Crystal structures of four chiral imine-substituted thio-phene derivatives.

A series of thio-phenes substituted in positions 2 and 5 by imine groups have been synthesized using a solvent-free approach, and their crystal structures determined. The substituents are chiral groups, and the expected absolute configuration for each mol-ecule was confirmed by refinement of the Flack parameter. The compounds are 2,5-bis-[(S)-(+)-(1,2,3,4-tetra-hydro-naphthalen-1-yl)imino]-thio-phene, C26H26N2S, (I), 2,5-bis-{[(R)-(-)-1-(4-meth-oxy-phen-yl)eth-yl]imino-meth-yl}thio-phene, C24H26N2O2S, (II), 2,5-bis-{[(R)-(-)-1-(4-fluoro-phen-yl)eth-yl]imino-meth-yl}thio-phene, C22H20F2N2S, (III), and 2,5-bis-{[(S)-(+)-1-(4-chloro-phen-yl)eth-yl]imino-meth-yl}thio-phene, C22H20Cl2N2S, (IV). A common feature of all four mol-ecules is the presence of twofold symmetry. For (I), which crystallizes in the triclinic space group P1, this symmetry is non-crystallographic, but for (II) in C2 and the isomorphous structures (III) and (IV) that crystallize in P21212, the twofold symmetry is crystallographically imposed with one half of each mol-ecule in the asymmetric unit. The comparable mol-ecular symmetry in the four structures is also reflected in similar packing, with mol-ecules aggregated to form chains through weak C-H⋯S inter-actions.

Chemical context

Thio­phene­dicarbaldehydes have a variety of applications (Dean, 1982a ▸,b ▸), for instance in the synthesis of annulenones and polyenyl-substituted thio­phenes (Sargent & Cresp, 1975 ▸), in the preparation of macrocyclic ligands for bimetallic complexes that are able to mimic enzymes (Nelson et al., 1983 ▸), in crown ether chemistry (Cram & Trueblood, 1981 ▸) and, more recently, in the preparation of azomethines for photovoltaic applications (Bolduc et al., 2013a ▸,b ▸; Petrus et al., 2014 ▸). In regard to this latter application, most of the conjugated materials used in organic electronics are synthesized using time-consuming Suzuki-, Wittig-, or Heck-type coupling reactions that require expensive catalysts, stringent reaction conditions, and tedious purification processes. In order to afford a more economic route towards organic photovoltaic materials, Schiff bases derived from 2,5-thio­phene­dicarbaldehyde as the conjugated linker unit have recently been used. The azomethine bond, which is isoelectronic with the vinyl bond and possesses similar optoelectronic and thermal properties, is easily accessible through the Schiff condensation under near ambient reaction conditions (Morgan et al., 1987 ▸; Pérez Guarìn et al., 2007 ▸; Sicard et al., 2013 ▸).

We report here the synthesis and X-ray characterization of such thio­phene derivatives, as a continuation of a partially published record (Bernès et al., 2013 ▸; Mendoza et al., 2014 ▸). We are improving a general solvent-free approach for these syntheses, recognising that ecological aspects in organic chemistry have become a priority, in order to minimize the qu­antity of toxic waste and by-products, and to decrease the amount of solvent in the reaction media or during work-up (Tanaka & Toda, 2000 ▸; Noyori, 2005 ▸).

In the synthesis of the thio­phenes reported here, the Schiff condensation generates a single by-product, water, and a one-step recrystallization affords the pure substituted thio­phene in nearly qu­anti­tative yields. Our protocol may be readily extended to any low mol­ecular weight 2,5-susbtituted thio­phene, providing that a liquid amine is used for the condensation. In the present work, the starting material is 2,5-thio­phene­dicarbaldehyde, a low melting-point compound (m.p. = 388–390 K), and four chiral amines were used. We took advantage of the anomalous dispersion of the sulfur sites to confirm that the configuration of the chiral amine is retained during the condensation.

Structural commentary

The first compound was synthesized using (S)-(+)-1-amino­tetra­line. The Schiff base (I), C26H26N2S, crystallizes in the space group P1, with the expected absolute configuration (Fig. 1 ▸). The general shape of the mol­ecule displays a pseudo-twofold axis, passing through the S atom and the midpoint of the thio­phene C—C σ-bond. As a consequence, the independent benzene rings are placed above and below the thio­phene ring, and are inclined to one another at a dihedral angle of 73.76 (15)°. The central core containing the thio­phene ring and the imine bonds is virtually planar, and the imine bonds are substituted by the tetra­lin ring systems, which present the same conformation. The aliphatic rings C9–C13/C18 and C19–C23/C28 each have a half-chair conformation.

Figure 1

The mol­ecular structure of (I), with displacement ellipsoids for non-H atoms at the 30% probability level.

Compound (II), C24H26N2O2S, was obtained using (R)-(+)-(4-meth­oxy)phenyl­ethyl­amine as the chiral component in the Schiff condensation. The twofold mol­ecular axis, which was a latent symmetry in the case of (I), is a true crystallographic symmetry in (II), and this compound crystallizes in the space group C2 (Fig. 2 ▸). The asymmetric unit thus contains half a mol­ecule, and the mol­ecular conformation for the complete mol­ecule is similar to that of (I). The benzene rings have a free relative orientation, since these rings are not fused in a bicyclic system, as in (I); the dihedral angle between symmetry-related rings is 61.30 (7)°.

Figure 2

The mol­ecular structure of (II), with displacement ellipsoids for non-H atoms at the 30% probability level. Non-labeled atoms are generated by symmetry code (1 − x, y, 1 − z).

Compounds (III) and (IV), synthesized with enanti­o­meri­cally pure (4-halogen)phenyl­ethyl­amines (halogen = F, Cl) are isomorphous and crystallize with ortho­rhom­bic unit cells. The latent twofold symmetry of (I) is again observed, since both mol­ecules lie on the crystallographic twofold axes of the space group P21212 (Fig. 3 ▸). The dihedral angle between the benzene rings is close to that observed for (II): 64.18 (8)° for (III) and 62.03 (9)° for (IV). The same Schiff base but with Br as the halogen substituent has been published previously (Mendoza et al., 2014 ▸), but is not isomorphous with (III) and (IV). Instead, this mol­ecule was found to crystallize in the space group C2, with unit-cell parameters and a crystal structure very similar to those of (II). A systematic trend is thus emerging for these 2,5-substituted thio­phenes, related to the potential twofold mol­ecular symmetry: they have a strong tendency to crystallize in space groups that include at least one C 2 axis, such as C2 and P21212 for the chiral crystals. This trend extends to achiral mol­ecules, which also have twofold crystallographic symmetry in the space group C2/c (Kudyakova et al., 2011 ▸; Suganya et al., 2014 ▸; Boyle et al., 2015 ▸; Moussallem et al., 2015 ▸). The features shared by these related compounds could also be a signature of a propensity towards polymorphism between monoclinic and ortho­rhom­bic systems.

Figure 3

The mol­ecular structures of isomorphous compounds (III) and (IV), with displacement ellipsoids for non-H atoms at the 30% probability level. Notice the different configuration for chiral center C5 in (III) and (IV). Non-labeled atoms are generated by symmetry codes (1 − x, −y, z) and (1 − x, 2 − y, z) for (III) and (IV), respectively.

The difference between non-crystallographic symmetry in (I) and exact C 2 mol­ecular symmetry in (II)–(IV) is also reflected in the degree of conjugation between thio­phene rings and imine bonds. For (I), dihedral angles between the thio­phene and C=N—C* mean planes (C* is the chiral C atom bonded to the imine functionality) are 6.9 (7) and 1.9 (6)°. Other crystals have a symmetry restriction, inducing a small deconjugation of the imine bonds. The corresponding dihedral angles with the thio­phene rings are 8.5 (4), 10.1 (3), and 9.8 (3)°, for (II), (III) and (IV), respectively.

Supra­molecular features

Although all compounds have benzene rings, neither π–π nor C—H⋯π contacts stabilize the crystal structures. However, these compounds share a common supra­molecular feature. Lone pairs of S atoms inter­act with thio­phenic CH groups of a neighboring mol­ecule in the crystal, forming chains along the short cell axes: [100] for (I), [010] for (II) and [001] for (III) and (IV). An example is presented in Fig. 4 ▸, for compound (II). These bifurcated S⋯C—H contacts have a significant strength for (I), perhaps as a consequence of the relaxed mol­ecular symmetry in space group P1. The contacts are weaker for (II), (III) and (IV), which have a geometry restrained by the crystallographic symmetry (Table 1 ▸).

Figure 4

Part of the crystal structure of (II), showing C—H⋯S hydrogen bonds (dashed lines) linking mol­ecules along [010]. [Symmetry codes: (i) 1 − x, y, 1 − z; (ii) x, 1 + y, z.]

Table 1

Comparison of C—H⋯S hydrogen bonds (Å, °) in compounds (I)–(IV)

Compound	Contact	C—H	H⋯S	C⋯S	C—H⋯S
(I)	C4—H4A⋯S1i	0.93	3.00	3.562 (5)	121
(I)	C5—H5A⋯S1i	0.93	2.97	3.547 (5)	122
(II)	C4—H4A⋯S1ii	0.93	2.99	3.572 (3)	122
(III)	C4—H4A⋯S1iii	0.93	3.15	3.743 (3)	124
(IV)	C4—H4A⋯S1iv	0.93	3.23	3.828 (4)	124

Symmetry codes: (i) x + 1, y, z; (ii) x, y + 1, z; (iii) x, y, z + 1; (iv) x, y, z − 1.

Database survey

Many thio­phenes substituted in the 2 and 5 positions by imine groups have been characterized; however, almost all were achiral compounds. X-ray structures have been reported mostly in space group C2/c (Suganya et al., 2014 ▸; Kudyakova et al., 2011 ▸, 2012 ▸; Bolduc et al., 2013b ▸). Other represented space groups for achiral mol­ecules are P21 (Skene & Dufresne, 2006 ▸) and P21/c (Wiedermann et al., 2005 ▸). Finally, a single case of a mol­ecule presenting mirror symmetry has been described (Fridman & Kaftory, 2007 ▸), in space group Pnma.

The group of chiral mol­ecules belonging to this family is much less populated, with two examples reported by our group in this journal. Both are mol­ecules with the C 2 point group and crystallize in space groups C2 (Mendoza et al., 2014 ▸) and P22121 (Bernès et al., 2013 ▸).

Synthesis and crystallization

Synthesis. The chiral amines used for the Schiff condensation were obtained directly from suppliers: (S)-(+)-1,2,3,4-tetra­hydro-1-naphthyl­amine for (I), (R)-(+)-1-(4-meth­oxy­phen­yl)ethyl­amine for (II), (R)-(+)-1-(4-fluoro­phen­yl)ethyl­amine for (III) and (S)-(−)-1-(4-chloro­phen­yl)ethyl­amine for (IV). 2,5-Thio­phene­dicarbaldehyde (100 mg, 0.71 mmol) and the chiral amine (1.4 mmol) in a 1:2 molar ratio were mixed at room temperature under solvent-free conditions, giving light-yellow (II and IV), colorless (III) or light-brown (IV) solids, in 95-97% yields. The crude solids were recrystallized from CH2Cl2, affording colorless crystals of (I)–(IV).

Spectroscopy. (I): m.p. 437–438 K. [α]20 D = +655.4 (c = 1, CHCl3). FTIR: 1616 cm−1 (C=N). 1H NMR (500 MHz, CHCl3/TMS): δ = 1.76–1.86 (m, 2H; H-al), 1.96–2.06 (m, 6H; H-al), 2.74–2.90 (m, 4H; H-al), 4.51 (t, 2H; H-al), 6.98–7.02 (m, 2H; H-ar), 7.09–7.15 (m, 6H; H-ar), 7.28 (s, 2H; H-ar), 8.36 (s, 2H; HC=N). 13C NMR: δ = 19.7, 29.3, 31.1, 67.7 (C-al), 125.7, 126.9, 128.7, 129.1, 129.6, 136.8, 137.1, 145.1 (C-ar), 153.1 (HC=N). MS–EI: m/z = 398 (M +).

(II): m.p. 405–406 K. [α]20 D = −626.8 (c = 1, CHCl3). FTIR: 1631 cm−1 (C=N). 1H NMR (500 MHz, CHCl3/TMS): δ = 1.53 (d, 6H; CHCH 3), 3.78 (s, 6H; OCH 3), 4.47 (q, 2H; CHCH3), 6.85–6.88 (m, 4H; H-ar), 7.19 (s, 2H; H-ar), 7.29–7.32 (m, 4H; H-ar), 8.33 (s, 2H; HC=N). 13C NMR: δ = 24.8 (CHCH3), 55.2 (OCH3), 68.1 (CHCH3), 113.7, 127.6, 129.6, 137.1, 145.2, 152.1 (C-ar), 158.5 (HC=N). MS–EI: m/z = 406 (M +).

(III): m.p. 420–421 K. [α]20 D = −542.5 (c = 1, CHCl3). FTIR: 1621 cm−1 (C=N). 1H NMR (500 MHz, CHCl3/TMS): δ = 1.53 (d, 6H; CHCH 3), 4.49 (q, 2H; CHCH3), 7.00–7.38 (m, 10H; H-ar), 8.37 (s, 2H; HC=N). 13C NMR: δ = 25.2 (CHCH3), 68.7 (CHCH3), 115.2 (d, J F-C = 21.2 Hz; C-ar), 128.1 (d, J F-C = 8.7 Hz; C-ar), 130.1 (C-ar), 140.7 (d, J F-C = 2.5 Hz; C-ar), 145.1 (C-ar), 161.1 (d, J F-C = 242.5 Hz; C-ar), 152.5 (HC=N). MS–EI: m/z = 382 (M +).

(IV): m.p. 434–435 K. [α]20 D = +726.5 (c = 1, CHCl3). FTIR: 1623 cm−1 (C=N). 1H NMR (500 MHz, CHCl3/TMS): δ = 1.53 (d, 6H; CHCH 3), 4.48 (q, 2H; CHCH3), 7.23–7.35 (m, 10H; H-ar), 8.37 (s, 2H; HC=N). 13C NMR: δ = 25.2 (CHCH3), 68.7 (CHCH3), 128.0, 128.6, 130.2, 132.5, 143.5, 145.1 (C-ar), 152.7 (HC=N).

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2 ▸. No unusual issues appeared, and refinements were carried out on non-restricted models. All H atoms were placed in calculated positions, and refined as riding on their carrier C atoms, with C—H bond lengths fixed to 0.93 (aromatic CH), 0.96 (methyl CH3), 0.97 (methyl­ene CH2), or 0.98 Å (methine CH). Isotropic displacement parameters were calculated as U iso(H) = 1.5U eq(C) for methyl H atoms and U iso(H) = 1.2U eq(C) for other H atoms. For all compounds, the absolute configuration was based on the refinement of the Flack parameter (Parsons et al., 2013 ▸), confirming that the configuration of the chiral amine used as the starting material was retained during the Schiff condensation.

Table 2

Experimental details

	(I)	(II)	(III)	(IV)
Crystal data
Chemical formula	C26H26N2S	C24H26N2O2S	C22H20F2N2S	C22H20Cl2N2S
M r	398.55	406.53	382.46	415.36
Crystal system, space group	Triclinic, P1	Monoclinic, C2	Orthorhombic, P21212	Orthorhombic, P21212
Temperature (K)	298	298	298	298
a, b, c (Å)	5.9093 (4), 7.6258 (5), 12.6570 (8)	25.3917 (13), 5.9488 (3), 7.5623 (4)	21.1153 (16), 7.7846 (6), 6.1343 (5)	21.893 (2), 7.9212 (6), 6.2315 (4)
α, β, γ (°)	87.802 (5), 78.329 (5), 87.427 (5)	90, 97.174 (4), 90	90, 90, 90	90, 90, 90
V (Å3)	557.76 (6)	1133.34 (10)	1008.32 (14)	1080.66 (15)
Z	1	2	2	2
Radiation type	Mo Kα	Mo Kα	Mo Kα	Mo Kα
μ (mm−1)	0.16	0.16	0.19	0.41
Crystal size (mm)	0.34 × 0.12 × 0.06	0.45 × 0.33 × 0.12	0.89 × 0.47 × 0.33	0.52 × 0.40 × 0.07
Data collection
Diffractometer	Agilent Xcalibur (Atlas, Gemini)	Agilent Xcalibur (Atlas, Gemini)	Agilent Xcalibur (Atlas, Gemini)	Agilent Xcalibur (Atlas, Gemini)
Absorption correction	Analytical CrysAlis PRO, (Agilent, 2013 ▸)	Analytical (CrysAlis PRO; Agilent, 2013 ▸)	Analytical CrysAlis PRO, (Agilent, 2013 ▸)	Multi-scan CrysAlis PRO, (Agilent, 2013 ▸)
T min, T max	0.969, 0.992	0.973, 0.993	0.904, 0.958	0.692, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections	6689, 4036, 2958	6341, 2221, 1892	12336, 2067, 1591	14195, 2743, 1534
R int	0.040	0.027	0.058	0.058
(sin θ/λ)max (Å−1)	0.618	0.618	0.625	0.692
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S	0.058, 0.127, 1.02	0.036, 0.085, 1.02	0.044, 0.092, 1.06	0.052, 0.117, 1.01
No. of reflections	4036	2221	2067	2743
No. of parameters	262	134	124	124
No. of restraints	3	1	0	0
H-atom treatment	H-atom parameters constrained	H-atom parameters constrained	H-atom parameters constrained	H-atom parameters constrained
Δρmax, Δρmin (e Å−3)	0.31, −0.19	0.11, −0.17	0.15, −0.25	0.13, −0.17
Absolute structure	Flack x determined using 962 quotients [(I +)−(I −)]/[(I +)+(I −)] (Parsons et al., 2013 ▸)	Flack x determined using 708 quotients [(I +)−(I −)]/[(I +)+(I −)] (Parsons et al., 2013 ▸)	Flack x determined using 518 quotients [(I +)−(I −)]/[(I +)+(I −)] (Parsons et al., 2013 ▸)	Flack x determined using 465 quotients [(I +)−(I −)]/[(I +)+(I −)] (Parsons et al., 2013 ▸)
Absolute structure parameter	−0.12 (7)	−0.02 (4)	0.07 (6)	0.10 (6)

Computer programs: CrysAlis PRO (Agilent, 2013 ▸), SHELXS97 (Sheldrick, 2008 ▸), SHELXT (Sheldrick, 2015a ▸), SHELXL2014 (Sheldrick, 2015b ▸) and Mercury (Macrae et al., 2008 ▸).

Crystal structure: contains datablock(s) I, II, III, IV, global. DOI: 10.1107/S2056989016002516/sj5495sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989016002516/sj5495Isup2.hkl

Structure factors: contains datablock(s) II. DOI: 10.1107/S2056989016002516/sj5495IIsup3.hkl

Structure factors: contains datablock(s) III. DOI: 10.1107/S2056989016002516/sj5495IIIsup4.hkl

Structure factors: contains datablock(s) IV. DOI: 10.1107/S2056989016002516/sj5495IVsup5.hkl

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989016002516/sj5495Isup6.cml

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989016002516/sj5495IIsup7.cml

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989016002516/sj5495IIIsup8.cml

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989016002516/sj5495IVsup9.cml

CCDC references: 1452795, 1452794, 1452793, 1452792

Additional supporting information: crystallographic information; 3D view; checkCIF report

C26H26N2S	F(000) = 212
Mr = 398.55	Dx = 1.187 Mg m−3
Triclinic, P1	Melting point: 437 K
a = 5.9093 (4) Å	Mo Kα radiation, λ = 0.71073 Å
b = 7.6258 (5) Å	Cell parameters from 2148 reflections
c = 12.6570 (8) Å	θ = 3.3–22.6°
α = 87.802 (5)°	µ = 0.16 mm−1
β = 78.329 (5)°	T = 298 K
γ = 87.427 (5)°	Plate, colorless
V = 557.76 (6) Å3	0.34 × 0.12 × 0.06 mm
Z = 1

Agilent Xcalibur (Atlas, Gemini) diffractometer	4036 independent reflections
Radiation source: Enhance (Mo) X-ray Source	2958 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.040
Detector resolution: 10.5564 pixels mm-1	θmax = 26.1°, θmin = 3.1°
ω scans	h = −7→7
Absorption correction: analytical CrysAlis PRO, (Agilent, 2013)	k = −9→9
Tmin = 0.969, Tmax = 0.992	l = −15→15
6689 measured reflections

Refinement on F2	Secondary atom site location: difference Fourier map
Least-squares matrix: full	Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058	H-atom parameters constrained
wR(F2) = 0.127	w = 1/[σ2(Fo2) + (0.0525P)2] where P = (Fo2 + 2Fc2)/3
S = 1.02	(Δ/σ)max < 0.001
4036 reflections	Δρmax = 0.31 e Å−3
262 parameters	Δρmin = −0.19 e Å−3
3 restraints	Absolute structure: Flack x determined using 962 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
0 constraints	Absolute structure parameter: −0.12 (7)
Primary atom site location: structure-invariant direct methods

	x	y	z	Uiso*/Ueq
S1	0.66581 (19)	0.49640 (17)	0.11819 (12)	0.0488 (4)
N1	0.5097 (7)	0.7980 (6)	0.2625 (3)	0.0507 (12)
C2	0.7239 (10)	0.7657 (7)	0.2474 (4)	0.0490 (13)
H2A	0.8132	0.8300	0.2834	0.059*
C3	0.8355 (8)	0.6297 (7)	0.1747 (4)	0.0469 (13)
C4	1.0622 (9)	0.5892 (7)	0.1402 (5)	0.0575 (15)
H4A	1.1792	0.6461	0.1628	0.069*
C5	1.1042 (8)	0.4510 (7)	0.0658 (5)	0.0595 (15)
H5A	1.2513	0.4075	0.0348	0.071*
C6	0.9068 (8)	0.3894 (6)	0.0450 (4)	0.0425 (12)
C7	0.8786 (9)	0.2528 (7)	−0.0268 (4)	0.0503 (14)
H7A	1.0094	0.1943	−0.0651	0.060*
N8	0.6816 (8)	0.2106 (6)	−0.0390 (3)	0.0518 (12)
C9	0.4190 (9)	0.9453 (7)	0.3325 (4)	0.0518 (13)
H9A	0.5365	0.9745	0.3730	0.062*
C10	0.3728 (12)	1.1032 (8)	0.2631 (5)	0.0772 (18)
H10A	0.2751	1.0713	0.2143	0.093*
H10B	0.5174	1.1431	0.2201	0.093*
C11	0.2537 (13)	1.2501 (8)	0.3345 (5)	0.0802 (19)
H11A	0.3449	1.2749	0.3875	0.096*
H11B	0.2407	1.3560	0.2909	0.096*
C12	0.0161 (11)	1.1958 (8)	0.3911 (5)	0.0682 (18)
H12A	−0.0468	1.2796	0.4462	0.082*
H12B	−0.0847	1.1991	0.3393	0.082*
C13	0.0174 (9)	1.0143 (7)	0.4429 (4)	0.0486 (14)
C14	−0.1721 (10)	0.9610 (9)	0.5196 (5)	0.0620 (16)
H14A	−0.2950	1.0410	0.5406	0.074*
C15	−0.1846 (11)	0.7955 (9)	0.5651 (5)	0.0749 (18)
H15A	−0.3143	0.7635	0.6159	0.090*
C16	−0.0009 (13)	0.6756 (9)	0.5347 (6)	0.080 (2)
H16A	−0.0068	0.5621	0.5644	0.095*
C17	0.1892 (11)	0.7268 (8)	0.4602 (5)	0.0665 (16)
H17A	0.3134	0.6471	0.4414	0.080*
C18	0.2020 (8)	0.8935 (7)	0.4123 (4)	0.0465 (12)
C19	0.6721 (9)	0.0655 (6)	−0.1121 (4)	0.0498 (13)
H19A	0.8294	0.0400	−0.1523	0.060*
C20	0.5911 (13)	−0.0955 (8)	−0.0465 (5)	0.0728 (17)
H20A	0.4515	−0.0668	0.0058	0.087*
H20B	0.7086	−0.1390	−0.0075	0.087*
C21	0.5425 (13)	−0.2380 (8)	−0.1206 (5)	0.0755 (19)
H21A	0.6802	−0.2628	−0.1750	0.091*
H21B	0.5024	−0.3453	−0.0786	0.091*
C22	0.3465 (11)	−0.1769 (9)	−0.1746 (5)	0.0688 (18)
H22A	0.3350	−0.2584	−0.2300	0.083*
H22B	0.2028	−0.1782	−0.1216	0.083*
C23	0.3768 (9)	0.0051 (8)	−0.2248 (4)	0.0503 (14)
C24	0.2515 (10)	0.0601 (9)	−0.3022 (4)	0.0624 (15)
H24A	0.1532	−0.0175	−0.3233	0.075*
C25	0.2684 (12)	0.2252 (10)	−0.3484 (5)	0.079 (2)
H25A	0.1830	0.2591	−0.4004	0.095*
C26	0.4143 (14)	0.3418 (9)	−0.3167 (6)	0.086 (2)
H26A	0.4269	0.4550	−0.3469	0.103*
C27	0.5398 (11)	0.2877 (8)	−0.2403 (5)	0.0671 (17)
H27A	0.6391	0.3653	−0.2199	0.080*
C28	0.5226 (8)	0.1213 (7)	−0.1928 (4)	0.0484 (13)

	U11	U22	U33	U12	U13	U23
S1	0.0351 (7)	0.0574 (8)	0.0551 (7)	−0.0009 (5)	−0.0088 (5)	−0.0201 (6)
N1	0.045 (3)	0.058 (3)	0.049 (3)	0.004 (2)	−0.006 (2)	−0.026 (2)
C2	0.049 (3)	0.055 (3)	0.047 (3)	−0.007 (3)	−0.013 (2)	−0.016 (3)
C3	0.039 (3)	0.058 (3)	0.048 (3)	−0.002 (2)	−0.016 (2)	−0.014 (3)
C4	0.036 (3)	0.071 (4)	0.070 (4)	0.000 (3)	−0.017 (3)	−0.027 (3)
C5	0.033 (3)	0.075 (4)	0.072 (4)	0.005 (3)	−0.010 (2)	−0.031 (3)
C6	0.031 (3)	0.050 (3)	0.046 (3)	0.004 (2)	−0.006 (2)	−0.011 (2)
C7	0.046 (3)	0.057 (3)	0.048 (3)	0.010 (3)	−0.007 (2)	−0.018 (3)
N8	0.048 (3)	0.059 (3)	0.050 (3)	−0.003 (2)	−0.008 (2)	−0.023 (2)
C9	0.049 (3)	0.053 (3)	0.054 (3)	−0.001 (3)	−0.009 (3)	−0.022 (3)
C10	0.102 (5)	0.061 (4)	0.060 (4)	−0.002 (3)	0.005 (3)	−0.015 (3)
C11	0.109 (5)	0.050 (4)	0.070 (4)	0.005 (3)	0.010 (4)	−0.007 (3)
C12	0.082 (5)	0.062 (4)	0.060 (4)	0.024 (3)	−0.015 (3)	−0.022 (3)
C13	0.048 (3)	0.057 (3)	0.043 (3)	0.002 (3)	−0.012 (3)	−0.016 (3)
C14	0.056 (3)	0.075 (4)	0.056 (3)	0.009 (3)	−0.009 (3)	−0.027 (3)
C15	0.075 (4)	0.082 (5)	0.062 (4)	−0.011 (4)	0.006 (3)	−0.022 (4)
C16	0.104 (5)	0.061 (4)	0.066 (4)	−0.012 (4)	0.001 (4)	−0.002 (4)
C17	0.072 (4)	0.059 (4)	0.064 (4)	0.007 (3)	−0.003 (3)	−0.011 (3)
C18	0.045 (3)	0.054 (3)	0.043 (3)	0.001 (3)	−0.012 (2)	−0.019 (3)
C19	0.052 (3)	0.053 (3)	0.044 (3)	0.000 (3)	−0.007 (2)	−0.017 (3)
C20	0.114 (5)	0.060 (4)	0.051 (3)	−0.010 (4)	−0.030 (3)	−0.011 (3)
C21	0.119 (5)	0.055 (4)	0.056 (4)	−0.012 (4)	−0.021 (4)	−0.009 (3)
C22	0.074 (4)	0.078 (5)	0.056 (4)	−0.028 (4)	−0.008 (3)	−0.017 (3)
C23	0.048 (3)	0.057 (3)	0.043 (3)	−0.007 (3)	0.001 (3)	−0.019 (3)
C24	0.056 (3)	0.079 (4)	0.054 (3)	0.003 (3)	−0.013 (3)	−0.028 (3)
C25	0.096 (5)	0.084 (5)	0.066 (4)	0.026 (4)	−0.037 (4)	−0.028 (4)
C26	0.129 (6)	0.057 (4)	0.080 (5)	0.016 (4)	−0.044 (5)	−0.010 (4)
C27	0.084 (4)	0.059 (4)	0.064 (4)	−0.003 (3)	−0.022 (4)	−0.019 (3)
C28	0.050 (3)	0.046 (3)	0.049 (3)	0.006 (2)	−0.006 (2)	−0.018 (3)

S1—C6	1.724 (5)	C14—H14A	0.9300
S1—C3	1.728 (5)	C15—C16	1.390 (9)
N1—C2	1.255 (6)	C15—H15A	0.9300
N1—C9	1.471 (6)	C16—C17	1.373 (9)
C2—C3	1.458 (7)	C16—H16A	0.9300
C2—H2A	0.9300	C17—C18	1.386 (8)
C3—C4	1.348 (7)	C17—H17A	0.9300
C4—C5	1.420 (7)	C19—C20	1.496 (7)
C4—H4A	0.9300	C19—C28	1.518 (7)
C5—C6	1.355 (6)	C19—H19A	0.9800
C5—H5A	0.9300	C20—C21	1.536 (8)
C6—C7	1.445 (7)	C20—H20A	0.9700
C7—N8	1.263 (6)	C20—H20B	0.9700
C7—H7A	0.9300	C21—C22	1.508 (9)
N8—C19	1.479 (6)	C21—H21A	0.9700
C9—C10	1.512 (8)	C21—H21B	0.9700
C9—C18	1.520 (7)	C22—C23	1.507 (9)
C9—H9A	0.9800	C22—H22A	0.9700
C10—C11	1.522 (8)	C22—H22B	0.9700
C10—H10A	0.9700	C23—C24	1.384 (8)
C10—H10B	0.9700	C23—C28	1.389 (7)
C11—C12	1.510 (9)	C24—C25	1.367 (9)
C11—H11A	0.9700	C24—H24A	0.9300
C11—H11B	0.9700	C25—C26	1.390 (10)
C12—C13	1.509 (8)	C25—H25A	0.9300
C12—H12A	0.9700	C26—C27	1.374 (8)
C12—H12B	0.9700	C26—H26A	0.9300
C13—C14	1.390 (8)	C27—C28	1.382 (7)
C13—C18	1.398 (7)	C27—H27A	0.9300
C14—C15	1.366 (9)
C6—S1—C3	91.5 (2)	C16—C15—H15A	120.4
C2—N1—C9	116.5 (4)	C17—C16—C15	119.2 (7)
N1—C2—C3	121.5 (5)	C17—C16—H16A	120.4
N1—C2—H2A	119.3	C15—C16—H16A	120.4
C3—C2—H2A	119.3	C16—C17—C18	122.1 (6)
C4—C3—C2	129.7 (5)	C16—C17—H17A	119.0
C4—C3—S1	111.3 (4)	C18—C17—H17A	119.0
C2—C3—S1	119.1 (4)	C17—C18—C13	118.7 (5)
C3—C4—C5	113.2 (5)	C17—C18—C9	120.0 (5)
C3—C4—H4A	123.4	C13—C18—C9	121.2 (5)
C5—C4—H4A	123.4	N8—C19—C20	109.4 (4)
C6—C5—C4	112.6 (5)	N8—C19—C28	110.1 (4)
C6—C5—H5A	123.7	C20—C19—C28	113.3 (4)
C4—C5—H5A	123.7	N8—C19—H19A	108.0
C5—C6—C7	129.0 (5)	C20—C19—H19A	108.0
C5—C6—S1	111.4 (4)	C28—C19—H19A	108.0
C7—C6—S1	119.6 (4)	C19—C20—C21	109.9 (4)
N8—C7—C6	121.9 (5)	C19—C20—H20A	109.7
N8—C7—H7A	119.1	C21—C20—H20A	109.7
C6—C7—H7A	119.1	C19—C20—H20B	109.7
C7—N8—C19	117.5 (4)	C21—C20—H20B	109.7
N1—C9—C10	109.1 (4)	H20A—C20—H20B	108.2
N1—C9—C18	110.3 (4)	C22—C21—C20	109.9 (5)
C10—C9—C18	111.6 (5)	C22—C21—H21A	109.7
N1—C9—H9A	108.6	C20—C21—H21A	109.7
C10—C9—H9A	108.6	C22—C21—H21B	109.7
C18—C9—H9A	108.6	C20—C21—H21B	109.7
C9—C10—C11	109.6 (5)	H21A—C21—H21B	108.2
C9—C10—H10A	109.7	C23—C22—C21	112.9 (5)
C11—C10—H10A	109.7	C23—C22—H22A	109.0
C9—C10—H10B	109.7	C21—C22—H22A	109.0
C11—C10—H10B	109.7	C23—C22—H22B	109.0
H10A—C10—H10B	108.2	C21—C22—H22B	109.0
C12—C11—C10	109.6 (5)	H22A—C22—H22B	107.8
C12—C11—H11A	109.7	C24—C23—C28	119.1 (5)
C10—C11—H11A	109.7	C24—C23—C22	119.5 (5)
C12—C11—H11B	109.7	C28—C23—C22	121.4 (5)
C10—C11—H11B	109.7	C25—C24—C23	121.8 (6)
H11A—C11—H11B	108.2	C25—C24—H24A	119.1
C13—C12—C11	112.9 (5)	C23—C24—H24A	119.1
C13—C12—H12A	109.0	C24—C25—C26	119.3 (6)
C11—C12—H12A	109.0	C24—C25—H25A	120.4
C13—C12—H12B	109.0	C26—C25—H25A	120.4
C11—C12—H12B	109.0	C27—C26—C25	119.1 (6)
H12A—C12—H12B	107.8	C27—C26—H26A	120.4
C14—C13—C18	118.4 (5)	C25—C26—H26A	120.4
C14—C13—C12	120.1 (5)	C26—C27—C28	121.9 (6)
C18—C13—C12	121.5 (5)	C26—C27—H27A	119.1
C15—C14—C13	122.5 (6)	C28—C27—H27A	119.1
C15—C14—H14A	118.8	C27—C28—C23	118.8 (5)
C13—C14—H14A	118.8	C27—C28—C19	119.8 (5)
C14—C15—C16	119.1 (6)	C23—C28—C19	121.3 (5)
C14—C15—H15A	120.4
C9—N1—C2—C3	−176.4 (5)	C12—C13—C18—C17	−177.8 (5)
N1—C2—C3—C4	172.4 (6)	C14—C13—C18—C9	−177.3 (5)
N1—C2—C3—S1	−6.2 (7)	C12—C13—C18—C9	5.4 (7)
C6—S1—C3—C4	−1.4 (5)	N1—C9—C18—C17	39.8 (6)
C6—S1—C3—C2	177.5 (4)	C10—C9—C18—C17	161.1 (5)
C2—C3—C4—C5	−177.8 (5)	N1—C9—C18—C13	−143.5 (4)
S1—C3—C4—C5	0.9 (6)	C10—C9—C18—C13	−22.1 (6)
C3—C4—C5—C6	0.2 (7)	C7—N8—C19—C20	105.5 (6)
C4—C5—C6—C7	178.9 (5)	C7—N8—C19—C28	−129.5 (5)
C4—C5—C6—S1	−1.3 (6)	N8—C19—C20—C21	170.8 (5)
C3—S1—C6—C5	1.5 (4)	C28—C19—C20—C21	47.7 (7)
C3—S1—C6—C7	−178.7 (4)	C19—C20—C21—C22	−64.0 (7)
C5—C6—C7—N8	−179.1 (6)	C20—C21—C22—C23	49.0 (7)
S1—C6—C7—N8	1.1 (7)	C21—C22—C23—C24	161.6 (5)
C6—C7—N8—C19	−178.2 (5)	C21—C22—C23—C28	−20.5 (8)
C2—N1—C9—C10	102.3 (6)	C28—C23—C24—C25	0.4 (8)
C2—N1—C9—C18	−134.9 (5)	C22—C23—C24—C25	178.4 (6)
N1—C9—C10—C11	173.7 (5)	C23—C24—C25—C26	−0.3 (9)
C18—C9—C10—C11	51.6 (7)	C24—C25—C26—C27	0.5 (10)
C9—C10—C11—C12	−66.2 (7)	C25—C26—C27—C28	−0.9 (10)
C10—C11—C12—C13	48.1 (7)	C26—C27—C28—C23	1.0 (8)
C11—C12—C13—C14	164.1 (5)	C26—C27—C28—C19	177.5 (6)
C11—C12—C13—C18	−18.7 (8)	C24—C23—C28—C27	−0.7 (7)
C18—C13—C14—C15	−0.5 (8)	C22—C23—C28—C27	−178.7 (6)
C12—C13—C14—C15	176.8 (5)	C24—C23—C28—C19	−177.2 (5)
C13—C14—C15—C16	0.5 (9)	C22—C23—C28—C19	4.9 (8)
C14—C15—C16—C17	0.5 (10)	N8—C19—C28—C27	41.7 (6)
C15—C16—C17—C18	−1.6 (10)	C20—C19—C28—C27	164.5 (5)
C16—C17—C18—C13	1.6 (9)	N8—C19—C28—C23	−141.9 (5)
C16—C17—C18—C9	178.4 (6)	C20—C19—C28—C23	−19.1 (7)
C14—C13—C18—C17	−0.5 (7)

D—H···A	D—H	H···A	D···A	D—H···A
C4—H4A···S1i	0.93	3.00	3.562 (5)	121
C5—H5A···S1i	0.93	2.97	3.547 (5)	122

C24H26N2O2S	Dx = 1.191 Mg m−3
Mr = 406.53	Melting point: 405 K
Monoclinic, C2	Mo Kα radiation, λ = 0.71073 Å
a = 25.3917 (13) Å	Cell parameters from 2504 reflections
b = 5.9488 (3) Å	θ = 3.0–24.2°
c = 7.5623 (4) Å	µ = 0.16 mm−1
β = 97.174 (4)°	T = 298 K
V = 1133.34 (10) Å3	Prism, colourless
Z = 2	0.45 × 0.33 × 0.12 mm
F(000) = 432

Agilent Xcalibur (Atlas, Gemini) diffractometer	2221 independent reflections
Radiation source: Enhance (Mo) X-ray Source	1892 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.027
ω scans	θmax = 26.1°, θmin = 3.0°
Absorption correction: analytical (CrysAlis PRO; Agilent, 2013)	h = −31→31
Tmin = 0.973, Tmax = 0.993	k = −7→7
6341 measured reflections	l = −9→9

Refinement on F2	Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: full	H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.036	w = 1/[σ2(Fo2) + (0.0393P)2 + 0.1801P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.085	(Δ/σ)max < 0.001
S = 1.02	Δρmax = 0.11 e Å−3
2221 reflections	Δρmin = −0.17 e Å−3
134 parameters	Absolute structure: Flack x determined using 708 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
1 restraint	Absolute structure parameter: −0.02 (4)

	x	y	z	Uiso*/Ueq
S1	0.5000	0.37429 (14)	0.5000	0.0490 (3)
N1	0.56565 (9)	0.3213 (4)	0.1855 (3)	0.0471 (6)
C2	0.55195 (11)	0.5176 (5)	0.2189 (4)	0.0469 (7)
H2A	0.5608	0.6324	0.1445	0.056*
C3	0.52314 (10)	0.5774 (5)	0.3665 (4)	0.0449 (6)
C4	0.51313 (13)	0.7856 (5)	0.4229 (4)	0.0596 (8)
H4A	0.5225	0.9159	0.3665	0.072*
C5	0.59848 (11)	0.2933 (4)	0.0386 (4)	0.0484 (7)
H5A	0.5949	0.4291	−0.0354	0.058*
C6	0.57863 (13)	0.0963 (6)	−0.0754 (4)	0.0658 (8)
H6A	0.5416	0.1162	−0.1164	0.099*
H6B	0.5835	−0.0394	−0.0065	0.099*
H6C	0.5981	0.0861	−0.1759	0.099*
C7	0.65613 (11)	0.2719 (4)	0.1189 (3)	0.0441 (6)
C8	0.69277 (11)	0.4349 (4)	0.0871 (4)	0.0494 (7)
H8A	0.6817	0.5585	0.0168	0.059*
C9	0.74515 (11)	0.4171 (5)	0.1576 (4)	0.0571 (8)
H9A	0.7692	0.5278	0.1343	0.069*
C10	0.76215 (11)	0.2354 (6)	0.2628 (4)	0.0546 (7)
C11	0.72642 (12)	0.0745 (6)	0.2994 (4)	0.0593 (8)
H11A	0.7375	−0.0469	0.3722	0.071*
C12	0.67374 (12)	0.0936 (6)	0.2275 (4)	0.0551 (8)
H12A	0.6497	−0.0161	0.2528	0.066*
O1	0.81556 (9)	0.2307 (5)	0.3227 (3)	0.0781 (7)
C13	0.83539 (15)	0.0345 (9)	0.4189 (5)	0.1010 (15)
H13A	0.8734	0.0434	0.4432	0.152*
H13B	0.8257	−0.0970	0.3487	0.152*
H13C	0.8204	0.0258	0.5292	0.152*

	U11	U22	U33	U12	U13	U23
S1	0.0540 (6)	0.0354 (5)	0.0603 (6)	0.000	0.0183 (4)	0.000
N1	0.0442 (13)	0.0512 (16)	0.0477 (13)	0.0014 (10)	0.0129 (10)	0.0058 (10)
C2	0.0460 (15)	0.0443 (18)	0.0507 (16)	−0.0021 (13)	0.0071 (13)	0.0121 (13)
C3	0.0421 (14)	0.0392 (14)	0.0534 (17)	−0.0002 (12)	0.0062 (13)	0.0052 (12)
C4	0.074 (2)	0.0365 (16)	0.071 (2)	0.0007 (13)	0.0193 (16)	0.0074 (13)
C5	0.0497 (16)	0.0537 (18)	0.0434 (15)	0.0015 (12)	0.0120 (12)	0.0097 (12)
C6	0.0626 (19)	0.079 (2)	0.0551 (19)	−0.0010 (18)	0.0058 (15)	−0.0036 (17)
C7	0.0468 (15)	0.0492 (15)	0.0387 (14)	0.0022 (13)	0.0147 (12)	0.0018 (12)
C8	0.0559 (17)	0.0500 (17)	0.0451 (14)	−0.0025 (13)	0.0169 (13)	0.0045 (12)
C9	0.0528 (17)	0.067 (2)	0.0548 (17)	−0.0139 (16)	0.0177 (14)	−0.0004 (16)
C10	0.0455 (16)	0.078 (2)	0.0414 (16)	0.0001 (15)	0.0080 (13)	−0.0080 (15)
C11	0.0575 (18)	0.068 (2)	0.0524 (18)	0.0087 (17)	0.0086 (14)	0.0150 (15)
C12	0.0527 (17)	0.0569 (17)	0.0574 (19)	−0.0031 (14)	0.0138 (14)	0.0147 (15)
O1	0.0478 (13)	0.121 (2)	0.0642 (14)	−0.0021 (14)	0.0011 (10)	−0.0011 (14)
C13	0.063 (2)	0.161 (4)	0.075 (3)	0.022 (3)	−0.0086 (19)	0.022 (3)

S1—C3i	1.724 (3)	C7—C12	1.381 (4)
S1—C3	1.724 (3)	C7—C8	1.385 (3)
N1—C2	1.253 (3)	C8—C9	1.374 (4)
N1—C5	1.480 (3)	C8—H8A	0.9300
C2—C3	1.453 (4)	C9—C10	1.379 (4)
C2—H2A	0.9300	C9—H9A	0.9300
C3—C4	1.345 (4)	C10—C11	1.371 (4)
C4—C4i	1.413 (6)	C10—O1	1.375 (3)
C4—H4A	0.9300	C11—C12	1.384 (4)
C5—C6	1.504 (4)	C11—H11A	0.9300
C5—C7	1.519 (4)	C12—H12A	0.9300
C5—H5A	0.9800	O1—C13	1.433 (5)
C6—H6A	0.9600	C13—H13A	0.9600
C6—H6B	0.9600	C13—H13B	0.9600
C6—H6C	0.9600	C13—H13C	0.9600
C3i—S1—C3	91.01 (19)	C12—C7—C5	121.8 (2)
C2—N1—C5	116.9 (2)	C8—C7—C5	120.4 (2)
N1—C2—C3	124.2 (3)	C9—C8—C7	121.2 (3)
N1—C2—H2A	117.9	C9—C8—H8A	119.4
C3—C2—H2A	117.9	C7—C8—H8A	119.4
C4—C3—C2	127.1 (3)	C8—C9—C10	120.1 (3)
C4—C3—S1	111.6 (2)	C8—C9—H9A	119.9
C2—C3—S1	121.3 (2)	C10—C9—H9A	119.9
C3—C4—C4i	112.91 (17)	C11—C10—O1	124.7 (3)
C3—C4—H4A	123.5	C11—C10—C9	119.8 (3)
C4i—C4—H4A	123.5	O1—C10—C9	115.5 (3)
N1—C5—C6	109.7 (2)	C10—C11—C12	119.7 (3)
N1—C5—C7	108.3 (2)	C10—C11—H11A	120.2
C6—C5—C7	113.7 (2)	C12—C11—H11A	120.2
N1—C5—H5A	108.3	C7—C12—C11	121.5 (3)
C6—C5—H5A	108.3	C7—C12—H12A	119.3
C7—C5—H5A	108.3	C11—C12—H12A	119.3
C5—C6—H6A	109.5	C10—O1—C13	117.0 (3)
C5—C6—H6B	109.5	O1—C13—H13A	109.5
H6A—C6—H6B	109.5	O1—C13—H13B	109.5
C5—C6—H6C	109.5	H13A—C13—H13B	109.5
H6A—C6—H6C	109.5	O1—C13—H13C	109.5
H6B—C6—H6C	109.5	H13A—C13—H13C	109.5
C12—C7—C8	117.8 (3)	H13B—C13—H13C	109.5
C5—N1—C2—C3	−175.3 (2)	C12—C7—C8—C9	1.5 (4)
N1—C2—C3—C4	171.0 (3)	C5—C7—C8—C9	−179.4 (3)
N1—C2—C3—S1	−5.7 (4)	C7—C8—C9—C10	−0.3 (4)
C3i—S1—C3—C4	−0.22 (17)	C8—C9—C10—C11	−1.1 (4)
C3i—S1—C3—C2	176.9 (3)	C8—C9—C10—O1	178.3 (2)
C2—C3—C4—C4i	−176.3 (3)	O1—C10—C11—C12	−178.1 (3)
S1—C3—C4—C4i	0.6 (4)	C9—C10—C11—C12	1.2 (4)
C2—N1—C5—C6	−136.4 (3)	C8—C7—C12—C11	−1.4 (4)
C2—N1—C5—C7	99.0 (3)	C5—C7—C12—C11	179.6 (3)
N1—C5—C7—C12	63.9 (3)	C10—C11—C12—C7	0.0 (5)
C6—C5—C7—C12	−58.3 (3)	C11—C10—O1—C13	4.8 (4)
N1—C5—C7—C8	−115.0 (3)	C9—C10—O1—C13	−174.6 (3)
C6—C5—C7—C8	122.7 (3)

D—H···A	D—H	H···A	D···A	D—H···A
C4—H4A···S1ii	0.93	2.99	3.572 (3)	122

C22H20F2N2S	Dx = 1.260 Mg m−3
Mr = 382.46	Melting point: 420 K
Orthorhombic, P21212	Mo Kα radiation, λ = 0.71073 Å
a = 21.1153 (16) Å	Cell parameters from 2744 reflections
b = 7.7846 (6) Å	θ = 3.8–23.2°
c = 6.1343 (5) Å	µ = 0.19 mm−1
V = 1008.32 (14) Å3	T = 298 K
Z = 2	Prism, colourless
F(000) = 400	0.89 × 0.47 × 0.33 mm

Agilent Xcalibur (Atlas, Gemini) diffractometer	2067 independent reflections
Radiation source: Enhance (Mo) X-ray Source	1591 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.058
Detector resolution: 10.5564 pixels mm-1	θmax = 26.4°, θmin = 3.8°
ω scans	h = −26→26
Absorption correction: analytical CrysAlis PRO, (Agilent, 2013)	k = −9→9
Tmin = 0.904, Tmax = 0.958	l = −7→7
12336 measured reflections

Refinement on F2	Secondary atom site location: difference Fourier map
Least-squares matrix: full	Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.044	H-atom parameters constrained
wR(F2) = 0.092	w = 1/[σ2(Fo2) + (0.0384P)2 + 0.0613P] where P = (Fo2 + 2Fc2)/3
S = 1.06	(Δ/σ)max < 0.001
2067 reflections	Δρmax = 0.15 e Å−3
124 parameters	Δρmin = −0.25 e Å−3
0 restraints	Absolute structure: Flack x determined using 518 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Primary atom site location: structure-invariant direct methods	Absolute structure parameter: 0.07 (6)

	x	y	z	Uiso*/Ueq
S1	0.5000	0.0000	1.06817 (15)	0.0479 (3)
F1	0.85802 (10)	0.3203 (3)	0.5731 (5)	0.1163 (9)
N1	0.58698 (11)	0.3119 (3)	1.0120 (4)	0.0498 (6)
C2	0.56853 (13)	0.2830 (4)	1.2046 (5)	0.0479 (8)
H2A	0.5795	0.3610	1.3130	0.057*
C3	0.53102 (13)	0.1344 (4)	1.2646 (4)	0.0461 (8)
C4	0.51751 (14)	0.0774 (4)	1.4690 (4)	0.0556 (8)
H4A	0.5300	0.1342	1.5953	0.067*
C5	0.62513 (14)	0.4679 (4)	0.9770 (5)	0.0568 (8)
H5A	0.6336	0.5216	1.1185	0.068*
C6	0.58661 (16)	0.5931 (5)	0.8368 (7)	0.0829 (12)
H6A	0.5476	0.6200	0.9094	0.124*
H6B	0.5777	0.5412	0.6983	0.124*
H6C	0.6105	0.6967	0.8149	0.124*
C7	0.68777 (14)	0.4223 (3)	0.8702 (5)	0.0462 (7)
C8	0.74419 (15)	0.4799 (4)	0.9563 (5)	0.0577 (8)
H8A	0.7436	0.5427	1.0852	0.069*
C9	0.80144 (15)	0.4470 (4)	0.8567 (7)	0.0697 (10)
H9A	0.8391	0.4873	0.9163	0.084*
C10	0.80134 (17)	0.3551 (5)	0.6707 (7)	0.0689 (10)
C11	0.74733 (18)	0.2932 (4)	0.5777 (5)	0.0654 (9)
H11A	0.7489	0.2301	0.4491	0.078*
C12	0.69042 (15)	0.3265 (4)	0.6789 (5)	0.0543 (8)
H12A	0.6532	0.2843	0.6184	0.065*

	U11	U22	U33	U12	U13	U23
S1	0.0499 (6)	0.0559 (6)	0.0379 (5)	−0.0056 (6)	0.000	0.000
F1	0.0687 (14)	0.1167 (19)	0.164 (2)	−0.0047 (14)	0.0485 (15)	−0.030 (2)
N1	0.0452 (14)	0.0502 (15)	0.0540 (16)	−0.0082 (12)	0.0032 (11)	−0.0028 (11)
C2	0.0405 (16)	0.054 (2)	0.0489 (18)	−0.0028 (15)	−0.0043 (14)	−0.0073 (16)
C3	0.0388 (15)	0.0544 (19)	0.0452 (17)	−0.0011 (15)	−0.0013 (13)	−0.0024 (14)
C4	0.056 (2)	0.071 (2)	0.0396 (15)	−0.0115 (15)	−0.0020 (13)	−0.0040 (14)
C5	0.0545 (18)	0.0513 (19)	0.0647 (18)	−0.0104 (16)	0.0112 (15)	−0.0111 (16)
C6	0.065 (2)	0.060 (2)	0.123 (3)	0.0111 (19)	0.023 (2)	0.016 (2)
C7	0.0468 (17)	0.0403 (15)	0.0514 (17)	−0.0063 (14)	0.0002 (14)	0.0001 (13)
C8	0.0576 (19)	0.0492 (17)	0.0662 (19)	−0.0090 (17)	0.0002 (16)	−0.0104 (18)
C9	0.047 (2)	0.064 (2)	0.099 (3)	−0.0114 (17)	−0.0023 (19)	−0.007 (2)
C10	0.054 (2)	0.058 (2)	0.095 (3)	−0.0009 (18)	0.021 (2)	0.001 (2)
C11	0.075 (2)	0.063 (2)	0.0577 (19)	0.000 (2)	0.011 (2)	−0.0053 (18)
C12	0.0499 (18)	0.0573 (19)	0.0557 (18)	−0.0058 (17)	−0.0063 (16)	−0.0020 (16)

S1—C3i	1.725 (3)	C6—H6A	0.9600
S1—C3	1.725 (3)	C6—H6B	0.9600
F1—C10	1.365 (4)	C6—H6C	0.9600
N1—C2	1.264 (4)	C7—C8	1.378 (4)
N1—C5	1.473 (4)	C7—C12	1.392 (4)
C2—C3	1.450 (4)	C8—C9	1.378 (4)
C2—H2A	0.9300	C8—H8A	0.9300
C3—C4	1.360 (4)	C9—C10	1.347 (5)
C4—C4i	1.414 (6)	C9—H9A	0.9300
C4—H4A	0.9300	C10—C11	1.363 (5)
C5—C7	1.518 (4)	C11—C12	1.377 (4)
C5—C6	1.533 (5)	C11—H11A	0.9300
C5—H5A	0.9800	C12—H12A	0.9300
C3i—S1—C3	91.4 (2)	H6A—C6—H6C	109.5
C2—N1—C5	116.8 (3)	H6B—C6—H6C	109.5
N1—C2—C3	123.2 (3)	C8—C7—C12	117.6 (3)
N1—C2—H2A	118.4	C8—C7—C5	120.8 (3)
C3—C2—H2A	118.4	C12—C7—C5	121.6 (3)
C4—C3—C2	127.5 (3)	C7—C8—C9	121.9 (3)
C4—C3—S1	111.5 (2)	C7—C8—H8A	119.1
C2—C3—S1	120.9 (2)	C9—C8—H8A	119.1
C3—C4—C4i	112.81 (18)	C10—C9—C8	118.2 (3)
C3—C4—H4A	123.6	C10—C9—H9A	120.9
C4i—C4—H4A	123.6	C8—C9—H9A	120.9
N1—C5—C7	110.3 (2)	C9—C10—C11	122.9 (3)
N1—C5—C6	108.4 (2)	C9—C10—F1	118.4 (3)
C7—C5—C6	111.6 (2)	C11—C10—F1	118.7 (3)
N1—C5—H5A	108.8	C10—C11—C12	118.4 (3)
C7—C5—H5A	108.8	C10—C11—H11A	120.8
C6—C5—H5A	108.8	C12—C11—H11A	120.8
C5—C6—H6A	109.5	C11—C12—C7	121.1 (3)
C5—C6—H6B	109.5	C11—C12—H12A	119.5
H6A—C6—H6B	109.5	C7—C12—H12A	119.5
C5—C6—H6C	109.5
C5—N1—C2—C3	−179.6 (2)	C6—C5—C7—C12	−67.4 (4)
N1—C2—C3—C4	168.6 (3)	C12—C7—C8—C9	1.0 (5)
N1—C2—C3—S1	−8.7 (4)	C5—C7—C8—C9	−176.9 (3)
C3i—S1—C3—C4	−0.29 (16)	C7—C8—C9—C10	−0.4 (5)
C3i—S1—C3—C2	177.4 (3)	C8—C9—C10—C11	−0.2 (5)
C2—C3—C4—C4i	−176.7 (3)	C8—C9—C10—F1	−179.1 (3)
S1—C3—C4—C4i	0.8 (4)	C9—C10—C11—C12	0.0 (6)
C2—N1—C5—C7	124.5 (3)	F1—C10—C11—C12	179.0 (3)
C2—N1—C5—C6	−113.0 (3)	C10—C11—C12—C7	0.6 (5)
N1—C5—C7—C8	−129.0 (3)	C8—C7—C12—C11	−1.1 (4)
C6—C5—C7—C8	110.4 (3)	C5—C7—C12—C11	176.7 (3)
N1—C5—C7—C12	53.2 (4)

C22H20Cl2N2S	Dx = 1.276 Mg m−3
Mr = 415.36	Melting point: 434 K
Orthorhombic, P21212	Mo Kα radiation, λ = 0.71073 Å
a = 21.893 (2) Å	Cell parameters from 2744 reflections
b = 7.9212 (6) Å	θ = 3.7–21.5°
c = 6.2315 (4) Å	µ = 0.41 mm−1
V = 1080.66 (15) Å3	T = 298 K
Z = 2	Prism, colorless
F(000) = 432	0.52 × 0.40 × 0.07 mm

Agilent Xcalibur (Atlas, Gemini) diffractometer	2743 independent reflections
Radiation source: Enhance (Mo) X-ray Source	1534 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.058
Detector resolution: 10.5564 pixels mm-1	θmax = 29.5°, θmin = 3.3°
ω scans	h = −28→27
Absorption correction: multi-scan CrysAlis PRO, (Agilent, 2013)	k = −10→9
Tmin = 0.692, Tmax = 1.000	l = −8→8
14195 measured reflections

Refinement on F2	Secondary atom site location: difference Fourier map
Least-squares matrix: full	Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.052	H-atom parameters constrained
wR(F2) = 0.117	w = 1/[σ2(Fo2) + (0.0483P)2] where P = (Fo2 + 2Fc2)/3
S = 1.01	(Δ/σ)max < 0.001
2743 reflections	Δρmax = 0.13 e Å−3
124 parameters	Δρmin = −0.17 e Å−3
0 restraints	Absolute structure: Flack x determined using 465 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013)
Primary atom site location: structure-invariant direct methods	Absolute structure parameter: 0.10 (6)

	x	y	z	Uiso*/Ueq
S1	0.5000	1.0000	−0.13764 (18)	0.0590 (4)
Cl1	0.15354 (6)	0.67176 (16)	0.4970 (2)	0.1059 (5)
N1	0.41391 (14)	0.6958 (3)	−0.0839 (5)	0.0612 (8)
C2	0.43185 (16)	0.7244 (4)	−0.2735 (6)	0.0589 (10)
H2A	0.4204	0.6496	−0.3812	0.071*
C3	0.46969 (15)	0.8689 (4)	−0.3311 (5)	0.0544 (9)
C4	0.48309 (16)	0.9247 (4)	−0.5338 (5)	0.0640 (10)
H4A	0.4711	0.8688	−0.6581	0.077*
C5	0.37559 (18)	0.5438 (4)	−0.0520 (7)	0.0677 (11)
H5A	0.3625	0.5021	−0.1927	0.081*
C6	0.4148 (2)	0.4087 (5)	0.0553 (9)	0.0986 (17)
H6A	0.4484	0.3803	−0.0369	0.148*
H6B	0.3905	0.3098	0.0810	0.148*
H6C	0.4302	0.4509	0.1892	0.148*
C7	0.31964 (17)	0.5839 (4)	0.0796 (5)	0.0555 (9)
C8	0.26313 (19)	0.5202 (5)	0.0255 (7)	0.0701 (10)
H8A	0.2593	0.4575	−0.0999	0.084*
C9	0.21198 (19)	0.5464 (5)	0.1512 (7)	0.0735 (11)
H9A	0.1744	0.5020	0.1109	0.088*
C10	0.21746 (18)	0.6384 (5)	0.3351 (6)	0.0640 (10)
C11	0.2728 (2)	0.7062 (5)	0.3945 (6)	0.0691 (10)
H11A	0.2761	0.7692	0.5199	0.083*
C12	0.32346 (18)	0.6802 (4)	0.2665 (5)	0.0623 (9)
H12A	0.3607	0.7276	0.3056	0.075*

	U11	U22	U33	U12	U13	U23
S1	0.0694 (9)	0.0596 (7)	0.0482 (6)	−0.0040 (7)	0.000	0.000
Cl1	0.0878 (9)	0.1061 (9)	0.1238 (10)	0.0069 (7)	0.0384 (8)	0.0026 (9)
N1	0.062 (2)	0.0569 (18)	0.0643 (19)	−0.0089 (15)	0.0064 (15)	0.0009 (14)
C2	0.055 (2)	0.060 (2)	0.061 (2)	0.0015 (17)	−0.0031 (19)	−0.0056 (18)
C3	0.050 (2)	0.060 (2)	0.0523 (19)	0.0004 (17)	−0.0008 (16)	−0.0008 (17)
C4	0.063 (3)	0.080 (2)	0.0487 (18)	−0.0130 (18)	−0.0011 (17)	−0.0059 (17)
C5	0.071 (3)	0.057 (2)	0.075 (2)	−0.0098 (18)	0.015 (2)	−0.0050 (18)
C6	0.085 (3)	0.064 (2)	0.147 (4)	0.011 (2)	0.040 (3)	0.019 (3)
C7	0.061 (2)	0.0442 (17)	0.061 (2)	−0.0052 (17)	−0.0039 (18)	0.0020 (16)
C8	0.073 (3)	0.061 (2)	0.076 (2)	−0.017 (2)	−0.002 (2)	−0.014 (2)
C9	0.063 (3)	0.067 (3)	0.091 (3)	−0.0168 (19)	−0.003 (2)	−0.007 (2)
C10	0.065 (3)	0.056 (2)	0.072 (2)	0.0010 (19)	0.007 (2)	0.007 (2)
C11	0.081 (3)	0.068 (2)	0.059 (2)	−0.002 (2)	−0.003 (2)	−0.0067 (18)
C12	0.059 (2)	0.065 (2)	0.063 (2)	−0.004 (2)	−0.010 (2)	−0.002 (2)

S1—C3	1.724 (3)	C6—H6A	0.9600
S1—C3i	1.724 (3)	C6—H6B	0.9600
Cl1—C10	1.746 (4)	C6—H6C	0.9600
N1—C2	1.265 (4)	C7—C8	1.378 (5)
N1—C5	1.481 (4)	C7—C12	1.394 (4)
C2—C3	1.458 (5)	C8—C9	1.382 (5)
C2—H2A	0.9300	C8—H8A	0.9300
C3—C4	1.370 (4)	C9—C10	1.363 (5)
C4—C4i	1.404 (7)	C9—H9A	0.9300
C4—H4A	0.9300	C10—C11	1.376 (5)
C5—C7	1.508 (5)	C11—C12	1.382 (5)
C5—C6	1.527 (5)	C11—H11A	0.9300
C5—H5A	0.9800	C12—H12A	0.9300
C3—S1—C3i	91.3 (2)	H6A—C6—H6C	109.5
C2—N1—C5	116.6 (3)	H6B—C6—H6C	109.5
N1—C2—C3	123.2 (3)	C8—C7—C12	117.3 (4)
N1—C2—H2A	118.4	C8—C7—C5	121.3 (3)
C3—C2—H2A	118.4	C12—C7—C5	121.4 (3)
C4—C3—C2	127.0 (3)	C7—C8—C9	122.2 (4)
C4—C3—S1	111.6 (3)	C7—C8—H8A	118.9
C2—C3—S1	121.3 (2)	C9—C8—H8A	118.9
C3—C4—C4i	112.8 (2)	C10—C9—C8	119.0 (4)
C3—C4—H4A	123.6	C10—C9—H9A	120.5
C4i—C4—H4A	123.6	C8—C9—H9A	120.5
N1—C5—C7	111.2 (3)	C9—C10—C11	120.8 (4)
N1—C5—C6	108.1 (3)	C9—C10—Cl1	119.8 (3)
C7—C5—C6	111.5 (3)	C11—C10—Cl1	119.4 (3)
N1—C5—H5A	108.7	C10—C11—C12	119.5 (3)
C7—C5—H5A	108.7	C10—C11—H11A	120.2
C6—C5—H5A	108.7	C12—C11—H11A	120.2
C5—C6—H6A	109.5	C11—C12—C7	121.0 (4)
C5—C6—H6B	109.5	C11—C12—H12A	119.5
H6A—C6—H6B	109.5	C7—C12—H12A	119.5
C5—C6—H6C	109.5
C5—N1—C2—C3	179.8 (3)	C6—C5—C7—C12	74.9 (4)
N1—C2—C3—C4	−168.8 (4)	C12—C7—C8—C9	−1.2 (5)
N1—C2—C3—S1	7.3 (5)	C5—C7—C8—C9	175.8 (3)
C3i—S1—C3—C4	0.42 (19)	C7—C8—C9—C10	0.0 (6)
C3i—S1—C3—C2	−176.3 (4)	C8—C9—C10—C11	0.8 (6)
C2—C3—C4—C4i	175.3 (4)	C8—C9—C10—Cl1	−179.6 (3)
S1—C3—C4—C4i	−1.1 (5)	C9—C10—C11—C12	−0.3 (6)
C2—N1—C5—C7	−132.2 (3)	Cl1—C10—C11—C12	−179.9 (3)
C2—N1—C5—C6	105.1 (4)	C10—C11—C12—C7	−1.0 (6)
N1—C5—C7—C8	137.3 (4)	C8—C7—C12—C11	1.7 (5)
C6—C5—C7—C8	−102.0 (4)	C5—C7—C12—C11	−175.3 (3)
N1—C5—C7—C12	−45.8 (4)