organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

1,2-Bis[5-(9-ethyl-9H-carbazol-3-yl)-2-methyl­thio­phen-3-yl]-3,3,4,4,5,5-hexa­fluoro­cyclo­pentene

aDivision of Natural Sciences, Osaka Kyoiku University, Kashiwara, Osaka 582-8582, Japan, and bInstitute for Materials Chemistry and Engineering, Kyushu University, Hakozaki 6-10-1, Higashi-ku, Fukuoka 812-8581, Japan
*Correspondence e-mail: kubono@cc.osaka-kyoiku.ac.jp

(Received 6 July 2011; accepted 21 July 2011; online 30 July 2011)

The title compound, C43H32F6N2S2, is a new symmetrical photochromic diaryl­ethene derivative with 9-ethyl­carbazol-3-yl substituents. The mol­ecule adopts a photoactive anti­parallel conformation [Irie (2000). Chem. Rev. 100, 1685–1716; Kobatake et al. (2002). Chem. Commun. pp. 2804–2805], with a dihedral angle between the mean planes of the two thio­phene rings of 56.23 (6)°. The distance between the two reactive C atoms is 3.497 (3) Å. In the crystal, two mol­ecules are associated through a pair of C—H⋯F inter­molecular hydrogen bonds, forming a centrosymmetric dimer. Dimers are linked by weak ππ inter­actions [centroid–centroid distance = 3.8872 (13) Å], forming chains along the c axis.

Related literature

For a review of diaryl­ethenes, see: Irie (2000[Irie, M. (2000). Chem. Rev. 100, 1685-1716.]). For related structures, see: Irie et al. (1995[Irie, M., Sakemura, K., Okinaka, M. & Uchida, K. (1995). J. Org. Chem. 60, 8305-8309.], 2001[Irie, M., Kobatake, S. & Horiuchi, M. (2001). Science, 291, 1769-1772.]); Kobatake et al. (2002[Kobatake, S., Uchida, K., Tsuchida, E. & Irie, M. (2002). Chem. Commun. pp. 2804-2805.]); Takami & Irie et al. (2004[Takami, S. & Irie, M. (2004). Tetrahedron, 60, 6155-6161.]). For a review of carbazole, see: Grigalevicius (2006[Grigalevicius, S. (2006). Synth. Met. 156, 1-12.]). For hydrogen-bond motifs, see: Bernstein et al. (1995[Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.]).

[Scheme 1]

Experimental

Crystal data
  • C43H32F6N2S2

  • Mr = 754.85

  • Monoclinic, P 21 /c

  • a = 14.6687 (7) Å

  • b = 17.0977 (8) Å

  • c = 14.0017 (7) Å

  • β = 95.798 (3)°

  • V = 3493.7 (3) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 1.97 mm−1

  • T = 123 K

  • 0.34 × 0.18 × 0.11 mm

Data collection
  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995[Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan.]) Tmin = 0.687, Tmax = 0.806

  • 40777 measured reflections

  • 6393 independent reflections

  • 5482 reflections with F2 > 2σ(F2)

  • Rint = 0.045

Refinement
  • R[F2 > 2σ(F2)] = 0.049

  • wR(F2) = 0.139

  • S = 1.00

  • 6393 reflections

  • 479 parameters

  • H-atom parameters constrained

  • Δρmax = 0.90 e Å−3

  • Δρmin = −0.50 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C26—H26⋯F2i 0.95 2.44 3.290 (2) 149 (1)
Symmetry code: (i) -x+1, -y+2, -z+1.

Data collection: PROCESS-AUTO (Rigaku, 2006[Rigaku (2006). PROCESS-AUTO. Rigaku Corporation, Tokyo, Japan.]); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC, 2006[Rigaku/MSC (2006). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.]); program(s) used to solve structure: SIR92 (Altomare et al., 1993[Altomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343-350.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: PLATON (Spek, 2009[Spek, A. L. (2009). Acta Cryst. D65, 148-155.]); software used to prepare material for publication: CrystalStructure.

Supporting information


Comment top

Diarylethenes are well known photochromic compounds both in solution and in solid state (Irie, 2000), and have attracted much attention because of their potential application to optical memory, photoswitches (Irie, et al. 2001), and display devices (Takami & Irie, 2004). It was reported that diarylethenes can undergo a photochemical ring-closure reaction in the crystalline phase when the ring-opening forms are in the anti-parallel conformation and where the distance between two reactive C atoms is shorter than 4.2 Å (Irie, et al. 1995; Kobatake, et al. 2002). Therefore, X-ray analysis of diarylethenes will give valuable information for their photochromism in solid state. We have prepared the title compound, (I), a symmetrical diarylethene derivative containing carbazole moiety as hole transport material (Grigalevicius, 2006) to study not only its photochromism but also its electrical properties. In this paper, the molecular and crystal structure of (I) is presented.

In the molecular structure of (I), the thiophene rings are located in a photoactive anti-parallel conformation which can effectively undergo photocyclization reactions; with the dihedral angle between the mean planes of two thiophene rings, S1/C6–C9 and S2/C26–C28, of 56.23 (6) ° (Fig. 1). The dihedral angles between the thiophene rings and adjacent carbazole moieties are 23.49 (5) ° for S1/C6–C9 and N1/C11–C22, and 23.19 (5) ° for S2/C26–C28 and N2/C30–C41. The distance between two reactive C atoms in ring-closure reaction, C7···C28, is 3.497 (3) Å. This distance is shorter than 4.2 Å, suggesting that (I) can undergo the ring-closure reaction and photochromism in the crystalline phase by UV irradiation.

In the crystal structure of (I), there are intermolecular C—H···F hydrogen bonds (Fig. 2 and Table 1). Two molecules are associated through a pair of C—H···F intermolecular hydrogen bonds, forming a centrosymmetric dimer with a R22(14) ring motif (Bernstein et al., 1995). In the crystal, intermolecular C···C distances between carbazole moieties for C30···C36ii and C34···C34ii [symmetry code: (ii) 1 - x, 2 - y, 2 - z] are 3.657 (3) and 3.659 (3) Å, respectively. Dimers are linked by weak ππ interactions between carbazole moieties to give one-dimensional supramolecular chains propagating along the c axis.

Related literature top

For a review of diarylethenes, see: Irie (2000). For related structures, see: Irie et al. (1995, 2001); Kobatake et al. (2002); Takami & Irie et al. (2004). For a review of carbazole, see: Grigalevicius (2006). For hydrogen-bond motifs, see: Bernstein et al. (1995).

Experimental top

The title compound, (I), was prepared by the treatment of 3-bromo-5-(9-ethylcarbazolyl)-2-methylthiophene with butyl lithium, then with octafluorocyclopentene. The product was recrystallized from benzene-hexane to give plate crystals, m.p. 458–460 K; 1H NMR (CDCl3, p.p.m. 400 MHz): 1.45 (t, J = 7.2 Hz, 6H, Et), 2.05 (s, 6H, CH3), 4.38 (q, J = 7.2 Hz, 4H, Et), 7.20–7.24 (m, 2H, carbazole), 7.32 (s, 2H, thiophene). 7.39–7.43 (m, 2H, carbazole), 7.47–7.52 (m, 2H, carbazole), 7.67 (dd, J = 7.8 Hz, J' = 1.6 Hz, 2H, carbazole), 8.11 (d, J = 7.8 Hz, 2H, carbazole), 8.25 (d, J = 1.6 Hz, 2H, carbazole); HRMS(FAB): calculated for C43H32F6N2S2: 754.1911, found(M+): 754.1908.

Refinement top

All H atoms bound to C atoms were placed at idealized positions and refined as a riding atoms, with C—H = 0.93–0.97Å and Uiso(H) = 1.2 Ueq(C) [1.5Ueq(C) for methyl H atoms]. Structure was refined with unique reflections and with a cut-off sigma = 2.00.

Computing details top

Data collection: PROCESS-AUTO (Rigaku, 2006); cell refinement: PROCESS-AUTO (Rigaku, 2006); data reduction: CrystalStructure (Rigaku/MSC, 2006); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: PLATON (Spek, 2009); software used to prepare material for publication: CrystalStructure (Rigaku/MSC, 2006).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) with the atom-labelling scheme and displacement ellipsoids are drawn at the 50% probability level. H atoms are omitted for clarity.
[Figure 2] Fig. 2. A packing diagram of (I), viewed down the b axis. The C—H···F hydrogen bonds are shown as dashed lines.
1,2-Bis[5-(9-ethyl-9H-carbazol-3-yl)-2-methylthiophen-3-yl]- 3,3,4,4,5,5-hexafluorocyclopentene top
Crystal data top
C43H32F6N2S2F(000) = 1560.00
Mr = 754.85Dx = 1.435 Mg m3
Monoclinic, P21/cCu Kα radiation, λ = 1.54187 Å
Hall symbol: -P 2ybcCell parameters from 36134 reflections
a = 14.6687 (7) Åθ = 3.0–68.3°
b = 17.0977 (8) ŵ = 1.97 mm1
c = 14.0017 (7) ÅT = 123 K
β = 95.798 (3)°Plate, blue
V = 3493.7 (3) Å30.34 × 0.18 × 0.11 mm
Z = 4
Data collection top
Rigaku R-AXIS RAPID
diffractometer
5482 reflections with F2 > 2σ(F2)
Detector resolution: 5.00 pixels mm-1Rint = 0.045
ω scansθmax = 68.3°
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
h = 1717
Tmin = 0.687, Tmax = 0.806k = 2020
40777 measured reflectionsl = 1616
6393 independent reflections
Refinement top
Refinement on F2H-atom parameters constrained
R[F2 > 2σ(F2)] = 0.049 w = 1/[σ2(Fo2) + (0.0796P)2 + 3.7293P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.139(Δ/σ)max = 0.001
S = 1.00Δρmax = 0.90 e Å3
6393 reflectionsΔρmin = 0.50 e Å3
479 parameters
Crystal data top
C43H32F6N2S2V = 3493.7 (3) Å3
Mr = 754.85Z = 4
Monoclinic, P21/cCu Kα radiation
a = 14.6687 (7) ŵ = 1.97 mm1
b = 17.0977 (8) ÅT = 123 K
c = 14.0017 (7) Å0.34 × 0.18 × 0.11 mm
β = 95.798 (3)°
Data collection top
Rigaku R-AXIS RAPID
diffractometer
6393 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
5482 reflections with F2 > 2σ(F2)
Tmin = 0.687, Tmax = 0.806Rint = 0.045
40777 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.049479 parameters
wR(F2) = 0.139H-atom parameters constrained
S = 1.00Δρmax = 0.90 e Å3
6393 reflectionsΔρmin = 0.50 e Å3
Special details top

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

Refinement. Refinement was performed using all reflections. The weighted R-factor (wR) and goodness of fit (S) are based on F2. R-factor (gt) are based on F. The threshold expression of F2 > 2.0 σ(F2) is used only for calculating R-factor (gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S10.22266 (5)0.77807 (4)0.34058 (5)0.03204 (16)
S20.20529 (4)0.90769 (4)0.72247 (4)0.02856 (16)
F10.28611 (10)1.07557 (9)0.27753 (10)0.0337 (3)
F20.42244 (10)1.03335 (9)0.32305 (11)0.0381 (3)
F30.28436 (11)1.17289 (9)0.41361 (11)0.0392 (3)
F40.43102 (11)1.17032 (10)0.40307 (11)0.0428 (4)
F50.33901 (11)1.13896 (8)0.58847 (10)0.0342 (3)
F60.46135 (10)1.07923 (9)0.55108 (10)0.0326 (3)
N10.06405 (14)0.78041 (12)0.06739 (15)0.0268 (4)
N20.50050 (14)0.87561 (12)1.12292 (14)0.0252 (4)
C10.30629 (15)0.99316 (13)0.41816 (16)0.0217 (4)
C20.34231 (16)1.05578 (14)0.35643 (17)0.0243 (4)
C30.35960 (17)1.12687 (14)0.42239 (17)0.0263 (5)
C40.37050 (16)1.09033 (14)0.52264 (17)0.0243 (5)
C50.31915 (15)1.01445 (13)0.51163 (16)0.0214 (4)
C60.26821 (16)0.92071 (14)0.37434 (17)0.0236 (4)
C70.28281 (17)0.84660 (14)0.41198 (18)0.0281 (5)
C80.17827 (16)0.84749 (14)0.25868 (17)0.0260 (5)
C90.21055 (16)0.91970 (14)0.28574 (17)0.0241 (4)
C100.34286 (19)0.81983 (15)0.49802 (19)0.0335 (5)
C110.11541 (16)0.82652 (14)0.17425 (17)0.0249 (5)
C120.06121 (16)0.75866 (14)0.17428 (17)0.0268 (5)
C130.00007 (16)0.73789 (14)0.09707 (18)0.0274 (5)
C140.00796 (16)0.78690 (14)0.01743 (18)0.0254 (5)
C150.04468 (16)0.85586 (14)0.01595 (17)0.0236 (4)
C160.10621 (16)0.87512 (14)0.09387 (17)0.0246 (5)
C170.04857 (16)0.84348 (14)0.12509 (17)0.0262 (5)
C180.01812 (16)0.89281 (14)0.07567 (17)0.0254 (5)
C190.04274 (17)0.96190 (15)0.11862 (18)0.0296 (5)
C200.00271 (19)0.97990 (16)0.20982 (19)0.0341 (5)
C210.06116 (18)0.92965 (16)0.25817 (19)0.0339 (6)
C220.08871 (18)0.86168 (16)0.21681 (18)0.0321 (5)
C230.13082 (18)0.71836 (16)0.0910 (2)0.0331 (5)
C240.0899 (2)0.64855 (16)0.1365 (2)0.0391 (6)
C250.29322 (16)0.97565 (13)0.59806 (16)0.0217 (4)
C260.35396 (16)0.96925 (13)0.68333 (16)0.0233 (4)
C270.31788 (16)0.93281 (13)0.75725 (17)0.0229 (4)
C280.20781 (16)0.94502 (14)0.60858 (17)0.0261 (5)
C290.12464 (17)0.94189 (17)0.53832 (18)0.0318 (5)
C300.36117 (16)0.91630 (13)0.85442 (17)0.0234 (4)
C310.30891 (17)0.90623 (14)0.93247 (17)0.0255 (5)
C320.34847 (17)0.89227 (14)1.02435 (17)0.0254 (5)
C330.44370 (17)0.88832 (13)1.03932 (16)0.0232 (4)
C340.49780 (16)0.89756 (13)0.96205 (16)0.0228 (4)
C350.45622 (17)0.91139 (13)0.87016 (17)0.0237 (4)
C360.59047 (17)0.87628 (13)1.10144 (17)0.0254 (5)
C370.59257 (16)0.88950 (13)1.00191 (17)0.0238 (4)
C380.67583 (17)0.89345 (15)0.96312 (18)0.0285 (5)
C390.75581 (17)0.88401 (15)1.02312 (19)0.0315 (5)
C400.75293 (18)0.87091 (16)1.12114 (19)0.0341 (5)
C410.67171 (18)0.86625 (15)1.16179 (18)0.0305 (5)
C420.47018 (19)0.86212 (15)1.21760 (17)0.0290 (5)
C430.4644 (2)0.77700 (17)1.2437 (2)0.0450 (7)
H90.19600.96550.24890.029*
H10A0.33750.76300.50460.040*
H10B0.32400.84540.55550.040*
H10C0.40660.83350.49060.040*
H120.06700.72590.22940.032*
H130.03570.69160.09830.033*
H160.14210.92130.09260.030*
H190.08630.99620.08600.036*
H200.01891.02700.23980.041*
H210.08630.94270.32140.041*
H220.13340.82850.24960.039*
H23A0.18170.73930.13560.040*
H23B0.15670.70150.03170.040*
H24A0.13740.60880.15110.047*
H24B0.04050.62680.09210.047*
H24C0.06530.66470.19600.047*
H260.41490.98880.68840.028*
H29A0.07480.91620.56790.038*
H29B0.13830.91230.48150.038*
H29C0.10610.99520.51930.038*
H310.24400.90920.92140.031*
H320.31190.88551.07600.030*
H350.49250.91750.81820.028*
H380.67780.90250.89640.034*
H390.81330.88650.99740.038*
H400.80890.86501.16100.041*
H410.67070.85661.22850.037*
H42A0.40910.88621.21980.035*
H42B0.51320.88861.26630.035*
H43A0.44400.77221.30790.054*
H43B0.52490.75281.24310.054*
H43C0.42060.75061.19700.054*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0406 (3)0.0251 (3)0.0276 (3)0.0005 (2)0.0101 (2)0.0004 (2)
S20.0251 (3)0.0382 (3)0.0217 (3)0.0050 (2)0.0011 (2)0.0071 (2)
F10.0398 (8)0.0397 (8)0.0191 (7)0.0037 (6)0.0086 (6)0.0084 (6)
F20.0342 (8)0.0433 (8)0.0394 (9)0.0045 (6)0.0168 (7)0.0049 (6)
F30.0533 (9)0.0322 (8)0.0310 (8)0.0156 (7)0.0006 (7)0.0054 (6)
F40.0499 (9)0.0477 (9)0.0298 (8)0.0243 (7)0.0007 (7)0.0087 (6)
F50.0527 (9)0.0269 (7)0.0232 (7)0.0022 (6)0.0045 (6)0.0030 (5)
F60.0269 (7)0.0406 (8)0.0281 (7)0.0080 (6)0.0077 (6)0.0069 (6)
N10.0246 (10)0.0311 (10)0.0234 (10)0.0023 (8)0.0044 (8)0.0039 (8)
N20.0310 (10)0.0295 (10)0.0144 (9)0.0024 (8)0.0012 (8)0.0004 (7)
C10.0197 (10)0.0258 (11)0.0189 (11)0.0023 (8)0.0020 (8)0.0019 (9)
C20.0209 (11)0.0331 (12)0.0183 (11)0.0031 (9)0.0010 (9)0.0026 (9)
C30.0283 (12)0.0272 (12)0.0229 (12)0.0027 (9)0.0004 (9)0.0062 (9)
C40.0251 (11)0.0289 (12)0.0177 (11)0.0002 (9)0.0027 (9)0.0001 (9)
C50.0196 (10)0.0249 (11)0.0189 (11)0.0020 (8)0.0019 (8)0.0022 (8)
C60.0245 (11)0.0272 (11)0.0185 (11)0.0015 (9)0.0013 (9)0.0004 (9)
C70.0322 (13)0.0266 (12)0.0239 (12)0.0009 (9)0.0054 (10)0.0012 (9)
C80.0258 (11)0.0295 (12)0.0218 (12)0.0016 (9)0.0026 (9)0.0010 (9)
C90.0269 (12)0.0267 (11)0.0180 (11)0.0015 (9)0.0011 (9)0.0003 (9)
C100.0382 (14)0.0282 (12)0.0312 (14)0.0046 (10)0.0108 (11)0.0018 (10)
C110.0234 (11)0.0282 (12)0.0224 (12)0.0017 (9)0.0014 (9)0.0013 (9)
C120.0291 (12)0.0281 (12)0.0225 (12)0.0006 (9)0.0002 (10)0.0017 (9)
C130.0270 (12)0.0280 (12)0.0270 (13)0.0037 (9)0.0011 (10)0.0016 (9)
C140.0228 (11)0.0280 (12)0.0251 (12)0.0006 (9)0.0007 (9)0.0053 (9)
C150.0229 (11)0.0260 (11)0.0221 (12)0.0001 (8)0.0031 (9)0.0018 (9)
C160.0237 (11)0.0248 (11)0.0250 (12)0.0013 (9)0.0002 (9)0.0017 (9)
C170.0251 (11)0.0294 (12)0.0240 (12)0.0044 (9)0.0010 (9)0.0041 (9)
C180.0249 (11)0.0293 (12)0.0219 (12)0.0037 (9)0.0026 (9)0.0016 (9)
C190.0300 (12)0.0308 (12)0.0282 (13)0.0006 (10)0.0032 (10)0.0015 (10)
C200.0386 (14)0.0347 (13)0.0290 (14)0.0076 (11)0.0040 (11)0.0061 (10)
C210.0364 (14)0.0424 (14)0.0221 (13)0.0139 (11)0.0007 (11)0.0024 (11)
C220.0291 (12)0.0405 (14)0.0255 (13)0.0076 (10)0.0032 (10)0.0055 (11)
C230.0278 (12)0.0384 (14)0.0317 (14)0.0070 (10)0.0043 (10)0.0019 (11)
C240.0435 (16)0.0335 (14)0.0381 (16)0.0071 (11)0.0072 (12)0.0054 (11)
C250.0240 (11)0.0217 (10)0.0184 (11)0.0009 (8)0.0028 (9)0.0007 (8)
C260.0247 (11)0.0261 (11)0.0182 (11)0.0027 (9)0.0024 (9)0.0007 (9)
C270.0240 (11)0.0229 (11)0.0214 (11)0.0013 (8)0.0000 (9)0.0011 (9)
C280.0261 (12)0.0300 (12)0.0212 (12)0.0021 (9)0.0017 (9)0.0025 (9)
C290.0244 (12)0.0454 (15)0.0245 (13)0.0013 (10)0.0038 (10)0.0073 (11)
C300.0273 (12)0.0228 (11)0.0192 (11)0.0004 (9)0.0014 (9)0.0011 (8)
C310.0255 (12)0.0268 (12)0.0238 (12)0.0008 (9)0.0006 (9)0.0018 (9)
C320.0292 (12)0.0271 (11)0.0202 (12)0.0004 (9)0.0041 (9)0.0028 (9)
C330.0310 (12)0.0216 (11)0.0167 (11)0.0001 (9)0.0010 (9)0.0002 (8)
C340.0275 (12)0.0225 (10)0.0179 (11)0.0001 (8)0.0009 (9)0.0004 (8)
C350.0279 (12)0.0251 (11)0.0181 (11)0.0015 (9)0.0017 (9)0.0006 (9)
C360.0317 (12)0.0229 (11)0.0210 (12)0.0023 (9)0.0004 (10)0.0017 (9)
C370.0273 (12)0.0233 (11)0.0199 (11)0.0014 (9)0.0025 (9)0.0012 (9)
C380.0322 (13)0.0329 (12)0.0198 (12)0.0025 (10)0.0008 (10)0.0008 (10)
C390.0264 (12)0.0365 (13)0.0309 (14)0.0039 (10)0.0008 (10)0.0051 (10)
C400.0324 (13)0.0362 (14)0.0311 (14)0.0075 (10)0.0089 (11)0.0053 (11)
C410.0361 (13)0.0337 (13)0.0195 (12)0.0049 (10)0.0075 (10)0.0026 (10)
C420.0388 (14)0.0341 (13)0.0141 (11)0.0055 (10)0.0023 (10)0.0026 (9)
C430.069 (2)0.0389 (15)0.0292 (14)0.0049 (14)0.0183 (14)0.0001 (11)
Geometric parameters (Å, º) top
S1—C71.724 (2)C30—C311.407 (3)
S1—C81.731 (2)C30—C351.392 (3)
S2—C271.728 (2)C31—C321.378 (3)
S2—C281.722 (2)C32—C331.393 (3)
F1—C21.353 (2)C33—C341.414 (3)
F2—C21.363 (2)C34—C351.387 (3)
F3—C31.351 (2)C34—C371.451 (3)
F4—C31.334 (3)C36—C371.415 (3)
F5—C41.357 (2)C36—C411.400 (3)
F6—C41.365 (2)C37—C381.388 (3)
N1—C141.379 (3)C38—C391.382 (3)
N1—C171.380 (3)C39—C401.395 (3)
N1—C231.459 (3)C40—C411.374 (3)
N2—C331.384 (2)C42—C431.505 (3)
N2—C361.383 (3)C9—H90.950
N2—C421.459 (3)C10—H10A0.980
C1—C21.505 (3)C10—H10B0.980
C1—C51.353 (3)C10—H10C0.980
C1—C61.468 (3)C12—H120.950
C2—C31.532 (3)C13—H130.950
C3—C41.530 (3)C16—H160.950
C4—C51.500 (3)C19—H190.950
C5—C251.464 (3)C20—H200.950
C6—C71.381 (3)C21—H210.950
C6—C91.429 (3)C22—H220.950
C7—C101.491 (3)C23—H23A0.990
C8—C91.362 (3)C23—H23B0.990
C8—C111.468 (3)C24—H24A0.980
C11—C121.407 (3)C24—H24B0.980
C11—C161.395 (3)C24—H24C0.980
C12—C131.381 (3)C26—H260.950
C13—C141.390 (3)C29—H29A0.980
C14—C151.411 (3)C29—H29B0.980
C15—C161.384 (3)C29—H29C0.980
C15—C181.448 (3)C31—H310.950
C17—C181.418 (3)C32—H320.950
C17—C221.393 (3)C35—H350.950
C18—C191.390 (3)C38—H380.950
C19—C201.385 (3)C39—H390.950
C20—C211.395 (3)C40—H400.950
C21—C221.377 (3)C41—H410.950
C23—C241.506 (3)C42—H42A0.990
C25—C261.420 (3)C42—H42B0.990
C25—C281.379 (3)C43—H43A0.980
C26—C271.360 (3)C43—H43B0.980
C27—C301.470 (3)C43—H43C0.980
C28—C291.489 (3)
C7—S1—C893.12 (11)C32—C33—C34120.7 (2)
C27—S2—C2893.41 (11)C33—C34—C35120.0 (2)
C14—N1—C17108.79 (19)C33—C34—C37106.56 (19)
C14—N1—C23125.6 (2)C35—C34—C37133.4 (2)
C17—N1—C23125.6 (2)C30—C35—C34119.8 (2)
C33—N2—C36108.73 (19)N2—C36—C37109.37 (19)
C33—N2—C42125.5 (2)N2—C36—C41129.8 (2)
C36—N2—C42125.75 (19)C37—C36—C41120.8 (2)
C2—C1—C5109.96 (19)C34—C37—C36106.2 (2)
C2—C1—C6120.08 (19)C34—C37—C38133.8 (2)
C5—C1—C6129.9 (2)C36—C37—C38120.1 (2)
F1—C2—F2105.41 (18)C37—C38—C39118.9 (2)
F1—C2—C1115.25 (18)C38—C39—C40120.6 (2)
F1—C2—C3110.11 (18)C39—C40—C41122.0 (2)
F2—C2—C1111.20 (18)C36—C41—C40117.6 (2)
F2—C2—C3109.51 (18)N2—C42—C43113.8 (2)
C1—C2—C3105.34 (19)C6—C9—H9122.9
F3—C3—F4107.96 (19)C8—C9—H9122.9
F3—C3—C2108.86 (18)C7—C10—H10A109.5
F3—C3—C4109.3 (2)C7—C10—H10B109.5
F4—C3—C2113.9 (2)C7—C10—H10C109.5
F4—C3—C4113.70 (19)H10A—C10—H10B109.5
C2—C3—C4102.98 (18)H10A—C10—H10C109.5
F5—C4—F6106.05 (17)H10B—C10—H10C109.5
F5—C4—C3111.22 (18)C11—C12—H12118.8
F5—C4—C5113.45 (19)C13—C12—H12118.8
F6—C4—C3109.44 (19)C12—C13—H13121.1
F6—C4—C5112.02 (18)C14—C13—H13121.0
C3—C4—C5104.71 (18)C11—C16—H16120.1
C1—C5—C4110.6 (2)C15—C16—H16120.1
C1—C5—C25130.9 (2)C18—C19—H19120.6
C4—C5—C25118.47 (19)C20—C19—H19120.5
C1—C6—C7125.3 (2)C19—C20—H20119.6
C1—C6—C9122.7 (2)C21—C20—H20119.6
C7—C6—C9112.1 (2)C20—C21—H21119.1
S1—C7—C6110.60 (17)C22—C21—H21119.1
S1—C7—C10119.07 (17)C17—C22—H22121.3
C6—C7—C10130.3 (2)C21—C22—H22121.3
S1—C8—C9109.89 (17)N1—C23—H23A109.1
S1—C8—C11121.97 (17)N1—C23—H23B109.1
C9—C8—C11128.1 (2)C24—C23—H23A109.1
C6—C9—C8114.3 (2)C24—C23—H23B109.1
C8—C11—C12120.7 (2)H23A—C23—H23B107.8
C8—C11—C16120.4 (2)C23—C24—H24A109.5
C12—C11—C16118.9 (2)C23—C24—H24B109.5
C11—C12—C13122.4 (2)C23—C24—H24C109.5
C12—C13—C14117.9 (2)H24A—C24—H24B109.5
N1—C14—C13129.5 (2)H24A—C24—H24C109.5
N1—C14—C15109.5 (2)H24B—C24—H24C109.5
C13—C14—C15120.9 (2)C25—C26—H26122.7
C14—C15—C16120.1 (2)C27—C26—H26122.7
C14—C15—C18106.20 (19)C28—C29—H29A109.5
C16—C15—C18133.7 (2)C28—C29—H29B109.5
C11—C16—C15119.8 (2)C28—C29—H29C109.5
N1—C17—C18108.99 (19)H29A—C29—H29B109.5
N1—C17—C22129.4 (2)H29A—C29—H29C109.5
C18—C17—C22121.6 (2)H29B—C29—H29C109.5
C15—C18—C17106.5 (2)C30—C31—H31118.8
C15—C18—C19134.1 (2)C32—C31—H31118.8
C17—C18—C19119.4 (2)C31—C32—H32121.0
C18—C19—C20118.9 (2)C33—C32—H32121.0
C19—C20—C21120.8 (2)C30—C35—H35120.1
C20—C21—C22121.8 (2)C34—C35—H35120.1
C17—C22—C21117.5 (2)C37—C38—H38120.6
N1—C23—C24112.7 (2)C39—C38—H38120.6
C5—C25—C26122.5 (2)C38—C39—H39119.7
C5—C25—C28125.1 (2)C40—C39—H39119.7
C26—C25—C28112.4 (2)C39—C40—H40119.0
C25—C26—C27114.6 (2)C41—C40—H40119.0
S2—C27—C26109.49 (16)C36—C41—H41121.2
S2—C27—C30121.63 (18)C40—C41—H41121.2
C26—C27—C30128.9 (2)N2—C42—H42A108.8
S2—C28—C25110.14 (16)N2—C42—H42B108.8
S2—C28—C29120.39 (18)C43—C42—H42A108.8
C25—C28—C29129.5 (2)C43—C42—H42B108.8
C27—C30—C31121.6 (2)H42A—C42—H42B107.7
C27—C30—C35119.4 (2)C42—C43—H43A109.5
C31—C30—C35119.0 (2)C42—C43—H43B109.5
C30—C31—C32122.4 (2)C42—C43—H43C109.5
C31—C32—C33118.1 (2)H43A—C43—H43B109.5
N2—C33—C32130.1 (2)H43A—C43—H43C109.5
N2—C33—C34109.2 (2)H43B—C43—H43C109.5
C7—S1—C8—C91.0 (2)C9—C6—C7—C10175.1 (2)
C7—S1—C8—C11179.0 (2)S1—C8—C9—C62.4 (2)
C8—S1—C7—C60.7 (2)S1—C8—C11—C1225.0 (3)
C8—S1—C7—C10176.9 (2)S1—C8—C11—C16157.19 (19)
C27—S2—C28—C250.17 (19)C9—C8—C11—C12155.0 (2)
C27—S2—C28—C29179.2 (2)C9—C8—C11—C1622.8 (3)
C28—S2—C27—C260.76 (18)C11—C8—C9—C6177.6 (2)
C28—S2—C27—C30179.51 (19)C8—C11—C12—C13178.6 (2)
C14—N1—C17—C181.0 (2)C8—C11—C16—C15178.0 (2)
C14—N1—C17—C22179.7 (2)C12—C11—C16—C150.2 (3)
C17—N1—C14—C13179.4 (2)C16—C11—C12—C130.8 (3)
C17—N1—C14—C150.6 (2)C11—C12—C13—C140.5 (3)
C14—N1—C23—C2488.1 (3)C12—C13—C14—N1179.0 (2)
C23—N1—C14—C131.2 (4)C12—C13—C14—C150.3 (3)
C23—N1—C14—C15177.6 (2)N1—C14—C15—C16179.8 (2)
C17—N1—C23—C2493.9 (2)N1—C14—C15—C180.0 (2)
C23—N1—C17—C18177.2 (2)C13—C14—C15—C160.9 (3)
C23—N1—C17—C222.0 (4)C13—C14—C15—C18178.9 (2)
C33—N2—C36—C370.1 (2)C14—C15—C16—C110.6 (3)
C33—N2—C36—C41179.9 (2)C14—C15—C18—C170.7 (2)
C36—N2—C33—C32179.6 (2)C14—C15—C18—C19178.0 (2)
C36—N2—C33—C340.1 (2)C16—C15—C18—C17179.6 (2)
C33—N2—C42—C4396.1 (2)C16—C15—C18—C191.7 (5)
C42—N2—C33—C320.8 (3)C18—C15—C16—C11179.1 (2)
C42—N2—C33—C34178.9 (2)N1—C17—C18—C151.0 (2)
C36—N2—C42—C4382.5 (3)N1—C17—C18—C19177.9 (2)
C42—N2—C36—C37178.7 (2)N1—C17—C22—C21179.2 (2)
C42—N2—C36—C411.3 (3)C18—C17—C22—C210.1 (2)
C2—C1—C5—C43.9 (2)C22—C17—C18—C15179.6 (2)
C2—C1—C5—C25177.4 (2)C22—C17—C18—C191.5 (3)
C5—C1—C2—F1134.0 (2)C15—C18—C19—C20179.9 (2)
C5—C1—C2—F2106.1 (2)C17—C18—C19—C201.4 (3)
C5—C1—C2—C312.4 (2)C18—C19—C20—C210.1 (3)
C2—C1—C6—C7138.9 (2)C19—C20—C21—C221.7 (4)
C2—C1—C6—C941.0 (3)C20—C21—C22—C171.6 (4)
C6—C1—C2—F148.5 (2)C5—C25—C26—C27178.7 (2)
C6—C1—C2—F271.4 (2)C5—C25—C28—S2177.96 (18)
C6—C1—C2—C3170.05 (19)C5—C25—C28—C291.4 (4)
C5—C1—C6—C738.0 (4)C26—C25—C28—S21.0 (2)
C5—C1—C6—C9142.0 (2)C26—C25—C28—C29178.3 (2)
C6—C1—C5—C4173.3 (2)C28—C25—C26—C271.7 (2)
C6—C1—C5—C255.4 (4)C25—C26—C27—S21.5 (2)
F1—C2—C3—F331.7 (2)C25—C26—C27—C30179.9 (2)
F1—C2—C3—F488.8 (2)S2—C27—C30—C3123.2 (3)
F1—C2—C3—C4147.60 (19)S2—C27—C30—C35157.56 (18)
F2—C2—C3—F3147.18 (18)C26—C27—C30—C31155.3 (2)
F2—C2—C3—F426.7 (2)C26—C27—C30—C3523.9 (3)
F2—C2—C3—C496.9 (2)C27—C30—C31—C32178.7 (2)
C1—C2—C3—F393.1 (2)C27—C30—C35—C34178.6 (2)
C1—C2—C3—F4146.34 (19)C31—C30—C35—C340.7 (3)
C1—C2—C3—C422.7 (2)C35—C30—C31—C320.5 (3)
F3—C3—C4—F532.1 (2)C30—C31—C32—C330.1 (2)
F3—C3—C4—F6148.90 (18)C31—C32—C33—N2179.6 (2)
F3—C3—C4—C590.8 (2)C31—C32—C33—C340.7 (3)
F4—C3—C4—F588.6 (2)N2—C33—C34—C35179.7 (2)
F4—C3—C4—F628.2 (2)N2—C33—C34—C370.3 (2)
F4—C3—C4—C5148.48 (19)C32—C33—C34—C350.5 (3)
C2—C3—C4—F5147.66 (19)C32—C33—C34—C37179.5 (2)
C2—C3—C4—F695.5 (2)C33—C34—C35—C300.1 (2)
C2—C3—C4—C524.8 (2)C33—C34—C37—C360.4 (2)
F5—C4—C5—C1140.05 (19)C33—C34—C37—C38179.2 (2)
F5—C4—C5—C2541.0 (2)C35—C34—C37—C36179.6 (2)
F6—C4—C5—C199.9 (2)C35—C34—C37—C380.8 (4)
F6—C4—C5—C2579.0 (2)C37—C34—C35—C30179.9 (2)
C3—C4—C5—C118.6 (2)N2—C36—C37—C340.3 (2)
C3—C4—C5—C25162.5 (2)N2—C36—C37—C38179.3 (2)
C1—C5—C25—C26135.6 (2)N2—C36—C41—C40179.0 (2)
C1—C5—C25—C2847.8 (3)C37—C36—C41—C401.0 (3)
C4—C5—C25—C2643.1 (3)C41—C36—C37—C34179.7 (2)
C4—C5—C25—C28133.5 (2)C41—C36—C37—C380.7 (3)
C1—C6—C7—S1177.90 (19)C34—C37—C38—C39179.0 (2)
C1—C6—C7—C104.9 (4)C36—C37—C38—C390.2 (3)
C1—C6—C9—C8177.0 (2)C37—C38—C39—C400.2 (3)
C7—C6—C9—C83.0 (3)C38—C39—C40—C410.5 (4)
C9—C6—C7—S12.1 (2)C39—C40—C41—C360.9 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C26—H26···F2i0.952.443.290 (2)149 (1)
Symmetry code: (i) x+1, y+2, z+1.

Experimental details

Crystal data
Chemical formulaC43H32F6N2S2
Mr754.85
Crystal system, space groupMonoclinic, P21/c
Temperature (K)123
a, b, c (Å)14.6687 (7), 17.0977 (8), 14.0017 (7)
β (°) 95.798 (3)
V3)3493.7 (3)
Z4
Radiation typeCu Kα
µ (mm1)1.97
Crystal size (mm)0.34 × 0.18 × 0.11
Data collection
DiffractometerRigaku R-AXIS RAPID
diffractometer
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.687, 0.806
No. of measured, independent and
observed [F2 > 2σ(F2)] reflections
40777, 6393, 5482
Rint0.045
(sin θ/λ)max1)0.602
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.049, 0.139, 1.00
No. of reflections6393
No. of parameters479
No. of restraints?
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.90, 0.50

Computer programs: PROCESS-AUTO (Rigaku, 2006), CrystalStructure (Rigaku/MSC, 2006), SIR92 (Altomare et al., 1993), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C26—H26···F2i0.952.443.290 (2)149.30 (14)
Symmetry code: (i) x+1, y+2, z+1.
 

Acknowledgements

This work was supported by a Grant-in-Aid for Science Research on Priority Area "New Frontiers in Photochromism (No. 471)" and Science Research(C) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan, and was performed under the Cooperative Research Program of "Network Joint Research Center for Materials and Devices".

References

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First citationRigaku/MSC (2006). CrystalStructure. Rigaku/MSC, The Woodlands, Texas, USA.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
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