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

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COMMUNICATIONS
ISSN: 2056-9890

Different inter­molecular inter­actions in solvated and unsolvated isatin-based di­thio­carbazate imine derivatives

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aEaStCHEM School of Chemistry, University of St Andrews, St Andrews, Fife KY16 9ST, United Kingdom, and bFaculty of Applied Sciences, Universiti Teknologi MARA, 40450 Shah Alam, Selangor, Malaysia
*Correspondence e-mail: [email protected]

Edited by W. T. A. Harrison, University of Aberdeen, United Kingdom (Received 25 November 2025; accepted 5 December 2025; online 1 January 2026)

The syntheses and structures of 2-fluoro­benzyl (Z)-2-(2-oxoindolin-3-yl­idene)hydrazine-1-carbodi­thio­ate dimethyl sulfoxide monosolvate, C16H12FN3OS2·C2H6OS (1) and 2-fluoro­benzyl (Z)-2-(5-bromo-2-oxoindolin-3-yl­idene)hydrazine-1-carbodi­thio­ate, C16H11BrFN3OS2 (2) are reported. Both structures feature a Z-configuration with respect to the C=N bond and the fluoro­benzyl ring is approximately orthogonal to the isatin moiety. For 1, the crystal packing features weak Car—H⋯S (ar = aromatic) hydrogen bonds that link adjacent mol­ecules in a C(10) fashion to form pleated chains propagating along [001] and short S⋯O contacts between dimethyl sulfoxide solvent mol­ecules forming chains along [010]. The N—H hydrogen bond donors in 1 form either intra­molecular or discrete N—H⋯O(DMSO) hydrogen bonds. In 2, alternating R22(8)-type pairwise N—H⋯O hydrogen bonds and short F⋯Br contacts link the mol­ecules into chains propagating along [210]. The later unsolvated structure is of notably poorer quality and exhibits disorder in its o-fluoro­benzyl group, with a 180° flip and a small twist around the S—C bond. These findings are consistent with the results of Hirshfeld surface analyses.

1. Chemical context

The use of solvent mol­ecules in reducing structural disorder is an emerging theme in crystal engineering. Controlled solvation can enhance crystallographic quality and provides a means to fine-tune the chemical and physical properties of solid-state materials, including functional organic frameworks, coordination complexes and pharmaceuticals (for recent reviews, see: Werner & Swift, 2021View full citation; Bolla et al., 2022View full citation). The inclusion of a solvent such as dimethyl sulfoxide (DMSO), in the crystal fills void space, introduces additional hydrogen-bond acceptors, and stabilizes conformations, leading to more rigid and well-defined structural units of crystalline motifs (Klitou et al., 2020View full citation; Li et al., 2021View full citation). For example, our recent crystallographic study on 2-fluoro­benzyl (Z)-2-(5-chloro-2-oxoindolin-3-yl­idene) hydrazine-1-carbodi­thio­ate dimethyl sulfoxide monosolvate highlighted the role of DMSO as a hydrogen bond acceptor by forming discrete directional N—H⋯O(DMSO) contacts and occupying voids in the crystal. The inclusion of the solvate increased packing complementarity, producing a more rigid asymmetric unit and fewer alternative conformers, resulting in a more stable mol­ecular conformation (McKay et al., 2025View full citation).

Isatin-based imines have been widely recognized as versatile scaffolds, displaying a broad range of application domains (Liu et al., 2025View full citation; Tok et al., 2025View full citation; Topkaya et al., 2024View full citation). Their functionalization allows chemists to modulate steric and electronic properties for tuning solid-state architectures, which can exhibit profound implications on physical properties and applications (Wang et al., 2023View full citation; Venugopal & Pansare 2025View full citation).

As part of our ongoing studies of organosulfur imines and their solid-state behaviour, we report here the syntheses, crystal structures and Hirshfeld-surface analyses of 2-fluoro­benzyl (Z)-2-(2-oxoindolin-3-yl­idene)hydrazine-1-carbodi­thio­ate dimethyl sulfoxide monosolvate, C16H12FN3OS2·C2H6OS (1) and 2-fluoro­benzyl (Z)-2-(5-bromo-2-oxoindolin-3-yl­idene)hydrazine-1-carbodi­thio­ate, C16H11BrFN3OS2 (2).

[Scheme 1]

2. Structural commentary

Compound 1 crystallizes in space group P21/c as a dimethyl sulfoxide solvate (Fig. 1[link]), while compound 2 crystallizes in the space group P[\overline{1}], without any solvent of crystallization (Fig. 2[link]). Both compounds display a Z configuration with respect to the C=N bond, resulting in the hydrazine (N4) hydrogen atom being directed towards the isatin (O2) oxygen atom generating an S(6) intra­molecular N—H⋯O hydrogen bond (Tables 1[link] and 2[link]) in the same manner as in previously reported related structures (Abdul Manan et al., 2023View full citation; Abdul Manan et al., 2024aView full citation,bView full citation,cView full citation; McKay et al., 2025View full citation). In both structures, the thione sulfur atom (S10) is orientated syn to the γ-lactam oxygen atom while the S-2-fluoro­benzyl moiety is orientated in the opposite direction. There is a small bow between the methyl­idenehydrazinecarbodi­thio­ate (MHT) and the γ-lactam moieties in both structures [6.70 (8) and 6.5 (3)° for 1 and 2, respectively] while the 2-fluoro­phenyl ring is twisted almost perpendicular to the MHT fragment [90.37 (7) and 72.5 (17)° for 1 and 2, respectively]. In compound 1, the H atom on the γ-lactam nitro­gen atom (N1) forms a discrete N—H⋯O hydrogen bond to the DMSO solvent mol­ecule (Table 1[link]) in the same manner as the previously reported 5-chloro analogue (McKay et al., 2025View full citation).

Table 1
Hydrogen-bond geometry (Å, °) for 1[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O21 0.78 (3) 2.05 (3) 2.820 (3) 174 (3)
N4—H4⋯O2 0.88 (3) 1.99 (3) 2.696 (3) 136 (3)
C7—H7⋯S10i 0.95 2.94 3.860 (3) 163
C21—H21C⋯O2ii 0.98 2.53 3.305 (3) 136
C22—H22C⋯O21iii 0.98 2.48 3.457 (3) 172
Symmetry codes: (i) [x, -y+{\script{3\over 2}}, z+{\script{1\over 2}}]; (ii) [-x+1, y+{\script{1\over 2}}, -z+{\script{1\over 2}}]; (iii) [-x+1, -y+2, -z+1].

Table 2
Hydrogen-bond geometry (Å, °) for (2)[link]

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O2i 0.88 1.96 2.821 (15) 165
N4—H4⋯O2 0.88 2.09 2.777 (16) 134
C11—H11D⋯S10 0.99 2.56 3.221 (14) 124
Symmetry code: (i) [-x+2, -y, -z+1].
[Figure 1]
Figure 1
The mol­ecular structure of 1 with ellipsoids drawn at the 50% probability level. Hydrogen bonds are shown as blue dashed lines.
[Figure 2]
Figure 2
The mol­ecular structure of 2 with ellipsoids drawn at 50% probability and the minor component of disorder omitted for clarity. Hydrogen bonds are shown as blue dashed lines.

3. Supra­molecular features

In the extended structure of 1 the fused benzo-ring of the isatin moiety forms non-classical Car—H⋯S and Car—H⋯F hydrogen bonds to the thione and the fluorine atoms (Table 1[link]). These inter­actions link adjacent mol­ecules in a C(10) fashion (with respect to the C—H⋯S hydrogen bond) to form pleated chains propagating along [001] (Fig. 3[link]). These pleated chains are similar to the pleated sheets reported in methyl (Z)-methyl 2-(−5-methyl-2-oxoindolin-3-yl­idene)hydrazine-1-carbodi­thio­ate (Abdul Manan et al., 2024cView full citation), which are formed by non-classical Car—H⋯S hydrogen bonds between adjacent N—H⋯O hydrogen bonded dimers. The pleated chains in 1 further stack together through both weak ππ stacking (Corne et al., 2016View full citation) from the fused benzo (C4–C9) of the isatin moiety to the C3=N3 bond [centroid⋯centroid separation = 3.302 (3) Å], and additional weaker non-classical Car—H⋯S hydrogen bonds from C16 in the fluoro­benzyl ring to the sulfide group (S11) of an adjacent mol­ecule [H16⋯S11 = 3.0363 (6) Å, C16⋯S11 = 3.770 (3) Å]. This packing motif is supported by chains of chalcogen-bonded DMSO solvent mol­ecules [S21⋯O21 = 3.188 (2) Å compared to a van der Waals separation of 3.32 Å; S21—O21⋯S21 = 169.37 (10)°] along [010], which are hydrogen-bonded to the γ-lactam nitro­gen atoms to form sheets lying in the (100) plane.

[Figure 3]
Figure 3
The packing of 1 into pleated sheets (left to right) through classical and non-classical hydrogen bonds (blue dashed lines) with chalcogen bonded (green dashed lines) DMSO solvent mol­ecules.

In contrast, 2 forms inversion dimers through reciprocal N—H⋯O hydrogen bonds in the typical R22(8) form (Table 2[link]) between adjacent γ-lactam units in the same manner as previously reported related structures (Abdul Manan et al., 2023View full citation, 2024aView full citation,bView full citation,cView full citation). The dimers link together into chains (Fig. 4[link]) propagating along [2[\overline{1}]0] through Br⋯S halogen bonds (Br6⋯S11 = 3.405 (5) Å, C6—Br6⋯S11 = 158.7 (6)°). These chains pack together into sheets in (001) through a combination of edge-to-face stacking between the fused benzo rings (C8) and fluoro­phenyl rings [H8⋯centroid = 3.20 (2) and 3.22 (2) Å, C8⋯centroid 3.91 (3) and 3.98 (3) Å, for the major and minor disordered parts, respectively], ππ stacking between adjacent γ-lactam rings [centroid–centroid separation = 3.467 (13) Å], weaker non-classical Car—H⋯S [H⋯S = 2.956 (4)–3.211 (4) Å, C⋯S = 3.68 (3)–4.01 (4) Å] and Car—H⋯Br [H5⋯Br6 = 3.201 (2) Å; C5⋯Br6 = 4.138 (16) Å] hydrogen bonds, and, depending on the orientation of the o-fluoro­benzyl ring, either very weak Type IV (Saha et al., 2023View full citation) Br⋯F [Br6⋯F13A = 3.35 (3) Å compared to a van der Waals separation of 3.37 Å; C6—Br6⋯F13A = 96.0 (7)°; C13A—F13A⋯Br6 = 104 (2)°] halogen bonds or weak non-classical Car—H⋯F [H17B⋯F13B = 2.65 (2) Å; C17B⋯F13B = 3.26 (4) Å] hydrogen bonds. These sheets assemble into the overall structure through additional weaker Car—H⋯S and Car—H⋯F inter­actions.

[Figure 4]
Figure 4
The packing of 2 into chains through alternating pairwise N—H⋯O hydrogen bonds (blue dashed lines) and S⋯Br halogen bonds (green dashed lines).

4. Hirshfeld surface analysis

Hirshfeld surface analyses of 1 (with the DMSO solvent mol­ecule external to the surface) and 2 (Fig. 5[link]) both show sharp H⋯O and H⋯S contacts (5.9 and 7.5%, and 17.0 and 13.8% of the surfaces, respectively). The H⋯S fingerprints for both structures show broad tails, highlighting the diverse range of H⋯S contacts occurring beyond the discrete C—H⋯S non-classical hydrogen bonds mentioned above. The majority of these contacts are likely electrostatic/van der Waals in character. The fingerprint of H⋯Br contacts in 2 (8.3% of surface) shows a sharp contact which corresponds to a long Car—H⋯Br inter­action [H5⋯Br6 = 3.201 (2) Å] supporting the halogen-bonding inter­action. The surface of 1 shows sharp H⋯F contacts (7.5% of surface) which correspond to a weak Car—H⋯F inter­action [H6⋯F13 = 2.6116 (15) Å; C6⋯F13 = 3.540 (3) Å] between the fused benzo ring of the istan grouping and an adjacent fluoro­benzyl ring while the surface of 2 only shows diffuse H⋯F contacts (4.5% of surface), likely due to the disorder of the fluoro­benzyl group. The surface of 2 also shows sharp S⋯Br contacts (2.9% of surface) consistent with the halogen bonds observed in the structure.

[Figure 5]
Figure 5
Hirshfeld surface fingerprint plots of 1 (left) and 2 (right) with various contacts highlighted.

5. Synthesis and crystallization

The 2-fluoro­benzyl hydrazinecarbodi­thio­ate precursor was synthesized using our previously published methods (McKay et al., 2025View full citation).

To prepare 1, a solution of isatin (1.47 g, 10.0 mmol, 1 eq.) in hot ethanol (40 ml) was added to a solution of the di­thio­carbazate precursor (2.16 g, 10.0 mmol, 1.0 e.q) in hot ethanol (40 ml). The mixture was heated (353 K) with continuous stirring for 15 min and later allowed to cool to room temperature and stand for about 20 min., until a precipitate formed, which was then collected by filtration and dried over silica gel. The crude solid was purified by recrystallization from ethanol solution to yield a yellow solid (yield: 2.87 g, 83%). m.p. 494–495 K; elemental analysis calculated for C16H12FN3OS2: C, 55.63; H, 3.50; N, 12.17%; found: C, 55.63; H, 3.12; N, 11.96%. FT–IR (KBr, ν, cm−1): 3175 (NH), 1688 (C=O); 1613 (C=N); 1079 (C=S); 1143 (N—N); 1H NMR (400 MHz, d6-DMSO) δ: (ppm): 4.56 (s, 2H), 6.94 (d, J = 7.9 Hz, 1H) 7.04–7.08 (m, 1H), 7.17–7.26 (m, 2H), 7.35–7.42 (m, 2H), 7.53–7.58 (m, 2H), 11.38 (s, 1H), 13.97 (s, 1H). Crystals of the DMSO solvate suitable for X-ray diffraction were grown by slow evaporation of a dimethyl sulfoxide solution at room temperature.

Compound 2 was prepared as follows: a solution of 5-bromo­isatin (2.26 g, 10.0 mmol, 1.0 eq.) in hot ethanol (40 ml) was added to a solution of the di­thio­carbazate precursor (2.16 g, 10.0 mmol, 1.0 e.q) in hot ethanol (40 ml). The mixture was heated (353 K with continuous stirring for 15 min and later allowed to cool to room temperature and stand for about 20 min., until a precipitate formed, which was then collected by filteration and dried over silica gel. The crude solid was purified by recrystallization from ethanol solution to give a yellow solid (3.39 g, yield: 80%). m.p 499–500 K. Elemental analysis calculated for C16H11BrFN3OS2: C, 45.29; H, 2.61; N, 9.90%. Found: C, 45.60; H, 2.31; N, 9.74%. FT–IR (KBr, ν, cm−1): 3157 (NH), 1694 (C=O); 1613 (C=N); 1068 (C=S); 1144 (N—N); 1H NMR (400 MHz, d6-DMSO) δ: (ppm): 4.56 (s, 2H), 6.90 (d, J = 8.2 Hz, 1H) 7.18–7.26 (m, 2H), 7.35–7.41 (m, 1H), 7.54–7.59 (m, 2H), 7.64 (d, J = 2.0 Hz, 1H), 11.48 (s, 1H), 13.89 (s, 1H). Crystals suitable for X-ray diffraction were grown by slow evaporation of an ethano­lic solution at room temperature.

6. Refinement

Crystal data, data collection, and structure refinement details are summarized in Table 3[link]. The N-bound H atoms in 1 were located in a difference map and refined isotropically without restraint. The C-bound H atoms, and N-bond H atoms in 2, were located geometrically (phenyl C—H = 0.95 Å, amide/thio­amide N—H = 0.88 Å, methyl­ene C—H = 0.99 Å, methyl C—H = 0.98 Å) and refined as riding atoms. The constraint Uiso(H) = 1.2 Ueq(carrier) or 1.5 Ueq(methyl C) was applied in all cases. Non-merohedral twinning in the structure of 2 with the twin matrix [–1.000 0.000 0.000 / 0.000 1.001 −0.005 / 0.000 0.333 −1.001] was processed using the TwinRotMat routine in PLATON (Spek, 2009View full citation) and refined as a two component twin with component 2 rotated by 0.26° around [061] (reciprocal) or [010] (direct), with a refined twin fraction of 0.417 (6). This structure also showed disorder in its o-fluoro­benzyl group, with a 180° flip and a small (∼8°) twist around the S11—C11 bond. The aromatic ring and fluoro subsitutent was modelled in two parts with geometric and displacement-factor restraints retained on both major and minor parts in a 0.52 (3):0.48 (3) ratio.

Table 3
Experimental details

  1 2
Crystal data
Chemical formula C16H12FN3OS2·C2H6OS C16H11BrFN3OS2
Mr 423.53 424.31
Crystal system, space group Monoclinic, P21/c Triclinic, P[\overline{1}]
Temperature (K) 100 100
a, b, c (Å) 21.6312 (10), 4.6850 (2), 18.9579 (8) 6.6979 (7), 8.0075 (9), 15.880 (2)
α, β, γ (°) 90, 91.519 (4), 90 84.917 (10), 80.544 (10), 89.948 (9)
V3) 1920.58 (14) 836.73 (17)
Z 4 2
Radiation type Mo Kα Cu Kα
μ (mm−1) 0.41 5.86
Crystal size (mm) 0.27 × 0.02 × 0.01 0.1 × 0.01 × 0.01
 
Data collection
Diffractometer Rigaku XtaLAB P200K Rigaku XtaLAB P200K
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2024View full citation) Multi-scan (CrysAlis PRO; Rigaku OD, 2024View full citation)
Tmin, Tmax 0.588, 1.000 0.695, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 23801, 4647, 3366 12408, 3262, 1900
Rint 0.069 0.139
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.055, 0.114, 1.02 0.132, 0.319, 1.16
No. of reflections 4647 3262
No. of parameters 254 282
No. of restraints 0 130
H-atom treatment H atoms treated by a mixture of independent and constrained refinement H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.51, −0.32 1.39, −1.23
Computer programs: CrysAlis PRO (Rigaku OD, 2023View full citation, 2024View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2019/3 (Sheldrick, 2015bView full citation), Mercury (Macrae et al., 2020View full citation), enCIFer (Allen et al., 2004View full citation) publCIF (Westrip, 2010View full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

2-Fluorobenzyl (Z)-2-(2-oxoindolin-3-ylidene)hydrazine-1-carbodithioate dimethyl sulfoxide monololvate (1) top
Crystal data top
C16H12FN3OS2·C2H6OSF(000) = 880
Mr = 423.53Dx = 1.465 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 21.6312 (10) ÅCell parameters from 5747 reflections
b = 4.6850 (2) Åθ = 2.2–26.9°
c = 18.9579 (8) ŵ = 0.41 mm1
β = 91.519 (4)°T = 100 K
V = 1920.58 (14) Å3Needle, yellow
Z = 40.27 × 0.02 × 0.01 mm
Data collection top
Rigaku XtaLAB P200K
diffractometer
4647 independent reflections
Radiation source: Rotating Anode, Rigaku FR-X3366 reflections with I > 2σ(I)
Rigaku Osmic Confocal Optical System monochromatorRint = 0.069
Detector resolution: 5.8140 pixels mm-1θmax = 29.4°, θmin = 2.2°
shutterless scansh = 2927
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2024)
k = 66
Tmin = 0.588, Tmax = 1.000l = 2524
23801 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.055H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.114 w = 1/[σ2(Fo2) + (0.0464P)2 + 1.708P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
4647 reflectionsΔρmax = 0.51 e Å3
254 parametersΔρmin = 0.32 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.

Refinement. Hydrogen atoms on N1 and N4 were located from the Fmap and refined isotropically without restraint. DMSO solvate in the asymmetric unit is positioned outside the cell to clearly show discrete hydrogen bonding interaction between O21 and N1

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S100.71801 (3)0.17029 (15)0.13746 (3)0.02101 (17)
S110.83457 (3)0.09873 (15)0.19938 (3)0.02130 (17)
F130.93202 (7)0.2497 (4)0.04837 (8)0.0317 (4)
O20.61299 (8)0.3901 (4)0.28556 (9)0.0196 (4)
N10.63062 (11)0.7489 (5)0.36760 (12)0.0188 (5)
H10.5968 (15)0.793 (7)0.3747 (17)0.037 (10)*
N30.75269 (9)0.3900 (5)0.28429 (10)0.0176 (5)
N40.72281 (10)0.2053 (5)0.23945 (11)0.0184 (5)
H40.6820 (16)0.196 (7)0.2376 (16)0.040 (9)*
C20.64701 (11)0.5455 (5)0.32149 (13)0.0169 (5)
C30.71713 (11)0.5460 (5)0.32265 (12)0.0156 (5)
C40.73668 (11)0.7572 (5)0.37423 (12)0.0164 (5)
C50.79386 (12)0.8519 (6)0.39943 (13)0.0211 (6)
H50.8309120.7762240.3811880.025*
C60.79602 (12)1.0589 (6)0.45168 (14)0.0238 (6)
H60.8349591.1233960.4697050.029*
C70.74203 (13)1.1734 (6)0.47810 (14)0.0231 (6)
H70.7445311.3137970.5142290.028*
C80.68421 (12)1.0844 (6)0.45213 (13)0.0213 (6)
H80.6472231.1646280.4694110.026*
C90.68241 (11)0.8767 (5)0.40063 (12)0.0163 (5)
C100.75457 (11)0.0472 (5)0.19318 (12)0.0172 (5)
C110.86058 (12)0.1306 (6)0.12843 (14)0.0239 (6)
H11A0.8454350.3279760.1350900.029*
H11B0.8446240.0595510.0822640.029*
C120.93023 (12)0.1248 (6)0.13096 (13)0.0207 (6)
C130.96358 (12)0.0615 (6)0.09076 (14)0.0226 (6)
C141.02731 (12)0.0685 (6)0.09125 (14)0.0267 (6)
H141.0486300.1994120.0623540.032*
C151.05949 (12)0.1200 (6)0.13488 (15)0.0271 (6)
H151.1034260.1198250.1360620.032*
C161.02768 (12)0.3084 (6)0.17671 (15)0.0264 (6)
H161.0497590.4371670.2067740.032*
C170.96361 (12)0.3096 (6)0.17480 (14)0.0237 (6)
H170.9421430.4388960.2039840.028*
S210.50131 (3)1.27070 (14)0.39185 (3)0.01653 (16)
O210.50964 (8)0.9499 (4)0.38887 (9)0.0216 (4)
C210.46100 (12)1.3699 (6)0.31267 (12)0.0199 (6)
H21A0.4882041.3457010.2725890.030*
H21B0.4481701.5700060.3157400.030*
H21C0.4243921.2485760.3060440.030*
C220.43948 (11)1.3253 (6)0.45068 (13)0.0226 (6)
H22A0.4034871.2133170.4347430.034*
H22B0.4285351.5282520.4513860.034*
H22C0.4524321.2643940.4982710.034*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S100.0165 (3)0.0279 (4)0.0185 (3)0.0028 (3)0.0018 (2)0.0033 (3)
S110.0125 (3)0.0290 (4)0.0224 (3)0.0004 (3)0.0002 (2)0.0075 (3)
F130.0314 (10)0.0376 (10)0.0260 (9)0.0043 (8)0.0014 (7)0.0036 (8)
O20.0134 (9)0.0255 (10)0.0197 (9)0.0011 (8)0.0014 (7)0.0019 (8)
N10.0121 (11)0.0216 (12)0.0228 (12)0.0015 (10)0.0022 (9)0.0021 (10)
N30.0164 (11)0.0197 (11)0.0165 (10)0.0025 (9)0.0009 (8)0.0010 (9)
N40.0126 (11)0.0246 (13)0.0178 (11)0.0019 (9)0.0012 (9)0.0017 (9)
C20.0139 (12)0.0195 (14)0.0173 (12)0.0012 (11)0.0002 (10)0.0039 (11)
C30.0125 (12)0.0188 (13)0.0157 (12)0.0001 (10)0.0007 (9)0.0020 (11)
C40.0181 (13)0.0181 (13)0.0131 (12)0.0005 (11)0.0009 (10)0.0009 (10)
C50.0172 (13)0.0244 (15)0.0217 (13)0.0011 (11)0.0003 (10)0.0020 (12)
C60.0219 (14)0.0271 (16)0.0221 (14)0.0054 (12)0.0038 (11)0.0006 (12)
C70.0279 (15)0.0236 (15)0.0177 (13)0.0037 (12)0.0001 (11)0.0019 (11)
C80.0213 (14)0.0232 (15)0.0195 (13)0.0001 (11)0.0054 (10)0.0015 (12)
C90.0151 (12)0.0163 (13)0.0176 (13)0.0004 (10)0.0016 (9)0.0032 (11)
C100.0156 (13)0.0222 (14)0.0139 (12)0.0002 (11)0.0006 (10)0.0040 (11)
C110.0178 (14)0.0314 (16)0.0224 (14)0.0011 (12)0.0008 (10)0.0078 (12)
C120.0166 (13)0.0264 (15)0.0189 (13)0.0041 (11)0.0007 (10)0.0087 (12)
C130.0221 (14)0.0247 (15)0.0209 (14)0.0041 (12)0.0013 (11)0.0049 (12)
C140.0229 (15)0.0321 (17)0.0253 (15)0.0045 (13)0.0061 (11)0.0058 (13)
C150.0157 (13)0.0325 (17)0.0331 (16)0.0014 (12)0.0007 (11)0.0099 (14)
C160.0194 (14)0.0293 (16)0.0302 (15)0.0053 (12)0.0054 (11)0.0044 (13)
C170.0220 (14)0.0262 (15)0.0229 (14)0.0018 (12)0.0004 (11)0.0039 (12)
S210.0130 (3)0.0207 (4)0.0158 (3)0.0007 (3)0.0007 (2)0.0009 (3)
O210.0183 (10)0.0216 (10)0.0248 (10)0.0020 (8)0.0005 (7)0.0001 (8)
C210.0182 (13)0.0252 (15)0.0163 (13)0.0024 (11)0.0003 (10)0.0002 (11)
C220.0178 (13)0.0327 (16)0.0175 (13)0.0037 (12)0.0026 (10)0.0004 (12)
Geometric parameters (Å, º) top
S10—C101.654 (3)C8—C91.378 (4)
S11—C101.748 (2)C11—H11A0.9900
S11—C111.822 (3)C11—H11B0.9900
F13—C131.364 (3)C11—C121.506 (4)
O2—C21.228 (3)C12—C131.376 (4)
N1—H10.78 (3)C12—C171.389 (4)
N1—C21.347 (3)C13—C141.379 (4)
N1—C91.403 (3)C14—H140.9500
N3—N41.364 (3)C14—C151.385 (4)
N3—C31.298 (3)C15—H150.9500
N4—H40.88 (3)C15—C161.382 (4)
N4—C101.350 (3)C16—H160.9500
C2—C31.517 (3)C16—C171.385 (4)
C3—C41.446 (3)C17—H170.9500
C4—C51.387 (3)S21—O211.5150 (19)
C4—C91.405 (3)S21—C211.778 (2)
C5—H50.9500S21—C221.783 (2)
C5—C61.386 (4)C21—H21A0.9800
C6—H60.9500C21—H21B0.9800
C6—C71.391 (4)C21—H21C0.9800
C7—H70.9500C22—H22A0.9800
C7—C81.396 (4)C22—H22B0.9800
C8—H80.9500C22—H22C0.9800
C10—S11—C11101.15 (12)H11A—C11—H11B108.6
C2—N1—H1125 (2)C12—C11—S11107.09 (18)
C2—N1—C9111.8 (2)C12—C11—H11A110.3
C9—N1—H1124 (2)C12—C11—H11B110.3
C3—N3—N4115.4 (2)C13—C12—C11122.2 (2)
N3—N4—H4121 (2)C13—C12—C17117.1 (2)
C10—N4—N3120.8 (2)C17—C12—C11120.8 (3)
C10—N4—H4118 (2)F13—C13—C12118.4 (2)
O2—C2—N1128.0 (2)F13—C13—C14118.3 (2)
O2—C2—C3126.4 (2)C12—C13—C14123.4 (3)
N1—C2—C3105.6 (2)C13—C14—H14120.8
N3—C3—C2126.8 (2)C13—C14—C15118.4 (3)
N3—C3—C4126.7 (2)C15—C14—H14120.8
C4—C3—C2106.6 (2)C14—C15—H15120.0
C5—C4—C3133.9 (2)C16—C15—C14120.0 (3)
C5—C4—C9119.7 (2)C16—C15—H15120.0
C9—C4—C3106.3 (2)C15—C16—H16120.0
C4—C5—H5120.6C15—C16—C17120.0 (3)
C6—C5—C4118.9 (2)C17—C16—H16120.0
C6—C5—H5120.6C12—C17—H17119.4
C5—C6—H6119.5C16—C17—C12121.1 (3)
C5—C6—C7121.0 (2)C16—C17—H17119.4
C7—C6—H6119.5O21—S21—C21106.50 (12)
C6—C7—H7119.6O21—S21—C22104.93 (12)
C6—C7—C8120.7 (2)C21—S21—C2297.55 (12)
C8—C7—H7119.6S21—C21—H21A109.5
C7—C8—H8121.0S21—C21—H21B109.5
C9—C8—C7118.0 (2)S21—C21—H21C109.5
C9—C8—H8121.0H21A—C21—H21B109.5
N1—C9—C4109.6 (2)H21A—C21—H21C109.5
C8—C9—N1128.7 (2)H21B—C21—H21C109.5
C8—C9—C4121.7 (2)S21—C22—H22A109.5
S10—C10—S11125.71 (15)S21—C22—H22B109.5
N4—C10—S10120.67 (19)S21—C22—H22C109.5
N4—C10—S11113.62 (18)H22A—C22—H22B109.5
S11—C11—H11A110.3H22A—C22—H22C109.5
S11—C11—H11B110.3H22B—C22—H22C109.5
S11—C11—C12—C1393.9 (3)C5—C4—C9—N1179.9 (2)
S11—C11—C12—C1785.9 (3)C5—C4—C9—C81.0 (4)
F13—C13—C14—C15179.2 (2)C5—C6—C7—C80.6 (4)
O2—C2—C3—N32.5 (4)C6—C7—C8—C91.2 (4)
O2—C2—C3—C4178.2 (2)C7—C8—C9—N1178.5 (2)
N1—C2—C3—N3177.4 (2)C7—C8—C9—C40.4 (4)
N1—C2—C3—C41.8 (3)C9—N1—C2—O2178.1 (2)
N3—N4—C10—S10178.38 (18)C9—N1—C2—C31.9 (3)
N3—N4—C10—S111.7 (3)C9—C4—C5—C61.6 (4)
N3—C3—C4—C51.8 (5)C10—S11—C11—C12175.81 (19)
N3—C3—C4—C9178.2 (2)C11—S11—C10—S102.4 (2)
N4—N3—C3—C21.0 (3)C11—S11—C10—N4177.65 (19)
N4—N3—C3—C4179.8 (2)C11—C12—C13—F131.2 (4)
C2—N1—C9—C41.3 (3)C11—C12—C13—C14179.0 (2)
C2—N1—C9—C8177.6 (2)C11—C12—C17—C16179.1 (2)
C2—C3—C4—C5179.0 (3)C12—C13—C14—C150.6 (4)
C2—C3—C4—C91.1 (3)C13—C12—C17—C161.1 (4)
C3—N3—N4—C10175.0 (2)C13—C14—C15—C160.2 (4)
C3—C4—C5—C6178.5 (3)C14—C15—C16—C170.3 (4)
C3—C4—C9—N10.1 (3)C15—C16—C17—C120.4 (4)
C3—C4—C9—C8179.0 (2)C17—C12—C13—F13178.6 (2)
C4—C5—C6—C70.8 (4)C17—C12—C13—C141.2 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O210.78 (3)2.05 (3)2.820 (3)174 (3)
N4—H4···O20.88 (3)1.99 (3)2.696 (3)136 (3)
C7—H7···S10i0.952.943.860 (3)163
C21—H21C···O2ii0.982.533.305 (3)136
C22—H22C···O21iii0.982.483.457 (3)172
Symmetry codes: (i) x, y+3/2, z+1/2; (ii) x+1, y+1/2, z+1/2; (iii) x+1, y+2, z+1.
2-Fluorobenzyl (Z)-2-(5-bromo-2-oxoindolin-3-ylidene)hydrazine-1-carbodithioate (2) top
Crystal data top
C16H11BrFN3OS2Z = 2
Mr = 424.31F(000) = 424
Triclinic, P1Dx = 1.684 Mg m3
a = 6.6979 (7) ÅCu Kα radiation, λ = 1.54184 Å
b = 8.0075 (9) ÅCell parameters from 1932 reflections
c = 15.880 (2) Åθ = 2.8–60.0°
α = 84.917 (10)°µ = 5.86 mm1
β = 80.544 (10)°T = 100 K
γ = 89.948 (9)°Needle, orange
V = 836.73 (17) Å30.1 × 0.01 × 0.01 mm
Data collection top
Rigaku XtaLAB P200K
diffractometer
3262 independent reflections
Radiation source: Rotating Anode, Rigaku MM-007HF1900 reflections with I > 2σ(I)
Rigaku Osmic Confocal Optical System monochromatorRint = 0.139
Detector resolution: 5.8140 pixels mm-1θmax = 75.8°, θmin = 2.8°
shutterless scansh = 88
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2024)
k = 910
Tmin = 0.695, Tmax = 1.000l = 1919
12408 measured reflections
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.132H-atom parameters constrained
wR(F2) = 0.319 w = 1/[σ2(Fo2) + 14.5238P]
where P = (Fo2 + 2Fc2)/3
S = 1.16(Δ/σ)max < 0.001
3262 reflectionsΔρmax = 1.39 e Å3
282 parametersΔρmin = 1.23 e Å3
130 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.

Refinement. Refined as a 2-component twin at [-1 0 0 0 1.001 -0.005 0 0.333 -1.001] with HKLF5 generated by TWINROTMAT running in PLATON. Ortho-fluorobenzyl group was disordered with fluoro group fliped 180°. fluoro- phenyl ring was split in two parts and refined with C—F and aromatic C—C distances restrained, C12A/B thermal parameters linked with SIMU, and general thermal restraints on both parts.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Br60.0746 (3)0.4658 (3)0.34527 (14)0.0526 (6)
S100.5773 (6)0.2120 (6)0.8720 (3)0.0532 (12)
S110.2188 (6)0.3262 (6)0.7844 (3)0.0493 (12)
F13A0.190 (3)0.587 (3)0.8641 (17)0.063 (8)0.48 (3)
F13B0.423 (3)0.628 (3)0.9211 (15)0.066 (7)0.52 (3)
O20.8662 (15)0.0741 (14)0.5997 (7)0.042 (3)
N10.7918 (17)0.1135 (16)0.4609 (9)0.038 (3)
H10.8979010.0660370.4327710.046*
N30.4653 (18)0.2489 (16)0.6398 (9)0.040 (3)
N40.5546 (17)0.2100 (17)0.7094 (8)0.040 (3)
H40.6724550.1599570.7034570.048*
C20.759 (2)0.124 (2)0.5459 (13)0.044 (4)
C30.560 (2)0.2145 (19)0.5670 (11)0.038 (4)
C40.491 (2)0.256 (2)0.4859 (11)0.040 (4)
C50.319 (2)0.331 (2)0.4627 (12)0.044 (4)
H50.2142410.3672520.5048140.053*
C60.303 (2)0.350 (2)0.3780 (14)0.052 (5)
C70.444 (2)0.287 (2)0.3158 (11)0.042 (4)
H70.4257990.2999140.2575380.051*
C80.614 (2)0.204 (2)0.3380 (12)0.044 (4)
H80.7116500.1590530.2959540.053*
C90.633 (2)0.189 (2)0.4224 (11)0.043 (4)
C100.465 (2)0.247 (2)0.7876 (13)0.050 (5)
C110.134 (2)0.3751 (17)0.8932 (11)0.044 (4)
H11A0.0029430.3267680.9136820.052*0.48 (3)
H11B0.2263750.3236850.9305610.052*0.48 (3)
H11C0.0064330.3135100.9169220.052*0.52 (3)
H11D0.2370240.3396710.9290800.052*0.52 (3)
C12A0.129 (7)0.563 (3)0.899 (7)0.041 (9)0.48 (3)
C12B0.101 (7)0.562 (3)0.895 (7)0.045 (9)0.52 (3)
C13A0.028 (4)0.667 (3)0.881 (3)0.048 (11)0.48 (3)
C13B0.242 (4)0.681 (4)0.905 (3)0.044 (9)0.52 (3)
C14A0.027 (6)0.838 (4)0.887 (3)0.051 (10)0.48 (3)
H14A0.1414860.9036030.8785260.061*0.48 (3)
C14B0.201 (5)0.849 (4)0.913 (3)0.053 (8)0.52 (3)
H14B0.2981010.9223740.9276660.064*0.52 (3)
C15A0.145 (5)0.910 (4)0.906 (3)0.055 (11)0.48 (3)
H15A0.1563511.0287980.9054310.066*0.48 (3)
C15B0.015 (5)0.905 (4)0.898 (3)0.051 (8)0.52 (3)
H15B0.0137161.0207490.9001130.061*0.52 (3)
C16A0.302 (6)0.808 (4)0.925 (3)0.061 (11)0.48 (3)
H16A0.4173290.8582940.9406890.073*0.48 (3)
C16B0.131 (5)0.798 (3)0.880 (2)0.049 (8)0.52 (3)
H16B0.2555760.8372530.8660290.059*0.52 (3)
C17A0.296 (6)0.638 (4)0.922 (3)0.046 (9)0.48 (3)
H17A0.4067880.5719990.9345370.056*0.48 (3)
C17B0.085 (6)0.631 (4)0.884 (3)0.044 (8)0.52 (3)
H17B0.1898610.5543270.8793540.053*0.52 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br60.0318 (8)0.0514 (12)0.0740 (14)0.0068 (8)0.0112 (8)0.0025 (10)
S100.049 (2)0.046 (3)0.066 (3)0.007 (2)0.016 (2)0.006 (2)
S110.046 (2)0.042 (3)0.059 (3)0.0194 (19)0.006 (2)0.005 (2)
F13A0.041 (11)0.043 (12)0.11 (2)0.002 (8)0.026 (11)0.003 (12)
F13B0.053 (11)0.070 (14)0.084 (16)0.013 (9)0.026 (11)0.037 (12)
O20.035 (5)0.039 (7)0.053 (7)0.012 (5)0.004 (5)0.012 (6)
N10.029 (6)0.027 (7)0.057 (9)0.003 (5)0.003 (6)0.006 (6)
N30.038 (7)0.025 (7)0.056 (9)0.003 (6)0.004 (6)0.008 (7)
N40.030 (6)0.040 (8)0.047 (8)0.009 (6)0.001 (6)0.009 (7)
C20.023 (7)0.029 (9)0.077 (14)0.000 (6)0.001 (8)0.002 (9)
C30.029 (7)0.026 (8)0.061 (11)0.006 (6)0.002 (7)0.020 (8)
C40.031 (7)0.036 (9)0.050 (10)0.006 (7)0.002 (7)0.003 (8)
C50.038 (8)0.034 (9)0.058 (11)0.008 (7)0.001 (8)0.004 (8)
C60.019 (7)0.037 (10)0.096 (15)0.013 (6)0.007 (8)0.005 (10)
C70.031 (8)0.040 (10)0.056 (11)0.013 (7)0.014 (7)0.008 (8)
C80.034 (8)0.034 (9)0.063 (12)0.008 (7)0.004 (8)0.011 (9)
C90.032 (8)0.045 (10)0.053 (11)0.002 (7)0.008 (7)0.002 (9)
C100.039 (9)0.025 (9)0.081 (14)0.010 (7)0.004 (9)0.004 (9)
C110.048 (9)0.031 (9)0.049 (10)0.001 (7)0.002 (8)0.008 (8)
C12A0.032 (14)0.040 (14)0.05 (2)0.009 (10)0.004 (14)0.001 (15)
C12B0.039 (12)0.042 (12)0.05 (2)0.002 (9)0.004 (13)0.003 (14)
C13A0.036 (14)0.032 (12)0.08 (3)0.005 (9)0.009 (15)0.007 (14)
C13B0.039 (11)0.044 (11)0.05 (2)0.003 (8)0.002 (11)0.004 (13)
C14A0.051 (18)0.034 (12)0.07 (3)0.005 (10)0.014 (18)0.008 (15)
C14B0.053 (10)0.049 (10)0.059 (13)0.001 (7)0.012 (8)0.008 (9)
C15A0.058 (19)0.029 (14)0.08 (3)0.003 (11)0.022 (17)0.003 (17)
C15B0.052 (10)0.045 (10)0.053 (12)0.003 (7)0.006 (8)0.004 (9)
C16A0.060 (18)0.041 (14)0.08 (3)0.002 (13)0.026 (19)0.009 (16)
C16B0.042 (13)0.044 (11)0.06 (2)0.006 (9)0.001 (14)0.011 (12)
C17A0.049 (18)0.038 (13)0.05 (2)0.003 (12)0.013 (18)0.020 (15)
C17B0.042 (10)0.043 (10)0.049 (12)0.005 (7)0.008 (9)0.008 (9)
Geometric parameters (Å, º) top
Br6—C61.910 (14)C11—H11B0.9900
S10—C101.644 (19)C11—H11C0.9900
S11—C101.774 (15)C11—H11D0.9900
S11—C111.804 (16)C11—C12A1.519 (19)
F13A—C13A1.342 (19)C11—C12B1.516 (18)
F13B—C13B1.339 (18)C12A—C13A1.390 (19)
O2—C21.246 (19)C12A—C17A1.38 (2)
N1—H10.8800C12B—C13B1.383 (19)
N1—C21.34 (2)C12B—C17B1.385 (19)
N1—C91.421 (19)C13A—C14A1.382 (19)
N3—N41.353 (18)C13B—C14B1.381 (19)
N3—C31.28 (2)C14A—H14A0.9500
N4—H40.8800C14A—C15A1.38 (2)
N4—C101.34 (2)C14B—H14B0.9500
C2—C31.517 (19)C14B—C15B1.372 (19)
C3—C41.45 (2)C15A—H15A0.9500
C4—C51.39 (2)C15A—C16A1.386 (19)
C4—C91.41 (2)C15B—H15B0.9500
C5—H50.9500C15B—C16B1.38 (2)
C5—C61.36 (3)C16A—H16A0.9500
C6—C71.38 (2)C16A—C17A1.369 (19)
C7—H70.9500C16B—H16B0.9500
C7—C81.39 (2)C16B—C17B1.370 (19)
C8—H80.9500C17A—H17A0.9500
C8—C91.36 (2)C17B—H17B0.9500
C11—H11A0.9900
C10—S11—C11103.1 (9)C12A—C11—H11A109.4
C2—N1—H1124.5C12A—C11—H11B109.4
C2—N1—C9111.0 (13)C12B—C11—S11110 (4)
C9—N1—H1124.5C12B—C11—H11C109.7
C3—N3—N4117.9 (13)C12B—C11—H11D109.7
N3—N4—H4119.6C13A—C12A—C11125 (3)
C10—N4—N3120.7 (12)C17A—C12A—C11118 (2)
C10—N4—H4119.6C17A—C12A—C13A117 (2)
O2—C2—N1128.7 (14)C13B—C12B—C11126 (3)
O2—C2—C3124.4 (16)C13B—C12B—C17B113 (2)
N1—C2—C3106.9 (14)C17B—C12B—C11121 (2)
N3—C3—C2129.1 (16)F13A—C13A—C12A115 (2)
N3—C3—C4124.8 (13)F13A—C13A—C14A121 (3)
C4—C3—C2106.1 (14)C14A—C13A—C12A123 (2)
C5—C4—C3134.1 (15)F13B—C13B—C12B118 (3)
C5—C4—C9119.0 (16)F13B—C13B—C14B117 (3)
C9—C4—C3106.7 (13)C14B—C13B—C12B124 (3)
C4—C5—H5120.9C13A—C14A—H14A121.1
C6—C5—C4118.2 (15)C15A—C14A—C13A118 (3)
C6—C5—H5120.9C15A—C14A—H14A121.1
C5—C6—Br6118.3 (13)C13B—C14B—H14B121.1
C5—C6—C7122.4 (14)C15B—C14B—C13B118 (3)
C7—C6—Br6119.3 (15)C15B—C14B—H14B121.1
C6—C7—H7119.8C14A—C15A—H15A120.4
C6—C7—C8120.3 (17)C14A—C15A—C16A119 (3)
C8—C7—H7119.8C16A—C15A—H15A120.4
C7—C8—H8121.3C14B—C15B—H15B119.1
C9—C8—C7117.4 (16)C14B—C15B—C16B122 (3)
C9—C8—H8121.3C16B—C15B—H15B119.1
C4—C9—N1109.3 (14)C15A—C16A—H16A118.9
C8—C9—N1128.2 (15)C17A—C16A—C15A122 (4)
C8—C9—C4122.4 (15)C17A—C16A—H16A118.9
S10—C10—S11127.5 (12)C15B—C16B—H16B121.9
N4—C10—S10121.5 (11)C17B—C16B—C15B116 (3)
N4—C10—S11110.9 (13)C17B—C16B—H16B121.9
S11—C11—H11A109.4C12A—C17A—H17A120.1
S11—C11—H11B109.4C16A—C17A—C12A120 (3)
S11—C11—H11C109.7C16A—C17A—H17A120.1
S11—C11—H11D109.7C12B—C17B—H17B116.9
H11A—C11—H11B108.0C16B—C17B—C12B126 (3)
H11C—C11—H11D108.2C16B—C17B—H17B116.9
C12A—C11—S11111 (4)
Br6—C6—C7—C8179.3 (12)C6—C7—C8—C90 (2)
S11—C11—C12A—C13A82 (9)C7—C8—C9—N1178.7 (15)
S11—C11—C12A—C17A95 (7)C7—C8—C9—C41 (2)
S11—C11—C12B—C13B91 (9)C9—N1—C2—O2179.0 (16)
S11—C11—C12B—C17B88 (8)C9—N1—C2—C30.1 (17)
F13A—C13A—C14A—C15A180 (4)C9—C4—C5—C66 (2)
F13B—C13B—C14B—C15B179 (4)C10—S11—C11—C12A107.9 (17)
O2—C2—C3—N33 (3)C10—S11—C11—C12B116.4 (16)
O2—C2—C3—C4177.5 (15)C11—S11—C10—S105.0 (14)
N1—C2—C3—N3178.0 (15)C11—S11—C10—N4177.6 (11)
N1—C2—C3—C41.6 (17)C11—C12A—C13A—F13A6 (11)
N3—N4—C10—S10176.1 (12)C11—C12A—C13A—C14A179 (7)
N3—N4—C10—S116.3 (19)C11—C12A—C17A—C16A177 (6)
N3—C3—C4—C53 (3)C11—C12B—C13B—F13B5 (11)
N3—C3—C4—C9177.2 (16)C11—C12B—C13B—C14B175 (7)
N4—N3—C3—C24 (2)C11—C12B—C17B—C16B176 (6)
N4—N3—C3—C4176.4 (14)C12A—C13A—C14A—C15A5 (9)
C2—N1—C9—C41.4 (18)C12B—C13B—C14B—C15B9 (8)
C2—N1—C9—C8179.6 (17)C13A—C12A—C17A—C16A0 (11)
C2—C3—C4—C5176.7 (18)C13A—C14A—C15A—C16A5 (7)
C2—C3—C4—C92.4 (17)C13B—C12B—C17B—C16B2 (11)
C3—N3—N4—C10178.2 (15)C13B—C14B—C15B—C16B3 (6)
C3—C4—C5—C6179.8 (17)C14A—C15A—C16A—C17A3 (7)
C3—C4—C9—N12.4 (18)C14B—C15B—C16B—C17B5 (6)
C3—C4—C9—C8179.3 (15)C15A—C16A—C17A—C12A1 (8)
C4—C5—C6—Br6176.1 (12)C15B—C16B—C17B—C12B8 (8)
C4—C5—C6—C75 (3)C17A—C12A—C13A—F13A177 (6)
C5—C4—C9—N1177.7 (14)C17A—C12A—C13A—C14A2 (11)
C5—C4—C9—C84 (3)C17B—C12B—C13B—F13B176 (6)
C5—C6—C7—C82 (3)C17B—C12B—C13B—C14B6 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···O2i0.881.962.821 (15)165
N4—H4···O20.882.092.777 (16)134
C11—H11D···S100.992.563.221 (14)124
Symmetry code: (i) x+2, y, z+1.
 

Acknowledgements

The authors acknowledge Universiti Teknologi MARA for financial support.

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