The bottom-up synthesis of structurally well-defined motifs of graphitic materials is crucial to understanding their physicochemical properties and to elicit new functions. Herein, we report the design and synthesis of TriQuinoline (TQ) as a molecular model for pyridinic-nitrogen defects in graphene sheets. TQ is a trimer of quinoline units concatenated at the 2- and 8-positions in a head-to-tail fashion, whose structure leads to unusual aromatisation behaviour at the final stage of the synthesis. The central atomic-sized void endows TQ with high proton affinity, which was confirmed empirically and computationally. TQ•H+ is a two-dimensional cationic molecule that displays both π–π and CH–π contact modes, culminating in the formation of the ternary complex (cycloparaphenylene(CPP) ⊃ (TQ•H+/coronene)) that consists of TQ•H+, coronene (flat), and cycloparaphenylene (CPP) (ring). The water-miscibility of TQ•H+ allows it to serve as an efficient DNA intercalator for e.g. the inhibition of topoisomerase I activity.
Molecular aesthetics is the primary driving force for the intuitive design of xenobiotic molecular entities, which has captivated chemists in the pursuit of novel chemical structures to elicit hitherto unknown physicochemical properties1. The rapidly growing applications of graphitic materials and polyaromatic hydrocarbons (PAHs) are spurring research on exotic polyaromatic molecules that feature skewed and non-flat three-dimensional (3D) architectures (Fig. 1a)2,3,4,5,6,7,8,9,10,11,12,13. Another area of intense research is the modification of the physicochemical properties of PAHs by strategic doping with heteroatoms14,15,16,17. Recent advances in analytical techniques have enabled the detailed analysis of individual heteroatom dopants in graphitic materials, which allows for identification of the distinctive nature of graphitic- and pyridinic-nitrogen sites18,19,20,21. Various methods have emerged for the preparation of graphitic materials with structural defects surrounded by three pyridinic nitrogens22,23,24, paving the way for the introduction of metal cations to impart, e.g., particular catalytic functionality25,26 with prospective applications in energy conversion27 and biocompatible catalysis28. However, the introduction of structurally defined defects is often random, and precise control over the position of such defects remains elusive. We were therefore particularly interested in a bottom-up and structurally defined synthesis of miniaturised graphitic-nitrogen sites that feature an inherent atomic-sized void that may potentially display the characteristic physicochemical properties of small molecules amenable to a variety of spectroscopic analysis techniques.
In the pursuit of such a model compound with minimal two-dimensional (2D) size, herein we describe TriQuinoline (TQ), a molecule that comprises three quinoline units concatenated at the 2- and 8-positions in a head-to-tail fashion (Fig. 1b). TQ represents a pseudo-C3h-symmetric virtually flat molecule with a central defect surrounded by three chemically identical sp2-hybridised nitrogen atoms. The applied indirect synthesis revealed an unusually rapid intermolecular hydride transfer that favours the formation of a quinoline via facilitated aromatisation. The atomic-size void located at the centre of the rigid 2D TQ scaffold displays remarkably high proton affinity, which in turn endows the molecule with water miscibility and the ability to engage in directional complexation with other graphitic materials via π (cation)–π and CH–π interactions.
Synthesis of TQ
Initially, we envisioned a retrosynthetic path that involves the disconnection of the three C–C bonds that interconnect the three quinoline units, which could then be linked via transition-metal-catalysed cross-coupling reactions of plausible intermediates that bear suitable functional groups (Fig. 1c). Indeed, acyclic intermediates that contain three quinoline units were readily accessible by standard synthetic protocols. However, the formation of the last C–C bond was unsuccessful, presumably owing to the rigid flat architecture of TQ, which is probably mismatched with the transition-state structure required for the cross-coupling to proceed. Hence we explored a mechanistically distinct reaction, employing a lithiated species to promote nucleophilic cyclisation, followed by spontaneous oxidative aromatisation to afford TQ (Supplementary Methods). Contrary to the expected lipophilic nature (C log P = 5.96), TQ was isolated solely in the water layer after aqueous work-up, which implies that TQ is readily protonated under neutral conditions. Although the identity of TQ was confirmed after reverse-phase high-performance liquid chromatography purification and lyophilisation, the extremely poor yield (5.7%) prompted us to devise an alternative synthetic strategy. We envisioned that intramolecular imine formation would be feasible given the absence of structural constraints and that a subsequent wall-reinforcement with an ethylene fragment could furnish the TQ framework (Fig. 1c).
On the basis of this assumption, we devised a corresponding synthetic protocol (Fig. 2). The Suzuki–Miyaura cross-coupling29 of 2,8-dichloroquinoline 1 and N-Boc-functionalised phenylboronic acid 2, in which the regioselective introduction of an aniline unit was achieved, afforded 3. Subsequently, the residual C–Cl bond was replaced with a C–B bond using Molander’s borylation protocol30,31, before the thus-obtained intermediate 4 was directly subjected to a second Suzuki–Miyaura cross-coupling with 2-chloro-8-methylquinoline 5 to furnish 6 in 66% yield over two steps. An ensuing two-fold benzylic radical bromination generated dibromide 7, which was exposed to aqueous Na2CO3 at 80 °C to deliver aldehyde 8. Removal of the N-Boc group with trifluoroacetic acid (TFA) led to the formation of the TFA salt of cyclic diquinoline imine (DQ-Im•TFA) 9. From 6 to DQ-Im•TFA 9, each step proceeded smoothly in almost quantitative conversion, which allowed the products to be utilised directly in consecutive steps without purification. n-Butyl vinyl ether (BVE) afforded the two requisite C–C bonds by gentle heating with DQ-Im•TFA 9 via a formal inverse-electron-demand hetero-Diels–Alder (IED-HDA) reaction, followed by a spontaneous elimination/aromatisation sequence, which furnished the desired TQ architecture in 46% yield in four steps. TQ•TFA 10 was extracted into the aqueous phase, and a subsequent lyophilisation allowed its isolation in pure form. The 1H NMR spectrum matched that of the sample obtained via the lithiated intermediate (Supplementary Fig. 1). The resonance of the central proton was observed at >22 ppm, which is comparable to the chemical shift of structurally related macrotricyclic aminopyridines32.
Mechanistic details of the unusual quinoline formation
Notably, the last step of the synthesis of TQ•TFA 10 exhibits unexpected behaviour compared to typical Povarov reactions. The Povarov reaction33,34, which was reported over 50 years ago, is classified as a formal IED-HDA reaction, specifically in the case of N-aryl imines to construct a tetrahydroquinoline (THQ) framework. To our surprise, any traces of the plausible primary and secondary products after elimination, i.e., THQ and 1,2-dihydroquinoline (DHQ), were not detected in the reaction of DQ-Im•TFA 9 and BVE (Supplementary Methods). 1H NMR monitoring of the reaction performed under rigorously inert conditions (degassed CD3CN at 25 °C under Ar in a dry box) allowed for detection of the complete consumption of DQ-Im•TFA 9 after 25 h with concomitant formation of a ca. 1:1 mixture of TQ•TFA 10 and the reduced DiQuinoline-Amine•TFA (DQ-Am•TFA) 11 (Fig. 3a, Supplementary Fig. 9). This observation confirmed the rapid elimination of n-butanol and that DQ-Im•TFA 9 serves not only as a substrate, but also as a hydride acceptor, thus transforming the intermediate DHQ into TQ•TFA. Indeed, DQ-Im•TFA 9 was readily reduced by a Hantzsch ester (25 °C, 10 min), i.e., a typical organic reductant, to generate DQ-Am•TFA 11 (Supplementary Fig. 7), which demonstrates the ability of DQ-Im•TFA 9 to accept a hydride from DHQ to furnish the TQ architecture (Supplementary Methods). Exposure of the aforementioned 1:1 mixture to an ambient atmosphere led to the gradual emergence of complex signals in the 1H NMR spectrum which converged into a single set of signals attributed to TQ•TFA 10, indicating that DQ-Am 11 is susceptible to oxidation by air, resulting in the reversion to DQ-Im•TFA 9 (Supplementary Figs. 7 and 8). This notion was confirmed by monitoring the reaction at 25 °C in air by 1H NMR spectroscopy, which revealed divergent concentrations of DQ-Im•TFA 9 and DQ-Am•TFA 11 under steady formation of TQ•TFA 10 (Fig. 3b, Supplementary Figs. 5 and 6). While BVE underwent undesired competitive hydrolysis to acetaldehyde at 25 °C and was consumed almost entirely within 25 h (Supplementary Fig. 5), the regenerated DQ-Im•TFA 9 slowly reacted even with the significantly less reactive acetaldehyde, resulting in a constant generation of TQ•TFA over time (Fig. 3b, Supplementary Figs. 12 and 13). To further investigate the unusual behaviour of such a continuous Povarov reaction, we carried out density functional theory (DFT) calculations at the ωB97XD/def2-TZVPP/SMD(acetonitrile)//B3LYP-D3/6-31G(d) level of theory in order to define the energy profile using DQ-Im•HCl and methyl vinyl ether (MVE) as model substrates (Supplementary Figs. 50 and 51)35,36,37,38. The initial 1,2-addition of MVE to DQ-Im•HCl, followed by Friedel–Crafts cyclisation to give the THQ intermediate was identified as the most energy-demanding step (∆G‡ = 20.5, 20.2 kcal mol–1). The energy barriers of the subsequent steps, i.e., the elimination of MeOH to afford DHQ (∆G‡ = 14.7 kcal mol–1) followed by hydride transfer from DHQ to DQ-Im (∆G‡ = 7.1 kcal mol–1), were estimated as sufficiently lower than that of the addition of MVE, rendering the THQ and DHQ intermediates virtually undetectable (Fig. 3c, Supplementary Fig. 5). The remarkably facilitated hydride transfer likely originates from the favourable formation of plane-to-plane complex I, which comprises DHQ and DQ-Im via attractive π-contacts, as qualitatively visualised by NCIPLOT (∆E = –30.2 kcal mol–1 after basis set superposition error (BSSE) correction; Supplementary Fig. 52)39. Inspection of the intrinsic reaction coordinate path revealed a change in the plane-to-plane distance of merely 2.0% of the travelling distance of the hydride (Supplementary Fig. 54), affording complex II, which comprises TQ and reduced amine DQ-Am. This unusual non-stop Povarov-type reaction was ascribed to the unique 2D structure of DQ-Im•TFA 9 and found to be also valid for the reaction using a different enol ether, e.g. 1,2-dihydrofuran, giving TQ derivative 12 (Supplementary Methods), which bears a hydroxyethyl group on the periphery that is amenable to further functionalisation (Fig. 3d).
Physicochemical properties of TQ
With a reliable and reproducible synthetic protocol for TQ•TFA 10 in hand, we then turned our attention to the physicochemical properties of the TQ architecture. Numerous attempts at removing the proton captured at the centre of the molecule were unsuccessful, and partial decomposition under basic conditions afforded an unidentified mixture of compounds (e.g. aqueous phase: NaOH, in acetonitrile: from weak Et3N to strong tert-butylimino-tri(pyrrolidino)phosphorene). Intuitively, the central void of the proton-free TQ is expected to be unstable due to repulsive overlap of the lone-pair orbitals of the three nitrogen atoms. Given that the three quinoline units are interconnected to form TQ with no topological constraints (bond angles and lengths), a computational evaluation of hypothetical homodesmotic reactions40 allowed the quantification of the negative contribution of the central part to the thermodynamic stability of TQ (Fig. 4a, Supplementary Methods, Supplementary Figs. 55 and 56). Proton-free TQ was found to be much less stable than the open form (∆H = –25.1 kcal mol–1), presumably due to repulsive interactions between the three nitrogen atoms, which is corroborated by the markedly different calculated energy for the corresponding homodesmotic reaction of protonated TQ•H+ (∆H = 6.4 kcal mol–1). Indeed, the calculated absolute proton affinity of TQ (277.0 kcal mol–1) is significantly higher than that of reference compound 1,8-bis(dimethylamino)naphthalene superbase (proton sponge) 13 (245.3 kcal mol–1) at the same level of theory (Supplementary Methods)41. The kinetic reluctance of TQ•H+ towards proton exchange was experimentally probed by 1H NMR spectroscopy (Fig. 4b). In sharp contrast to the rapid decay of the proton signal of 13•TFA in CD3OD (<30 min), the resonance of TQ•TFA 10 persisted for a significantly longer period (>10% of H+ remained even after 1 week) (Fig. 4b, Supplementary Methods, Supplementary Figs. 14–29). Although TQ•H+ and DQ-Im•H+ share structural characteristics, specifically the size of the cavity surrounded by three sp2-hybridised nitrogen atoms, the retention time of the captured proton was drastically different, i.e., DQ-Im•H+ released the proton virtually instantaneously. Molecular dynamics simulations on TQ•H+ and DQ-Im•H+ by the atom-centred density matrix propagation (ADMP) method suggested that TQ•H+ is structurally more rigid than DQ-Im•H+, which renders the proton captured by the former kinetically less labile (Supplementary Methods, Supplementary Fig. 57)42.
The discernible π-contacts found in complex I (DHQ and DQ-Im in Fig. 3c) by DFT calculations at the hydride transfer step suggest that TQ•H+ is capable of emulating non-covalent interactions to build supramolecular entities (Supplementary Methods)43. Coronene, a neutral π-sheet with a 2D size similar to that of TQ, exhibited a characteristic upfield shift (9.10 to 8.82 ppm) of its 1H NMR (DMSO-d6) spectrum in the presence of TQ•TFA 10, corroborating the formation of plane-to-plane π-complex TQ/coronene 14 (Fig. 5a, b, e)44. Intriguingly, TQ•TFA 10 was also able to form a binary complex via edge-to-plane contacts with cycloparaphenylene (CPP), a ring-shaped π-wall molecule (Fig. 5a, c, f)45,46,47. In contrast to the case of coronene, the signal derived from CPP experienced a downfield shift (from 7.76 to 7.90 ppm), indicating that TQ•H+ is able to magnetically deshield the proton resonance of CPP, similar to the case of CPP ⊃ C60 inclusion complexes48,49. As expected, the complexation of TQ and CPP is size- and shape-specific; no evidence of complexation by 1H NMR analysis was found for the combination of the smaller CPP ring and TQ•TFA 10 (Supplementary Fig. 44), or that of CPP and 2-hydroxyethyl-TQ•TFA 12 (Fig. 5b, i, j, k, Supplementary Fig. 43). These observations strongly imply that the complex presents a spoke-and-rim topology and that CH–π interactions are the primary source of attraction50,51,52. Recurrently, stark differences were observed between TQ and DQ-Im; DQ-Im•TFA 9 failed to form a similar inclusion complex with CPP, even though TQ and DQ-Im share a similar 2D structure (Fig. 5g, h, i, Supplementary Fig. 41). NMR titration together with non-linear regression analysis revealed the formation of the 1:1 and 1:2 inclusion complexes CPP ⊃ TQ•H+ 15 and CPP ⊃ (TQ•H+)2 16, respectively, both of which exhibit comparable association constants K1 = (1.20 ± 0.035) × 103 M–1 and K2 = (1.07 ± 0.011) × 103 M–1 (Fig. 5c, Supplementary Fig. 34)53,54,55. An electrospray ionisation time-of-flight (ESI-TOF) MS analysis provided further experimental support for the formation of inclusion complexes 15 and 16 as well as plane-to-plane complex 14 (Supplementary Figs. 30 and 32).
The favourable interactions in these π-rich molecules were competently reproduced by simulations using density functionals adopting empirical dispersion corrections (Supplementary Methods). Calculations on the cationic complex CPP ⊃ TQ•H+ 15 without a counter anion at the ωB97XD/def2-TZVPP/SMD(acetonitrile)//B3LYP-D3/6-31G(d,p) level of theory provided the free energy of association (∆G‡ = –7.94 kcal mol–1), while the attractive interactions appeared to be overestimated (Supplementary Fig. 58). Decomposition of the interaction energy by symmetry-adapted perturbation theory revealed that dispersion interactions are the main contributor towards the formation of the inclusion complex (Supplementary Fig. 66)56. The upfield and downfield shifts in the spectra of TQ•H+ and CPP, respectively, were qualitatively reproduced through estimation of the shielding effect by gauge-independent atomic orbital calculations (Supplementary Fig. 65). The uniform upfield shift of the proton resonance of TQ•H+ is thereby consistent with the previous literature on the structurally related CH–π-driven inclusion complex. Isobe et al.57,58 reported an inclusion complex featuring a bowl-in-tube topology comprising corannulene (bowl) and cyclic chrysene tetramer (tube), where 10 CH–π hydrogen bonds are responsible for the formation of the inclusion complex. To further probe the potential contribution of CH–π interactions to the formation of CPP ⊃ TQ•H+ 15, we performed a topological analysis on the electron density (ρ(rc)) of the complex in the context of Bader’s quantum theory of atoms-in-molecules (QTAIM)59,60,61. A total of 15 intermolecular bond paths between the peripheral hydrogens of TQ•H+ and proximal carbons of CPP were found together with [3, –1] bond critical points (BCPs) (Fig. 6a). The electron density ρ(rc), the Laplacian of the electron density (∇2ρ(rc)), and the ratio of the curvature of the density at the BCPs (|λ1|/λ3) have been proposed as the principal descriptors to characterise CH–π interactions, and typically fall in the ranges of 0.002 < ρ(rc) < 0.0034, 0.02 < ∇2ρ(rc) < 0.14, and |λ1|/λ3 < 1, respectively57,62,63. Among the 15 intermolecular BCPs found, 9 of these involve the protons at the 4-, 5-, and 6-positions of each quinoline unit that are geometrically close to the π-plane of CPP and satisfy the aforementioned criteria, which strongly suggests that CH–π interactions play a dominant role in the formation of inclusion complex 15 (Fig. 6a). The presence of CH–π interactions was also determined for CPP ⊃ (TQ•H+)2 16 by QTAIM analysis, where the BCPs interconnecting protons at the 5- and 6-positions of each quinoline meet the criteria, and the plane-to-plane distance (3.35 Å) between two TQ•H+ molecules is indicative of attractive π-contacts. The observation of plane-to-plane and edge-to-plane interactions prompted us to construct a ternary inclusion complex composed of three different molecules. The incremental addition of coronene to a mixture of CPP and TQ•TFA in DMSO-d6 led to a significant enhancement of the upfield and downfield shifts of the coronene and CPP signals, respectively, while the resonance of TQ•TFA were shifted even further upfield (Fig. 5d). Assuming the absence of complexation between CPP and coronene due to a size mismatch (Supplementary Fig. 45), the enhanced downfield shift of CPP was exclusively attributed to the formation of ternary complex CPP ⊃ (TQ•H+/coronene) 17, which was supported by ESI-TOF MS measurements (Fig. 5d, Supplementary Fig. 31). As such, TQ•TFA plays a pivotal role as a liaison to assemble CPP and coronene, an inherently non-associative pair of molecules, via simultaneous π–π and CH–π interactions. The corresponding theoretical calculations suggest that the deformation energy of the apparently distorted CPP (∆E = 3.1 kcal mol–1) is compensated by a large negative association energy (∆E = –81.7 kcal mol–1 after BSSE correction) (Supplementary Fig. 64).
π–π interactions in aqueous phase
By taking advantage of the water miscibility of TQ•TFA 10, its π-stacking properties were further assessed in aqueous media by topoisomerase assays (Fig. 6b, Supplementary Methods). The potential applicability of 10 as a DNA intercalator was evaluated against the ability of topoisomerase I to relax supercoiled plasmid DNA. TQ•TFA 10 exhibited an inhibitory effect in a concentration-dependent fashion that is comparable to that of doxorubicin64, a proven intercalator clinically used for cancer chemotherapy, which indicates that TQ•TFA 10 may be a potent intercalator for DNA. This study further revealed that the inhibitory properties of TQ•TFA 10 are distinct from those of structurally familiar DQ-Im•TFA 9, whereby the latter failed to inhibit the DNA relaxation under otherwise identical conditions, which could likely be attributed to a higher conformational flexibility that decreases its propensity towards intercalation.
We have designed and synthesised TriQuinoline (TQ), a 2D miniaturised molecular model for an atomic-sized defect surrounded by pyridinic-nitrogen sites in the structure of graphene. The strategic use of a cyclic DiQuinoline imine (DQ-Im) as the key intermediate was crucial for the high-yielding and reliable access to this unique flat molecule. DQ-Im was subjected to a Povarov reaction, i.e., a formal [4 + 2] cycloaddition reaction with enol ethers, to construct alkoxy tetrahydroquinoline, which resulted in unexpected sequential reactions under mild conditions that culminated in the successful synthesis of TQ. DFT calculations suggested that this unusual non-stop behaviour likely originates from the flat molecular topology, which facilitates the subsequent elimination and hydride transfer processes. TQ exhibits remarkably high proton affinity, whereby the exchange of the captured proton is kinetically hindered. TQ•H+ is amenable to the formation of supramolecular complexes via plane-to-plane and edge-to-plane contact modes. The formation of binary complexes of plane-to-plane TQ•H+/coronene and edge-to-plane inclusion complexes cycloparaphenylene(CPP) ⊃ (TQ•H+)n(1–2) was supported by NMR and ESI-TOF measurements and corroborated by computational calculations. The two-directional non-covalent interactions of TQ•H+ enabled the construction of the ternary complex CPP ⊃ (TQ•H+/coronene), in which TQ serves as a liaison to assemble the inherently non-associative molecules CPP and coronene. Moreover, the non-covalent interactions of water-miscible TQ•H+ are also operative in aqueous media, as confirmed by intercalation assays. Despite their considerable structural similarity, the remarkable features of TQ are absent in DQ-Im, further highlighting the significant impact of the rigid 2D architecture of TQ. These intriguing properties are revealed by the strategic bottom-up synthesis of TQ as a discrete small molecular mimic for a defective graphitic sheet featuring pyridinic nitrogens, allowing for an in-depth understanding of its inherent physicochemical properties. Building up polymeric entities including TQ units as well as potential analogues with distinct defect sizes and topologies will provide more opportunity to identify hitherto unknown functional materials, and as such is currently underway in our laboratory.
Unless otherwise noted, materials were obtained from the commercial suppliers and used without further purification. THF, CH2Cl2, and CH3CN were purified by passing through a solvent purification system. Thin layer chromatography (TLC) was performed on glass TLC plates (0.25 mm) with silica gel 60 F254 and visualised by UV quenching and staining with KMnO4. Flash column chromatography was performed using silica gel (neutral, spherical, 50–60 μm) or CombiFlash systems with a Redisep column. See Supplementary Methods for experimental details.
Infrared (IR) spectra were recorded on a HORIBA FT210 Fourier transform infrared spectrophotometer. NMR spectra were recorded on a Bruker AVANCE III HD400 or a JEOL ECZ-600R spectrometer. Chemical shifts (δ) are given in p.p.m. relative to residual solvent peaks. High-resolution mass spectra were measured on a ThermoFisher Scientific LTQ Orbitrap XL. ESI-TOF-MS spectra of supramolecular complexes were measured on a Bruker micrOTOF-II implemented with a CryoSpray source. Full characterisation data are supplied in Supplementary Methods with 1H, 13C, and 19F NMR spectra (Supplementary Figs. 69–97).
All quantum chemical calculations were performed using the Gaussian 16 programme35. DFT calculations employed an ultrafine integral grid (99 radial shells, 590 angular points). Structural optimisations were conducted at the level of theory specified in Supplementary Methods and the optimised geometries are supplied in Supplementary Tables 5–33. Frequency calculations confirmed the identity of geometry minima (no imaginary frequencies) and transitions states (one imaginary frequency). All transition-state structures were verified to connect the reactant and the product of interest by performing IRC calculations. Zero-point energies and thermal corrections were obtained at 298 K and are unscaled.
Synthesis of 3
A pressure-proof glass vial capable of being sealed with a Teflon cap was charged with 2,8-dichloroquinoline 1 (668 mg, 3.37 mol, 1.0 equiv), 2-(t-butoxycarbonylamino)phenylboronic acid 2 (800 mg, 3.37 mol, 1.0 equiv), K2CO3 (3.50 g, 25.3 mmol, 7.5 equiv), and Pd(PPh3)4 (204 mg, 0.176 mmol, 5.0 mol%) and was evacuated and back-filled with argon. To the mixture, 1,4-dioxane (12.7 mL) and H2O (5.9 mL) were added at 0 °C, and the vial was evacuated, back-filled with argon for several times, and sealed. The reaction mixture was stirred at 85 °C for 15 h. The resulting mixture was diluted with EtOAc/H2O and extracted three times with EtOAc. The combined organic layer was dried over Na2SO4, filtered, and concentrated. The residue was purified by flash column chromatography (n-hexane/EtOAc, 100/0–5.7/1) to give 3 (589 mg, 49% yield).
Synthesis of 6
To an oven dried pressure-proof glass vial capable of being sealed with a Teflon cap were added XPhos Pd G2 (9.97 mg, 0.0127 mmol, 1.0 mol%), XPhos (12.1 mg, 0.0253 mmol, 2.0 mol%), tetrahydroxydiboron (170 mg, 1.90 mmol, 1.5 equiv), KOAc (373 mg, 3.80 mmol, 3.0 equiv), and 3 (450 mg, 1.27 mmol, 1.0 equiv). The vial was sealed, evacuated, and filled with argon (four times). EtOH (12.7 mL) was added at 0 °C via syringe followed by the addition of ethylene glycol (212 μL 3.80 mmol, 3.0 equiv). The mixture was stirred at 80 °C for 1 h. After cooling the mixture to room temperature and removing the seal, K2CO3 (263 mg, 1.90 mmol, 1.50 equiv), PPh3 (9.97 mg, 0.0380 mmol, 3.0 mol%), and Pd(PPh3)4 (73.2 mg, 0.0633 mmol, 5.0 mol%) were added. After adding H2O (3.68 mL) via a syringe, the mixture was left stand for 5 min. After subsequent addition of 2-chloro-8-methylquinoline 5 (248 mg, 1.39 mmol, 1.1 equiv), the vial was sealed, evacuated, and back-filled with argon (four times). The resulting mixture was stirred at 83 °C for 24 h. The reaction mixture was diluted with EtOAc/H2O and extracted three times with EtOAc. The organic layer was dried over Na2SO4, filtered, and concentrated. The residue was purified by flash column chromatography (n-hexane/EtOAc, 100/0–3/1) to give 6 (385 mg, 66% yield).
Synthesis of TQ•TFA 10
To a pressure-proof glass vial capable of being sealed with a Teflon cap were added 6 (40.5 mg, 0.0877 mmol, 1.0 equiv), N-bromosuccinimide (NBS, 38.7 mg, 0.218 mmol, 2.5 equiv), azobisisobutyronitrile (AIBN, 2.55 mg, 0.0155 mmol, 0.18 equiv), and carbon tetrachloride (2.0 mL). The vial was flushed with argon and sealed. The reaction mixture was stirred at 77 °C for 5 h. The resulting mixture was dissolved in CH2Cl2 and subsequently washed with 1 N NaOH (aq.), H2O, and brine. The organic layer was dried over Na2SO4, filtered, and concentrated to afford crude 7 in high purity. To a solution of crude 7 in degassed dioxane (9.0 mL) in a round-bottomed flask, degassed 10% Na2CO3 aq. (10.0 mL) was added. The flask was then equipped with a reflux condenser fitted with a three-way stopcock opened to an argon-filled balloon. The reaction mixture was stirred at 80 °C for 16 h under argon. The resulting mixture was diluted with EtOAc/H2O and extracted three times with EtOAc. The combined organic layer was dried over Na2SO4, filtered, and concentrated to afford crude 8 in high purity, which was used in the next reaction without further purification. To a round-bottomed flask containing crude 8 was added 1,2-dichloroethane (7.42 mL) and trifluoroacetic acid (TFA, 67.2 μL, 0.877 mmol, 10 equiv). The flask was then equipped with a reflux condenser fitted with a three-way stopcock opened to an argon-filled balloon. The reaction mixture was stirred at 70 °C for 18 h under argon. The resulting mixture was concentrated and dissolved in water (16.4 mL). The aqueous solution was lyophilised to afford crude DQ-Im•TFA 9 in high purity. To a round-bottomed flask containing crude DQ-Im•TFA 9 was added CH3CN (8.35 mL) and butyl vinyl ether (BVE, 114 μL, 0.877 mmol, 10 equiv). The reaction mixture was stirred at 45 °C for 25 h. The resulting mixture was concentrated and dissolved in water, and washed with CH2Cl2 (eight times). The aqueous layer was lyophilised to afford 10 in pure form (19.9 mg, 46% yield over four steps from 6).
The X-ray crystallographic coordinates for structures reported in this study have been deposited at the Cambridge Crystallographic Data Centre (CCDC), under deposition numbers CCDC-1909996 (compound 6) and CCDC-1909994 (compound S4). These data can be obtained free of charge from the CCDC via www.ccdc.cam.ac.uk/data_request/cif. All other data support findings of this study are available from the corresponding author upon reasonable request.
Hoffmann, R. & Hopf, H. Learning from molecules in distress. Angew. Chem. Int. Ed. 47, 4474–4481 (2008).
Kawasumi, K., Zhang, Q., Segawa, Y., Scott, L. T. & Itami, K. A grossly warped nanographene and the consequences of multiple odd-membered-ring defects. Nat. Chem. 5, 739–744 (2013).
Matsui, K., Segawa, Y., Namikawa, T., Kamada, K. & Itami, K. Synthesis and properties of all-benzene carbon nanocages: a junction unit of branched carbon nanotubes. Chem. Sci. 4, 84–88 (2013).
Kayahara, E. et al. Synthesis and physical properties of a ball-like three-dimensional π-conjugated molecule. Nat. Commun. 4, 2694 (2013).
Matsui, K., Segawa, Y. & Itami, K. All-benzene carbon nanocages: size-selective synthesis, photophysical properties, and crystal structure. J. Am. Chem. Soc. 136, 16452–16458 (2014).
Hosokawa, T. et al. Synthesis, structures, and properties of hexapole helicenes: assembling six helicene substructures into highly twisted aromatic systems. J. Am. Chem. Soc. 139, 18512–18521 (2017).
Povie, G., Segawa, Y., Nishihara, T., Miyauchi, Y. & Itami, K. Synthesis of a carbon nanobelt. Science 356, 172–175 (2017).
Cui, S. et al. A three-dimensional capsule-like carbon nanocage as a segment model of capped zigzag [12,0] carbon nanotubes: synthesis, characterization, and complexation with C70. Angew. Chem. Int. Ed. 57, 9330–9335 (2018).
Povie, G., Segawa, Y., Nishihara, T., Miyauchi, Y. & Itami, K. Synthesis and size-dependent properties of , , and carbon nanobelts. J. Am. Chem. Soc. 140, 10054–10059 (2018).
Cheung, K. Y. et al. Synthesis of armchair and chiral carbon nanobelts. Chem 5, 838–847 (2019).
Hayase, N., Nogami, J., Shibata, Y. & Tanaka, K. Synthesis of a strained spherical carbon nanocage by regioselective alkyne cyclotrimerization. Angew. Chem. Int. Ed. 58, 9439–9442 (2019).
Sun, Z. et al. Finite phenine nanotubes with periodic vacancy defects. Science 363, 151–155 (2019).
Yano, Y. et al. Living annulative π-extension polymerization for graphene nanoribbon synthesis. Nature 571, 387–392 (2019).
von Grotthuss, E., John, A., Kaese, T. & Wagner, M. Doping polycyclic aromatics with boron for superior performance in materials science and catalysis. Asian J. Org. Chem. 7, 37–53 (2018).
Hu, C., Liu, D., Xiao, Y. & Dai, L. Functionalization of graphene materials by heteroatom-doping for energy conversion and storage. Pro. Nat. Sci.-Mater. 28, 121–132 (2018).
Inagaki, M., Toyoda, M., Soneda, Y. & Morishita, T. Nitrogen-doped carbon materials. Carbon 132, 104–140 (2018).
Xu, H., Ma, L. & Jin, Z. Nitrogen-doped graphene: synthesis, characterizations and energy applications. J. Energy Chem. 27, 146–160 (2018).
Bangert, U. et al. Ion implantation of graphene-toward IC compatible technologies. Nano Lett. 13, 4902–4907 (2013).
Nicholls, R. J. et al. Probing the bonding in nitrogen-doped graphene using electron energy loss spectroscopy. ACS Nano 7, 7145–7150 (2013).
Arenal, R. et al. Atomic configuration of nitrogen-doped single-walled carbon nanotubes. Nano Lett. 14, 5509–5516 (2014).
Warner, J. H., Lin, Y.-C., He, K., Koshino, M. & Suenaga, K. Stability and spectroscopy of single nitrogen dopants in graphene at elevated temperatures. ACS Nano 8, 11806–11815 (2014).
Lin, Y. C. et al. Structural and chemical dynamics of pyridinic-nitrogen defects in graphene. Nano Lett. 15, 7408–7413 (2015).
Jia, Y., Jiang, K., Wang, H. & Yao, X. The role of defect sites in nanomaterials for electrocatalytic energy conversion. Chem 5, 1–27 (2019).
Wang, Y. et al. Catalysis with two-dimensional materials confining single atoms: concept, design, and applications. Chem. Rev. 119, 1806–1854 (2019).
Zhao, Q. et al. Single nickel atoms anchored on nitrogen-doped graphene as a highly active cocatalyst for photocatalytic H2 evolution. ACS Catal. 8, 11863–11874 (2018).
Hou, Y. et al. Atomically dispersed nickel-nitrogen-sulfur species anchored on porous carbon nanosheets for efficient water oxidation. Nat. Commun. 10, 1392 (2019).
Carrero-Sánchez, J. C. et al. Biocompatibility and toxicological studies of carbon nanotubes doped with nitrogen. Nano Lett. 6, 1609–1616 (2006).
Elias, A. L. et al. Viability studies of pure carbon- and nitrogen-doped nanotubes with entamoeba histolytica: from amoebicidal to biocompatible structures. Small 3, 1723–1729 (2007).
Suzuki, A. Cross-coupling reactions of organoboranes: an easy way to construct C-C bonds (nobel lecture). Angew. Chem., Int. Ed. 50, 6722–6737 (2011).
Molander, G. A., Trice, S. L. J. & Dreher, S. D. Palladium-catalyzed, direct boronic acid synthesis from aryl chlorides: a simplified route to diverse boronate ester derivatives. J. Am. Chem. Soc. 132, 17701–11703 (2010).
Molander, G. A., Trice, S. L. & Tschaen, B. A modified procedure for the palladium catalyzed borylation/Suzuki-Miyaura cross-coupling of aryl and heteroaryl halides utilizing bis-boronic acid. Tetrahedron 71, 5758–5764 (2015).
Uchida, N. et al. Synthesis, characterization, and catalytic reactivity of a highly basic macrotricyclic aminopyridine. Org. Lett. 12, 5242–5245 (2010).
Povarov, L. S. α,β-unsaturated ethers and their analogues in reactions of diene synthesis. Russ. Chem. Rev. 36, 656–670 (1967).
Fochi, M., Caruana, L. & Bernardi, L. Catalytic asymmetric aza-Diels–Alder reactions: the Povarov cycloaddition reaction. Synthesis 46, 135–157 (2014).
Gaussian 16, Revision A.03 (Gaussian, Inc., Wallingford, CT, 2016). See the Supplementary Information for the full citation.
Weigend, F. & Ahlrichs, R. Balanced basis sets of split valence, triple zeta valence and quadruple zeta valence quality for H to Rn: Design and assessment of accuracy. Phys. Chem. Chem. Phys. 7, 3297–3305 (2005).
Marenich, A. V., Cramer, C. J. & Truhlar, D. G. Universal solvation model based on solute electron density and on a continuum model of the solvent defined by the bulk dielectric constant and atomic surface tensions. J. Phys. Chem. B 113, 6378–6396 (2009).
Grimme, S., Ehrlich, S. & Goerigk, L. Effect of the damping function in dispersion corrected density functional theory. J. Comput. Chem. 32, 1456–1465 (2011).
Contreras-Garcia, J. et al. Nciplot: A program for plotting non-covalent interaction regions. J. Chem. Theory Comput. 7, 625–632 (2011).
Wheeler, S. E. Homodesmotic reactions for thermochemistry. WIREs Comput. Mol. Sci. 2, 204–220 (2012).
Ishikawa, T. Superbases for Organic Synthesis: Guanidines, Amidines, Phosphazenes and Related Organocatalysts (John Wiley & Sons, Chichester, UK, 2009).
Iyengar, S. S., Schlegel, B. & Voth, G. A. Atom-centered density matrix propagation (ADMP): generalizations using bohmian mechanics. J. Phys. Chem. A 107, 7269–7277 (2003).
Iyoda, M. & Shimizu, H. Multifunctional π-expanded oligothiophene macrocycles. Chem. Soc. Rev. 44, 6411–6424 (2015).
Hahn, R. et al. Donor-acceptor interactions between cyclic trinuclear pyridinate gold(I)-complexes and electron-poor guests: nature and energetics of guest-binding and templating on graphite. Chem. Sci. 9, 3477–3483 (2018).
Jasti, R., Bhattacharjee, J., Neaton, J. B. & Bertozzi, C. R. Synthesis, characterization, and theory of -, -, and cycloparaphenylene: carbon nanohoop structures. J. Am. Chem. Soc. 130, 17646–17647 (2008).
Takaba, H., Omachi, H., Yamamoto, Y., Bouffard, J. & Itami, K. Selective synthesis of cycloparaphenylene. Angew. Chem. Int. Ed. 48, 6112–6116 (2009).
Yamago, S., Watanabe, Y. & Iwamoto, T. Synthesis of cycloparaphenylene from a square-shaped tetranuclear platinum complex. Angew. Chem., Int. Ed. 49, 757–759 (2010).
Iwamoto, T., Watanabe, Y., Sadahiro, T., Haino, T. & Yamago, S. Size-selective encapsulation of C60 by cycloparaphenylene: formation of the shortest fullerene-peapod. Angew. Chem. Int. Ed. 50, 8342–8344 (2011).
Yamago, S., Kayahara, E. & Iwamoto, T. Organoplatinum-mediated synthesis of cyclic π-conjugated molecules: towards a new era of three-dimensional aromatic compounds. Chem. Rec. 14, 84–100 (2014).
Yamamoto, Y., Tsurumaki, E., Wakamatsu, K. & Toyota, S. Nano-saturn: experimental evidence of complex formation of an anthracene cyclic ring with C60. Angew. Chem. Int. Ed. 57, 8199–8202 (2018).
Toyota, S. & Tsurumaki, E. Exploration of nano-saturns: a spectacular sphere-ring supramolecular system. Chem. Eur. J. 25, 6878–6890 (2019).
Sala, P. D. et al. Tuning cycloparaphenylene host properties by chemical modification. J. Org. Chem. 82, 9885–9889 (2017).
Thordarson, P. Determining association constants from titration experiments in supramolecular chemistry. Chem. Soc. Rev. 40, 1305–1323 (2011).
Brynn Hibbert, D. & Thordarson, P. The death of the job plot, transparency, open science and online tools, uncertainty estimation methods and other developments in supramolecular chemistry data analysis. Chem. Commun. 52, 12792–12805 (2016).
Thordarson, P. Supramolecular.org. (2015). http://supramolecular.org
Jeziorski, B., Moszynski, R. & Szalewicz, K. Perturbation theory approach to intermolecular potential energy surfaces of van der Waals complexes. Chem. Rev. 94, 1887–1930 (1994).
Matsuno, T., Fujita, M., Fukunaga, K., Sato, S. & Isobe, H. Concyclic CH–π arrays for single-axis rotations of a bowl in a tube. Nat. Commun. 9, 3779 (2018).
Y. Xu & M. von Delius. The supramolecular chemistry of strained carbon nanohoops. Angew. Chem. Int. Ed. https://doi.org/10.1002/anie.201906069.
T. A. K. AIMAll (Version 19.02.13). TK Gristmill Software (Overland Park KS, 2019) (aim.tkgristmill.com).
Bader, R. F. W. A quantum theory of molecular structure and its applications. Chem. Rev. 91, 893–928 (1991).
Matta, C. F. & Boyd, R. J. The Quantum Theory of Atoms in Molecules: From Solid State to DNA and Drug Design (Wiley-VCH, Weinheim, 2007).
Koch, U. & Popelier, P. L. A. Characterization of C–H-O hydrogen bonds on the basis of the charge density. J. Phys. Chem. 99, 9747–9754 (1995).
Takahashi, O., Kohno, Y. & Saito, K. Molecular orbital calculations of the substituent effect on intermolecular CH/π interaction in C2H3X–C6H6 complexes (X=H, F, Cl, Br, and OH). Chem. Phys. Lett. 378, 509–515 (2003).
Tacar, O., Sriamornsak, P. & Dass, C. R. Doxorubicin: an update on anticancer molecular action, toxicity and novel drug delivery systems. J. Pharm. Pharmacol. 65, 157–170 (2013).
This work was financially supported by a Grant-in-Aid for Scientific Research B (KAKENHI 17H03025) and Precisely Designed Catalysts by Customised Scaffolding (KAKENHI JP16H01043) from the JSPS. Dr. Naoki Takizawa is gratefully acknowledged for carrying out the topoisomerase I assays. The authors thank Dr. Tomoyuki Kimura for the X-ray crystallographic analysis of compounds 6 and S4, as well as Dr. Ryuichi Sawa, Ms. Yumiko Kubota, and Dr. Kiyoko Iijima for technical assistance with the NMR analyses. Part of the computation resources in this work was provided by the Research Centre for Computational Science, Okazaki, Japan.
The authors declare no competing interests.
Peer review information: Nature Communications thanks the anonymous reviewers for their contribution to the peer review of this work. Peer reviewer reports are available.
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
About this article
Cite this article
Adachi, S., Shibasaki, M. & Kumagai, N. TriQuinoline. Nat Commun 10, 3820 (2019). https://doi.org/10.1038/s41467-019-11818-1
Triquinoline‐ versus Fullerene‐Based Cycloparaphenylene Ionic Complexes: Comparison of Photoinduced Charge‐Shift Reactions
Chemistry – A European Journal (2020)