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The title compound, C13H10FNO, which was synthesized from the reaction of tosyl­oxytropone and 4-fluoroaniline, has two independent mol­ecules of similar bond dimensions in the asymmetric unit. Adjacent mol­ecules are linked by hydrogen bonds and C—H...F inter­actions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807050271/ng2336sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807050271/ng2336Isup2.hkl
Contains datablock I

CCDC reference: 667383

Key indicators

  • Single-crystal X-ray study
  • T = 100 K
  • Mean [sigma](C-C) = 0.002 Å
  • R factor = 0.032
  • wR factor = 0.083
  • Data-to-parameter ratio = 14.2

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT480_ALERT_4_C Long H...A H-Bond Reported H45 .. F24 .. 2.72 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H23 .. F44 .. 2.57 Ang.
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 2 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

In the current paper the title compound, (I), is presented as an example of a product formed during the exchange reaction of tosyloxytropone and the corresponding 4-flouroaniline. The compound is the first of a series of halogenated derivatives of tropolone type molecules, see Fig. 1. Two closely related derivatives of N-alkyl (Roesky & Burgstein, 1999) and N-aryl (Hicks & Brookhart, 2001) have been reported. The addition of a halogen moiety to the compound can drastically affect the packing of the molecule in the solid state.

Two independent molecules are present in the asymmetric unit, with the only observable difference being the rotation of the phenyl moiety compared to the tropone molecule. This is clearly illustrated by the torsional twist of the C—N—C—C (see Table 1) and the interplanar dihedral angle formed by the phenyl and seven membered tropone ring systems of 46.04 (3) and 41.45 (4) °, respectively.

Weak intra- and intermolecular interactions is observed in the solid state, see Table 2. The weak intermolecular hydrogen bonds form dimeric systems in the solid state consisting of the two independent units. The flouro moieties do have a significant effect on the packing of the molecule in the solid state, with C—F···H interactions being observed.

Related literature top

For general background, see: Hicks & Brookhart (2001); Kubo et al. (2005, 2006); Polonsky et al. (1981); Roesky & Burgstein (1999); Yamamoto et al. (2001). For related diketonato complexes, see: Janse van Rensburg & Roodt (2006); Janse van Rensburg et al. (2006).

Experimental top

The title compound was obtained during the coupling tosyloxytropone and 4-flouroaniline in a 1:1 ration in toluene. On evaporation of the solvent; crystals suitable for X-Ray crystallography was obtained.

Refinement top

H atoms were positioned geometrically and refined using a riding model, with C—H = 0.95 Å and with Uiso(H) = 1.2 times Ueq(C aromatic).

Structure description top

In the current paper the title compound, (I), is presented as an example of a product formed during the exchange reaction of tosyloxytropone and the corresponding 4-flouroaniline. The compound is the first of a series of halogenated derivatives of tropolone type molecules, see Fig. 1. Two closely related derivatives of N-alkyl (Roesky & Burgstein, 1999) and N-aryl (Hicks & Brookhart, 2001) have been reported. The addition of a halogen moiety to the compound can drastically affect the packing of the molecule in the solid state.

Two independent molecules are present in the asymmetric unit, with the only observable difference being the rotation of the phenyl moiety compared to the tropone molecule. This is clearly illustrated by the torsional twist of the C—N—C—C (see Table 1) and the interplanar dihedral angle formed by the phenyl and seven membered tropone ring systems of 46.04 (3) and 41.45 (4) °, respectively.

Weak intra- and intermolecular interactions is observed in the solid state, see Table 2. The weak intermolecular hydrogen bonds form dimeric systems in the solid state consisting of the two independent units. The flouro moieties do have a significant effect on the packing of the molecule in the solid state, with C—F···H interactions being observed.

For general background, see: Hicks & Brookhart (2001); Kubo et al. (2005, 2006); Polonsky et al. (1981); Roesky & Burgstein (1999); Yamamoto et al. (2001). For related diketonato complexes, see: Janse van Rensburg & Roodt (2006); Janse van Rensburg et al. (2006).

Computing details top

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus (Bruker, 2004) and XPREP (Bruker, 2004); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg & Putz, 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1] Fig. 1. : Representation of the title compound (I), showing the numbering scheme and displacement ellipsoids (50% probability).
2-(4-Flouroanilino)tropone top
Crystal data top
C13H10FNOF(000) = 896
Mr = 215.22Dx = 1.353 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 9979 reflections
a = 9.9075 (3) Åθ = 2.4–28.3°
b = 17.5746 (5) ŵ = 0.10 mm1
c = 12.2212 (4) ÅT = 100 K
β = 96.714 (1)°Cuboid, yellow
V = 2113.37 (11) Å30.19 × 0.18 × 0.18 mm
Z = 8
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
4116 independent reflections
Radiation source: fine-focus sealed tube3581 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.026
Detector resolution: 512 pixels mm-1θmax = 26.0°, θmin = 2.0°
φ and ω scansh = 1212
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
k = 2021
Tmin = 0.982, Tmax = 0.983l = 1414
37801 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)] = 0.032Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.083H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0338P)2 + 0.8256P]
where P = (Fo2 + 2Fc2)/3
4116 reflections(Δ/σ)max = 0.001
289 parametersΔρmax = 0.20 e Å3
0 restraintsΔρmin = 0.20 e Å3
Crystal data top
C13H10FNOV = 2113.37 (11) Å3
Mr = 215.22Z = 8
Monoclinic, P21/nMo Kα radiation
a = 9.9075 (3) ŵ = 0.10 mm1
b = 17.5746 (5) ÅT = 100 K
c = 12.2212 (4) Å0.19 × 0.18 × 0.18 mm
β = 96.714 (1)°
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
4116 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 1998)
3581 reflections with I > 2σ(I)
Tmin = 0.982, Tmax = 0.983Rint = 0.026
37801 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0320 restraints
wR(F2) = 0.083H-atom parameters constrained
S = 1.05Δρmax = 0.20 e Å3
4116 reflectionsΔρmin = 0.20 e Å3
289 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
F240.33924 (10)0.60818 (5)0.00722 (6)0.0470 (2)
F440.09980 (9)0.38655 (5)0.11523 (7)0.0468 (2)
O310.32909 (8)0.31212 (5)0.52144 (7)0.0265 (2)
O110.50514 (8)0.63320 (5)0.65968 (7)0.0294 (2)
N320.20137 (9)0.33470 (6)0.33231 (8)0.0213 (2)
H320.28740.34230.35690.018*
N120.42537 (10)0.59783 (6)0.46111 (8)0.0221 (2)
H120.50130.62020.48870.019*
C210.39972 (12)0.59728 (6)0.34498 (10)0.0210 (2)
C460.23044 (12)0.40892 (7)0.17152 (10)0.0256 (3)
H460.29020.44120.21680.031*
C410.16614 (11)0.34861 (7)0.21878 (10)0.0208 (2)
C260.50927 (12)0.59112 (7)0.28413 (10)0.0240 (3)
H260.59820.58390.32100.029*
C420.07791 (11)0.30169 (7)0.15148 (10)0.0225 (3)
H420.03400.26040.18300.027*
C110.39801 (11)0.59507 (7)0.64867 (10)0.0214 (2)
C220.26927 (12)0.60873 (7)0.29035 (10)0.0250 (3)
H220.19410.61370.33150.030*
C150.13306 (12)0.49457 (7)0.67800 (10)0.0260 (3)
H150.05930.46830.70390.031*
C130.24472 (12)0.51698 (7)0.50645 (10)0.0218 (2)
H130.23530.50170.43140.026*
C310.20423 (12)0.29945 (6)0.51716 (10)0.0222 (3)
C320.12203 (11)0.31135 (6)0.40904 (10)0.0207 (2)
C440.12025 (13)0.37460 (8)0.00410 (11)0.0307 (3)
C140.15145 (12)0.48383 (7)0.56961 (10)0.0236 (3)
H140.09120.44820.53130.028*
C160.21218 (12)0.54045 (7)0.75443 (10)0.0252 (3)
H160.18210.54310.82540.030*
C170.32642 (12)0.58199 (7)0.74198 (10)0.0237 (3)
H170.36520.60670.80740.028*
C250.48976 (14)0.59541 (7)0.17019 (11)0.0296 (3)
H250.56430.59130.12820.035*
C120.34890 (11)0.56856 (6)0.53560 (9)0.0200 (2)
C230.24943 (14)0.61280 (7)0.17668 (11)0.0301 (3)
H230.16100.62040.13900.036*
C340.11526 (12)0.27952 (7)0.45227 (11)0.0290 (3)
H340.20570.27740.41660.035*
C370.14884 (13)0.27657 (7)0.61475 (11)0.0292 (3)
H370.21360.27400.67840.035*
C430.05403 (12)0.31496 (7)0.03915 (10)0.0272 (3)
H430.00660.28360.00690.033*
C240.35972 (15)0.60573 (7)0.11933 (10)0.0310 (3)
C450.20782 (13)0.42200 (7)0.05935 (11)0.0309 (3)
H450.25180.46280.02680.037*
C350.10052 (13)0.25745 (7)0.56042 (12)0.0320 (3)
H350.18020.24010.58900.038*
C330.01810 (12)0.30469 (7)0.38593 (11)0.0242 (3)
H330.05380.31960.31360.029*
C360.01932 (14)0.25768 (7)0.63340 (12)0.0327 (3)
H360.00940.24250.70660.039*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F240.0714 (6)0.0513 (5)0.0165 (4)0.0117 (5)0.0026 (4)0.0076 (3)
F440.0561 (5)0.0553 (6)0.0255 (5)0.0206 (4)0.0100 (4)0.0137 (4)
O310.0221 (4)0.0298 (5)0.0274 (5)0.0002 (3)0.0023 (3)0.0019 (4)
O110.0238 (4)0.0413 (5)0.0232 (5)0.0093 (4)0.0032 (3)0.0070 (4)
N320.0170 (5)0.0237 (5)0.0233 (5)0.0024 (4)0.0026 (4)0.0001 (4)
N120.0195 (5)0.0287 (5)0.0178 (5)0.0012 (4)0.0005 (4)0.0028 (4)
C210.0264 (6)0.0172 (6)0.0188 (6)0.0018 (4)0.0007 (5)0.0002 (4)
C460.0262 (6)0.0231 (6)0.0271 (7)0.0047 (5)0.0015 (5)0.0001 (5)
C410.0181 (5)0.0209 (6)0.0237 (6)0.0023 (4)0.0029 (4)0.0011 (5)
C260.0278 (6)0.0216 (6)0.0226 (7)0.0030 (5)0.0031 (5)0.0010 (5)
C420.0180 (5)0.0213 (6)0.0282 (7)0.0003 (4)0.0035 (5)0.0019 (5)
C110.0203 (6)0.0225 (6)0.0208 (6)0.0016 (5)0.0004 (4)0.0020 (4)
C220.0263 (6)0.0223 (6)0.0257 (7)0.0025 (5)0.0000 (5)0.0002 (5)
C150.0222 (6)0.0253 (6)0.0302 (7)0.0018 (5)0.0019 (5)0.0057 (5)
C130.0234 (6)0.0211 (6)0.0199 (6)0.0037 (5)0.0021 (5)0.0018 (4)
C310.0241 (6)0.0161 (6)0.0271 (7)0.0030 (4)0.0059 (5)0.0002 (4)
C320.0225 (6)0.0146 (5)0.0261 (6)0.0016 (4)0.0072 (5)0.0004 (4)
C440.0330 (7)0.0353 (7)0.0218 (7)0.0042 (6)0.0044 (5)0.0080 (5)
C140.0209 (6)0.0186 (6)0.0297 (7)0.0015 (4)0.0044 (5)0.0012 (5)
C160.0268 (6)0.0272 (6)0.0220 (6)0.0012 (5)0.0050 (5)0.0031 (5)
C170.0266 (6)0.0252 (6)0.0190 (6)0.0000 (5)0.0016 (5)0.0018 (5)
C250.0411 (7)0.0261 (7)0.0230 (7)0.0010 (5)0.0101 (5)0.0006 (5)
C120.0192 (5)0.0209 (6)0.0196 (6)0.0056 (4)0.0010 (4)0.0002 (4)
C230.0354 (7)0.0254 (6)0.0265 (7)0.0003 (5)0.0087 (5)0.0042 (5)
C340.0216 (6)0.0251 (6)0.0419 (8)0.0019 (5)0.0107 (5)0.0026 (5)
C370.0326 (7)0.0276 (7)0.0280 (7)0.0057 (5)0.0068 (5)0.0067 (5)
C430.0230 (6)0.0290 (6)0.0281 (7)0.0041 (5)0.0034 (5)0.0009 (5)
C240.0512 (8)0.0248 (6)0.0157 (6)0.0043 (6)0.0019 (6)0.0036 (5)
C450.0343 (7)0.0271 (7)0.0306 (7)0.0078 (5)0.0007 (5)0.0078 (5)
C350.0285 (6)0.0276 (7)0.0435 (8)0.0010 (5)0.0190 (6)0.0026 (6)
C330.0222 (6)0.0217 (6)0.0293 (7)0.0031 (5)0.0059 (5)0.0002 (5)
C360.0398 (7)0.0273 (7)0.0343 (8)0.0060 (6)0.0179 (6)0.0081 (5)
Geometric parameters (Å, º) top
F24—C241.3621 (15)C13—C121.3886 (16)
F44—C441.3658 (15)C13—C141.3985 (17)
O11—C111.2491 (14)C13—H130.9500
N12—C121.3522 (15)C31—C371.4277 (17)
N12—C211.4124 (15)C31—C321.4837 (17)
O31—C311.2520 (14)C32—C331.3890 (16)
N32—C321.3558 (15)C44—C431.3746 (18)
N32—C411.4118 (15)C44—C451.3750 (18)
N32—H320.8800C14—H140.9500
N12—H120.8800C16—C171.3702 (17)
C21—C261.3898 (17)C16—H160.9500
C21—C221.3982 (16)C17—H170.9500
C46—C451.3821 (18)C25—C241.375 (2)
C46—C411.3961 (16)C25—H250.9500
C46—H460.9500C23—C241.371 (2)
C41—C421.3973 (16)C23—H230.9500
C26—C251.3853 (18)C34—C351.3689 (19)
C26—H260.9500C34—C331.4007 (17)
C42—C431.3852 (18)C34—H340.9500
C42—H420.9500C37—C361.3701 (18)
C11—C171.4302 (17)C37—H370.9500
C11—C121.4853 (16)C43—H430.9500
C22—C231.3819 (18)C45—H450.9500
C22—H220.9500C35—C361.399 (2)
C15—C141.3712 (18)C35—H350.9500
C15—C161.4020 (18)C33—H330.9500
C15—H150.9500C36—H360.9500
C12—N12—C21128.67 (10)C15—C14—C13130.31 (11)
C32—N32—C41129.45 (10)C15—C14—H14114.8
C32—N32—H32115.3C13—C14—H14114.8
C41—N32—H32115.3C17—C16—C15129.59 (12)
C12—N12—H12115.7C17—C16—H16115.2
C21—N12—H12115.7C15—C16—H16115.2
C26—C21—C22119.46 (11)C16—C17—C11131.85 (11)
C26—C21—N12118.57 (10)C16—C17—H17114.1
C22—C21—N12121.77 (11)C11—C17—H17114.1
C45—C46—C41120.51 (11)C24—C25—C26118.34 (12)
C45—C46—H46119.7C24—C25—H25120.8
C41—C46—H46119.7C26—C25—H25120.8
C46—C41—C42119.26 (11)N12—C12—C13122.26 (11)
C46—C41—N32117.76 (10)N12—C12—C11111.02 (10)
C42—C41—N32122.83 (10)C13—C12—C11126.60 (11)
C25—C26—C21120.51 (12)C24—C23—C22118.75 (12)
C25—C26—H26119.7C24—C23—H23120.6
C21—C26—H26119.7C22—C23—H23120.6
C43—C42—C41120.44 (11)C35—C34—C33130.19 (12)
C43—C42—H42119.8C35—C34—H34114.9
C41—C42—H42119.8C33—C34—H34114.9
O11—C11—C17119.65 (11)C36—C37—C31131.77 (13)
O11—C11—C12116.76 (10)C36—C37—H37114.1
C17—C11—C12123.53 (10)C31—C37—H37114.1
C23—C22—C21120.15 (12)C44—C43—C42118.39 (11)
C23—C22—H22119.9C44—C43—H43120.8
C21—C22—H22119.9C42—C43—H43120.8
C14—C15—C16126.56 (11)F24—C24—C23118.52 (12)
C14—C15—H15116.7F24—C24—C25118.70 (12)
C16—C15—H15116.7C23—C24—C25122.78 (12)
C12—C13—C14130.51 (11)C44—C45—C46118.49 (12)
C12—C13—H13114.7C44—C45—H45120.8
C14—C13—H13114.7C46—C45—H45120.8
O31—C31—C37119.31 (11)C34—C35—C36126.98 (12)
O31—C31—C32116.68 (10)C34—C35—H35116.5
C37—C31—C32123.99 (11)C36—C35—H35116.5
N32—C32—C33122.10 (11)C32—C33—C34130.33 (12)
N32—C32—C31110.88 (10)C32—C33—H33114.8
C33—C32—C31126.92 (11)C34—C33—H33114.8
F44—C44—C43118.53 (11)C37—C36—C35129.50 (13)
F44—C44—C45118.56 (11)C37—C36—H36115.2
C43—C44—C45122.90 (12)C35—C36—H36115.2
C12—N12—C21—C26145.61 (12)C21—N12—C12—C11168.38 (10)
C12—N12—C21—C2239.51 (17)C14—C13—C12—N12176.39 (11)
C45—C46—C41—C420.32 (18)C14—C13—C12—C117.9 (2)
C45—C46—C41—N32175.26 (11)O11—C11—C12—N125.99 (15)
C32—N32—C41—C46143.54 (12)C17—C11—C12—N12171.17 (11)
C32—N32—C41—C4241.05 (18)O11—C11—C12—C13170.11 (11)
C22—C21—C26—C250.71 (18)C17—C11—C12—C1312.73 (18)
N12—C21—C26—C25175.71 (11)C21—C22—C23—C240.27 (18)
C46—C41—C42—C430.23 (17)O31—C31—C37—C36178.35 (13)
N32—C41—C42—C43175.56 (11)C32—C31—C37—C363.2 (2)
C26—C21—C22—C230.91 (18)F44—C44—C43—C42178.23 (11)
N12—C21—C22—C23175.74 (11)C45—C44—C43—C420.7 (2)
C41—N32—C32—C336.94 (18)C41—C42—C43—C440.72 (18)
C41—N32—C32—C31176.37 (10)C22—C23—C24—F24178.64 (11)
O31—C31—C32—N320.01 (14)C22—C23—C24—C250.6 (2)
C37—C31—C32—N32178.46 (11)C26—C25—C24—F24178.45 (11)
O31—C31—C32—C33176.51 (11)C26—C25—C24—C230.79 (19)
C37—C31—C32—C331.97 (19)F44—C44—C45—C46178.76 (12)
C16—C15—C14—C133.7 (2)C43—C44—C45—C460.2 (2)
C12—C13—C14—C152.4 (2)C41—C46—C45—C440.3 (2)
C14—C15—C16—C172.9 (2)C33—C34—C35—C362.6 (2)
C15—C16—C17—C113.2 (2)N32—C32—C33—C34177.67 (12)
O11—C11—C17—C16176.82 (13)C31—C32—C33—C346.2 (2)
C12—C11—C17—C166.1 (2)C35—C34—C33—C323.3 (2)
C21—C26—C25—C240.12 (18)C31—C37—C36—C352.1 (2)
C21—N12—C12—C1315.32 (18)C34—C35—C36—C372.7 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N12—H12···O31i0.882.072.8891 (13)154
N32—H32···O11i0.882.132.9524 (12)155
C45—H45···F240.952.723.6058 (15)156
C23—H23···F44ii0.952.573.4538 (16)155
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y+1, z.

Experimental details

Crystal data
Chemical formulaC13H10FNO
Mr215.22
Crystal system, space groupMonoclinic, P21/n
Temperature (K)100
a, b, c (Å)9.9075 (3), 17.5746 (5), 12.2212 (4)
β (°) 96.714 (1)
V3)2113.37 (11)
Z8
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.19 × 0.18 × 0.18
Data collection
DiffractometerBruker SMART 1K CCD area-detector
Absorption correctionMulti-scan
(SADABS; Bruker, 1998)
Tmin, Tmax0.982, 0.983
No. of measured, independent and
observed [I > 2σ(I)] reflections
37801, 4116, 3581
Rint0.026
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.032, 0.083, 1.05
No. of reflections4116
No. of parameters289
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.20, 0.20

Computer programs: APEX2 (Bruker, 2005), SAINT-Plus (Bruker, 2004) and XPREP (Bruker, 2004), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), DIAMOND (Brandenburg & Putz, 2006).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N12—H12···O31i0.882.072.8891 (13)153.6
N32—H32···O11i0.882.132.9524 (12)154.7
C45—H45···F240.952.723.6058 (15)156.0
C23—H23···F44ii0.952.573.4538 (16)155.0
Symmetry codes: (i) x+1, y+1, z+1; (ii) x, y+1, z.
 

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