Two-dimensional (2-D) micro- and nano-architectures are attractive because of their unique properties. However, the formation of 2-D supramolecular highly symmetrical structures with considerable control is still a major challenge. Here we present a simple approach for the preparation of regular and homogeneous 2-D fluorescent square non-crystallization micelles with conjugated diblock copolymers PPV12-b-P2VP n through a process of dissolving–cooling–aging. The scale of the formed micelles can be controlled by the ratio of PPV/P2VP blocks and the concentration of the solution. The results reveal that the micelles of PPV12-b-P2VP n initially form 1-D structures and then grow into 2-D structures in solution, and the growth is driven by intermolecular π–π interactions with the PPV12 blocks. The formation of 2-D square micelles is induced by herringbone arrangement of the molecules, which is closely related to the presence of the branched alkyl chains attached to conjugated PPV12 cores.
Recently, nanoscale two-dimensional (2-D) self-assembled architectures have attracted a great deal of attention as a result of their unique properties caused by their ultrathin and flat morphologies1,2. Over the past few years, various 2-D micro- and nano-structures have been constructed from inorganic metal salts3, organic molecules4, proteins5,6, and block copolymers (BCPs)7,8,9. Crystallization-driven processes have a vital role in the methods of preparing 2-D assembled nanostructures and the shapes of these formed 2-D nanostructures are thus controlled by the symmetry of the unit cell. Therefore, 2-D micro- and nano-architectures with high symmetry, including equilateral triangular, square-shaped, hexagonal, and circular assemblies, are still not commonly reported. As the creation of synthetic 2-D materials represents an attractive challenge that is ultimately driven by their prospective uses in, e.g., electronics, biomedicine, catalysis, sensing, and as membranes for separation and filtration1, the acquisition of uniform 2-D assemblies with regular shapes has more important significance. Achieving such a uniform architecture through non-crystallization-derived approaches10 such as Van der Waals’ forces, hydrophilic/hydrophobic interactions, hydrogen bonds, and π–π interactions is particularly challenging and fascinating.
A bottom-up self-assembly of crystalline homopolymers and BCPs is a commonly used strategy to prepare 2-D materials. In recent years, a series of analogous polymers have been studied for 2-D self-assembly and colloidally stable 2-D nanostructures were formed in solution11,12,13. The classic poly(ferrocenyldimethylsilane) BCPs have been reported to yield unique 2-D lenticular and rectangular platelet block co-micelles with semi-crystalline properties by a seeded growth processes14,15,16. However, it is difficult to substantially control the structures of the 2-D BCP micelles and non-crystalline regular 2-D architectures are still rarely obtained. Generating uniform colloidally stable 2-D micro- and nano- structures with controlling their shapes and dimensions remains a key challenge.
Poly(p-phenylenevinylene) (PPV) is a classic type of π-conjugated material with fascinating optical and electronic properties17,18. The long conjugated backbones allow PPV to achieve tight intermolecular packing19 with intense sheet-forming assembling tendency. However, although a certain number of PPV-based BCPs have been utilized as building blocks for supramolecular self-assembly20,21,22,23, few of them, which were always irregular one-dimensional (1-D) cylindrical or fibrous, took advantage of the packing inclination to achieve uniform 2-D aggregates24.
In this study, we combine PPV blocks and poly (2-vinyl pyridine) (P2VP) to build amphiphilic diblock copolymers PPV12-b-P2VP n with sheet–coil-type structures, and colloidally stable 2-D fluorescent square micelles are formed in certain solvents, such as isopropanol, with easy approaches. Low dispersities and good dimensional control over the 2-D square micelles are achieved by adjusting the ratio of P2VP and PPV blocks, as well as the concentration of the solution. Furthermore, it is found that the assembly process of 2-D micelles in solution is closely related to the temperature. Intermolecular π–π interactions and the herringbone molecular arrangement have vital roles in the formation of square micelle films. In view of the perfect optical and electronic properties of PPV blocks, the forming square micelles should have potential applications in the fields of organic field effect transistors (OFET), organic photovoltaic (OPV), and biosensing.
Design and preparation of π-conjugated BCP micelles
To use π–π interactions to form self-assembly architectures, we built a series of supramolecular BCPs composed of a core-forming π-conjugated block of poly(2,5-di(2′-ethylhexyloxy)-1,4-phenylenevinylene) (PPV) and a corona block of P2VP. The PPV-aldehyde homopolymer was prepared by Siegrist polycondensation and the monomer number of PPV block was calculated to be 12 by nuclear magnetic resonance (NMR), whose polydispersity was 1.05 determined by gel permeation chromatography (GPC). Then a series of diblock copolymers PPV12-b-P2VP n (the subscript n describes the number-average degrees of polymerization) were synthesized through quenching the anionic polymerization of P2VP with the PPV aldehyde. The degrees of polymerization n was 12, 16, 22, 36, 46, and 71 (RPPV/P2VP, which was short for the block ratio of PPV and P2VP, was nearly 1 : 1, 1 : 1.3, 1 : 2, 1 : 3, 1 : 4, and 1 : 6), respectively, characterized by NMR and GPC (see Supplementary Methods, Supplementary Figs. 1–12, and Table 1).
The obtained BCPs PPV12-b-P2VP n are typically amphiphilic, so they should readily assemble into ordered micelles in solutions. To confirm whether the π–π interactions of PPV12 blocks could take effect in the formation of the simple micelles, we attempted to dissolve the BCPs PPV12-b-P2VP n in 2-propanol (2-PrOH), which is a selective solvent for P2VP coronas. The solution was heated at 85 °C for 45 min, then it was slowly cooled to room temperature (25 °C) followed by aging for 24 h. Interestingly, uniform regular 2-D square micelles of PPV12-b-P2VP n were yielded from the resulting colloidally stable solutions by this simple approach, which was observed under transmission electron microscopy (TEM).
Tuning the scale of the square micelles by varying building block ratios and solution concentrations
It was observed that the scales and morphologies of the achieved 2-D micelles were influenced by the ratio of PPV/P2VP blocks (RPPV/P2VP). The number-average diagonal length (Dn, the subscripts refer to the number-average diagonal length) of the square micelles formed in a 0.01 mg ml−1 solution of PPV12-b-P2VP12 (RPPV/P2VP = 1 : 1) in 2-PrOH was calculated to be 2,747 nm (Fig. 1a,b and Supplementary Fig. 13a) and the diagonal length dispersity Dw/Dn = 1.02 (Dw = 2,788 nm, Dw is the weight-average diagonal length, Fig. 1c). These square micelles were highly flexible and they were easily cracked and wrinkled because of membrane mechanics (Supplementary Fig. 14a); these features were clearly observed by scanning electron microscope (SEM) (Supplementary Fig. 16). Meanwhile, the large square micelles readily packed with each other. As the value of RPPV/P2VP was reduced, the scales of the formed square micelles clearly decreased, and the uniformity and integrity of the micelles improved. Dn of square micelles of PPV12-b-PPV16 (RPPV/P2VP = 1 : 1.3, 0.01 mg ml−1 in 2-PrOH solution) reduced to 1,808 nm (Dw = 1,815 nm, Dw/Dn = 1.00, Fig. 1d–f, and Supplementary Fig. 13b and 14b). When RPPV/P2VP was reduced to nearly 1 : 2, the obtained square micelles of PPV12-b-P2VP22 from 0.05 mg ml−1 2-PrOH solution showed decreased scales (Dn = 542 nm), improved homogeneity (Dw/Dn = 1.02, D w = 551 nm), and more uniform morphologies (Fig. 1g–i and Supplementary Fig. 14c). While the Dn of square micelles of PPV12-b-P2VP36 (RPPV/P2VP = 1 : 3, prepared in 0.05 mg ml−1 2-PrOH solution) was only 235 nm with a narrow diagonal length dispersity (Dw/Dn = 1.01, Dw = 238 nm, Fig. 1j–l and Supplementary Fig. 14d). When RPPV/P2VP was reduced to 1 : 4, 2-D supramolecular architectures were also achieved from 2-PrOH solution, but the scales of the formed nanostructures were not smaller than those of PPV12-b-P2VP36 and the morphologies were no longer regular squares (Supplementary Fig 15a, b). In addition, the PPV12-b-P2VP71 (RPPV/P2VP = 1 : 6) assembled into noticeably smaller irregular dot-like 2-D nanostructures (Supplementary Fig 15c, d).
The heights of the 2-D square micelles of the copolymers with RPPV/P2VP of 1 : 1, 1 : 1.3, 1 : 2, and 1 : 3 were calculated to be 10, 12, 14, and 16 nm (Fig. 2a–d), respectively, using atomic force microscopy (AFM). It was obvious that the thickness of the formed platelet 2-D square micelles of PPV12-b-P2VP n increased as the length of the corona of P2VP was increased. Furthermore, the structure of the conjugated PPV12 block and P2VP n blocks were optimized by density functional theory (DFT) calculations with the Gaussian09 suite25 of programs at the B3LYP level of theory26,27 with the 6-31G* basis set28,29,30. The PPV12 block exhibited a rigid skeleton and its length was calculated as 7.97 nm (Fig. 2e), whereas the length of the coronas of the P2VP12, P2VP16, P2VP22, and P2VP36 blocks were estimated to be 2.97, 3.86, 5.33, and 8.70 nm, respectively (Supplementary Fig. 17). The flexible P2VP coronas are probably folded and twined on the upper and lower surfaces of the formed platelet 2-D square micelles, and a single layer of PPV12 blocks packing with each other by π–π interactions are sandwiched in as illustrated in Fig. 2f, and these conformations are consistent with the individual thicknesses of the 2-D square micelles determined from AFM measurements.
To control the scales of the achieved square micelles, we investigated the concentration dependence of the self-assembly of PPV12-b-P2VP n and the results were quite interesting. The scales of the formed square micelles of PPV12-b-P2VP12 were significantly concentration dependent. The diagonal length of the square micelles formed in 0.01 mg ml−1 2-PrOH solution was ~2,750 nm, whereas the diagonal length was reduced to ~2,000 nm when the concentration of the solution was decreased to 0.005 mg ml−1. When the solution concentration was halved again, the diagonal length of the formed square micelles further decreased to only ~1,300 nm (Fig. 3a–c). The obtained 2-D square micelles of PPV12-b-P2VP16 also showed concentration dependence, but the phenomenon was not as obvious as it was with the micelles of PPV12-b-P2VP12. The diagonal length of the square micelles formed in 2-PrOH solutions continued to decrease as the concentrations were halved from 0.01 all the way to 0.0025 mg ml−1; the diagonal lengths were ~ 1,950, 1,400, and 850 nm (Fig. 3d–f), respectively. When the P2VP blocks of the copolymer became longer, meaning that the RPPV/P2VP value was <1 : 2, the concentration dependence of the self-assembly of PPV12-b-P2VP n disappeared completely. For example, the diagonal lengths of the square micelles of PPV12-b-P2VP22 formed in 2-PrOH solution with concentrations of 0.05, 0.02, and 0.01 mg ml−1 were all ~550 nm with very little variation. Similarly, the diagonal lengths of the formed square micelles of PPV12-b-P2VP36 were only ~250 nm, which did not change when the concentration of the solution was decreased.
The formation of square micelles should be driven by both hydrophobic interaction and π-π interactions of the PPV12 blocks. The aggregation of the diblocks driven by hydrophobic interaction should be dynamic with regard to the exchange of the unimer building blocks, as reported previously31. As the dynamic process is significantly dependent on the concentration, the scales of 2-D square micelles formed by PPV12-b-P2VP12 and PPV12-b-P2VP16 with low RPPV/P2VP, whose dynamic exchanges were strong, were clearly influenced by the solution concentration. When the length of the P2VP corona was increased, the dynamic effect caused by hydrophobic interactions could be suppressed, so the process became slow enough compared with the time scale of the formation of the square platelet micelles. Therefore, the scales of the platelet square micelles of PPV12-b-P2VP22 and PPV12-b-P2VP36 with longer coronas did not vary as the solution concentration changed.
Growth process of the platelet 2-D square micelles
Owing to the π-conjugated PPV12 blocks, the PPV12-b-P2VP n copolymers displayed strong fluorescence in solutions. Compared with PPV12-b-P2VP n in 0.01 mg ml−1 tetrahydrofuran (THF) solutions, where the copolymer molecules dissolved completely, PPV12-b-P2VP n , after aging in 0.01 mg ml−1 2-PrOH solutions for 48 h, displayed blue-shifted emission peaks (at ~549 nm with a shoulder at 584 nm), broader photoluminescence (PL) and lower fluorescence quantum efficiency (ΦF, changed from 0.27 to 0.09) (Supplementary Fig 18). These changes originated from the formation of platelet 2-D square micelles in 2-PrOH solutions, which was induced by the aggregation of the copolymer molecules. The significant changes in fluorescence of PPV12-b-P2VP12 and PPV12-b-P2VP16 in solution are likely caused by the stacking of the large square micelles. In addition, if a drop of a solution of PPV12-b-P2VP12 or PPV12-b-P2VP16 that had been aged for 24 h was placed on a slide, the fluorescent square micelles could be clearly observed in solution by laser scanning confocal microscopy (LSCM). The Dn of the 2-D square micelles of PPV12-b-P2VP12 (RPPV/P2VP = 1 : 1) in 0.01 and 0.005 mg ml−1 solution of 2-PrOH was calculated to be 3,200 nm and 2,300 nm, respectively, and those of PPV12-b-P2VP16 (RPPV/P2VP = 1 : 1.3) in 0.01 and 0.005 mg ml−1 solution of 2-PrOH was calculated to be 2,200 and 1,700 nm. From the LSCM images, although the scales of the observed fluorescent square micelles were larger than those observed by TEM because of light scattering, the concentration dependence of the scales of 2-D square micelles formed by PPV12-b-P2VP12 and PPV12-b-P2VP16 with low RPPV/P2VP were clearly observed, which was consistent with the results observed by TEM (Fig. 4). However, in a solution of PPV12-b-P2VP22 solution, only the fluorescent dot-like structures could be seen by LSCM, because the formed 2-D square micelles were too small to be clearly observed (Supplementary Fig 19). These observations from LSCM indicated that the self-assembly process of the formation of the 2-D square micelles occurred in the solution instead of occurring as the solvent evaporated, which had been further confirmed by the observation of the freely moving fluorescent aggregates in 0.01 mg ml−1 solutions of PPV12-b-P2VP12, although the square shape of the aggregates was unable to be clearly observed because of the scattering effect and the moving effect (Supplementary Movie 1).
To explore the assembly process of the BCPs from 2-PrOH solutions, we measured the UV-Vis absorption spectra of PPV12-b-P2VP n in 2-PrOH as the temperature and the aging time changed (Fig. 5). All four PPV12-b-P2VP n BCPs showed a peak at ~ 474 nm in the UV-Vis spectra in 2-PrOH solutions at 85 °C, whereas the molecules of PPV12-b-P2VP n should completely dissolve in the solution and move freely. As the temperature of the solution decreased to 40~50 °C, the UV-Vis spectra of PPV12-b-P2VP n exhibited slight bathochromic shifts of 6~8 nm, which indicated that the copolymer molecules had begun to aggregate in the solution because of the hydrophobic interactions of the conjugated core and the side alkyl chains. Then, the intensities of the spectra at 440~445 nm began to increase as the temperature was further decreased and the peaks almost disappeared when the solutions were cooled down to near room temperature. Finally, after aging for ~20 h, the peaks at ~440 nm appeared in the UV-Vis spectra of the copolymer solutions. The significant blue-shift of the absorption spectra suggested the formation of 2-D square micelles was driven by H-aggregation of the PPV12 blocks21,23. The UV-Vis spectra of PPV12-b-P2VP n solutions all tended to change similarly as the solutions were cooled from 85 °C to room temperature, indicating that aggregation of the molecules was affected by the temperature. During the aging period at room temperature, the differences in the UV-Vis spectra of the four copolymers were substantially different from each other, suggesting their aggregating rates were different. For PPV12-b-P2VP12 and PPV12-b-P2VP16 with low RPPV/P2VP values, the absorption intensities between 460 and 480 nm were lower in solutions that had aged for 1 h compared with those that had just been cooled to room temperature, and this deviation was caused by H-aggregation of the approaching molecules. After aging for 3 h, the intensities of the UV-Vis spectra between 460 and 480 nm continued to decline, but after aging for 20 h, the spectra of the high concentration solutions of PPV12-b-P2VP12 and PPV12-b-P2VP16 stopped changing; the intensities of the UV-Vis spectra of solutions with low concentrations decreased only a little in the 460~480 nm region compared with those of the solutions aged for 3 h. These changes may have occurred because square micelles of PPV12-b-P2VP12 and PPV12-b-P2VP16 with low RPPV/P2VP formed from solutions with high concentration tended to pile with each other, and the piling effect became weaker in solutions of low concentration, which was consistent with the TEM observations. PPV12-b-P2VP22 in a 2-PrOH solution can assemble into homogeneous and regular 2-D square micelles with no concentration dependence. Therefore, the intensities of its UV-Vis spectra in the 460~480 nm region could decline completely after aging regardless of concentration. The trends observed in the intensities of the peaks in the UV-Vis spectra of PPV12-b-P2VP36 in solution were similar with those of low concentration solution spectra of PPV12-b-P2VP16. The incompletely declined intensities in the 460~480 nm region compared with PPV12-b-P2VP22 should be attributed to the partial H-aggregation caused by the longer P2VP coronas. The change in the spectra indicated that the aggregation rate of the PPV12-b-P2VP36 molecules was far slower than that of the other three copolymers; the complete aggregation of PPV12-b-P2VP36 molecules in 0.01 mg ml−1 2-PrOH solution required 72 h of aging.
Based on the changes in the UV-Vis spectra caused by changes in temperature and time, we could conclude that the molecular aggregation in solution was likely dependent on the temperature before cooling to room temperature. To characterize the aggregating state in solution during the cooling process, the 0.02 mg ml−1 2-PrOH solution of PPV12-b-P2VP22 was examined by dynamic light scattering (DLS) and static light scattering (SLS), because molecules of PPV12-b-P2VP22 in 2-PrOH could completely assemble by H-aggregation without micelles stacking and concentration dependence. When we measured the solution by DLS above 50 °C, the scattering strength was too low to be detected, showing that the molecules in solution appeared dissolved with no particles large enough, which is consistent with the UV-Vis results. When the solution was cooled to 48 °C, features could be observed in the DLS detect and the hydrodynamic diameter (Dh) of the aggregated micelle particles was determined to be 61.3 nm. As the solution was cooled to room temperature, the aggregated particle size quickly increased to 208.8 nm. Then, the rate of the increase in particle size slowed and the Dh changed from 208.8 nm to 275.7 nm after aging for 3.5 h (Supplementary Fig. 20). It is well known that the morphologies of particles can be revealed by their Rg/Rh values (the morphology factor, ρ) in solution32. At a certain temperature, we calculated the Dhθ of the sample solution at different angles by DLS and extrapolated the value of Rh, and the root mean square radius of gyration (Rg) was calculated by measuring the SLS results of the copolymer solution at multiple angles less than 90°33. The Rg and Rh values of the self-assembled 2-D square micelles of PPV12-b-P2VP22 in the 2-PrOH solution after aged for 2 days were measured as 196.7 and 144.9 nm, respectively, and the Rg/Rh value was calculated to be 1.36. According to previous reports34,35, the Rg/Rh value of spherical micelles is close to 1, whereas that of coiled micelles and rigid rods are larger than 1.5. As we know, the researches of the Rg/Rh value about 2-D materials, especially those with regular shapes, were rarely reported. The analogous particle system was regular stars whose value of Rg/Rh was 1.33, which was surely close to the value of the formed 2-D square micelles. The geometric symmetry of 2-D platelet square micelles is higher than that of a coil but lower than that of a sphere, so it is reasonable that the Rg/Rh value of these micelles is between 1 and 1.5. The Rg/Rh values of particles assembled in solutions at 45, 40, 35, 30, and 25 °C were measured to be 2.59, 2.17, 2.00, 1.74, and 1.41, respectively (Fig. 6c, Supplementary Fig. 21, and Table 3). It could be concluded that the originally formed aggregates of PPV12-b-P2VP22 at around 45 °C were one-dimensional, because the Rg/Rh value was much larger than 2. As the temperature of the solution decreased, the Rg/Rh value of the aggregates in solution gradually decreased until it reached ~1.36, which was the morphology factor (ρ) of 2-D platelet square micelles. The trend in the change in the Rg/Rh values at different temperatures revealed that the molecules of PPV12-b-P2VP n initially assembled into 1-D aggregates in the solution during the cooling process, gradually grew into 2-D square micelles as the solution cooled to room temperature, and finally the scales of the 2-D square micelles increased slowly during the aging period35.
Molecular packing of platelet 2-D square micelles
We used diblock copolymers of PPV12-b-P2VP n to achieve regular and homogeneous supramolecular 2-D fluorescent square micelles by dissolving–cooling–aging process. The scales of the achieved 2-D square micelles were controlled by the block ratio of PPV/P2VP and the concentration of the solution. In previous reports, the OPV copolymer with linear alkyl chains can be used to prepare monodisperse fiber-like micelles22,23,24. Therefore, we inferred that the formation of 2-D morphology is caused by the unique molecular packing related to the branched alkyl side chains. As discussed above, the conjugated PPV12 blocks should be arranged edge-on in the 2-D square micelles, which was confirmed by AFM measurements and DFT calculations.
To reveal the details of the molecular arrangements, appropriate characterization techniques for 2-D square micelles were necessary. First, we hoped to have the aid of selected-area electron diffraction (SAED). However, the SAED pattern indicated the formed 2-D square micelles were almost non-crystalline (Supplementary Fig. 22a). High-resolution TEM (HRTEM) photographs also confirmed the non-crystalline morphology of the 2-D square micelles, as there was no clear crystal lattice observed on the surface of the square micelle (Supplementary Fig. 22b).
Then, 2-D square micelles of PPV12-b-P2VP22 and PPV12-b-P2VP36 were characterized by grazing incidence wide-angle X-ray scattering (GIWAXS) to investigate the molecular packing in the assembly structures (Fig. 6d and Supplementary Fig. 25a). The 2-D square micelles of the two BCPs exhibited similar 2-D GIWAXS patterns. From the profiles along the in-plane direction (Fig. 6e), the reflections (100) and (200) were clearly visible, and no periodic reflection peaks along q z were observed. This suggested that PPV12-b-P2VP22 and PPV12-b-P2VP36 molecules favor an edge-on configuration in the 2-D platelet square micelles, which is consistent with previously discussed data. The d spacing of PPV12-b-P2VP22 molecules arranged in the 2-D square micelles was calculated as 9.46 Å. The reflection peak, q = 1.505 Å−1, could be attributed to the (010) reflection, and the d spacing of 3.70 Å, calculated from peak q = 1.699 Å−1, originates from the π–π stacking of the PPV12 backbones parallel to the substrate. The angle of the adjacent molecular chain was 135° (Supplementary Fig. 26). A similar result could also be obtained from GIWAXS measurement of PPV12-b-P2VP36. According to the previous literatures36,37, the PPV molecules without side chains should adopt a herringbone molecular arrangement, where molecules are packed in layer-by-layer mode and within one layer the adjacent molecules are parallel to each other. This herringbone molecular arrangement agreed with the data measured by our GIWAXS experiments, indicating that the molecules of PPV12-b-P2VP n in the 2-D platelet square micelles should pack through π–π interactions and probably adopt a herringbone configuration. This molecular arrangement was also supported by molecular dynamics simulations (Fig. 6f). From the simulation results, the PPV12 blocks and the P2VP blocks aggregated together respectively because of the hydrophilic–hydrophobic interactions. The PPV12 blocks interlaced with each other, and the adjacent π-conjugated PPV12 blocks arranged to form a V shape with the side alkyl chains inserted between them. In the diagonal direction, the molecules had the same advantage of growing orientation, which possibly caused the formation of the square shapes of the 2-D micelles38.
As illustrated in Fig. 6g, the process by which the platelet 2-D square micelles form could be determined. Initially, at 85 °C, the molecules of PPV12-b-P2VP n are completely dissolved in 2-PrOH and move freely in solution. As the temperature of the solution decreased, the quickly moving molecules started to aggregate driven by the hydrophobic interaction producing close distances for the PPV blocks. Then, the initially formed aggregates should be 1-D polymer micelles derived from π-π intermolecular interactions of the PPV12 cores, and these architectures gradually grow into 2-D platelet square micelles because of intermolecular π-π stacking of the rigid conjugated PPV12 cores from two directions. It was observed that the branched alkyl chains of the PPV12 cores played a crucial role in the formation of the platelet 2-D square micelles. First, the branched alkyl chains improved the solubility of the PPV12 cores in 2-PrOH, changed the hydrophilic-hydrophobic interactions and slowed the aggregation rate of PPV12-b-P2VP n BCPs. More importantly, it was the existence of the branched alkyl chains that led to the herringbone molecular arrangement, which induced the formation of the square micelles.
Platelet 2-D square micelles as carrier of SiO2 NPs
As described above, the P2VP coronas were distributed on the top and bottom surfaces of the platelet 2-D square micelles. It is known that SiO2 nanoparticles (NPs) can combine with P2VP coronas through hydrogen bonding39. Therefore, we hoped the formed 2-D square micelles of PPV12-b-P2VP n could be functionalized carrier templates of SiO2 NPs. We selected 2-D square micelles originating from PPV12-b-P2VP22 and mixed them with SiO2 NPs (diameter = 20 nm) in ethanol. After aging for 1 day, all the platelet 2-D square micelles were loaded with SiO2 NPs. The sizes of the patterns of SiO2 NPs loading on square micelles were consistent with the scales of the square platelets (Supplementary Fig. 27). The SiO2 NPs were more concentrated on the platelet edges perhaps because the steric encumbrance at the boundary was lower40.
In summary, we have described a simple strategy for the preparation of uniform, colloidally stable, 2-D platelet square micro- and nano-structures of PPV12-b-P2VP n BCPs through intermolecular π–π stacking interactions and hydrophobic interactions. The size and thickness of the formed 2-D square micelles could be effectively controlled by the ratio of PPV/P2VP blocks and they exhibited different concentration dependences. The square micelles initially form 1-D structures in 2-PrOH and then grow into 2-D architectures, and the growth is related to temperature and aging time. The formation of the square shapes is likely induced by the herringbone molecular arrangement, which is caused by the branched alkyl chains attached to the conjugated PPV12 cores. This strategy is practical and expected to be easily applicable to other conjugated block based copolymer systems. Moreover, these 2-D square film micelles possess high stability and flexibility, large area-to-volume ratios and definite fluorescence storage, which have potential applications in the fields of biosensors, catalysis, template building, and optoelectronics on the nanoscale.
Equipment and materials
The BCP poly(2,5-di(2′-ethylhexyloxy)-1,4-phenylenevinylene)12-aldehyde (PPV12-CHO) homopolymer was prepared by literature procedures33, and the fluorescent diblock copolymers PPV12-b-P2VP n used for building blocks of self-assembly were synthesized by quenching the anionic polymerization of P2VP with the PPV12-CHO41. The detailed procedures were described in Supplementary Methods. The anionic polymerization was carried out in a glove box filled with nitrogen atmosphere. The block ratios of BCPs were determined by GPC and 1H NMR spectroscopy. GPC measurements were carried out on a Viscotek VE 2001 triple-detector gel permeation chromatograph equipped with an automatic sampler, a pump, an injector, an inline degasser, and a column oven (40 °C). The elution columns consist of styrene/divinyl benzene gels with pore sizes of 500 and 100,000 Å. THF was used as the eluent, with a flow rate of 1.0 ml min−1. Samples were dissolved in the eluent (1 mg ml−1) and filtered with an organic phase filter (polytetrafluoroethylene membrane of 0.45 mm pore size) before analysis. The calibration was conducted using a PolyCALTM polystyrene standard from Viscotek. 1H NMR spectra were measured on a Bruker AVANCE 400 MHz spectrometer with tetramethylsilane as the internal standard.
Preparation of platelet 2-D square micelles
A 0.01 mg ml−1 solution of PPV12-b-P2VP12 or PPV12-b-P2VP16 with spectrum pure 2-PrOH was prepared in a 20 ml sealed vial, and for PPV12-b-P2VP n with lower ratio of PPV/P2VP blocks, the initial concentration of prepared solution was commonly 0.05 mg ml−1. Then the first prepared concentrated solution was diluted to a certain concentration. The prepared solution was heated at 85 °C for 45 min and then the pale yellow solution was slowly cooled to room temperature (25 °C) and aged for 24 h. The formed platelet 2-D square micelles were observed by TEM analysis of the drop-cast solution.
Transmission electron microscopy
TEM samples were prepared by drop-casting 5 μl of the micelle-formed solution onto a carbon-coated copper grid followed by solvent evaporated. TEM micrographs were obtained on a Hitachi HT7700 microscope operating at 80 kV and equipped with an AMF-5016 charge-coupled device camera. For the statistical analysis, the obtained images were analyzed by using DigitalMicrograph software package developed by the US Gatan company. The diagonal length was calculated to characterize the scale of the platelet 2-D square micelles. Two hundred 2-D square micelles from TEM images were traced by hand. Dn (number-average diagonal length) and Dw (weight-average diagonal length) of each sample of platelet 2-D square micelles were determined from these data by using Eqs (1) and (2), respectively (where D i is the diagonal length of individual platelet 2-D square micelles, N i is the number of diagonal length D i ).
HRTEM photographs were obtained on a Tecnai F30 microscope operating at 120 kV. Used TEM samples were prepared by drop-casting 5 μl of the micelle-formed solution onto a micro copper grid followed by solvent evaporated. SAED patterns for 2-D platelet square micelles were also collected by Tecnai F30 TEM.
Atomic force microscopy
The AFM samples for detecting were prepared by drop-coating about 15 μl of the 2-D square micelle solution onto a pre-cleaned and treated silicon wafer and evaporating the solvent 2-PrOH. The silicon wafers used for substrate were cleaned in piranha solution for 30 min, then ultrasound treated successively in ethanol, water, ultrapure water, and finally dried with blowing nitrogen. The images were obtained using an Asylum Research AFM in AC mode under ambient conditions. The used sensor cantilevers was Silicon probe reflex coated with aluminum manufactured by Budgetsensors Company. Images were analyzed using IGOR Pro software developed by WaveMetrics Inc.
The ground state geometries were fully optimized by the DFT method with the Becke three-parameter hybrid exchange and the Lee–Yang–Parr correlation functional (B3LYP) and 6–31G* basis set using the Gaussian 09 software package.
Scanning electron microscopy
Samples for SEM were prepared by drop-casting about 15 μl of the 2-D square micelle solution onto a pre-cleaned and treated silicon wafer and evaporating the solvent 2-PrOH. The silicon wafer was treated the same with AFM substrates as described above. Imaging was performed using a Zeiss Merlin SEM microscope at 5 kV accelerate voltage and 100 pA beam intensity.
Laser scanning confocal microscopy
LSCM images were performed using a Leica SP8 confocal attached to a Leica DMI6000 inverted epifluorescence microscope with a × 63 (numerical aperture1.4) oil-immersion objective lens. A drop of sample solution of micelles was put on a cleaned slide followed sealing with a cover slip, which was prepared for observing. The samples of formed 2-D square micelles in solution were excited using an argon laser operating at 405 nm and the confocal images were obtained using digital detectors with observation windows of 530–630 nm. The Supplementary Movie 1 was obtained by collecting three frames of confocal images per second.
UV-Vis absorption spectra
The UV-Vis absorption spectra were recorded by an Agilent Cary 60 UV-Vis spectrophotometer. A capped cuvette filled with 2-PrOH solution of PPV12-b-P2VP n was placed in the holder of spectrophotometer that was linked with a temperature controller. The solution in cuvette was heated to 85 °C and kept the temperature for 45 min. Then the heating was stopped, and the solution was spontaneous cooled to room temperature. The UV-Vis spectrum and the real-time temperature of the solution was recorded every 3 min during cooling down process. After the sample solution was cooled to room temperature, the measurement was changed to be carried out every 30 min until after aging for 20 h (for the 0.01 mg ml−1 2-PrOH solution of PPV12-b-P2VP36, the measurement lasted to 72 h).
PL spectra and fluorescence quantum efficiency
The PL spectra were recorded by an Edinburgh FS5 spectrofluorometer and the fluorescence quantum efficiencies were detected on a Hamamatsu C11347 absolute PL quantum yield spectrometer. The samples were prepared by dissolving PPV12-b-P2VP n in THF and 2-PrOH under concentration of 0.01 mg ml−1 and the prepared 2-PrOH solutions were heated at 85 °C for 45 min, cooled to room temperature (25 °C), and aged for 24 h.
DLS and SLS measurements
DLS and SLS measurements were performed using a Brookhaven BI-200SM wide-angle laser light-scattering apparatus equipped with a 635 nm red laser. PPV12-b-P2VP22 solution of 0.05 mg ml−1 in 2-PrOH was placed in sealed glass cuvette, and the cuvette was placed in pool full of matching fluids whose temperature was controlled by a water cycle system. The solution in cuvette was heated at 85 °C for 45 min and then spontaneously cooled to room temperature with DLS measurement carried out every 5 min. After sample solution was cooled to room temperature, the DLS was measured every 10 min until aging for 2 h, and then the measurement interval was changed to 1 h. The morphology factor ρ was calculated by the ratio of Rg/Rh. Rh represents the hydrodynamic radius and Rg represents the root mean square radius of gyration. Rh was calculated with the method of measuring Dh of the sample solution under different angles by DLS. PPV12-b-P2VP22 solution of 0.05 mg ml−1 in 2-PrOH placed in sealed glass cuvette was heated at 85 °C for 45 min and then it was cooled to a certain temperature. Under the temperature, hydrodynamic diameter of particles in sample solution was measured at 30°, 45°, 60°, 75°, and 90°, respectively. Drew a plot of q2 versus Dhθ, extrapolated the value of Dh0 by least squares curve fitting method and obtained the value of Rh. At the same temperature, SLS was measured under 30°, 45°, 60°, 75°, and 90°, respectively. Rg is consistent with Eq. (3). As the size of particles at different concentrations does not vary greatly, the Eq. (3) can be simplified to Eq. (4) (I stand for scattering intensity; q represent for scattering vector, and it can be calculated by Eq. (5); in Eq. (5), n is refractive index of solution, λ is laser wavelength, and θ is measuring angle). Then the value of Rg can be calculated from primary function Eq. (4).
Wide-angle X-ray diffraction
The wide-angle X-ray diffraction (WXRD) samples for detecting were prepared by drop-coating about 15 μl of the 2-D square micelle solution onto a pre-cleaned and treated silicon wafer and evaporating the solvent 2-PrOH for 10 times. The silicon wafer was treated the same with AFM substrates as described above. The WXRD spectrum was recorded using a Rigaku Smartlab 9 kW X-ray diffractometer using CuKα radiation (λ = 1.5418 Å).
The GIWAXS samples for detecting were prepared by drop-coating about 15 μl of the 2-D square micelle solution onto a pre-cleaned and treated silicon wafer and evaporating the solvent 2-PrOH for five times. The silicon wafer was treated the same with AFM substrates as described above. GIWAXS measurements were performed at the 8ID-E beamline at the Advanced Photon Source, Argonne National Laboratory, using X-rays with a wavelength of λ = 1.1385 Å, and a beam size of 200 μm (h) and 20 μm (v). A 2-D PILATUS 1M-F detector was used to capture the scattering patterns and was situated at 208.7 mm from samples. Typical GIWAXS patterns were taken at an incidence angle of 0.13°, above the critical angles of conjugated polymer and below the critical angle of the silicon substrate. Consequently, the entire structure could be detected. In addition, the q y scan was obtained from a linecut across the reflection beam center, while the q z scan was achieved by a linecut at q y = 0 Å−1, using the reflected beam center as 0.
Molecular dynamics simulation methods and details
First, we built a single PPV12-b-P2VP12 molecule by using Material Studio software package developed by the US Accelrys company and we optimized the configuration of this molecule with a steep descent energy minimization step. Thereafter, we packed 12 molecules on a 4 × 3 lattice with large enough intermolecular distances to avoid the initial direct contact between these molecules. All molecules were aligned parallel to the z direction of the simulation box. Periodic boundary conditions were used in our simulation. The simulation box had an initial box size of 18 nm in x and y direction, and 20 nm in the z-direction. This initial bundle of 12 molecules was put in the center of the simulation box. Afterward, the isopropanol solvent molecules were added into the simulation box at random positions. The initial mass density of the initial configuration was 0.2 g cm−3. From the initial configuration, we performed full atomistic MD simulations by using GROMACS 5.1 software package, all simulations were performed by applying hybrid/heterogeneous acceleration paralleled on two central processing units (CPU) (Intel(R) Xeon(R) CPU E5-2673 V3) and four graphics processing units (GPU) (NVIDIA 1080). Through steep descent energy minimization, the initial configuration was locally equilibrated. Furthermore, a designed NPT run of 10 ns is performed for equilibration of the system density. The final mass density of the system was 0.814 g cm−3. After which, the system had a size of 10.94 nm in x and y direction, and 16.73 nm in z direction. Afterward, we performed the production run for another 50 ns in NVT (N represents atomic number in system, V represents volume and T represents temperature) ensemble. In the initial equilibration run, the Berendsen thermostat and barostat were used with a thermostat coupling time of 0.2 ps, and a barstat coupling time of 1 ps, respectively. However, in the final NVT production run the Nosé–Hoover thermostat was used. The optimized potentials for liquid simulations-all atom (OPLS-AA) force field parameters were used in our simulation. The simulation temperature T was set at 298 K. The particle-mesh Ewald method was used to treat the electrostatic interactions in the system. The leapfrog algorithm is employed to integrate Newtons’ equations of motion with a time step of 1 fs.
The data that support the findings of this study, including the Supplementary Information, are available from the corresponding author on request.
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We acknowledge financial support from SUSTech, the Recruitment Program of Global Youth Experts of China, the National Natural Science Foundation of China (51773087 and 21733005), the Natural Science Foundation of Guangdong Province (2016A030313637), the Shenzhen Fundamental Research Programs (JCYJ20160504151536406 and JCYJ20160226193029593), and Shenzhen Peacock Program (KQTD20140630110339343). W.C. gratefully acknowledges financial support from the US Department of Energy, Office of Science, Materials Science and Engineering Division. We thank the Analysis and Test Center, Life Science Platform of SUSTech, for our TEM work; we are grateful to Zan Li for her help in taking part of TEM images and to Dongsheng He for his help in taking HRTEM images and SAED patterns. We also thank Tonghuan Zhang of SUSTech for his help of theoretical calculations.
The authors declare no competing interests.
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