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ISSN: 2056-9890

Crystal structure and Hirshfeld surface analysis of 10-([2,3′-bi­thio­phen]-5′-yl)-5,5-di­fluoro-5H-4λ4,5λ4-di­pyrrolo­[1,2-c:2′,1′-f][1,3,2]di­aza­borinine

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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, Khirdalan, Absheron AZ0101, Azerbaijan
*Correspondence e-mail: [email protected]

Edited by C. Schulzke, Universität Greifswald, Germany (Received 28 May 2026; accepted 21 June 2026; online 26 June 2026)

In the title compound, C17H11BF2N2S2, the mol­ecular conformation is consolidated by an intra­molecular C—H⋯S inter­action forming an S(6) ring. In the crystal, mol­ecules are linked by C—H⋯F inter­actions, forming a three-dimensional network. The terminal thio­phene ring is disordered in a 0.659 (3):0.341 (3) ratio around the C—C bond that connects the thio­phene rings, with a rotation of approximately 180° around the ring. According to a Hirshfeld surface analysis, H⋯H (34.8%), C⋯H/H⋯C (22.1%) and F⋯H/H⋯F (18.6%) inter­actions are the main contributors to the crystal packing.

1. Chemical context

BODIPY, 4,4-di­fluoro-4-bora-3a,4a-di­aza-s-indacene, and its derivatives are well known for their properties as fluoro­phores. First synthesized in 1968, whereas the core scaffold was isolated and described only in 2009, these compounds represent a prominent class of functional compounds with favorable photophysical properties, including a large molar absorption coefficient, narrow absorption and emission bands, high fluorescence quantum yield, and excellent photochemical stability (Treibs & Kreuzer, 1968View full citation; Schmitt et al., 2009View full citation; Yadav & Misra, 2023View full citation). Owing to these characteristics, they have found widespread applications as fluorescent probes, in cell imaging, as organic light-emitting diodes (OLEDs), dye-sensitized solar cells (DSCs) and in phototherapy (Gai et al., 2023View full citation; Gawale et al., 2024View full citation; Mao et al., 2023View full citation). In particular, BODIPYs have been shown to be promising photosensitizers for photodynamic therapy (PDT), despite certain drawbacks such as absorption at wavelengths below 600 nm, hydro­phobicity, and poor tissue penetration (Zhang et al., 2021View full citation). The structural versatility of BODIPYs, including modifications at specific positions of the core, enables fine-tuning of their chemical and photophysical properties (e.g., singlet-oxygen generation, emission wavelength, and fluorescence efficiency), thereby enhancing their photodynamic efficacy, biocompatibility, and overall role in imaging and therapeutic applications in PDT (Prieto-Montero et al., 2020View full citation; Malacarne et al., 2022View full citation). Thus, the photophysical behavior of BODIPY may be governed by the substituent at the meso-position, yet replacing the typical six-membered aryl ring with five-membered heterocycles (e.g., furan, thio­phene, pyrrole, seleno­phene) has received limited attention. For example, the insertion of a thio­phene ring into this position, followed by modification with a nitro­genous base and the creation of a nucleotide based on it, makes it possible to effectively use the resulting BODIPY scaffold as a fluorescent DNA probe to study bacterial metabolism (Šoltysová et al., 2025View full citation). Therefore, studying the introduction of various heterocycles, especially thio­phene derivatives, into the meso-position remains relevant. Herein, we report the synthesis of a BODIPY derivative functionalized with a thio­phene ring at the meso-position to investigate its influence on the structural, electronic, and photophysical properties of the resultant fluoro­phore. Previously, we described a two-stage method for obtaining BODIPY-type structures, where various heterocyclic aldehydes were utilized as starting compounds (Sadikhova et al., 2024View full citation; Polianskaia et al., 2026View full citation). This strategy was also applied in this study: [2,3′-bi­thio­phene]-5′-carbaldehyde was taken as the starting mol­ecule and introduced into a condensation reaction with pyrrole under acid catalysis in inert atmosphere. The resulting inter­mediate dipyrrolmethane 1 was then oxidized with DDQ in CH2Cl2 (30 min), followed by neutralization with DIPEA and subsequent treatment with BF3·OEt2, providing the corresponding BODIPY complex. The target meso-thienyl-substituted BODIPY 2 was isolated in 58% yield after silica gel column chromatography.

[Scheme 1]

2. Structural commentary

The mean plane of the twelve-membered ring system (C1–C9/N1/B1/N2 with an r.m.s. deviation of fitted atoms of 0.0819 Å) makes a dihedral angle of 37.3 (1)°, with the thio­phene ring (S1/C10–C13), while the angles subtended the major and minor components (S2/C14–C17 and S2′/C14/C15′–C17′) of the terminal thio­phene ring and the twelve-membered ring system are 50.9 (3) and 48.8 (6)°, respectively (Fig. 1[link]). The mol­ecular conformation is consolidated by an intra­molecular C7—H7⋯S1 hydrogen bond, forming an S(6) motif (Fig. 1[link], Table 1[link]; Bernstein et al., 1995View full citation). The BODIPY torsion angles F1—B1—N1—C4 and F2—B1—N2—C6 are −103.5 (2) and −135.5 (2)°, respectively. All geometric parameters are normal and consistent with those of related compounds discussed in the Database survey.

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C3—H3⋯F2i 0.95 2.55 3.362 (2) 144
C7—H7⋯S1 0.95 2.68 3.1895 (19) 114
C8—H8⋯F1ii 0.95 2.43 3.229 (2) 142
C11—H11⋯F1iii 0.95 2.54 3.4360 (19) 156
C15—H15⋯F1iii 0.95 2.49 3.426 (13) 168
C17—H17⋯F1iv 0.95 2.38 3.255 (11) 153
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 1]
Figure 1
Mol­ecular structure of 2 showing the atomic labelling. Displacement ellipsoids are drawn at the 50% probability level. The intra­molecular hydrogen bond is shown as a dashed line.

3. Supra­molecular features and Hirshfeld surface analysis

In the crystal, mol­ecules are linked by C—H⋯F inter­actions, forming a three-dimensional framework (Table 1[link]). A detailed overview of the C—H⋯F inter­actions within the unit cell is given in Fig. 2[link]. Crystal packing views along the a and c axes are shown in Figs. 3[link] and 4[link], respectively. C—H⋯π and π-π inter­actions are not observed.

[Figure 2]
Figure 2
A general view of the C—H⋯F inter­actions (dashed lines) in the unit cell. For symmetry codes, see Table 1.[link].
[Figure 3]
Figure 3
Crystal packing viewed along the a axis showing the C—H⋯F inter­actions (dashed lines). H atoms not involved in hydrogen bonding are omitted.
[Figure 4]
Figure 4
Crystal packing viewed along the c axis.

The Hirshfeld surface and associated two-dimensional fingerprint plots for the title compound were calculated employing established procedures in CrystalExplorer17.5 (Spackman et al., 2021View full citation) to determine the influence of weak inter­molecular inter­actions on the mol­ecular packing. The Hirshfeld surfaces mapped over dnorm using a fixed colour scale of −0.24 (red) to 1.22 (blue) a.u. are shown in Fig. 5[link]. The few red spots indicate inter­molecular contacts involved in inter­actions (Tables 1[link] and 2[link]).

Table 2
Summary of short inter­atomic contacts (Å)

Contact Distance Symmetry operation
H7⋯H16Aa 2.57 1 − x, Mathematical equation + y, 2 − z
F1⋯H15a 2.49 1 − x, −Mathematical equation + y, 1 − z
S2a⋯H1 3.18 x, y, 1 + z
F1⋯*H17 2.38 −1 + x, y, −1 + z
F1⋯H8 2.43 x, −Mathematical equation + y, 1 − z
H2⋯H9 2.56 1 + x, y, z
Note: (a) Atom of the minor occupancy disorder component.
[Figure 5]
Figure 5
Three-dimensional Hirshfeld surface mapped over dnorm.

Fig. 6[link] shows the full two-dimensional fingerprint plot and those delineated into H⋯H (34.8%), C⋯H/H⋯C (22.1%) and F⋯H/H⋯F (18.6%) contacts. The most important inter­action is H⋯H, contributing 34.8% to the overall crystal packing, which is reflected in Fig. 6[link]b as widely scattered points of high density due to the large hydrogen content of the mol­ecule, with small split tips at dedi = 1.25 Å. The pair of characteristic wings in the fingerprint plot arising from C⋯H/H⋯C contacts, Fig. 7c, has a 22.1% contribution to the Hirshfeld surface with the tips at de + di = 2.70 Å. The F⋯H/H⋯F inter­actions have a 18.6% contribution to the Hirshfeld surface with a pair of sharp spikes characteristic of quite strong inter­actions and de + di ≃ 2.25 Å (Fig. 6[link]d). Other contacts with smaller contributions to the Hirshfeld surface have a less significant effect on the crystal packing: S⋯H/H⋯S (7.1%), C⋯C (6.9%), S⋯C/C⋯S (3.5%), N⋯H/H⋯N (3.3%), F⋯C/C⋯F (2.3%), N⋯C/C⋯N (0.9%), S⋯S (0.3%) and F⋯S/S⋯F (0.2%).

[Figure 6]
Figure 6
The two-dimensional fingerprint plots showing (a) all inter­actions, and those delineated into (b) H⋯H, (c) C⋯H/H⋯C and (d) F⋯H/H⋯F 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, updated April 2025; Groom et al., 2016View full citation) for a thio­phene-substituted BODIPY revealed five compounds: CSD refcodes DICJOP (Choi et al., 2007View full citation), IQOTAM (Ordóñez-Hernández et al., 2021View full citation), ROHXEV (Farfán–Paredes et al., 2023View full citation), XAHZEO (Xochitiotzi-Flores et al., 2016View full citation), and ZEQKEP (Martínez-Bourget et al., 2022View full citation); when substitutions on pyrrole were allowed, thirty-four compounds were found (Fig. 7[link]).

[Figure 7]
Figure 7
Chemical formulae of compounds DICJOP, IQOTAM, ROHXEV, XAHZEO and ZEQKEP.

DICJOP crystallizes in the ortho­rhom­bic P212121 space group. IQOTAM and ZEQKEP crystallize in the monoclinic space group P21, while ROHXEV and XAHZEO crystallize in the triclinic PMathematical equation space group.

In DICJOP, C—H⋯F inter­actions link mol­ecules to form layers parallel to the ac plane (010) with an R44(26) motif protruding along the crystallographic c axis and an R22(14) motif expanding the layer into the a direction. In IQOTAM, there are two independent mol­ecules in the asymmetric unit, which are inversion conformers. They form an extensive three-dimensional network with C—H⋯F plus C—H⋯O, C—H⋯S, C—H⋯. and ππ inter­actions. In ROHXEV, the mol­ecules are linked along the a-axis direction by C—H⋯F inter­actions, forming C(8) zigzag chains. These chains are extended into ribbons by bidirectional C—H⋯F hydrogen bonds forming R22(10) motifs. The chains are linked along the b-axis direction by what may be considered weak C—H⋯π inter­actions, forming layers parallel to the ab plane. In XAHZEO, a bidirectional C—H⋯F hydrogen-bonding inter­action of one fluorine with one adjacent mol­ecule forms an R22(10) ring motif. The second F atom of the BODIPY moiety forms the same hydrogen-bonding motif to the next mol­ecule in the a-axis direction. The inter­actions therefore result in broad ribbons extending along the a-axis direction. The ribbons are linked by C—H⋯O bonds involving an aldehyde function to form layers in the (012) plane. In ZEQKEP, C—H⋯F inter­actions form chains along the ac diagonal. C—H⋯O bonds running parallel to the crystallographic b axis link the ribbons into zigzag layers somewhat coplanar with the (401) plane.

In conclusion, the observation of C—H⋯F inter­actions in all of these structures suggests that this inter­action may be generally important in mol­ecular packaging regulation, in particular, for BODIPY derivatives.

5. Synthesis and crystallization

The BODIPY synthesis procedure was reported previously (Sadikhova et al., 2024View full citation; Polianskaia et al., 2026View full citation). The starting [2,3′-bi­thio­phene]-5′-carbaldehyde (0.45 g, 2.00 mmol) and pyrrole (3.89 g, 58.00 mmol) were placed into a two-neck flask. The reaction mixture was purged with argon for 10 min. Tri­fluoro­acetic acid (TFA, 26.0 mg, 0.20 mmol) was added dropwise to the reaction under stirring at r.t. After that, the reaction mixture was stirred for an hour under argon. Then Et3N (50 µL) was added to pH ∼7. The reaction mixture was poured into water (50 mL) and extracted with ethyl acetate (3 × 10 mL). The target product was purified by column chromatography (eluent: hepta­ne–ethyl acetate 10:1, TLC: hepta­ne/ethyl acetate 4:1); greyish green powdery crystals, yield 89%, 550 mg (1.77 mmol). 1H NMR (700.2 MHz, CDCl3) (J, Hz): δ 8.06 (br.s, 2H, NH), 7.27 (d, J = 1.4 Hz, 1 H, H-2′ Thien), 7.19 (dd, J = 5.0, 0.9 Hz, 1 H, H-5 Thien), 7.14 (dd, J = 3.6, 0.9 Hz, 1 H, H-3 Thien), 7.13 (br.s, 1 H, H-4′ Thien), 7.02 (dd, J = 5.0, 3.6 Hz, 1 H, H-4 Thien), 6.75–6.73 (m, 2 H, H-5,5′ Pyr), 6.19 (m, 2 H, H-4,4′ Pyr), 6.10 (br.s, 2 H, H-3,3′ Pyr), 5.75 (s, 1 H, CH). 13C NMR (176.1 MHz, CDCl3): δ 146.8, 139.1, 135.2, 131.5 (2 C), 127.6, 124.6, 123.8, 123.1, 118.7, 117.6 (2 C), 108.6 (2 C), 107.2 (2 C), 39.3. Dipyrrolmethane 1 (542 mg, 1.7 mmol) was dissolved in dry dichloromethane (DCM, 30 ml), after 2,3-di­chloro-5,6-di­cyano­benzo­quinone (DDQ, 1.21 g, 5.3 mmol) was added; the reaction mixture was stirred for 30 min (TLC control), poured into water (80 mL) and extracted with DCM (3 × 30 mL). The organic layer was dried with anhydrous Na2SO4, concentrated in vacuo and the residue was dissolved in dry DCM (20 ml) without further purification. Boron trifluoride etherate (4.5 ml, 34.9 mmol) and an equal volume of diiso­propyl­ethyl­amine (DIPEA, 4.5 ml) were added. The solution was stirred under room temperature for 1 h (TLC control) and then poured into water (80 mL), extracted with DCM (3 × 30 mL) and washed with saturated Na2CO3 (3 × 30 mL). The organic layer was dried with anhydrous Na2SO4, the target product 2 was purified by column chromatography (eluent: ethyl acetate/hexane 1:10); dark-red crystals, yield 58%, 330 mg (0.92 mmol), m.p. 431–432 K. Single crystals of the title compound were grown using the mixed solvents ethyl acetate–hexane at 281 K. 1H NMR (700.2 MHz, CDCl3) (J, Hz): δ 7.96 (s, 2 H, H-5,5′ Pyr), 7.73 (dd, J = 7.6, 1.4 Hz, 2 H, H-4,4′ Pyr), 7.34–7.28 (m, 4 H, H-2′,3,4′,5 Thien), 7.10 (dd, J = 5.2, 3.6 Hz, 1 H, H-4 Thien), 6.61 (m, 2 H, H-3,3′ Pyr). 13C NMR (176.1 MHz, CDCl3): δ 144.2 (2 C), 138.8, 137.5, 136.8, 135.2, 134.2, 131.4 (2 C), 131.2, 128.0, 125.0 (2 C), 124.9, 124.2, 118.7 (2 C). 19F NMR (658.8 MHz, CDCl3): δ −144.8–−145.5 (m, 2 F). MS (ESI) m/z: [M]+ 356.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 3[link]. All C-bound hydrogen atoms were positioned geometrically (C—H = 0.95 Å) and refined using a riding model, with Uiso(H) = 1.2 Ueq(C). The terminal thio­phene ring (S2/C14–C17) is disordered by a 180° rotation over two orientations around the C12—C14 bond in a 0.659 (3):0.341 (3) ratio. The geometries of the disordered components were restrained to be similar (SAME in SHELXL). The rigid bond and similar displacement parameter restraints (DELU and SIMU, respectively) were applied for the atoms involved. One outlier reflection (001), affected by the incident beam-stop, was omitted in the last cycles of the refinement.

Table 3
Experimental details

Crystal data
Chemical formula C17H11BF2N2S2
Mr 356.21
Crystal system, space group Monoclinic, P21
Temperature (K) 100
a, b, c (Å) 9.4693 (2), 7.2412 (1), 11.2392 (2)
β (°) 95.512 (1)
V3) 767.10 (2)
Z 2
Radiation type Mo Kα
μ (mm−1) 0.37
Crystal size (mm) 0.20 × 0.12 × 0.10
 
Data collection
Diffractometer Bruker D8 QUEST PHOTON-III area detector
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.674, 0.746
No. of measured, independent and observed [I > 2σ(I)] reflections 24975, 5559, 5142
Rint 0.041
(sin θ/λ)max−1) 0.758
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.030, 0.072, 1.03
No. of reflections 5559
No. of parameters 255
No. of restraints 147
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.35, −0.22
Absolute structure Refined as an inversion twin
Absolute structure parameter 0.29 (6)
Computer programs: APEX3 (Bruker, 2013View full citation), SAINT (Bruker, 2018View full citation), SHELXS97 (Sheldrick, 2008View full citation), SHELXL2014 (Sheldrick, 2015View full citation), ORTEP-3 for Windows (Farrugia, 2012View full citation) and PLATON (Spek, 2020View full citation).

Supporting information


Computing details top

10-([2,3'-Bithiophen]-5'-yl)-5,5-difluoro-5H-4λ4,5λ4-dipyrrolo[1,2-c:2',1'-f][1,3,2]diazaborinine top
Crystal data top
C17H11BF2N2S2F(000) = 364
Mr = 356.21Dx = 1.542 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 9.4693 (2) ÅCell parameters from 9989 reflections
b = 7.2412 (1) Åθ = 3.0–32.3°
c = 11.2392 (2) ŵ = 0.37 mm1
β = 95.512 (1)°T = 100 K
V = 767.10 (2) Å3Prism, red
Z = 20.20 × 0.12 × 0.10 mm
Data collection top
Bruker D8 QUEST PHOTON-III area detector
diffractometer
5142 reflections with I > 2σ(I)
Radiation source: fine-focus sealed X-ray tubeRint = 0.041
φ and ω scansθmax = 32.6°, θmin = 2.7°
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
h = 1414
Tmin = 0.674, Tmax = 0.746k = 1010
24975 measured reflectionsl = 1717
5559 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)] = 0.030H-atom parameters constrained
wR(F2) = 0.072 w = 1/[σ2(Fo2) + (0.0365P)2 + 0.1049P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
5559 reflectionsΔρmax = 0.35 e Å3
255 parametersΔρmin = 0.22 e Å3
147 restraintsAbsolute structure: Refined as an inversion twin
Primary atom site location: difference Fourier mapAbsolute structure parameter: 0.29 (6)
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.

Refinement. Refined as a 2-component inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
S10.33169 (4)0.33970 (7)0.83032 (3)0.01449 (9)
C140.71857 (18)0.4686 (3)0.97857 (15)0.0151 (3)
S20.7570 (2)0.3378 (3)1.1014 (2)0.0156 (3)0.659 (3)
C150.8301 (13)0.5897 (19)0.9628 (11)0.027 (2)0.659 (3)
H150.8285880.6734750.8976550.032*0.659 (3)
C160.9441 (13)0.5772 (19)1.0512 (11)0.0196 (13)0.659 (3)
H161.0270200.6514891.0544910.024*0.659 (3)
C170.9198 (11)0.445 (2)1.1313 (11)0.0156 (14)0.659 (3)
H170.9855890.4134501.1974360.019*0.659 (3)
S2'0.8456 (6)0.6140 (8)0.9467 (5)0.0186 (7)0.341 (3)
C15'0.768 (2)0.368 (3)1.0892 (19)0.021 (3)0.341 (3)
H15A0.7140980.2733691.1218880.026*0.341 (3)
C16'0.899 (2)0.425 (4)1.141 (2)0.017 (3)0.341 (3)
H16A0.9444800.3813111.2151290.020*0.341 (3)
C17'0.953 (3)0.551 (4)1.071 (2)0.022 (3)0.341 (3)
H17A1.0445870.6028671.0888250.027*0.341 (3)
F10.21820 (11)0.35646 (18)0.28958 (9)0.0187 (2)
F20.23232 (12)0.66759 (18)0.26818 (11)0.0211 (2)
N10.41373 (15)0.5112 (2)0.39744 (12)0.0127 (3)
N20.17288 (15)0.5490 (2)0.45742 (13)0.0138 (3)
C10.52374 (18)0.4979 (3)0.33101 (16)0.0154 (3)
H10.5175540.5108990.2465610.018*
C20.64899 (19)0.4620 (3)0.40412 (16)0.0154 (3)
H20.7414250.4490500.3789630.019*
C30.61206 (17)0.4491 (3)0.52039 (16)0.0138 (3)
H30.6743940.4230980.5897100.017*
C40.46383 (17)0.4819 (2)0.51653 (15)0.0122 (3)
C50.37090 (17)0.4875 (2)0.60681 (15)0.0119 (3)
C60.22474 (18)0.5219 (2)0.57619 (15)0.0131 (3)
C70.11248 (18)0.5563 (3)0.64747 (16)0.0157 (3)
H70.1170530.5480410.7321130.019*
C80.00633 (19)0.6045 (3)0.57061 (18)0.0184 (4)
H80.0978300.6349970.5927170.022*
C90.03554 (19)0.5994 (3)0.45480 (18)0.0178 (4)
H90.0242000.6272990.3843110.021*
C100.42658 (17)0.4603 (2)0.73114 (15)0.0125 (3)
C110.55834 (17)0.5100 (2)0.78462 (15)0.0128 (3)
H110.6248070.5805310.7455890.015*
C120.58456 (18)0.4450 (2)0.90406 (15)0.0135 (3)
C130.46880 (17)0.3523 (3)0.93995 (14)0.0154 (3)
H130.4657550.3010061.0174510.018*
B10.2566 (2)0.5224 (3)0.34767 (17)0.0146 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.01389 (16)0.01582 (17)0.01392 (16)0.00373 (16)0.00209 (13)0.00032 (17)
C140.0145 (7)0.0175 (8)0.0128 (7)0.0011 (6)0.0000 (6)0.0020 (6)
S20.0171 (5)0.0170 (8)0.0122 (5)0.0015 (5)0.0016 (4)0.0033 (4)
C150.038 (4)0.024 (4)0.018 (3)0.004 (3)0.001 (2)0.006 (2)
C160.020 (3)0.022 (3)0.018 (3)0.002 (2)0.005 (2)0.004 (2)
C170.012 (3)0.022 (4)0.012 (3)0.0026 (19)0.002 (2)0.001 (2)
S2'0.0174 (9)0.0240 (15)0.0129 (13)0.0027 (8)0.0057 (9)0.0055 (10)
C15'0.023 (4)0.021 (7)0.021 (6)0.006 (4)0.009 (3)0.002 (4)
C16'0.020 (6)0.018 (5)0.012 (4)0.001 (4)0.006 (4)0.006 (3)
C17'0.018 (4)0.028 (8)0.019 (7)0.000 (4)0.005 (4)0.004 (4)
F10.0164 (4)0.0208 (5)0.0188 (5)0.0043 (5)0.0012 (4)0.0067 (5)
F20.0189 (5)0.0240 (6)0.0193 (5)0.0007 (4)0.0029 (4)0.0068 (4)
N10.0118 (6)0.0140 (6)0.0121 (6)0.0017 (5)0.0010 (5)0.0003 (5)
N20.0108 (6)0.0146 (6)0.0156 (6)0.0000 (5)0.0008 (5)0.0015 (5)
C10.0151 (7)0.0169 (8)0.0143 (7)0.0023 (6)0.0026 (6)0.0005 (6)
C20.0132 (7)0.0167 (8)0.0168 (7)0.0007 (6)0.0040 (6)0.0003 (6)
C30.0116 (7)0.0137 (7)0.0161 (7)0.0001 (6)0.0010 (6)0.0006 (6)
C40.0109 (6)0.0134 (7)0.0121 (7)0.0005 (6)0.0006 (5)0.0003 (6)
C50.0116 (6)0.0102 (7)0.0135 (7)0.0010 (5)0.0004 (5)0.0013 (5)
C60.0112 (6)0.0137 (7)0.0143 (7)0.0005 (6)0.0011 (5)0.0027 (6)
C70.0128 (7)0.0166 (8)0.0178 (7)0.0012 (6)0.0023 (6)0.0043 (6)
C80.0113 (7)0.0191 (8)0.0246 (9)0.0011 (6)0.0016 (7)0.0057 (7)
C90.0116 (7)0.0180 (8)0.0231 (9)0.0013 (6)0.0025 (7)0.0028 (7)
C100.0132 (7)0.0122 (7)0.0124 (7)0.0013 (6)0.0026 (5)0.0001 (6)
C110.0126 (7)0.0129 (7)0.0130 (7)0.0010 (6)0.0018 (5)0.0006 (6)
C120.0138 (7)0.0145 (7)0.0122 (7)0.0007 (6)0.0011 (6)0.0007 (6)
C130.0164 (7)0.0165 (7)0.0133 (6)0.0017 (7)0.0010 (5)0.0001 (7)
B10.0134 (8)0.0158 (8)0.0142 (8)0.0018 (7)0.0008 (6)0.0006 (7)
Geometric parameters (Å, º) top
S1—C131.7043 (17)N2—C91.348 (2)
S1—C101.7334 (17)N2—C61.391 (2)
C14—C151.397 (10)N2—B11.541 (2)
C14—C121.462 (2)C1—C21.401 (2)
C14—C15'1.476 (18)C1—H10.9500
C14—S2'1.664 (5)C2—C31.388 (2)
C14—S21.685 (3)C2—H20.9500
S2—C171.729 (9)C3—C41.420 (2)
C15—C161.398 (15)C3—H30.9500
C15—H150.9500C4—C51.406 (2)
C16—C171.350 (9)C5—C61.416 (2)
C16—H160.9500C5—C101.459 (2)
C17—H170.9500C6—C71.413 (2)
S2'—C17'1.705 (18)C7—C81.395 (3)
C15'—C16'1.39 (2)C7—H70.9500
C15'—H15A0.9500C8—C91.397 (3)
C16'—C17'1.341 (17)C8—H80.9500
C16'—H16A0.9500C9—H90.9500
C17'—H17A0.9500C10—C111.380 (2)
F1—B11.399 (2)C11—C121.422 (2)
F2—B11.385 (2)C11—H110.9500
N1—C11.342 (2)C12—C131.378 (2)
N1—C41.393 (2)C13—H130.9500
N1—B11.541 (2)
C13—S1—C1091.83 (8)C2—C3—C4107.31 (15)
C15—C14—C12128.8 (5)C2—C3—H3126.3
C12—C14—C15'127.7 (7)C4—C3—H3126.3
C12—C14—S2'123.8 (2)N1—C4—C5120.68 (14)
C15'—C14—S2'108.4 (7)N1—C4—C3107.41 (14)
C15—C14—S2110.5 (5)C5—C4—C3131.91 (15)
C12—C14—S2120.73 (15)C4—C5—C6119.64 (15)
C14—S2—C1791.5 (4)C4—C5—C10119.58 (14)
C14—C15—C16114.2 (9)C6—C5—C10120.77 (15)
C14—C15—H15122.9N2—C6—C7107.68 (15)
C16—C15—H15122.9N2—C6—C5120.32 (15)
C17—C16—C15110.6 (11)C7—C6—C5131.62 (16)
C17—C16—H16124.7C8—C7—C6107.38 (16)
C15—C16—H16124.7C8—C7—H7126.3
C16—C17—S2113.2 (9)C6—C7—H7126.3
C16—C17—H17123.4C7—C8—C9106.62 (16)
S2—C17—H17123.4C7—C8—H8126.7
C14—S2'—C17'92.4 (8)C9—C8—H8126.7
C16'—C15'—C14114.1 (15)N2—C9—C8110.27 (17)
C16'—C15'—H15A122.9N2—C9—H9124.9
C14—C15'—H15A122.9C8—C9—H9124.9
C17'—C16'—C15'109 (2)C11—C10—C5127.63 (15)
C17'—C16'—H16A125.5C11—C10—S1110.75 (13)
C15'—C16'—H16A125.5C5—C10—S1121.47 (12)
C16'—C17'—S2'116 (2)C10—C11—C12113.17 (15)
C16'—C17'—H17A122.1C10—C11—H11123.4
S2'—C17'—H17A122.1C12—C11—H11123.4
C1—N1—C4108.23 (14)C13—C12—C11111.46 (15)
C1—N1—B1125.17 (14)C13—C12—C14124.08 (16)
C4—N1—B1125.80 (14)C11—C12—C14124.43 (16)
C9—N2—C6108.06 (15)C12—C13—S1112.74 (13)
C9—N2—B1125.85 (15)C12—C13—H13123.6
C6—N2—B1126.08 (14)S1—C13—H13123.6
N1—C1—C2110.22 (15)F2—B1—F1109.36 (15)
N1—C1—H1124.9F2—B1—N1111.66 (15)
C2—C1—H1124.9F1—B1—N1108.84 (15)
C3—C2—C1106.81 (15)F2—B1—N2110.79 (15)
C3—C2—H2126.6F1—B1—N2110.52 (15)
C1—C2—H2126.6N1—B1—N2105.61 (14)
C15—C14—S2—C170.2 (9)C6—C7—C8—C90.2 (2)
C12—C14—S2—C17179.4 (6)C6—N2—C9—C80.6 (2)
C12—C14—C15—C16180.0 (9)B1—N2—C9—C8178.19 (17)
S2—C14—C15—C160.9 (14)C7—C8—C9—N20.5 (2)
C14—C15—C16—C171.4 (19)C4—C5—C10—C1132.3 (3)
C15—C16—C17—S21.2 (18)C6—C5—C10—C11146.84 (18)
C14—S2—C17—C160.6 (13)C4—C5—C10—S1142.80 (14)
C12—C14—S2'—C17'179.3 (12)C6—C5—C10—S138.0 (2)
C15'—C14—S2'—C17'1.2 (17)C13—S1—C10—C111.23 (14)
C12—C14—C15'—C16'178.6 (19)C13—S1—C10—C5174.63 (15)
S2'—C14—C15'—C16'3 (3)C5—C10—C11—C12173.38 (17)
C14—C15'—C16'—C17'4 (4)S1—C10—C11—C122.2 (2)
C15'—C16'—C17'—S2'3 (4)C10—C11—C12—C132.2 (2)
C14—S2'—C17'—C16'1 (3)C10—C11—C12—C14176.20 (16)
C4—N1—C1—C20.7 (2)C15—C14—C12—C13165.1 (8)
B1—N1—C1—C2170.93 (16)C15'—C14—C12—C1315.0 (14)
N1—C1—C2—C31.3 (2)S2'—C14—C12—C13167.3 (3)
C1—C2—C3—C41.4 (2)S2—C14—C12—C1316.0 (3)
C1—N1—C4—C5179.88 (16)C15—C14—C12—C1116.7 (8)
B1—N1—C4—C59.8 (3)C15'—C14—C12—C11163.2 (14)
C1—N1—C4—C30.1 (2)S2'—C14—C12—C1114.5 (4)
B1—N1—C4—C3169.99 (16)S2—C14—C12—C11162.26 (19)
C2—C3—C4—N10.9 (2)C11—C12—C13—S11.2 (2)
C2—C3—C4—C5179.35 (18)C14—C12—C13—S1177.18 (14)
N1—C4—C5—C60.4 (2)C10—S1—C13—C120.02 (16)
C3—C4—C5—C6179.24 (18)C1—N1—B1—F255.8 (2)
N1—C4—C5—C10178.71 (15)C4—N1—B1—F2135.73 (17)
C3—C4—C5—C101.6 (3)C1—N1—B1—F165.0 (2)
C9—N2—C6—C70.5 (2)C4—N1—B1—F1103.45 (19)
B1—N2—C6—C7178.32 (16)C1—N1—B1—N2176.27 (16)
C9—N2—C6—C5173.11 (16)C4—N1—B1—N215.2 (2)
B1—N2—C6—C58.1 (3)C9—N2—B1—F245.9 (2)
C4—C5—C6—N20.4 (2)C6—N2—B1—F2135.48 (17)
C10—C5—C6—N2179.52 (16)C9—N2—B1—F175.5 (2)
C4—C5—C6—C7171.47 (19)C6—N2—B1—F1103.14 (19)
C10—C5—C6—C77.7 (3)C9—N2—B1—N1166.97 (17)
N2—C6—C7—C80.2 (2)C6—N2—B1—N114.4 (2)
C5—C6—C7—C8172.44 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···F2i0.952.553.362 (2)144
C7—H7···S10.952.683.1895 (19)114
C8—H8···F1ii0.952.433.229 (2)142
C11—H11···F1iii0.952.543.4360 (19)156
C15—H15···F1iii0.952.493.426 (13)168
C17—H17···F1iv0.952.383.255 (11)153
Symmetry codes: (i) x+1, y1/2, z+1; (ii) x, y+1/2, z+1; (iii) x+1, y+1/2, z+1; (iv) x+1, y, z+1.
Summary of short interatomic contacts (Å) top
ContactDistanceSymmetry operation
H7···H16Aa2.571 - x, 1/2 + y, 2 - z
F1···H15a2.491 - x, -1/2 + y, 1 - z
S2a···H13.18x, y, 1 + z
F1···*H172.38-1 + x, y, -1 + z
F1···H82.43-x, -1/2 + y, 1 - z
H2···H92.561 + x, y, z
Note: (a) Atom of the minor occupancy disorder component.
 

Acknowledgements

The authors' contributions are as follows; conceptualization AVG, MA and GMM; synthesis, DKP and ZAP; X-ray analysis VNK; founding KAA; writing (review and editing of the manuscript) KAA and MA; supervision AVG, MA and GMM.

Funding information

This publication was supported by the RUDN University (project within the framework of the competition for grant funding of young scientists ‘Joint start: Making science together') as well as by the Azerbaijan Medical University and Baku Engineering University.

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