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The cooperative roles of various structural motifs associated with the presence of different intermolecular interactions in the formation of molecular crystals are investigated in a series of tri­fluoro­methyl­ated phenyl­hydrazones. Out of the six compounds analysed, two exhibit three-dimensional structural similarities with geometrically equivalent building blocks, while a third exists as two polymorphic forms crystallized from ethanol solutions at low temperature (277 K) and room temperature (298 K), respectively. The compounds were characterized via single-crystal and powder X-ray diffraction techniques and differential scanning calorimetry. In the absence of any strong hydrogen bonding, the supramolecular constructs are primarily stabilized via molecular pairs with a high dispersion-energy contribution, due to the presence of molecular stacking along the molecular backbone along with C—H...π interactions in the solid state, in preference to an electrostatic contribution. The interaction energies for the most stabilizing molecular building blocks are in the range −29 to −43 kJ mol−1. In addition, weak N—H...F, C—H...F and N—H...C interactions and F...F, F...C, F...N and C...N contacts act as secondary motifs, providing additional stability to the crystal packing. The overall molecular arrangements are carefully analysed in terms of their nature and energetics, and the roles of different molecular pairs towards the crystal structure are delineated. A topological study using the quantum theory of atoms in molecules was used to characterize all the atomic interactions in the solid state. It established the presence of (3, −1) bond critical points and the closed-shell nature of all the interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520617006643/ao5033sup1.cif
Contains datablocks HT03, HT11, HT13, HT20, HT31, HT33C, HT33P

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT03sup2.hkl
Contains datablock HT03

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT11sup3.hkl
Contains datablock HT11

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT13sup4.hkl
Contains datablock HT13

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT20sup5.hkl
Contains datablock HT20

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT31sup6.hkl
Contains datablock HT31

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT33Csup7.hkl
Contains datablock HT33C

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520617006643/ao5033HT33Psup8.hkl
Contains datablock HT33P

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520617006643/ao5033sup9.pdf
Additional tables and figures

CCDC references: 1524421; 1524423; 1524425; 1547660; 1547661; 1547662; 1547663

Computing details top

Program(s) used to refine structure: SHELXL2016/6 (Sheldrick, 2016) for HT03, HT33C, HT33P; SHELXL2014/7 (Sheldrick, 2014) for HT11, HT13, HT20, HT31.

(HT03) top
Crystal data top
C14H11F3N2Z = 4
Mr = 264.25F(000) = 544
Triclinic, P1Dx = 1.425 Mg m3
a = 9.6399 (12) ÅMo Kα radiation, λ = 0.71073 Å
b = 10.3142 (14) ÅCell parameters from 9812 reflections
c = 13.4202 (18) Åθ = 2.3–30.9°
α = 99.961 (4)°µ = 0.12 mm1
β = 107.306 (4)°T = 100 K
γ = 97.321 (4)°Plate, colorless
V = 1231.8 (3) Å30.23 × 0.16 × 0.14 mm
Data collection top
Bruker APEX-II CCD
diffractometer
4928 reflections with I > 2σ(I)
φ and ω scansRint = 0.055
Absorption correction: multi-scan
SADABS
θmax = 28.4°, θmin = 2.3°
Tmin = 0.703, Tmax = 0.737h = 1212
30881 measured reflectionsk = 1313
6111 independent reflectionsl = 1717
Refinement top
Refinement on F2548 restraints
Least-squares matrix: fullHydrogen site location: mixed
R[F2 > 2σ(F2)] = 0.048H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.124 w = 1/[σ2(Fo2) + (0.055P)2 + 0.6217P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
6111 reflectionsΔρmax = 0.44 e Å3
405 parametersΔρmin = 0.33 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N10.23936 (13)0.62820 (11)0.54396 (9)0.0167 (2)
H10.2395 (18)0.5622 (15)0.5750 (13)0.020*
N20.16039 (12)0.60842 (11)0.43844 (9)0.0150 (2)
C10.33177 (14)0.75036 (13)0.59865 (10)0.0146 (3)
C20.42060 (14)0.76117 (13)0.70445 (11)0.0158 (3)
H20.4139820.6869680.7371310.019*
C30.51780 (15)0.87919 (13)0.76154 (11)0.0169 (3)
H3A0.5781210.8859020.8332340.020*
C40.52747 (15)0.98833 (13)0.71413 (11)0.0176 (3)
C50.43638 (15)0.97912 (13)0.60999 (11)0.0185 (3)
H50.4411091.0546110.5785510.022*
C60.33865 (15)0.86086 (13)0.55151 (11)0.0168 (3)
H60.2771340.8550110.4802890.020*
C70.01590 (14)0.46567 (13)0.28024 (10)0.0149 (3)
C80.11617 (15)0.34381 (13)0.23482 (11)0.0167 (3)
H80.1259670.2814260.2778750.020*
C90.20148 (15)0.31347 (14)0.12722 (12)0.0206 (3)
H90.2701560.2310600.0972390.025*
C100.18654 (17)0.40317 (15)0.06361 (12)0.0233 (3)
H100.2445070.3821830.0100310.028*
C110.08605 (17)0.52454 (14)0.10800 (12)0.0223 (3)
H110.0752660.5857360.0642120.027*
C120.00211 (15)0.55618 (13)0.21538 (11)0.0179 (3)
H120.0650510.6394640.2452440.021*
C130.07305 (14)0.49443 (13)0.39366 (10)0.0148 (3)
H130.0662500.4285990.4343840.018*
C140.63196 (17)1.11600 (15)0.77569 (12)0.0239 (3)
F1A0.7513 (12)1.0972 (13)0.8470 (10)0.062 (2)0.52 (3)
F2A0.6828 (8)1.1842 (7)0.7131 (5)0.0326 (13)0.52 (3)
F3A0.5726 (9)1.2001 (8)0.8287 (9)0.0603 (19)0.52 (3)
F1B0.7327 (14)1.1018 (12)0.8623 (9)0.059 (2)0.48 (3)
F2B0.7044 (14)1.1698 (11)0.7195 (8)0.071 (2)0.48 (3)
F3B0.5636 (9)1.2113 (7)0.8104 (7)0.0412 (14)0.48 (3)
N30.34435 (13)0.46537 (12)0.24783 (10)0.0209 (3)
H30.2836 (18)0.4659 (18)0.2838 (13)0.025*
N40.48449 (13)0.53773 (11)0.29437 (9)0.0177 (2)
C150.30515 (15)0.37512 (13)0.15058 (11)0.0164 (3)
C160.17094 (15)0.28393 (14)0.11733 (11)0.0183 (3)
H160.1085630.2869050.1604280.022*
C170.12891 (15)0.18950 (13)0.02187 (11)0.0189 (3)
H170.0373740.1282040.0007570.023*
C180.22011 (16)0.18417 (14)0.04081 (11)0.0199 (3)
C190.35307 (16)0.27573 (14)0.00898 (11)0.0201 (3)
H190.4147020.2724730.0526320.024*
C200.39576 (15)0.37159 (14)0.08619 (11)0.0183 (3)
H200.4859600.4344520.1075010.022*
C210.66223 (15)0.69155 (13)0.44605 (11)0.0171 (3)
C220.69568 (16)0.75596 (14)0.55336 (11)0.0194 (3)
H220.6246540.7425380.5885870.023*
C230.83248 (16)0.83967 (14)0.60895 (12)0.0218 (3)
H230.8541270.8837510.6816070.026*
C240.93690 (16)0.85853 (14)0.55810 (12)0.0220 (3)
H241.0302840.9153820.5959410.026*
C250.90481 (16)0.79407 (14)0.45147 (12)0.0202 (3)
H250.9767720.8068200.4169280.024*
C260.76847 (15)0.71136 (13)0.39536 (11)0.0181 (3)
H260.7471570.6681580.3225300.022*
C270.51562 (15)0.60782 (14)0.38946 (11)0.0184 (3)
H270.4425200.6054700.4238100.022*
C280.17097 (19)0.08438 (16)0.14493 (13)0.0292 (3)
F4A0.0779 (8)0.0231 (7)0.1451 (8)0.0322 (12)0.509 (19)
F5A0.1186 (19)0.1286 (7)0.2270 (5)0.083 (3)0.509 (19)
F6A0.2884 (6)0.0254 (6)0.1564 (9)0.0600 (19)0.509 (19)
F4B0.1032 (13)0.0328 (8)0.1446 (9)0.051 (2)0.491 (19)
F5B0.0608 (6)0.1258 (6)0.2210 (5)0.0393 (12)0.491 (19)
F6B0.2697 (5)0.0756 (13)0.1940 (6)0.065 (3)0.491 (19)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0192 (6)0.0140 (5)0.0137 (5)0.0004 (4)0.0015 (5)0.0038 (4)
N20.0140 (5)0.0168 (5)0.0130 (5)0.0022 (4)0.0038 (4)0.0018 (4)
C10.0118 (6)0.0162 (6)0.0156 (6)0.0023 (5)0.0054 (5)0.0014 (5)
C20.0151 (6)0.0172 (6)0.0165 (6)0.0040 (5)0.0061 (5)0.0050 (5)
C30.0149 (6)0.0205 (6)0.0139 (6)0.0039 (5)0.0038 (5)0.0013 (5)
C40.0157 (6)0.0159 (6)0.0186 (7)0.0009 (5)0.0057 (5)0.0009 (5)
C50.0209 (7)0.0148 (6)0.0200 (7)0.0026 (5)0.0073 (6)0.0043 (5)
C60.0172 (7)0.0177 (6)0.0152 (6)0.0038 (5)0.0045 (5)0.0035 (5)
C70.0136 (6)0.0155 (6)0.0153 (6)0.0036 (5)0.0054 (5)0.0013 (5)
C80.0155 (6)0.0161 (6)0.0186 (7)0.0022 (5)0.0067 (5)0.0025 (5)
C90.0168 (7)0.0188 (6)0.0214 (7)0.0002 (5)0.0038 (6)0.0018 (5)
C100.0230 (7)0.0246 (7)0.0167 (7)0.0071 (6)0.0006 (6)0.0007 (6)
C110.0276 (8)0.0198 (7)0.0197 (7)0.0069 (6)0.0054 (6)0.0071 (5)
C120.0189 (7)0.0141 (6)0.0186 (7)0.0021 (5)0.0044 (5)0.0018 (5)
C130.0140 (6)0.0155 (6)0.0161 (6)0.0037 (5)0.0063 (5)0.0037 (5)
C140.0247 (8)0.0203 (7)0.0211 (7)0.0022 (6)0.0050 (6)0.0008 (6)
F1A0.031 (2)0.041 (3)0.081 (5)0.0117 (17)0.026 (3)0.019 (4)
F2A0.040 (2)0.0220 (17)0.0269 (19)0.0106 (15)0.0050 (15)0.0058 (14)
F3A0.052 (3)0.044 (3)0.072 (4)0.025 (2)0.045 (3)0.039 (2)
F1B0.070 (5)0.024 (2)0.039 (2)0.014 (3)0.034 (3)0.0036 (15)
F2B0.069 (4)0.068 (4)0.057 (4)0.049 (3)0.042 (3)0.024 (3)
F3B0.051 (3)0.0140 (17)0.050 (2)0.0083 (17)0.008 (2)0.0029 (18)
N30.0138 (6)0.0259 (6)0.0194 (6)0.0004 (5)0.0063 (5)0.0029 (5)
N40.0143 (5)0.0175 (5)0.0184 (6)0.0022 (4)0.0028 (4)0.0011 (4)
C150.0170 (6)0.0166 (6)0.0143 (6)0.0054 (5)0.0030 (5)0.0020 (5)
C160.0167 (7)0.0194 (6)0.0187 (7)0.0038 (5)0.0061 (5)0.0032 (5)
C170.0170 (7)0.0164 (6)0.0208 (7)0.0018 (5)0.0040 (5)0.0028 (5)
C180.0225 (7)0.0179 (6)0.0169 (6)0.0043 (5)0.0041 (6)0.0010 (5)
C190.0207 (7)0.0228 (7)0.0181 (7)0.0059 (5)0.0083 (6)0.0036 (5)
C200.0157 (6)0.0198 (6)0.0182 (7)0.0022 (5)0.0040 (5)0.0044 (5)
C210.0170 (7)0.0150 (6)0.0189 (7)0.0056 (5)0.0043 (5)0.0032 (5)
C220.0186 (7)0.0206 (6)0.0192 (7)0.0053 (5)0.0072 (5)0.0021 (5)
C230.0230 (7)0.0193 (7)0.0185 (7)0.0041 (5)0.0029 (6)0.0012 (5)
C240.0195 (7)0.0159 (6)0.0251 (7)0.0003 (5)0.0010 (6)0.0037 (5)
C250.0187 (7)0.0186 (6)0.0242 (7)0.0028 (5)0.0073 (6)0.0073 (5)
C260.0209 (7)0.0167 (6)0.0168 (6)0.0047 (5)0.0061 (5)0.0031 (5)
C270.0160 (7)0.0196 (6)0.0189 (7)0.0044 (5)0.0058 (5)0.0016 (5)
C280.0346 (9)0.0249 (7)0.0245 (8)0.0015 (6)0.0129 (7)0.0044 (6)
F4A0.0323 (18)0.029 (3)0.026 (2)0.0080 (15)0.0092 (13)0.0101 (18)
F5A0.184 (8)0.0357 (17)0.0163 (15)0.003 (4)0.022 (3)0.0047 (12)
F6A0.0490 (19)0.044 (2)0.079 (4)0.0083 (15)0.044 (2)0.034 (2)
F4B0.095 (6)0.0132 (16)0.032 (2)0.002 (2)0.006 (3)0.0010 (14)
F5B0.060 (3)0.0294 (15)0.0146 (17)0.0110 (15)0.0056 (14)0.0013 (12)
F6B0.0395 (18)0.086 (5)0.049 (3)0.013 (2)0.0248 (18)0.042 (3)
Geometric parameters (Å, º) top
N1—N21.3586 (16)N3—N41.3609 (16)
N1—C11.3873 (17)N3—C151.3817 (18)
N1—H10.857 (13)N3—H30.863 (14)
N2—C131.2862 (17)N4—C271.2802 (18)
C1—C61.3996 (18)C15—C201.399 (2)
C1—C21.3998 (18)C15—C161.3996 (19)
C2—C31.3806 (19)C16—C171.3831 (19)
C2—H20.9500C16—H160.9500
C3—C41.3918 (19)C17—C181.386 (2)
C3—H3A0.9500C17—H170.9500
C4—C51.3914 (19)C18—C191.394 (2)
C4—C141.4905 (19)C18—C281.490 (2)
C5—C61.3883 (19)C19—C201.387 (2)
C5—H50.9500C19—H190.9500
C6—H60.9500C20—H200.9500
C7—C81.4001 (18)C21—C221.3991 (19)
C7—C121.4017 (19)C21—C261.401 (2)
C7—C131.4638 (18)C21—C271.4640 (19)
C8—C91.3896 (19)C22—C231.394 (2)
C8—H80.9500C22—H220.9500
C9—C101.385 (2)C23—C241.386 (2)
C9—H90.9500C23—H230.9500
C10—C111.396 (2)C24—C251.393 (2)
C10—H100.9500C24—H240.9500
C11—C121.384 (2)C25—C261.388 (2)
C11—H110.9500C25—H250.9500
C12—H120.9500C26—H260.9500
C13—H130.9500C27—H270.9500
C14—F2B1.313 (7)C28—F5A1.256 (6)
C14—F1B1.319 (7)C28—F4B1.300 (7)
C14—F3A1.320 (6)C28—F6B1.313 (4)
C14—F1A1.321 (7)C28—F4A1.334 (6)
C14—F2A1.343 (5)C28—F6A1.386 (5)
C14—F3B1.344 (6)C28—F5B1.405 (5)
N2—N1—C1120.38 (11)N4—N3—C15120.71 (12)
N2—N1—H1119.6 (11)N4—N3—H3119.5 (12)
C1—N1—H1119.7 (11)C15—N3—H3119.0 (12)
C13—N2—N1117.10 (11)C27—N4—N3116.51 (12)
N1—C1—C6122.28 (12)N3—C15—C20122.13 (12)
N1—C1—C2117.89 (12)N3—C15—C16118.11 (12)
C6—C1—C2119.82 (12)C20—C15—C16119.75 (12)
C3—C2—C1120.30 (12)C17—C16—C15120.15 (13)
C3—C2—H2119.8C17—C16—H16119.9
C1—C2—H2119.8C15—C16—H16119.9
C2—C3—C4120.05 (12)C16—C17—C18120.10 (13)
C2—C3—H3A120.0C16—C17—H17120.0
C4—C3—H3A120.0C18—C17—H17120.0
C5—C4—C3119.77 (12)C17—C18—C19120.12 (13)
C5—C4—C14120.04 (12)C17—C18—C28119.33 (13)
C3—C4—C14120.16 (13)C19—C18—C28120.48 (13)
C6—C5—C4120.76 (12)C20—C19—C18120.26 (13)
C6—C5—H5119.6C20—C19—H19119.9
C4—C5—H5119.6C18—C19—H19119.9
C5—C6—C1119.25 (12)C19—C20—C15119.60 (13)
C5—C6—H6120.4C19—C20—H20120.2
C1—C6—H6120.4C15—C20—H20120.2
C8—C7—C12119.02 (12)C22—C21—C26119.16 (13)
C8—C7—C13119.21 (12)C22—C21—C27118.82 (13)
C12—C7—C13121.77 (12)C26—C21—C27122.01 (13)
C9—C8—C7120.48 (13)C23—C22—C21120.47 (13)
C9—C8—H8119.8C23—C22—H22119.8
C7—C8—H8119.8C21—C22—H22119.8
C10—C9—C8120.11 (13)C24—C23—C22119.93 (13)
C10—C9—H9119.9C24—C23—H23120.0
C8—C9—H9119.9C22—C23—H23120.0
C9—C10—C11119.83 (13)C23—C24—C25119.95 (13)
C9—C10—H10120.1C23—C24—H24120.0
C11—C10—H10120.1C25—C24—H24120.0
C12—C11—C10120.38 (13)C26—C25—C24120.46 (14)
C12—C11—H11119.8C26—C25—H25119.8
C10—C11—H11119.8C24—C25—H25119.8
C11—C12—C7120.18 (13)C25—C26—C21120.03 (13)
C11—C12—H12119.9C25—C26—H26120.0
C7—C12—H12119.9C21—C26—H26120.0
N2—C13—C7120.32 (12)N4—C27—C21120.97 (13)
N2—C13—H13119.8N4—C27—H27119.5
C7—C13—H13119.8C21—C27—H27119.5
F2B—C14—F1B106.4 (7)F4B—C28—F6B112.1 (5)
F3A—C14—F1A106.2 (7)F5A—C28—F4A110.1 (7)
F3A—C14—F2A105.7 (5)F5A—C28—F6A108.0 (4)
F1A—C14—F2A105.2 (7)F4A—C28—F6A100.0 (4)
F2B—C14—F3B105.4 (6)F4B—C28—F5B101.5 (5)
F1B—C14—F3B105.3 (7)F6B—C28—F5B100.3 (5)
F2B—C14—C4113.2 (4)F5A—C28—C18116.0 (4)
F1B—C14—C4113.1 (5)F4B—C28—C18115.3 (5)
F3A—C14—C4113.4 (3)F6B—C28—C18115.6 (3)
F1A—C14—C4112.9 (6)F4A—C28—C18112.0 (4)
F2A—C14—C4112.8 (3)F6A—C28—C18109.6 (4)
F3B—C14—C4112.8 (4)F5B—C28—C18109.9 (3)
C1—N1—N2—C13177.66 (12)C15—N3—N4—C27172.59 (13)
N2—N1—C1—C65.5 (2)N4—N3—C15—C2012.4 (2)
N2—N1—C1—C2174.27 (11)N4—N3—C15—C16166.81 (12)
N1—C1—C2—C3178.08 (12)N3—C15—C16—C17178.34 (13)
C6—C1—C2—C31.7 (2)C20—C15—C16—C170.9 (2)
C1—C2—C3—C40.2 (2)C15—C16—C17—C180.5 (2)
C2—C3—C4—C51.5 (2)C16—C17—C18—C191.3 (2)
C2—C3—C4—C14179.81 (13)C16—C17—C18—C28178.22 (13)
C3—C4—C5—C61.9 (2)C17—C18—C19—C200.8 (2)
C14—C4—C5—C6179.88 (13)C28—C18—C19—C20177.65 (14)
C4—C5—C6—C10.4 (2)C18—C19—C20—C150.6 (2)
N1—C1—C6—C5178.38 (13)N3—C15—C20—C19177.79 (13)
C2—C1—C6—C51.4 (2)C16—C15—C20—C191.4 (2)
C12—C7—C8—C90.4 (2)C26—C21—C22—C230.5 (2)
C13—C7—C8—C9179.64 (12)C27—C21—C22—C23178.08 (12)
C7—C8—C9—C100.8 (2)C21—C22—C23—C240.6 (2)
C8—C9—C10—C110.3 (2)C22—C23—C24—C250.2 (2)
C9—C10—C11—C120.5 (2)C23—C24—C25—C260.3 (2)
C10—C11—C12—C70.9 (2)C24—C25—C26—C210.4 (2)
C8—C7—C12—C110.4 (2)C22—C21—C26—C250.0 (2)
C13—C7—C12—C11178.79 (13)C27—C21—C26—C25178.51 (12)
N1—N2—C13—C7179.90 (11)N3—N4—C27—C21178.71 (12)
C8—C7—C13—N2176.47 (12)C22—C21—C27—N4173.82 (13)
C12—C7—C13—N24.3 (2)C26—C21—C27—N47.6 (2)
C5—C4—C14—F2B44.7 (8)C17—C18—C28—F5A100.5 (9)
C3—C4—C14—F2B137.0 (8)C19—C18—C28—F5A76.4 (9)
C5—C4—C14—F1B165.8 (8)C17—C18—C28—F4B39.4 (7)
C3—C4—C14—F1B15.9 (8)C19—C18—C28—F4B143.7 (6)
C5—C4—C14—F3A88.1 (7)C17—C18—C28—F6B172.9 (8)
C3—C4—C14—F3A90.2 (7)C19—C18—C28—F6B10.2 (8)
C5—C4—C14—F1A151.1 (8)C17—C18—C28—F4A27.0 (5)
C3—C4—C14—F1A30.7 (8)C19—C18—C28—F4A156.2 (5)
C5—C4—C14—F2A32.0 (4)C17—C18—C28—F6A137.0 (5)
C3—C4—C14—F2A149.7 (3)C19—C18—C28—F6A46.2 (5)
C5—C4—C14—F3B74.8 (4)C17—C18—C28—F5B74.6 (3)
C3—C4—C14—F3B103.5 (4)C19—C18—C28—F5B102.3 (3)
(HT11) top
Crystal data top
C15H10F6N2F(000) = 672
Mr = 332.25Dx = 1.621 Mg m3
Monoclinic, CcMo Kα radiation, λ = 0.71073 Å
a = 15.2831 (9) ÅCell parameters from 3889 reflections
b = 4.8177 (3) Åθ = 2.7–29.3°
c = 19.0386 (11) ŵ = 0.16 mm1
β = 103.740 (3)°T = 100 K
V = 1361.69 (14) Å3Needle, colorless
Z = 40.20 × 0.07 × 0.05 mm
Data collection top
Bruker APEX-II CCD
diffractometer
2757 reflections with I > 2σ(I)
φ and ω scansRint = 0.026
Absorption correction: multi-scan
SADABS
θmax = 27.1°, θmin = 2.2°
Tmin = 0.678, Tmax = 0.746h = 1919
9984 measured reflectionsk = 66
2939 independent reflectionsl = 2421
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.031 w = 1/[σ2(Fo2) + (0.0328P)2 + 0.2219P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.069(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.22 e Å3
2939 reflectionsΔρmin = 0.24 e Å3
207 parametersAbsolute structure: Refined as an inversion twin.
2 restraintsAbsolute structure parameter: 0.3 (6)
Special details top

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

Refinement. Refined as a 2-component inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N1A0.2455 (13)0.913 (2)0.1997 (6)0.0173 (5)0.530 (16)
H1A0.30410.91780.21740.021*0.530 (16)
N2A0.1982 (8)0.740 (5)0.2269 (16)0.0173 (5)0.530 (16)
C13A0.2373 (16)0.564 (3)0.2747 (6)0.0173 (5)0.530 (16)
H13A0.30110.55030.28580.021*0.530 (16)
N1B0.2376 (15)0.581 (3)0.2818 (5)0.0173 (5)0.470 (16)
H1B0.29640.59540.29770.021*0.470 (16)
N2B0.1915 (9)0.742 (6)0.2271 (18)0.0173 (5)0.470 (16)
C13B0.2477 (19)0.893 (3)0.1946 (8)0.0173 (5)0.470 (16)
H13B0.31100.86460.20670.021*0.470 (16)
F10.39523 (9)1.3340 (3)0.19583 (7)0.0342 (4)
F20.39901 (9)1.3893 (3)0.08448 (8)0.0324 (4)
F30.39014 (10)0.9814 (3)0.12653 (9)0.0312 (4)
F50.35928 (10)0.0578 (3)0.45536 (8)0.0335 (4)
F40.36261 (9)0.4746 (3)0.41749 (8)0.0298 (4)
F60.37466 (9)0.1345 (3)0.34775 (7)0.0319 (4)
C10.20646 (15)1.0945 (5)0.14188 (12)0.0171 (5)
C20.25917 (15)1.2605 (5)0.10773 (11)0.0175 (5)
C30.21822 (17)1.4507 (5)0.05472 (12)0.0213 (5)
H30.25441.56550.03240.026*
C40.12533 (17)1.4730 (5)0.03444 (12)0.0234 (6)
H40.09771.60180.00190.028*
C50.07297 (16)1.3063 (5)0.06741 (13)0.0227 (5)
H50.00921.32090.05340.027*
C60.11246 (16)1.1186 (5)0.12061 (12)0.0203 (5)
H60.07571.00570.14280.024*
C70.18740 (15)0.3871 (5)0.31236 (11)0.0177 (5)
C80.23037 (15)0.2138 (5)0.36963 (12)0.0188 (5)
C90.18003 (16)0.0311 (5)0.40094 (12)0.0229 (5)
H90.20960.08580.43950.027*
C100.08752 (17)0.0184 (5)0.37649 (14)0.0256 (6)
H100.05350.10720.39790.031*
C110.04469 (17)0.1905 (5)0.32051 (13)0.0243 (6)
H110.01900.18310.30380.029*
C120.09348 (16)0.3724 (5)0.28873 (12)0.0211 (5)
H120.06300.48890.25040.025*
C140.35948 (17)1.2428 (5)0.12792 (13)0.0221 (5)
C150.33020 (16)0.2192 (5)0.39745 (12)0.0216 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N1A0.0175 (8)0.0168 (9)0.0174 (9)0.0006 (11)0.0038 (13)0.0004 (6)
N2A0.0175 (8)0.0168 (9)0.0174 (9)0.0006 (11)0.0038 (13)0.0004 (6)
C13A0.0175 (8)0.0168 (9)0.0174 (9)0.0006 (11)0.0038 (13)0.0004 (6)
N1B0.0175 (8)0.0168 (9)0.0174 (9)0.0006 (11)0.0038 (13)0.0004 (6)
N2B0.0175 (8)0.0168 (9)0.0174 (9)0.0006 (11)0.0038 (13)0.0004 (6)
C13B0.0175 (8)0.0168 (9)0.0174 (9)0.0006 (11)0.0038 (13)0.0004 (6)
F10.0242 (7)0.0495 (10)0.0264 (8)0.0057 (7)0.0008 (6)0.0094 (7)
F20.0264 (8)0.0358 (9)0.0382 (9)0.0077 (7)0.0142 (6)0.0071 (7)
F30.0243 (7)0.0256 (8)0.0471 (9)0.0039 (6)0.0154 (7)0.0015 (7)
F50.0342 (8)0.0316 (9)0.0281 (7)0.0005 (7)0.0059 (6)0.0118 (7)
F40.0288 (8)0.0223 (8)0.0332 (9)0.0058 (7)0.0026 (6)0.0022 (6)
F60.0228 (8)0.0424 (10)0.0297 (8)0.0061 (7)0.0051 (6)0.0056 (7)
C10.0213 (11)0.0143 (11)0.0145 (11)0.0004 (9)0.0021 (9)0.0037 (9)
C20.0205 (12)0.0167 (12)0.0159 (11)0.0005 (10)0.0057 (9)0.0038 (9)
C30.0292 (13)0.0180 (13)0.0174 (12)0.0024 (11)0.0072 (10)0.0005 (9)
C40.0317 (14)0.0196 (13)0.0179 (13)0.0045 (11)0.0036 (10)0.0010 (9)
C50.0203 (12)0.0253 (13)0.0209 (11)0.0038 (11)0.0018 (9)0.0007 (10)
C60.0207 (11)0.0197 (13)0.0209 (12)0.0011 (10)0.0056 (9)0.0004 (9)
C70.0214 (12)0.0149 (12)0.0175 (11)0.0007 (9)0.0059 (9)0.0021 (9)
C80.0241 (13)0.0164 (12)0.0166 (11)0.0011 (10)0.0062 (9)0.0031 (9)
C90.0315 (14)0.0195 (13)0.0181 (12)0.0013 (11)0.0069 (10)0.0006 (9)
C100.0330 (14)0.0223 (14)0.0248 (13)0.0074 (11)0.0132 (11)0.0013 (10)
C110.0218 (11)0.0221 (14)0.0295 (13)0.0036 (11)0.0069 (10)0.0046 (10)
C120.0220 (12)0.0197 (12)0.0212 (12)0.0023 (10)0.0045 (10)0.0002 (10)
C140.0229 (12)0.0214 (13)0.0230 (12)0.0028 (10)0.0070 (10)0.0002 (10)
C150.0258 (12)0.0181 (13)0.0189 (12)0.0004 (10)0.0012 (9)0.0012 (9)
Geometric parameters (Å, º) top
N1A—N2A1.29 (3)C2—C31.396 (3)
N1A—C11.422 (13)C2—C141.492 (3)
N1A—H1A0.8800C3—C41.384 (3)
N2A—C13A1.28 (2)C3—H30.9500
C13A—C71.443 (19)C4—C51.385 (3)
C13A—H13A0.9500C4—H40.9500
N1B—N2B1.36 (3)C5—C61.385 (3)
N1B—C71.418 (18)C5—H50.9500
N1B—H1B0.8800C6—H60.9500
N2B—C13B1.38 (4)C7—C121.400 (3)
C13B—C11.430 (18)C7—C81.406 (3)
C13B—H13B0.9500C8—C91.393 (3)
F1—C141.352 (3)C8—C151.492 (3)
F2—C141.336 (3)C9—C101.381 (3)
F3—C141.346 (3)C9—H90.9500
F5—C151.336 (3)C10—C111.386 (4)
F4—C151.347 (3)C10—H100.9500
F6—C151.352 (3)C11—C121.380 (3)
C1—C21.400 (3)C11—H110.9500
C1—C61.402 (3)C12—H120.9500
N2A—N1A—C1122.4 (15)C1—C6—H6119.9
N2A—N1A—H1A118.8C12—C7—C8118.3 (2)
C1—N1A—H1A118.8C12—C7—N1B121.0 (8)
C13A—N2A—N1A120.0 (13)C8—C7—N1B120.7 (8)
N2A—C13A—C7122.1 (17)C12—C7—C13A119.5 (8)
N2A—C13A—H13A118.9C8—C7—C13A122.1 (8)
C7—C13A—H13A118.9C9—C8—C7120.2 (2)
N2B—N1B—C7117.4 (17)C9—C8—C15118.8 (2)
N2B—N1B—H1B121.3C7—C8—C15121.0 (2)
C7—N1B—H1B121.3C10—C9—C8120.6 (2)
N1B—N2B—C13B112.5 (14)C10—C9—H9119.7
N2B—C13B—C1117 (2)C8—C9—H9119.7
N2B—C13B—H13B121.4C9—C10—C11119.4 (2)
C1—C13B—H13B121.4C9—C10—H10120.3
C2—C1—C6118.8 (2)C11—C10—H10120.3
C2—C1—N1A122.0 (8)C12—C11—C10120.8 (2)
C6—C1—N1A119.2 (8)C12—C11—H11119.6
C2—C1—C13B120.5 (11)C10—C11—H11119.6
C6—C1—C13B120.6 (11)C11—C12—C7120.7 (2)
C3—C2—C1120.1 (2)C11—C12—H12119.6
C3—C2—C14118.7 (2)C7—C12—H12119.6
C1—C2—C14121.1 (2)F2—C14—F3105.75 (19)
C4—C3—C2120.4 (2)F2—C14—F1106.30 (19)
C4—C3—H3119.8F3—C14—F1105.04 (19)
C2—C3—H3119.8F2—C14—C2113.47 (19)
C3—C4—C5119.6 (2)F3—C14—C2112.9 (2)
C3—C4—H4120.2F1—C14—C2112.65 (19)
C5—C4—H4120.2F5—C15—F4105.67 (19)
C6—C5—C4120.8 (2)F5—C15—F6106.13 (19)
C6—C5—H5119.6F4—C15—F6105.2 (2)
C4—C5—H5119.6F5—C15—C8113.2 (2)
C5—C6—C1120.3 (2)F4—C15—C8113.1 (2)
C5—C6—H6119.9F6—C15—C8112.83 (19)
C1—N1A—N2A—C13A174.1 (13)C12—C7—C8—C90.7 (3)
N1A—N2A—C13A—C7173 (2)N1B—C7—C8—C9177.8 (6)
C7—N1B—N2B—C13B171 (2)C13A—C7—C8—C9175.3 (6)
N1B—N2B—C13B—C1172.9 (14)C12—C7—C8—C15180.0 (2)
N2A—N1A—C1—C2173 (2)N1B—C7—C8—C152.9 (6)
N2A—N1A—C1—C610 (2)C13A—C7—C8—C154.0 (6)
N2B—C13B—C1—C2178 (2)C7—C8—C9—C100.3 (3)
N2B—C13B—C1—C65 (2)C15—C8—C9—C10179.6 (2)
C6—C1—C2—C31.5 (3)C8—C9—C10—C110.3 (3)
N1A—C1—C2—C3175.4 (5)C9—C10—C11—C120.4 (4)
C13B—C1—C2—C3178.0 (6)C10—C11—C12—C70.0 (3)
C6—C1—C2—C14179.7 (2)C8—C7—C12—C110.6 (3)
N1A—C1—C2—C143.3 (5)N1B—C7—C12—C11177.6 (6)
C13B—C1—C2—C143.2 (7)C13A—C7—C12—C11175.5 (6)
C1—C2—C3—C41.3 (3)C3—C2—C14—F28.9 (3)
C14—C2—C3—C4179.9 (2)C1—C2—C14—F2172.35 (19)
C2—C3—C4—C50.4 (3)C3—C2—C14—F3129.2 (2)
C3—C4—C5—C60.3 (4)C1—C2—C14—F352.0 (3)
C4—C5—C6—C10.0 (4)C3—C2—C14—F1112.0 (2)
C2—C1—C6—C50.9 (3)C1—C2—C14—F166.8 (3)
N1A—C1—C6—C5176.2 (4)C9—C8—C15—F55.5 (3)
C13B—C1—C6—C5177.4 (7)C7—C8—C15—F5175.2 (2)
N2B—N1B—C7—C122.5 (14)C9—C8—C15—F4125.7 (2)
N2B—N1B—C7—C8179.5 (15)C7—C8—C15—F455.0 (3)
N2A—C13A—C7—C1210.4 (16)C9—C8—C15—F6115.1 (2)
N2A—C13A—C7—C8173.7 (17)C7—C8—C15—F664.2 (3)
(HT13) top
Crystal data top
C15H10F6N2Z = 2
Mr = 332.25F(000) = 336
Triclinic, P1Dx = 1.635 Mg m3
a = 8.189 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.376 (2) ÅCell parameters from 3907 reflections
c = 11.623 (4) Åθ = 2.8–27.4°
α = 72.723 (18)°µ = 0.16 mm1
β = 82.222 (17)°T = 100 K
γ = 62.417 (15)°Plate, colorless
V = 674.7 (4) Å30.25 × 0.21 × 0.16 mm
Data collection top
Bruker APEX-II CCD
diffractometer
2297 reflections with I > 2σ(I)
φ and ω scansRint = 0.037
Absorption correction: multi-scan
SADABS
θmax = 27.6°, θmin = 1.8°
Tmin = 0.652, Tmax = 0.746h = 810
9731 measured reflectionsk = 1010
3006 independent reflectionsl = 1515
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.040H-atom parameters constrained
wR(F2) = 0.131 w = 1/[σ2(Fo2) + (0.0689P)2]
where P = (Fo2 + 2Fc2)/3
S = 1.16(Δ/σ)max < 0.001
3006 reflectionsΔρmax = 0.32 e Å3
208 parametersΔρmin = 0.31 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.08534 (16)0.13161 (18)0.64301 (10)0.0424 (3)
F51.01180 (12)0.09260 (13)1.10761 (9)0.0281 (3)
F40.90269 (12)0.38568 (14)1.01897 (8)0.0288 (3)
F30.08720 (14)0.12992 (17)0.48772 (10)0.0426 (3)
F20.10402 (14)0.38777 (15)0.52583 (10)0.0402 (3)
F61.02271 (13)0.27945 (15)1.19544 (9)0.0343 (3)
N10.55943 (18)0.17255 (19)0.85231 (12)0.0220 (3)
H10.67390.13270.82630.026*
N20.51622 (18)0.22265 (18)0.95703 (12)0.0201 (3)
C140.0173 (2)0.2117 (2)0.57707 (15)0.0237 (4)
C40.1605 (2)0.1999 (2)0.65025 (14)0.0198 (3)
C50.1150 (2)0.2424 (2)0.76076 (15)0.0222 (4)
H50.00760.27730.78980.027*
C60.2454 (2)0.2343 (2)0.82870 (14)0.0205 (4)
H60.21300.26320.90420.025*
C10.4250 (2)0.1835 (2)0.78591 (14)0.0190 (3)
C130.6416 (2)0.2265 (2)1.00875 (15)0.0209 (4)
H130.76030.19590.97340.025*
C70.6022 (2)0.2785 (2)1.12307 (14)0.0181 (3)
C80.7305 (2)0.2955 (2)1.18163 (14)0.0199 (4)
C150.9145 (2)0.2647 (2)1.12693 (15)0.0226 (4)
C90.6868 (2)0.3462 (2)1.28937 (15)0.0231 (4)
H90.77550.35631.32790.028*
C100.5153 (2)0.3820 (2)1.34076 (15)0.0263 (4)
H100.48520.41711.41430.032*
C110.3875 (2)0.3661 (2)1.28366 (15)0.0255 (4)
H110.26910.39101.31830.031*
C120.4304 (2)0.3147 (2)1.17750 (15)0.0217 (4)
H120.34120.30351.14030.026*
C30.3386 (2)0.1510 (2)0.60751 (15)0.0218 (4)
H30.37040.12300.53170.026*
C20.4699 (2)0.1428 (2)0.67455 (15)0.0222 (4)
H20.59200.10920.64470.027*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0451 (7)0.0676 (8)0.0341 (6)0.0456 (6)0.0038 (5)0.0045 (6)
F50.0186 (5)0.0272 (6)0.0355 (6)0.0067 (4)0.0016 (4)0.0095 (4)
F40.0262 (5)0.0328 (6)0.0290 (6)0.0180 (5)0.0040 (4)0.0040 (4)
F30.0331 (6)0.0681 (9)0.0430 (7)0.0231 (6)0.0012 (5)0.0372 (6)
F20.0381 (7)0.0330 (6)0.0489 (7)0.0132 (5)0.0228 (6)0.0046 (5)
F60.0237 (5)0.0538 (7)0.0380 (6)0.0233 (5)0.0023 (5)0.0185 (5)
N10.0161 (7)0.0308 (8)0.0221 (7)0.0112 (6)0.0001 (6)0.0097 (6)
N20.0227 (7)0.0214 (7)0.0187 (7)0.0118 (6)0.0006 (6)0.0051 (5)
C140.0243 (9)0.0263 (9)0.0244 (9)0.0137 (8)0.0003 (7)0.0081 (7)
C40.0214 (8)0.0186 (8)0.0218 (8)0.0110 (7)0.0022 (7)0.0042 (6)
C50.0199 (8)0.0258 (9)0.0246 (9)0.0132 (7)0.0025 (7)0.0075 (7)
C60.0225 (8)0.0254 (9)0.0184 (8)0.0135 (7)0.0023 (7)0.0086 (7)
C10.0206 (8)0.0172 (8)0.0214 (8)0.0107 (7)0.0032 (7)0.0026 (6)
C130.0185 (8)0.0223 (8)0.0238 (9)0.0112 (7)0.0009 (7)0.0055 (7)
C70.0191 (8)0.0156 (8)0.0189 (8)0.0086 (7)0.0029 (6)0.0010 (6)
C80.0200 (8)0.0175 (8)0.0223 (8)0.0095 (7)0.0019 (7)0.0026 (6)
C150.0214 (8)0.0247 (9)0.0256 (9)0.0122 (7)0.0034 (7)0.0074 (7)
C90.0266 (9)0.0240 (9)0.0216 (8)0.0138 (8)0.0038 (7)0.0042 (7)
C100.0310 (10)0.0279 (9)0.0218 (9)0.0143 (8)0.0039 (8)0.0089 (7)
C110.0217 (9)0.0273 (9)0.0262 (9)0.0122 (8)0.0051 (7)0.0055 (7)
C120.0191 (8)0.0220 (8)0.0243 (9)0.0112 (7)0.0037 (7)0.0014 (7)
C30.0243 (9)0.0232 (8)0.0198 (8)0.0116 (7)0.0009 (7)0.0070 (7)
C20.0175 (8)0.0272 (9)0.0225 (8)0.0105 (7)0.0023 (7)0.0079 (7)
Geometric parameters (Å, º) top
F1—C141.3366 (19)C1—C21.394 (2)
F5—C151.3579 (19)C13—C71.469 (2)
F4—C151.3406 (19)C13—H130.9500
F3—C141.3318 (19)C7—C121.396 (2)
F2—C141.341 (2)C7—C81.406 (2)
F6—C151.3358 (18)C8—C91.389 (2)
N1—N21.3535 (17)C8—C151.490 (2)
N1—C11.3818 (19)C9—C101.382 (2)
N1—H10.8800C9—H90.9500
N2—C131.2751 (19)C10—C111.386 (2)
C14—C41.490 (2)C10—H100.9500
C4—C31.384 (2)C11—C121.375 (2)
C4—C51.391 (2)C11—H110.9500
C5—C61.377 (2)C12—H120.9500
C5—H50.9500C3—C21.376 (2)
C6—C11.393 (2)C3—H30.9500
C6—H60.9500C2—H20.9500
N2—N1—C1120.44 (13)C9—C8—C7120.96 (14)
N2—N1—H1119.8C9—C8—C15118.71 (14)
C1—N1—H1119.8C7—C8—C15120.30 (14)
C13—N2—N1117.74 (13)F6—C15—F4106.80 (12)
F3—C14—F1106.31 (13)F6—C15—F5105.58 (13)
F3—C14—F2106.07 (14)F4—C15—F5105.29 (13)
F1—C14—F2104.76 (14)F6—C15—C8113.05 (14)
F3—C14—C4113.29 (14)F4—C15—C8112.55 (14)
F1—C14—C4112.45 (14)F5—C15—C8112.94 (13)
F2—C14—C4113.27 (13)C10—C9—C8120.38 (15)
C3—C4—C5119.46 (15)C10—C9—H9119.8
C3—C4—C14120.27 (15)C8—C9—H9119.8
C5—C4—C14120.26 (14)C9—C10—C11119.16 (16)
C6—C5—C4120.91 (14)C9—C10—H10120.4
C6—C5—H5119.5C11—C10—H10120.4
C4—C5—H5119.5C12—C11—C10120.70 (15)
C5—C6—C1119.51 (15)C12—C11—H11119.7
C5—C6—H6120.2C10—C11—H11119.7
C1—C6—H6120.2C11—C12—C7121.47 (15)
N1—C1—C6120.97 (14)C11—C12—H12119.3
N1—C1—C2119.52 (14)C7—C12—H12119.3
C6—C1—C2119.50 (15)C2—C3—C4120.13 (15)
N2—C13—C7119.88 (14)C2—C3—H3119.9
N2—C13—H13120.1C4—C3—H3119.9
C7—C13—H13120.1C3—C2—C1120.48 (15)
C12—C7—C8117.32 (15)C3—C2—H2119.8
C12—C7—C13119.77 (14)C1—C2—H2119.8
C8—C7—C13122.92 (14)
C1—N1—N2—C13173.54 (14)C13—C7—C8—C151.4 (2)
F3—C14—C4—C315.1 (2)C9—C8—C15—F64.0 (2)
F1—C14—C4—C3135.70 (16)C7—C8—C15—F6177.76 (13)
F2—C14—C4—C3105.75 (17)C9—C8—C15—F4117.10 (16)
F3—C14—C4—C5166.40 (15)C7—C8—C15—F461.12 (19)
F1—C14—C4—C545.8 (2)C9—C8—C15—F5123.83 (16)
F2—C14—C4—C572.72 (19)C7—C8—C15—F558.0 (2)
C3—C4—C5—C60.7 (2)C7—C8—C9—C100.4 (2)
C14—C4—C5—C6179.20 (14)C15—C8—C9—C10177.84 (14)
C4—C5—C6—C10.2 (2)C8—C9—C10—C110.2 (2)
N2—N1—C1—C64.2 (2)C9—C10—C11—C120.3 (2)
N2—N1—C1—C2175.88 (14)C10—C11—C12—C70.6 (3)
C5—C6—C1—N1179.43 (14)C8—C7—C12—C110.4 (2)
C5—C6—C1—C20.4 (2)C13—C7—C12—C11179.12 (15)
N1—N2—C13—C7179.51 (13)C5—C4—C3—C20.6 (2)
N2—C13—C7—C123.1 (2)C14—C4—C3—C2179.09 (14)
N2—C13—C7—C8176.45 (14)C4—C3—C2—C10.0 (2)
C12—C7—C8—C90.0 (2)N1—C1—C2—C3179.33 (13)
C13—C7—C8—C9179.59 (14)C6—C1—C2—C30.5 (2)
C12—C7—C8—C15178.13 (14)
(HT20) top
Crystal data top
C14H11F3N2Dx = 1.466 Mg m3
Mr = 264.25Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pna21Cell parameters from 9925 reflections
a = 11.5823 (6) Åθ = 2.9–30.5°
b = 13.8757 (7) ŵ = 0.12 mm1
c = 7.4479 (3) ÅT = 100 K
V = 1196.97 (10) Å3Plate, colorless
Z = 40.25 × 0.13 × 0.10 mm
F(000) = 544
Data collection top
Bruker APEX-II CCD
diffractometer
3036 reflections with I > 2σ(I)
φ and ω scansRint = 0.048
Absorption correction: multi-scan
SADABS
θmax = 30.5°, θmin = 2.9°
Tmin = 0.645, Tmax = 0.734h = 1616
22984 measured reflectionsk = 1919
3414 independent reflectionsl = 109
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.037 w = 1/[σ2(Fo2) + (0.0503P)2 + 0.1985P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.090(Δ/σ)max < 0.001
S = 1.04Δρmax = 0.33 e Å3
3414 reflectionsΔρmin = 0.25 e Å3
173 parametersAbsolute structure: Refined as an inversion twin.
1 restraintAbsolute structure parameter: 0.2 (7)
Special details top

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

Refinement. Refined as a 2-component inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F10.75926 (15)0.45385 (9)0.8262 (2)0.0393 (4)
F20.77569 (12)0.43847 (8)1.10965 (18)0.0292 (3)
F30.60943 (10)0.42710 (8)0.9882 (3)0.0367 (3)
N10.49483 (13)0.07978 (10)1.0378 (2)0.0183 (3)
H10.44010.05691.10780.022*
N20.58217 (11)0.02168 (10)0.9834 (2)0.0160 (3)
C40.48248 (16)0.37130 (13)0.8904 (3)0.0201 (4)
H40.47980.43770.85980.024*
C50.57785 (15)0.31531 (12)0.8440 (3)0.0187 (3)
H50.64020.34400.78090.022*
C60.58311 (14)0.21814 (12)0.8887 (2)0.0163 (3)
H60.64830.18060.85560.020*
C10.49170 (13)0.17618 (11)0.9827 (3)0.0142 (3)
C130.57933 (15)0.06664 (11)1.0366 (2)0.0153 (3)
H130.51830.08841.11150.018*
C70.67070 (13)0.13348 (11)0.9811 (2)0.0144 (3)
C80.65452 (14)0.23272 (11)1.0061 (2)0.0147 (3)
H80.58730.25591.06480.018*
C90.73760 (14)0.29681 (12)0.9442 (2)0.0153 (3)
C100.83839 (14)0.26481 (12)0.8620 (2)0.0179 (3)
H100.89450.30960.82070.021*
C140.71941 (15)0.40342 (12)0.9658 (3)0.0185 (3)
C30.39164 (15)0.32866 (12)0.9818 (3)0.0191 (3)
H30.32630.36641.01370.023*
C20.39466 (14)0.23121 (12)1.0276 (3)0.0168 (3)
H20.33140.20251.08870.020*
C120.77315 (15)0.10110 (13)0.8998 (3)0.0167 (3)
H120.78590.03390.88500.020*
C110.85590 (15)0.16615 (13)0.8410 (3)0.0185 (3)
H110.92470.14330.78620.022*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.0746 (11)0.0182 (5)0.0253 (7)0.0081 (6)0.0148 (7)0.0038 (5)
F20.0395 (7)0.0197 (5)0.0284 (7)0.0013 (5)0.0086 (6)0.0092 (5)
F30.0233 (5)0.0163 (5)0.0704 (10)0.0041 (4)0.0029 (7)0.0029 (6)
N10.0181 (7)0.0128 (6)0.0241 (8)0.0017 (5)0.0072 (6)0.0026 (6)
N20.0175 (6)0.0144 (6)0.0161 (7)0.0016 (5)0.0007 (6)0.0002 (6)
C40.0236 (8)0.0130 (7)0.0236 (9)0.0017 (6)0.0054 (8)0.0004 (6)
C50.0194 (8)0.0165 (7)0.0201 (8)0.0045 (6)0.0011 (7)0.0015 (7)
C60.0152 (7)0.0157 (7)0.0181 (9)0.0012 (6)0.0002 (6)0.0001 (6)
C10.0161 (7)0.0121 (6)0.0146 (7)0.0001 (5)0.0009 (7)0.0004 (6)
C130.0166 (7)0.0142 (7)0.0153 (8)0.0002 (6)0.0000 (6)0.0004 (6)
C70.0166 (7)0.0129 (7)0.0135 (7)0.0002 (5)0.0010 (7)0.0010 (6)
C80.0164 (7)0.0133 (7)0.0144 (8)0.0005 (5)0.0007 (6)0.0008 (6)
C90.0189 (7)0.0140 (7)0.0129 (8)0.0007 (6)0.0019 (6)0.0007 (6)
C100.0171 (7)0.0206 (8)0.0160 (8)0.0047 (6)0.0003 (6)0.0013 (7)
C140.0227 (8)0.0142 (7)0.0184 (8)0.0036 (6)0.0002 (7)0.0002 (7)
C30.0192 (7)0.0164 (7)0.0216 (9)0.0046 (6)0.0018 (7)0.0017 (7)
C20.0155 (7)0.0165 (7)0.0184 (8)0.0007 (6)0.0019 (6)0.0006 (6)
C120.0178 (7)0.0161 (7)0.0163 (8)0.0022 (6)0.0015 (7)0.0020 (6)
C110.0144 (7)0.0228 (8)0.0184 (8)0.0007 (6)0.0011 (7)0.0040 (7)
Geometric parameters (Å, º) top
F1—C141.335 (2)C13—H130.9500
F2—C141.345 (2)C7—C81.402 (2)
F3—C141.326 (2)C7—C121.406 (2)
N1—N21.3555 (19)C8—C91.389 (2)
N1—C11.400 (2)C8—H80.9500
N1—H10.8800C9—C101.391 (2)
N2—C131.288 (2)C9—C141.503 (2)
C4—C31.386 (3)C10—C111.393 (2)
C4—C51.394 (3)C10—H100.9500
C4—H40.9500C3—C21.395 (2)
C5—C61.390 (2)C3—H30.9500
C5—H50.9500C2—H20.9500
C6—C11.396 (2)C12—C111.388 (2)
C6—H60.9500C12—H120.9500
C1—C21.399 (2)C11—H110.9500
C13—C71.467 (2)
N2—N1—C1120.01 (14)C8—C9—C10121.54 (15)
N2—N1—H1120.0C8—C9—C14119.85 (15)
C1—N1—H1120.0C10—C9—C14118.61 (15)
C13—N2—N1117.06 (14)C9—C10—C11119.03 (15)
C3—C4—C5119.04 (16)C9—C10—H10120.5
C3—C4—H4120.5C11—C10—H10120.5
C5—C4—H4120.5F3—C14—F1107.47 (16)
C6—C5—C4121.06 (17)F3—C14—F2105.99 (16)
C6—C5—H5119.5F1—C14—F2105.25 (14)
C4—C5—H5119.5F3—C14—C9113.08 (13)
C5—C6—C1119.42 (15)F1—C14—C9112.59 (16)
C5—C6—H6120.3F2—C14—C9111.91 (15)
C1—C6—H6120.3C4—C3—C2120.99 (16)
C6—C1—C2120.08 (14)C4—C3—H3119.5
C6—C1—N1121.73 (14)C2—C3—H3119.5
C2—C1—N1118.18 (15)C3—C2—C1119.38 (16)
N2—C13—C7119.77 (15)C3—C2—H2120.3
N2—C13—H13120.1C1—C2—H2120.3
C7—C13—H13120.1C11—C12—C7120.73 (15)
C8—C7—C12118.93 (15)C11—C12—H12119.6
C8—C7—C13119.16 (14)C7—C12—H12119.6
C12—C7—C13121.89 (14)C12—C11—C10120.23 (16)
C9—C8—C7119.49 (15)C12—C11—H11119.9
C9—C8—H8120.3C10—C11—H11119.9
C7—C8—H8120.3
C1—N1—N2—C13179.05 (16)C14—C9—C10—C11179.86 (17)
C3—C4—C5—C60.3 (3)C8—C9—C14—F321.2 (3)
C4—C5—C6—C10.4 (3)C10—C9—C14—F3158.81 (18)
C5—C6—C1—C21.5 (3)C8—C9—C14—F1143.29 (17)
C5—C6—C1—N1177.18 (17)C10—C9—C14—F136.7 (2)
N2—N1—C1—C67.3 (3)C8—C9—C14—F298.38 (18)
N2—N1—C1—C2174.06 (16)C10—C9—C14—F281.6 (2)
N1—N2—C13—C7179.44 (15)C5—C4—C3—C20.1 (3)
N2—C13—C7—C8166.32 (16)C4—C3—C2—C10.9 (3)
N2—C13—C7—C1212.2 (3)C6—C1—C2—C31.7 (3)
C12—C7—C8—C92.4 (2)N1—C1—C2—C3177.00 (16)
C13—C7—C8—C9176.19 (17)C8—C7—C12—C111.6 (3)
C7—C8—C9—C101.7 (3)C13—C7—C12—C11176.98 (17)
C7—C8—C9—C14178.30 (16)C7—C12—C11—C100.0 (3)
C8—C9—C10—C110.2 (3)C9—C10—C11—C120.7 (3)
(HT31) top
Crystal data top
C15H10F6N2Z = 2
Mr = 332.25F(000) = 336
Triclinic, P1Dx = 1.611 Mg m3
a = 8.2523 (3) ÅMo Kα radiation, λ = 0.71073 Å
b = 8.3039 (4) ÅCell parameters from 7617 reflections
c = 11.7930 (5) Åθ = 3.6–30.6°
α = 82.823 (2)°µ = 0.15 mm1
β = 74.769 (2)°T = 100 K
γ = 61.428 (2)°Plate, colorless
V = 684.78 (5) Å30.27 × 0.19 × 0.11 mm
Data collection top
Bruker APEX-II CCD
diffractometer
2989 reflections with I > 2σ(I)
φ and ω scansRint = 0.030
Absorption correction: multi-scan
SADABS
θmax = 28.3°, θmin = 1.8°
Tmin = 0.672, Tmax = 0.746h = 1010
12775 measured reflectionsk = 1111
3365 independent reflectionsl = 1515
Refinement top
Refinement on F20 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037H-atom parameters constrained
wR(F2) = 0.107 w = 1/[σ2(Fo2) + (0.0551P)2 + 0.1675P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max < 0.001
3365 reflectionsΔρmax = 0.38 e Å3
208 parametersΔρmin = 0.35 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
F50.62347 (13)0.07084 (12)0.14015 (7)0.0417 (2)
F30.88394 (11)0.90018 (10)0.52754 (6)0.03319 (19)
F60.61995 (14)0.10368 (11)0.00975 (8)0.0463 (2)
F40.88364 (11)0.09672 (12)0.02874 (8)0.0427 (2)
F10.58489 (10)1.00671 (9)0.59823 (7)0.03223 (19)
F20.75744 (13)1.03172 (10)0.69678 (7)0.0382 (2)
N10.73844 (14)0.63879 (12)0.51673 (8)0.0226 (2)
H10.71320.74680.48380.027*
N20.73659 (13)0.50728 (12)0.45998 (8)0.0213 (2)
C40.86588 (17)0.53006 (18)0.84821 (10)0.0281 (3)
H40.89490.50470.92330.034*
C50.85966 (17)0.39823 (17)0.78996 (10)0.0280 (2)
H50.88500.28220.82580.034*
C60.81712 (16)0.43322 (15)0.68056 (10)0.0236 (2)
H60.81310.34160.64230.028*
C10.78009 (14)0.60302 (14)0.62630 (9)0.0197 (2)
C130.69992 (15)0.54917 (14)0.35821 (9)0.0219 (2)
H130.67320.66820.32730.026*
C70.69878 (15)0.41539 (14)0.28903 (9)0.0203 (2)
C80.65799 (17)0.46521 (15)0.17848 (10)0.0247 (2)
H80.62920.58570.14980.030*
C90.65913 (16)0.33982 (15)0.10996 (9)0.0242 (2)
H90.63080.37460.03490.029*
C100.70167 (15)0.16435 (15)0.15161 (9)0.0212 (2)
C150.70684 (17)0.02672 (16)0.07780 (10)0.0256 (2)
C140.75457 (17)0.91702 (15)0.62872 (10)0.0249 (2)
C20.78710 (15)0.73623 (14)0.68521 (9)0.0208 (2)
C110.74380 (17)0.11242 (16)0.26174 (10)0.0252 (2)
H110.77380.00860.28980.030*
C120.74174 (17)0.23748 (15)0.32996 (9)0.0235 (2)
H120.76970.20230.40510.028*
C30.82925 (16)0.69861 (16)0.79544 (10)0.0248 (2)
H30.83290.78960.83480.030*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F50.0604 (5)0.0469 (5)0.0367 (4)0.0409 (4)0.0055 (4)0.0072 (3)
F30.0375 (4)0.0294 (4)0.0326 (4)0.0187 (3)0.0033 (3)0.0033 (3)
F60.0737 (6)0.0394 (4)0.0427 (5)0.0274 (4)0.0388 (4)0.0022 (4)
F40.0347 (4)0.0440 (5)0.0481 (5)0.0147 (4)0.0028 (3)0.0259 (4)
F10.0315 (4)0.0213 (3)0.0412 (4)0.0067 (3)0.0149 (3)0.0012 (3)
F20.0586 (5)0.0274 (4)0.0404 (4)0.0244 (4)0.0193 (4)0.0042 (3)
N10.0313 (5)0.0181 (4)0.0205 (4)0.0116 (4)0.0084 (4)0.0021 (3)
N20.0228 (4)0.0211 (4)0.0214 (4)0.0105 (4)0.0044 (3)0.0048 (3)
C40.0310 (6)0.0351 (6)0.0198 (5)0.0157 (5)0.0085 (4)0.0016 (4)
C50.0312 (6)0.0271 (5)0.0246 (5)0.0133 (5)0.0068 (4)0.0034 (4)
C60.0270 (5)0.0222 (5)0.0221 (5)0.0122 (4)0.0039 (4)0.0024 (4)
C10.0183 (5)0.0214 (5)0.0185 (5)0.0087 (4)0.0024 (4)0.0033 (4)
C130.0242 (5)0.0189 (5)0.0216 (5)0.0086 (4)0.0055 (4)0.0026 (4)
C70.0192 (5)0.0214 (5)0.0199 (5)0.0088 (4)0.0043 (4)0.0027 (4)
C80.0304 (6)0.0201 (5)0.0232 (5)0.0100 (4)0.0095 (4)0.0006 (4)
C90.0281 (5)0.0252 (5)0.0195 (5)0.0108 (4)0.0090 (4)0.0003 (4)
C100.0217 (5)0.0240 (5)0.0204 (5)0.0117 (4)0.0050 (4)0.0039 (4)
C150.0300 (6)0.0285 (5)0.0233 (5)0.0155 (5)0.0088 (4)0.0031 (4)
C140.0288 (6)0.0221 (5)0.0260 (5)0.0118 (4)0.0078 (4)0.0043 (4)
C20.0203 (5)0.0207 (5)0.0212 (5)0.0094 (4)0.0034 (4)0.0036 (4)
C110.0342 (6)0.0232 (5)0.0243 (5)0.0166 (5)0.0110 (4)0.0025 (4)
C120.0311 (6)0.0257 (5)0.0193 (5)0.0157 (4)0.0101 (4)0.0017 (4)
C30.0245 (5)0.0299 (6)0.0222 (5)0.0131 (4)0.0052 (4)0.0059 (4)
Geometric parameters (Å, º) top
F5—C151.3375 (15)C1—C21.4085 (14)
F3—C141.3464 (14)C13—C71.4630 (14)
F6—C151.3321 (13)C13—H130.9500
F4—C151.3373 (14)C7—C81.3952 (14)
F1—C141.3583 (14)C7—C121.3971 (15)
F2—C141.3321 (12)C8—C91.3907 (15)
N1—N21.3582 (12)C8—H80.9500
N1—C11.3842 (13)C9—C101.3821 (16)
N1—H10.8800C9—H90.9500
N2—C131.2802 (14)C10—C111.3955 (15)
C4—C31.3835 (17)C10—C151.4993 (14)
C4—C51.3904 (17)C14—C21.4927 (15)
C4—H40.9500C2—C31.3931 (15)
C5—C61.3853 (15)C11—C121.3823 (15)
C5—H50.9500C11—H110.9500
C6—C11.3986 (15)C12—H120.9500
C6—H60.9500C3—H30.9500
N2—N1—C1120.00 (9)C9—C10—C11120.38 (10)
N2—N1—H1120.0C9—C10—C15120.28 (10)
C1—N1—H1120.0C11—C10—C15119.34 (10)
C13—N2—N1116.51 (9)F6—C15—F4106.54 (10)
C3—C4—C5119.16 (10)F6—C15—F5106.46 (10)
C3—C4—H4120.4F4—C15—F5105.43 (10)
C5—C4—H4120.4F6—C15—C10112.77 (10)
C6—C5—C4121.11 (11)F4—C15—C10112.67 (9)
C6—C5—H5119.4F5—C15—C10112.42 (9)
C4—C5—H5119.4F2—C14—F3106.83 (10)
C5—C6—C1120.23 (10)F2—C14—F1106.29 (9)
C5—C6—H6119.9F3—C14—F1104.65 (9)
C1—C6—H6119.9F2—C14—C2113.54 (9)
N1—C1—C6120.61 (9)F3—C14—C2112.47 (9)
N1—C1—C2120.78 (10)F1—C14—C2112.43 (9)
C6—C1—C2118.61 (10)C3—C2—C1120.26 (10)
N2—C13—C7120.61 (10)C3—C2—C14119.41 (10)
N2—C13—H13119.7C1—C2—C14120.31 (9)
C7—C13—H13119.7C12—C11—C10119.85 (10)
C8—C7—C12119.18 (10)C12—C11—H11120.1
C8—C7—C13119.28 (10)C10—C11—H11120.1
C12—C7—C13121.53 (9)C11—C12—C7120.39 (10)
C9—C8—C7120.51 (10)C11—C12—H12119.8
C9—C8—H8119.7C7—C12—H12119.8
C7—C8—H8119.7C4—C3—C2120.63 (10)
C10—C9—C8119.69 (10)C4—C3—H3119.7
C10—C9—H9120.2C2—C3—H3119.7
C8—C9—H9120.2
C1—N1—N2—C13178.91 (10)C11—C10—C15—F543.98 (15)
C3—C4—C5—C60.15 (18)N1—C1—C2—C3179.97 (10)
C4—C5—C6—C10.23 (18)C6—C1—C2—C30.31 (16)
N2—N1—C1—C61.18 (16)N1—C1—C2—C141.62 (16)
N2—N1—C1—C2178.48 (9)C6—C1—C2—C14178.05 (10)
C5—C6—C1—N1179.66 (10)F2—C14—C2—C34.37 (15)
C5—C6—C1—C20.01 (16)F3—C14—C2—C3117.09 (11)
N1—N2—C13—C7178.64 (9)F1—C14—C2—C3125.09 (11)
N2—C13—C7—C8179.89 (10)F2—C14—C2—C1177.26 (9)
N2—C13—C7—C121.56 (17)F3—C14—C2—C161.28 (13)
C12—C7—C8—C90.30 (17)F1—C14—C2—C156.55 (13)
C13—C7—C8—C9178.88 (10)C9—C10—C11—C120.44 (17)
C7—C8—C9—C100.22 (18)C15—C10—C11—C12179.21 (10)
C8—C9—C10—C110.14 (17)C10—C11—C12—C70.37 (18)
C8—C9—C10—C15178.91 (10)C8—C7—C12—C110.00 (17)
C9—C10—C15—F616.88 (16)C13—C7—C12—C11178.55 (10)
C11—C10—C15—F6164.34 (11)C5—C4—C3—C20.17 (17)
C9—C10—C15—F4103.79 (13)C1—C2—C3—C40.40 (17)
C11—C10—C15—F474.99 (14)C14—C2—C3—C4177.97 (11)
C9—C10—C15—F5137.25 (11)
(HT33C) top
Crystal data top
C15H10F6N2F(000) = 672
Mr = 332.25Dx = 1.539 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
a = 14.330 (4) ÅCell parameters from 7210 reflections
b = 13.658 (5) Åθ = 3.0–30.1°
c = 7.938 (2) ŵ = 0.15 mm1
β = 112.607 (11)°T = 100 K
V = 1434.2 (8) Å3Rod, yellow
Z = 40.25 × 0.10 × 0.09 mm
Data collection top
Bruker APEX-II CCD
diffractometer
1298 reflections with I > 2σ(I)
φ and ω scansRint = 0.059
Absorption correction: multi-scan
SADABS
θmax = 28.7°, θmin = 4.0°
Tmin = 6.458, Tmax = 7.651h = 1918
8765 measured reflectionsk = 1718
1857 independent reflectionsl = 1010
Refinement top
Refinement on F2153 restraints
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.051H-atom parameters constrained
wR(F2) = 0.142 w = 1/[σ2(Fo2) + (0.0578P)2 + 0.8161P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
1857 reflectionsΔρmax = 0.24 e Å3
133 parametersΔρmin = 0.22 e Å3
Special details top

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

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N10.07197 (10)1.02718 (10)0.37806 (18)0.0301 (3)0.5
H10.0703011.0915940.3767820.036*0.5
C10.15098 (10)0.97792 (11)0.51595 (18)0.0255 (3)
C20.15391 (11)0.87562 (11)0.53043 (19)0.0292 (3)
H20.1010470.8375350.4461240.035*
C30.23302 (11)0.83002 (12)0.6663 (2)0.0334 (4)
H30.2344010.7606560.6758100.040*
C40.31105 (11)0.88544 (13)0.78971 (19)0.0335 (4)
C50.30827 (11)0.98695 (13)0.7767 (2)0.0352 (4)
H50.3612051.0247820.8614310.042*
C60.22905 (12)1.03299 (12)0.6415 (2)0.0324 (4)
H60.2275131.1024130.6335250.039*
C70.07197 (10)1.02718 (10)0.37806 (18)0.0301 (3)0.5
H70.0701681.0967180.3766800.036*0.5
N20.0000000.97709 (13)0.2500000.0256 (4)
C80.39592 (12)0.83321 (16)0.9345 (2)0.0461 (5)
F1A0.4811 (5)0.8775 (5)1.0104 (13)0.093 (3)0.503 (14)
F2A0.4246 (3)0.7440 (4)0.8740 (6)0.0555 (12)0.503 (14)
F3A0.3715 (5)0.7930 (5)1.0663 (8)0.0715 (18)0.503 (14)
F1B0.4531 (4)0.9049 (4)1.0556 (6)0.0572 (12)0.497 (14)
F2B0.4537 (7)0.7947 (11)0.8687 (6)0.109 (4)0.497 (14)
F3B0.3658 (4)0.7795 (4)1.0373 (9)0.0681 (17)0.497 (14)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0390 (8)0.0236 (7)0.0336 (7)0.0025 (6)0.0205 (6)0.0027 (5)
C10.0260 (7)0.0308 (8)0.0232 (7)0.0040 (6)0.0135 (6)0.0029 (5)
C20.0269 (7)0.0316 (8)0.0247 (7)0.0065 (6)0.0051 (6)0.0034 (6)
C30.0328 (8)0.0322 (8)0.0295 (8)0.0030 (7)0.0058 (6)0.0006 (6)
C40.0261 (8)0.0468 (10)0.0263 (8)0.0060 (7)0.0086 (6)0.0021 (6)
C50.0287 (8)0.0481 (10)0.0279 (8)0.0145 (7)0.0097 (6)0.0120 (6)
C60.0372 (9)0.0315 (8)0.0318 (8)0.0102 (7)0.0168 (7)0.0091 (6)
C70.0390 (8)0.0236 (7)0.0336 (7)0.0025 (6)0.0205 (6)0.0027 (5)
N20.0274 (8)0.0280 (9)0.0242 (8)0.0000.0129 (7)0.000
C80.0290 (8)0.0674 (13)0.0328 (9)0.0022 (8)0.0017 (7)0.0056 (8)
F1A0.039 (2)0.070 (3)0.113 (5)0.025 (2)0.034 (2)0.026 (3)
F2A0.0375 (17)0.075 (3)0.0407 (15)0.0222 (16)0.0004 (11)0.0062 (14)
F3A0.083 (4)0.098 (4)0.046 (2)0.054 (3)0.039 (2)0.0273 (19)
F1B0.0353 (19)0.067 (2)0.0432 (17)0.0027 (16)0.0133 (12)0.0087 (13)
F2B0.073 (4)0.196 (9)0.0484 (18)0.090 (5)0.012 (2)0.002 (3)
F3B0.045 (2)0.042 (2)0.086 (3)0.0133 (18)0.0097 (19)0.0318 (19)
Geometric parameters (Å, º) top
C1—C61.397 (2)C5—H50.9500
C1—C21.401 (2)C6—H60.9500
C1—C71.407 (2)C7—N21.3263 (16)
C2—C31.377 (2)C7—H70.9500
C2—H20.9500C8—F2B1.252 (4)
C3—C41.393 (2)C8—F1A1.286 (4)
C3—H30.9500C8—F3B1.288 (5)
C4—C51.390 (3)C8—F3A1.342 (5)
C4—C81.495 (2)C8—F1B1.395 (5)
C5—C61.378 (2)C8—F2A1.427 (5)
C6—C1—C2119.18 (14)C1—C6—H6119.9
C6—C1—C7118.79 (14)N2—C7—C1120.37 (14)
C2—C1—C7122.03 (13)N2—C7—H7119.8
C3—C2—C1120.33 (13)C1—C7—H7119.8
C3—C2—H2119.8C7—N2—N1i117.89 (18)
C1—C2—H2119.8F2B—C8—F3B117.4 (6)
C2—C3—C4120.11 (15)F1A—C8—F3A108.2 (4)
C2—C3—H3119.9F2B—C8—F1B106.0 (5)
C4—C3—H3119.9F3B—C8—F1B102.3 (3)
C5—C4—C3119.83 (15)F1A—C8—F2A102.4 (5)
C5—C4—C8121.66 (15)F3A—C8—F2A96.2 (3)
C3—C4—C8118.52 (16)F2B—C8—C4110.7 (3)
C6—C5—C4120.30 (14)F1A—C8—C4118.8 (3)
C6—C5—H5119.9F3B—C8—C4112.8 (3)
C4—C5—H5119.9F3A—C8—C4114.6 (3)
C5—C6—C1120.25 (15)F1B—C8—C4106.5 (3)
C5—C6—H6119.9F2A—C8—C4113.8 (2)
C6—C1—C2—C30.3 (2)C5—C4—C8—F2B105.1 (9)
C7—C1—C2—C3179.38 (13)C3—C4—C8—F2B75.2 (9)
C1—C2—C3—C40.4 (2)C5—C4—C8—F1A22.0 (8)
C2—C3—C4—C50.7 (2)C3—C4—C8—F1A158.3 (7)
C2—C3—C4—C8179.62 (13)C5—C4—C8—F3B121.0 (4)
C3—C4—C5—C60.5 (2)C3—C4—C8—F3B58.6 (4)
C8—C4—C5—C6179.89 (14)C5—C4—C8—F3A108.0 (4)
C4—C5—C6—C10.2 (2)C3—C4—C8—F3A71.6 (4)
C2—C1—C6—C50.5 (2)C5—C4—C8—F1B9.6 (3)
C7—C1—C6—C5179.13 (12)C3—C4—C8—F1B170.0 (3)
C6—C1—C7—N2175.80 (11)C5—C4—C8—F2A142.7 (3)
C2—C1—C7—N23.86 (18)C3—C4—C8—F2A37.7 (3)
C1—C7—N2—N1i179.16 (13)
Symmetry code: (i) x, y, z+1/2.
(HT33P) top
Crystal data top
C15H10F6N2Dx = 1.583 Mg m3
Mr = 332.25Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pna21Cell parameters from 6485 reflections
a = 11.2082 (4) Åθ = 2.3–30.6°
b = 16.2891 (5) ŵ = 0.15 mm1
c = 15.2689 (7) ÅT = 100 K
V = 2787.67 (18) Å3Plate, yellow
Z = 80.27 × 0.24 × 0.13 mm
F(000) = 1344
Data collection top
Bruker APEX-II CCD
diffractometer
6821 reflections with I > 2σ(I)
φ and ω scansRint = 0.038
Absorption correction: multi-scan
SADABS
θmax = 30.5°, θmin = 2.5°
Tmin = 0.645, Tmax = 0.753h = 1516
36037 measured reflectionsk = 2222
8421 independent reflectionsl = 2121
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.050 w = 1/[σ2(Fo2) + (0.0647P)2 + 1.2842P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.133(Δ/σ)max = 0.001
S = 1.03Δρmax = 0.42 e Å3
8421 reflectionsΔρmin = 0.26 e Å3
444 parametersAbsolute structure: Refined as an inversion twin.
154 restraintsAbsolute structure parameter: 0.5 (8)
Special details top

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

Refinement. Refined as a 2-component inversion twin.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N20.6704 (2)0.86570 (15)0.23643 (16)0.0217 (5)
N10.7356 (2)0.79996 (16)0.21635 (18)0.0273 (5)
H10.8061410.8058950.1918430.033*
C10.6911 (2)0.72100 (18)0.23451 (18)0.0207 (6)
C20.7612 (3)0.65184 (18)0.2148 (2)0.0247 (6)
H20.8382680.6586780.1900170.030*
C30.7180 (3)0.57393 (19)0.2314 (2)0.0255 (6)
H30.7653490.5274320.2170850.031*
C40.6057 (3)0.56284 (18)0.2688 (2)0.0229 (6)
C50.5369 (3)0.63096 (18)0.2894 (2)0.0236 (6)
H50.4607630.6236890.3156490.028*
C60.5780 (3)0.70933 (18)0.2721 (2)0.0235 (6)
H60.5294950.7554550.2856730.028*
C70.6433 (2)1.01008 (17)0.23852 (18)0.0204 (5)
C80.6867 (3)1.08751 (18)0.2160 (2)0.0244 (6)
H80.7633821.0928000.1901080.029*
C90.6182 (3)1.15654 (18)0.2315 (2)0.0256 (6)
H90.6477701.2091870.2158440.031*
C100.5063 (3)1.14928 (18)0.2699 (2)0.0226 (6)
C110.4627 (3)1.07240 (19)0.2935 (2)0.0247 (6)
H110.3863321.0676530.3199690.030*
C120.5305 (3)1.00287 (18)0.2783 (2)0.0240 (6)
H120.5010360.9503940.2947010.029*
C130.7135 (2)0.93787 (17)0.21903 (19)0.0187 (5)
H130.7905540.9431880.1937070.022*
C140.5600 (3)0.47802 (19)0.2834 (2)0.0266 (6)
F10.64434 (19)0.42569 (12)0.30791 (18)0.0450 (6)
F20.4756 (2)0.47425 (13)0.34551 (16)0.0437 (5)
F30.5089 (3)0.44770 (14)0.21128 (16)0.0547 (7)
C150.4316 (3)1.22396 (19)0.2828 (2)0.0285 (6)
F40.4875 (3)1.28266 (14)0.3288 (2)0.0641 (8)
F50.4023 (3)1.26036 (18)0.20802 (17)0.0619 (8)
F60.3314 (3)1.21005 (14)0.3253 (2)0.0719 (10)
N40.4060 (2)0.63372 (14)0.02680 (16)0.0213 (5)
N30.4485 (2)0.55848 (16)0.04156 (18)0.0261 (6)
H3A0.5199420.5520210.0644200.031*
C160.3783 (2)0.48913 (16)0.02033 (18)0.0185 (5)
C170.4274 (2)0.41075 (17)0.02981 (19)0.0204 (5)
H170.5077870.4048410.0486080.024*
C180.3597 (3)0.34178 (16)0.01195 (19)0.0218 (5)
H180.3934110.2886080.0184830.026*
C190.2421 (2)0.35054 (17)0.01563 (18)0.0207 (5)
C200.1932 (2)0.42812 (17)0.0266 (2)0.0226 (6)
H200.1133840.4337510.0465900.027*
C210.2603 (2)0.49723 (16)0.00847 (19)0.0210 (5)
H210.2264020.5502520.0155770.025*
C220.4341 (3)0.77815 (17)0.02572 (18)0.0200 (5)
C230.5038 (2)0.84472 (18)0.0536 (2)0.0218 (6)
H230.5794260.8352220.0797560.026*
C240.4626 (3)0.92424 (19)0.0430 (2)0.0245 (6)
H240.5089200.9691400.0635060.029*
C250.3528 (2)0.93851 (17)0.0021 (2)0.0224 (5)
C260.2850 (3)0.87208 (18)0.0280 (2)0.0246 (6)
H260.2111070.8815260.0566910.030*
C270.3254 (3)0.79285 (18)0.0159 (2)0.0227 (6)
H270.2788300.7479650.0360700.027*
C280.4765 (2)0.69677 (17)0.04278 (19)0.0191 (5)
H280.5545850.6883090.0653200.023*
C290.1681 (3)0.27560 (19)0.0308 (2)0.0264 (6)
F70.2233 (2)0.21865 (13)0.07827 (18)0.0496 (6)
F80.1376 (2)0.23782 (16)0.04374 (15)0.0505 (6)
F90.0658 (2)0.29164 (13)0.0721 (2)0.0568 (7)
C300.3056 (3)1.02408 (19)0.0050 (2)0.0278 (6)
F10A0.2293 (3)1.03321 (16)0.0731 (2)0.0490 (9)0.858 (7)
F11A0.3883 (2)1.07933 (18)0.0172 (4)0.0642 (14)0.858 (7)
F12A0.2404 (4)1.04626 (19)0.0632 (2)0.0584 (12)0.858 (7)
F10B0.348 (3)1.0627 (13)0.0682 (17)0.088 (9)0.142 (7)
F11B0.348 (2)1.0685 (10)0.0662 (15)0.072 (7)0.142 (7)
F12B0.1985 (11)1.0295 (12)0.000 (2)0.073 (7)0.142 (7)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N20.0228 (11)0.0228 (12)0.0193 (11)0.0007 (9)0.0002 (9)0.0001 (9)
N10.0272 (12)0.0252 (13)0.0296 (13)0.0013 (10)0.0045 (11)0.0033 (11)
C10.0202 (13)0.0244 (15)0.0175 (13)0.0020 (10)0.0007 (10)0.0003 (10)
C20.0223 (13)0.0264 (14)0.0253 (14)0.0043 (11)0.0036 (11)0.0012 (11)
C30.0273 (14)0.0240 (14)0.0253 (15)0.0071 (11)0.0007 (12)0.0000 (11)
C40.0228 (13)0.0243 (14)0.0218 (13)0.0021 (11)0.0049 (11)0.0012 (11)
C50.0195 (12)0.0278 (15)0.0234 (14)0.0006 (11)0.0004 (11)0.0002 (11)
C60.0213 (13)0.0229 (13)0.0263 (14)0.0035 (11)0.0034 (11)0.0013 (11)
C70.0197 (12)0.0233 (13)0.0182 (13)0.0005 (10)0.0004 (10)0.0004 (10)
C80.0224 (13)0.0237 (14)0.0271 (14)0.0025 (11)0.0051 (12)0.0032 (11)
C90.0289 (14)0.0200 (13)0.0278 (14)0.0041 (11)0.0039 (12)0.0031 (11)
C100.0256 (14)0.0181 (13)0.0242 (14)0.0006 (10)0.0019 (11)0.0012 (10)
C110.0196 (12)0.0274 (14)0.0272 (15)0.0017 (11)0.0049 (11)0.0010 (12)
C120.0232 (14)0.0195 (13)0.0294 (15)0.0072 (11)0.0039 (12)0.0017 (11)
C130.0176 (12)0.0160 (12)0.0227 (13)0.0003 (10)0.0028 (10)0.0015 (10)
C140.0277 (15)0.0255 (14)0.0268 (15)0.0026 (12)0.0041 (12)0.0009 (11)
F10.0360 (10)0.0278 (10)0.0714 (16)0.0013 (9)0.0081 (11)0.0105 (10)
F20.0479 (12)0.0345 (11)0.0487 (13)0.0088 (9)0.0146 (11)0.0025 (9)
F30.0881 (18)0.0431 (12)0.0331 (11)0.0298 (13)0.0221 (12)0.0018 (10)
C150.0310 (15)0.0245 (15)0.0301 (16)0.0013 (12)0.0036 (13)0.0015 (12)
F40.0759 (18)0.0271 (11)0.089 (2)0.0140 (11)0.0330 (17)0.0203 (12)
F50.0775 (17)0.0706 (17)0.0375 (13)0.0487 (15)0.0010 (13)0.0066 (12)
F60.0672 (16)0.0328 (12)0.116 (3)0.0134 (12)0.0602 (18)0.0052 (14)
N40.0219 (11)0.0194 (11)0.0227 (12)0.0004 (9)0.0011 (9)0.0021 (9)
N30.0230 (12)0.0280 (13)0.0274 (13)0.0038 (10)0.0051 (10)0.0042 (10)
C160.0177 (12)0.0188 (12)0.0189 (13)0.0001 (10)0.0026 (10)0.0021 (9)
C170.0178 (11)0.0220 (13)0.0213 (13)0.0030 (10)0.0002 (10)0.0011 (10)
C180.0234 (13)0.0162 (12)0.0257 (14)0.0022 (10)0.0021 (11)0.0026 (10)
C190.0227 (13)0.0197 (12)0.0197 (13)0.0035 (10)0.0015 (11)0.0014 (10)
C200.0180 (12)0.0235 (13)0.0263 (14)0.0013 (10)0.0030 (11)0.0004 (11)
C210.0201 (12)0.0175 (12)0.0255 (14)0.0014 (10)0.0012 (11)0.0026 (10)
C220.0217 (12)0.0178 (13)0.0204 (13)0.0014 (10)0.0025 (10)0.0020 (10)
C230.0183 (12)0.0214 (13)0.0258 (14)0.0032 (10)0.0012 (11)0.0003 (11)
C240.0226 (13)0.0226 (14)0.0283 (15)0.0041 (11)0.0014 (12)0.0015 (11)
C250.0207 (12)0.0201 (13)0.0264 (14)0.0015 (10)0.0050 (11)0.0020 (10)
C260.0204 (13)0.0271 (15)0.0263 (14)0.0006 (11)0.0015 (11)0.0004 (11)
C270.0214 (12)0.0226 (13)0.0242 (14)0.0025 (11)0.0021 (11)0.0014 (11)
C280.0151 (11)0.0195 (13)0.0227 (13)0.0002 (10)0.0038 (10)0.0002 (10)
C290.0299 (15)0.0241 (15)0.0253 (14)0.0047 (12)0.0001 (12)0.0045 (11)
F70.0603 (14)0.0282 (11)0.0602 (14)0.0150 (10)0.0239 (12)0.0199 (10)
F80.0668 (15)0.0537 (14)0.0310 (11)0.0381 (12)0.0075 (11)0.0020 (10)
F90.0480 (13)0.0331 (11)0.089 (2)0.0112 (10)0.0379 (14)0.0027 (12)
C300.0214 (13)0.0244 (14)0.0375 (17)0.0003 (11)0.0043 (12)0.0023 (12)
F10A0.0640 (19)0.0319 (13)0.0513 (18)0.0136 (13)0.0239 (16)0.0031 (13)
F11A0.0223 (12)0.0228 (13)0.148 (4)0.0038 (9)0.0036 (18)0.014 (2)
F12A0.085 (3)0.0449 (17)0.0449 (17)0.0400 (18)0.0250 (18)0.0110 (13)
F10B0.14 (2)0.035 (11)0.090 (12)0.038 (12)0.066 (13)0.044 (10)
F11B0.100 (15)0.025 (8)0.091 (12)0.030 (9)0.043 (11)0.031 (8)
F12B0.020 (6)0.051 (10)0.15 (2)0.006 (6)0.008 (8)0.021 (12)
Geometric parameters (Å, º) top
N2—C131.299 (4)N3—C161.414 (4)
N2—N11.332 (3)N3—H3A0.8800
N1—C11.407 (4)C16—C171.398 (4)
N1—H10.8800C16—C211.399 (4)
C1—C61.405 (4)C17—C181.383 (4)
C1—C21.406 (4)C17—H170.9500
C2—C31.381 (4)C18—C191.392 (4)
C2—H20.9500C18—H180.9500
C3—C41.395 (4)C19—C201.387 (4)
C3—H30.9500C19—C291.494 (4)
C4—C51.387 (4)C20—C211.382 (4)
C4—C141.490 (4)C20—H200.9500
C5—C61.382 (4)C21—H210.9500
C5—H50.9500C22—C271.394 (4)
C6—H60.9500C22—C231.402 (4)
C7—C81.395 (4)C22—C281.432 (4)
C7—C121.407 (4)C23—C241.385 (4)
C7—C131.446 (4)C23—H230.9500
C8—C91.382 (4)C24—C251.400 (4)
C8—H80.9500C24—H240.9500
C9—C101.390 (4)C25—C261.399 (4)
C9—H90.9500C25—C301.495 (4)
C10—C111.392 (4)C26—C271.380 (4)
C10—C151.490 (4)C26—H260.9500
C11—C121.384 (4)C27—H270.9500
C11—H110.9500C28—H280.9500
C12—H120.9500C29—F71.330 (4)
C13—H130.9500C29—F91.333 (4)
C14—F11.327 (4)C29—F81.339 (4)
C14—F31.335 (4)C30—F12B1.206 (13)
C14—F21.341 (4)C30—F10B1.247 (14)
C15—F61.317 (4)C30—F11A1.305 (4)
C15—F51.328 (4)C30—F12A1.322 (4)
C15—F41.341 (4)C30—F10A1.355 (4)
N4—C281.319 (4)C30—F11B1.387 (14)
N4—N31.334 (3)
C13—N2—N1118.4 (2)C16—N3—H3A120.1
N2—N1—C1119.7 (2)C17—C16—C21119.4 (2)
N2—N1—H1120.2C17—C16—N3119.1 (2)
C1—N1—H1120.2C21—C16—N3121.5 (2)
C6—C1—C2118.9 (3)C18—C17—C16120.3 (3)
C6—C1—N1121.6 (3)C18—C17—H17119.8
C2—C1—N1119.5 (3)C16—C17—H17119.8
C3—C2—C1120.1 (3)C17—C18—C19119.8 (3)
C3—C2—H2119.9C17—C18—H18120.1
C1—C2—H2119.9C19—C18—H18120.1
C2—C3—C4120.7 (3)C20—C19—C18120.3 (3)
C2—C3—H3119.7C20—C19—C29120.4 (3)
C4—C3—H3119.7C18—C19—C29119.3 (3)
C5—C4—C3119.4 (3)C21—C20—C19120.2 (3)
C5—C4—C14121.1 (3)C21—C20—H20119.9
C3—C4—C14119.4 (3)C19—C20—H20119.9
C6—C5—C4120.7 (3)C20—C21—C16120.0 (2)
C6—C5—H5119.7C20—C21—H21120.0
C4—C5—H5119.7C16—C21—H21120.0
C5—C6—C1120.2 (3)C27—C22—C23119.5 (3)
C5—C6—H6119.9C27—C22—C28122.1 (3)
C1—C6—H6119.9C23—C22—C28118.4 (3)
C8—C7—C12119.7 (3)C24—C23—C22120.2 (3)
C8—C7—C13119.7 (3)C24—C23—H23119.9
C12—C7—C13120.6 (3)C22—C23—H23119.9
C9—C8—C7120.0 (3)C23—C24—C25120.0 (3)
C9—C8—H8120.0C23—C24—H24120.0
C7—C8—H8120.0C25—C24—H24120.0
C8—C9—C10120.3 (3)C26—C25—C24119.7 (3)
C8—C9—H9119.9C26—C25—C30120.4 (3)
C10—C9—H9119.9C24—C25—C30119.9 (3)
C9—C10—C11120.2 (3)C27—C26—C25120.1 (3)
C9—C10—C15119.6 (3)C27—C26—H26120.0
C11—C10—C15120.2 (3)C25—C26—H26120.0
C12—C11—C10120.0 (3)C26—C27—C22120.5 (3)
C12—C11—H11120.0C26—C27—H27119.7
C10—C11—H11120.0C22—C27—H27119.7
C11—C12—C7119.8 (3)N4—C28—C22119.2 (2)
C11—C12—H12120.1N4—C28—H28120.4
C7—C12—H12120.1C22—C28—H28120.4
N2—C13—C7119.4 (2)F7—C29—F9106.3 (3)
N2—C13—H13120.3F7—C29—F8105.1 (3)
C7—C13—H13120.3F9—C29—F8105.8 (3)
F1—C14—F3107.5 (3)F7—C29—C19113.3 (3)
F1—C14—F2105.8 (3)F9—C29—C19113.0 (3)
F3—C14—F2105.3 (3)F8—C29—C19112.6 (3)
F1—C14—C4113.1 (3)F12B—C30—F10B112.9 (19)
F3—C14—C4111.6 (3)F11A—C30—F12A108.5 (4)
F2—C14—C4113.0 (3)F11A—C30—F10A105.2 (3)
F6—C15—F5106.8 (3)F12A—C30—F10A103.0 (3)
F6—C15—F4105.3 (3)F12B—C30—F11B104.7 (16)
F5—C15—F4104.3 (3)F10B—C30—F11B102.3 (16)
F6—C15—C10113.8 (3)F12B—C30—C25114.6 (10)
F5—C15—C10112.9 (3)F10B—C30—C25113.0 (10)
F4—C15—C10112.9 (3)F11A—C30—C25113.7 (3)
C28—N4—N3118.0 (2)F12A—C30—C25113.2 (3)
N4—N3—C16119.7 (2)F10A—C30—C25112.4 (3)
N4—N3—H3A120.1F11B—C30—C25108.0 (7)
C13—N2—N1—C1180.0 (3)C21—C16—C17—C180.8 (4)
N2—N1—C1—C61.2 (4)N3—C16—C17—C18178.1 (3)
N2—N1—C1—C2178.8 (3)C16—C17—C18—C190.0 (4)
C6—C1—C2—C30.8 (4)C17—C18—C19—C201.0 (4)
N1—C1—C2—C3179.3 (3)C17—C18—C19—C29177.3 (3)
C1—C2—C3—C40.9 (5)C18—C19—C20—C211.3 (5)
C2—C3—C4—C50.1 (5)C29—C19—C20—C21177.0 (3)
C2—C3—C4—C14178.1 (3)C19—C20—C21—C160.5 (5)
C3—C4—C5—C60.8 (5)C17—C16—C21—C200.5 (4)
C14—C4—C5—C6177.1 (3)N3—C16—C21—C20178.4 (3)
C4—C5—C6—C11.0 (5)C27—C22—C23—C242.6 (4)
C2—C1—C6—C50.2 (4)C28—C22—C23—C24176.2 (3)
N1—C1—C6—C5179.8 (3)C22—C23—C24—C251.9 (5)
C12—C7—C8—C91.1 (5)C23—C24—C25—C260.0 (5)
C13—C7—C8—C9177.6 (3)C23—C24—C25—C30176.7 (3)
C7—C8—C9—C100.4 (5)C24—C25—C26—C271.1 (5)
C8—C9—C10—C110.3 (5)C30—C25—C26—C27175.6 (3)
C8—C9—C10—C15177.5 (3)C25—C26—C27—C220.4 (5)
C9—C10—C11—C120.3 (5)C23—C22—C27—C261.5 (4)
C15—C10—C11—C12177.5 (3)C28—C22—C27—C26177.3 (3)
C10—C11—C12—C70.4 (5)N3—N4—C28—C22178.7 (3)
C8—C7—C12—C111.1 (5)C27—C22—C28—N46.9 (4)
C13—C7—C12—C11177.6 (3)C23—C22—C28—N4171.8 (3)
N1—N2—C13—C7178.7 (3)C20—C19—C29—F7134.3 (3)
C8—C7—C13—N2176.9 (3)C18—C19—C29—F747.4 (4)
C12—C7—C13—N21.8 (4)C20—C19—C29—F913.4 (4)
C5—C4—C14—F1144.8 (3)C18—C19—C29—F9168.4 (3)
C3—C4—C14—F137.3 (4)C20—C19—C29—F8106.5 (3)
C5—C4—C14—F393.9 (4)C18—C19—C29—F871.8 (4)
C3—C4—C14—F384.0 (4)C26—C25—C30—F12B30.6 (18)
C5—C4—C14—F224.6 (4)C24—C25—C30—F12B146.1 (18)
C3—C4—C14—F2157.5 (3)C26—C25—C30—F10B101 (2)
C9—C10—C15—F6175.5 (3)C24—C25—C30—F10B83 (2)
C11—C10—C15—F66.7 (5)C26—C25—C30—F11A147.8 (4)
C9—C10—C15—F562.5 (4)C24—C25—C30—F11A35.5 (5)
C11—C10—C15—F5115.3 (4)C26—C25—C30—F12A87.8 (4)
C9—C10—C15—F455.6 (4)C24—C25—C30—F12A88.9 (4)
C11—C10—C15—F4126.6 (3)C26—C25—C30—F10A28.4 (4)
C28—N4—N3—C16176.2 (3)C24—C25—C30—F10A154.9 (3)
N4—N3—C16—C17175.1 (3)C26—C25—C30—F11B146.9 (13)
N4—N3—C16—C216.0 (4)C24—C25—C30—F11B29.8 (14)
 

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