­­oxy­isoindol-1(6H)-one

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aRUDN University, 6 Miklukho-Maklaya St., Moscow 117198, Russian Federation, bZelinsky Institute of Organic Chemistry of RAS, Leninsky Prospect 47, Moscow 119991, Russian Federation, cDepartment of Physics, Faculty of Sciences, Erciyes University, 38039 Kayseri, Türkiye, dDepartment of Chemistry, University of Gondar, PO Box 196, Gondar, Ethiopia, eAzerbaijan Medical University, Scientific Research Centre (SRC), A. Kasumzade St. 14, AZ 1022, Baku, Azerbaijan, and fDepartment of Chemical Engineering, Baku Engineering University, Hasan Aliyev str. 120, AZ0101, Khirdalan, Absheron, Azerbaijan
*Correspondence e-mail: [email protected]

Edited by B. Therrien, University of Neuchâtel, Switzerland (Received 24 July 2026; accepted 6 August 2026; online 14 August 2026)

In the crystal, enanti­omeric mol­ecules of C14H7BrF5NO2 are linked by C—H⋯O hydrogen bonds, forming layers parallel to the (101) plane. In addition, C—H⋯π inter­actions and Br⋯π contacts create layers parallel to the (101) plane. According to Hirshfeld surface analysis, the most important contributions to the crystal packing are F⋯H / H⋯F (32.4%), O⋯H / H⋯O (12.4%), F⋯F (11.5%), Br⋯F / F⋯Br (8.4%) and C⋯H / H⋯C (8.4%) inter­actions.

1. Chemical context

Fluorinated organic compounds occupy a special place among functionally substituted mol­ecules, since the introduction of fluorine atoms significantly affects the electronic structure and polarity of mol­ecules (Reichenbächer et al., 2005View full citation; Cole & Taylor, 2022View full citation). In this regard, polyfluorinated aromatic systems containing halogen atoms capable of acting as a halogen-bond donor are of particular inter­est. According to modern concepts, a halogen bond occurs when an electrophilic region associated with a halogen atom inter­acts with the nucleophilic centre of another mol­ecule or the same mol­ecule (Desiraju et al., 2013View full citation; Huseynov et al., 2021View full citation). The directionality of such a bond is usually explained by the presence of a σ-hole region of positive electrostatic potential on the continuation of the C—X bond (Politzer et al., 2010View full citation; Maslova et al., 2026View full citation). Polyfluorination of the aromatic fragment enhances the electron-acceptor character of the system and can increase the positive potential on the halogen atom, thereby increasing the ability of the compound to form halogen bonds (Riley et al., 2011View full citation; Mamedov et al., 2024View full citation; Javadzade et al., 2026View full citation). Although bromine-containing donors usually form weaker inter­actions compared to iodine-containing analogues, the presence of a penta­fluoro­phenyl fragment makes such systems promising candidates for studying Br⋯N, Br⋯O, and Br⋯π contacts (Yang et al., 2018View full citation; Guseinov et al., 2025View full citation; Makhmudova et al., 2022View full citation). We therefore synthesized and elucidated the crystal structure of the title compound.

[Scheme 1]

2. Structural commentary

The title compound crystallizes in the centrosymmetric space group P21/n, and therefore occurs as a racemic mixture of the 3aR,6S,7aS and 3aS,6R,7aR enantiomers. In the seven-membered ring system (O8/C3A/C4–C7/C7A) of the mol­ecule (Fig. 1[link]), the two five-membered A and B rings (A: O8/C3A/C4–C6 and B: O8/C3A/C6/C7/C7A) have the puckering parameters Q(2) = 0.6054 (19) Å, φ(2) = 355.9 (2)°, and Q(2) = 0.267 (2) Å, φ(2) = 282.7 (4)°, respectively, and adopt an envelope conformation on the O8 atom. The six-membered ring (C: C3A/C4–C7/C7A) has the puckering parameters QT = 0.947 (2) Å, θ = 90.74 (12)°, φ = 177.46 (13)° and exhibits a boat conformation. The five-membered pyrrolidine ring (D: N2/C1/C3/C3A/C7A) fused to the seven-membered ring system (O8/C3A/C4–C7/C7A) has the puckering parameters Q(2) = 0.267 (2) Å, φ(2) = 282.7 (4) ° and adopts an envelope conformation on atom C3A. The angles between the pentafluoro­phenyl ring (E: C8–C13) and the C (C3A/C4–C7/C7A) and D (N2/C1/C3/C3A/C7A) planes are 45.95 (11) and 69.23 (10)°, respectively. The C and D rings subtend an angle of 39.15 (12)°. The bond lengths and angles are comparable to those in the related structures discussed in the Database survey section.

[Figure 1]
Figure 1
Mol­ecular structure showing the atom labelling and ring system with displacement ellipsoids at 50% probability level.

3. Supra­molecular features and Hirshfeld surface analysis

In the crystal, mol­ecules are linked by C—H⋯O hydrogen bonds, forming layers parallel to the (Mathematical equation01) plane (Table 1[link], Fig. 2[link]). In addition, C—H⋯π (Table 1[link]) and Br⋯π inter­actions [(C6)Br1⋯Cg5ii: C6—Br1 = 1.9249 (18) Å, Br1⋯Cg5ii = 3.6147 (9) Å, C6⋯Cg5ii = 3.988 (2) Å and C6—Br1⋯Cg5ii = 86.43 (6)°; Cg5 is the centroid of the penta­fluoro­phenyl ring (C8–C13); symmetry code (ii) −x + 1, −y + 1, −z + 1] act in opposite directions of the plane of the penta­fluoro­phenyl ring, bonding mol­ecules form layers parallel to the (10Mathematical equation) plane (Fig. 3[link]).

Table 1
Hydrogen-bond geometry (Å, °)

Cg5 is the centroid of the penta­fluoro­phenyl ring (C8–C13).

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3A⋯O1i 0.99 2.60 3.167 (2) 117
C3—H3B⋯O8ii 0.99 2.60 3.410 (2) 140
C4—H4⋯O1iii 0.95 2.38 3.309 (3) 167
C7A—H7C⋯O1i 1.00 2.48 3.109 (3) 120
C7A—H7CCg5i 1.00 2.87 3.790 (2) 153
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation.
[Figure 2]
Figure 2
Partial packing view showing the C—H⋯O hydrogen bonds.
[Figure 3]
Figure 3
Partial packing view showing the C—H⋯π inter­actions and Br⋯π contacts with centroids of penta­fluoro­phenyl rings.

In order to qu­antify the inter­molecular inter­actions, a Hirshfeld surface analysis was carried out using Crystal Explorer 21 (Spackman et al., 2021View full citation) and the associated two-dimensional fingerprint plots were generated. The Hirshfeld surface mapped over dnorm in the range −0.2735 to +1.2893 a.u. is shown in Fig. 4[link], using colours to indicate contacts that are shorter (red areas), equal to (white areas), or longer than (blue areas) the sum of the van der Waals radii. The C—H⋯O inter­actions are indicated by red areas on the Hirshfeld surfaces (Tables 1[link] and 2[link]).

Table 2
Summary of short inter­atomic contacts (Å)

Contact Distance Symmetry operation
Br1⋯H5 3.11 Mathematical equation − x, Mathematical equation + y, Mathematical equation − z
F1⋯F1 2.64 1 − x, 2 − y, 1 − z
H3B⋯O8 2.60 1 − x, 1 − y, 1 − z
H7B⋯F3 2.56 Mathematical equation + x, Mathematical equation − y, −Mathematical equation + z
O1⋯H4 2.38 x, 1 + y, z
F4⋯F3 2.97 x, 2 − y, 1 − z
F4⋯F4 2.80 x, 1 − y, 1 − z
H7C⋯O1 2.48 Mathematical equation − x, −Mathematical equation + y, Mathematical equation − z
[Figure 4]
Figure 4
View of the three-dimensional Hirshfeld surface plotted over dnorm in the range −0.2735 to 1.2893 a.u.

The two-dimensional fingerprint plots provide qu­anti­tative information about the non-covalent inter­actions and the crystal packing in terms of the percentage contribution of the inter­atomic contacts. The overall two-dimensional fingerprint plot is shown in Fig. 5[link]a. The dominant inter­actions in the crystal packing are F⋯H/H⋯F (32.4%), O⋯H/H⋯O (12.4%), F⋯F (11.5%), Br⋯F / F⋯Br (8.4%) and C⋯H/H⋯C (8.4%) contacts; see Fig. 5bf[link]. The other contacts (H⋯H 6.7%, Br⋯H/H⋯Br 5.9%, Br⋯C/C⋯Br 4.6%, O⋯C/C⋯O 2.5%, F⋯O/O⋯F 2.2%, F⋯C/C⋯F 1.7%, C⋯C 1.6%, Br⋯Br 1.2%, O⋯N/N⋯O 0.3% and N⋯H/H⋯N 0.1%) only make a minor contribution to the crystal packing.

[Figure 5]
Figure 5
The two-dimensional fingerprint plots showing (a) all inter­actions, and those delineated into (b) F⋯H/H⋯F, (c) O⋯H/H⋯O, (d) F⋯F, (e) Br⋯F/F⋯Br and (f) C⋯H/H⋯C inter­actions. The di and de values are the closest inter­nal and external distances (in Å) from given points on the Hirshfeld surface.

4. Database survey

A search of the Cambridge Structural Database (CSD, Version 6.00, update of April 2025; Groom et al., 2016View full citation) for the 1,2,3,6,7,7a-hexa­hydro-3a,6-ep­oxy­iso­indole unit revealed five analogues: BILLEP (Mitchell et al., 2013View full citation), BILLAL (Mitchell et al., 2013View full citation), VAMREL (Shchevnikov et al., 2026View full citation), DUBYUX (Tan et al., 2020View full citation) and DUBZAE (Tan et al., 2020View full citation).

Although there are no conventional hydrogen bonds in BILLEP, there are weaker inter­actions between the mol­ecules, such as C—H⋯O and C—H⋯N, as compared to N—H⋯O hydrogen bonds in BILLAL. Compound BILLAL packs head-to-head with hydrogen bonding, whereas compound BILLEP packs head-to-tail with regard to the ether groups.

The asymmetric unit of VAMREL contains two crystallographically independent mol­ecules in which the cyclo­hexene and pyrrole rings are in boat and envelope conformations, respectively. In the crystal, C—H⋯O and N—H⋯Se hydrogen bonds link the mol­ecules into [100] chains, enclosing R22(20), R33(18) and R44(4) ring motifs (Bernstein et al., 1995View full citation). C—H⋯π (ring) inter­actions help to consolidate the packing.

In DUBYUX, mol­ecules are linked by ππ inter­actions into chains along the b-axis direction. At the same time, C—H⋯π inter­actions also link DUBYUX mol­ecules into chains extending along the b-axis direction. These inter­actions form layers parallel to the ab plane. In the crystal structure of DUBZAE, hydrogen bonds, C— H⋯π and ππ inter­actions occur between mol­ecules.

5. Synthesis and crystallization

Penta­fluoro­aniline (1045 mg, 5.71 mmol) was added to the corresponding 5-bromo­furfural (1000 mg, 5.71 mmol) in toluene (20 ml). The reaction mixture was heated under reflux for 5 days using a Dean–Stark trap (TLC control). After the reaction was completed, the solution was concentrated. The residue was dissolved in methanol (15 ml) and sodium borohydride (430 mg, 11.4 mmol) was added portionwise (36 mg in every 5 min) over a period of 1 h. The resulting mixture was stirred at room temperature for 24 h (TLC control, hexa­ne–EtOAc, 10:1). The reaction mixture was poured into water (30 ml) and extracted with DCM (3 × 30 ml). The organic layers were dried with anhydrous MgSO4, concentrated and purified by column chromatography (SiO2, 23 × 1.6 cm, eluent hexane-EtOAc, 50:1) to afford N-[(5-bromo­furan-2-yl)meth­yl]-2,3,4,5,6-penta­fluoro­aniline in good yield. Yellow oil, yield 63%, 1228 mg (3.59 mmol). 1H NMR (700.2 MHz, CDCl3), (J, Hz) δ 6.22 (s, 2 H, H-3 and H-4 Fur), 4.42 (d, J = 7.2 Hz, 2 H, NCH2), 4.01 (br. s, 1 H, NH). 13C NMR (176.1 MHz, CDCl3) δ 153.8, 138.4 (dm, J = 244.4 Hz, 2 C, C—F), 138.1 (dm, J = 248.5 Hz, 2 C, C—F), 134.3 (dm, J = 245.8 Hz, 1 C, C—F), 122.5 (t, J = 12.1 Hz, 1 C, C—Ar), 121.9, 112.0, 110.7, 42.9 (t, J = 4.1 Hz, 1 C, CH2). 19F NMR (658.8 MHz, CDCl3) δ −158.0 (d, J = 21.5 Hz, 2 F, F-2,6 Ar), −163.9 (t, J = 21.5 Hz, 2 F, F-3,5 Ar), −169.5 (d, J = 21.5 Hz, 1 F, F-4 Ar). IR (KBr, cm−1): νmax = 3316 (NH), 1124, 1011, 964, 787 (C-Hal). GC—MS (EI, 70 eV) m/z: 343 [M, Br81]+, 341 [M, Br79]+, 194 (10), 161 (98), 159 (100), 155 (14), 133 (45), 131 (47), 117 (13), 51 (26).

N-[(5-bromo­furan-2-yl)meth­yl]-2,3,4,5,6-penta­fluoro­aniline (1200 mg, 3.51 mmol), and Et3N (1.1 ml, 8.07 mmol) were dissolved in pseudocumene (50 ml) and stirred for 5 min. Acryloyl chloride was added (0.51 ml, 6.32 mmol), and the reaction mixture was heated under reflux for 5 days (TLC control, hexa­ne–EtOAc, 1:1). After cooling, the reaction mixture was filtered, and the filtrate was poured into water (30 ml) and extracted with EtOAc (3 × 30 ml). The organic layers were dried with anhydrous MgSO4. The solvent was evaporated at reduced pressure, and the residue was triturated with ether (2 × 15 ml) to isolate 6-bromo-2-(penta­fluoro­phen­yl)-2,3,7,7a-tetra­hydro-3a,6-ep­oxy­isoindol-1(6H)-one. The precipitate was filtered off and washed with ether (2 × 15 ml). Brown powder, yield 47%, 653 mg (1.65 mmol), m.p. 453–455 K. Single crystals were grown in DMSO at 281 K. 1H NMR (700.2 MHz, CDCl3), (J, Hz) δ 6.56 and 6.55 (two d, J = 5.7 Hz, 2 H, H-4 and H-5), 4.41 (d, J = 11.4 Hz, 1 H, H-3A), 4.08 (d, J = 11.4 Hz, 1 H, H-3B), 2.83 (dd, J = 8.6, 3.6 Hz, 1 H, H-7a), 2.66 (dd, J = 12.2, 3.6 Hz, 1 H, H-7A), 2.35 (dd, J = 12.2, 8.6 Hz, 1 H, H-7B). 13C NMR (176.1 MHz, CDCl3) δ 172.0, 144.1 (dm, J = 253.9 Hz, 2 C, C—F), 141.6, 141.2 (dm, J = 255.9 Hz, 1 C, C—F), 138.0 (dm, J = 247.8 Hz, 2 C, C—F), 133.6, 112.7 (t, J = 11.5 Hz, 1 C, C—Ar), 88.8, 88.5, 51.3, 49.4, 39.6. 19F NMR (658.8 MHz, DMSO-d6) δ −144.3 (br. s, 2 F, F-2,6 Ar), −155.5 (d, J = 21.5 Hz, 1 F, F-4 Ar), −162.8 (t, J = 21.5 Hz, 2 F, F-3,5 Ar). IR (KBr, cm−1): νmax = 1709 (C=O), 1120, 1095, 953, 926, 840, 718, 662 (C–Hal). GC—MS (EI, 70 eV) m/z: 397 [M, Br81]+, 395 [M, Br79]+, 316 (100), 220 (31), 194 (36), 167 (13), 161 (62), 159 (60), 132 (15), 131 (23), 117 (12), 77 (15), 55 (58).

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. All C-bound H atoms were positioned geometrically and refined using a riding model, with C—H = 0.95–1.00 Å and Uiso(H) = 1.2Ueq(C).

Table 3
Experimental details

Crystal data
Chemical formula C14H7BrF5NO2
Mr 396.11
Crystal system, space group Monoclinic, P21/n
Temperature (K) 100
a, b, c (Å) 13.4425 (1), 7.0992 (1), 14.9829 (2)
β (°) 106.241 (1)
V3) 1372.77 (3)
Z 4
Radiation type Cu Kα
μ (mm−1) 4.76
Crystal size (mm) 0.45 × 0.33 × 0.20
 
Data collection
Diffractometer Rigaku XtaLAB Synergy-S, HyPix-6000HE area-detector
Absorption correction Analytical [CrysAlis PRO (Agilent, 2014View full citation). Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by Clark & Reid (1995View full citation)]
Tmin, Tmax 0.385, 0.622
No. of measured, independent and observed [I > 2σ(I)] reflections 15639, 2965, 2814
Rint 0.041
(sin θ/λ)max−1) 0.638
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.033, 0.094, 1.08
No. of reflections 2965
No. of parameters 209
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.56, −0.65
Computer programs: CrysAlis PRO (Agilent, 2014View full citation), SHELXT (Sheldrick, 2015aView full citation), SHELXL (Sheldrick, 2015bView full citation), ORTEP-3 for Windows (Farrugia, 2012View full citation), Mercury (Macrae et al., 2020View full citation) and PLATON (Spek, 2020View full citation).

Supporting information


Computing details top

6-Bromo-2-(pentafluorophenyl)-2,3,7,7a-tetrahydro-3a,6-epoxyisoindol-1(6H)-one top
Crystal data top
C14H7BrF5NO2F(000) = 776
Mr = 396.11Dx = 1.917 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54184 Å
a = 13.4425 (1) ÅCell parameters from 10823 reflections
b = 7.0992 (1) Åθ = 3.9–79.2°
c = 14.9829 (2) ŵ = 4.76 mm1
β = 106.241 (1)°T = 100 K
V = 1372.77 (3) Å3Prism, colourless
Z = 40.45 × 0.33 × 0.20 mm
Data collection top
Rigaku XtaLAB Synergy-S, HyPix-6000HE area-detector
diffractometer
2814 reflections with I > 2σ(I)
Radiation source: micro-focus sealed X-ray tubeRint = 0.041
φ and ω scansθmax = 79.7°, θmin = 3.9°
Absorption correction: analytical
[CrysAlisPro (Agilent, 2014). Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by Clark & Reid (1995)]
h = 1715
Tmin = 0.385, Tmax = 0.622k = 89
15639 measured reflectionsl = 1919
2965 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.094 w = 1/[σ2(Fo2) + (0.0604P)2 + 0.7868P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
2965 reflectionsΔρmax = 0.56 e Å3
209 parametersΔρmin = 0.65 e Å3
0 restraintsExtinction correction: SHELXL-2019/2 (Sheldrick, 2015b), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: difference Fourier mapExtinction coefficient: 0.00042 (4)
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
Br10.71543 (2)0.50666 (3)0.31376 (2)0.02411 (12)
F10.41520 (9)0.89713 (18)0.47110 (8)0.0256 (3)
F20.31108 (11)1.11945 (18)0.56004 (9)0.0331 (3)
F30.11978 (14)1.01534 (19)0.57004 (12)0.0346 (4)
F40.03644 (10)0.6834 (2)0.49575 (11)0.0366 (3)
F50.14074 (10)0.45924 (19)0.40680 (9)0.0269 (3)
O10.31755 (10)0.8046 (2)0.27300 (9)0.0210 (3)
C10.34540 (13)0.6469 (3)0.30167 (12)0.0169 (3)
N20.33237 (12)0.5708 (2)0.38162 (11)0.0173 (3)
C30.37373 (14)0.3779 (3)0.40281 (13)0.0179 (4)
H3A0.3175460.2829580.3890510.021*
H3B0.4150500.3657950.4685470.021*
C3A0.44098 (13)0.3599 (3)0.33735 (12)0.0174 (3)
C40.46877 (15)0.1797 (3)0.29634 (14)0.0225 (4)
H40.4351220.0610710.2922470.027*
C50.55086 (15)0.2237 (3)0.26714 (14)0.0231 (4)
H50.5873210.1437990.2363010.028*
C60.57366 (14)0.4291 (3)0.29374 (13)0.0192 (4)
C70.49343 (14)0.5591 (3)0.22739 (13)0.0193 (4)
H7A0.5101240.6940530.2398260.023*
H7B0.4865880.5308680.1612310.023*
C7A0.39609 (16)0.5001 (2)0.25605 (14)0.0175 (4)
H7C0.3441710.4370420.2035140.021*
O80.54265 (9)0.4439 (2)0.37751 (9)0.0176 (3)
C80.27993 (13)0.6742 (3)0.43498 (12)0.0175 (4)
C90.32160 (14)0.8430 (3)0.47564 (13)0.0202 (4)
C100.26888 (18)0.9572 (3)0.52161 (14)0.0239 (4)
C110.17202 (16)0.9045 (3)0.52701 (14)0.0249 (4)
C120.12954 (15)0.7358 (3)0.48870 (14)0.0239 (4)
C130.18329 (14)0.6216 (3)0.44315 (13)0.0200 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br10.01600 (16)0.02940 (18)0.02836 (17)0.00105 (6)0.00857 (11)0.00042 (7)
F10.0191 (5)0.0281 (6)0.0304 (6)0.0076 (4)0.0084 (4)0.0045 (5)
F20.0456 (8)0.0238 (6)0.0326 (6)0.0059 (6)0.0155 (6)0.0088 (5)
F30.0433 (9)0.0313 (7)0.0382 (8)0.0107 (5)0.0261 (7)0.0001 (5)
F40.0260 (6)0.0386 (8)0.0543 (8)0.0011 (5)0.0262 (6)0.0023 (6)
F50.0237 (6)0.0256 (6)0.0341 (7)0.0083 (5)0.0126 (5)0.0035 (5)
O10.0180 (6)0.0217 (7)0.0235 (6)0.0021 (5)0.0064 (5)0.0053 (5)
C10.0131 (7)0.0196 (9)0.0175 (8)0.0031 (6)0.0036 (6)0.0004 (6)
N20.0156 (7)0.0181 (8)0.0188 (7)0.0011 (6)0.0059 (6)0.0015 (6)
C30.0189 (8)0.0161 (9)0.0195 (8)0.0004 (7)0.0068 (7)0.0018 (6)
C3A0.0156 (8)0.0183 (8)0.0182 (8)0.0019 (6)0.0046 (6)0.0004 (6)
C40.0248 (9)0.0169 (9)0.0262 (9)0.0000 (7)0.0078 (7)0.0024 (7)
C50.0246 (9)0.0204 (9)0.0255 (9)0.0026 (7)0.0089 (7)0.0028 (7)
C60.0159 (8)0.0214 (10)0.0219 (9)0.0001 (7)0.0082 (7)0.0006 (7)
C70.0160 (8)0.0234 (9)0.0191 (8)0.0003 (7)0.0061 (7)0.0030 (7)
C7A0.0175 (10)0.0187 (10)0.0163 (9)0.0009 (6)0.0046 (7)0.0010 (6)
O80.0143 (6)0.0205 (6)0.0180 (6)0.0020 (5)0.0047 (5)0.0008 (5)
C80.0159 (8)0.0194 (9)0.0173 (8)0.0013 (6)0.0046 (6)0.0022 (7)
C90.0173 (8)0.0224 (9)0.0208 (8)0.0028 (7)0.0053 (7)0.0009 (7)
C100.0315 (11)0.0187 (9)0.0221 (9)0.0013 (8)0.0084 (8)0.0021 (8)
C110.0291 (10)0.0261 (10)0.0236 (9)0.0079 (8)0.0144 (8)0.0031 (8)
C120.0200 (8)0.0270 (10)0.0282 (9)0.0020 (7)0.0124 (7)0.0053 (8)
C130.0184 (8)0.0216 (9)0.0204 (8)0.0018 (7)0.0061 (7)0.0017 (7)
Geometric parameters (Å, º) top
Br1—C61.9249 (18)C4—C51.333 (3)
F1—C91.335 (2)C4—H40.9500
F2—C101.341 (2)C5—C61.520 (3)
F3—C111.335 (2)C5—H50.9500
F4—C121.338 (2)C6—O81.433 (2)
F5—C131.334 (2)C6—C71.550 (3)
O1—C11.220 (2)C7—C7A1.545 (3)
C1—N21.369 (2)C7—H7A0.9900
C1—C7A1.509 (3)C7—H7B0.9900
N2—C81.411 (2)C7A—H7C1.0000
N2—C31.479 (2)C8—C131.389 (3)
C3—C3A1.514 (2)C8—C91.389 (3)
C3—H3A0.9900C9—C101.381 (3)
C3—H3B0.9900C10—C111.379 (3)
C3A—O81.458 (2)C11—C121.381 (3)
C3A—C41.511 (3)C12—C131.386 (3)
C3A—C7A1.558 (3)
O1—C1—N2124.63 (17)C7A—C7—H7A112.0
O1—C1—C7A127.38 (16)C6—C7—H7A112.0
N2—C1—C7A107.96 (15)C7A—C7—H7B112.0
C1—N2—C8119.81 (16)C6—C7—H7B112.0
C1—N2—C3114.88 (15)H7A—C7—H7B109.7
C8—N2—C3125.28 (15)C1—C7A—C7117.64 (15)
N2—C3—C3A101.29 (14)C1—C7A—C3A102.24 (15)
N2—C3—H3A111.5C7—C7A—C3A102.56 (15)
C3A—C3—H3A111.5C1—C7A—H7C111.2
N2—C3—H3B111.5C7—C7A—H7C111.2
C3A—C3—H3B111.5C3A—C7A—H7C111.2
H3A—C3—H3B109.3C6—O8—C3A94.44 (13)
O8—C3A—C4101.77 (14)C13—C8—C9117.71 (17)
O8—C3A—C3111.03 (14)C13—C8—N2122.55 (17)
C4—C3A—C3126.55 (16)C9—C8—N2119.55 (16)
O8—C3A—C7A100.07 (14)F1—C9—C10118.60 (18)
C4—C3A—C7A107.98 (15)F1—C9—C8119.73 (17)
C3—C3A—C7A106.37 (15)C10—C9—C8121.67 (18)
C5—C4—C3A104.88 (17)F2—C10—C11120.07 (19)
C5—C4—H4127.6F2—C10—C9120.28 (19)
C3A—C4—H4127.6C11—C10—C9119.7 (2)
C4—C5—C6105.28 (16)F3—C11—C10120.1 (2)
C4—C5—H5127.4F3—C11—C12119.99 (19)
C6—C5—H5127.4C10—C11—C12119.90 (18)
O8—C6—C5102.30 (15)F4—C12—C11119.69 (18)
O8—C6—C7101.40 (14)F4—C12—C13120.31 (19)
C5—C6—C7110.46 (15)C11—C12—C13120.00 (18)
O8—C6—Br1111.13 (12)F5—C13—C12118.90 (17)
C5—C6—Br1115.69 (13)F5—C13—C8120.05 (17)
C7—C6—Br1114.25 (13)C12—C13—C8121.04 (18)
C7A—C7—C698.75 (14)
O1—C1—N2—C82.6 (3)Br1—C6—O8—C3A174.99 (12)
C7A—C1—N2—C8175.69 (15)C4—C3A—O8—C652.09 (16)
O1—C1—N2—C3179.22 (16)C3—C3A—O8—C6170.87 (15)
C7A—C1—N2—C32.5 (2)C7A—C3A—O8—C658.85 (15)
C1—N2—C3—C3A14.4 (2)C1—N2—C8—C13111.4 (2)
C8—N2—C3—C3A167.53 (16)C3—N2—C8—C1366.6 (2)
N2—C3—C3A—O883.26 (17)C1—N2—C8—C963.5 (2)
N2—C3—C3A—C4152.88 (17)C3—N2—C8—C9118.5 (2)
N2—C3—C3A—C7A24.69 (18)C13—C8—C9—F1178.66 (16)
O8—C3A—C4—C534.54 (19)N2—C8—C9—F16.2 (3)
C3—C3A—C4—C5162.19 (18)C13—C8—C9—C100.9 (3)
C7A—C3A—C4—C570.3 (2)N2—C8—C9—C10174.27 (18)
C3A—C4—C5—C61.7 (2)F1—C9—C10—F20.5 (3)
C4—C5—C6—O832.27 (19)C8—C9—C10—F2179.92 (18)
C4—C5—C6—C775.0 (2)F1—C9—C10—C11179.84 (17)
C4—C5—C6—Br1153.23 (14)C8—C9—C10—C110.6 (3)
O8—C6—C7—C7A41.07 (17)F2—C10—C11—F30.4 (3)
C5—C6—C7—C7A66.82 (18)C9—C10—C11—F3178.97 (19)
Br1—C6—C7—C7A160.68 (12)F2—C10—C11—C12178.90 (19)
O1—C1—C7A—C752.6 (3)C9—C10—C11—C121.8 (3)
N2—C1—C7A—C7129.20 (17)F3—C11—C12—F40.6 (3)
O1—C1—C7A—C3A163.98 (17)C10—C11—C12—F4178.65 (19)
N2—C1—C7A—C3A17.80 (19)F3—C11—C12—C13179.31 (18)
C6—C7—C7A—C1115.08 (18)C10—C11—C12—C131.4 (3)
C6—C7—C7A—C3A3.86 (17)F4—C12—C13—F50.1 (3)
O8—C3A—C7A—C189.03 (15)C11—C12—C13—F5179.93 (17)
C4—C3A—C7A—C1164.97 (15)F4—C12—C13—C8179.81 (17)
C3—C3A—C7A—C126.57 (18)C11—C12—C13—C80.1 (3)
O8—C3A—C7A—C733.29 (17)C9—C8—C13—F5178.79 (17)
C4—C3A—C7A—C772.70 (18)N2—C8—C13—F56.2 (3)
C3—C3A—C7A—C7148.89 (15)C9—C8—C13—C121.3 (3)
C5—C6—O8—C3A50.93 (15)N2—C8—C13—C12173.77 (17)
C7—C6—O8—C3A63.21 (15)
Hydrogen-bond geometry (Å, º) top
Cg5 is the centroid of the pentafluorophenyl ring (C8–C13).
D—H···AD—HH···AD···AD—H···A
C3—H3A···O1i0.992.603.167 (2)117
C3—H3B···O8ii0.992.603.410 (2)140
C4—H4···O1iii0.952.383.309 (3)167
C7A—H7C···O1i1.002.483.109 (3)120
C7A—H7C···Cg5i1.002.873.790 (2)153
Symmetry codes: (i) x+1/2, y1/2, z+1/2; (ii) x+1, y+1, z+1; (iii) x, y1, z.
Summary of short interatomic contacts (Å) top
ContactDistanceSymmetry operation
Br1···H53.113/2-x, 1/2+y, 1/2-z
F1···F12.641-x, 2-y, 1-z
H3B···O82.601-x, 1-y, 1-z
H7B···F32.561/2+x, 3/2-y, -1/2+z
O1···H42.38x, 1+y, z
F4···F32.97-x, 2-y, 1-z
F4···F42.80-x, 1-y, 1-z
H7C···O12.481/2-x, -1/2+y, 1/2-z
 

Acknowledgements

The authors' contributions are as follows; conceptualization MA and GMM; synthesis, VSM and VMC; X-ray analysis VNK; writing (review and editing of the manuscript) MA, KIH and NAG; supervision MA and GMM.

Funding information

Funding for this research was provided by: the RUDN University Scientific Projects Grant System (grant No. 021422-2-000), the Azerbaijan Medical University and Baku Engineering University.

References

Return to citationAgilent (2014). CrysAlis PRO. Agilent Technologies Ltd, Yarnton, England.  Google Scholar
Return to citationBernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555–1573.  CrossRef CAS Web of Science Google Scholar
Return to citationClark, R. C. & Reid, J. S. (1995). Acta Cryst. A51, 887–897.  CrossRef CAS Web of Science IUCr Journals Google Scholar
Return to citationCole, J. C. & Taylor, R. (2022). Cryst. Growth Des. 22, 1352–1364.  Web of Science CrossRef CAS Google Scholar
Return to citationDesiraju, G. R., Ho, P. S., Kloo, L., Legon, A. C., Marquardt, R., Metrangolo, P., Politzer, P., Resnati, G. & Rissanen, K. (2013). Pure Appl. Chem. 85, 1711–1713.  Web of Science CrossRef CAS Google Scholar
Return to citationFarrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationGroom, C. R., Bruno, I. J., Lightfoot, M. P. & Ward, S. C. (2016). Acta Cryst. B72, 171–179.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationGuseinov, F. I., Samigullina, A. I., Hökelek, T., Hamidov, S. Z., Lasri, J., Hasanov, K. I., Javadzade, T. A. & Belay, A. N. (2025). Acta Cryst. E81, 672–675.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationHuseynov, F. E., Mahmoudi, G., Hajiyeva, S. R., Shamilov, N. T., Zubkov, F. I., Nikitina, E. V., Prisyazhnyuk, E. D. & Kopylovich, M. N. (2021). Polyhedron 209, 115453.  Web of Science CrossRef Google Scholar
Return to citationJavadzade, T. A., Hajiyeva, S. R., Chyragov, F. M., Nunes, A. V. M., Lasri, J., Hamidov, S. Z., Hasanov, K. I. & Mahmudov, K. T. (2026). J. Organomet. Chem. 1046, 123901.  Web of Science CrossRef Google Scholar
Return to citationMacrae, C. F., Sovago, I., Cottrell, S. J., Galek, P. T. A., McCabe, P., Pidcock, E., Platings, M., Shields, G. P., Stevens, J. S., Towler, M. & Wood, P. A. (2020). J. Appl. Cryst. 53, 226–235.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationMakhmudova, N. I., Mammadov, E. S., Kerimli, F. S., Ilyasli, T. M., Akhmedova, N. F. & Mammadov, S. E. (2022). Bull. Chem. React. Eng. Catal. 17, 725–732.  Web of Science CrossRef CAS Google Scholar
Return to citationMamedov, İ. G., Khrustalev, V. N., Akkurt, M., Kerimli, F. S., Bhattarai, A., Khalilov, A. N. & Naghiyev, F. N. (2024). Acta Cryst. E80, 495–500.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationMaslova, V. S., Gomila, R. M., Dikusar, E. A., Zaytsev, V. P., Khrustalev, V. N., Zubkov, F. I. & Frontera, A. (2026). J. Mol. Struct. 1361, 145700.  Web of Science CrossRef Google Scholar
Return to citationMitchell, L. A., Stanley, J. M., Espinosa DeHoyos, L. & Holliday, B. J. (2013). Acta Cryst. C69, 638–641.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationPolitzer, P., Murray, J. S. & Clark, T. (2010). Phys. Chem. Chem. Phys. 12, 7748–7757.  Web of Science CrossRef CAS PubMed Google Scholar
Return to citationReichenbächer, K., Süss, H. I. & Hulliger, J. (2005). Chem. Soc. Rev. 34, 22–30.  Web of Science CrossRef PubMed Google Scholar
Return to citationRiley, K. E., Murray, J. S., Fanfrlík, J., Řezáč, J., Solá, R. J., Concha, M. C., Ramos, F. M. & Politzer, P. (2011). J. Mol. Model. 17, 3309–3318.  Web of Science CrossRef CAS PubMed Google Scholar
Return to citationShchevnikov, D. M., Gurbanov, A. V., Khrustalev, V. N., Woldemariam, M. M., Hökelek, T. & Litvinov, R. A. (2026). Acta Cryst. E82, 572–577.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSpackman, P. R., Turner, M. J., McKinnon, J. J., Wolff, S. K., Grimwood, D. J., Jayatilaka, D. & Spackman, M. A. (2021). J. Appl. Cryst. 54, 1006–1011.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationSpek, A. L. (2020). Acta Cryst. E76, 1–11.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationTan, X.-J., Liu, S., Hei, X.-M., Yang, F.-C., He, P.-B., Guo, F. & Xing, D.-X. (2020). Acta Cryst. C76, 75–86.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationYang, F.-L., Yang, X., Wu, R.-Z., Yan, C.-X., Yang, F., Ye, W., Zhang, L.-W. & Zhou, P.-P. (2018). Phys. Chem. Chem. Phys. 20, 11386–11395.  Web of Science CrossRef CAS PubMed Google Scholar

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