In the title 1:2 co-crystal, C—I⋯N halogen bonds between one of the 1,2,3,5-tetrafluoro-4,6-diiodobenzene molecules and the 5-{[4-(dimethylamino)phenyl]ethynyl}pyrimidine molecule form [110] chains while the second 1,2,3,5-tetrafluoro-4,6-diiodobenzene molecule resides in [100] channels.
Keywords: crystal structure; halogen bonding; co-crystal; 1,2,3,5-tetrafluoro-4,6-diiodobenzene solvate
Abstract
The treatment of 5-{[4-(dimethylamino)phenyl]ethynyl}pyrimidine with a threefold excess of 1,2,3,5-tetrafluoro-4,6-diiodobenzene in dichloromethane solution led to the formation of the unexpected 1:2 title co-crystal, C14H13N3·2CF4I2. In the extended structure, two unique C—I⋯N halogen bonds from one of the 1,2,3,5-tetrafluoro-4,6-diiodobenzene molecules to the pyrimidine N atoms of the 5-{[4-(dimethylamino)phenyl]ethynyl}pyrimidine molecule generate [110] chains and layers of these chains are π-stacked along the a-axis direction. The second 1,2,3,5-tetrafluoro-4,6-diiodobenzene molecule resides in channels formed parallel to the a-axis direction between stacks of 5-{[4-(dimethylamino)phenyl]ethynyl}pyrimidine molecules and interacts with them via C—I⋯π(alkyne) contacts.
Structure description
Halogen bonding is now a widely studied and accepted non-covalent interaction wherein a halogen atom, most commonly iodine, interacts with a Lewis base as halogen-bond acceptor (Cavallo et al., 2016 ▸). This interaction has predictable geometry and has accordingly been incorporated in strategies for the self-assembly of multicomponent molecular solids (Mir et al., 2019 ▸). Among the most studied ditopic halogen-bond donors are the three isomeric diiodotetrafluorobenzenes as the halogen-bond donor ability is increased by substitution of iodobenzenes with electronegative fluorine atoms (Roper et al., 2010 ▸). Herein we report a rare example of inclusion of a 1,2,3,5-tetrafluoro-4,6-diiodobenzene molecule in a co-crystal in which one of the 1,2,3,5-tetrafluoro-4,6-diiodobenzene molecules does not interact with the primary Lewis base.
In the 1:2 co-crystal (Fig. 1 ▸) formed between 5-{[4-(dimethylamino)phenyl]ethynyl}pyrimidine, C14H13N3 (APEP) and 1,2,3,5-tetrafluoro-4,6-diiodobenzene, C6F4I2 (13DIFP), only one of the 13DIFP molecules is halogen bonded to the APEP. The APEP and the halogen-bonded 13DIFP molecule are essentially coplanar: the interplanar angle between the pyrimidine ring and the aminophenyl ring is 4.24 (15)° and the interplanar angle between the pyrimidine ring and the halogen-bonded 13DIFP molecule is 6.63 (15)°. The two unique C—I⋯N halogen bonds that combine to form a zigzag alternating halogen-bonded chain, shown in Fig. 2 ▸, have separations of I1⋯N1 and I2⋯N2i = 2.853 (2) and 2.901 (2) Å and angles C15—I1⋯N1 and C17—I2⋯N2i = 174.8 (9) and 173.8 (8)°, respectively [symmetry code: (i) −1 + x, −1 + y, z]. These distances and angles are similar to those previously reported in the 1:1 co-crystal formed between these two molecules of 2.920 (2) Å and 178.27 (6)° (Nwachukwu et al., 2020 ▸). The Hirshfeld surface (Spackman et al., 2021 ▸) of the halogen-bonded 13DIFB molecules shown in Fig. 3 ▸ highlights these two interactions.
Figure 1.
The molecular structure of the title compound with displacement ellipsoids drawn at 50% and the halogen bond shown as a dashed line.
Figure 2.
Partial view of a chain of halogen-bonded APEP and 13DIFB molecules with pairs of 13DIFB molecules shown between APEP molecules.
Figure 3.
Hirshfeld surface highlighting the halogen-bonding interactions to pyrimidine APEP.
In the extended structure, the APEP molecules are offset π-stacked in a head-to-tail manner such that the halogen-bonded 13DIFB molecules are also alternately π-stacked as shown in Fig. 4 ▸. With this arrangement, the second non-halogen-bonded 13DIFB molecule is located as a π-stacked pair in channels that lie parallel to the a-axis direction (Fig. 4 ▸).
Figure 4.
View of crystal packing of the title compound viewed along the a-axis direction.
The pair of loosely π-stacked 13DIFB molecules interact with the surrounding molecules as shown in the Hirshfeld surface plot in Fig. 5 ▸. This highlights a close I⋯π contact to a neighboring alkyne group with I4⋯C6ii and I4⋯C5ii [symmetry code: (ii) 1 − x, 2 − y, 1 − z] separations of 3.276 (3) and 3.316 (3) Å, respectively. These are significantly less than the sum of the van der Waals radii of 3.68 Å at 89 and 90%, respectively. The second I atom has close I⋯F contacts to two neighboring 13DIFB molecules with I3⋯F6iii and I3⋯F3iv separations of 3.2142 (17) and 3.30129 (15) Å as compared to the sum of the van der Waals radii of 3.38 Å [symmetry codes: (iii) 1 + x, y, z; (iv) x, 1 + y, −1 + z].
Figure 5.
Hirshfeld surface highlighting the close contacts to the solvate 13DIFB molecule.
Synthesis and crystallization
The pyrimidine APEP (8.3 mg) was dissolved in 2 ml of dichloromethane in a screw-cap vial. Three equivalents of 13DIFB were added and the solvent was allowed to slowly evaporate until crystals formed when the vial was sealed to prevent further loss of solvent.
Refinement
Crystal data, data collection and structure refinement details are summarized in Table 1 ▸.
Table 1. Experimental details.
Crystal data | |
Chemical formula | C14H13N3·2C6F4I2 |
M r | 1026.99 |
Crystal system, space group | Triclinic, P
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Temperature (K) | 100 |
a, b, c (Å) | 9.1574 (5), 12.0339 (6), 14.0667 (7) |
α, β, γ (°) | 91.989 (1), 96.924 (1), 102.996 (1) |
V (Å3) | 1496.35 (13) |
Z | 2 |
Radiation type | Mo Kα |
μ (mm−1) | 4.24 |
Crystal size (mm) | 0.52 × 0.28 × 0.20 |
Data collection | |
Diffractometer | Bruker APEXI CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2014 ▸) |
T min, T max | 0.518, 0.746 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 19410, 6594, 6107 |
R int | 0.023 |
(sin θ/λ)max (Å−1) | 0.641 |
Refinement | |
R[F 2 > 2σ(F 2)], wR(F 2), S | 0.020, 0.046, 1.09 |
No. of reflections | 6594 |
No. of parameters | 372 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.69, −0.56 |
Supplementary Material
Crystal structure: contains datablock(s) I. DOI: 10.1107/S2414314622003807/hb4404sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2414314622003807/hb4404Isup2.hkl
Supporting information file. DOI: 10.1107/S2414314622003807/hb4404Isup3.cdx
Supporting information file. DOI: 10.1107/S2414314622003807/hb4404Isup4.cml
CCDC reference: 2164881
Additional supporting information: crystallographic information; 3D view; checkCIF report
Acknowledgments
EB acknowledges the Missouri State University Provost Incentive Fund for the purchase of the X-ray diffractometer used in this contribution.
full crystallographic data
Crystal data
C14H13N3·2C6F4I2 | Z = 2 |
Mr = 1026.99 | F(000) = 948 |
Triclinic, P1 | Dx = 2.279 Mg m−3 |
a = 9.1574 (5) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 12.0339 (6) Å | Cell parameters from 9920 reflections |
c = 14.0667 (7) Å | θ = 2.3–27.1° |
α = 91.989 (1)° | µ = 4.24 mm−1 |
β = 96.924 (1)° | T = 100 K |
γ = 102.996 (1)° | Irregular cut block, colourless |
V = 1496.35 (13) Å3 | 0.52 × 0.28 × 0.20 mm |
Data collection
Bruker APEXI CCD diffractometer | 6594 independent reflections |
Radiation source: fine-focus sealed tube | 6107 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.023 |
Detector resolution: 8.3660 pixels mm-1 | θmax = 27.1°, θmin = 2.2° |
phi and ω scans | h = −11→11 |
Absorption correction: multi-scan (SADABS; Bruker, 2014) | k = −15→15 |
Tmin = 0.518, Tmax = 0.746 | l = −17→18 |
19410 measured reflections |
Refinement
Refinement on F2 | Primary atom site location: dual |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.020 | H-atom parameters constrained |
wR(F2) = 0.046 | w = 1/[σ2(Fo2) + (0.0204P)2 + 0.5553P] where P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max = 0.002 |
6594 reflections | Δρmax = 0.69 e Å−3 |
372 parameters | Δρmin = −0.56 e Å−3 |
0 restraints |
Special details
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)
x | y | z | Uiso*/Ueq | ||
I1 | 0.49323 (2) | 0.32275 (2) | 0.93280 (2) | 0.02074 (5) | |
F1 | 0.21264 (18) | 0.11841 (13) | 0.85256 (11) | 0.0253 (4) | |
N1 | 0.6063 (3) | 0.52854 (19) | 0.84397 (16) | 0.0228 (5) | |
C1 | 0.5221 (3) | 0.5211 (2) | 0.75898 (19) | 0.0203 (6) | |
H1 | 0.442392 | 0.455214 | 0.742023 | 0.024* | |
I2 | 0.02348 (2) | −0.12845 (2) | 0.89212 (2) | 0.01983 (5) | |
F2 | 0.23180 (18) | −0.14839 (13) | 1.08815 (11) | 0.0245 (3) | |
N2 | 0.7521 (3) | 0.70747 (19) | 0.80721 (16) | 0.0228 (5) | |
C2 | 0.7169 (3) | 0.6221 (2) | 0.8639 (2) | 0.0215 (6) | |
H2 | 0.776741 | 0.628608 | 0.924803 | 0.026* | |
I3 | 1.23452 (2) | 0.97142 (2) | 0.34507 (2) | 0.02347 (5) | |
F3 | 0.47643 (17) | −0.00515 (14) | 1.18660 (11) | 0.0240 (3) | |
N3 | −0.0078 (3) | 0.5104 (2) | 0.17456 (18) | 0.0288 (6) | |
C3 | 0.6668 (3) | 0.6985 (2) | 0.7221 (2) | 0.0229 (6) | |
H3 | 0.689419 | 0.757418 | 0.679287 | 0.027* | |
I4 | 0.70571 (2) | 1.18190 (2) | 0.39166 (2) | 0.01903 (5) | |
F4 | 0.58522 (17) | 0.20184 (14) | 1.12306 (11) | 0.0256 (4) | |
C4 | 0.5460 (3) | 0.6057 (2) | 0.69404 (19) | 0.0176 (5) | |
F5 | 1.03550 (16) | 1.15246 (12) | 0.36927 (11) | 0.0219 (3) | |
C5 | 0.4513 (3) | 0.5954 (2) | 0.6039 (2) | 0.0203 (6) | |
F6 | 0.56017 (17) | 0.91354 (14) | 0.39466 (14) | 0.0306 (4) | |
C6 | 0.3687 (3) | 0.5801 (2) | 0.5296 (2) | 0.0199 (5) | |
F7 | 0.67827 (19) | 0.72914 (14) | 0.38368 (16) | 0.0402 (5) | |
C7 | 0.2714 (3) | 0.5631 (2) | 0.44040 (19) | 0.0192 (5) | |
F8 | 0.97066 (19) | 0.75248 (14) | 0.36268 (14) | 0.0338 (4) | |
C8 | 0.2961 (3) | 0.6402 (2) | 0.36941 (19) | 0.0200 (5) | |
H8 | 0.378242 | 0.705295 | 0.381043 | 0.024* | |
C9 | 0.2039 (3) | 0.6246 (2) | 0.2823 (2) | 0.0203 (6) | |
H9 | 0.223836 | 0.678728 | 0.235226 | 0.024* | |
C10 | 0.0812 (3) | 0.5295 (2) | 0.2628 (2) | 0.0202 (5) | |
C11 | 0.0557 (3) | 0.4526 (2) | 0.3355 (2) | 0.0236 (6) | |
H11 | −0.027198 | 0.387958 | 0.324617 | 0.028* | |
C12 | 0.1480 (3) | 0.4689 (2) | 0.4219 (2) | 0.0239 (6) | |
H12 | 0.127870 | 0.415619 | 0.469581 | 0.029* | |
C13 | 0.0052 (4) | 0.6021 (3) | 0.1095 (2) | 0.0473 (10) | |
H13A | −0.025722 | 0.666905 | 0.138573 | 0.071* | |
H13B | −0.060174 | 0.575019 | 0.048978 | 0.071* | |
H13C | 0.110369 | 0.626297 | 0.097130 | 0.071* | |
C14 | −0.1542 (3) | 0.4298 (3) | 0.1657 (3) | 0.0378 (8) | |
H14A | −0.139652 | 0.353862 | 0.180913 | 0.057* | |
H14B | −0.204986 | 0.426549 | 0.099927 | 0.057* | |
H14C | −0.216383 | 0.454809 | 0.210428 | 0.057* | |
C15 | 0.4006 (3) | 0.1649 (2) | 0.98576 (19) | 0.0193 (5) | |
C16 | 0.2772 (3) | 0.0880 (2) | 0.93589 (18) | 0.0179 (5) | |
C17 | 0.2162 (3) | −0.0179 (2) | 0.96755 (18) | 0.0174 (5) | |
C18 | 0.2848 (3) | −0.0463 (2) | 1.05331 (19) | 0.0186 (5) | |
C19 | 0.4083 (3) | 0.0263 (2) | 1.10472 (18) | 0.0176 (5) | |
C20 | 0.4647 (3) | 0.1320 (2) | 1.07115 (19) | 0.0188 (5) | |
C21 | 1.0096 (3) | 0.9535 (2) | 0.36423 (18) | 0.0171 (5) | |
C22 | 0.9461 (3) | 1.0476 (2) | 0.37107 (18) | 0.0162 (5) | |
C23 | 0.7959 (3) | 1.0382 (2) | 0.38056 (18) | 0.0167 (5) | |
C24 | 0.7064 (3) | 0.9287 (2) | 0.3845 (2) | 0.0201 (6) | |
C25 | 0.7661 (3) | 0.8338 (2) | 0.3796 (2) | 0.0246 (6) | |
C26 | 0.9165 (3) | 0.8463 (2) | 0.3691 (2) | 0.0207 (6) |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.02265 (9) | 0.01765 (9) | 0.01957 (9) | −0.00020 (7) | 0.00227 (7) | 0.00274 (7) |
F1 | 0.0277 (9) | 0.0261 (9) | 0.0181 (8) | 0.0016 (7) | −0.0051 (7) | 0.0070 (7) |
N1 | 0.0279 (13) | 0.0181 (11) | 0.0208 (12) | 0.0025 (10) | 0.0016 (10) | 0.0021 (9) |
C1 | 0.0222 (14) | 0.0143 (12) | 0.0224 (14) | 0.0011 (10) | 0.0016 (11) | −0.0002 (10) |
I2 | 0.01730 (9) | 0.02003 (9) | 0.01945 (9) | 0.00009 (7) | 0.00027 (7) | −0.00083 (7) |
F2 | 0.0278 (9) | 0.0195 (8) | 0.0241 (8) | −0.0002 (6) | 0.0041 (7) | 0.0074 (6) |
N2 | 0.0216 (12) | 0.0219 (12) | 0.0209 (12) | −0.0008 (9) | −0.0009 (10) | −0.0006 (10) |
C2 | 0.0225 (14) | 0.0240 (14) | 0.0178 (13) | 0.0069 (11) | 0.0000 (11) | −0.0014 (11) |
I3 | 0.01585 (9) | 0.02765 (10) | 0.03083 (10) | 0.00845 (7) | 0.00992 (7) | 0.00949 (8) |
F3 | 0.0245 (8) | 0.0328 (9) | 0.0135 (7) | 0.0048 (7) | −0.0003 (6) | 0.0060 (7) |
N3 | 0.0262 (13) | 0.0250 (13) | 0.0287 (13) | −0.0008 (10) | −0.0095 (11) | 0.0027 (11) |
C3 | 0.0248 (14) | 0.0195 (13) | 0.0227 (14) | 0.0020 (11) | 0.0021 (11) | 0.0031 (11) |
I4 | 0.02028 (9) | 0.01707 (9) | 0.02182 (9) | 0.00801 (7) | 0.00392 (7) | 0.00142 (7) |
F4 | 0.0234 (8) | 0.0289 (9) | 0.0181 (8) | −0.0044 (7) | −0.0027 (7) | −0.0003 (7) |
C4 | 0.0180 (13) | 0.0159 (12) | 0.0190 (13) | 0.0052 (10) | 0.0018 (10) | −0.0016 (10) |
F5 | 0.0188 (8) | 0.0159 (7) | 0.0305 (9) | 0.0005 (6) | 0.0071 (7) | 0.0045 (6) |
C5 | 0.0225 (14) | 0.0145 (12) | 0.0236 (14) | 0.0043 (10) | 0.0027 (11) | −0.0004 (11) |
F6 | 0.0127 (8) | 0.0240 (9) | 0.0551 (12) | 0.0025 (6) | 0.0081 (8) | 0.0028 (8) |
C6 | 0.0207 (13) | 0.0178 (13) | 0.0222 (14) | 0.0080 (10) | 0.0021 (11) | −0.0034 (11) |
F7 | 0.0230 (9) | 0.0150 (8) | 0.0807 (15) | −0.0028 (7) | 0.0133 (9) | 0.0034 (9) |
C7 | 0.0176 (13) | 0.0199 (13) | 0.0211 (13) | 0.0081 (10) | 0.0004 (11) | −0.0032 (11) |
F8 | 0.0280 (9) | 0.0184 (8) | 0.0603 (12) | 0.0122 (7) | 0.0135 (9) | 0.0039 (8) |
C8 | 0.0162 (13) | 0.0177 (13) | 0.0238 (14) | 0.0012 (10) | 0.0009 (11) | −0.0037 (11) |
C9 | 0.0195 (13) | 0.0187 (13) | 0.0222 (14) | 0.0026 (10) | 0.0034 (11) | 0.0019 (11) |
C10 | 0.0182 (13) | 0.0196 (13) | 0.0225 (14) | 0.0064 (10) | −0.0023 (11) | −0.0016 (11) |
C11 | 0.0206 (14) | 0.0186 (13) | 0.0270 (15) | −0.0023 (11) | −0.0020 (12) | 0.0013 (11) |
C12 | 0.0274 (15) | 0.0175 (13) | 0.0259 (15) | 0.0032 (11) | 0.0023 (12) | 0.0031 (11) |
C13 | 0.057 (2) | 0.041 (2) | 0.0320 (18) | −0.0005 (17) | −0.0209 (17) | 0.0090 (16) |
C14 | 0.0239 (16) | 0.0400 (19) | 0.0421 (19) | 0.0014 (14) | −0.0120 (14) | −0.0023 (15) |
C15 | 0.0206 (13) | 0.0180 (13) | 0.0188 (13) | 0.0020 (10) | 0.0052 (11) | 0.0017 (10) |
C16 | 0.0189 (13) | 0.0228 (13) | 0.0127 (12) | 0.0072 (11) | 0.0004 (10) | 0.0006 (10) |
C17 | 0.0147 (12) | 0.0193 (13) | 0.0167 (13) | 0.0014 (10) | 0.0017 (10) | −0.0020 (10) |
C18 | 0.0191 (13) | 0.0188 (13) | 0.0181 (13) | 0.0026 (10) | 0.0064 (10) | 0.0026 (10) |
C19 | 0.0173 (13) | 0.0235 (14) | 0.0125 (12) | 0.0051 (10) | 0.0026 (10) | 0.0021 (10) |
C20 | 0.0166 (13) | 0.0218 (13) | 0.0158 (13) | 0.0001 (10) | 0.0017 (10) | −0.0018 (10) |
C21 | 0.0126 (12) | 0.0230 (13) | 0.0168 (13) | 0.0052 (10) | 0.0041 (10) | 0.0036 (10) |
C22 | 0.0166 (12) | 0.0167 (12) | 0.0147 (12) | 0.0022 (10) | 0.0020 (10) | 0.0017 (10) |
C23 | 0.0166 (12) | 0.0166 (12) | 0.0184 (13) | 0.0061 (10) | 0.0034 (10) | 0.0003 (10) |
C24 | 0.0123 (12) | 0.0212 (13) | 0.0264 (14) | 0.0025 (10) | 0.0038 (11) | 0.0014 (11) |
C25 | 0.0205 (14) | 0.0151 (13) | 0.0370 (17) | 0.0007 (11) | 0.0053 (12) | 0.0018 (12) |
C26 | 0.0233 (14) | 0.0149 (13) | 0.0256 (14) | 0.0068 (11) | 0.0052 (11) | 0.0031 (11) |
Geometric parameters (Å, º)
I1—C15 | 2.099 (3) | F8—C26 | 1.336 (3) |
F1—C16 | 1.348 (3) | C8—C9 | 1.382 (4) |
N1—C2 | 1.330 (3) | C8—H8 | 0.9500 |
N1—C1 | 1.331 (3) | C9—C10 | 1.405 (4) |
C1—C4 | 1.390 (4) | C9—H9 | 0.9500 |
C1—H1 | 0.9500 | C10—C11 | 1.408 (4) |
I2—C17 | 2.099 (2) | C11—C12 | 1.375 (4) |
F2—C18 | 1.347 (3) | C11—H11 | 0.9500 |
N2—C2 | 1.328 (3) | C12—H12 | 0.9500 |
N2—C3 | 1.335 (4) | C13—H13A | 0.9800 |
C2—H2 | 0.9500 | C13—H13B | 0.9800 |
I3—C21 | 2.074 (2) | C13—H13C | 0.9800 |
F3—C19 | 1.350 (3) | C14—H14A | 0.9800 |
N3—C10 | 1.382 (3) | C14—H14B | 0.9800 |
N3—C13 | 1.451 (4) | C14—H14C | 0.9800 |
N3—C14 | 1.456 (4) | C15—C20 | 1.382 (4) |
C3—C4 | 1.392 (4) | C15—C16 | 1.386 (4) |
C3—H3 | 0.9500 | C16—C17 | 1.383 (4) |
I4—C23 | 2.086 (2) | C17—C18 | 1.382 (4) |
F4—C20 | 1.343 (3) | C18—C19 | 1.371 (4) |
C4—C5 | 1.432 (4) | C19—C20 | 1.383 (4) |
F5—C22 | 1.344 (3) | C21—C26 | 1.387 (4) |
C5—C6 | 1.196 (4) | C21—C22 | 1.389 (4) |
F6—C24 | 1.336 (3) | C22—C23 | 1.378 (4) |
C6—C7 | 1.428 (4) | C23—C24 | 1.394 (4) |
F7—C25 | 1.341 (3) | C24—C25 | 1.376 (4) |
C7—C8 | 1.391 (4) | C25—C26 | 1.377 (4) |
C7—C12 | 1.401 (4) | ||
C2—N1—C1 | 116.2 (2) | N3—C14—H14A | 109.5 |
N1—C1—C4 | 122.7 (2) | N3—C14—H14B | 109.5 |
N1—C1—H1 | 118.7 | H14A—C14—H14B | 109.5 |
C4—C1—H1 | 118.7 | N3—C14—H14C | 109.5 |
C2—N2—C3 | 116.5 (2) | H14A—C14—H14C | 109.5 |
N2—C2—N1 | 126.5 (3) | H14B—C14—H14C | 109.5 |
N2—C2—H2 | 116.7 | C20—C15—C16 | 117.2 (2) |
N1—C2—H2 | 116.7 | C20—C15—I1 | 120.76 (19) |
C10—N3—C13 | 118.6 (2) | C16—C15—I1 | 122.0 (2) |
C10—N3—C14 | 118.7 (3) | F1—C16—C17 | 118.4 (2) |
C13—N3—C14 | 116.1 (3) | F1—C16—C15 | 118.2 (2) |
N2—C3—C4 | 122.2 (3) | C17—C16—C15 | 123.4 (2) |
N2—C3—H3 | 118.9 | C18—C17—C16 | 116.9 (2) |
C4—C3—H3 | 118.9 | C18—C17—I2 | 121.17 (19) |
C1—C4—C3 | 115.8 (2) | C16—C17—I2 | 121.86 (19) |
C1—C4—C5 | 121.1 (2) | F2—C18—C19 | 118.1 (2) |
C3—C4—C5 | 123.1 (2) | F2—C18—C17 | 120.1 (2) |
C6—C5—C4 | 176.0 (3) | C19—C18—C17 | 121.8 (2) |
C5—C6—C7 | 179.2 (3) | F3—C19—C18 | 120.7 (2) |
C8—C7—C12 | 117.9 (2) | F3—C19—C20 | 119.9 (2) |
C8—C7—C6 | 120.9 (2) | C18—C19—C20 | 119.4 (2) |
C12—C7—C6 | 121.2 (3) | F4—C20—C15 | 120.5 (2) |
C9—C8—C7 | 121.6 (2) | F4—C20—C19 | 118.3 (2) |
C9—C8—H8 | 119.2 | C15—C20—C19 | 121.2 (2) |
C7—C8—H8 | 119.2 | C26—C21—C22 | 117.7 (2) |
C8—C9—C10 | 120.7 (3) | C26—C21—I3 | 120.75 (19) |
C8—C9—H9 | 119.6 | C22—C21—I3 | 121.58 (19) |
C10—C9—H9 | 119.6 | F5—C22—C23 | 118.5 (2) |
N3—C10—C9 | 121.2 (3) | F5—C22—C21 | 118.6 (2) |
N3—C10—C11 | 121.4 (2) | C23—C22—C21 | 122.9 (2) |
C9—C10—C11 | 117.4 (2) | C22—C23—C24 | 117.4 (2) |
C12—C11—C10 | 121.5 (2) | C22—C23—I4 | 121.67 (19) |
C12—C11—H11 | 119.3 | C24—C23—I4 | 120.92 (19) |
C10—C11—H11 | 119.3 | F6—C24—C25 | 118.3 (2) |
C11—C12—C7 | 120.9 (3) | F6—C24—C23 | 120.6 (2) |
C11—C12—H12 | 119.6 | C25—C24—C23 | 121.2 (2) |
C7—C12—H12 | 119.6 | F7—C25—C24 | 120.3 (2) |
N3—C13—H13A | 109.5 | F7—C25—C26 | 119.8 (2) |
N3—C13—H13B | 109.5 | C24—C25—C26 | 119.8 (2) |
H13A—C13—H13B | 109.5 | F8—C26—C25 | 118.5 (2) |
N3—C13—H13C | 109.5 | F8—C26—C21 | 120.5 (2) |
H13A—C13—H13C | 109.5 | C25—C26—C21 | 121.0 (2) |
H13B—C13—H13C | 109.5 |
Funding Statement
Funding for this research was provided by: National Science Foundation, Directorate for Mathematical and Physical Sciences (grant No. 1606556).
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I. DOI: 10.1107/S2414314622003807/hb4404sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S2414314622003807/hb4404Isup2.hkl
Supporting information file. DOI: 10.1107/S2414314622003807/hb4404Isup3.cdx
Supporting information file. DOI: 10.1107/S2414314622003807/hb4404Isup4.cml
CCDC reference: 2164881
Additional supporting information: crystallographic information; 3D view; checkCIF report