Download citation
Download citation
link to html
Fluorinated indolyl­fulgides are a class of photochromic organic compounds that meet many of the requirements for use as optical memory media and optical switches. The X-ray crystal structures of a series of five photochromic fluorinated indolyl­fulgides have been determined, namely (3Z)-3-[1-(1,2-di­methyl-1H-indol-3-yl)-2,2,2-tri­fluoro­ethyl­idene]-4-(1-methyl­ethyl­idene)­dihydrofuran-2,5-dione (tri­fluoro­methyl­iso­propyl­idene­indolyl­fulgide), C19H16F3NO3, (I), (3Z)-3-[1-(1,2-dimethyl-1H-indol-3-yl)-2,2,3,3,3-penta­fluoro­propyl­idene]-4-(1-methyl­ethyl­idene)­dihydrofuran-2,5-dione (penta­fluoro­ethyl­iso­propyl­idene­indolyl­fulgide), C20H16F5NO3, (II), (3Z)-3-[1-(1,2-di­methyl-1H-indol-3-yl)-2,2,3,3,4,4,4-hepta­fluoro­butyl­idene]-4-(1-methyl­ethyl­idene)­dihydrofuran-2,5-dione (hepta­fluoro­propyl­iso­propyl­idene­indolyl­fulgide), C21H16F7NO3, (III), (3Z)-3-[1-(1,2-di­methyl-1H-indol-3-yl)-2,2,2-tri­fluoro­ethyl­idene]-4-(tri­cyclo­[3.3.1.13,7]­decyl­idene­)dihydrofuran-2,5-dione (tri­fluoro­methyl­adamantyl­idene­indolyl­fulgide), C26H24F3NO3, (IV), and (3Z)-3-[1-(1,2-di­methyl-1H-indol-3-yl)-2,2,3,3,4,4,4-hepta­fluoro­butyl­idene]-4-(tri­cyclo­[3.3.1.13,7]­decyl­idene­)dihydrofuran-2,5-dione (hepta­fluoro­propyl­adamantylidenein­dolyl­fulgide), C28H24F7NO3, (V). The photochromic property of fulgides is based on the photochemically allowed electrocyclic ring closure of a hexatriene system to form a cyclo­hexa­diene. For each fulgide examined, the bond lengths within the hexatriene system alternate between short and long, as expected. Comparing the structures of the five fulgides with each other demonstrates no significant difference in bond lengths, bond angles or dihedral angles within the hexatriene systems. The distance between the bond-forming C atoms at each end of the hexatriene system does vary. Correlations of structural properties with optical properties are addressed.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270102008041/bk1655sup1.cif
Contains datablocks global, I, II, III, IV, V

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102008041/bk1655Isup2.hkl
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102008041/bk1655IIsup3.hkl
Contains datablock II

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102008041/bk1655IIIsup4.hkl
Contains datablock III

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102008041/bk1655IVsup5.hkl
Contains datablock IV

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270102008041/bk1655Vsup6.hkl
Contains datablock V

CCDC references: 192971; 192972; 192973; 192974; 192975

Comment top

Fulgides are an important class of organic photochromic compounds that undergo reversible color changes upon wavelength-specific illumination (Crano et al., 1999; Durr & Bousas-Laurent, 1990). Widely used in specialty inks and dyes, they are of particular interest for incorporation in high-density optical memory devices (Yokoyama, 2000). In such devices, binary information is encoded using two differently colored forms which are interconverted by the photochemical transformations of coloration (ring closure of the cyclizable form) and bleaching (ring opening of the C form); this is illustrated in the reaction Scheme below for commercially available Aberchrome 540 (Heller, 1986). There are many stringent requirements for photochromic materials intended for use as optical memory, including readily distinguishable absorption spectra for the separate colored forms, efficient photoreactions, high extinction coefficients, and both thermal and photochemical stability. \sch

Recently discovered fluorinated isopropylidene indolylfulgides are promising candidates for optical memory that feature greatly enhanced photochemical fatigue resistance in comparison with other members of the fulgide family (Wolak et al., 2001; Yokoyama & Takahashi, 1996). Additionally, they possess improved coloration quantum yields in solution relative to their non-fluorinated analogs. They are further characterized by a considerable bathochromic shift in absorption maxima for the cyclizable Z form. Adamantylidene-substituted fluorinated indolylfulgides possess many of the favorable properties of isopropylidene indolylfulgides, in addition to greater thermal stability for the cyclizable form (Wolak et al., 2002).

To aid in the preparation of further improved photochromic materials, we sought to identify relationships between crystal structure and optical properties. Herein, we examine in detail the structural attributes of a series of five cyclizable-form fluorinated indolylfulgides containing either isopropylidene or adamantylidene substitution, the title compounds, (I)-(V). Bond lengths, bond and dihedral angles, and distances between bond-forming C atoms are presented for each compound. Furthermore, we compare our findings with the reported photochemical yields for the coloration event, the optical property most likely to be associated with the structure of the cyclizable form (Wolak et al., 2001, 2002).

The structures of compounds (I)-(V) are depicted in Fig. 3. When fulgides are transformed from the cyclizable form to the cyclic form with light, the hexatriene system is converted to a cyclohexadiene system (see reaction Scheme above). Because the photochromic nature of fulgides is intimately associated with the hexatriene system (see Scheme below), we sought to examine how substituents altered the structure of the system, and to investigate whether structural trends were predictive of optical properties. The bond lengths, and bond and dihedral angles for the hexatriene systems of the five indolylfulgides are shown in Table 1.

As expected, within the hexatriene system of the cyclizable form,the bond lengths alternate between short and long, corresponding to alternating double and single bonds. For a given bond, the bond lengths amongst the five compounds varied by no more than 0.02 Å. The minimal variations fall within the expected experimental error owing to molecular motion and the use of spherical scattering factors for small-molecule carbon structures (Dunitz, 1999; Seiler et al., 1984). Thus, although bond lengths appear to vary with the substitution pattern around the hexatriene system, it is difficult to say with certainty that observable trends exist. Similarly, the range of values for a given bond or dihedral angle corresponds approximately to the experimental error limits. Within the hexatriene system, the dihedral angles are observed to alternate between close to 0° and close to -50°. Bonds with dihedral angles of close to 0° correspond to double bonds, and those with values in the vicinity of -50° correspond to single bonds.

Previous reports have suggested that the dihedral angle of the efgh bond or the distance between atoms b and g in the cyclizable form might be correlated with the quantum yield of coloration (Ilge & Colditz, 1990; Yokoyama et al., 1996). The quantum yield of coloration, Φcoloration, is a measure of the efficiency of the photoreaction that forms a new bond between atoms b and g. One might imagine that the spatial proximity of atoms b and g in the cyclizable form would be a determining factor in the efficiency of the photocyclization reaction.

The distance between atoms b and g is always greater for the adamantylidene derivatives than for the corresponding isopropylidene derivatives (Table 2). Within the isopropylidene series, the b-g distance decreased when the fluorinated substituent was changed from CF3 in (I) to C3F7 in (III). In contrast, the data suggest that the opposite trend exists for the adamantylidene series. In Table 2, the b-g distances are compared with the quantum yields measured in toluene at 427 nm. The quantum yields of the isopropylidene derivatives were greater than those of the adamantylidene derivatives and the b-g distances were smaller, as expected. Within the isopropylidene serie,the quantum yields remained relatively constant while the b-g distance decreased, thus suggesting that other factors may be important.

Experimental top

The five title compounds were synthesized as previously reported by Thomas et al. (2001). The isopropylidene fulgides, (I)-(III), were recrystallized from propan-2-ol. The adamantylidene fulgides, (IV) and (V), were recrystallized from toluene-ligroin.

Refinement top

H atoms were placed in geometric positions and refined as riding, with C—H = 0.93–0.98 Å and Uiso(H) = 1.2Ueq(C). Are these the correct contsraints? The largest peak in the final difference map of structure (III) is located 1.3 Å from atom H9A, 1.4 Å from atom H9C and 1.6 Å from atom H7A.

Computing details top

For all compounds, data collection: Please provide missing details; cell refinement: Please provide missing details; data reduction: Please provide missing details; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: Please provide missing details.

Figures top
[Figure 1] Fig. 1. Views of the molecules of fulgides (I)-(V). Displacement ellipsoids are drawn at the 50% probability level and H atoms have been omitted for clarity. The unit cell for (I) contains two rotamers, (I) and (Ia). Only rotamer (I), which is homologous to structures (II)-(V), is considered here.
(I) (3Z)-3-[1-(1,2-dimethyl-1H-indol-3-yl)-2,2,2- trifluoroethylidene]-4-(1-methylethylidene)dihydrofuran-2,5-dione top
Crystal data top
C19H16F3NO3F(000) = 1504
Mr = 363.33Dx = 1.412 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 11.660 (1) ÅCell parameters from 6045 reflections
b = 17.164 (2) Åθ = 1.7–25.1°
c = 17.102 (2) ŵ = 0.12 mm1
β = 92.75 (2)°T = 90 K
V = 3418.9 (6) Å3Plate, yellow
Z = 80.25 × 0.16 × 0.04 mm
Data collection top
Bruker P4 with CCD area-detector
diffractometer
6045 independent reflections
Radiation source: fine-focus sealed tube2878 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.065
Detector resolution: 512 x 512 pixels mm-1θmax = 25.1°, θmin = 1.7°
ϕ and ω scansh = 1313
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 2019
Tmin = 0.971, Tmax = 0.995l = 2018
17999 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.051Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.160H-atom parameters constrained
S = 0.99 w = 1/[σ2(Fo2) + (0.0666P)2 + 0.6437P]
where P = (Fo2 + 2Fc2)/3
6045 reflections(Δ/σ)max = 0.009
477 parametersΔρmax = 0.18 e Å3
0 restraintsΔρmin = 0.17 e Å3
Crystal data top
C19H16F3NO3V = 3418.9 (6) Å3
Mr = 363.33Z = 8
Monoclinic, P21/nMo Kα radiation
a = 11.660 (1) ŵ = 0.12 mm1
b = 17.164 (2) ÅT = 90 K
c = 17.102 (2) Å0.25 × 0.16 × 0.04 mm
β = 92.75 (2)°
Data collection top
Bruker P4 with CCD area-detector
diffractometer
6045 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2878 reflections with I > 2σ(I)
Tmin = 0.971, Tmax = 0.995Rint = 0.065
17999 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0510 restraints
wR(F2) = 0.160H-atom parameters constrained
S = 0.99Δρmax = 0.18 e Å3
6045 reflectionsΔρmin = 0.17 e Å3
477 parameters
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 of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.22613 (19)1.09785 (11)0.43470 (14)0.0904 (7)
F20.0949 (2)1.10349 (12)0.34558 (14)0.0960 (7)
F30.0573 (2)1.06714 (13)0.46133 (14)0.1015 (8)
F40.2333 (2)1.12479 (12)0.94786 (14)0.0924 (7)
F50.1038 (2)1.14106 (11)0.85706 (13)0.0938 (7)
F60.05982 (19)1.10020 (12)0.97093 (12)0.0841 (7)
O10.0978 (3)1.0120 (3)0.3540 (2)0.1347 (15)
O20.1001 (2)1.05884 (18)0.86356 (16)0.0973 (9)
O30.13110 (19)0.93079 (19)0.86106 (14)0.0787 (8)
O40.1153 (2)0.80151 (19)0.85582 (17)0.1003 (10)
O50.1091 (3)0.8839 (3)0.3340 (2)0.1192 (13)
O60.0736 (3)0.7585 (2)0.3072 (2)0.1595 (18)
C10.3814 (2)0.98033 (17)0.38844 (18)0.0450 (8)
C20.4146 (3)1.04229 (19)0.34213 (19)0.0565 (9)
H20.35991.07400.31670.068*
C30.5292 (3)1.0558 (2)0.3346 (2)0.0738 (11)
H30.55221.09790.30490.089*
C40.6120 (3)1.0077 (3)0.3707 (2)0.0779 (11)
H40.68921.01850.36480.094*
C50.5824 (3)0.9452 (2)0.4143 (2)0.0679 (10)
H50.63790.91270.43770.082*
C60.4666 (3)0.93187 (19)0.42256 (18)0.0514 (8)
C70.4723 (3)0.8113 (2)0.5064 (2)0.0838 (12)
H7A0.49830.77240.47100.126*
H7B0.42110.78790.54190.126*
H7C0.53710.83310.53540.126*
C80.2951 (3)0.88273 (18)0.45241 (18)0.0516 (8)
C90.2144 (3)0.8295 (2)0.4912 (2)0.0752 (11)
H9A0.13890.85210.48900.113*
H9B0.24000.82200.54480.113*
H9C0.21210.78020.46460.113*
C100.2727 (2)0.94845 (17)0.40768 (17)0.0455 (8)
C110.1586 (3)0.97712 (18)0.38420 (18)0.0503 (8)
C120.0760 (3)0.9320 (2)0.3490 (2)0.0589 (9)
C130.0489 (4)0.9515 (3)0.3463 (3)0.0898 (14)
C140.0360 (5)0.8222 (4)0.3193 (3)0.1089 (18)
C150.0827 (3)0.8532 (2)0.3167 (2)0.0716 (11)
C160.1642 (4)0.8194 (2)0.2740 (2)0.0768 (12)
C170.2717 (3)0.8586 (2)0.2544 (2)0.0763 (11)
H17A0.26090.91400.25580.114*
H17B0.29220.84320.20300.114*
H17C0.33200.84420.29180.114*
C180.1493 (5)0.7382 (2)0.2398 (3)0.129 (2)
H18A0.10280.70750.27290.193*
H18B0.22320.71410.23640.193*
H18C0.11260.74170.18840.193*
C190.1329 (3)1.0612 (2)0.4066 (2)0.0639 (10)
C200.2987 (3)0.90792 (17)0.94785 (17)0.0469 (8)
C210.2374 (3)0.85341 (18)0.98906 (18)0.0557 (9)
H240.15830.85810.99210.067*
C220.2952 (3)0.7924 (2)1.0253 (2)0.0735 (11)
H230.25450.75521.05220.088*
C230.4140 (4)0.7856 (2)1.0222 (2)0.0781 (11)
H220.45090.74391.04740.094*
C240.4770 (3)0.8380 (2)0.9837 (2)0.0669 (10)
H210.55640.83340.98250.080*
C250.4184 (3)0.89923 (19)0.94566 (18)0.0508 (8)
C260.5810 (3)0.9712 (2)0.8870 (2)0.0758 (11)
H28A0.60000.93850.84400.114*
H28B0.62780.95730.93260.114*
H28C0.59461.02470.87390.114*
C270.3709 (3)1.00808 (18)0.87842 (18)0.0526 (8)
C280.3908 (3)1.0760 (2)0.8268 (2)0.0727 (11)
H27A0.42661.11720.85710.109*
H27B0.31871.09390.80410.109*
H27C0.43981.06080.78600.109*
C290.2697 (3)0.97747 (16)0.90483 (17)0.0464 (8)
C300.1540 (3)1.00961 (18)0.88983 (18)0.0499 (8)
C310.0610 (3)0.96745 (18)0.86320 (17)0.0502 (8)
C320.0601 (3)0.9951 (3)0.8630 (2)0.0669 (10)
C330.0672 (3)0.8631 (3)0.8529 (2)0.0682 (10)
C340.0518 (3)0.88525 (19)0.83957 (18)0.0513 (8)
C350.1218 (3)0.84008 (19)0.79878 (19)0.0578 (9)
C360.2275 (3)0.8695 (2)0.76425 (19)0.0654 (10)
H34A0.22470.92530.76150.098*
H34B0.23300.84850.71250.098*
H34C0.29330.85370.79630.098*
C370.0954 (4)0.7560 (2)0.7798 (3)0.0998 (14)
H35A0.03470.73820.81130.150*
H35B0.16280.72500.79060.150*
H35C0.07190.75140.72550.150*
C380.1379 (3)1.0939 (2)0.9157 (2)0.0659 (10)
N10.4118 (2)0.87325 (15)0.46166 (16)0.0567 (7)
N20.4605 (2)0.96075 (16)0.90300 (15)0.0555 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0758 (15)0.0578 (13)0.136 (2)0.0155 (11)0.0108 (14)0.0230 (12)
F20.1108 (18)0.0761 (15)0.0998 (17)0.0305 (13)0.0076 (14)0.0283 (13)
F30.1003 (18)0.0990 (18)0.1089 (18)0.0332 (14)0.0424 (15)0.0058 (14)
F40.0962 (17)0.0581 (13)0.120 (2)0.0052 (12)0.0189 (14)0.0310 (12)
F50.138 (2)0.0572 (13)0.0843 (16)0.0290 (13)0.0105 (14)0.0141 (12)
F60.0951 (16)0.0847 (15)0.0721 (14)0.0306 (12)0.0013 (13)0.0186 (11)
O10.0510 (19)0.166 (4)0.186 (4)0.025 (2)0.009 (2)0.039 (3)
O20.0806 (19)0.110 (2)0.099 (2)0.0499 (18)0.0162 (16)0.0040 (17)
O30.0427 (14)0.117 (2)0.0751 (18)0.0028 (16)0.0063 (12)0.0012 (15)
O40.0766 (19)0.111 (2)0.112 (2)0.0411 (18)0.0047 (17)0.0013 (18)
O50.062 (2)0.176 (4)0.117 (3)0.049 (2)0.0237 (18)0.041 (3)
O60.166 (3)0.158 (3)0.149 (3)0.119 (3)0.052 (3)0.043 (3)
C10.0416 (19)0.0429 (19)0.0499 (19)0.0039 (15)0.0059 (15)0.0077 (15)
C20.044 (2)0.058 (2)0.067 (2)0.0031 (16)0.0006 (17)0.0023 (18)
C30.064 (3)0.076 (3)0.083 (3)0.014 (2)0.013 (2)0.007 (2)
C40.045 (2)0.103 (3)0.085 (3)0.008 (2)0.001 (2)0.022 (3)
C50.051 (2)0.082 (3)0.070 (3)0.016 (2)0.0115 (19)0.019 (2)
C60.042 (2)0.057 (2)0.054 (2)0.0092 (17)0.0093 (16)0.0132 (17)
C70.098 (3)0.066 (3)0.084 (3)0.032 (2)0.032 (2)0.000 (2)
C80.054 (2)0.047 (2)0.053 (2)0.0023 (16)0.0082 (16)0.0019 (16)
C90.082 (3)0.068 (2)0.074 (3)0.009 (2)0.007 (2)0.0196 (19)
C100.0393 (18)0.0438 (19)0.052 (2)0.0015 (14)0.0086 (15)0.0007 (15)
C110.0396 (19)0.056 (2)0.055 (2)0.0030 (16)0.0025 (16)0.0100 (16)
C120.039 (2)0.072 (3)0.065 (2)0.0050 (17)0.0090 (17)0.0223 (19)
C130.052 (3)0.122 (4)0.093 (3)0.010 (3)0.011 (2)0.039 (3)
C140.107 (4)0.127 (5)0.089 (4)0.067 (4)0.037 (3)0.044 (3)
C150.071 (3)0.073 (3)0.068 (3)0.028 (2)0.029 (2)0.020 (2)
C160.098 (3)0.053 (2)0.075 (3)0.012 (2)0.040 (3)0.004 (2)
C170.076 (3)0.079 (3)0.072 (3)0.011 (2)0.022 (2)0.020 (2)
C180.179 (5)0.072 (3)0.130 (4)0.012 (3)0.061 (4)0.022 (3)
C190.049 (2)0.068 (3)0.075 (3)0.0167 (19)0.004 (2)0.008 (2)
C200.052 (2)0.0437 (19)0.0443 (19)0.0009 (15)0.0061 (16)0.0031 (15)
C210.053 (2)0.057 (2)0.057 (2)0.0021 (17)0.0065 (17)0.0010 (17)
C220.080 (3)0.059 (2)0.080 (3)0.000 (2)0.005 (2)0.013 (2)
C230.084 (3)0.063 (3)0.085 (3)0.016 (2)0.019 (2)0.011 (2)
C240.051 (2)0.072 (3)0.076 (3)0.015 (2)0.018 (2)0.008 (2)
C250.046 (2)0.053 (2)0.053 (2)0.0071 (16)0.0083 (16)0.0092 (17)
C260.049 (2)0.101 (3)0.076 (3)0.012 (2)0.0008 (19)0.017 (2)
C270.054 (2)0.050 (2)0.052 (2)0.0038 (17)0.0055 (17)0.0072 (16)
C280.086 (3)0.064 (2)0.068 (3)0.017 (2)0.001 (2)0.0008 (19)
C290.050 (2)0.0418 (19)0.0469 (19)0.0003 (15)0.0073 (16)0.0039 (14)
C300.053 (2)0.047 (2)0.049 (2)0.0097 (16)0.0033 (16)0.0016 (15)
C310.047 (2)0.059 (2)0.0438 (19)0.0133 (17)0.0054 (16)0.0071 (16)
C320.060 (3)0.089 (3)0.051 (2)0.020 (2)0.0099 (18)0.003 (2)
C330.058 (2)0.087 (3)0.059 (2)0.010 (2)0.0066 (19)0.000 (2)
C340.047 (2)0.056 (2)0.050 (2)0.0032 (16)0.0110 (16)0.0004 (16)
C350.057 (2)0.055 (2)0.059 (2)0.0012 (17)0.0165 (19)0.0032 (17)
C360.064 (2)0.074 (2)0.058 (2)0.0101 (19)0.0030 (18)0.0150 (18)
C370.108 (3)0.062 (3)0.128 (4)0.010 (2)0.006 (3)0.031 (2)
C380.073 (3)0.058 (2)0.066 (3)0.016 (2)0.007 (2)0.001 (2)
N10.0581 (18)0.0470 (16)0.0629 (19)0.0138 (14)0.0186 (14)0.0020 (14)
N20.0435 (16)0.0604 (18)0.0623 (18)0.0061 (14)0.0008 (14)0.0080 (14)
Geometric parameters (Å, º) top
F1—C191.326 (4)C16—C181.517 (5)
F2—C191.331 (4)C17—H17A0.9600
F3—C191.319 (4)C17—H17B0.9600
F4—C381.327 (4)C17—H17C0.9600
F5—C381.336 (4)C18—H18A0.9600
F6—C381.347 (4)C18—H18B0.9600
O1—C131.195 (5)C18—H18C0.9600
O2—C321.190 (4)C20—C211.390 (4)
O3—C321.379 (4)C20—C251.405 (4)
O3—C331.391 (4)C20—C291.434 (4)
O4—C331.199 (4)C21—C221.377 (4)
O5—C131.366 (5)C21—H240.9300
O5—C141.390 (6)C22—C231.393 (5)
O6—C141.193 (5)C22—H230.9300
C1—C21.392 (4)C23—C241.353 (5)
C1—C61.401 (4)C23—H220.9300
C1—C101.433 (4)C24—C251.398 (4)
C2—C31.368 (4)C24—H210.9300
C2—H20.9300C25—N21.387 (4)
C3—C41.392 (5)C26—N21.455 (4)
C3—H30.9300C26—H28A0.9600
C4—C51.360 (5)C26—H28B0.9600
C4—H40.9300C26—H28C0.9600
C5—C61.383 (4)C27—N21.373 (4)
C5—H50.9300C27—C291.387 (4)
C6—N11.382 (4)C27—C281.487 (4)
C7—N11.471 (4)C28—H27A0.9600
C7—H7A0.9600C28—H27B0.9600
C7—H7B0.9600C28—H27C0.9600
C7—H7C0.9600C29—C301.469 (4)
C8—N11.372 (4)C30—C311.364 (4)
C8—C101.381 (4)C30—C381.526 (5)
C8—C91.490 (4)C31—C341.470 (4)
C9—H9A0.9600C31—C321.489 (5)
C9—H9B0.9600C33—C341.468 (5)
C9—H9C0.9600C34—C351.345 (4)
C10—C111.457 (4)C35—C361.480 (5)
C11—C121.354 (4)C35—C371.507 (5)
C11—C191.526 (5)C36—H34A0.9600
C12—C151.465 (5)C36—H34B0.9600
C12—C131.493 (5)C36—H34C0.9600
C14—C151.484 (6)C37—H35A0.9600
C15—C161.357 (5)C37—H35B0.9600
C16—C171.476 (5)C37—H35C0.9600
C32—O3—C33110.3 (3)C25—C20—C29106.6 (3)
C13—O5—C14111.1 (4)C22—C21—C20119.2 (3)
C2—C1—C6118.7 (3)C22—C21—H24120.4
C2—C1—C10134.1 (3)C20—C21—H24120.4
C6—C1—C10107.2 (3)C21—C22—C23120.8 (4)
C3—C2—C1118.8 (3)C21—C22—H23119.6
C3—C2—H2120.6C23—C22—H23119.6
C1—C2—H2120.6C24—C23—C22121.9 (3)
C2—C3—C4121.2 (4)C24—C23—H22119.1
C2—C3—H3119.4C22—C23—H22119.1
C4—C3—H3119.4C23—C24—C25117.4 (3)
C5—C4—C3121.5 (3)C23—C24—H21121.3
C5—C4—H4119.2C25—C24—H21121.3
C3—C4—H4119.2N2—C25—C24129.8 (3)
C4—C5—C6117.4 (3)N2—C25—C20108.1 (3)
C4—C5—H5121.3C24—C25—C20122.1 (3)
C6—C5—H5121.3N2—C26—H28A109.5
N1—C6—C5130.3 (3)N2—C26—H28B109.5
N1—C6—C1107.3 (3)H28A—C26—H28B109.5
C5—C6—C1122.4 (3)N2—C26—H28C109.5
N1—C7—H7A109.5H28A—C26—H28C109.5
N1—C7—H7B109.5H28B—C26—H28C109.5
H7A—C7—H7B109.5N2—C27—C29108.8 (3)
N1—C7—H7C109.5N2—C27—C28120.5 (3)
H7A—C7—H7C109.5C29—C27—C28130.5 (3)
H7B—C7—H7C109.5C27—C28—H27A109.5
N1—C8—C10108.7 (3)C27—C28—H27B109.5
N1—C8—C9121.3 (3)H27A—C28—H27B109.5
C10—C8—C9129.9 (3)C27—C28—H27C109.5
C8—C9—H9A109.5H27A—C28—H27C109.5
C8—C9—H9B109.5H27B—C28—H27C109.5
H9A—C9—H9B109.5C27—C29—C20107.4 (3)
C8—C9—H9C109.5C27—C29—C30126.1 (3)
H9A—C9—H9C109.5C20—C29—C30126.5 (3)
H9B—C9—H9C109.5C31—C30—C29124.6 (3)
C8—C10—C1107.1 (3)C31—C30—C38119.5 (3)
C8—C10—C11125.0 (3)C29—C30—C38115.4 (3)
C1—C10—C11127.9 (3)C30—C31—C34130.3 (3)
C12—C11—C10123.4 (3)C30—C31—C32124.8 (3)
C12—C11—C19120.6 (3)C34—C31—C32104.4 (3)
C10—C11—C19115.9 (3)O2—C32—O3120.0 (3)
C11—C12—C15130.2 (3)O2—C32—C31131.7 (4)
C11—C12—C13123.9 (4)O3—C32—C31108.3 (3)
C15—C12—C13105.4 (3)O4—C33—O3118.6 (4)
O1—C13—O5120.7 (4)O4—C33—C34133.0 (4)
O1—C13—C12131.4 (5)O3—C33—C34108.3 (3)
O5—C13—C12107.9 (4)C35—C34—C33122.2 (3)
O6—C14—O5120.4 (5)C35—C34—C31131.2 (3)
O6—C14—C15131.2 (7)C33—C34—C31105.2 (3)
O5—C14—C15108.3 (4)C34—C35—C36123.2 (3)
C16—C15—C12130.5 (3)C34—C35—C37122.7 (3)
C16—C15—C14122.7 (4)C36—C35—C37113.9 (3)
C12—C15—C14104.6 (4)C35—C36—H34A109.5
C15—C16—C17123.5 (3)C35—C36—H34B109.5
C15—C16—C18122.0 (4)H34A—C36—H34B109.5
C17—C16—C18114.5 (4)C35—C36—H34C109.5
C16—C17—H17A109.5H34A—C36—H34C109.5
C16—C17—H17B109.5H34B—C36—H34C109.5
H17A—C17—H17B109.5C35—C37—H35A109.5
C16—C17—H17C109.5C35—C37—H35B109.5
H17A—C17—H17C109.5H35A—C37—H35B109.5
H17B—C17—H17C109.5C35—C37—H35C109.5
C16—C18—H18A109.5H35A—C37—H35C109.5
C16—C18—H18B109.5H35B—C37—H35C109.5
H18A—C18—H18B109.5F4—C38—F5106.4 (3)
C16—C18—H18C109.5F4—C38—F6105.0 (3)
H18A—C18—H18C109.5F5—C38—F6106.9 (3)
H18B—C18—H18C109.5F4—C38—C30112.8 (3)
F3—C19—F1105.7 (3)F5—C38—C30113.1 (3)
F3—C19—F2107.8 (3)F6—C38—C30112.1 (3)
F1—C19—F2105.2 (3)C8—N1—C6109.7 (2)
F3—C19—C11113.4 (3)C8—N1—C7126.5 (3)
F1—C19—C11111.9 (3)C6—N1—C7123.8 (3)
F2—C19—C11112.4 (3)C27—N2—C25109.2 (3)
C21—C20—C25118.5 (3)C27—N2—C26126.6 (3)
C21—C20—C29134.9 (3)C25—N2—C26124.2 (3)
C6—C1—C2—C33.0 (5)C29—C20—C25—N20.1 (3)
C10—C1—C2—C3178.2 (3)C21—C20—C25—C240.2 (5)
C1—C2—C3—C41.6 (5)C29—C20—C25—C24178.4 (3)
C2—C3—C4—C50.4 (6)N2—C27—C29—C200.1 (3)
C3—C4—C5—C61.0 (5)C28—C27—C29—C20175.4 (3)
C4—C5—C6—N1178.8 (3)N2—C27—C29—C30178.7 (3)
C4—C5—C6—C10.5 (5)C28—C27—C29—C303.4 (5)
C2—C1—C6—N1176.9 (3)C21—C20—C29—C27178.4 (3)
C10—C1—C6—N10.5 (3)C25—C20—C29—C270.0 (3)
C2—C1—C6—C52.5 (5)C21—C20—C29—C302.9 (6)
C10—C1—C6—C5178.9 (3)C25—C20—C29—C30178.8 (3)
N1—C8—C10—C10.3 (3)C27—C29—C30—C31130.6 (3)
C9—C8—C10—C1176.7 (3)C20—C29—C30—C3147.9 (5)
N1—C8—C10—C11179.0 (3)C27—C29—C30—C3856.8 (4)
C9—C8—C10—C114.5 (5)C20—C29—C30—C38124.7 (3)
C2—C1—C10—C8175.7 (3)C29—C30—C31—C343.6 (5)
C6—C1—C10—C80.2 (3)C38—C30—C31—C34175.9 (3)
C2—C1—C10—C113.0 (6)C29—C30—C31—C32167.0 (3)
C6—C1—C10—C11178.5 (3)C38—C30—C31—C325.3 (5)
C8—C10—C11—C1251.5 (5)C33—O3—C32—O2174.1 (3)
C1—C10—C11—C12127.0 (3)C33—O3—C32—C315.2 (4)
C8—C10—C11—C19124.4 (3)C30—C31—C32—O223.2 (6)
C1—C10—C11—C1957.1 (4)C34—C31—C32—O2164.2 (4)
C10—C11—C12—C159.9 (6)C30—C31—C32—O3157.6 (3)
C19—C11—C12—C15174.4 (3)C34—C31—C32—O315.0 (3)
C10—C11—C12—C13160.7 (3)C32—O3—C33—O4174.8 (3)
C19—C11—C12—C1315.0 (5)C32—O3—C33—C346.9 (4)
C14—O5—C13—O1174.3 (4)O4—C33—C34—C3526.3 (6)
C14—O5—C13—C126.8 (5)O3—C33—C34—C35151.7 (3)
C11—C12—C13—O120.9 (7)O4—C33—C34—C31165.8 (4)
C15—C12—C13—O1166.5 (5)O3—C33—C34—C3116.2 (3)
C11—C12—C13—O5157.8 (3)C30—C31—C34—C3540.1 (6)
C15—C12—C13—O514.8 (4)C32—C31—C34—C35147.9 (4)
C13—O5—C14—O6179.9 (4)C30—C31—C34—C33153.5 (3)
C13—O5—C14—C153.9 (5)C32—C31—C34—C3318.5 (3)
C11—C12—C15—C1641.1 (6)C33—C34—C35—C36161.2 (3)
C13—C12—C15—C16147.0 (4)C31—C34—C35—C363.3 (6)
C11—C12—C15—C14155.5 (4)C33—C34—C35—C3714.8 (5)
C13—C12—C15—C1416.4 (4)C31—C34—C35—C37179.3 (3)
O6—C14—C15—C1623.6 (7)C31—C30—C38—F4173.3 (3)
O5—C14—C15—C16152.1 (4)C29—C30—C38—F40.3 (4)
O6—C14—C15—C12171.4 (5)C31—C30—C38—F565.9 (4)
O5—C14—C15—C1213.0 (4)C29—C30—C38—F5121.1 (3)
C12—C15—C16—C173.2 (6)C31—C30—C38—F655.0 (4)
C14—C15—C16—C17164.0 (4)C29—C30—C38—F6118.0 (3)
C12—C15—C16—C18174.4 (4)C10—C8—N1—C60.6 (3)
C14—C15—C16—C1813.5 (6)C9—C8—N1—C6177.5 (3)
C12—C11—C19—F365.5 (4)C10—C8—N1—C7178.9 (3)
C10—C11—C19—F3110.5 (3)C9—C8—N1—C72.1 (5)
C12—C11—C19—F1175.0 (3)C5—C6—N1—C8178.6 (3)
C10—C11—C19—F18.9 (4)C1—C6—N1—C80.7 (3)
C12—C11—C19—F257.0 (4)C5—C6—N1—C71.8 (5)
C10—C11—C19—F2126.9 (3)C1—C6—N1—C7178.8 (3)
C25—C20—C21—C220.9 (5)C29—C27—N2—C250.1 (3)
C29—C20—C21—C22179.1 (3)C28—C27—N2—C25176.0 (3)
C20—C21—C22—C231.1 (5)C29—C27—N2—C26179.1 (3)
C21—C22—C23—C240.2 (6)C28—C27—N2—C263.2 (5)
C22—C23—C24—C250.9 (6)C24—C25—N2—C27178.2 (3)
C23—C24—C25—N2179.3 (3)C20—C25—N2—C270.2 (3)
C23—C24—C25—C201.1 (5)C24—C25—N2—C262.5 (5)
C21—C20—C25—N2178.8 (3)C20—C25—N2—C26179.1 (3)
(II) (3Z)-3-[1-(1,2-dimethyl-1H-indol-3-yl)-2,2,3,3,3- pentafluoropropylidene]-4-(1-methylethylidene)dihydrofuran-2,5-dione top
Crystal data top
C20H16F5NO3F(000) = 848
Mr = 413.34Dx = 1.471 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 9.539 (1) ÅCell parameters from 3291 reflections
b = 16.716 (1) Åθ = 2.1–25.0°
c = 11.720 (1) ŵ = 0.13 mm1
β = 92.90 (1)°T = 90 K
V = 1866.6 (3) Å3Plate, yellow
Z = 40.24 × 0.16 × 0.12 mm
Data collection top
Bruker P4 with CCD area-detector
diffractometer
3291 independent reflections
Radiation source: fine-focus sealed tube1625 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.053
Detector resolution: 512 x 512 pixels mm-1θmax = 25.0°, θmin = 2.1°
ϕ and ω scansh = 1111
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 1519
Tmin = 0.970, Tmax = 0.982l = 1213
10009 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.057H-atom parameters constrained
wR(F2) = 0.181 w = 1/[σ2(Fo2) + (0.0903P)2 + 0.1488P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.002
3291 reflectionsΔρmax = 0.24 e Å3
267 parametersΔρmin = 0.19 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.011 (2)
Crystal data top
C20H16F5NO3V = 1866.6 (3) Å3
Mr = 413.34Z = 4
Monoclinic, P21/cMo Kα radiation
a = 9.539 (1) ŵ = 0.13 mm1
b = 16.716 (1) ÅT = 90 K
c = 11.720 (1) Å0.24 × 0.16 × 0.12 mm
β = 92.90 (1)°
Data collection top
Bruker P4 with CCD area-detector
diffractometer
3291 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1625 reflections with I > 2σ(I)
Tmin = 0.970, Tmax = 0.982Rint = 0.053
10009 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0570 restraints
wR(F2) = 0.181H-atom parameters constrained
S = 1.01Δρmax = 0.24 e Å3
3291 reflectionsΔρmin = 0.19 e Å3
267 parameters
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 of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.1019 (3)1.11780 (13)0.76904 (17)0.0865 (8)
F20.0741 (2)1.09325 (14)0.94562 (17)0.0794 (7)
F30.4088 (3)1.11339 (19)0.9155 (3)0.1466 (15)
F40.2623 (3)1.19415 (19)0.9822 (3)0.1334 (12)
F50.3052 (4)1.1986 (2)0.8093 (3)0.1545 (14)
O10.2639 (4)1.0424 (2)1.1005 (2)0.1088 (12)
O20.2524 (3)0.9091 (2)1.1214 (2)0.0840 (9)
O30.2561 (4)0.7769 (2)1.0951 (3)0.1043 (11)
C10.2339 (3)0.9997 (2)0.6232 (2)0.0489 (9)
C20.3333 (4)1.0571 (2)0.5971 (3)0.0630 (10)
H20.37891.08730.65440.076*
C30.3620 (4)1.0677 (3)0.4850 (3)0.0775 (12)
H30.42801.10580.46610.093*
C40.2938 (5)1.0220 (3)0.3972 (3)0.0763 (13)
H40.31391.03170.32170.092*
C50.2010 (4)0.9653 (2)0.4206 (3)0.0635 (10)
H50.15730.93480.36280.076*
C60.1718 (4)0.9533 (2)0.5346 (3)0.0509 (9)
C70.0035 (4)0.8401 (2)0.5183 (3)0.0738 (12)
H7A0.04730.80490.57060.111*
H7B0.05350.80940.46920.111*
H7C0.07440.86810.47310.111*
C80.0894 (4)0.9077 (2)0.6987 (3)0.0518 (9)
C90.0031 (4)0.8562 (2)0.7711 (3)0.0703 (11)
H9A0.09130.85390.73880.105*
H9B0.00280.87830.84680.105*
H9C0.04220.80330.77470.105*
C100.1797 (3)0.9700 (2)0.7281 (2)0.0499 (9)
C110.2103 (3)1.0002 (2)0.8444 (2)0.0510 (9)
C120.2562 (3)0.9532 (2)0.9333 (3)0.0548 (10)
C130.2572 (4)0.9783 (3)1.0569 (3)0.0757 (12)
C140.2646 (4)0.8416 (3)1.0536 (3)0.0733 (12)
C150.2935 (4)0.8683 (2)0.9362 (3)0.0571 (10)
C160.3695 (4)0.8242 (2)0.8651 (3)0.0604 (10)
C170.4348 (4)0.8593 (2)0.7641 (3)0.0705 (11)
H19A0.37860.84650.69630.106*
H19B0.52740.83770.75820.106*
H19C0.44050.91630.77260.106*
C180.4007 (5)0.7371 (2)0.8843 (4)0.0944 (14)
H20A0.35700.71930.95190.142*
H20B0.50030.72940.89370.142*
H20C0.36460.70670.81980.142*
C190.1698 (4)1.0877 (2)0.8638 (3)0.0626 (10)
C200.2892 (6)1.1463 (3)0.8951 (4)0.0893 (14)
N10.0841 (3)0.89758 (17)0.5823 (2)0.0568 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.120 (2)0.0799 (16)0.0573 (13)0.0276 (14)0.0156 (12)0.0024 (11)
F20.0753 (15)0.1020 (18)0.0614 (13)0.0155 (13)0.0102 (11)0.0204 (12)
F30.0700 (19)0.122 (3)0.244 (4)0.0082 (18)0.028 (2)0.061 (3)
F40.149 (3)0.121 (2)0.130 (2)0.015 (2)0.001 (2)0.068 (2)
F50.186 (4)0.130 (3)0.150 (3)0.051 (3)0.032 (3)0.004 (2)
O10.155 (3)0.118 (3)0.0509 (17)0.026 (2)0.0202 (18)0.0313 (18)
O20.091 (2)0.121 (3)0.0397 (14)0.0076 (19)0.0005 (13)0.0052 (18)
O30.124 (3)0.110 (3)0.077 (2)0.021 (2)0.0134 (18)0.038 (2)
C10.051 (2)0.056 (2)0.0388 (19)0.0042 (18)0.0032 (15)0.0016 (16)
C20.072 (3)0.074 (3)0.042 (2)0.002 (2)0.0004 (18)0.0015 (18)
C30.081 (3)0.095 (3)0.058 (3)0.010 (2)0.010 (2)0.007 (2)
C40.086 (3)0.105 (4)0.038 (2)0.005 (3)0.004 (2)0.003 (2)
C50.072 (3)0.079 (3)0.039 (2)0.009 (2)0.0045 (17)0.0108 (19)
C60.060 (2)0.058 (2)0.0331 (18)0.0114 (19)0.0077 (16)0.0043 (17)
C70.078 (3)0.079 (3)0.062 (2)0.001 (2)0.0227 (19)0.022 (2)
C80.055 (2)0.062 (2)0.0380 (19)0.0066 (19)0.0042 (15)0.0041 (17)
C90.069 (3)0.082 (3)0.060 (2)0.006 (2)0.0005 (19)0.001 (2)
C100.057 (2)0.061 (2)0.0310 (17)0.0039 (18)0.0033 (15)0.0033 (16)
C110.053 (2)0.063 (2)0.0367 (19)0.0021 (18)0.0033 (15)0.0070 (17)
C120.054 (2)0.075 (3)0.0346 (18)0.0017 (19)0.0046 (15)0.0065 (18)
C130.082 (3)0.105 (4)0.040 (2)0.017 (3)0.0110 (19)0.003 (3)
C140.068 (3)0.091 (3)0.059 (3)0.009 (2)0.014 (2)0.018 (3)
C150.058 (2)0.074 (3)0.0386 (19)0.004 (2)0.0095 (16)0.0022 (19)
C160.064 (2)0.063 (3)0.052 (2)0.005 (2)0.0160 (19)0.001 (2)
C170.069 (3)0.083 (3)0.060 (2)0.013 (2)0.0037 (19)0.009 (2)
C180.119 (4)0.075 (3)0.087 (3)0.013 (3)0.015 (3)0.004 (3)
C190.068 (2)0.078 (3)0.0407 (19)0.005 (2)0.0029 (18)0.0088 (19)
C200.102 (4)0.090 (4)0.076 (3)0.020 (3)0.006 (3)0.024 (3)
N10.0604 (19)0.064 (2)0.0447 (16)0.0021 (16)0.0103 (14)0.0104 (15)
Geometric parameters (Å, º) top
F1—C191.354 (4)C7—H7C0.9600
F2—C191.360 (4)C8—N11.373 (4)
F3—C201.278 (6)C8—C101.384 (5)
F4—C201.333 (5)C8—C91.486 (5)
F5—C201.348 (5)C9—H9A0.9600
O1—C131.188 (5)C9—H9B0.9600
O2—C131.384 (5)C9—H9C0.9600
O2—C141.388 (5)C10—C111.469 (4)
O3—C141.190 (4)C11—C121.359 (4)
C1—C21.393 (5)C11—C191.533 (5)
C1—C61.403 (4)C12—C151.463 (5)
C1—C101.446 (4)C12—C131.508 (5)
C2—C31.367 (5)C14—C151.485 (5)
C2—H20.9300C15—C161.351 (5)
C3—C41.413 (5)C16—C171.486 (5)
C3—H30.9300C16—C181.501 (5)
C4—C51.336 (5)C17—H19A0.9600
C4—H40.9300C17—H19B0.9600
C5—C61.393 (5)C17—H19C0.9600
C5—H50.9300C18—H20A0.9600
C6—N11.387 (4)C18—H20B0.9600
C7—N11.456 (4)C18—H20C0.9600
C7—H7A0.9600C19—C201.532 (6)
C7—H7B0.9600
C13—O2—C14111.2 (3)C11—C12—C13124.1 (3)
C2—C1—C6119.0 (3)C15—C12—C13105.0 (3)
C2—C1—C10134.4 (3)O1—C13—O2121.4 (4)
C6—C1—C10106.4 (3)O1—C13—C12131.5 (4)
C3—C2—C1118.1 (3)O2—C13—C12107.0 (4)
C3—C2—H2120.9O3—C14—O2119.7 (4)
C1—C2—H2120.9O3—C14—C15132.1 (5)
C2—C3—C4121.5 (4)O2—C14—C15108.1 (4)
C2—C3—H3119.2C16—C15—C12130.7 (3)
C4—C3—H3119.2C16—C15—C14122.6 (4)
C5—C4—C3121.3 (3)C12—C15—C14104.9 (3)
C5—C4—H4119.3C15—C16—C17122.4 (3)
C3—C4—H4119.3C15—C16—C18123.0 (3)
C4—C5—C6117.8 (3)C17—C16—C18114.5 (3)
C4—C5—H5121.1C16—C17—H19A109.5
C6—C5—H5121.1C16—C17—H19B109.5
N1—C6—C5129.5 (3)H19A—C17—H19B109.5
N1—C6—C1108.3 (3)C16—C17—H19C109.5
C5—C6—C1122.2 (4)H19A—C17—H19C109.5
N1—C7—H7A109.5H19B—C17—H19C109.5
N1—C7—H7B109.5C16—C18—H20A109.5
H7A—C7—H7B109.5C16—C18—H20B109.5
N1—C7—H7C109.5H20A—C18—H20B109.5
H7A—C7—H7C109.5C16—C18—H20C109.5
H7B—C7—H7C109.5H20A—C18—H20C109.5
N1—C8—C10109.3 (3)H20B—C18—H20C109.5
N1—C8—C9120.2 (3)F1—C19—F2104.1 (3)
C10—C8—C9130.4 (3)F1—C19—C20106.1 (4)
C8—C9—H9A109.5F2—C19—C20107.7 (3)
C8—C9—H9B109.5F1—C19—C11110.3 (3)
H9A—C9—H9B109.5F2—C19—C11110.7 (3)
C8—C9—H9C109.5C20—C19—C11117.1 (4)
H9A—C9—H9C109.5F3—C20—F4108.6 (4)
H9B—C9—H9C109.5F3—C20—F5106.5 (5)
C8—C10—C1107.0 (3)F4—C20—F5102.4 (4)
C8—C10—C11125.6 (3)F3—C20—C19114.6 (4)
C1—C10—C11127.5 (3)F4—C20—C19113.5 (4)
C12—C11—C10123.6 (3)F5—C20—C19110.3 (4)
C12—C11—C19120.8 (3)C8—N1—C6109.0 (3)
C10—C11—C19115.2 (3)C8—N1—C7125.7 (3)
C11—C12—C15130.3 (3)C6—N1—C7125.3 (3)
C6—C1—C2—C32.5 (5)C11—C12—C15—C1643.8 (6)
C10—C1—C2—C3177.6 (4)C13—C12—C15—C16144.8 (4)
C1—C2—C3—C40.2 (6)C11—C12—C15—C14151.8 (4)
C2—C3—C4—C51.7 (7)C13—C12—C15—C1419.5 (4)
C3—C4—C5—C61.0 (6)O3—C14—C15—C1627.4 (6)
C4—C5—C6—N1177.9 (4)O2—C14—C15—C16149.8 (3)
C4—C5—C6—C11.5 (5)O3—C14—C15—C12166.7 (4)
C2—C1—C6—N1176.2 (3)O2—C14—C15—C1216.2 (4)
C10—C1—C6—N10.2 (4)C12—C15—C16—C171.0 (6)
C2—C1—C6—C53.3 (5)C14—C15—C16—C17161.0 (3)
C10—C1—C6—C5179.7 (3)C12—C15—C16—C18178.0 (4)
N1—C8—C10—C10.3 (4)C14—C15—C16—C1816.1 (5)
C9—C8—C10—C1179.0 (3)C12—C11—C19—F1168.0 (3)
N1—C8—C10—C11178.4 (3)C10—C11—C19—F15.0 (4)
C9—C8—C10—C110.3 (6)C12—C11—C19—F253.4 (4)
C2—C1—C10—C8175.3 (4)C10—C11—C19—F2119.6 (3)
C6—C1—C10—C80.3 (4)C12—C11—C19—C2070.6 (5)
C2—C1—C10—C116.1 (6)C10—C11—C19—C20116.4 (4)
C6—C1—C10—C11178.4 (3)F1—C19—C20—F3131.8 (4)
C8—C10—C11—C1254.5 (5)F2—C19—C20—F3117.2 (4)
C1—C10—C11—C12127.0 (4)C11—C19—C20—F38.3 (6)
C8—C10—C11—C19118.3 (4)F1—C19—C20—F4102.6 (5)
C1—C10—C11—C1960.1 (5)F2—C19—C20—F48.4 (6)
C10—C11—C12—C154.2 (6)C11—C19—C20—F4133.8 (4)
C19—C11—C12—C15176.6 (3)F1—C19—C20—F511.7 (5)
C10—C11—C12—C13165.7 (3)F2—C19—C20—F5122.7 (4)
C19—C11—C12—C136.7 (5)C11—C19—C20—F5111.9 (4)
C14—O2—C13—O1171.7 (4)C10—C8—N1—C60.2 (4)
C14—O2—C13—C126.8 (4)C9—C8—N1—C6179.1 (3)
C11—C12—C13—O126.4 (7)C10—C8—N1—C7177.4 (3)
C15—C12—C13—O1161.6 (5)C9—C8—N1—C71.5 (5)
C11—C12—C13—O2155.3 (3)C5—C6—N1—C8179.4 (3)
C15—C12—C13—O216.7 (4)C1—C6—N1—C80.0 (4)
C13—O2—C14—O3176.7 (4)C5—C6—N1—C73.0 (6)
C13—O2—C14—C155.8 (4)C1—C6—N1—C7177.6 (3)
(III) (3Z)-3-[1-(1,2-dimethyl-1H-indol-3-yl)-2,2,3,3,4,4,4- heptafluorobutylidene]-4-(1-methylethylidene)dihydrofuran-2,5-dione top
Crystal data top
C21H16F7NO3Z = 2
Mr = 463.35F(000) = 472
Triclinic, P1Dx = 1.526 Mg m3
a = 10.070 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 11.003 (2) ÅCell parameters from 5487 reflections
c = 11.266 (2) Åθ = 2.0–25.0°
α = 93.75 (3)°µ = 0.15 mm1
β = 111.33 (3)°T = 93 K
γ = 115.80 (2)°Rhomb, yellow
V = 1008.9 (5) Å30.17 × 0.16 × 0.14 mm
Data collection top
Bruker P4 with CCD area-detector
diffractometer
3520 independent reflections
Radiation source: fine-focus sealed tube2421 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.025
Detector resolution: 512 x 512 pixels mm-1θmax = 25.0°, θmin = 2.0°
ϕ and ω scansh = 911
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 1213
Tmin = 0.975, Tmax = 0.980l = 1310
5487 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.152H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0794P)2 + 0.3462P]
where P = (Fo2 + 2Fc2)/3
3520 reflections(Δ/σ)max = 0.002
293 parametersΔρmax = 0.77 e Å3
0 restraintsΔρmin = 0.27 e Å3
Crystal data top
C21H16F7NO3γ = 115.80 (2)°
Mr = 463.35V = 1008.9 (5) Å3
Triclinic, P1Z = 2
a = 10.070 (2) ÅMo Kα radiation
b = 11.003 (2) ŵ = 0.15 mm1
c = 11.266 (2) ÅT = 93 K
α = 93.75 (3)°0.17 × 0.16 × 0.14 mm
β = 111.33 (3)°
Data collection top
Bruker P4 with CCD area-detector
diffractometer
3520 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2421 reflections with I > 2σ(I)
Tmin = 0.975, Tmax = 0.980Rint = 0.025
5487 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0540 restraints
wR(F2) = 0.152H-atom parameters constrained
S = 1.03Δρmax = 0.77 e Å3
3520 reflectionsΔρmin = 0.27 e Å3
293 parameters
Special details top

Experimental. DMAX > DTEST*.75 Q1 0.3515 - 0.0714 0.5546 0.77 1.29 H9A 1.43 H9C 1.54 C9 1.57 H7A

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 of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.2438 (2)0.28738 (19)0.89667 (16)0.0365 (5)
F20.4746 (2)0.38509 (17)1.07248 (15)0.0325 (4)
F30.1734 (2)0.03881 (19)0.90118 (18)0.0495 (5)
F40.4231 (2)0.08767 (19)1.02647 (18)0.0445 (5)
F50.1861 (2)0.1991 (2)1.11469 (19)0.0543 (6)
F60.2062 (3)0.0128 (2)1.1371 (2)0.0602 (6)
F70.4196 (2)0.2170 (2)1.23604 (17)0.0504 (5)
O10.7216 (3)0.3377 (3)1.1624 (2)0.0459 (6)
O20.8667 (3)0.3205 (2)1.0591 (2)0.0437 (6)
O30.9762 (3)0.3160 (3)0.9179 (3)0.0645 (8)
C10.2455 (3)0.2559 (3)0.6406 (3)0.0280 (7)
C20.2116 (4)0.3673 (3)0.6537 (3)0.0340 (7)
H20.26080.43290.73660.041*
C30.1042 (4)0.3760 (4)0.5411 (3)0.0456 (9)
H30.07960.44970.54670.055*
C40.0289 (4)0.2775 (4)0.4163 (4)0.0498 (10)
H40.04670.28590.34150.060*
C50.0620 (4)0.1739 (4)0.4020 (3)0.0419 (9)
H50.01220.10890.31860.050*
C60.1730 (4)0.1650 (3)0.5149 (3)0.0313 (7)
C70.1848 (4)0.0453 (4)0.4188 (3)0.0500 (10)
H7A0.28260.04220.41660.075*
H7B0.11860.03730.33420.075*
H7C0.12000.13430.43390.075*
C80.3434 (4)0.1036 (3)0.6554 (3)0.0322 (7)
C90.4241 (4)0.0168 (3)0.6970 (4)0.0459 (9)
H9A0.34060.08260.66400.069*
H9B0.48080.04200.79380.069*
H9C0.50340.03420.66050.069*
C100.3549 (3)0.2167 (3)0.7297 (3)0.0271 (7)
C110.4639 (3)0.2792 (3)0.8726 (3)0.0280 (7)
C120.6283 (4)0.3219 (3)0.9233 (3)0.0302 (7)
C130.7340 (4)0.3303 (3)1.0615 (3)0.0365 (8)
C140.8675 (4)0.3221 (4)0.9347 (4)0.0446 (9)
C150.7282 (4)0.3389 (3)0.8497 (3)0.0334 (7)
C160.7256 (4)0.3893 (3)0.7427 (3)0.0371 (8)
C170.6171 (4)0.4491 (3)0.6801 (3)0.0404 (8)
H19A0.52050.37870.60130.061*
H19B0.67770.53190.65480.061*
H19C0.58230.47580.74330.061*
C180.8354 (4)0.3938 (4)0.6784 (4)0.0508 (10)
H20A0.92270.49060.70050.076*
H20B0.77060.35820.58220.076*
H20C0.88410.33540.71090.076*
C190.3794 (3)0.2756 (3)0.9615 (3)0.0276 (7)
C200.3157 (4)0.1371 (3)1.0033 (3)0.0338 (7)
C210.2813 (4)0.1430 (4)1.1248 (3)0.0411 (8)
N10.2347 (3)0.0717 (3)0.5265 (3)0.0381 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0301 (10)0.0577 (12)0.0326 (10)0.0277 (9)0.0163 (8)0.0169 (9)
F20.0317 (10)0.0355 (10)0.0300 (9)0.0161 (8)0.0141 (8)0.0065 (8)
F30.0433 (12)0.0437 (11)0.0364 (11)0.0031 (10)0.0159 (10)0.0059 (9)
F40.0557 (12)0.0451 (12)0.0540 (12)0.0317 (10)0.0344 (10)0.0266 (10)
F50.0522 (13)0.0826 (16)0.0512 (12)0.0389 (12)0.0370 (11)0.0283 (11)
F60.0694 (15)0.0549 (14)0.0533 (13)0.0168 (12)0.0393 (12)0.0258 (10)
F70.0548 (13)0.0610 (13)0.0309 (11)0.0257 (11)0.0174 (10)0.0156 (10)
O10.0423 (14)0.0655 (17)0.0350 (14)0.0329 (13)0.0137 (12)0.0161 (12)
O20.0284 (12)0.0555 (15)0.0532 (15)0.0247 (12)0.0179 (11)0.0203 (12)
O30.0459 (16)0.089 (2)0.093 (2)0.0467 (16)0.0459 (16)0.0422 (17)
C10.0222 (15)0.0285 (16)0.0299 (17)0.0078 (13)0.0135 (13)0.0100 (13)
C20.0261 (17)0.0440 (19)0.0311 (17)0.0153 (15)0.0131 (14)0.0172 (15)
C30.042 (2)0.049 (2)0.051 (2)0.0253 (18)0.0201 (18)0.0252 (18)
C40.033 (2)0.066 (3)0.043 (2)0.0184 (19)0.0131 (17)0.0276 (19)
C50.0385 (19)0.042 (2)0.0284 (18)0.0050 (17)0.0162 (16)0.0089 (15)
C60.0242 (16)0.0372 (18)0.0266 (17)0.0049 (14)0.0171 (14)0.0131 (14)
C70.049 (2)0.045 (2)0.037 (2)0.0015 (18)0.0282 (18)0.0011 (16)
C80.0268 (17)0.0364 (18)0.0345 (18)0.0111 (15)0.0200 (15)0.0095 (14)
C90.040 (2)0.0347 (19)0.073 (3)0.0172 (17)0.037 (2)0.0110 (18)
C100.0203 (15)0.0286 (16)0.0301 (16)0.0077 (13)0.0142 (13)0.0074 (13)
C110.0262 (16)0.0291 (16)0.0309 (17)0.0140 (14)0.0138 (14)0.0101 (13)
C120.0273 (17)0.0299 (17)0.0364 (18)0.0145 (14)0.0164 (14)0.0102 (13)
C130.0269 (18)0.0356 (19)0.044 (2)0.0155 (15)0.0127 (16)0.0120 (15)
C140.0330 (19)0.046 (2)0.058 (2)0.0196 (17)0.0232 (18)0.0180 (18)
C150.0250 (16)0.0305 (17)0.0436 (19)0.0115 (14)0.0169 (15)0.0083 (14)
C160.0244 (17)0.0320 (18)0.047 (2)0.0070 (14)0.0171 (16)0.0068 (15)
C170.0346 (19)0.0390 (19)0.044 (2)0.0104 (16)0.0227 (17)0.0131 (16)
C180.042 (2)0.058 (2)0.062 (2)0.0208 (19)0.037 (2)0.0197 (19)
C190.0214 (15)0.0346 (17)0.0261 (16)0.0142 (14)0.0091 (13)0.0075 (13)
C200.0297 (17)0.0349 (18)0.0300 (17)0.0117 (15)0.0119 (15)0.0077 (14)
C210.040 (2)0.043 (2)0.037 (2)0.0155 (18)0.0199 (17)0.0140 (16)
N10.0341 (15)0.0362 (16)0.0406 (17)0.0087 (13)0.0243 (14)0.0058 (12)
Geometric parameters (Å, º) top
F1—C191.362 (3)C7—H7B0.9800
F2—C191.363 (3)C7—H7C0.9800
F3—C201.355 (3)C8—N11.369 (4)
F4—C201.363 (4)C8—C101.389 (4)
F5—C211.326 (4)C8—C91.500 (4)
F6—C211.343 (4)C9—H9A0.9800
F7—C211.335 (4)C9—H9B0.9800
O1—C131.189 (4)C9—H9C0.9800
O2—C131.396 (4)C10—C111.477 (4)
O2—C141.406 (4)C11—C121.373 (4)
O3—C141.206 (4)C11—C191.525 (4)
C1—C61.402 (4)C12—C151.483 (4)
C1—C21.421 (4)C12—C131.501 (5)
C1—C101.440 (4)C14—C151.480 (4)
C2—C31.377 (4)C15—C161.356 (5)
C2—H20.9500C16—C171.500 (5)
C3—C41.427 (5)C16—C181.513 (4)
C3—H30.9500C17—H19A0.9800
C4—C51.335 (5)C17—H19B0.9800
C4—H40.9500C17—H19C0.9800
C5—C61.398 (4)C18—H20A0.9800
C5—H50.9500C18—H20B0.9800
C6—N11.403 (4)C18—H20C0.9800
C7—N11.474 (4)C19—C201.555 (4)
C7—H7A0.9800C20—C211.534 (4)
C13—O2—C14111.1 (2)O1—C13—C12133.4 (3)
C6—C1—C2118.8 (3)O2—C13—C12107.6 (3)
C6—C1—C10107.0 (3)O3—C14—O2118.9 (3)
C2—C1—C10134.0 (3)O3—C14—C15132.8 (4)
C3—C2—C1117.1 (3)O2—C14—C15108.2 (3)
C3—C2—H2121.4C16—C15—C14121.9 (3)
C1—C2—H2121.4C16—C15—C12130.8 (3)
C2—C3—C4121.8 (3)C14—C15—C12105.9 (3)
C2—C3—H3119.1C15—C16—C17123.0 (3)
C4—C3—H3119.1C15—C16—C18122.9 (3)
C5—C4—C3121.7 (3)C17—C16—C18114.1 (3)
C5—C4—H4119.2C16—C17—H19A109.5
C3—C4—H4119.2C16—C17—H19B109.5
C4—C5—C6117.2 (3)H19A—C17—H19B109.5
C4—C5—H5121.4C16—C17—H19C109.5
C6—C5—H5121.4H19A—C17—H19C109.5
C5—C6—C1123.3 (3)H19B—C17—H19C109.5
C5—C6—N1128.9 (3)C16—C18—H20A109.5
C1—C6—N1107.8 (3)C16—C18—H20B109.5
N1—C7—H7A109.5H20A—C18—H20B109.5
N1—C7—H7B109.5C16—C18—H20C109.5
H7A—C7—H7B109.5H20A—C18—H20C109.5
N1—C7—H7C109.5H20B—C18—H20C109.5
H7A—C7—H7C109.5F1—C19—F2105.0 (2)
H7B—C7—H7C109.5F1—C19—C11110.0 (2)
N1—C8—C10109.6 (3)F2—C19—C11113.1 (2)
N1—C8—C9120.1 (3)F1—C19—C20105.0 (2)
C10—C8—C9130.3 (3)F2—C19—C20108.6 (2)
C8—C9—H9A109.5C11—C19—C20114.5 (2)
C8—C9—H9B109.5F3—C20—F4106.5 (2)
H9A—C9—H9B109.5F3—C20—C21106.8 (3)
C8—C9—H9C109.5F4—C20—C21107.3 (3)
H9A—C9—H9C109.5F3—C20—C19108.6 (2)
H9B—C9—H9C109.5F4—C20—C19110.5 (2)
C8—C10—C1106.8 (3)C21—C20—C19116.6 (3)
C8—C10—C11123.4 (3)F5—C21—F7108.4 (3)
C1—C10—C11129.7 (3)F5—C21—F6108.6 (3)
C12—C11—C10121.7 (3)F7—C21—F6107.0 (3)
C12—C11—C19121.9 (3)F5—C21—C20111.5 (3)
C10—C11—C19115.9 (2)F7—C21—C20111.6 (3)
C11—C12—C15127.8 (3)F6—C21—C20109.5 (3)
C11—C12—C13125.6 (3)C8—N1—C6108.7 (2)
C15—C12—C13105.4 (3)C8—N1—C7125.6 (3)
O1—C13—O2119.0 (3)C6—N1—C7125.6 (3)
C6—C1—C2—C32.0 (4)C13—C12—C15—C16152.9 (3)
C10—C1—C2—C3175.5 (3)C11—C12—C15—C14154.7 (3)
C1—C2—C3—C40.3 (5)C13—C12—C15—C1413.3 (3)
C2—C3—C4—C51.7 (5)C14—C15—C16—C17160.4 (3)
C3—C4—C5—C60.5 (5)C12—C15—C16—C173.9 (5)
C4—C5—C6—C12.0 (5)C14—C15—C16—C1817.8 (5)
C4—C5—C6—N1176.7 (3)C12—C15—C16—C18177.9 (3)
C2—C1—C6—C53.3 (4)C12—C11—C19—F1154.9 (3)
C10—C1—C6—C5178.4 (3)C10—C11—C19—F132.9 (3)
C2—C1—C6—N1175.7 (2)C12—C11—C19—F237.8 (4)
C10—C1—C6—N10.5 (3)C10—C11—C19—F2149.9 (2)
N1—C8—C10—C10.3 (3)C12—C11—C19—C2087.2 (3)
C9—C8—C10—C1177.3 (3)C10—C11—C19—C2085.0 (3)
N1—C8—C10—C11179.0 (3)F1—C19—C20—F342.1 (3)
C9—C8—C10—C113.4 (5)F2—C19—C20—F3154.0 (2)
C6—C1—C10—C80.5 (3)C11—C19—C20—F378.6 (3)
C2—C1—C10—C8174.6 (3)F1—C19—C20—F4158.6 (2)
C6—C1—C10—C11178.7 (3)F2—C19—C20—F489.5 (3)
C2—C1—C10—C114.7 (5)C11—C19—C20—F437.9 (3)
C8—C10—C11—C1252.8 (4)F1—C19—C20—C2178.5 (3)
C1—C10—C11—C12126.3 (3)F2—C19—C20—C2133.4 (3)
C8—C10—C11—C19119.5 (3)C11—C19—C20—C21160.9 (3)
C1—C10—C11—C1961.4 (4)F3—C20—C21—F570.3 (3)
C10—C11—C12—C1512.3 (5)F4—C20—C21—F5175.8 (3)
C19—C11—C12—C15175.9 (3)C19—C20—C21—F551.2 (4)
C10—C11—C12—C13153.4 (3)F3—C20—C21—F7168.3 (3)
C19—C11—C12—C1318.4 (5)F4—C20—C21—F754.3 (3)
C14—O2—C13—O1176.1 (3)C19—C20—C21—F770.2 (4)
C14—O2—C13—C126.6 (3)F3—C20—C21—F649.9 (3)
C11—C12—C13—O120.9 (6)F4—C20—C21—F664.0 (3)
C15—C12—C13—O1170.9 (4)C19—C20—C21—F6171.4 (3)
C11—C12—C13—O2155.9 (3)C10—C8—N1—C60.0 (3)
C15—C12—C13—O212.4 (3)C9—C8—N1—C6177.9 (3)
C13—O2—C14—O3179.1 (3)C10—C8—N1—C7177.4 (3)
C13—O2—C14—C152.0 (4)C9—C8—N1—C70.5 (4)
O3—C14—C15—C1618.7 (6)C5—C6—N1—C8178.5 (3)
O2—C14—C15—C16158.0 (3)C1—C6—N1—C80.3 (3)
O3—C14—C15—C12173.6 (4)C5—C6—N1—C74.1 (5)
O2—C14—C15—C129.8 (3)C1—C6—N1—C7177.0 (3)
C11—C12—C15—C1639.1 (5)
(IV) (3Z)-3-[1-(1,2-dimethyl-1H-indol-3-yl)-2,2,2-trifluoroethylidene]- 4-(tricyclo[3.3.1.13,7]decylidene)dihydrofuran-2,5-dione top
Crystal data top
C26H24F3NO3F(000) = 952
Mr = 455.46Dx = 1.419 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 7.721 (1) ÅCell parameters from 5081 reflections
b = 20.737 (2) Åθ = 1.8–28.3°
c = 13.496 (1) ŵ = 0.11 mm1
β = 99.35 (1)°T = 90 K
V = 2132.1 (4) Å3Plate, yellow
Z = 40.27 × 0.15 × 0.06 mm
Data collection top
Bruker P4 with CCD area-detector
diffractometer
5081 independent reflections
Radiation source: fine-focus sealed tube4050 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.050
Detector resolution: 512 x 512 pixels mm-1θmax = 28.3°, θmin = 1.8°
ϕ and ω scansh = 99
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 2719
Tmin = 0.975, Tmax = 0.992l = 1717
13914 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.056Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.140H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.0498P)2 + 1.976P]
where P = (Fo2 + 2Fc2)/3
5081 reflections(Δ/σ)max < 0.001
300 parametersΔρmax = 0.40 e Å3
0 restraintsΔρmin = 0.29 e Å3
Crystal data top
C26H24F3NO3V = 2132.1 (4) Å3
Mr = 455.46Z = 4
Monoclinic, P21/nMo Kα radiation
a = 7.721 (1) ŵ = 0.11 mm1
b = 20.737 (2) ÅT = 90 K
c = 13.496 (1) Å0.27 × 0.15 × 0.06 mm
β = 99.35 (1)°
Data collection top
Bruker P4 with CCD area-detector
diffractometer
5081 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
4050 reflections with I > 2σ(I)
Tmin = 0.975, Tmax = 0.992Rint = 0.050
13914 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0560 restraints
wR(F2) = 0.140H-atom parameters constrained
S = 1.09Δρmax = 0.40 e Å3
5081 reflectionsΔρmin = 0.29 e Å3
300 parameters
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 of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.14714 (17)0.09928 (7)0.10374 (9)0.0263 (3)
F20.41207 (18)0.07228 (7)0.11760 (9)0.0295 (3)
F30.3423 (2)0.17173 (7)0.10914 (9)0.0330 (4)
O10.2247 (2)0.02341 (8)0.03207 (11)0.0292 (4)
O20.2026 (2)0.03651 (7)0.12990 (11)0.0217 (3)
O30.2305 (2)0.03111 (7)0.29719 (11)0.0231 (3)
C10.5495 (3)0.21715 (10)0.07583 (14)0.0174 (4)
C20.6910 (3)0.21212 (11)0.02387 (16)0.0221 (4)
H10.70250.17660.01670.027*
C30.8137 (3)0.26134 (11)0.03428 (17)0.0253 (5)
H20.90870.25890.00000.030*
C40.7974 (3)0.31510 (11)0.09593 (16)0.0249 (5)
H30.88220.34730.10160.030*
C50.6599 (3)0.32104 (10)0.14772 (15)0.0223 (4)
H40.64990.35650.18860.027*
C60.5357 (3)0.27182 (10)0.13662 (15)0.0195 (4)
C70.3325 (3)0.30971 (11)0.25344 (18)0.0290 (5)
H7A0.20910.30420.25390.044*
H7B0.35440.35290.23320.044*
H7C0.39620.30200.31960.044*
C80.3146 (3)0.20524 (10)0.15613 (15)0.0180 (4)
C90.1579 (3)0.18219 (11)0.19753 (17)0.0248 (5)
H9A0.19260.16980.26640.037*
H9B0.10770.14570.15940.037*
H9C0.07270.21620.19340.037*
C100.4078 (3)0.17502 (9)0.08963 (14)0.0164 (4)
C110.3630 (3)0.11204 (10)0.04251 (15)0.0168 (4)
C120.3493 (3)0.05692 (9)0.09420 (14)0.0156 (4)
C130.2561 (3)0.00294 (10)0.05117 (16)0.0200 (4)
C140.2698 (3)0.00862 (9)0.22235 (15)0.0173 (4)
C150.3888 (3)0.04474 (9)0.20366 (14)0.0146 (4)
C160.5299 (3)0.06242 (9)0.27210 (14)0.0140 (4)
C170.6847 (3)0.09922 (9)0.24674 (14)0.0153 (4)
H220.66500.11070.17530.018*
C180.7123 (3)0.16085 (10)0.31196 (15)0.0197 (4)
H21A0.81310.18450.29670.024*
H21B0.60990.18850.29720.024*
C190.7422 (3)0.14206 (10)0.42377 (15)0.0213 (4)
H200.75820.18100.46530.026*
C200.5818 (3)0.10477 (10)0.44576 (15)0.0207 (4)
H19A0.47830.13180.43090.025*
H19B0.59780.09360.51640.025*
C210.5548 (3)0.04270 (10)0.38175 (14)0.0164 (4)
H180.45160.01910.39590.020*
C220.7197 (3)0.00052 (10)0.40592 (15)0.0183 (4)
H24A0.73720.01180.47620.022*
H24B0.70480.03850.36570.022*
C230.8799 (3)0.03771 (10)0.38364 (15)0.0186 (4)
H260.98470.01050.39870.022*
C240.9053 (3)0.09909 (10)0.44753 (15)0.0218 (4)
H25A1.00760.12240.43350.026*
H25B0.92480.08780.51820.026*
C250.8486 (3)0.05553 (10)0.27145 (14)0.0175 (4)
H23A0.83170.01660.23120.021*
H23B0.95050.07790.25500.021*
C260.3164 (3)0.11332 (10)0.07177 (15)0.0208 (4)
N10.3896 (2)0.26411 (8)0.18304 (13)0.0193 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0211 (6)0.0333 (7)0.0217 (6)0.0024 (5)0.0051 (5)0.0007 (5)
F20.0302 (7)0.0400 (8)0.0186 (6)0.0059 (6)0.0044 (5)0.0045 (6)
F30.0508 (9)0.0262 (7)0.0186 (6)0.0121 (6)0.0046 (6)0.0066 (5)
O10.0401 (10)0.0238 (8)0.0217 (8)0.0050 (7)0.0013 (7)0.0051 (6)
O20.0214 (7)0.0190 (7)0.0242 (7)0.0055 (6)0.0025 (6)0.0020 (6)
O30.0233 (8)0.0217 (8)0.0262 (8)0.0031 (6)0.0093 (6)0.0028 (6)
C10.0203 (10)0.0154 (9)0.0153 (9)0.0020 (8)0.0010 (7)0.0038 (7)
C20.0252 (11)0.0214 (10)0.0198 (10)0.0011 (8)0.0040 (8)0.0030 (8)
C30.0248 (11)0.0279 (12)0.0250 (11)0.0032 (9)0.0092 (9)0.0042 (9)
C40.0282 (12)0.0219 (11)0.0236 (10)0.0079 (9)0.0015 (9)0.0036 (8)
C50.0308 (12)0.0168 (10)0.0179 (10)0.0034 (8)0.0001 (8)0.0023 (8)
C60.0247 (11)0.0154 (9)0.0170 (9)0.0011 (8)0.0014 (8)0.0033 (7)
C70.0368 (13)0.0194 (11)0.0315 (12)0.0028 (9)0.0079 (10)0.0045 (9)
C80.0199 (10)0.0160 (9)0.0172 (9)0.0022 (8)0.0002 (8)0.0028 (7)
C90.0230 (11)0.0258 (11)0.0263 (11)0.0045 (9)0.0062 (9)0.0012 (9)
C100.0184 (10)0.0161 (9)0.0133 (8)0.0002 (7)0.0015 (7)0.0023 (7)
C110.0152 (9)0.0184 (10)0.0165 (9)0.0005 (7)0.0014 (7)0.0013 (7)
C120.0143 (9)0.0156 (9)0.0168 (9)0.0003 (7)0.0023 (7)0.0021 (7)
C130.0193 (10)0.0168 (10)0.0229 (10)0.0000 (8)0.0007 (8)0.0000 (8)
C140.0130 (9)0.0157 (9)0.0231 (10)0.0013 (7)0.0031 (8)0.0014 (8)
C150.0153 (9)0.0129 (9)0.0166 (9)0.0003 (7)0.0052 (7)0.0009 (7)
C160.0156 (9)0.0126 (9)0.0147 (8)0.0019 (7)0.0052 (7)0.0004 (7)
C170.0161 (9)0.0159 (9)0.0137 (8)0.0021 (7)0.0020 (7)0.0030 (7)
C180.0230 (10)0.0161 (10)0.0186 (9)0.0019 (8)0.0008 (8)0.0007 (8)
C190.0283 (11)0.0182 (10)0.0156 (9)0.0011 (8)0.0014 (8)0.0024 (8)
C200.0254 (11)0.0229 (10)0.0142 (9)0.0066 (8)0.0037 (8)0.0015 (8)
C210.0176 (10)0.0189 (10)0.0137 (9)0.0011 (7)0.0053 (7)0.0029 (7)
C220.0212 (10)0.0173 (9)0.0166 (9)0.0020 (8)0.0034 (8)0.0027 (7)
C230.0170 (10)0.0211 (10)0.0173 (9)0.0035 (8)0.0020 (8)0.0022 (8)
C240.0234 (11)0.0233 (11)0.0168 (9)0.0033 (8)0.0022 (8)0.0028 (8)
C250.0159 (10)0.0208 (10)0.0166 (9)0.0011 (8)0.0049 (7)0.0023 (8)
C260.0213 (10)0.0209 (10)0.0188 (9)0.0010 (8)0.0007 (8)0.0003 (8)
N10.0213 (9)0.0174 (8)0.0193 (8)0.0013 (7)0.0036 (7)0.0003 (7)
Geometric parameters (Å, º) top
F1—C261.340 (2)C11—C261.526 (3)
F2—C261.342 (3)C12—C151.481 (3)
F3—C261.339 (2)C12—C131.503 (3)
O1—C131.188 (3)C14—C151.485 (3)
O2—C131.388 (3)C15—C161.359 (3)
O2—C141.396 (2)C16—C171.504 (3)
O3—C141.196 (3)C16—C211.517 (3)
C1—C21.394 (3)C17—C181.547 (3)
C1—C61.413 (3)C17—C251.548 (3)
C1—C101.435 (3)C17—H220.9800
C2—C31.385 (3)C18—C191.539 (3)
C2—H10.9300C18—H21A0.9700
C3—C41.409 (3)C18—H21B0.9700
C3—H20.9300C19—C201.529 (3)
C4—C51.368 (3)C19—C241.534 (3)
C4—H30.9300C19—H200.9800
C5—C61.392 (3)C20—C211.545 (3)
C5—H40.9300C20—H19A0.9700
C6—N11.385 (3)C20—H19B0.9700
C7—N11.459 (3)C21—C221.536 (3)
C7—H7A0.9600C21—H180.9800
C7—H7B0.9600C22—C231.528 (3)
C7—H7C0.9600C22—H24A0.9700
C8—N11.375 (3)C22—H24B0.9700
C8—C101.388 (3)C23—C241.532 (3)
C8—C91.491 (3)C23—C251.539 (3)
C9—H9A0.9600C23—H260.9800
C9—H9B0.9600C24—H25A0.9700
C9—H9C0.9600C24—H25B0.9700
C10—C111.469 (3)C25—H23A0.9700
C11—C121.352 (3)C25—H23B0.9700
C13—O2—C14111.26 (15)C18—C17—H22110.1
C2—C1—C6119.41 (19)C25—C17—H22110.1
C2—C1—C10134.0 (2)C19—C18—C17109.48 (16)
C6—C1—C10106.38 (18)C19—C18—H21A109.8
C3—C2—C1118.2 (2)C17—C18—H21A109.8
C3—C2—H1120.9C19—C18—H21B109.8
C1—C2—H1120.9C17—C18—H21B109.8
C2—C3—C4121.2 (2)H21A—C18—H21B108.2
C2—C3—H2119.4C20—C19—C24109.22 (17)
C4—C3—H2119.4C20—C19—C18108.73 (16)
C5—C4—C3121.6 (2)C24—C19—C18109.83 (18)
C5—C4—H3119.2C20—C19—H20109.7
C3—C4—H3119.2C24—C19—H20109.7
C4—C5—C6117.2 (2)C18—C19—H20109.7
C4—C5—H4121.4C19—C20—C21110.64 (16)
C6—C5—H4121.4C19—C20—H19A109.5
N1—C6—C5129.3 (2)C21—C20—H19A109.5
N1—C6—C1108.28 (18)C19—C20—H19B109.5
C5—C6—C1122.3 (2)C21—C20—H19B109.5
N1—C7—H7A109.5H19A—C20—H19B108.1
N1—C7—H7B109.5C16—C21—C22109.27 (16)
H7A—C7—H7B109.5C16—C21—C20107.75 (16)
N1—C7—H7C109.5C22—C21—C20108.90 (16)
H7A—C7—H7C109.5C16—C21—H18110.3
H7B—C7—H7C109.5C22—C21—H18110.3
N1—C8—C10109.34 (18)C20—C21—H18110.3
N1—C8—C9121.22 (19)C23—C22—C21109.90 (16)
C10—C8—C9129.44 (19)C23—C22—H24A109.7
C8—C9—H9A109.5C21—C22—H24A109.7
C8—C9—H9B109.5C23—C22—H24B109.7
H9A—C9—H9B109.5C21—C22—H24B109.7
C8—C9—H9C109.5H24A—C22—H24B108.2
H9A—C9—H9C109.5C22—C23—C24110.02 (17)
H9B—C9—H9C109.5C22—C23—C25108.17 (16)
C8—C10—C1107.17 (18)C24—C23—C25109.85 (17)
C8—C10—C11124.80 (19)C22—C23—H26109.6
C1—C10—C11128.02 (19)C24—C23—H26109.6
C12—C11—C10124.12 (18)C25—C23—H26109.6
C12—C11—C26120.71 (18)C23—C24—C19109.83 (16)
C10—C11—C26114.98 (17)C23—C24—H25A109.7
C11—C12—C15129.65 (18)C19—C24—H25A109.7
C11—C12—C13124.85 (18)C23—C24—H25B109.7
C15—C12—C13104.64 (16)C19—C24—H25B109.7
O1—C13—O2120.25 (19)H25A—C24—H25B108.2
O1—C13—C12132.2 (2)C23—C25—C17110.17 (16)
O2—C13—C12107.56 (16)C23—C25—H23A109.6
O3—C14—O2118.99 (18)C17—C25—H23A109.6
O3—C14—C15133.07 (19)C23—C25—H23B109.6
O2—C14—C15107.88 (16)C17—C25—H23B109.6
C16—C15—C12130.11 (18)H23A—C25—H23B108.1
C16—C15—C14122.33 (17)F3—C26—F1105.83 (16)
C12—C15—C14105.29 (16)F3—C26—F2105.83 (18)
C15—C16—C17124.14 (17)F1—C26—F2107.15 (16)
C15—C16—C21123.42 (17)F3—C26—C11111.78 (16)
C17—C16—C21112.29 (16)F1—C26—C11112.28 (17)
C16—C17—C18109.32 (16)F2—C26—C11113.43 (17)
C16—C17—C25107.82 (16)C8—N1—C6108.78 (17)
C18—C17—C25109.20 (16)C8—N1—C7126.05 (19)
C16—C17—H22110.1C6—N1—C7125.07 (18)
C6—C1—C2—C30.2 (3)C12—C15—C16—C21176.53 (19)
C10—C1—C2—C3174.4 (2)C14—C15—C16—C2116.3 (3)
C1—C2—C3—C40.3 (3)C15—C16—C17—C18124.7 (2)
C2—C3—C4—C50.2 (3)C21—C16—C17—C1859.6 (2)
C3—C4—C5—C60.3 (3)C15—C16—C17—C25116.7 (2)
C4—C5—C6—N1176.8 (2)C21—C16—C17—C2559.0 (2)
C4—C5—C6—C10.8 (3)C16—C17—C18—C1958.6 (2)
C2—C1—C6—N1177.49 (17)C25—C17—C18—C1959.2 (2)
C10—C1—C6—N11.6 (2)C17—C18—C19—C2059.3 (2)
C2—C1—C6—C50.7 (3)C17—C18—C19—C2460.1 (2)
C10—C1—C6—C5175.19 (18)C24—C19—C20—C2159.3 (2)
N1—C8—C10—C10.8 (2)C18—C19—C20—C2160.6 (2)
C9—C8—C10—C1178.7 (2)C15—C16—C21—C22116.7 (2)
N1—C8—C10—C11178.18 (17)C17—C16—C21—C2259.0 (2)
C9—C8—C10—C112.3 (3)C15—C16—C21—C20125.1 (2)
C2—C1—C10—C8175.5 (2)C17—C16—C21—C2059.2 (2)
C6—C1—C10—C80.5 (2)C19—C20—C21—C1659.3 (2)
C2—C1—C10—C115.5 (4)C19—C20—C21—C2259.1 (2)
C6—C1—C10—C11179.41 (18)C16—C21—C22—C2358.6 (2)
C8—C10—C11—C1257.6 (3)C20—C21—C22—C2358.8 (2)
C1—C10—C11—C12123.6 (2)C21—C22—C23—C2459.8 (2)
C8—C10—C11—C26117.4 (2)C21—C22—C23—C2560.2 (2)
C1—C10—C11—C2661.4 (3)C22—C23—C24—C1959.7 (2)
C10—C11—C12—C156.0 (3)C25—C23—C24—C1959.2 (2)
C26—C11—C12—C15179.31 (19)C20—C19—C24—C2359.1 (2)
C10—C11—C12—C13161.72 (19)C18—C19—C24—C2360.1 (2)
C26—C11—C12—C1313.0 (3)C22—C23—C25—C1761.2 (2)
C14—O2—C13—O1172.97 (19)C24—C23—C25—C1758.9 (2)
C14—O2—C13—C127.2 (2)C16—C17—C25—C2359.9 (2)
C11—C12—C13—O125.6 (4)C18—C17—C25—C2358.7 (2)
C15—C12—C13—O1164.2 (2)C12—C11—C26—F3178.57 (19)
C11—C12—C13—O2154.21 (19)C10—C11—C26—F36.2 (3)
C15—C12—C13—O216.0 (2)C12—C11—C26—F162.7 (3)
C13—O2—C14—O3177.72 (18)C10—C11—C26—F1112.5 (2)
C13—O2—C14—C154.7 (2)C12—C11—C26—F259.0 (3)
C11—C12—C15—C1645.9 (3)C10—C11—C26—F2125.81 (19)
C13—C12—C15—C16144.5 (2)C10—C8—N1—C61.8 (2)
C11—C12—C15—C14151.3 (2)C9—C8—N1—C6177.76 (18)
C13—C12—C15—C1418.3 (2)C10—C8—N1—C7178.46 (19)
O3—C14—C15—C1627.3 (3)C9—C8—N1—C71.1 (3)
O2—C14—C15—C16149.80 (18)C5—C6—N1—C8174.4 (2)
O3—C14—C15—C12168.2 (2)C1—C6—N1—C82.1 (2)
O2—C14—C15—C1214.7 (2)C5—C6—N1—C72.3 (3)
C12—C15—C16—C171.3 (3)C1—C6—N1—C7178.79 (19)
C14—C15—C16—C17158.96 (18)
(V) (3Z)-3-[1-(1,2-dimethyl-1H-indol-3-yl)-2,2,3,3,4,4,4-heptafluorobutylidene]- 4-(tricyclo[3.3.1.13,7]decylidene)dihydrofuran-2,5-dione top
Crystal data top
C28H24F7NO3Z = 2
Mr = 555.48F(000) = 572
Triclinic, P1Dx = 1.470 Mg m3
a = 10.313 (1) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.924 (1) ÅCell parameters from 4383 reflections
c = 11.729 (1) Åθ = 1.8–25.0°
α = 87.67 (1)°µ = 0.13 mm1
β = 82.65 (1)°T = 90 K
γ = 73.24 (1)°Plate, yellow
V = 1254.8 (2) Å30.21 × 0.15 × 0.08 mm
Data collection top
Bruker P4 with CCD area-detector
diffractometer
4383 independent reflections
Radiation source: fine-focus sealed tube3293 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.030
Detector resolution: 512 x 512 pixels mm-1θmax = 25.0°, θmin = 1.8°
ϕ and ω scansh = 1012
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
k = 1212
Tmin = 0.978, Tmax = 0.990l = 1313
6916 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.110H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0485P)2 + 0.2697P]
where P = (Fo2 + 2Fc2)/3
4383 reflections(Δ/σ)max = 0.003
354 parametersΔρmax = 0.30 e Å3
0 restraintsΔρmin = 0.24 e Å3
Crystal data top
C28H24F7NO3γ = 73.24 (1)°
Mr = 555.48V = 1254.8 (2) Å3
Triclinic, P1Z = 2
a = 10.313 (1) ÅMo Kα radiation
b = 10.924 (1) ŵ = 0.13 mm1
c = 11.729 (1) ÅT = 90 K
α = 87.67 (1)°0.21 × 0.15 × 0.08 mm
β = 82.65 (1)°
Data collection top
Bruker P4 with CCD area-detector
diffractometer
4383 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
3293 reflections with I > 2σ(I)
Tmin = 0.978, Tmax = 0.990Rint = 0.030
6916 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0440 restraints
wR(F2) = 0.110H-atom parameters constrained
S = 1.03Δρmax = 0.30 e Å3
4383 reflectionsΔρmin = 0.24 e Å3
354 parameters
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 of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.34257 (12)1.23487 (11)0.77112 (11)0.0299 (3)
F20.22772 (14)1.21890 (11)0.63358 (10)0.0317 (3)
F30.07838 (12)1.22282 (12)0.91734 (11)0.0300 (3)
F40.00043 (12)1.27194 (12)0.75383 (12)0.0355 (3)
F50.17664 (13)1.42570 (12)0.90584 (11)0.0318 (3)
F60.03227 (13)1.47875 (13)0.87176 (12)0.0394 (4)
F70.12849 (15)1.46782 (12)0.73239 (12)0.0401 (4)
O10.33893 (17)1.16043 (15)0.98669 (14)0.0377 (4)
O20.34123 (16)0.96665 (15)1.05525 (13)0.0330 (4)
O30.34825 (19)0.76020 (17)1.08011 (14)0.0434 (5)
C10.2327 (2)0.96503 (19)0.56842 (18)0.0206 (5)
C20.3237 (2)0.9970 (2)0.48103 (19)0.0269 (5)
H20.38041.04500.49690.032*
C30.3271 (3)0.9551 (2)0.3704 (2)0.0334 (6)
H30.38820.97390.31180.040*
C40.2399 (3)0.8846 (2)0.34530 (19)0.0346 (6)
H40.24310.85950.26990.042*
C50.1512 (2)0.8521 (2)0.4282 (2)0.0314 (6)
H50.09350.80580.41080.038*
C60.1496 (2)0.89063 (19)0.54049 (19)0.0233 (5)
C70.0196 (2)0.7876 (2)0.6455 (2)0.0357 (6)
H7A0.09200.82920.60100.054*
H7B0.05670.78010.72390.054*
H7C0.02630.70400.61490.054*
C80.1124 (2)0.9158 (2)0.73193 (19)0.0227 (5)
C90.0474 (2)0.9039 (2)0.85114 (19)0.0310 (5)
H9A0.04980.92610.85190.046*
H9B0.06980.96050.90090.046*
H9C0.08040.81740.87750.046*
C100.2076 (2)0.98050 (19)0.69132 (18)0.0199 (5)
C110.2667 (2)1.04772 (19)0.76731 (18)0.0208 (5)
C120.3296 (2)0.98912 (19)0.85813 (18)0.0205 (5)
C130.3386 (2)1.0545 (2)0.96619 (19)0.0269 (5)
C140.3538 (2)0.8441 (2)1.0130 (2)0.0300 (5)
C150.3722 (2)0.8507 (2)0.88647 (18)0.0213 (5)
C160.4449 (2)0.7498 (2)0.81970 (18)0.0200 (5)
C170.4932 (2)0.7611 (2)0.69414 (18)0.0218 (5)
H170.46140.85010.66850.026*
C180.4930 (2)0.6145 (2)0.86389 (19)0.0251 (5)
H180.45980.61040.94560.030*
C190.6504 (2)0.5684 (2)0.84545 (19)0.0257 (5)
H19A0.68690.62170.88890.031*
H19B0.68200.48110.87280.031*
C200.7011 (2)0.5752 (2)0.71720 (19)0.0277 (5)
H200.80100.54640.70560.033*
C210.6508 (2)0.7143 (2)0.67766 (19)0.0273 (5)
H21A0.68410.72130.59720.033*
H21B0.68640.76790.72170.033*
C220.4377 (2)0.6747 (2)0.6250 (2)0.0309 (6)
H22A0.33870.70280.63550.037*
H22B0.46840.68070.54380.037*
C230.4884 (2)0.5360 (2)0.6659 (2)0.0336 (6)
H230.45240.48120.62220.040*
C240.4363 (2)0.5300 (2)0.7934 (2)0.0333 (6)
H24A0.46470.44230.82040.040*
H24B0.33740.55910.80400.040*
C250.6443 (2)0.4903 (2)0.6490 (2)0.0351 (6)
H25A0.67720.49370.56800.042*
H25B0.67540.40240.67480.042*
C260.2392 (2)1.1913 (2)0.74699 (18)0.0224 (5)
C270.1029 (2)1.2733 (2)0.81294 (18)0.0220 (5)
C280.0946 (2)1.4139 (2)0.8314 (2)0.0272 (5)
N10.07762 (17)0.86315 (17)0.64040 (16)0.0253 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0225 (7)0.0240 (7)0.0445 (8)0.0097 (5)0.0004 (6)0.0057 (6)
F20.0494 (9)0.0204 (7)0.0228 (7)0.0074 (6)0.0019 (6)0.0028 (5)
F30.0280 (7)0.0278 (7)0.0305 (7)0.0046 (6)0.0018 (6)0.0033 (6)
F40.0267 (7)0.0339 (8)0.0463 (9)0.0025 (6)0.0167 (6)0.0099 (6)
F50.0325 (7)0.0276 (7)0.0367 (8)0.0066 (6)0.0113 (6)0.0076 (6)
F60.0310 (8)0.0307 (8)0.0494 (9)0.0070 (6)0.0110 (6)0.0132 (7)
F70.0621 (10)0.0204 (7)0.0348 (8)0.0067 (7)0.0086 (7)0.0047 (6)
O10.0453 (11)0.0253 (10)0.0426 (10)0.0036 (8)0.0174 (8)0.0113 (8)
O20.0410 (10)0.0279 (9)0.0236 (9)0.0029 (7)0.0086 (7)0.0048 (7)
O30.0631 (13)0.0335 (10)0.0235 (9)0.0018 (9)0.0019 (8)0.0057 (8)
C10.0208 (11)0.0156 (11)0.0222 (11)0.0016 (9)0.0072 (9)0.0025 (9)
C20.0297 (13)0.0198 (12)0.0256 (12)0.0022 (10)0.0047 (10)0.0020 (9)
C30.0423 (15)0.0254 (13)0.0232 (12)0.0022 (11)0.0016 (10)0.0020 (10)
C40.0569 (17)0.0236 (13)0.0179 (12)0.0004 (12)0.0117 (11)0.0015 (10)
C50.0388 (14)0.0210 (12)0.0333 (14)0.0008 (10)0.0175 (11)0.0016 (10)
C60.0230 (12)0.0154 (11)0.0282 (12)0.0041 (9)0.0128 (9)0.0022 (9)
C70.0287 (14)0.0278 (13)0.0556 (17)0.0102 (11)0.0184 (12)0.0013 (12)
C80.0202 (11)0.0173 (11)0.0294 (12)0.0007 (9)0.0092 (9)0.0000 (9)
C90.0254 (13)0.0347 (14)0.0326 (13)0.0102 (11)0.0004 (10)0.0035 (11)
C100.0186 (11)0.0155 (11)0.0240 (11)0.0013 (9)0.0053 (9)0.0005 (9)
C110.0174 (11)0.0185 (11)0.0247 (12)0.0032 (9)0.0006 (9)0.0015 (9)
C120.0185 (11)0.0178 (11)0.0232 (11)0.0019 (9)0.0024 (9)0.0016 (9)
C130.0211 (12)0.0279 (14)0.0274 (12)0.0028 (10)0.0092 (9)0.0042 (10)
C140.0318 (13)0.0280 (13)0.0246 (12)0.0011 (10)0.0042 (10)0.0023 (11)
C150.0206 (11)0.0215 (12)0.0219 (11)0.0055 (9)0.0057 (9)0.0033 (9)
C160.0177 (11)0.0198 (11)0.0237 (11)0.0053 (9)0.0079 (9)0.0026 (9)
C170.0239 (12)0.0146 (11)0.0244 (12)0.0000 (9)0.0069 (9)0.0013 (9)
C180.0287 (12)0.0188 (11)0.0270 (12)0.0043 (9)0.0072 (10)0.0034 (9)
C190.0282 (12)0.0189 (11)0.0287 (12)0.0009 (9)0.0127 (10)0.0029 (9)
C200.0223 (12)0.0224 (12)0.0328 (13)0.0026 (9)0.0048 (10)0.0019 (10)
C210.0267 (12)0.0261 (12)0.0257 (12)0.0029 (10)0.0027 (10)0.0041 (10)
C220.0356 (14)0.0234 (12)0.0302 (13)0.0029 (10)0.0167 (11)0.0031 (10)
C230.0394 (14)0.0198 (12)0.0433 (15)0.0031 (10)0.0231 (12)0.0037 (11)
C240.0294 (13)0.0186 (12)0.0523 (16)0.0049 (10)0.0119 (11)0.0032 (11)
C250.0446 (15)0.0221 (13)0.0312 (14)0.0056 (11)0.0110 (11)0.0029 (10)
C260.0264 (12)0.0199 (11)0.0215 (11)0.0069 (9)0.0045 (9)0.0002 (9)
C270.0218 (11)0.0211 (12)0.0235 (11)0.0048 (9)0.0091 (9)0.0024 (9)
C280.0265 (12)0.0225 (12)0.0290 (13)0.0008 (10)0.0077 (10)0.0018 (10)
N10.0232 (10)0.0213 (10)0.0337 (11)0.0074 (8)0.0105 (8)0.0040 (8)
Geometric parameters (Å, º) top
F1—C261.351 (2)C11—C121.359 (3)
F2—C261.364 (2)C11—C261.526 (3)
F3—C271.347 (2)C12—C151.484 (3)
F4—C271.347 (2)C12—C131.506 (3)
F5—C281.325 (2)C14—C151.474 (3)
F6—C281.331 (3)C15—C161.355 (3)
F7—C281.334 (3)C16—C171.505 (3)
O1—C131.193 (3)C16—C181.510 (3)
O2—C131.387 (3)C17—C221.539 (3)
O2—C141.411 (3)C17—C211.546 (3)
O3—C141.193 (3)C17—H170.9800
C1—C21.403 (3)C18—C241.541 (3)
C1—C61.413 (3)C18—C191.544 (3)
C1—C101.440 (3)C18—H180.9800
C2—C31.386 (3)C19—C201.534 (3)
C2—H20.9300C19—H19A0.9700
C3—C41.405 (3)C19—H19B0.9700
C3—H30.9300C20—C251.529 (3)
C4—C51.357 (3)C20—C211.531 (3)
C4—H40.9300C20—H200.9800
C5—C61.396 (3)C21—H21A0.9700
C5—H50.9300C21—H21B0.9700
C6—N11.375 (3)C22—C231.533 (3)
C7—N11.466 (3)C22—H22A0.9700
C7—H7A0.9600C22—H22B0.9700
C7—H7B0.9600C23—C241.528 (4)
C7—H7C0.9600C23—C251.529 (3)
C8—N11.371 (3)C23—H230.9800
C8—C101.395 (3)C24—H24A0.9700
C8—C91.489 (3)C24—H24B0.9700
C9—H9A0.9600C25—H25A0.9700
C9—H9B0.9600C25—H25B0.9700
C9—H9C0.9600C26—C271.559 (3)
C10—C111.468 (3)C27—C281.536 (3)
C13—O2—C14111.02 (17)C24—C18—H18110.2
C2—C1—C6118.8 (2)C19—C18—H18110.2
C2—C1—C10134.7 (2)C20—C19—C18109.71 (17)
C6—C1—C10106.17 (18)C20—C19—H19A109.7
C3—C2—C1118.3 (2)C18—C19—H19A109.7
C3—C2—H2120.8C20—C19—H19B109.7
C1—C2—H2120.8C18—C19—H19B109.7
C2—C3—C4121.2 (2)H19A—C19—H19B108.2
C2—C3—H3119.4C25—C20—C21109.90 (18)
C4—C3—H3119.4C25—C20—C19109.66 (19)
C5—C4—C3121.7 (2)C21—C20—C19108.17 (18)
C5—C4—H4119.2C25—C20—H20109.7
C3—C4—H4119.2C21—C20—H20109.7
C4—C5—C6117.7 (2)C19—C20—H20109.7
C4—C5—H5121.2C20—C21—C17110.46 (18)
C6—C5—H5121.2C20—C21—H21A109.6
N1—C6—C5129.4 (2)C17—C21—H21A109.6
N1—C6—C1108.35 (18)C20—C21—H21B109.6
C5—C6—C1122.2 (2)C17—C21—H21B109.6
N1—C7—H7A109.5H21A—C21—H21B108.1
N1—C7—H7B109.5C23—C22—C17109.59 (17)
H7A—C7—H7B109.5C23—C22—H22A109.8
N1—C7—H7C109.5C17—C22—H22A109.8
H7A—C7—H7C109.5C23—C22—H22B109.8
H7B—C7—H7C109.5C17—C22—H22B109.8
N1—C8—C10108.79 (19)H22A—C22—H22B108.2
N1—C8—C9121.32 (19)C24—C23—C25109.74 (18)
C10—C8—C9129.8 (2)C24—C23—C22108.29 (19)
C8—C9—H9A109.5C25—C23—C22110.3 (2)
C8—C9—H9B109.5C24—C23—H23109.5
H9A—C9—H9B109.5C25—C23—H23109.5
C8—C9—H9C109.5C22—C23—H23109.5
H9A—C9—H9C109.5C23—C24—C18110.28 (19)
H9B—C9—H9C109.5C23—C24—H24A109.6
C8—C10—C1107.11 (18)C18—C24—H24A109.6
C8—C10—C11122.89 (19)C23—C24—H24B109.6
C1—C10—C11130.00 (19)C18—C24—H24B109.6
C12—C11—C10122.26 (19)H24A—C24—H24B108.1
C12—C11—C26121.41 (19)C23—C25—C20109.79 (19)
C10—C11—C26115.96 (17)C23—C25—H25A109.7
C11—C12—C15128.52 (19)C20—C25—H25A109.7
C11—C12—C13125.41 (19)C23—C25—H25B109.7
C15—C12—C13104.52 (17)C20—C25—H25B109.7
O1—C13—O2119.3 (2)H25A—C25—H25B108.2
O1—C13—C12133.4 (2)F1—C26—F2105.45 (16)
O2—C13—C12107.26 (18)F1—C26—C11112.55 (17)
O3—C14—O2118.8 (2)F2—C26—C11109.92 (17)
O3—C14—C15133.4 (2)F1—C26—C27109.19 (17)
O2—C14—C15107.80 (18)F2—C26—C27105.18 (16)
C16—C15—C14122.87 (19)C11—C26—C27113.96 (17)
C16—C15—C12129.95 (19)F3—C27—F4107.01 (16)
C14—C15—C12105.25 (18)F3—C27—C28107.04 (17)
C15—C16—C17123.66 (18)F4—C27—C28107.40 (16)
C15—C16—C18123.96 (19)F3—C27—C26110.91 (16)
C17—C16—C18112.30 (18)F4—C27—C26108.69 (17)
C16—C17—C22108.77 (18)C28—C27—C26115.42 (18)
C16—C17—C21108.22 (16)F5—C28—F6108.05 (18)
C22—C17—C21109.16 (18)F5—C28—F7108.37 (18)
C16—C17—H17110.2F6—C28—F7107.96 (17)
C22—C17—H17110.2F5—C28—C27111.81 (17)
C21—C17—H17110.2F6—C28—C27110.03 (18)
C16—C18—C24107.54 (17)F7—C28—C27110.51 (18)
C16—C18—C19109.31 (17)C8—N1—C6109.57 (17)
C24—C18—C19109.22 (18)C8—N1—C7126.36 (19)
C16—C18—H18110.2C6—N1—C7124.07 (19)
C6—C1—C2—C30.7 (3)C17—C16—C18—C1958.8 (2)
C10—C1—C2—C3173.8 (2)C16—C18—C19—C2058.7 (2)
C1—C2—C3—C41.3 (3)C24—C18—C19—C2058.7 (2)
C2—C3—C4—C51.5 (3)C18—C19—C20—C2559.8 (2)
C3—C4—C5—C60.3 (3)C18—C19—C20—C2160.1 (2)
C4—C5—C6—N1175.0 (2)C25—C20—C21—C1758.7 (2)
C4—C5—C6—C12.4 (3)C19—C20—C21—C1761.0 (2)
C2—C1—C6—N1175.26 (18)C16—C17—C21—C2059.6 (2)
C10—C1—C6—N10.4 (2)C22—C17—C21—C2058.7 (2)
C2—C1—C6—C52.6 (3)C16—C17—C22—C2359.1 (2)
C10—C1—C6—C5177.48 (19)C21—C17—C22—C2358.8 (2)
N1—C8—C10—C10.5 (2)C17—C22—C23—C2460.3 (2)
C9—C8—C10—C1178.0 (2)C17—C22—C23—C2559.8 (2)
N1—C8—C10—C11179.81 (18)C25—C23—C24—C1859.2 (2)
C9—C8—C10—C112.7 (3)C22—C23—C24—C1861.3 (2)
C2—C1—C10—C8173.6 (2)C16—C18—C24—C2359.9 (2)
C6—C1—C10—C80.1 (2)C19—C18—C24—C2358.6 (2)
C2—C1—C10—C115.6 (4)C24—C23—C25—C2059.7 (2)
C6—C1—C10—C11179.3 (2)C22—C23—C25—C2059.5 (2)
C8—C10—C11—C1254.4 (3)C21—C20—C25—C2358.7 (2)
C1—C10—C11—C12124.7 (2)C19—C20—C25—C2360.1 (2)
C8—C10—C11—C26118.8 (2)C12—C11—C26—F138.7 (3)
C1—C10—C11—C2662.1 (3)C10—C11—C26—F1148.08 (17)
C10—C11—C12—C1511.6 (3)C12—C11—C26—F2155.90 (19)
C26—C11—C12—C15175.6 (2)C10—C11—C26—F230.9 (2)
C10—C11—C12—C13152.0 (2)C12—C11—C26—C2786.3 (2)
C26—C11—C12—C1320.8 (3)C10—C11—C26—C2786.9 (2)
C14—O2—C13—O1174.3 (2)F1—C26—C27—F390.0 (2)
C14—O2—C13—C128.1 (2)F2—C26—C27—F3157.22 (15)
C11—C12—C13—O128.1 (4)C11—C26—C27—F336.8 (2)
C15—C12—C13—O1165.1 (2)F1—C26—C27—F4152.60 (16)
C11—C12—C13—O2149.0 (2)F2—C26—C27—F439.8 (2)
C15—C12—C13—O217.8 (2)C11—C26—C27—F480.6 (2)
C13—O2—C14—O3175.0 (2)F1—C26—C27—C2831.9 (2)
C13—O2—C14—C155.0 (2)F2—C26—C27—C2880.8 (2)
O3—C14—C15—C1630.4 (4)C11—C26—C27—C28158.70 (18)
O2—C14—C15—C16149.5 (2)F3—C27—C28—F554.3 (2)
O3—C14—C15—C12164.0 (3)F4—C27—C28—F5168.89 (17)
O2—C14—C15—C1216.1 (2)C26—C27—C28—F569.7 (2)
C11—C12—C15—C1649.8 (3)F3—C27—C28—F665.8 (2)
C13—C12—C15—C16144.0 (2)F4—C27—C28—F648.8 (2)
C11—C12—C15—C14146.0 (2)C26—C27—C28—F6170.21 (17)
C13—C12—C15—C1420.2 (2)F3—C27—C28—F7175.07 (16)
C14—C15—C16—C17164.9 (2)F4—C27—C28—F770.3 (2)
C12—C15—C16—C173.1 (3)C26—C27—C28—F751.1 (2)
C14—C15—C16—C1811.7 (3)C10—C8—N1—C60.7 (2)
C12—C15—C16—C18173.5 (2)C9—C8—N1—C6178.50 (19)
C15—C16—C17—C22123.1 (2)C10—C8—N1—C7179.87 (19)
C18—C16—C17—C2259.9 (2)C9—C8—N1—C72.1 (3)
C15—C16—C17—C21118.4 (2)C5—C6—N1—C8176.9 (2)
C18—C16—C17—C2158.6 (2)C1—C6—N1—C80.7 (2)
C15—C16—C18—C24123.3 (2)C5—C6—N1—C72.5 (3)
C17—C16—C18—C2459.7 (2)C1—C6—N1—C7179.92 (18)
C15—C16—C18—C19118.2 (2)

Experimental details

(I)(II)(III)(IV)
Crystal data
Chemical formulaC19H16F3NO3C20H16F5NO3C21H16F7NO3C26H24F3NO3
Mr363.33413.34463.35455.46
Crystal system, space groupMonoclinic, P21/nMonoclinic, P21/cTriclinic, P1Monoclinic, P21/n
Temperature (K)90909390
a, b, c (Å)11.660 (1), 17.164 (2), 17.102 (2)9.539 (1), 16.716 (1), 11.720 (1)10.070 (2), 11.003 (2), 11.266 (2)7.721 (1), 20.737 (2), 13.496 (1)
α, β, γ (°)90, 92.75 (2), 9090, 92.90 (1), 9093.75 (3), 111.33 (3), 115.80 (2)90, 99.35 (1), 90
V3)3418.9 (6)1866.6 (3)1008.9 (5)2132.1 (4)
Z8424
Radiation typeMo KαMo KαMo KαMo Kα
µ (mm1)0.120.130.150.11
Crystal size (mm)0.25 × 0.16 × 0.040.24 × 0.16 × 0.120.17 × 0.16 × 0.140.27 × 0.15 × 0.06
Data collection
DiffractometerBruker P4 with CCD area-detector
diffractometer
Bruker P4 with CCD area-detector
diffractometer
Bruker P4 with CCD area-detector
diffractometer
Bruker P4 with CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Multi-scan
(SADABS; Sheldrick, 1996)
Multi-scan
(SADABS; Sheldrick, 1996)
Multi-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.971, 0.9950.970, 0.9820.975, 0.9800.975, 0.992
No. of measured, independent and
observed [I > 2σ(I)] reflections
17999, 6045, 2878 10009, 3291, 1625 5487, 3520, 2421 13914, 5081, 4050
Rint0.0650.0530.0250.050
(sin θ/λ)max1)0.5960.5950.5950.667
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.051, 0.160, 0.99 0.057, 0.181, 1.01 0.054, 0.152, 1.03 0.056, 0.140, 1.09
No. of reflections6045329135205081
No. of parameters477267293300
H-atom treatmentH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.18, 0.170.24, 0.190.77, 0.270.40, 0.29


(V)
Crystal data
Chemical formulaC28H24F7NO3
Mr555.48
Crystal system, space groupTriclinic, P1
Temperature (K)90
a, b, c (Å)10.313 (1), 10.924 (1), 11.729 (1)
α, β, γ (°)87.67 (1), 82.65 (1), 73.24 (1)
V3)1254.8 (2)
Z2
Radiation typeMo Kα
µ (mm1)0.13
Crystal size (mm)0.21 × 0.15 × 0.08
Data collection
DiffractometerBruker P4 with CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.978, 0.990
No. of measured, independent and
observed [I > 2σ(I)] reflections
6916, 4383, 3293
Rint0.030
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.110, 1.03
No. of reflections4383
No. of parameters354
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.30, 0.24

Computer programs: Please provide missing details, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997).

A comparison of the geometry of compounds (I)-(V) (Å, °) top
(I)(II)(III)(IV)(V)
b-c1.381 (4)1.384 (5)1.389 (4)1.388 (3)1.395 (3)
c-d1.457 (4)1.469 (4)1.477 (4)1.469 (3)1.468 (3)
d-e1.354 (4)1.359 (4)1.373 (4)1.352 (3)1.359 (3)
e-f1.465 (5)1.463 (5)1.483 (4)1.481 (3)1.484 (3)
f-g1.357 (5)1.351 (5)1.356 (5)1.359 (3)1.355 (3)
b-c-d125.0 (3)125.6 (3)123.4 (3)124.80 (19)122.89 (19)
c-d-e123.4 (3)123.6 (3)121.7 (3)124.12 (18)122.26 (19)
d-e-f130.2 (3)130.3 (3)127.8 (3)129.65 (18)128.52 (19)
e-f-g130.5 (3)130.7 (3)130.8 (3)130.11 (18)129.95 (19)
a-b-c-d-4.5 (5)0.3 (6)-3.4 (5)2.3 (3)-2.7 (3)
b-c-d-e-51.5 (5)-54.5 (5)-52.8 (4)-57.6 (3)-54.4 (3)
c-d-e-f-9.9 (6)-4.2 (6)-12.3 (5)-6.0 (3)-11.6 (3)
d-e-f-g-41.1 (6)-43.8 (6)-39.1 (5)-45.9 (3)-49.8 (3)
e-f-g-h3.2 (6)-1.0 (6)-3.9 (5)-1.3 (3)3.1 (3)
Distances between bond-forming atoms (Å) and coloration quantum yields top
(I)(II)(III)(IV)(V)
b-g3.517 (5)3.517 (5)3.459 (4)3.625 (3)3.644 (3)
Φcoloration0.200.150.180.0510.040
 

Follow Acta Cryst. C
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds