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

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COMMUNICATIONS
ISSN: 2056-9890

Structural elucidation and Hirshfeld surface analysis of a fused thio­phene ester: methyl 3-[(naphtho­[2,1-b]thio­phen-5-yl)meth­yl]-1-benzo­thio­phene-2-carboxyl­ate

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aDepartment of Physics, SRM Institute of Science and Technology, Ramapuram, Bharathi Salai, Chennai 600089, Tamilnadu, India, and bDepartment of Organic Chemistry, University of Madras, Guindy Campus, Chennai - 600 025, Tamilnadu, India
*Correspondence e-mail: [email protected]

Edited by M. Weil, Vienna University of Technology, Austria (Received 8 January 2026; accepted 28 February 2026; online 5 March 2026)

The title compound, C23H16O2S2, is a benzo[b]thio­phene-2-carboxyl­ate derivative and consists of naphtho­thio­phene and benzo­thio­phene moieties bridged by a methyl­ene group. The dihedral angle between the two aromatic ring systems is 88.5 (2)°. Intra­molecular C—H⋯O inter­actions generate an S(6) ring motif. The acetate group assumes an extended conformation. Weak C—H⋯π and ππ stacking inter­actions are present in the crystal structure, together with a short S⋯S inter­action of 3.77 (8) Å. A Hirshfeld surface analysis indicates that H⋯H inter­actions contribute the most to the crystal packing (34.9%).Please give email addresses for all authors

1. Chemical context

Benzo­thio­phenes are important components of organic semiconductors (OSCs) due to their potential for elongated and highly delocalized electronic structures (Huang et al., 2012View full citation). OSCs have consistently attracted attention for their distinctive properties, such as mechanical flexibility and chemical versatility (Katz et al., 2001View full citation). In this regard, benzothieno[3,2-b]benzo­thio­phene derivatives are also highly promising materials for organic light-emitting diodes (OLEDs) (Izawa et al., 2009View full citation) and organic field-effect transistors (OFET). In this context, we present here the synthesis, crystal structure and Hirshfeld surface analysis of the benzo­thio­phene derivative C23H16O2S2.

[Scheme 1]

2. Structural commentary

The mol­ecular structure of the title compound is displayed in Fig. 1[link]. The naphtho­thio­phene group makes a dihedral angle of 88.5 (2)° with the benzo­thio­phene group. Atom S2 deviates by 0.064 (1) Å from the least-squares plane of the naphtho­thio­phene group; atom C8 deviates by −0.018 (2) Å from the least-squares plane of the benzo­thio­phene group, most probably due to the bulky substitution by an acetate moiety. The latter assumes an extended conformation as can be seen from the C10—O2—C9—C8 torsion angle of −175.2 (2)°. The benzo­thio­phene-2-carboxyl­ate moiety is nearly planar, with the largest deviation from the least-squares plane of 0.011 (2) Å for atom C7. The mol­ecular conformation is stabilized by a weak intra­molecular C11—H11B⋯O1hydrogen bond involving the methyl­ene group (C11) and the keto group (C9=O1) (Table 1[link], Fig. 2[link]), which generates an S(6) ring motif (Bernstein et al., 1995View full citation).

Table 1
Hydrogen-bond geometry (Å, °)

Cg2 and Cg4 are the centroids of the S2/C19/C20/C22/C23 and C12/C13/C18-C21 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C11—H11B⋯O1 0.97 2.44 3.007 (3) 117
C10—H10ACg2i 0.96 2.86 3.397 (3) 116
C17—H17⋯Cg4ii 0.93 2.98 3.689 (2) 134
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation.
[Figure 1]
Figure 1
The mol­ecular structure of the title compound showing the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2]
Figure 2
C—H⋯π and intra­molecular C—H⋯O inter­action (dashed line) in the title structure.

3. Supra­molecular features

There are no hydrogen-bonding inter­actions in the crystal. Instead, C—H⋯Cg inter­actions (Cg is the centre of gravity of an aromatic ring) are present, viz. C10—H10ACg2i between the methyl group and the thio­phene ring (S2/C19/C20/C22/C23) attached to the naptho group, and C17—H17⋯Cg4ii between a carbon atom of the naptho group and the central phenyl ring (C12/C13/C18-C21) of an adjacent naphtho­thio­phene group (Table 1[link], Fig. 2[link]). In addition, ππ stacking is realized (Fig. 3[link]) between the thio­phene ring of the benzo­thio­phene group (Cg1; S1,C1,C6–C8) and the phenyl ring (Cg3; C1–C6) of the benzo­thio­phene group of an adjacent mol­ecule (symmetry code: 2 − x, −y, 1 − z) at a Cg1⋯Cg3 distance of 3.9275 (2) Å with a slippage of 1.705 (3) Å. The mol­ecular packing is shown in Fig. 4[link].

[Figure 3]
Figure 3
Relevant ππ inter­actions in the crystal of the title compound.
[Figure 4]
Figure 4
The mol­ecular packing viewed down the a axis.

4. Hirshfeld surface analysis

Hirshfeld surface (HS) analysis (Hirshfeld, 1977View full citation) was carried out using CrystalExplorer (Spackman et al., 2021View full citation). In the HS plotted over dnorm, the white surface indicates contacts with distances equal to the sum of the van der Waals radii, and the red and blue colours indicate distances shorter (in close contact) or longer (distinct contacts) than the van der Waals radii, respectively (Venkatesan et al., 2016View full citation). The Hirshfeld surfaces plotted over different qu­anti­ties are depicted in Fig. 5[link]. Two-dimensional fingerprint plots showing the occurrence of all inter­molecular contacts (McKinnon et al., 2007View full citation) are presented in Fig. 6[link]. The most important inter­action originates from H⋯H contacts, contributing 34.9% to the overall crystal packing, which is reflected as widely scattered points of high density due to the large hydrogen content of the mol­ecule. Almost as significant is the contribution from the C⋯H/H⋯C inter­actions (33.0%), indicating that the C—H⋯π inter­actions contribute significantly, likely hydrogen atoms inter­act with the π-electron-rich region to favour layered or offset stacking. Through electrostatic stabilization assisted by dispersion, three-dimensional packing efficiency is enhanced with a slight directionality. More contributions due to S⋯H/H⋯S inter­actions (15.6%) stem from the polarizability of the sulfur atom in weak hydrogen bond-like contacts. Sulfur atoms have soft donor properties, which allow them to participate in stabilizing inter­molecular inter­actions. In the same way, O⋯H/H⋯O inter­actions (9.3%) define classical weak hydrogen-bonding pathways mediated by electronegative oxygen atoms. Electrostatic stabilization occurs as a consequence of these contacts and arrangement of mol­ecules in the lattice in a suitable manner. This lessens the rotational and translational degrees of freedom. The S⋯S contacts (1.5%) represent only a small percentage, but they are structurally important. The presence of short chalcogen–chalcogen contacts is known to enhance the lattice compactness via favourable overlap of their orbitals and associated dispersion inter­actions that lead to local densification. Such changes also promote packing rigidity. These inter­actions can often serve as reinforcing elements of the packing within a crystal. When combined, these inter­actions give rise to a hierarchy of stabilization. The global stabilization is induced by the H⋯H dispersion forces, while the mol­ecular stacking is being controlled by C—H⋯π inter­actions. Also, the directional locking and local reinforcement is conferred by the heteroatom-mediated contacts (S⋯H, O⋯H, S⋯S).

[Figure 5]
Figure 5
View of the three-dimensional Hirshfeld surface of the title compound mapped over (a) dnorm, (b) di, (c) de, (d) shape index and (e) curvedness.
[Figure 6]
Figure 6
Two-dimensional fingerprint plots for the compound, showing (a) all inter­actions, and delineated into (b) H⋯H (c) C⋯H (d) H⋯O / O⋯H, (e) S⋯S and (f) S⋯H inter­actions. The di and de values are the closest inter­nal and external distances (in Å) from given points on the Hirshfeld surface.

To analyse the crystal mechanical stability of the title crystal, a void evaluation was performed by summing the electron densities of the spherically symmetric atoms included in the asymmetric unit (Fig. 7[link]). The void surface is recognized as an isosurface. The crystal voids within the unit cell are characterized by their volume and surface, which are 213.21 Å3 and 654.88 Å2, respectively. Considering the crystal volume of 1861.12 Å3, the proportion of void space within the unit cell is 11.45%.

[Figure 7]
Figure 7
Plot showing the crystal voids in the crystal structure.

5. Database survey

A search of the Cambridge Structural Database (Version 5.37; Groom et al., 2016View full citation). for benzo­thio­phene-2-carboxyl­ate moieties resulted in 18 hits. Entries CUDLEV (Ivachtchenko et al., 2019View full citation) and QAVXOD (Shen et al., 2017View full citation) are the closest analogues of the title compound. CUDLEV crystallizes in the monoclinic space group P21/c. QAVXOD crystallizes in the monoclinic space group P21/n. In CUDLEV, all atoms of the benzo­thio­phene fragment lie in the plane within 0.02 Å. In CUDLEV, the ester substituent is turned significantly to the bicyclic system and the mol­ecules are bound by very weak C—H⋯O inter­molecular hydrogen bonds. Both related structures are distinguished by the nature of their substituents (morpholine-4-sulfonyl and biphenyl-4-yl groups, respectively), thus reflecting the structural flexibility of these compounds.

6. Synthesis and crystallization

The domino reaction of methyl 3-(bromo­meth­yl)-1-benzo­thio­phene-2-carboxyl­ate (0.3 g, 1.05 mmol) with naphtho­[2,1-b]thio­phene (0.19 g, 1.05 mmol) using ZnBr2 (0.47 g, 2.10 mmol) was carried out in dry 1,2-di­chloro­ethane (10 ml) at room temperature under N2 atmosphere for 6 h. The reaction mixture was then poured into crushed ice (50 g) and acidified with conc. HCl (2 ml). The crude product was then extracted with di­chloro­methane (3 × 10 ml) and dried with Na2SO4. The subsequent removal of the solvent in vacuo was followed by column chromatographic purification on silica gel (eluent: 2% ethyl acetate in hexa­ne) afforded the title compound (0.23 g, 69%) as a colorless solid. Single crystals suitable for X-ray diffraction were obtained by slow evaporation of a solution in ethyl acetate at room temperature.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. All hydrogen atoms were positioned geometrically and refined as riding with C—H = 0.93 Å (aromatic CH) with Uiso(H) = 1.5Ueq(C) for methyl groups and 1.2Ueq(C) for other H atoms.

Table 2
Experimental details

Crystal data
Chemical formula C23H16O2S2
Mr 388.48
Crystal system, space group Monoclinic, P21/c
Temperature (K) 293
a, b, c (Å) 8.8381 (4), 22.0387 (9), 9.5910 (3)
β (°) 94.968 (1)
V3) 1861.12 (13)
Z 4
Radiation type Mo Kα
μ (mm−1) 0.30
Crystal size (mm) 0.27 × 0.12 × 0.08
 
Data collection
Diffractometer Bruker APEXII CCD area detector diffractometer
Absorption correction Multi-scan (SADABS; Krause et al., 2015View full citation)
Tmin, Tmax 0.922, 0.976
No. of measured, independent and observed [I > 2σ(I)] reflections 38099, 4271, 3717
Rint 0.068
(sin θ/λ)max−1) 0.651
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.122, 1.06
No. of reflections 4271
No. of parameters 246
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.42, −0.30
Computer programs: APEX4 and SAINT (Bruker, 2018View full citation), SHELXS (Sheldrick, 2008View full citation), SHELXL (Sheldrick, 2015View full citation), ORTEP-3 for Windows (Farrugia, 2012View full citation) and PLATON (Spek, 2020View full citation).

Supporting information


Computing details top

Methyl 3-[(naphtho[2,1-b]thiophen-5-yl)methyl]-1-benzothiophene-2-carboxylate top
Crystal data top
C23H16O2S2F(000) = 808
Mr = 388.48Dx = 1.386 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 8.8381 (4) ÅCell parameters from 3717 reflections
b = 22.0387 (9) Åθ = 2.5–27.6°
c = 9.5910 (3) ŵ = 0.30 mm1
β = 94.968 (1)°T = 293 K
V = 1861.12 (13) Å3Block, colourless
Z = 40.27 × 0.12 × 0.08 mm
Data collection top
Bruker APEXII CCD area detector
diffractometer
3717 reflections with I > 2σ(I)
ω and φ scansRint = 0.068
Absorption correction: multi-scan
(SADABS; Krause et al., 2015)
θmax = 27.6°, θmin = 2.5°
Tmin = 0.922, Tmax = 0.976h = 1111
38099 measured reflectionsk = 2828
4271 independent reflectionsl = 1212
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.047H-atom parameters constrained
wR(F2) = 0.122 w = 1/[σ2(Fo2) + (0.0483P)2 + 0.840P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
4271 reflectionsΔρmax = 0.42 e Å3
246 parametersΔρmin = 0.30 e Å3
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.34542 (6)0.43934 (2)0.98904 (5)0.05024 (18)
S20.62927 (6)0.69125 (3)0.75510 (5)0.05271 (18)
C120.20885 (19)0.61820 (7)0.69839 (17)0.0356 (4)
C180.2214 (2)0.71310 (8)0.56103 (18)0.0388 (4)
C210.35626 (19)0.62550 (8)0.74821 (18)0.0390 (4)
H210.4026110.5970430.8094870.047*
C130.13745 (19)0.66204 (7)0.60185 (17)0.0357 (4)
C200.43935 (19)0.67627 (8)0.70710 (17)0.0377 (4)
C110.1169 (2)0.56398 (9)0.7392 (2)0.0463 (4)
H11A0.0219740.5785230.7707240.056*
H11B0.0922800.5393240.6566010.056*
C190.3754 (2)0.72038 (8)0.61743 (18)0.0392 (4)
C80.2809 (2)0.47487 (8)0.83337 (19)0.0449 (4)
C70.1938 (2)0.52451 (8)0.85167 (19)0.0407 (4)
C60.1804 (2)0.53600 (8)0.9982 (2)0.0451 (4)
O20.4202 (2)0.40316 (7)0.72290 (17)0.0672 (4)
C140.0138 (2)0.65562 (9)0.5444 (2)0.0460 (4)
H140.0708180.6226260.5701220.055*
C220.4825 (3)0.76670 (9)0.5912 (2)0.0534 (5)
H220.4590310.8002840.5347150.064*
C170.1512 (2)0.75430 (10)0.4623 (2)0.0559 (5)
H170.2061700.7872420.4331740.067*
C10.2574 (2)0.49295 (9)1.0853 (2)0.0484 (5)
C150.0784 (2)0.69733 (11)0.4510 (2)0.0597 (6)
H150.1788740.6926400.4151140.072*
C90.3271 (3)0.45074 (10)0.7011 (2)0.0550 (5)
C230.6207 (3)0.75655 (10)0.6568 (2)0.0577 (5)
H230.7032060.7822160.6497180.069*
C50.1042 (3)0.58349 (10)1.0601 (2)0.0576 (5)
H50.0525880.6127571.0046880.069*
C30.1833 (3)0.54270 (13)1.2871 (3)0.0724 (7)
H30.1834390.5454601.3838850.087*
C20.2580 (3)0.49621 (11)1.2304 (2)0.0604 (6)
H20.3084920.4671391.2872430.072*
O10.2888 (3)0.47072 (10)0.58721 (17)0.0950 (7)
C40.1066 (3)0.58634 (13)1.2031 (3)0.0750 (7)
H40.0563880.6177831.2444850.090*
C160.0055 (3)0.74655 (11)0.4097 (3)0.0663 (6)
H160.0388490.7743020.3455230.080*
C100.4826 (4)0.37858 (14)0.6016 (3)0.0848 (9)
H10A0.4020800.3626500.5385020.127*
H10B0.5526520.3466620.6296340.127*
H10C0.5347570.4100000.5556470.127*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0610 (3)0.0447 (3)0.0441 (3)0.0015 (2)0.0002 (2)0.01029 (19)
S20.0415 (3)0.0644 (3)0.0513 (3)0.0154 (2)0.0015 (2)0.0013 (2)
C120.0382 (8)0.0342 (8)0.0347 (8)0.0025 (7)0.0046 (6)0.0031 (6)
C180.0417 (9)0.0341 (8)0.0417 (9)0.0039 (7)0.0095 (7)0.0038 (7)
C210.0385 (9)0.0397 (9)0.0385 (8)0.0011 (7)0.0011 (7)0.0060 (7)
C130.0373 (8)0.0355 (8)0.0350 (8)0.0023 (6)0.0071 (6)0.0021 (6)
C200.0360 (8)0.0417 (9)0.0357 (8)0.0051 (7)0.0039 (6)0.0027 (7)
C110.0429 (10)0.0451 (10)0.0497 (10)0.0087 (8)0.0017 (8)0.0133 (8)
C190.0444 (9)0.0346 (8)0.0397 (9)0.0036 (7)0.0098 (7)0.0013 (7)
C80.0537 (11)0.0416 (9)0.0389 (9)0.0077 (8)0.0022 (8)0.0064 (7)
C70.0428 (9)0.0348 (9)0.0440 (9)0.0096 (7)0.0020 (7)0.0084 (7)
C60.0476 (10)0.0403 (9)0.0479 (10)0.0133 (8)0.0064 (8)0.0041 (8)
O20.0871 (12)0.0582 (9)0.0584 (9)0.0076 (8)0.0173 (8)0.0084 (7)
C140.0388 (9)0.0500 (10)0.0494 (10)0.0007 (8)0.0045 (8)0.0096 (8)
C220.0599 (12)0.0437 (10)0.0576 (12)0.0141 (9)0.0114 (9)0.0052 (9)
C170.0540 (12)0.0453 (11)0.0691 (13)0.0046 (9)0.0102 (10)0.0228 (10)
C10.0546 (11)0.0476 (10)0.0431 (10)0.0133 (9)0.0040 (8)0.0044 (8)
C150.0395 (10)0.0728 (14)0.0656 (13)0.0062 (10)0.0018 (9)0.0188 (11)
C90.0650 (13)0.0511 (12)0.0492 (11)0.0099 (10)0.0063 (9)0.0003 (9)
C230.0567 (12)0.0579 (12)0.0593 (12)0.0260 (10)0.0092 (10)0.0006 (10)
C50.0621 (13)0.0470 (11)0.0655 (13)0.0057 (10)0.0162 (10)0.0015 (9)
C30.0880 (18)0.0823 (17)0.0487 (12)0.0267 (15)0.0168 (12)0.0091 (12)
C20.0714 (14)0.0693 (14)0.0408 (10)0.0208 (11)0.0061 (9)0.0033 (10)
O10.1355 (19)0.1086 (16)0.0410 (9)0.0244 (14)0.0078 (10)0.0073 (9)
C40.0850 (18)0.0702 (16)0.0741 (16)0.0156 (14)0.0316 (14)0.0211 (13)
C160.0545 (13)0.0663 (14)0.0773 (15)0.0120 (11)0.0016 (11)0.0347 (12)
C100.092 (2)0.0868 (19)0.0798 (18)0.0116 (16)0.0312 (15)0.0345 (15)
Geometric parameters (Å, º) top
S1—C11.726 (2)O2—C101.436 (3)
S1—C81.7377 (18)C14—C151.373 (3)
S2—C231.719 (2)C14—H140.9300
S2—C201.7334 (17)C22—C231.343 (3)
C12—C211.358 (2)C22—H220.9300
C12—C131.445 (2)C17—C161.353 (3)
C12—C111.516 (2)C17—H170.9300
C18—C171.416 (3)C1—C21.393 (3)
C18—C131.421 (2)C15—C161.391 (3)
C18—C191.430 (3)C15—H150.9300
C21—C201.413 (2)C9—O11.199 (3)
C21—H210.9300C23—H230.9300
C13—C141.408 (2)C5—C41.371 (4)
C20—C191.385 (2)C5—H50.9300
C11—C71.502 (2)C3—C21.358 (4)
C11—H11A0.9700C3—C41.393 (4)
C11—H11B0.9700C3—H30.9300
C19—C221.429 (2)C2—H20.9300
C8—C71.358 (3)C4—H40.9300
C8—C91.466 (3)C16—H160.9300
C7—C61.443 (3)C10—H10A0.9600
C6—C11.401 (3)C10—H10B0.9600
C6—C51.404 (3)C10—H10C0.9600
O2—C91.338 (3)
C1—S1—C891.25 (9)C23—C22—C19112.82 (19)
C23—S2—C2091.03 (10)C23—C22—H22123.6
C21—C12—C13119.91 (15)C19—C22—H22123.6
C21—C12—C11121.49 (15)C16—C17—C18121.10 (19)
C13—C12—C11118.58 (15)C16—C17—H17119.4
C17—C18—C13118.88 (17)C18—C17—H17119.4
C17—C18—C19121.93 (17)C2—C1—C6121.4 (2)
C13—C18—C19119.16 (15)C2—C1—S1127.37 (18)
C12—C21—C20120.11 (16)C6—C1—S1111.26 (14)
C12—C21—H21119.9C14—C15—C16120.4 (2)
C20—C21—H21119.9C14—C15—H15119.8
C14—C13—C18118.18 (16)C16—C15—H15119.8
C14—C13—C12122.05 (16)O1—C9—O2123.5 (2)
C18—C13—C12119.76 (15)O1—C9—C8125.3 (2)
C19—C20—C21122.34 (16)O2—C9—C8111.24 (18)
C19—C20—S2111.39 (13)C22—C23—S2113.05 (15)
C21—C20—S2126.25 (14)C22—C23—H23123.5
C7—C11—C12115.01 (15)S2—C23—H23123.5
C7—C11—H11A108.5C4—C5—C6119.4 (2)
C12—C11—H11A108.5C4—C5—H5120.3
C7—C11—H11B108.5C6—C5—H5120.3
C12—C11—H11B108.5C2—C3—C4121.2 (2)
H11A—C11—H11B107.5C2—C3—H3119.4
C20—C19—C22111.70 (17)C4—C3—H3119.4
C20—C19—C18118.67 (15)C3—C2—C1118.6 (2)
C22—C19—C18129.57 (17)C3—C2—H2120.7
C7—C8—C9127.41 (18)C1—C2—H2120.7
C7—C8—S1113.54 (14)C5—C4—C3120.8 (2)
C9—C8—S1119.02 (15)C5—C4—H4119.6
C8—C7—C6111.25 (16)C3—C4—H4119.6
C8—C7—C11126.90 (17)C17—C16—C15120.40 (19)
C6—C7—C11121.84 (17)C17—C16—H16119.8
C1—C6—C5118.58 (19)C15—C16—H16119.8
C1—C6—C7112.68 (17)O2—C10—H10A109.5
C5—C6—C7128.74 (19)O2—C10—H10B109.5
C9—O2—C10116.3 (2)H10A—C10—H10B109.5
C15—C14—C13120.99 (18)O2—C10—H10C109.5
C15—C14—H14119.5H10A—C10—H10C109.5
C13—C14—H14119.5H10B—C10—H10C109.5
C13—C12—C21—C200.8 (3)C11—C7—C6—C1178.39 (16)
C11—C12—C21—C20179.42 (16)C8—C7—C6—C5178.07 (19)
C17—C18—C13—C141.5 (3)C11—C7—C6—C52.4 (3)
C19—C18—C13—C14179.66 (16)C18—C13—C14—C150.3 (3)
C17—C18—C13—C12177.65 (17)C12—C13—C14—C15178.87 (19)
C19—C18—C13—C120.5 (2)C20—C19—C22—C231.1 (3)
C21—C12—C13—C14178.28 (17)C18—C19—C22—C23176.02 (19)
C11—C12—C13—C140.4 (3)C13—C18—C17—C161.7 (3)
C21—C12—C13—C180.9 (2)C19—C18—C17—C16179.7 (2)
C11—C12—C13—C18179.58 (16)C5—C6—C1—C20.7 (3)
C12—C21—C20—C190.8 (3)C7—C6—C1—C2179.98 (17)
C12—C21—C20—S2177.49 (14)C5—C6—C1—S1179.07 (15)
C23—S2—C20—C190.66 (14)C7—C6—C1—S10.2 (2)
C23—S2—C20—C21179.08 (17)C8—S1—C1—C2179.21 (19)
C21—C12—C11—C77.8 (3)C8—S1—C1—C60.54 (15)
C13—C12—C11—C7173.54 (16)C13—C14—C15—C160.9 (4)
C21—C20—C19—C22179.62 (16)C10—O2—C9—O14.1 (4)
S2—C20—C19—C221.1 (2)C10—O2—C9—C8175.28 (19)
C21—C20—C19—C182.1 (3)C7—C8—C9—O12.9 (4)
S2—C20—C19—C18176.38 (13)S1—C8—C9—O1179.0 (2)
C17—C18—C19—C20176.14 (18)C7—C8—C9—O2176.42 (19)
C13—C18—C19—C201.9 (2)S1—C8—C9—O21.6 (2)
C17—C18—C19—C220.9 (3)C19—C22—C23—S20.6 (2)
C13—C18—C19—C22178.91 (18)C20—S2—C23—C220.00 (18)
C1—S1—C8—C71.23 (15)C1—C6—C5—C40.3 (3)
C1—S1—C8—C9177.06 (16)C7—C6—C5—C4179.4 (2)
C9—C8—C7—C6176.57 (18)C4—C3—C2—C10.3 (4)
S1—C8—C7—C61.5 (2)C6—C1—C2—C30.7 (3)
C9—C8—C7—C113.9 (3)S1—C1—C2—C3179.00 (18)
S1—C8—C7—C11177.94 (14)C6—C5—C4—C30.1 (4)
C12—C11—C7—C892.0 (2)C2—C3—C4—C50.1 (4)
C12—C11—C7—C688.6 (2)C18—C17—C16—C150.5 (4)
C8—C7—C6—C11.1 (2)C14—C15—C16—C170.8 (4)
Hydrogen-bond geometry (Å, º) top
Cg2 and Cg4 are the centroids of the S2/C19/C20/C22/C23 and C12/C13/C18-C21 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C11—H11B···O10.972.443.007 (3)117
C10—H10A···Cg2i0.962.863.397 (3)116
C17—H17···Cg4ii0.932.983.689 (2)134
Symmetry codes: (i) x+1, y, z+2; (ii) x, y1/2, z1/2.
 

Acknowledgements

We acknowledge the Nanotechnology Research Centre (NRC), SRMIST for providing the research facilities.

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