research communications
accessCrystal structure of racemic chloramphenicol
aInstitute of Bioorganic Chemistry, Academy of Sciences of Uzbekistan, Mirzo Ulugbek Str. 83, Tashkent 100125, Uzbekistan, bNational University of Uzbekistan named after Mirzo Ulugbek, 4 University St., Tashkent 100174, Uzbekistan, cHacettepe University, Department of Physics, 06800 Beytepe-Ankara, Türkiye, dDepartment of Chemistry, Bahir Dar University, PO Box 79, Bahir Dar, Ethiopia, eAzerbaijan Medical University, Scientific Research Centre (SRC), A. Kasumzade St. 14, AZ 1022, Baku, Azerbaijan, and fDepartment of Technology of Chemical and Inorganic Substances, Azerbaijan State Oil and Industry University, Azadliq Avenue 34, AZ1010, Baku, Azerbaijan
*Correspondence e-mail: [email protected]
The racemic title compound {systematic name: 2,2-dichloro-N-[(1R,2R)-1,3-dihydroxy-1-(4-nitrophenyl)propan-2-yl]acetamide}, C11H12Cl2N2O5, crystallizes in the space group P1. In the crystal, O—H⋯O, N—H⋯O and C—H⋯O hydrogen bonds link the molecules into a three-dimensional architecture, enclosing R22(14), R22(12), R22(10) and R44(4) loops. The title compound complements the known orthorhombic form of natural (homochiral) chloramphenicol [Acharya et al. (1979
). Acta Cryst. B35, 1360–1363], which crystallizes in space group C2221. The Hirshfeld surface analysis of the crystal structure indicates that the most important contributions for the crystal packing are from H⋯O/O⋯H (39.4%), H⋯H (21.7%), H⋯C/C⋯H (15.5%) and Cl⋯C/C⋯Cl (8.3%) interactions.
Keywords: chloramphenicol; crystal structure; noncovalent interactions.
CCDC reference: 2582935
1. Chemical context
Chloramphenicol, C11H12Cl2N2O5, was originally isolated from the bacteria Streptomyces venezuelae in 1948 and has been used to treat bacterial conjunctivitis, which is a bacterial infection involving the mucous membrane of the surface of the eye (Ehrlich et al., 1947
; Feder et al., 1981
). The crystal structure of natural chloramphenicol has been reported several times in the orthorhombic space group C2221 (Acharya et al., 1979
; Chatterjee et al., 1979
; Dunitz, 1952
; Staples, 2022
; Sundaralingam et al., 1971
). In this work, we report the crystal structure of synthetic (racemic) chloramphenicol (I), and compare it with the natural form.
2. Structural commentary
Compound (I) crystallizes in the centrosymmetric triclinic space group P with one molecule in the asymmetric unit. The molecule consists of p-nitrobenzene, dichloracetyl and 2-amino-propanediol fragments (Fig. 1
), where the dichloracetyl moiety is an aliphatic haloacetyl side-chain and the propanediol moiety possesses two stereogenic carbon atoms (C7 and C8), carrying the hydroxyl group and the amide side chain, respectively. In the arbitrarily chosen asymmetric molecule of (I), C7 and C8 both have R configuration, but crystal symmetry generates a racemic mixture. In natural, chiral, chloramphenicol, the equivalent atoms also have R configurations. In the p-nitrobenzene moiety in (I), the nitro (N1/O1/O2) group is oriented at a dihedral angle of 4.3 (3)° with respect the the C1–C6 benzene ring and atoms N1 and C7 are −0.037 (3) and −0.041 (2) Å away from the benzene ring plane. In the dichloracetyl moiety, atoms Cl3 and Cl4 are −1.3541 (8) and 1.5347 (8) Å, respectively, away from the best plane of the O5/N2/C10/C11 acetyl group (r.m.s. deviation = 0.008 Å). In the 2-amino-propanediol moiety, the dihedral angles between the A (O4/N2/C8/C9) [r.m.s. deviation = 0.013Å], B (N2/C7/C8) and C (O3/C7/C8) fragments are A/B = 56.46 (16)°, A/C = 77.92 (9)° and B/C = 43.64 (18)°. On the other hand, the O3—C7—C8—C9, O3—C7—C8—N2 and O4—C9—C8—N2 torsion angles are −78.3 (2), 43.6 (2) and 177.91 (16)°, respectively. The bond lengths and angles in the title triclinic polymorph are significantly different from the corresponding values in the orthorhombic polymorph of chloramphenicol (Acharya et al., 1979
; Chatterjee et al., 1979
; Dunitz, 1952
)
|
Figure 1
The molecular structure of (I) showing 50% probability ellipsoids. |
3. Supramolecular features
In the extended structure of (I), O—H⋯O and N—H⋯O hydrogen bonds (Table 1
) link the molecules, enclosing
R22(12),
R22(14) and
R44(4) ring motifs, into a three-dimensional network (Figs. 2
and 3
). The packing is consolidated by C—H⋯O hydrogen bonds and aromatic π–π stacking interactions between the benzene rings with centroid- to-centroid distance of 3.7524 (13) Å (slippage = 1.330 Å). Unlike the intramolecular O—H⋯O hydrogen bond in natural chloramphenicol (Staples, 2022
; CSD refcode CLMPCL04), in (I), both –OH groups participate in intermolecular O—H⋯O interactions with O⋯O contact distances of 2.706 (2) Å and 2.780 (2) Å (Table 1
).
|
|
Figure 2
A partial packing diagram of (I) showing the intermolecular N—H⋯O and O—H⋯O hydrogen bonds as dashed lines. |
|
Figure 3
A partial packing diagram of (I) showing C—H⋯O hydrogen bonds as dashed lines. |
The intermolecular interactions in the crystal of (I) were visualized by carrying out a Hirshfeld surface (HS) analysis using CrystalExplorer 17.5 (Spackman et al., 2021
). The red spots (Fig. 4
) indicate their roles as the respective donors and/or acceptors atoms in hydrogen bonding, as discussed above. The overall two-dimensional fingerprint plot is shown in Fig. 5
a and those delineated into different contact types in Fig. 5
b–n. According to these data, the H⋯O/O⋯H, H⋯H, H⋯C/C⋯H and C⋯Cl/Cl⋯Cl contacts make the most significant contributions to the HS, at 39.4%, 21.7%, 15.5% and 8.3%, respectively (Fig. 7).
|
Figure 4
View of the three-dimensional Hirshfeld surface for (I) plotted over dnorm in the range from −0.67 to 1.50 a.u. |
|
Figure 5
The two-dimensional fingerprint plots for (I), showing (a) all interactions, and delineated into different contact types (b)–(n). The di and de values are the closest internal and external distances (in Å) from given points on the Hirshfeld surface. |
The volume of the crystal voids (see figure in the supporting information) and the percentage of free space in the unit cell of (I) are 115.2 Å3 and 16.3%, respectively. These values compare with 324.1 Å3 and 11.9%, respectively in CLMPCL04, which suggests that the homochiral molecules in CLMPCL04 pack more effectively in space group C2221 than do the racemic molecules in space group P in (I). This is supported by the difference in unit-cell volumes [707.30 (3) Å3 for (I) (Z = 2) and 2733.30 (6) Å3 for CLMPCL04 (Z = 8)], although it should be noted that the intensity data for (I) were collected at 292 K and those for CLMPCL04 at 100 K.
For further computational chemistry results (electrostatic potential, shape-index, void volume figures, interaction energies), see the supporting information.
4. Database survey
A survey of the Cambridge Structural Database (CSD, July 2025 update; Groom et al., 2016
) revealed six structures of natural chloramphenicol: CSD refcode CLMPCL (Sundaralingam et al., 1971
), CLMPCL01 (Acharya et al., 1979
), CLMPCL02 (Chatterjee et al., 1979
), CLMPCL03 (Dunitz, 1952
), CLMPCL04 (Staples, 2022
) and EJILUH (Ma et al., 2020
). The first five crystallize in space group C2221 with a ≃ 7.34, b ≃ 17.34, c ≃ 21.49 Å (or equivalent setting of the unit cell) and the final structure is a clathrate.
5. Synthesis and crystallization
A commercial sample of chloramphenicol was recrystallised by slow evaporation of an ethanol–water (1:1 v/v) solution at room temperature.
6. Refinement
Crystal data, data collection and structure refinement details are summarized in Table 2
. The NH hydrogen atom was located from a difference Fourier map and refined isotropically. The O- and C-bound hydrogen-atom positions were calculated geometrically at distances of 0.82 Å (for OH), 0.93–0.98 Å (for CH), and refined using a riding model with the constraint of Uiso = k × Ueq (C, O), where k = 1.5 for OH hydrogen atoms and k = 1.2 for other hydrogen atoms.
|
Supporting information
CCDC reference: 2582935
Crystal structure: contains datablocks I, global. DOI: https://doi.org/10.1107/S2056989026008765/hb8237sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989026008765/hb8237Isup2.hkl
Electrostatic potential. DOI: https://doi.org/10.1107/S2056989026008765/hb8237sup3.docx
Shape index. DOI: https://doi.org/10.1107/S2056989026008765/hb8237sup4.docx
Void volume. DOI: https://doi.org/10.1107/S2056989026008765/hb8237sup5.docx
Energy framework. DOI: https://doi.org/10.1107/S2056989026008765/hb8237sup6.docx
Supporting information file. DOI: https://doi.org/10.1107/S2056989026008765/hb8237Isup7.cml
| C11H12Cl2N2O5 | Z = 2 |
| Mr = 323.13 | F(000) = 332 |
| Triclinic, P1 | Dx = 1.517 Mg m−3 |
| a = 8.0656 (2) Å | Cu Kα radiation, λ = 1.54184 Å |
| b = 8.9248 (2) Å | Cell parameters from 4694 reflections |
| c = 11.0003 (2) Å | θ = 4.3–71.5° |
| α = 97.522 (2)° | µ = 4.34 mm−1 |
| β = 105.938 (2)° | T = 292 K |
| γ = 107.280 (2)° | Block, colourless |
| V = 707.30 (3) Å3 | 0.3 × 0.24 × 0.15 mm |
| XtaLAB Synergy, Single source at home/near, HyPix3000 diffractometer | 2718 independent reflections |
| Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source | 2507 reflections with I > 2σ(I) |
| Mirror monochromator | Rint = 0.034 |
| Detector resolution: 10.0000 pixels mm-1 | θmax = 71.4°, θmin = 4.3° |
| ω scans | h = −9→8 |
| Absorption correction: multi-scan ((CrysAlisPro; Rigaku OD, 2023) | k = −10→10 |
| Tmin = 0.656, Tmax = 1.000 | l = −10→13 |
| 5967 measured reflections |
| Refinement on F2 | Hydrogen site location: mixed |
| Least-squares matrix: full | H atoms treated by a mixture of independent and constrained refinement |
| R[F2 > 2σ(F2)] = 0.052 | w = 1/[σ2(Fo2) + (0.0747P)2 + 0.5048P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.141 | (Δ/σ)max < 0.001 |
| S = 1.05 | Δρmax = 0.59 e Å−3 |
| 2718 reflections | Δρmin = −0.68 e Å−3 |
| 188 parameters | Extinction correction: SHELXL-2016/6 (Sheldrick 2016), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| 0 restraints | Extinction coefficient: 0.0140 (14) |
| Primary atom site location: dual |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
| x | y | z | Uiso*/Ueq | ||
| Cl3 | 0.47682 (11) | 0.44633 (10) | 0.32614 (7) | 0.0589 (3) | |
| Cl4 | 0.19337 (11) | 0.49969 (11) | 0.12769 (7) | 0.0643 (3) | |
| O4 | −0.1306 (2) | 0.79888 (19) | 0.50133 (18) | 0.0361 (4) | |
| H4 | −0.151263 | 0.726781 | 0.540228 | 0.054* | |
| O3 | 0.3697 (2) | 1.04729 (17) | 0.57744 (15) | 0.0286 (4) | |
| H3 | 0.302019 | 1.094821 | 0.545594 | 0.043* | |
| O5 | 0.1354 (2) | 0.46694 (18) | 0.39138 (18) | 0.0389 (4) | |
| O1 | 0.8908 (3) | 0.8840 (4) | 1.1205 (2) | 0.0880 (10) | |
| O2 | 0.6514 (4) | 0.7306 (4) | 1.1442 (2) | 0.0762 (8) | |
| N1 | 0.7258 (3) | 0.8144 (3) | 1.0840 (2) | 0.0472 (6) | |
| N2 | 0.2773 (2) | 0.7375 (2) | 0.44290 (17) | 0.0247 (4) | |
| H2 | 0.355 (4) | 0.814 (3) | 0.430 (2) | 0.026 (6)* | |
| C11 | 0.3536 (3) | 0.5760 (3) | 0.2873 (2) | 0.0335 (5) | |
| H11 | 0.439319 | 0.683345 | 0.294084 | 0.040* | |
| C10 | 0.2461 (3) | 0.5879 (2) | 0.3806 (2) | 0.0272 (4) | |
| C8 | 0.1641 (3) | 0.7676 (2) | 0.51967 (19) | 0.0230 (4) | |
| H8 | 0.131957 | 0.677095 | 0.560800 | 0.028* | |
| C2 | 0.5884 (3) | 0.9648 (3) | 0.7853 (2) | 0.0345 (5) | |
| H2A | 0.643424 | 1.030383 | 0.737875 | 0.041* | |
| C7 | 0.2722 (3) | 0.9228 (2) | 0.6273 (2) | 0.0243 (4) | |
| H7 | 0.182310 | 0.958821 | 0.655455 | 0.029* | |
| C4 | 0.6133 (3) | 0.8411 (3) | 0.9648 (2) | 0.0349 (5) | |
| C9 | −0.0134 (3) | 0.7752 (3) | 0.4297 (2) | 0.0305 (5) | |
| H9A | 0.015934 | 0.863249 | 0.386989 | 0.037* | |
| H9B | −0.076981 | 0.675638 | 0.363211 | 0.037* | |
| C5 | 0.4241 (3) | 0.7678 (3) | 0.9267 (2) | 0.0377 (5) | |
| H5 | 0.369825 | 0.701347 | 0.973919 | 0.045* | |
| C6 | 0.3185 (3) | 0.7963 (3) | 0.8166 (2) | 0.0348 (5) | |
| H6 | 0.191082 | 0.748704 | 0.789635 | 0.042* | |
| C1 | 0.3986 (3) | 0.8948 (2) | 0.7449 (2) | 0.0267 (4) | |
| C3 | 0.6970 (3) | 0.9380 (3) | 0.8960 (2) | 0.0399 (6) | |
| H3A | 0.824555 | 0.984839 | 0.923189 | 0.048* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cl3 | 0.0632 (5) | 0.0683 (5) | 0.0572 (5) | 0.0432 (4) | 0.0213 (4) | 0.0035 (3) |
| Cl4 | 0.0564 (5) | 0.0918 (6) | 0.0335 (4) | 0.0162 (4) | 0.0097 (3) | 0.0113 (3) |
| O4 | 0.0248 (8) | 0.0325 (8) | 0.0591 (11) | 0.0137 (6) | 0.0178 (7) | 0.0201 (7) |
| O3 | 0.0227 (7) | 0.0236 (7) | 0.0407 (8) | 0.0074 (6) | 0.0111 (6) | 0.0115 (6) |
| O5 | 0.0389 (9) | 0.0249 (8) | 0.0556 (11) | 0.0050 (7) | 0.0257 (8) | 0.0110 (7) |
| O1 | 0.0376 (12) | 0.147 (3) | 0.0639 (15) | 0.0123 (14) | −0.0005 (11) | 0.0559 (16) |
| O2 | 0.0597 (14) | 0.118 (2) | 0.0545 (13) | 0.0253 (14) | 0.0152 (11) | 0.0530 (14) |
| N1 | 0.0421 (13) | 0.0662 (15) | 0.0320 (11) | 0.0186 (11) | 0.0086 (9) | 0.0157 (10) |
| N2 | 0.0229 (9) | 0.0217 (8) | 0.0311 (9) | 0.0050 (7) | 0.0134 (7) | 0.0079 (7) |
| C11 | 0.0325 (12) | 0.0288 (11) | 0.0363 (12) | 0.0062 (9) | 0.0148 (9) | 0.0006 (9) |
| C10 | 0.0243 (10) | 0.0244 (10) | 0.0328 (11) | 0.0071 (8) | 0.0099 (8) | 0.0079 (8) |
| C8 | 0.0210 (10) | 0.0214 (9) | 0.0280 (10) | 0.0066 (7) | 0.0102 (8) | 0.0071 (7) |
| C2 | 0.0266 (11) | 0.0386 (12) | 0.0354 (12) | 0.0058 (9) | 0.0099 (9) | 0.0125 (9) |
| C7 | 0.0201 (9) | 0.0242 (9) | 0.0302 (10) | 0.0074 (7) | 0.0115 (8) | 0.0061 (8) |
| C4 | 0.0344 (12) | 0.0445 (13) | 0.0243 (11) | 0.0151 (10) | 0.0069 (9) | 0.0066 (9) |
| C9 | 0.0220 (10) | 0.0312 (11) | 0.0354 (11) | 0.0076 (8) | 0.0064 (9) | 0.0092 (9) |
| C5 | 0.0380 (13) | 0.0455 (13) | 0.0308 (11) | 0.0103 (10) | 0.0160 (10) | 0.0134 (10) |
| C6 | 0.0261 (11) | 0.0439 (13) | 0.0339 (12) | 0.0086 (9) | 0.0123 (9) | 0.0105 (10) |
| C1 | 0.0267 (11) | 0.0266 (10) | 0.0265 (10) | 0.0095 (8) | 0.0098 (8) | 0.0023 (8) |
| C3 | 0.0257 (11) | 0.0493 (14) | 0.0378 (12) | 0.0079 (10) | 0.0052 (9) | 0.0107 (10) |
| Cl3—C11 | 1.758 (2) | C8—C7 | 1.538 (3) |
| Cl4—C11 | 1.771 (2) | C8—C9 | 1.527 (3) |
| O4—H4 | 0.8200 | C2—H2A | 0.9300 |
| O4—C9 | 1.429 (3) | C2—C1 | 1.384 (3) |
| O3—H3 | 0.8200 | C2—C3 | 1.387 (3) |
| O3—C7 | 1.425 (2) | C7—H7 | 0.9800 |
| O5—C10 | 1.223 (3) | C7—C1 | 1.512 (3) |
| O1—N1 | 1.212 (3) | C4—C5 | 1.384 (3) |
| O2—N1 | 1.199 (3) | C4—C3 | 1.371 (4) |
| N1—C4 | 1.469 (3) | C9—H9A | 0.9700 |
| N2—H2 | 0.83 (3) | C9—H9B | 0.9700 |
| N2—C10 | 1.334 (3) | C5—H5 | 0.9300 |
| N2—C8 | 1.459 (3) | C5—C6 | 1.378 (3) |
| C11—H11 | 0.9800 | C6—H6 | 0.9300 |
| C11—C10 | 1.527 (3) | C6—C1 | 1.391 (3) |
| C8—H8 | 0.9800 | C3—H3A | 0.9300 |
| C9—O4—H4 | 109.5 | O3—C7—H7 | 107.4 |
| C7—O3—H3 | 109.5 | O3—C7—C1 | 111.64 (16) |
| O1—N1—C4 | 118.1 (2) | C8—C7—H7 | 107.4 |
| O2—N1—O1 | 122.5 (2) | C1—C7—C8 | 112.27 (16) |
| O2—N1—C4 | 119.3 (2) | C1—C7—H7 | 107.4 |
| C10—N2—H2 | 118.5 (17) | C5—C4—N1 | 118.1 (2) |
| C10—N2—C8 | 120.61 (17) | C3—C4—N1 | 119.7 (2) |
| C8—N2—H2 | 120.5 (17) | C3—C4—C5 | 122.2 (2) |
| Cl3—C11—Cl4 | 110.43 (12) | O4—C9—C8 | 110.65 (18) |
| Cl3—C11—H11 | 109.6 | O4—C9—H9A | 109.5 |
| Cl4—C11—H11 | 109.6 | O4—C9—H9B | 109.5 |
| C10—C11—Cl3 | 109.68 (16) | C8—C9—H9A | 109.5 |
| C10—C11—Cl4 | 107.81 (16) | C8—C9—H9B | 109.5 |
| C10—C11—H11 | 109.6 | H9A—C9—H9B | 108.1 |
| O5—C10—N2 | 124.1 (2) | C4—C5—H5 | 121.0 |
| O5—C10—C11 | 120.72 (19) | C6—C5—C4 | 118.0 (2) |
| N2—C10—C11 | 115.15 (18) | C6—C5—H5 | 121.0 |
| N2—C8—H8 | 108.4 | C5—C6—H6 | 119.3 |
| N2—C8—C7 | 110.40 (16) | C5—C6—C1 | 121.4 (2) |
| N2—C8—C9 | 109.22 (17) | C1—C6—H6 | 119.3 |
| C7—C8—H8 | 108.4 | C2—C1—C7 | 123.15 (19) |
| C9—C8—H8 | 108.4 | C2—C1—C6 | 119.0 (2) |
| C9—C8—C7 | 112.08 (16) | C6—C1—C7 | 117.86 (19) |
| C1—C2—H2A | 119.7 | C2—C3—H3A | 120.6 |
| C1—C2—C3 | 120.5 (2) | C4—C3—C2 | 118.9 (2) |
| C3—C2—H2A | 119.7 | C4—C3—H3A | 120.6 |
| O3—C7—C8 | 110.49 (16) | ||
| Cl3—C11—C10—O5 | −57.1 (3) | C10—N2—C8—C9 | −82.3 (2) |
| Cl3—C11—C10—N2 | 125.53 (18) | C8—N2—C10—O5 | −6.5 (3) |
| Cl4—C11—C10—O5 | 63.2 (3) | C8—N2—C10—C11 | 170.81 (18) |
| Cl4—C11—C10—N2 | −114.18 (18) | C8—C7—C1—C2 | 115.6 (2) |
| O3—C7—C1—C2 | −9.1 (3) | C8—C7—C1—C6 | −65.8 (2) |
| O3—C7—C1—C6 | 169.51 (18) | C7—C8—C9—O4 | −59.4 (2) |
| O1—N1—C4—C5 | −176.9 (3) | C4—C5—C6—C1 | 0.4 (4) |
| O1—N1—C4—C3 | 2.4 (4) | C9—C8—C7—O3 | −78.3 (2) |
| O2—N1—C4—C5 | 0.1 (4) | C9—C8—C7—C1 | 156.31 (17) |
| O2—N1—C4—C3 | 179.4 (3) | C5—C4—C3—C2 | 0.7 (4) |
| N1—C4—C5—C6 | 178.4 (2) | C5—C6—C1—C2 | 0.2 (4) |
| N1—C4—C3—C2 | −178.5 (2) | C5—C6—C1—C7 | −178.5 (2) |
| N2—C8—C7—O3 | 43.6 (2) | C1—C2—C3—C4 | −0.1 (4) |
| N2—C8—C7—C1 | −81.7 (2) | C3—C2—C1—C7 | 178.3 (2) |
| N2—C8—C9—O4 | 177.91 (16) | C3—C2—C1—C6 | −0.4 (4) |
| C10—N2—C8—C7 | 154.03 (18) | C3—C4—C5—C6 | −0.9 (4) |
| D—H···A | D—H | H···A | D···A | D—H···A |
| O4—H4···O5i | 0.82 | 2.00 | 2.780 (2) | 159 |
| O3—H3···O4ii | 0.82 | 1.90 | 2.706 (2) | 170 |
| N2—H2···O3iii | 0.83 (3) | 2.23 (3) | 3.010 (2) | 155 (2) |
| C11—H11···O3iii | 0.98 | 2.42 | 3.302 (3) | 149 |
| C8—H8···O5i | 0.98 | 2.39 | 3.163 (2) | 135 |
| C3—H3A···O1iv | 0.93 | 2.46 | 3.298 (4) | 151 |
| Symmetry codes: (i) −x, −y+1, −z+1; (ii) −x, −y+2, −z+1; (iii) −x+1, −y+2, −z+1; (iv) −x+2, −y+2, −z+2. |
Acknowledgements
The author's contributions are as follows. Conceptualization, TH and ANB; crystallization, OC and JA; X-ray analysis, BT, JA and TH; Hirshfeld surface analysis, TH; writing (review and editing of the manuscript) TH, RSH and KIH; supervision, TH and ANB. This research was conducted at the Laboratory of Complex Compounds, Institute of Bioorganic Chemistry, Academy of Sciences of the Republic of Uzbekistan. It was financially supported by government funding from the Republic of Uzbekistan. This work has been supported by the Azerbaijan Medical University and the Azerbaijan State Oil and Industry University. TH is also grateful to Hacettepe University Scientific Research Project Unit (grant No. 013 D04 602 004).
References
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