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ISSN: 2056-9890

Crystal structure and Hirshfeld surface analysis of 3,3′-(sulfanedi­yl)bis­­(2-iodo-1-methyl-1H-indole)

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aGeorgia Southern University, 521 College of Education Dr., Department of Chemistry, Biochemistry and Physics, Statesboro, GA 30458, USA, and bGeorgia Southern University, 11935 Abercorn St., Department of Chemistry, Biochemistry and Physics, Savannah, GA 31419, USA
*Correspondence e-mail: [email protected]

Edited by F. F. Ferreira, Universidade Federal do ABC, Brazil (Received 16 January 2026; accepted 18 March 2026; online 27 March 2026)

The title compound, C18H14I2N2S, comprises two N-methyl-2-iodo­indole fragments linked at the 3-positions by a thio­ether bridge. The sulfur atom adopts a typical thio­ether geometry, and the C—S—C linkage is gauche on both sides, with C—S—C—C torsion angles of −64.1 (11) and −48.3 (10)°. The indole units are essentially planar and are strongly inclined to one another, with an inter­planar angle of 103.3 (3)°. The compound crystallizes in the ortho­rhom­bic space group Fdd2; the mol­ecule lacks classical hydrogen-bond donors, and no significant hydrogen bonding or ππ stacking is observed. The packing is dominated by van der Waals inter­actions together with short I⋯C and I⋯π contacts, giving a herringbone arrangement and forming chains along the b axis. Hirshfeld surface analysis indicates that H⋯H (33.1%), H⋯C/C⋯H (25.5%) and H⋯I/I⋯H (24.4%) contacts make the largest contributions to the crystal packing.

1. Chemical context

Sulfur-bridged indolyl compounds have attracted inter­est because of their relevance to medicinal chemistry (Xalxo et al., 2023View full citation; Silveira et al., 2013View full citation) and materials science (Yuan et al., 2022View full citation), as well as their ability to serve as versatile synthons in organic chemistry (Wang, 2024View full citation). Di­aryl­ated thio­ethers (ar­yl–S–aryl motifs) are used in functional materials; for example, thio­ether-linked polymeric systems have been developed for adsorption/capture applications such as iodine uptake (Shetty et al., 2022View full citation), and porous poly(aryl thio­ether) frameworks have also been explored for metal capture, sensing, and heterogeneous catalysis (Rivero-Crespo et al., 2021View full citation). Thieno­indole-based π-systems have also been incorporated into conjugated polymers for organic electronic applications (Jeong et al., 2016View full citation). The motivation for studying these motifs comes from the central role of indole scaffolds in drug discovery (Mo et al., 2024View full citation) and from literature reports that indole-based aryl sulfides can exhibit potent anti­bacterial activity against Staphylococcus aureus (Lavekar et al., 2024View full citation). Organosulfur compounds containing thio­ether (sulfane) linkages are known to influence mol­ecular conformation, electronic properties, and inter­molecular inter­actions in the solid state (Gundermann, 1963View full citation). Incorporation of a sulfide bridge between two indole moieties can enhance structural rigidity while allowing conformational flexibility about the C–S–C linkage (Mohanty et al., 2025View full citation). The presence of iodine atoms at the 2-position of the indole rings provides opportunities for specific inter­molecular contacts, while N-methyl­ation suppresses classical N—H hydrogen bonding, allowing a clearer assessment of the roles played by halogen⋯halogen, halogen⋯π, and sulfur-involved inter­actions in the crystal structure (Bergman & Janosik, 2002View full citation). 3,3′-Sulfanediylbis(2-iodo-1-methyl-1H-indole) serves as a model system for assessing I⋯I, I⋯π and sulfur-involving contacts in the absence of classical hydrogen-bond donors, providing guidance for the crystal engineering of closely related derivatives. Herein, we report its synthesis and single-crystal X-ray diffraction analysis.

[Scheme 1]

2. Structural commentary

The mol­ecular structure of 3,3′-sulfanediylbis(2-iodo-1-methyl-1H-indole), (I), consists of two N-methyl-2-iodo­indole fragments linked through a thio­ether bridge at the 3-position (Fig. 1[link]). The C—I bond lengths are similar [I1—C1 = 2.079 (12) Å and I2—C10 = 2.080 (9) Å]. The sulfur atom adopts a typical thio­ether geometry with S1—C2 = 1.761 (11) Å and S1—C11 = 1.770 (11) Å, and a C2—S1—C11 angle of 100.6 (5)°. The conformation about the S bridge is gauche on both sides, as shown by the torsion angles C11—S1—C2—C1 = −64.1 (11)° and C2—S1—C11—C12 = −48.3 (10)°. Both indole ring systems are essentially planar, with r.m.s. deviations of 0.012 Å for the N1/C1–C8 system and 0.017 Å for the N2/C10–C17 system. The two indole mean planes are strongly inclined, with an inter­planar angle (normal-to-normal) of 76.3 (3)°.

[Figure 1]
Figure 1
The mol­ecular structure of (I) with displacement ellipsoids drawn at the 50% probability level.

3. Supra­molecular features

Compound (I)[link] crystallizes in the ortho­rhom­bic space group Fdd2. In the crystal, the mol­ecule lacks classical hydrogen-bond donors and no significant hydrogen-bonding inter­actions are observed; likewise, no ππ stacking between indole rings is evident. The packing (Fig. 2[link]) is dominated primarily by van der Waals contacts, but with shorter than van der Waals inter­molecular I⋯C contacts, C14⋯I1i = 3.341 (12) Å and C5⋯I2i = 3.433 (14) Å [symmetry code: (i) Mathematical equation − x, Mathematical equation + y, −Mathematical equation + z]. The mol­ecules pack in a herringbone pattern with each iodine substituent oriented toward the six-membered π-system of an indole ring in a neighbouring, symmetry-related mol­ecule, giving rise to I⋯π contacts. For I1, the perpendicular separation from the plane of the C12–C17 ring is 3.217 (13) Å and the iodine-to-centroid distance is I1⋯Cg(C12–C17)i = 3.906 (5) Å; the C1—I1 vector makes an angle of 152.7 (4)° with the ring-plane normal and the C1—I1⋯Cgi angle is 166.8 (3)°. Similarly, I2 lies 3.323 (14) Å from the plane of the C3–C8 ring with I2⋯Cg(C3–C8)i = 3.999 (5) Å; the C10–I2 vector makes an angle of 25.0 (4)° with the ring-plane normal and the C10—I2⋯Cgi angle is 171.2 (3)°. These I⋯π contacts link the mol­ecules into chains running parallel to the b axis.

[Figure 2]
Figure 2
A view along the c-axis direction of the crystal packing of (I)

4. Hirshfeld surface analysis

The inter­molecular inter­actions were further investigated by qu­anti­tative analysis of the Hirshfeld surface, and visualized with Crystal Explorer 21.5 (Spackman et al., 2021View full citation) and the two-dimensional fingerprint plots (McKinnon et al., 2007View full citation). The shorter and longer contacts are indicated as red and blue spots, respectively, on the Hirshfeld surfaces, and contacts with distances approximately equal to the sum of the van der Waals radii are colored white. The function dnorm is a ratio enclosing the distances of any surface point to the nearest inter­ior (di) and exterior (de) atom and the van der Waals (vdW) radii of the atoms. The dnorm plots were mapped with a color scale between −0.19 a.u. (red) and +1.2 a.u. (blue).

Fig. 3[link] shows the dnorm Hirshfeld surface of the title compound. The most intense red regions on the surface correspond to short inter­molecular contacts involving H⋯I and H⋯C inter­actions, indicating their importance in the crystal packing. No pronounced red–blue triangular features are observed on the shape-index surface, suggesting the absence of significant ππ stacking inter­actions. Analysis of the two-dimensional fingerprint plots reveals that H⋯H contacts make the largest contribution to the Hirshfeld surface (33.1%), highlighting the dominant role of van der Waals inter­actions in the packing. This is followed by H⋯C/C⋯H (25.5%) and H⋯I/I⋯H (24.4%) inter­actions, which together account for a substantial fraction of the inter­molecular contacts. Smaller contributions arise from C⋯I/I⋯C (5.2%), H⋯S/S⋯H (4.9%), and H⋯N/N⋯H (2.6%) contacts, while all remaining inter­actions contribute less than 2% individually, see Table 1[link].

Table 1
Contributions of selected inter­molecular contacts (%) to the Hirshfeld surfaces of (I)

Contact (%)
H⋯H 33.1
H⋯C/C⋯H 25.5
H⋯I/I⋯H 24.4
C⋯I/I⋯C 5.2
H⋯S/S⋯H 4.9
H⋯N/N⋯H 2.6
I⋯S/S⋯I 1.7
C⋯S/S⋯C 1.4
S⋯N/N⋯S 0.9
I⋯I 0.2
[Figure 3]
Figure 3
Hirshfeld surface for (I) mapped over dnorm.

5. Database survey

A search of the Cambridge Structural Database (CSD; website, accessed on 6 January 2026; Groom et al., 2016View full citation) for structures related to the title compound, 3,3′-sulfanediylbis(2-iodo-1-methyl-1H-indole), returned nine relevant entries. Three structures feature the 3,3′-thio­ether-linked bis­(indole) motif: GETCAK, 1,1′-bis­(t-butyl­dimethyl­sil­yl)-3,3′-bis­(1H-indol-3-yl)sulfide (Shirani et al., 2006View full citation), LOJTOX, 3,3′-sulfanediylbis(2-methyl-1H-indole) (Sharma et al., 2024View full citation), and YIQPEV, 3,3′-sulfanediylbis(1-methyl-1H-indole) (Shibahara et al., 2014View full citation); among these, YIQPEV is the closest analogue in terms of N-methyl­ation, but it lacks the 2-iodo substitution present in the title compound. The remaining entries comprise iodinated indole derivatives with differing substitution patterns and functionalization, including JEVQOR, 2,3-di­iodo-1-(phenyl­sulfon­yl)-1H-indole (Rinderspacher et al., 2007View full citation), KAGQIV, 2-iodo-1-phenyl-1H-indole (Messaoud et al., 2015View full citation), iodo­indole benzamide derivatives KAGGEJ and KAGGIN (Kim et al., 2025View full citation), and 2-iodo-3-[(tri­fluoro­meth­yl)selan­yl]indole derivatives KOYFAJ and KOYFIR (Huang et al., 2024View full citation).

6. Synthesis and crystallization

Di-tert-butyl di­sulfide (200 mg, 1.12 mmol) and N-methyl indole (147 mg, 1.12 mmol) were placed in a round-bottomed flask along with 2 mL of DMSO. The mixture was flushed with argon and iodine (710 mg, 2.8 mmol) and one drop of DBU (1,8-diazabicyclo[5.4.0]undec-7-ene) were added successively. The reaction mixture was then allowed to stir at room temperature for 12 h. After satisfactory conversion as indicated on TLC (10% ethyl acetate: hexa­ne), the reaction mixture was washed with dilute sodium thio­sulfate and the product was extracted in ethyl acetate. The crude product was subjected to purification using column chromatography to obtain a white solid (200 mg, 66%). Crystals for X-ray analysis were obtained by slow evaporation from ethyl acetate solution at room temperature.

Spectroscopic data: 1H NMR (400 MHz, CDCl3) δ = 7.75 (d, J = 6.3 Hz, 2H), 7.27 (m, 2H), 7.15 (m, 4H), 3.78 (s, 6H). 13C NMR (101 MHz, CDCl3) δ = 138.8, 129.6, 122.2, 120.1, 119.9, 112.6, 109.7, 97.12, 35.1.

7. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. H atoms were positioned geometrically (C—H = 0.93–0.96 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(Cmeth­yl).

Table 2
Experimental details

Crystal data
Chemical formula C18H14I2N2S
Mr 544.17
Crystal system, space group Orthorhombic, Fdd2
Temperature (K) 298
a, b, c (Å) 37.8416 (4), 31.6009 (3), 5.94404 (5)
V3) 7108.05 (11)
Z 16
Radiation type Cu Kα
μ (mm−1) 28.89
Crystal size (mm) 0.15 × 0.05 × 0.02
 
Data collection
Diffractometer XtaLAB Synergy, Single source at home/near, HyPix3000
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2023View full citation)
Tmin, Tmax 0.401, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 9127, 2434, 2352
Rint 0.099
(sin θ/λ)max−1) 0.608
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.052, 0.146, 1.18
No. of reflections 2434
No. of parameters 210
No. of restraints 1
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.90, −1.60
Absolute structure Flack x determined using 558 quotients [(I+)−(I)]/[(I+)+(I)] (Parsons et al., 2013View full citation)
Absolute structure parameter −0.034 (16)
Computer programs: CrysAlis PRO (Rigaku OD, 2023View full citation), SHELXL2018/3 (Sheldrick, 2015View full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

2-Iodo-3-[(2-iodo-1-methyl-1H-indol-3-yl)sulfanyl]-1-methyl-1H-indole top
Crystal data top
C18H14I2N2SDx = 2.034 Mg m3
Mr = 544.17Cu Kα radiation, λ = 1.54184 Å
Orthorhombic, Fdd2Cell parameters from 7695 reflections
a = 37.8416 (4) Åθ = 2.8–69.4°
b = 31.6009 (3) ŵ = 28.89 mm1
c = 5.94404 (5) ÅT = 298 K
V = 7108.05 (11) Å3Needle, clear colourless
Z = 160.15 × 0.05 × 0.02 mm
F(000) = 4128
Data collection top
XtaLAB Synergy, Single source at home/near, HyPix3000
diffractometer
2434 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source2352 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.099
Detector resolution: 10.0000 pixels mm-1θmax = 69.6°, θmin = 3.7°
ω scansh = 4539
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2023)
k = 3838
Tmin = 0.401, Tmax = 1.000l = 75
9127 measured reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.052 w = 1/[σ2(Fo2) + (0.1145P)2]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.146(Δ/σ)max = 0.001
S = 1.18Δρmax = 0.90 e Å3
2434 reflectionsΔρmin = 1.60 e Å3
210 parametersAbsolute structure: Flack x determined using 558 quotients [(I+)-(I-)]/[(I+)+(I-)]
(Parsons et al., 2013)
1 restraintAbsolute structure parameter: 0.034 (16)
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
I10.32692 (2)0.48490 (2)0.93756 (14)0.0508 (3)
I20.43892 (2)0.47566 (2)0.71981 (17)0.0578 (3)
S10.36946 (6)0.53925 (8)0.4606 (5)0.0439 (6)
C50.2780 (3)0.6351 (4)0.230 (3)0.061 (3)
H50.2796420.6541300.1110820.073*
C140.3706 (3)0.6641 (3)0.938 (3)0.055 (3)
H140.3568600.6882800.9209130.066*
C70.2432 (3)0.6070 (4)0.538 (3)0.052 (3)
H70.2225700.6066000.6227750.062*
C160.4158 (3)0.6273 (4)1.158 (2)0.052 (3)
H160.4310690.6251791.2800300.063*
C90.2490 (3)0.5395 (4)0.926 (2)0.047 (2)
H9A0.2450210.5095410.9270820.071*
H9B0.2272400.5539220.8943350.071*
H9C0.2578640.5483631.0694720.071*
C60.2476 (4)0.6347 (4)0.360 (3)0.061 (3)
H60.2295740.6537190.3268930.073*
C120.3896 (2)0.5966 (3)0.815 (2)0.037 (2)
C130.3671 (3)0.6333 (4)0.786 (2)0.050 (3)
H130.3511470.6352440.6675070.060*
C180.4594 (4)0.5450 (5)1.140 (3)0.067 (4)
H18A0.4809970.5404541.0581170.101*
H18B0.4527500.5193781.2151690.101*
H18C0.4628960.5670631.2485550.101*
N10.2752 (2)0.5500 (3)0.7496 (16)0.0410 (18)
C170.4136 (3)0.5951 (4)0.998 (2)0.043 (2)
C150.3947 (3)0.6622 (4)1.128 (2)0.055 (3)
H150.3958480.6845381.2291330.066*
C100.4193 (2)0.5350 (3)0.805 (2)0.039 (2)
C110.3936 (2)0.5572 (3)0.697 (2)0.039 (2)
C40.3058 (3)0.6082 (3)0.272 (2)0.047 (3)
H40.3260160.6086040.1828580.057*
C10.3086 (2)0.5320 (3)0.723 (2)0.040 (2)
N20.4320 (2)0.5572 (3)0.986 (2)0.047 (2)
C30.3025 (3)0.5800 (3)0.454 (2)0.042 (2)
C20.3259 (2)0.5495 (3)0.550 (2)0.039 (2)
C80.2712 (3)0.5797 (3)0.5853 (19)0.039 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I10.0529 (4)0.0460 (4)0.0535 (5)0.0002 (3)0.0029 (3)0.0119 (3)
I20.0527 (4)0.0459 (4)0.0748 (6)0.0076 (3)0.0014 (4)0.0028 (4)
S10.0357 (10)0.0523 (13)0.0437 (14)0.0027 (10)0.0002 (10)0.0062 (12)
C50.067 (7)0.046 (5)0.069 (8)0.012 (5)0.021 (7)0.020 (6)
C140.044 (5)0.041 (5)0.079 (9)0.008 (4)0.023 (7)0.002 (6)
C70.041 (5)0.054 (6)0.061 (7)0.001 (5)0.006 (5)0.009 (6)
C160.045 (5)0.060 (6)0.052 (7)0.012 (5)0.001 (5)0.010 (6)
C90.040 (4)0.060 (6)0.042 (6)0.007 (5)0.005 (5)0.003 (5)
C60.059 (6)0.045 (6)0.080 (10)0.004 (5)0.028 (7)0.002 (6)
C120.031 (4)0.037 (4)0.043 (5)0.002 (3)0.003 (4)0.006 (4)
C130.047 (6)0.053 (6)0.051 (7)0.023 (5)0.017 (5)0.011 (5)
C180.067 (8)0.064 (8)0.071 (9)0.014 (6)0.018 (8)0.009 (7)
N10.037 (4)0.043 (4)0.043 (5)0.001 (3)0.004 (4)0.001 (4)
C170.042 (4)0.045 (5)0.043 (6)0.006 (4)0.000 (5)0.001 (5)
C150.058 (6)0.051 (6)0.057 (8)0.012 (5)0.004 (6)0.016 (6)
C100.033 (4)0.031 (4)0.054 (7)0.002 (4)0.007 (4)0.001 (4)
C110.037 (4)0.033 (4)0.046 (6)0.002 (4)0.002 (5)0.004 (4)
C40.048 (5)0.042 (5)0.051 (7)0.008 (5)0.004 (5)0.007 (5)
C10.033 (4)0.033 (4)0.053 (6)0.007 (3)0.001 (5)0.004 (5)
N20.037 (4)0.044 (4)0.059 (6)0.005 (4)0.006 (4)0.001 (5)
C30.040 (4)0.037 (4)0.048 (6)0.000 (4)0.001 (5)0.000 (5)
C20.033 (4)0.037 (5)0.047 (6)0.012 (4)0.010 (4)0.005 (5)
C80.038 (4)0.031 (4)0.047 (5)0.002 (4)0.006 (4)0.004 (4)
Geometric parameters (Å, º) top
I1—C12.079 (12)C6—H60.9300
I2—C102.080 (9)C12—C131.448 (17)
S1—C111.770 (11)C12—C171.418 (16)
S1—C21.761 (11)C12—C111.436 (13)
C5—H50.9300C13—H130.9300
C5—C61.39 (2)C18—H18A0.9600
C5—C41.375 (18)C18—H18B0.9600
C14—H140.9300C18—H18C0.9600
C14—C131.336 (17)C18—N21.435 (17)
C14—C151.452 (19)N1—C11.393 (12)
C7—H70.9300N1—C81.364 (14)
C7—C61.38 (2)C17—N21.390 (14)
C7—C81.394 (15)C15—H150.9300
C16—H160.9300C10—C111.361 (14)
C16—C171.392 (16)C10—N21.369 (16)
C16—C151.373 (19)C4—H40.9300
C9—H9A0.9600C4—C31.409 (16)
C9—H9B0.9600C1—C21.342 (17)
C9—H9C0.9600C3—C21.428 (14)
C9—N11.476 (14)C3—C81.417 (15)
C2—S1—C11100.6 (5)C1—N1—C9126.6 (9)
C6—C5—H5119.0C8—N1—C9126.0 (9)
C4—C5—H5119.0C8—N1—C1107.4 (9)
C4—C5—C6121.9 (12)C16—C17—C12122.7 (10)
C13—C14—H14118.1N2—C17—C16129.3 (11)
C13—C14—C15123.8 (12)N2—C17—C12108.0 (10)
C15—C14—H14118.1C14—C15—H15120.0
C6—C7—H7121.5C16—C15—C14120.0 (11)
C6—C7—C8117.0 (12)C16—C15—H15120.0
C8—C7—H7121.5C11—C10—I2127.2 (9)
C17—C16—H16121.3C11—C10—N2111.0 (9)
C15—C16—H16121.3N2—C10—I2121.9 (7)
C15—C16—C17117.5 (12)C12—C11—S1127.6 (8)
H9A—C9—H9B109.5C10—C11—S1125.4 (8)
H9A—C9—H9C109.5C10—C11—C12107.0 (10)
H9B—C9—H9C109.5C5—C4—H4121.2
N1—C9—H9A109.5C5—C4—C3117.5 (12)
N1—C9—H9B109.5C3—C4—H4121.2
N1—C9—H9C109.5N1—C1—I1121.7 (8)
C5—C6—H6119.0C2—C1—I1127.0 (7)
C7—C6—C5122.1 (11)C2—C1—N1111.3 (10)
C7—C6—H6119.0C17—N2—C18124.2 (11)
C17—C12—C13119.5 (10)C10—N2—C18128.0 (9)
C17—C12—C11106.2 (9)C10—N2—C17107.8 (9)
C11—C12—C13134.3 (10)C4—C3—C2132.7 (11)
C14—C13—C12116.5 (13)C4—C3—C8120.1 (10)
C14—C13—H13121.8C8—C3—C2107.2 (10)
C12—C13—H13121.8C1—C2—S1127.9 (8)
H18A—C18—H18B109.5C1—C2—C3106.3 (9)
H18A—C18—H18C109.5C3—C2—S1125.8 (9)
H18B—C18—H18C109.5C7—C8—C3121.4 (10)
N2—C18—H18A109.5N1—C8—C7130.8 (11)
N2—C18—H18B109.5N1—C8—C3107.8 (9)
N2—C18—H18C109.5
I1—C1—C2—S12.6 (15)C17—C12—C11—C101.5 (12)
I1—C1—C2—C3179.6 (8)C15—C14—C13—C121.3 (16)
I2—C10—C11—S12.4 (15)C15—C16—C17—C122.7 (17)
I2—C10—C11—C12179.0 (7)C15—C16—C17—N2179.0 (11)
I2—C10—N2—C180.6 (18)C11—S1—C2—C164.1 (11)
I2—C10—N2—C17179.7 (7)C11—S1—C2—C3113.3 (10)
C5—C4—C3—C2177.0 (12)C11—C12—C13—C14178.3 (11)
C5—C4—C3—C80.6 (16)C11—C12—C17—C16176.7 (10)
C16—C17—N2—C183 (2)C11—C12—C17—N21.9 (12)
C16—C17—N2—C10176.9 (11)C11—C10—N2—C18179.0 (13)
C9—N1—C1—I10.9 (14)C11—C10—N2—C170.7 (13)
C9—N1—C1—C2178.3 (10)C4—C5—C6—C71 (2)
C9—N1—C8—C70.2 (18)C4—C3—C2—S11.5 (18)
C9—N1—C8—C3179.3 (10)C4—C3—C2—C1179.4 (11)
C6—C5—C4—C30.3 (19)C4—C3—C8—C70.1 (16)
C6—C7—C8—N1178.5 (11)C4—C3—C8—N1179.5 (10)
C6—C7—C8—C31.0 (17)C1—N1—C8—C7179.0 (11)
C12—C17—N2—C18178.1 (12)C1—N1—C8—C30.6 (11)
C12—C17—N2—C101.6 (12)N2—C10—C11—S1178.0 (8)
C13—C14—C15—C160.7 (18)N2—C10—C11—C120.6 (12)
C13—C12—C17—C162.1 (16)C2—S1—C11—C1248.3 (10)
C13—C12—C17—N2179.3 (9)C2—S1—C11—C10130.0 (10)
C13—C12—C11—S11.5 (18)C2—C3—C8—C7178.3 (10)
C13—C12—C11—C10180.0 (11)C2—C3—C8—N11.3 (12)
N1—C1—C2—S1176.6 (8)C8—C7—C6—C51.3 (19)
N1—C1—C2—C31.3 (13)C8—N1—C1—I1179.7 (7)
C17—C16—C15—C141.3 (17)C8—N1—C1—C20.5 (12)
C17—C12—C13—C140.1 (15)C8—C3—C2—S1176.3 (8)
C17—C12—C11—S1177.0 (8)C8—C3—C2—C11.6 (12)
Contributions of selected intermolecular contacts (%) to the Hirshfeld surfaces of (I) top
Contact(%)
H···H33.1
H···C/C···H25.5
H···I/I···H24.4
C···I/I···C5.2
H···S/S···H4.9
H···N/N···H2.6
I···S/S···I1.7
C···S/S···C1.4
S···N/N···S0.9
I···I0.2
 

Acknowledgements

The authors thank the Department of Biochemistry, Chemistry, and Physics at Georgia Southern University for the financial support of this work and the National Science Foundation Major Research Instrumentation fund for the purchase of the X-ray diffractometer.

Funding information

Funding for this research was provided by: NSF Major Research Instrumentation (MRI) program (grant No. 2215812).

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