organic compounds
Orthorhombic polymorph of 4-(2,2′:6′,2′′-terpyridin-4′-yl)aniline
aDepartment of Chemistry, University of St. Joseph, West Hartford, CT, 06032, USA, and bDepartment of Chemistry and Chemical Biology, Harvard University, Cambridge, MA, 02138, USA
*Correspondence e-mail: [email protected]
Crystallographic data for the title compound, C21H16N4, are reported herein. The compound was recrystallized from a methanol/acetonitrile solvent system at 298 K. It crystallizes in the Pca21 at 100 K compared to the previously reported monoclinic polymorph and displays intermolecular hydrogen bonding, through N—H⋯N contacts, and π–π interactions. None of the rings in the structure is coplanar – dihedral angles defined by atoms of the peripheral rings with the central pyridine range from −7.1 (3) to 29.8 (3)°.
Keywords: crystal structure; aniline; terpyridine.
CCDC reference: 2527593
Structure description
a class of compounds that possess at least one C—N bond, are indispensable in organic chemistry. They are utilized extensively as starting materials and reagents in the synthesis of compounds involving reductive amination, nucleophilic substitution and amide coupling reactions (Afanasyev et al., 2019
; Dunetz et al., 2016
; Mondal & Malakar, 2020
). Amines are key moieties in biologically active compounds such as antihistamines, antidepressants and antipsychotics and hence these moieties are featured in a vast number of studies in medicinal and pharmaceutical chemistry (George et al., 2026
; Qurrat-ul-ain et al., 2024
). Expansion of synthetic methodologies for amines has led to a plethora of new structures with a host of chemical and physical properties (Li et al., 2016
; Salvatore et al., 2001
; Umar & Luo, 2023
; Afanasenko et al., 2025
). Amines are also used as building blocks in the synthesis of polymers, sensors and as catalysts (Tanaka, 2023
; Froidevaux et al., 2016
). The properties of amines are due in part to their ability to engage in hydrogen bonding and other intermolecular interactions, and hence there is keen interest in the structural characterization of amines.
The single-crystal X-ray analysis of the title compound, C21H16N4, in the space group Pca21, is reported herein. This compound was recrystallized from a methanol/acetonitrile solvent system at 298 K. This moiety is known for its ability to coordinate metals and is featured in molecules that serve as ligands, polymers and catalysts (Schubert et al. 2011a
,b
; Winter & Schubert, 2020
; Kainat et al., 2024
).
The molecular structure of the title compound is shown in Fig. 1
. It features the 2,2′:6′,2′′ terpyridine moiety in the trans trans conformation with respect to the pyridyl nitrogen atoms. The degree of coplanarity of the rings was determined by dihedral angles formed by atoms of the peripheral rings with atoms in the central pyridine ring. The dihedral angles formed by atoms C9—C10—C11—N3, N1—C5—C6—C7 and C9—C8—C16—C21 were determined to be −7.1 (3), 11.8 (3) and 29.8 (3)° respectively indicating that none of the rings is coplanar; the greatest deviation from planarity evidenced by benzene ring bearing the amino group and the central pyridine.
| Figure 1 Perspective view of the title compound with the atom-numbering scheme showing 50% probability displacement ellipsoids. |
In the crystal, molecules are linked by intermolecular N—H⋯N interactions, forming a three-dimensional network (Table 1
, Figs. 2
and 3
). In addition, the structure includes π–π interactions (Figs. 2
and 3
) with the distances between two pyridine ring planes being 3.6273 (19) Å [slippage = 1.451 (3) Å] and 3.417 (2) Å [slippage = 1.893 (3) Å].
| |||||||||||||||||
| Figure 2 The unit cell showing the intermolecular N—H⋯N and π–π interactions. |
| Figure 3 The three-dimensional supramolecular architecture formed through intermolecular N—H⋯N and π–π interactions. |
Crystals of this compound were previously obtained from a chloroform–methanol solution by Storrier and co-workers, and single-crystal X-ray data in the P21/c were reported (Storrier et al., 1997
). Two crystallographically independent molecules were found in the asymmetric unit of the previous data set. These molecules differ primarily in the orientation of one pyridine ring (Fig. 4
a), with a maximum distance between equivalent atoms (Max·D), calculated using Mercury (Macrae et al., 2020
), of up to 1.0697 Å. In contrast, the current data set contains only one crystallographically independent molecule in the asymmetric unit. This molecule overlaps well with one of the two molecules from the previous data set (Fig. 4
b, Max·D = 0.2102 Å), but shows poor overlap with the other due to a different orientation of one of the pyridine rings (Fig. 4
c, Max·D = 1.1220 Å).
| | Figure 4 (A) The overlap of the two crystallographically independent molecules of the title compound in the unit cell reported by Storrier et al. (1997 |
The title compound is used as a means of introducing the 2,2′:6′,2′′-terpyridine moiety in larger architectures (Trigo-López et al., 2016
; Constable et al., 2014
; Lainé et al., 2002
; Perales et al., 2020
; Dong et al., 2019
). This moiety is known for its ability to coordinate metals and is featured in molecules that serve as ligands, polymers and catalysts (Schubert et al. 2011a
,b
; Winter & Schubert, 2020
; Kainat et al., 2024
).
Synthesis and crystallization
4-(2,2′:6′,2′′-Terpyridin-4′-yl)aniline was purchased from Sigma Aldrich (CAS:178265–65-1) C21H16N4 and used as received. Dark-brown crystals were obtained upon the evaporation of a concentrated solution of the compound in an acetonitrile/methanol solvent system at 298 K. These crystals were characterized by single-crystal X-ray diffraction.
Refinement
Crystal data, data collection and structure details are summarized in Table 2
.
|
Structural data
CCDC reference: 2527593
contains datablock I. DOI: https://doi.org/10.1107/S2414314626001069/bv4057sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314626001069/bv4057Isup3.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314626001069/bv4057Isup3.cml
| C21H16N4 | Dx = 1.387 Mg m−3 |
| Mr = 324.38 | Cu Kα radiation, λ = 1.54178 Å |
| Orthorhombic, Pca21 | Cell parameters from 9698 reflections |
| a = 11.3105 (4) Å | θ = 4.7–66.5° |
| b = 17.3565 (5) Å | µ = 0.67 mm−1 |
| c = 7.9110 (2) Å | T = 100 K |
| V = 1553.01 (8) Å3 | Plate, colorless |
| Z = 4 | 0.14 × 0.12 × 0.10 mm |
| F(000) = 680 |
| Bruker D8 goniometer with Photon III-C14 area detector diffractometer | 2660 reflections with I > 2σ(I) |
| Radiation source: IµS microfocus tube | Rint = 0.043 |
| ω and phi scans | θmax = 66.7°, θmin = 2.6° |
| Absorption correction: multi-scan (SADABS; Krause et al., 2015). | h = −11→13 |
| Tmin = 0.735, Tmax = 0.864 | k = −20→20 |
| 46277 measured reflections | l = −9→9 |
| 2730 independent reflections |
| Refinement on F2 | Hydrogen site location: mixed |
| Least-squares matrix: full | H atoms treated by a mixture of independent and constrained refinement |
| R[F2 > 2σ(F2)] = 0.028 | w = 1/[σ2(Fo2) + (0.0442P)2 + 0.2595P] where P = (Fo2 + 2Fc2)/3 |
| wR(F2) = 0.077 | (Δ/σ)max < 0.001 |
| S = 1.09 | Δρmax = 0.14 e Å−3 |
| 2730 reflections | Δρmin = −0.15 e Å−3 |
| 234 parameters | Absolute structure: Flack x determined using 1188 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons et al., 2013) |
| 1 restraint | Absolute structure parameter: 0.0 (2) |
| Primary atom site location: dual |
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. 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 > 2sigma(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for 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. All non-H atoms were located in difference-Fourier maps, and then refined anisotropically. . Analysis of the using likelihood methods (Hooft, et al., 2008) was performed using PLATON (Spek, 2009). The results also indicated that the had been correctly assigned. The method calculated that the probability that the structure is inverted is 0.2E-10. The carbon-bound H atoms were placed in calculated positions and refined isotropically using the riding model, with C—H distances ranging from 0.95 Å and Uiso(H) set to 1.2 Ueq(C). The nitrogen-bound H atoms were were located in difference-Fourier maps, and then refined freely. |
| x | y | z | Uiso*/Ueq | ||
| N1 | 0.69467 (15) | 0.86075 (10) | 0.3804 (2) | 0.0272 (4) | |
| N2 | 0.39690 (14) | 0.82007 (9) | 0.5146 (2) | 0.0240 (4) | |
| N3 | 0.14473 (15) | 0.70669 (10) | 0.6424 (2) | 0.0301 (4) | |
| N4 | 0.75980 (19) | 0.44154 (11) | 0.9566 (3) | 0.0364 (5) | |
| H4A | 0.822 (3) | 0.4522 (15) | 1.026 (4) | 0.048 (8)* | |
| H4B | 0.715 (2) | 0.3956 (17) | 0.976 (4) | 0.052 (8)* | |
| C1 | 0.7536 (2) | 0.91333 (12) | 0.2907 (3) | 0.0299 (5) | |
| H1 | 0.834151 | 0.903192 | 0.264762 | 0.036* | |
| C2 | 0.70507 (19) | 0.98175 (13) | 0.2328 (3) | 0.0314 (5) | |
| H2 | 0.750727 | 1.017411 | 0.169298 | 0.038* | |
| C3 | 0.5876 (2) | 0.99629 (13) | 0.2710 (3) | 0.0317 (5) | |
| H3 | 0.551174 | 1.042731 | 0.234521 | 0.038* | |
| C4 | 0.52393 (19) | 0.94264 (12) | 0.3625 (3) | 0.0278 (5) | |
| H4 | 0.443089 | 0.951447 | 0.388699 | 0.033* | |
| C5 | 0.58030 (17) | 0.87523 (11) | 0.4158 (3) | 0.0242 (4) | |
| C6 | 0.51511 (17) | 0.81394 (11) | 0.5090 (3) | 0.0235 (4) | |
| C7 | 0.57655 (15) | 0.75270 (12) | 0.5821 (3) | 0.0245 (4) | |
| H7 | 0.660335 | 0.750702 | 0.574948 | 0.029* | |
| C8 | 0.51507 (17) | 0.69450 (11) | 0.6657 (3) | 0.0234 (4) | |
| C9 | 0.39189 (17) | 0.70053 (11) | 0.6684 (3) | 0.0238 (4) | |
| H9 | 0.345844 | 0.662200 | 0.723321 | 0.029* | |
| C10 | 0.33687 (16) | 0.76277 (11) | 0.5906 (3) | 0.0237 (4) | |
| C11 | 0.20508 (16) | 0.76825 (11) | 0.5855 (3) | 0.0248 (4) | |
| C12 | 0.14940 (17) | 0.83300 (12) | 0.5207 (3) | 0.0282 (4) | |
| H12 | 0.194414 | 0.875495 | 0.480903 | 0.034* | |
| C13 | 0.02703 (18) | 0.83466 (12) | 0.5151 (3) | 0.0311 (5) | |
| H13 | −0.013144 | 0.878785 | 0.473220 | 0.037* | |
| C14 | −0.03546 (17) | 0.77184 (12) | 0.5706 (3) | 0.0308 (5) | |
| H14 | −0.119402 | 0.771222 | 0.566808 | 0.037* | |
| C15 | 0.02704 (18) | 0.70949 (13) | 0.6322 (3) | 0.0321 (5) | |
| H15 | −0.016465 | 0.665894 | 0.669645 | 0.039* | |
| C16 | 0.57716 (17) | 0.62892 (11) | 0.7449 (3) | 0.0242 (4) | |
| C17 | 0.69150 (17) | 0.63765 (12) | 0.8096 (3) | 0.0257 (4) | |
| H17 | 0.728850 | 0.686605 | 0.803817 | 0.031* | |
| C18 | 0.7511 (2) | 0.57657 (12) | 0.8817 (3) | 0.0277 (4) | |
| H18 | 0.828548 | 0.584060 | 0.925107 | 0.033* | |
| C19 | 0.69869 (18) | 0.50378 (12) | 0.8915 (3) | 0.0282 (4) | |
| C20 | 0.58456 (18) | 0.49475 (11) | 0.8264 (3) | 0.0293 (5) | |
| H20 | 0.547567 | 0.445650 | 0.830645 | 0.035* | |
| C21 | 0.52508 (17) | 0.55630 (11) | 0.7561 (3) | 0.0264 (4) | |
| H21 | 0.447071 | 0.549060 | 0.714568 | 0.032* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0226 (8) | 0.0295 (9) | 0.0293 (9) | −0.0012 (7) | −0.0001 (7) | −0.0010 (7) |
| N2 | 0.0207 (8) | 0.0242 (8) | 0.0272 (9) | 0.0013 (6) | −0.0004 (7) | −0.0043 (7) |
| N3 | 0.0220 (9) | 0.0302 (9) | 0.0381 (10) | 0.0005 (7) | 0.0006 (8) | −0.0025 (8) |
| N4 | 0.0314 (10) | 0.0337 (10) | 0.0441 (12) | 0.0050 (9) | −0.0015 (9) | 0.0077 (9) |
| C1 | 0.0229 (10) | 0.0368 (11) | 0.0301 (12) | −0.0040 (9) | 0.0009 (9) | −0.0005 (9) |
| C2 | 0.0333 (11) | 0.0323 (11) | 0.0286 (12) | −0.0071 (8) | 0.0015 (9) | 0.0026 (10) |
| C3 | 0.0357 (12) | 0.0276 (10) | 0.0317 (12) | 0.0004 (8) | −0.0013 (9) | 0.0014 (9) |
| C4 | 0.0252 (10) | 0.0279 (10) | 0.0302 (12) | −0.0003 (8) | −0.0001 (8) | −0.0017 (9) |
| C5 | 0.0227 (10) | 0.0261 (10) | 0.0237 (11) | −0.0014 (7) | −0.0015 (8) | −0.0044 (8) |
| C6 | 0.0216 (10) | 0.0243 (9) | 0.0245 (10) | 0.0003 (7) | −0.0009 (9) | −0.0049 (8) |
| C7 | 0.0182 (8) | 0.0266 (9) | 0.0287 (10) | −0.0003 (8) | −0.0010 (9) | −0.0035 (8) |
| C8 | 0.0214 (10) | 0.0238 (10) | 0.0250 (10) | 0.0005 (7) | −0.0014 (8) | −0.0061 (8) |
| C9 | 0.0208 (10) | 0.0241 (10) | 0.0266 (10) | −0.0023 (7) | 0.0007 (8) | −0.0032 (8) |
| C10 | 0.0214 (9) | 0.0240 (10) | 0.0257 (10) | 0.0007 (7) | −0.0007 (8) | −0.0060 (8) |
| C11 | 0.0208 (9) | 0.0271 (10) | 0.0264 (10) | 0.0006 (7) | −0.0008 (8) | −0.0071 (8) |
| C12 | 0.0243 (10) | 0.0290 (11) | 0.0313 (11) | 0.0019 (8) | −0.0014 (9) | −0.0031 (9) |
| C13 | 0.0255 (10) | 0.0344 (11) | 0.0334 (11) | 0.0073 (8) | −0.0044 (9) | −0.0041 (10) |
| C14 | 0.0196 (10) | 0.0388 (12) | 0.0338 (12) | 0.0023 (8) | −0.0012 (9) | −0.0106 (9) |
| C15 | 0.0223 (10) | 0.0340 (12) | 0.0401 (13) | −0.0024 (8) | 0.0010 (9) | −0.0031 (10) |
| C16 | 0.0214 (10) | 0.0251 (10) | 0.0260 (10) | 0.0017 (7) | 0.0015 (8) | −0.0016 (8) |
| C17 | 0.0236 (11) | 0.0248 (10) | 0.0286 (11) | −0.0008 (7) | 0.0004 (9) | −0.0033 (8) |
| C18 | 0.0216 (9) | 0.0328 (10) | 0.0286 (11) | 0.0025 (8) | −0.0025 (8) | −0.0024 (9) |
| C19 | 0.0272 (10) | 0.0301 (11) | 0.0272 (11) | 0.0049 (8) | 0.0035 (9) | 0.0016 (9) |
| C20 | 0.0261 (11) | 0.0250 (10) | 0.0367 (12) | −0.0017 (7) | 0.0030 (9) | 0.0016 (9) |
| C21 | 0.0197 (9) | 0.0281 (10) | 0.0315 (11) | 0.0000 (7) | −0.0001 (8) | −0.0027 (8) |
| N1—C1 | 1.335 (3) | C8—C16 | 1.477 (3) |
| N1—C5 | 1.347 (3) | C9—C10 | 1.391 (3) |
| N2—C6 | 1.342 (2) | C9—H9 | 0.9500 |
| N2—C10 | 1.346 (3) | C10—C11 | 1.494 (2) |
| N3—C15 | 1.334 (3) | C11—C12 | 1.386 (3) |
| N3—C11 | 1.346 (3) | C12—C13 | 1.385 (3) |
| N4—C19 | 1.382 (3) | C12—H12 | 0.9500 |
| N4—H4A | 0.91 (3) | C13—C14 | 1.372 (3) |
| N4—H4B | 0.96 (3) | C13—H13 | 0.9500 |
| C1—C2 | 1.386 (3) | C14—C15 | 1.381 (3) |
| C1—H1 | 0.9500 | C14—H14 | 0.9500 |
| C2—C3 | 1.386 (3) | C15—H15 | 0.9500 |
| C2—H2 | 0.9500 | C16—C21 | 1.394 (3) |
| C3—C4 | 1.382 (3) | C16—C17 | 1.399 (3) |
| C3—H3 | 0.9500 | C17—C18 | 1.380 (3) |
| C4—C5 | 1.398 (3) | C17—H17 | 0.9500 |
| C4—H4 | 0.9500 | C18—C19 | 1.398 (3) |
| C5—C6 | 1.490 (3) | C18—H18 | 0.9500 |
| C6—C7 | 1.396 (3) | C19—C20 | 1.399 (3) |
| C7—C8 | 1.393 (3) | C20—C21 | 1.380 (3) |
| C7—H7 | 0.9500 | C20—H20 | 0.9500 |
| C8—C9 | 1.397 (3) | C21—H21 | 0.9500 |
| C1—N1—C5 | 117.55 (18) | C9—C10—C11 | 120.52 (17) |
| C6—N2—C10 | 117.31 (17) | N3—C11—C12 | 122.48 (17) |
| C15—N3—C11 | 117.18 (17) | N3—C11—C10 | 116.52 (17) |
| C19—N4—H4A | 116.8 (17) | C12—C11—C10 | 120.98 (18) |
| C19—N4—H4B | 116.7 (17) | C13—C12—C11 | 118.87 (19) |
| H4A—N4—H4B | 119 (3) | C13—C12—H12 | 120.6 |
| N1—C1—C2 | 124.3 (2) | C11—C12—H12 | 120.6 |
| N1—C1—H1 | 117.9 | C14—C13—C12 | 119.20 (19) |
| C2—C1—H1 | 117.9 | C14—C13—H13 | 120.4 |
| C3—C2—C1 | 117.7 (2) | C12—C13—H13 | 120.4 |
| C3—C2—H2 | 121.2 | C13—C14—C15 | 118.17 (18) |
| C1—C2—H2 | 121.2 | C13—C14—H14 | 120.9 |
| C4—C3—C2 | 119.4 (2) | C15—C14—H14 | 120.9 |
| C4—C3—H3 | 120.3 | N3—C15—C14 | 124.1 (2) |
| C2—C3—H3 | 120.3 | N3—C15—H15 | 118.0 |
| C3—C4—C5 | 119.0 (2) | C14—C15—H15 | 118.0 |
| C3—C4—H4 | 120.5 | C21—C16—C17 | 117.72 (18) |
| C5—C4—H4 | 120.5 | C21—C16—C8 | 121.52 (18) |
| N1—C5—C4 | 122.12 (19) | C17—C16—C8 | 120.75 (18) |
| N1—C5—C6 | 116.40 (17) | C18—C17—C16 | 121.30 (19) |
| C4—C5—C6 | 121.43 (18) | C18—C17—H17 | 119.3 |
| N2—C6—C7 | 122.87 (18) | C16—C17—H17 | 119.3 |
| N2—C6—C5 | 116.93 (17) | C17—C18—C19 | 120.7 (2) |
| C7—C6—C5 | 120.18 (17) | C17—C18—H18 | 119.7 |
| C8—C7—C6 | 120.03 (16) | C19—C18—H18 | 119.7 |
| C8—C7—H7 | 120.0 | N4—C19—C18 | 121.0 (2) |
| C6—C7—H7 | 120.0 | N4—C19—C20 | 120.7 (2) |
| C7—C8—C9 | 116.78 (18) | C18—C19—C20 | 118.18 (19) |
| C7—C8—C16 | 121.52 (18) | C21—C20—C19 | 120.78 (19) |
| C9—C8—C16 | 121.69 (18) | C21—C20—H20 | 119.6 |
| C10—C9—C8 | 119.84 (18) | C19—C20—H20 | 119.6 |
| C10—C9—H9 | 120.1 | C20—C21—C16 | 121.32 (19) |
| C8—C9—H9 | 120.1 | C20—C21—H21 | 119.3 |
| N2—C10—C9 | 123.10 (17) | C16—C21—H21 | 119.3 |
| N2—C10—C11 | 116.37 (17) | ||
| C5—N1—C1—C2 | 0.4 (3) | C15—N3—C11—C10 | −177.32 (18) |
| N1—C1—C2—C3 | 0.0 (3) | N2—C10—C11—N3 | 172.02 (19) |
| C1—C2—C3—C4 | −0.6 (3) | C9—C10—C11—N3 | −7.1 (3) |
| C2—C3—C4—C5 | 0.6 (3) | N2—C10—C11—C12 | −6.3 (3) |
| C1—N1—C5—C4 | −0.3 (3) | C9—C10—C11—C12 | 174.62 (19) |
| C1—N1—C5—C6 | 177.18 (18) | N3—C11—C12—C13 | 0.3 (3) |
| C3—C4—C5—N1 | −0.2 (3) | C10—C11—C12—C13 | 178.51 (18) |
| C3—C4—C5—C6 | −177.60 (19) | C11—C12—C13—C14 | −1.2 (3) |
| C10—N2—C6—C7 | −2.0 (3) | C12—C13—C14—C15 | 0.8 (3) |
| C10—N2—C6—C5 | 176.47 (17) | C11—N3—C15—C14 | −1.4 (3) |
| N1—C5—C6—N2 | −166.66 (18) | C13—C14—C15—N3 | 0.5 (4) |
| C4—C5—C6—N2 | 10.9 (3) | C7—C8—C16—C21 | −149.1 (2) |
| N1—C5—C6—C7 | 11.8 (3) | C9—C8—C16—C21 | 29.8 (3) |
| C4—C5—C6—C7 | −170.62 (19) | C7—C8—C16—C17 | 30.1 (3) |
| N2—C6—C7—C8 | −0.1 (3) | C9—C8—C16—C17 | −150.9 (2) |
| C5—C6—C7—C8 | −178.45 (19) | C21—C16—C17—C18 | 0.2 (3) |
| C6—C7—C8—C9 | 1.2 (3) | C8—C16—C17—C18 | −179.0 (2) |
| C6—C7—C8—C16 | −179.86 (19) | C16—C17—C18—C19 | 0.2 (3) |
| C7—C8—C9—C10 | −0.3 (3) | C17—C18—C19—N4 | 177.0 (2) |
| C16—C8—C9—C10 | −179.25 (19) | C17—C18—C19—C20 | 0.0 (3) |
| C6—N2—C10—C9 | 2.9 (3) | N4—C19—C20—C21 | −177.7 (2) |
| C6—N2—C10—C11 | −176.15 (17) | C18—C19—C20—C21 | −0.7 (3) |
| C8—C9—C10—N2 | −1.8 (3) | C19—C20—C21—C16 | 1.1 (3) |
| C8—C9—C10—C11 | 177.20 (17) | C17—C16—C21—C20 | −0.9 (3) |
| C15—N3—C11—C12 | 0.9 (3) | C8—C16—C21—C20 | 178.3 (2) |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N4—H4B···N3i | 0.96 (3) | 2.72 (3) | 3.154 (3) | 108.4 (19) |
| Symmetry code: (i) −x+1, −y+1, z+1/2. |
Funding information
The authors acknowledge the support to the X-ray core facility from the Major Research Instrumentation (MRI) Program of the National Science Foundation (NSF) under award No. 2216066.
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