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

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890

Crystal structure of tris­­[4-(3,4-di­meth­­oxy­thio­phen-2-yl)phen­yl]amine

crossmark logo

aKansai University, 3-3-35 Yamate-cho, Suita, Osaka 564-8680, Japan, bOsaka Research Institute of Industrial Science and Technology, 1-6-50, Morinomiya, Joto-ku, Osaka 536-8553, Japan, and cOkayama University, 3-1-1 Tsushima-naka, Kita-ku, Okayama 700-8530, Japan
*Correspondence e-mail: [email protected]

Edited by Y. Ozawa, University of Hyogo, Japan (Received 25 November 2025; accepted 4 January 2026; online 8 January 2026)

In the title compound tris­[4-(3,4-di­meth­oxy­thio­phen-2-yl)phen­yl]amine (DMOT-TPA), C36H33NO6S3, the central nitro­gen atom shows no pyramidalization, with the three para-phenyl­ene rings arranged in a propeller-like geometry. Each thio­phene ring is twisted by about 25–29° relative to the adjacent phenyl­ene ring, giving a distorted π-conjugated framework. In the crystal, mol­ecules are linked through multiple C—H⋯π inter­actions into two-dimensional sheets, which extend into a three-dimensional network. A Cambridge Structural Database survey revealed no prior examples of tri­phenyl­amines bearing 3,4-di­meth­oxy­thio­phen units at the para positions. This unique structure provides new insights into the design of redox-active organic materials.

1. Chemical context

Tri­aryl­amines (TAAs) are well-known electron donors and continue to be the subject of much theoretical and experimental research. Since TAA derivatives with various substituents in the para-position give stable radical cations by one-electron oxidation in solution, they are used in the fields of positively charged purely organic high-spin systems (Sato et al., 1997View full citation) as well as for organic mixed-valence mol­ecular systems (Lambert et al., 1999View full citation). TAAs with extra aromatic rings in the para-position have received notable attention as components of redox-active organic materials (Yen & Liou, 2012View full citation; Thelakkat, 2002View full citation). Among them, tris­(4-(thio­phene-2-yl)phen­yl)amine and its π-extended derivatives have been developed into electroactive polymer electrodes and electrochromic polymer materials, and many derivatives continue to be reported (Golba et al., 2015View full citation). Thio­phenes with strong electron-donating substituents at the β-position show enhanced donor properties and high stability. Consequently, a tri­phenyl­amine derivative incorporating three 3,4-di­meth­oxy­thio­phene groups is expected to behave as a redox-active core that enables facile electron transfer in both solution and the solid state, with potential relevance to mol­ecular electronic materials. We report herein on the crystal structure of the title compound.

[Scheme 1]

2. Structural commentary

The mol­ecular structure of the title compound is shown in Fig. 1[link]. The central N10 atom shows no pyramidalization, with a deviation from the plane of the bonded C atoms (C18, C30, and C42) of 0.025 (2) Å. The three para-phenyl­ene rings are bonded to the N10 atom in a propeller-type fashion, which is a common arrangement for Ph3N fragments. The torsion angles C17—C18—N10—C42, C29—C30—N10—C18 and C41—C42—N10—C30 are −49.7 (2), −30.3 (2) and −29.8 (2)°, respectively. The mean planes of the para-phenyl­ene rings and the neighboring thio­phene ring are inclined to each other by 24.19 (10)° for (C15–C20)/(S1/C11–C14), 28.73 (9)° for (C27–C32)/(S2/C23–C26) and 26.67 (9)° for (C39–C44)/(S3/C35–C38).

[Figure 1]
Figure 1
The mol­ecular structure of the title compound with the atom labeling. Displacement ellipsoids are drawn at the 50% probability level. H atoms are represented by spheres of arbitrary radius.

3. Supra­molecular features

In the crystal, each mol­ecule inter­acts with five others via four inter­molecular C—H⋯π inter­actions (Table 1[link]). The mol­ecules are linked by complementary C—H⋯π inter­actions between the meth­oxy group and a neighboring thio­phene ring [C22—H22CCg3ii and C45—H45ACg1ii; Cg3 and Cg1 are the centroids of the S3/C35–C38 and S1/C11–C14 rings, respectively; symmetry code: (ii) −x + 1, −y + 1, −z + 1], forming an inversion dimer (Fig. 2[link]). The other two C—H⋯π inter­actions [C21—H21BCg5i and C32—H32⋯Cg5iii; Cg5 is the centroid of the C27–C32 ring; symmetry code: (i) −x + Mathematical equation, y + Mathematical equation, −z + Mathematical equation; (iii) −x + Mathematical equation, y − Mathematical equation, −z + Mathematical equation] form one-dimensional chain structures parallel to the b-axis (Figs. 3[link] and 4[link]), and these inter­actions form two-dimensional sheets in the ac plane. As a result, the two-dimensional sheets are linked by complementary C—H⋯π inter­actions, forming the dimers mentioned above into a three-dimensional network. Weak inter­molecular inter­actions [O5⋯H45C—H45iv and O9⋯H34B—C34iii; symmetry code: (iv) −x + 1, −y + 2, −z + 1] are also shown in Table 1[link]. There are no significant inter­molecular inter­actions around Cg2, Cg4 and Cg6 (the centroids of the S2/C23–C26, C15–C20 and C39–C44 rings, respectively).

Table 1
Hydrogen-bond geometry (Å, °)

Cg1, Cg3 and Cg5 are the centroids of the S1/C11–C14,S3/C35–C38 and C27–C32 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C21—H21BCg5i 0.98 2.95 3.686 (3) 133
C22—H22CCg3ii 0.98 2.85 3.678 (2) 143
C32—H32⋯Cg5iii 0.95 2.87 3.518 (2) 126
C45—H45ACg1ii 0.98 2.89 3.820 (2) 160
O5—H45C⋯C45iv 0.98 2.69 3.336 (3) 123
O9—H34B⋯C34iii 0.98 2.77 3.177 (3) 106
Symmetry codes: (i) Mathematical equation; (ii) Mathematical equation; (iii) Mathematical equation; (iv) Mathematical equation.
[Figure 2]
Figure 2
The centrosymmetric dimeric structure of the title compound. The inter­molecular C—H⋯π inter­actions are shown as dashed lines. H atoms not involved in these inter­actions have been omitted for clarity. [Symmetry code: (ii) −x + 1, −y + 1, −z + 1.]
[Figure 3]
Figure 3
A portion of the crystal packing of the title compound showing the spiral chain formed via a 21 screw axis. The inter­molecular C—H⋯π inter­actions are shown as dashed lines. H atoms not involved in these inter­actions have been omitted for clarity. [Symmetry code: (i) −x + Mathematical equation, y + Mathematical equation, −z + Mathematical equation.]
[Figure 4]
Figure 4
A portion of the crystal packing of the title compound showing the spiral chain formed via a 21 screw axis. The inter­molecular C—H⋯π inter­actions are shown as dashed lines. H atoms not involved in these inter­actions have been omitted for clarity. [Symmetry code: (iii) −x + Mathematical equation, y − Mathematical equation, −z + Mathematical equation.]

In order to further characterize the inter­molecular inter­actions in the crystal of the title compound, a Hirshfeld surface analysis (Spackman & Jayatilaka, 2009View full citation) was carried out using CrystalExplorer (version 21.3; Spackman et al., 2021View full citation). The Hirshfeld surface mapped over dnorm (Fig. 5[link]) shows several localized red spots, which correspond to short C—H⋯O and C—H⋯S contacts between neighboring mol­ecules. The associated two-dimensional fingerprint plots (McKinnon et al., 2007View full citation) provide qu­anti­tative information on the inter­molecular inter­actions in terms of percentage contributions (Spackman & McKinnon, 2002View full citation). As illustrated in Fig. 6[link], H⋯H contacts contribute 46.8% to the Hirshfeld surface and dominate the crystal packing, followed by H⋯O/O⋯H (12.7%) and H⋯S/S⋯H (12.8%) contacts.

[Figure 5]
Figure 5
Hirshfeld surface mapped over dnorm for the title compound. (a) Front view and (b) back view. Red spots indicate short C—H⋯O and C—H⋯S contacts.
[Figure 6]
Figure 6
Two-dimensional fingerprint plots for the title compound. (a) Full fingerprint plot showing the overall distribution of di and de. Fingerprint plots highlighting the (b) H⋯O/O⋯H contacts and (c) H⋯S/S⋯H contacts.

4. Database survey

A search of the Cambridge Structural Database (CSD, Version 6.00, update August 2025; Groom et al., 2016View full citation) for compounds containing tri­phenyl­amines yielded 9691 hits (including 8428 hits for non-polymeric compounds). Limiting the search to non-polymeric tri­phenyl­amines with at least one thio­phene ring bonded to tri­phenyl­amine core at the 4-position of phenyl group gave 167 hits (149 compounds), which included five hits (five compounds) with the thio­phene ring having oxygen atoms at the two β-positions. There was one report of TPA cores bound to EDOT units (BUSZIC; Yuan et al., 2021View full citation). There are five compounds with thio­phene rings at the three para-positions of tri­phenyl­amine, three of which do not contain metal ions: tris­(2-thio­phenyl-4-phen­yl)amine (AXELIZ; Wang et al., 2011View full citation), its tri­formyl­ated compound tris­[2-(5-formyl­thio­phen­yl)-4-phenl­yl]amine (PAYXAQ; Par­thasarathy et al., 2011View full citation) and tris­(2-{5-[N-(butan-2-yl)-2-cyano­prop-2-enamide]­thio­phen­yl}-4-phenl­yl)amine (SODXOB; Adelizzi et al., 2019View full citation). These three compounds adopt a similar propeller-type TPA geometry. A search for compounds containing 2,3-di­meth­oxy­thio­phene yielded nine hits of which six are non-macrocyclic compounds. Of these six compounds, only two structures contain an aryl-substituent at the α-position of thio­phene [ILIWAF (Peng et al., 2025aView full citation) and ILIWEJ Peng et al., 2025bView full citation)]. The inter­molecular inter­actions around 2,3-di­meth­oxy­thio­phene were not shown in ILIWEJ, whereas in contrast only a thio­phenyl S⋯H—N inter­action was suggested in ILIWAF.

5. Synthesis and crystallization

DMOT-TPA was synthesized under Negishi coupling conditions using the method we previously reported (Yano et al., 2022View full citation). To a solution of 3,4-di­meth­oxy­thio­phene (0.10 mL, 0.91 mmol) in tetra­hydro­furan (THF, 1.20 mL) were added 1.6 M of n-BuLi in hexane (0.60 mL, 0.96 mmol) at 195 K. After stirring at 195 K for 1 h, 1.0 M of ZnCl2 in THF (0.96 mL, 0.96 mmol) was slowly added and stirred for 0.5 h at 273 K. 4,4′,4′′-Tri­bromo­tri­phenyl­amine (0.11 g, 0.22 mmol) and tris­(di­benzyl­ideneacetone)dipalladium(0)·CHCl3 (3.4 mg, 0.006 mmol), 2-di­cyclo­hexyl­phosphino-2′,6′-di­meth­oxy­biphenyl (SPhos, 8.5 mg, 0.020 mmol) were added and stirred at 343 K for 1 h. The resulting solution was quenched with water, extracted with chloro­form, and dried over sodium sulfate. Upon addition of an excess amount of methanol to this solution, a yellow powder was precipitated (111 mg, 76%). 1H NMR (400 MHz, CDCl3): δ 3.84 (s, 9H), 3.86 (s, 9H), 6.10 (s, 3H), 7.12 (d, J = 8.8 Hz, 6H), 7.60 (d, J = 8.8 Hz, 6H). Pale-yellow crystals of DMOT-TPA suitable for X-ray diffraction were obtained by slowly evaporating a solution dissolved in a mixture of aceto­nitrile and toluene.

6. Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link]. The C-bound H atoms were placed in geometrically calculated positions (C—H = 0.95–0.99 Å) and were constrained using a riding model with Uiso(H) = 1.2 Ueq(C) for aromatic H atoms and Uiso(H) = 1.5Ueq(C) for methyl H atoms. Anisotropic displacement parameters for the C25 and O7 were refined with enhanced rigid bond (RIGU) restraints.

Table 2
Experimental details

Crystal data
Chemical formula C36H33NO6S3
Mr 671.81
Crystal system, space group Monoclinic, P21/n
Temperature (K) 100
a, b, c (Å) 15.5226 (2), 7.7010 (1), 26.7200 (3)
β (°) 91.204 (1)
V3) 3193.39 (7)
Z 4
Radiation type Cu Kα
μ (mm−1) 2.53
Crystal size (mm) 0.21 × 0.16 × 0.06
 
Data collection
Diffractometer XtaLAB Synergy, Dualflex, HyPix
Absorption correction Multi-scan (CrysAlis PRO; Rigaku OD, 2023View full citation)
Tmin, Tmax 0.743, 1.000
No. of measured, independent and observed [I > 2σ(I)] reflections 22361, 6361, 5681
Rint 0.033
(sin θ/λ)max−1) 0.632
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.041, 0.111, 1.02
No. of reflections 6361
No. of parameters 421
No. of restraints 3
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.94, −0.42
Computer programs: CrysAlis PRO (Rigaku OD, 2023View full citation), SHELXT2018/2 (Sheldrick, 2015aView full citation), SHELXL2018/3 (Sheldrick, 2015bView full citation) and OLEX2 (Dolomanov et al., 2009View full citation).

Supporting information


Computing details top

Tris[4-(3,4-dimethoxythiophen-2-yl)phenyl]amine top
Crystal data top
C36H33NO6S3F(000) = 1408
Mr = 671.81Dx = 1.397 Mg m3
Monoclinic, P21/nCu Kα radiation, λ = 1.54184 Å
a = 15.5226 (2) ÅCell parameters from 14178 reflections
b = 7.7010 (1) Åθ = 3.3–76.6°
c = 26.7200 (3) ŵ = 2.53 mm1
β = 91.204 (1)°T = 100 K
V = 3193.39 (7) Å3Block, colourless
Z = 40.21 × 0.16 × 0.06 mm
Data collection top
XtaLAB Synergy, Dualflex, HyPix
diffractometer
6361 independent reflections
Radiation source: micro-focus sealed X-ray tube, PhotonJet (Cu) X-ray Source5681 reflections with I > 2σ(I)
Mirror monochromatorRint = 0.033
Detector resolution: 10.0000 pixels mm-1θmax = 77.2°, θmin = 3.3°
ω scansh = 1813
Absorption correction: multi-scan
(CrysAlisPro; Rigaku OD, 2023)
k = 89
Tmin = 0.743, Tmax = 1.000l = 3333
22361 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)] = 0.041H-atom parameters constrained
wR(F2) = 0.111 w = 1/[σ2(Fo2) + (0.0509P)2 + 3.2582P]
where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
6361 reflectionsΔρmax = 0.94 e Å3
421 parametersΔρmin = 0.42 e Å3
3 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. 1. Fixed Uiso At 1.2 times of: All C(H) groups At 1.5 times of: All C(H,H,H) groups 2. Rigid body (RIGU) restrains C25, O7 with sigma for 1-2 distances of 0.004 and sigma for 1-3 distances of 0.004 3.a Aromatic/amide H refined with riding coordinates: C11(H11), C16(H16), C17(H17), C19(H19), C20(H20), C23(H23), C28(H28), C29(H29), C31(H31), C32(H32), C35(H35), C40(H40), C41(H41), C43(H43), C44(H44) 3.b Idealised Me refined as rotating group: C21(H21A,H21B,H21C), C22(H22A,H22B,H22C), C33(H33A,H33B,H33C), C34(H34A,H34B, H34C), C45(H45A,H45B,H45C), C46(H46A,H46B,H46C)

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.15454 (3)0.61897 (6)0.74361 (2)0.02413 (12)
S20.88651 (3)0.67913 (7)0.84372 (2)0.02604 (13)
S30.65454 (3)0.69538 (7)0.42247 (2)0.02619 (13)
O40.01202 (9)0.8147 (2)0.64844 (6)0.0328 (4)
O50.15437 (8)0.84512 (19)0.61326 (5)0.0249 (3)
O60.80763 (10)0.6858 (2)0.98068 (5)0.0340 (4)
O70.66877 (9)0.7054 (2)0.91195 (5)0.0268 (3)
O80.89878 (9)0.7417 (2)0.39631 (6)0.0321 (3)
O90.86873 (8)0.70643 (19)0.49969 (5)0.0267 (3)
N100.56623 (9)0.6838 (2)0.66955 (6)0.0187 (3)
C110.05196 (12)0.6737 (3)0.72270 (8)0.0272 (4)
H110.0008900.6524590.7406950.033*
C120.05418 (12)0.7512 (3)0.67704 (8)0.0253 (4)
C130.13939 (12)0.7672 (3)0.65852 (7)0.0225 (4)
C140.20158 (12)0.7025 (2)0.69029 (7)0.0204 (4)
C150.29556 (11)0.6979 (2)0.68452 (7)0.0190 (4)
C160.33683 (12)0.8166 (2)0.65342 (7)0.0198 (4)
H160.3037300.9008600.6355630.024*
C170.42564 (11)0.8124 (2)0.64839 (7)0.0196 (4)
H170.4529210.8946210.6274730.024*
C180.47490 (11)0.6885 (2)0.67382 (7)0.0179 (4)
C190.43444 (12)0.5700 (3)0.70489 (7)0.0219 (4)
H190.4676240.4849140.7223640.026*
C200.34577 (12)0.5757 (3)0.71040 (7)0.0221 (4)
H200.3188980.4953810.7320900.027*
C210.09498 (13)0.8072 (3)0.67058 (10)0.0395 (6)
H21A0.1372250.8666660.6488670.059*
H21B0.0925170.8641100.7033790.059*
H21C0.1120740.6855830.6746680.059*
C220.15958 (17)0.7259 (3)0.57280 (9)0.0398 (5)
H22A0.1715140.7893020.5419080.060*
H22B0.1047720.6636640.5689010.060*
H22C0.2060300.6425310.5796910.060*
C230.90087 (14)0.6775 (3)0.90789 (8)0.0299 (4)
H230.9551810.6692820.9247750.036*
C240.82440 (13)0.6896 (3)0.93090 (7)0.0244 (4)
C250.75199 (12)0.7020 (2)0.89652 (7)0.0233 (4)
C260.77498 (12)0.6958 (2)0.84772 (7)0.0228 (4)
C270.71990 (12)0.6918 (2)0.80234 (7)0.0200 (4)
C280.63873 (12)0.7722 (3)0.80027 (7)0.0215 (4)
H280.6179200.8295200.8290870.026*
C290.58852 (11)0.7691 (2)0.75675 (7)0.0203 (4)
H290.5338690.8247010.7560970.024*
C300.61729 (11)0.6852 (2)0.71385 (7)0.0176 (4)
C310.69720 (11)0.6013 (2)0.71623 (7)0.0201 (4)
H310.7172900.5405050.6878190.024*
C320.74708 (11)0.6062 (3)0.75967 (7)0.0214 (4)
H320.8014410.5494420.7603930.026*
C330.88133 (17)0.6453 (4)1.01196 (9)0.0425 (6)
H33A0.9048780.5325111.0021320.064*
H33B0.8640430.6403951.0469970.064*
H33C0.9253420.7352221.0080880.064*
C340.64284 (15)0.8624 (3)0.93519 (8)0.0350 (5)
H34A0.6483220.9588190.9115270.053*
H34B0.6796110.8842970.9647820.053*
H34C0.5827160.8523900.9452850.053*
C350.74226 (14)0.7185 (3)0.38445 (7)0.0276 (4)
H350.7391700.7237290.3489380.033*
C360.81654 (13)0.7282 (3)0.41233 (8)0.0246 (4)
C370.80256 (12)0.7177 (2)0.46504 (7)0.0217 (4)
C380.71760 (12)0.7016 (2)0.47683 (7)0.0203 (4)
C390.67883 (11)0.6946 (2)0.52628 (7)0.0191 (4)
C400.71954 (11)0.7724 (2)0.56792 (7)0.0205 (4)
H400.7735630.8281830.5640310.025*
C410.68258 (11)0.7693 (2)0.61449 (7)0.0190 (4)
H410.7113570.8237850.6420150.023*
C420.60348 (11)0.6873 (2)0.62174 (7)0.0175 (4)
C430.56175 (11)0.6112 (3)0.58047 (7)0.0209 (4)
H430.5075400.5561460.5843830.025*
C440.59910 (12)0.6156 (3)0.53377 (7)0.0213 (4)
H440.5696340.5635370.5061080.026*
C450.90692 (16)0.7684 (3)0.34378 (8)0.0382 (5)
H45A0.8907810.6618290.3258590.057*
H45B0.9667130.7983440.3364880.057*
H45C0.8688420.8632810.3329210.057*
C460.91999 (14)0.8600 (3)0.50474 (9)0.0358 (5)
H46A0.9439760.8901150.4722410.054*
H46B0.9670670.8392030.5290200.054*
H46C0.8840580.9557730.5164310.054*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0224 (2)0.0272 (2)0.0230 (2)0.00434 (18)0.00633 (17)0.00136 (18)
S20.0185 (2)0.0349 (3)0.0245 (2)0.00048 (18)0.00314 (17)0.00117 (19)
S30.0242 (2)0.0361 (3)0.0182 (2)0.00494 (19)0.00025 (18)0.00181 (19)
O40.0132 (6)0.0371 (8)0.0480 (9)0.0029 (6)0.0003 (6)0.0004 (7)
O50.0197 (6)0.0288 (7)0.0264 (7)0.0023 (5)0.0011 (5)0.0050 (6)
O60.0402 (9)0.0420 (9)0.0196 (7)0.0003 (7)0.0071 (6)0.0000 (6)
O70.0210 (7)0.0417 (8)0.0178 (6)0.0034 (6)0.0034 (5)0.0005 (6)
O80.0291 (7)0.0366 (8)0.0312 (8)0.0035 (6)0.0155 (6)0.0029 (6)
O90.0185 (6)0.0320 (8)0.0295 (7)0.0016 (5)0.0001 (5)0.0009 (6)
N100.0128 (7)0.0260 (8)0.0172 (7)0.0002 (6)0.0005 (6)0.0001 (6)
C110.0190 (9)0.0273 (10)0.0359 (11)0.0046 (8)0.0102 (8)0.0074 (9)
C120.0152 (9)0.0239 (10)0.0369 (11)0.0006 (7)0.0026 (8)0.0059 (8)
C130.0172 (9)0.0222 (9)0.0282 (10)0.0004 (7)0.0029 (7)0.0021 (8)
C140.0182 (9)0.0208 (9)0.0223 (9)0.0025 (7)0.0034 (7)0.0015 (7)
C150.0172 (9)0.0218 (9)0.0179 (8)0.0010 (7)0.0010 (7)0.0023 (7)
C160.0178 (9)0.0219 (9)0.0197 (9)0.0015 (7)0.0018 (7)0.0016 (7)
C170.0174 (8)0.0222 (9)0.0191 (8)0.0022 (7)0.0002 (7)0.0021 (7)
C180.0130 (8)0.0231 (9)0.0176 (8)0.0004 (7)0.0013 (6)0.0023 (7)
C190.0194 (9)0.0233 (9)0.0228 (9)0.0008 (7)0.0019 (7)0.0034 (7)
C200.0202 (9)0.0241 (9)0.0220 (9)0.0028 (7)0.0013 (7)0.0025 (7)
C210.0132 (9)0.0449 (14)0.0606 (16)0.0004 (9)0.0051 (9)0.0135 (12)
C220.0530 (14)0.0392 (13)0.0273 (11)0.0008 (11)0.0006 (10)0.0005 (10)
C230.0282 (10)0.0326 (11)0.0283 (10)0.0029 (8)0.0100 (8)0.0008 (9)
C240.0306 (10)0.0229 (9)0.0196 (9)0.0015 (8)0.0054 (8)0.0003 (7)
C250.0229 (9)0.0217 (9)0.0253 (9)0.0017 (7)0.0010 (7)0.0007 (7)
C260.0233 (9)0.0205 (9)0.0242 (9)0.0013 (7)0.0044 (7)0.0012 (7)
C270.0199 (9)0.0205 (9)0.0195 (9)0.0037 (7)0.0040 (7)0.0041 (7)
C280.0226 (9)0.0236 (9)0.0182 (8)0.0025 (7)0.0001 (7)0.0014 (7)
C290.0166 (8)0.0232 (9)0.0211 (9)0.0013 (7)0.0002 (7)0.0014 (7)
C300.0146 (8)0.0201 (9)0.0181 (8)0.0018 (7)0.0021 (6)0.0023 (7)
C310.0174 (8)0.0219 (9)0.0209 (9)0.0011 (7)0.0004 (7)0.0007 (7)
C320.0163 (8)0.0229 (9)0.0249 (9)0.0010 (7)0.0032 (7)0.0030 (7)
C330.0535 (15)0.0492 (15)0.0240 (11)0.0042 (12)0.0190 (10)0.0024 (10)
C340.0400 (12)0.0367 (12)0.0286 (11)0.0050 (10)0.0034 (9)0.0030 (9)
C350.0344 (11)0.0284 (10)0.0202 (9)0.0049 (8)0.0058 (8)0.0013 (8)
C360.0266 (10)0.0207 (9)0.0267 (10)0.0023 (8)0.0089 (8)0.0023 (8)
C370.0205 (9)0.0204 (9)0.0243 (9)0.0005 (7)0.0029 (7)0.0008 (7)
C380.0206 (9)0.0217 (9)0.0185 (9)0.0021 (7)0.0000 (7)0.0012 (7)
C390.0176 (8)0.0210 (9)0.0189 (9)0.0014 (7)0.0005 (7)0.0001 (7)
C400.0142 (8)0.0238 (9)0.0234 (9)0.0018 (7)0.0005 (7)0.0001 (7)
C410.0160 (8)0.0213 (9)0.0195 (9)0.0011 (7)0.0017 (7)0.0012 (7)
C420.0150 (8)0.0210 (9)0.0166 (8)0.0026 (7)0.0008 (6)0.0012 (7)
C430.0154 (8)0.0263 (10)0.0211 (9)0.0038 (7)0.0008 (7)0.0001 (7)
C440.0191 (8)0.0260 (10)0.0188 (9)0.0036 (7)0.0027 (7)0.0012 (7)
C450.0472 (13)0.0383 (13)0.0300 (11)0.0083 (11)0.0221 (10)0.0078 (10)
C460.0248 (10)0.0436 (13)0.0391 (12)0.0110 (9)0.0030 (9)0.0059 (10)
Geometric parameters (Å, º) top
S1—C111.729 (2)C15—C201.396 (3)
S1—C141.7381 (19)C16—C171.388 (3)
S2—C231.724 (2)C17—C181.391 (3)
S2—C261.742 (2)C18—C191.392 (3)
S3—C351.725 (2)C19—C201.388 (3)
S3—C381.7351 (19)C23—C241.351 (3)
O4—C121.359 (2)C24—C251.440 (3)
O4—C211.430 (3)C25—C261.360 (3)
O5—C131.374 (2)C26—C271.469 (3)
O5—C221.422 (3)C27—C281.404 (3)
O6—C241.361 (2)C27—C321.390 (3)
O6—C331.437 (3)C28—C291.386 (3)
O7—C251.364 (2)C29—C301.397 (3)
O7—C341.421 (3)C30—C311.399 (2)
O8—C361.359 (2)C31—C321.382 (3)
O8—C451.427 (3)C35—C361.362 (3)
O9—C371.371 (2)C36—C371.432 (3)
O9—C461.430 (3)C37—C381.368 (3)
N10—C181.425 (2)C38—C391.464 (3)
N10—C301.411 (2)C39—C401.402 (3)
N10—C421.414 (2)C39—C441.397 (3)
C11—C121.359 (3)C40—C411.381 (3)
C12—C131.427 (3)C41—C421.398 (3)
C13—C141.366 (3)C42—C431.396 (3)
C14—C151.471 (2)C43—C441.387 (3)
C15—C161.400 (3)
S1i···H45A2.93C26iv···H412.89
O5ii···H45C2.69C27vii···H312.87
O6iii···H22A2.71C28vii···H322.85
O9iv···C343.177 (3)C29vii···H322.80
C11v···H192.83C36i···H22C2.88
C13ii···H45C2.86C46viii···C463.303 (3)
C17vi···H33B2.88H21Aix···H412.38
C24iv···C403.285 (3)H44i···H442.39
C26vii···H312.82
C11—S1—C1492.56 (9)O7—C25—C24122.67 (18)
C23—S2—C2692.71 (10)C26—C25—O7124.03 (17)
C35—S3—C3892.97 (10)C26—C25—C24113.10 (18)
C12—O4—C21115.45 (18)C25—C26—S2110.04 (14)
C13—O5—C22113.62 (16)C25—C26—C27129.21 (18)
C24—O6—C33114.01 (18)C27—C26—S2120.65 (15)
C25—O7—C34115.28 (16)C28—C27—C26121.98 (17)
C36—O8—C45115.09 (18)C32—C27—C26120.36 (17)
C37—O9—C46114.76 (16)C32—C27—C28117.67 (16)
C30—N10—C18118.36 (14)C29—C28—C27120.92 (17)
C30—N10—C42121.67 (14)C28—C29—C30120.82 (17)
C42—N10—C18119.88 (14)C29—C30—N10120.56 (16)
C12—C11—S1110.90 (14)C29—C30—C31118.34 (16)
O4—C12—C11129.03 (18)C31—C30—N10121.10 (16)
O4—C12—C13117.98 (19)C32—C31—C30120.40 (17)
C11—C12—C13112.98 (18)C31—C32—C27121.82 (17)
O5—C13—C12121.20 (17)C36—C35—S3110.69 (15)
C14—C13—O5125.14 (17)O8—C36—C35128.47 (19)
C14—C13—C12113.64 (18)O8—C36—C37118.49 (18)
C13—C14—S1109.92 (14)C35—C36—C37113.01 (17)
C13—C14—C15129.30 (17)O9—C37—C36122.75 (17)
C15—C14—S1120.78 (14)C38—C37—O9123.42 (17)
C16—C15—C14120.92 (16)C38—C37—C36113.49 (17)
C20—C15—C14120.61 (17)C37—C38—S3109.83 (14)
C20—C15—C16118.47 (17)C37—C38—C39128.88 (17)
C17—C16—C15120.67 (17)C39—C38—S3121.27 (14)
C16—C17—C18120.36 (17)C40—C39—C38120.88 (16)
C17—C18—N10121.06 (16)C44—C39—C38121.83 (17)
C17—C18—C19119.38 (16)C44—C39—C40117.26 (16)
C19—C18—N10119.54 (16)C41—C40—C39121.25 (17)
C20—C19—C18120.22 (17)C40—C41—C42121.01 (17)
C19—C20—C15120.89 (17)C41—C42—N10120.73 (16)
C24—C23—S2110.83 (15)C43—C42—N10120.93 (16)
O6—C24—C25117.53 (18)C43—C42—C41118.33 (16)
C23—C24—O6129.13 (18)C44—C43—C42120.28 (17)
C23—C24—C25113.30 (18)C43—C44—C39121.86 (17)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y+2, z+1; (iii) x1/2, y+1/2, z1/2; (iv) x+3/2, y1/2, z+3/2; (v) x+1/2, y+1/2, z+3/2; (vi) x3/2, y+1/2, z3/2; (vii) x+3/2, y+1/2, z+3/2; (viii) x+2, y+2, z+1; (ix) x1, y, z.
Hydrogen-bond geometry (Å, º) top
Cg1, Cg3 and Cg5 are the centroids of the S1/C11–C14,S3/C35–C38 and C27–C32 rings, respectively.
D—H···AD—HH···AD···AD—H···A
C21—H21B···Cg5v0.982.953.686 (3)133
C22—H22C···Cg3i0.982.853.678 (2)143
C32—H32···Cg5iv0.952.873.518 (2)126
C41—H41···Cg2vii0.952.963.2346 (17)98
C45—H45A···Cg1i0.982.893.820 (2)160
S1—H20···C20v
O5—H45C···C45ii0.982.693.336 (3)123
O9—H34B···C34iv0.982.773.177 (3)106
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y+2, z+1; (iv) x+3/2, y1/2, z+3/2; (v) x+1/2, y+1/2, z+3/2; (vii) x+3/2, y+1/2, z+3/2.
 

Funding information

Funding for this research was provided by: KAKENHI (grant No. JP23K04711 to M. Y.); ESPEC Foundation for Global Environment Research and Technology (grant to M. Y.).

References

Return to citationAdelizzi, B., Rösch, A. T., van Rijen, D. J., Martire, R. S., Esiner, S., Lutz, M., Palmans, A. R. A. & Meijer, E. W. (2019). Helv. Chim. Acta 102, e1900065.  Web of Science CSD CrossRef Google Scholar
Return to citationDolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationGolba, S., Starczewska, O. & Idzik, K. (2015). Des. Monomers Polym. 18, 770–779.  Web of Science CrossRef CAS Google Scholar
Return to citationGroom, C. R., Bruno, I. J., Lightfoot, M. P. & Ward, S. C. (2016). Acta Cryst. B72, 171–179.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationLambert, C. & Nöll, G. (1999). J. Am. Chem. Soc. 121, 8434–8442.  Web of Science CrossRef CAS Google Scholar
Return to citationMcKinnon, J. J., Jayatilaka, D. & Spackman, M. A. (2007). Chem. Commun. pp. 3814–3816.  Web of Science CrossRef Google Scholar
Return to citationParthasarathy, V., Fery–Forgues, S., Campioli, E., Recher, G., Terenziani, F. & Blanchard-Desce, M. (2011). Small 7, 3219–3229.  Web of Science CSD CrossRef CAS PubMed Google Scholar
Return to citationPeng, Z. (2025a). CSD Communication (refcode ILIWAF, CCDC 2412701). CCDC, Cambridge, England.  Google Scholar
Return to citationPeng, Z. (2025b). CSD Communication (refcode ILIWEJ, CCDC 2412703). CCDC, Cambridge, England.  Google Scholar
Return to citationRigaku OD (2023). CrysAlis PRO. Rigaku Oxford Diffraction, Yarnton, England.  Google Scholar
Return to citationSato, K., Yano, M., Furuichi, M., Shiomi, D., Takui, T., Abe, K., Itoh, K., Higuchi, A., Katsuma, K. & Shirota, Y. (1997). J. Am. Chem. Soc. 119, 6607–6613.  CrossRef CAS Web of Science Google Scholar
Return to citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
Return to citationSpackman, M. A. & Jayatilaka, D. (2009). CrystEngComm 11, 19–32.  Web of Science CrossRef CAS Google Scholar
Return to citationSpackman, M. A. & McKinnon, J. J. (2002). CrystEngComm 4, 378–392.  Web of Science CrossRef CAS Google Scholar
Return to citationSpackman, P. R., Turner, M. J., McKinnon, J. J., Wolff, S. K., Grimwood, D. J., Jayatilaka, D. & Spackman, M. A. (2021). J. Appl. Cryst. 54, 1006–1011.  Web of Science CrossRef CAS IUCr Journals Google Scholar
Return to citationThelakkat, M. (2002). Macromol. Mater. Eng. 287, 442–461.  CrossRef CAS Google Scholar
Return to citationWang, Q., He, Z., Wild, A., Wu, H., Cao, Y., Schubert, U. S., Chui, C. H. & Wong, W. Y. (2011). Chem. ? An. Asia. J. 6, 1766–1777.  Google Scholar
Return to citationYano, M., Inada, Y., Hayashi, Y., Nakai, M., Mitsudo, K. & Kashiwagi, Y. (2022). Dyes Pigments 197, 109929.  Web of Science CrossRef Google Scholar
Return to citationYen, H.-J. & Liou, G.-S. (2012). Polym. Chem. 3, 255–264.  Web of Science CrossRef CAS Google Scholar
Return to citationYuan, G., Lv, C., Liang, J., Zhong, X., Li, Y., He, J., Zhao, A., Li, L., Shao, Y., Zhang, X., Wang, S., Cheng, Y. & He, H. (2021). Adv. Funct. Mater. 31, 2104026.  Web of Science CSD CrossRef Google Scholar

This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.

Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds