Bilayer graphene consists of two stacked graphene layers bound together by van der Waals interaction. As the molecular analog of bilayer graphene, molecular bilayer graphene (MBLG) can offer useful insights into the structural and functional properties of bilayer graphene. However, synthesis of MBLG, which requires discrete assembly of two graphene fragments, has proved to be challenging. Here, we show the synthesis and characterization of two structurally well-defined MBLGs, both consisting of two π−π stacked nanographene sheets. We find they have excellent stability against variation of concentration, temperature and solvents. The MBLGs show sharp absorption and emission peaks, and further time-resolved spectroscopic studies reveal drastically different lifetimes for the bright and dark Davydov states in these MBLGs.
Single-layer graphene (SLG) possesses a variety of unique optical and electronic properties, which stem from its mono-atomic network of sp2 carbons1. SLG sheets display an inherent tendency to stack into multilayered structures due to the inter-planar π−π interaction2,3. As the simplest manifestation of such structures, bilayer graphene (BLG) exhibits novel characteristics absent in SLG, such as bandgap opening4, bound excitons5,6, etc., and therefore provides a fertile ground7 for studying two-dimensional materials. Advances in construction and characterization of BLG have also provided theoretical frameworks and instrumental tools in exploring the emerging field of van der Waals heterostructures8,9. However, current methods, such as chemical vapor deposition10,11 and layer-by-layer assembly12, often restrict BLG formation on substrate surfaces. Moreover, tendency of solution-dispersed graphene sheets to self-aggregation2,3 leads to a mixture of multi-layered graphene sheets in solution and merely the dispersions of enriched bilayer or trilayer graphene sheets could be achieved by exfoliation of specific graphite intercalation compounds13.
Nanographene is widely regarded as the molecular model of graphene14. Research on nanographene has provided deep insights into the structure–property relationships of graphene15 and stimulated the field of organic synthesis of graphenic materials with a well-defined architecture16. Although peripheral substitution of nanographene with sterically bulky substituents can preserve its monolayer structure17,18,19, stacking nanographenes in a discrete bilayer form is much more challenging. By using surface supramolecular assembly method, bilayer assembly of nanographene can only be found at liquid/solid interfaces in a very limited amount20,21. This problem is further compounded by the fact that the generated bilayer nanographene is often bound to, and thus difficult to be separated from, the substrate surface. An alternative strategy involves tethering two nanographene sheets together with a covalent linker22,23. However, the resultant product cannot be considered as a molecular cutout of bilayer graphene because the covalent attachment disrupts the van der Waals interactions between the two layers. On the other hand, although stable bilayer nanographene assembled by π−π interaction can qualify as molecular bilayer graphene (MBLG), to the best of our knowledge, such an MBLG has not been obtained in a pure form so far, because the propensity for multilayer stacking of nanographene often results in a dynamic mixture of columnar superstructures with indefinite numbers of layers24,25,26,27,28.
Herein we report the synthesis and characterization of two stable MBLGs [(C114H24R6)2, 1 and (C96H24R6)2, 2, R = mesityl], each formed by π−π stacking of two identical nanographene sheets. Mass spectrometric analysis shows that these MBLGs possess a bilayer structure and can dissociate into the corresponding monolayer when exposed to enhanced laser ablation. Nuclear magnetic resonance (NMR) spectroscopy and single-crystal X-ray diffraction (SXRD) clearly validate their bilayer structures. The interlayer H···H proximity in the bilayer structure is revealed by two-dimensional (2D) nuclear overhauser effect spectroscopy (NOESY). The bilayer structure of MBLGs is highly stable against varying temperature, concentration, and solvent. The absorption and emission of the MBLG shows clear vibronic fine structures. The time-resolved fluorescence (TRPL) and transient absorption (TA) spectroscopies indicate that the bright and dark Davydov states of MBLGs have drastically different lifetimes.
Synthesis and mass spectroscopy of MBLGs
The formation of discrete bilayer stacking requires the balance of the π−π stacking of conjugated π systems with the stereo-hindrance effects of peripheral groups. The peripheral groups have been found to be effective for the modulation of aggregation behavior of nanographenes and a series of literature have been reported on controlling the stacking of nanographenes29,30,31,32,33. For example, the bulky mesityl group has been introduced at the peripheral to hinder interlay stacking17,18,19. On the other hand, on increasing the size of inner nanographene core, the enhanced π−π interaction can outweigh the stereo-hindrance of the mesityl group, facilitating the π−π stacking. Owing to the large size of the mesityl group17,18,34, the π−π stacking of mesityl-functionalized nanographenes demands the interlocking of mesityl groups at both layers along the peripheral. After dimerization, the interlocked peripheral mesityl groups become congested, which could hinder further aggregation to higher oligomers. Therefore, we propose that stacking nanographenes into discrete bilayers could be achieved by making a large nanographene core functionalized with appropriate mesityl groups. Here we choose the nanographene C114 and C96 functionalized with six mesityl groups as the monomer of MBLGs.
Both 1 and 2 were prepared by first synthesizing the polyphenylene precursors with mesityl substituents, followed by dehydrocyclization using the Scholl reaction (Supplementary Figs. 1 and 2, Supplementary Note 1). The m/z values of 1 and 2 in matrix-assisted laser desorption/ionization-time-of-flight mass spectrometry (Fig. 1 and Supplementary Fig. 3) were 4216.3 and 3784.3 Da, respectively, which precisely match the theoretical molecular mass of the corresponding bilayer structures. The experimental isotopic distributions fit the chemical formulae of 1 and 2, respectively (Fig. 1). As the laser power increases, an additional peak appears in the spectrum of 1 at 2107.6 Da, which matches the predicted molecular weight of the monolayer fragment of 1. Similarly, the use of more intense laser results in the generation of the monolayer fragment signal at 1891.7 Da in the spectrum of 2. Both peaks of monolayer fragment become increasingly intense with greater laser power (Fig. 1), suggesting that 1 and 2 exist as van der Waals dimers that can dissociate into the corresponding monomers as a result of laser ablation.
Structure of MBLGs
The peripheral mesityl groups generally adopt a conformation perpendicular to the inner core due to the steric hindrance caused by the ortho methyl substituents17,18,34. When two monolayers self-assembled into the corresponding MBLG, the mirror symmetry along the monomer plane is lost. The perpendicular conformation of mesityl leads to the two ortho methyl groups being in different chemical environments, as one of them points toward (inward-facing) and the other away from (outward-facing) the interlayer spacing of MBLG (Fig. 2). These structural characteristics are clearly revealed by the 1H-NMR spectroscopic data. For example, the 1H-NMR spectrum of 1 consists of seven singlets with the intensity ratio of 2:2:1:1:3:3:3 (Fig. 2c, d). Among them, the two low-field peaks, Ha and Hb, could be assigned to the two inequivalent peripheral hydrogen around the C114 core. Notably, the two mid-field singlets, Hd and Hf, correspond to the two phenyl hydrogen in the mesityl moiety and the three methyl groups are manifested by the three peaks in the high field, corresponding to Hc, He, and Hg. This is consistent with the structure of 1 described above, in which both the two phenyl hydrogen and the two ortho methyl groups in each peripheral mesityl substituent are diastereotopic due to their inward- and outward-spacing orientations (Fig. 2a, b). Not surprisingly, the predicted 1H-NMR spectrum (Supplementary Fig. 4) for the monolayer structure of 1 is composed of only five singlets, due to the gained mirror symmetry along the graphene plane. The same rationale could be used to explain the presence of six distinct high-field singlets in the 1H-NMR spectrum of 2 (Hy, Hn, Hp, Hw, Hr, and Hu), which correspond to the six methyl groups on the two inequivalent peripheral mesityl moieties (Fig. 2e–g). These assignments can be further corroborated by the 13C NMR and 13C-1H correlation spectroscopic spectra of 1 and 2 (Supplementary Figs. 5–8).
The structures of both MLBGs are calculated by using density functional theory (DFT) (Supplementary Fig. 9) and the theoretical NMR spectra computed with the optimized structures (orange lines in Fig. 2d, h) are in good agreement with the experimental patterns (Fig. 2d, h). The presence of a bilayer structure could be further validated by the observation of 2D NOE signals attributable to interlayer proton coupling. For example, the 1H signal of Hj in 2 could be easily identified as the sole triplet (Figs. 2h and 3b). If considering the proton proximity within one layer only, Hj is far away from the all the methyl hydrogens (>5 Å), (Fig. 3a), and therefore would not be able to couple with methyl hydrogen. In comparison, considering the bilayer structure, the inward-facing methyl hydrogen Hn and Hy from one layer are considerably closer to Hj of another layer (Fig. 3a). Indeed, structural modeling of 2 indicates Hj being 2.89 Å away from Hn and 3.00 Å away from Hy. These distances are sufficiently close for spatial H···H coupling, to be detectable by 2D NOESY (Fig. 3b). However, Hj is still too distant from the outward-facing methyl hydrogen Hr and Hu (7.26 and 6.71 Å). This is consistent with the fact that there are only two Hj-related NOE signals in Fig. 3b. The same argument could also be applied to the interpretation of the 2D NOESY of 1 (Supplementary Fig. 10).
The single crystals of both 1 and 2 can be obtained but are highly instable due to efflorescence. We modified peripheral substituents of 2 from mesityl to 2,6-dimethylphenyl and synthesized MBLG 2’ [(C96H24R’6)2, R’ = 2,6-dimethylphenyl] (Supplementary Fig. 11). The bilayer structure of 2’ was also confirmed by mass and NMR spectroscopies (Supplementary Fig. 11). Fortunately, the crystals of 2’ are stable enough to be measured by SXRD (Supplementary Fig. 12), which clearly discloses the bilayer structure of 2’ (Fig. 3c, d). Two cofacially stacked C96 cores in 2’ exhibit a staggered arrangement with an interlayer distance of 3.42 Å and all the 2,6-dimethylphenyl groups adopt a perpendicular conformation as expected (Fig. 3c, d), which are in good agreement with computed structures of 1 and 2 (Supplementary Fig. 9).
Stability of MBLG
Generally, dimeric assemblies based on π−π interactions are often in a dynamic aggregation/disaggregation equilibrium with the corresponding monomers35,36. We thus investigated the stability of the MBLGs by varying the concentration, temperature, and solvent. The 1H NMR (Supplementary Figs. 13 and 14), absorption (Supplementary Figs. 15 and 16), and emission (Supplementary Fig. 17) spectra of 1 and 2 all remain unchanged in the concentration range of 10−4–10−7 mol mL−1, suggesting that neither MBLG undergoes dissociation as a result of dilution. Similarly, the variable-temperature 1H NMR spectra of 1 and 2 show no significant alteration on chemical shifts of 1H signals between 10 and 120 °C, confirming that both MBLG are sufficiently stable in this temperature range (Supplementary Figs. 18 and 19). Even after adding the poor solvent, such as methanol, their absorption and emission spectra remain the same (Supplementary Fig. 20), which rules out the possibility of further π–π stacking of 1 and 2 into trimer or oligomers. The remarkable stability of the MBLGs is further supported by DFT calculations37,38,39,40,41,42,43, which show a large stabilization energy (Supplementary Table 1 and Supplementary Note 3) due to the formation of the bilayer structure.
Optical properties of MBLGs
The photophysical properties of MBLGs were also investigated. The absorption and emission spectra of both 1 and 2 consist of a series of sharp peaks, corresponding to different vibronic lines. According to the Frank–Condon principle, the overall spectral shapes between the absorption and emission spectra exhibit an approximate mirror symmetry (Fig. 4a). The narrow line width (the same as that for single molecules) and Lorentzian line shape suggest the absence of inhomogeneous broadening. Compared with the emission spectral shape of the monolayer counterpart with alkyl groups28,44 (Supplementary Note 4), the first vibronic line intensity is suppressed while the second one is enhanced. Similar spectral evolution was also observed during the formation of molecular π stacks45.
The lifetimes of the excited states are examined by the TRPL and TA spectroscopies. The TRPL kinetics monitored at the main emission peak (Fig. 4b) measures the lifetimes of both samples, which are determined to be 28.5 and 118 ns for 1 and 2, respectively, from bi-exponential fitting (Fig. 4b). On the contrary, the TA measurements (Supplementary Note 5) indicate much longer lifetimes for both MBLGs, i.e., 5.9 and 5.0 μs for 1 and 2, respectively, as shown in Fig. 4c, d. This discrepancy arises from the different nature of the detected states. The TRPL kinetics is mainly sensitive to the bright (emissive) state. On the other hand, the recovery kinetics of the first vibronic state bleach from the TA measurement represents the recovery rate of the ground state after optical excitation. Thus the much longer TA lifetime suggests the presence of dark (non-emissive) states that cause the TA bleach but cannot be detected by the TRPL.
Owing to the van der Waals interaction between two aggregated molecules, originally degenerate excited states from the two monomers will form excited states with different energies (Davydov splitting) after forming a dimer. The optical transition to one of these two Davydov states is allowed, while the transition to the other one is forbidden. The energetics of the allowed and forbidden states depend on the transition dipole alignment46. If the transition dipoles of the two monomers are in parallel alignment (such as in the case of 1 and 2, two monomers stack facially), the upper level is the allowed state (bright state). On the other hand, if the transition dipoles are in in-line alignment, the upper level is the forbidden state (dark state). Owing to the parallel dipole alignment in π–π stacking configuration of 1 and 2, the optical transition from ground state to the upper and lower Davydov states are allowed and forbidden, respectively46. Taking into account this energy splitting, we tentatively attribute the bright and dark state to the upper and lower states, respectively, and the fast energy relaxation from upper to lower states is responsible for the short lifetime of bright states.
We have demonstrated the chemical synthesis of well-defined MBLGs and validated their structures. The MBLGs are remarkably stable, showing no sign of aggregation or dissociation. The MBLGs here offer the well-defined molecular cutout of bilayer graphene and can help in the understanding of structure and properties of bilayer graphene at the molecular level. Further investigation on rational design of MBLGs with tunable size, edge, and twist angle could be readily envisioned, and perhaps even more ambitious goals, such as hetero-structural MBLG and bilayer graphene nanoribbons, could be aimed. Our current study can also inspire the synthesis of other stable bilayer carbonic nanomolecules, such as geodesic polyarenes, carbon nanobelt, and nanorings.
The X-ray crystallographic coordinates for structure reported in this study have been deposited at the Cambridge Crystallographic Data Centre (CCDC), under deposition number 1873164. These data can be obtained free of charge from The Cambridge Crystallographic Data Centre via www.ccdc.cam.ac.uk/data_request/cif.
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This work was financially supported by the National Natural Science Foundation of China (21771155, 21721001), the Ministry of Science and Technology of China (2017YFA0204902), the Fundamental Research Funds for the Central Universities (20720180035), and the Major Science and Technology Project between University-Industry Cooperation in Fujian Province (2016H6023). We acknowledge Zhiwei Lin for the mass spectroscopic measurements and Liubin Feng for variable-temperature NMR measurements.
The authors declare no competing interests.
Peer review information: Nature Communications thanks Xinran Wang and the other anonymous reviewer(s) for their contribution to the peer review of this work. Peer reviewer reports are available.
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