Gregory I.
Peterson†
*,
Sanghee
Yang†
and
Tae-Lim
Choi
*
Department of Chemistry, Seoul National University, Seoul 08826, Republic of Korea. E-mail: gpeterson@snu.ac.kr; tlc@snu.ac.kr
First published on 9th December 2020
Polymer self-assembly is a widely utilized method to prepare a wide range of nano-objects in solution. Typically, preparation of such objects relies on the use of block copolymers and challenging post-polymerization treatment steps. While polymerization induced self-assembly (PISA) can simplify their preparation, the resulting nano-objects typically have poor stability (including sensitivity to solvent, temperature, and mechanical stimuli). An alternative approach is to use conjugated polymers, with a strong driving force for self-assembly, to achieve semiconducting nano-objects. This process is termed in situ nanoparticlization of conjugated polymers (INCP) or PISA using conjugated polymers. With INCP, self-assembled nano-objects can be obtained (without any post-polymerization treatment steps) from block copolymers, using one-pot or one-shot methods, or even homopolymers. Due to the use of conjugated polymers, the nano-objects from INCP have the potential for use in various optoelectronic applications. In this Perspective, we summarize the development of INCP by discussing synthetic methods, accessible nano-objects morphologies, and mechanisms of nano-object formation.
Fig. 1 Preparation of nano-objects during polymerization. Similarities and differences between conventional PISA (with non-conjugated polymers) and INCP. |
The core-forming blocks of nanostructures used in PISA are generally sensitive to solvent, temperature, and concentration. Even small changes in these conditions can alter or break-up the nanostructures. While the stability can be greatly enhanced with cross-linking, this requires additional post-polymerization treatment steps and can make obtaining non-spherical nano-objects challenging (in the case of in situ cross-linking).15 In 2012, we developed another PISA strategy to achieve highly stable nano-objects, which was termed in situ nanoparticlization of conjugated polymers (INCP, Fig. 1).16,17 In regard to terminology, “INCP” is analogous to “PISA of conjugated polymers”, although we use the former term in this Perspective as only a few papers that conduct self-assembly of conjugated polymers use the PISA term. With INCP, strong π–π or CH–π interactions drive self-assembly, resulting in nano-objects that are highly stable toward different temperatures, solvents, and mechanical stimuli. The features that further differentiate conventional PISA (with non-conjugated polymers) and INCP is that the latter is not limited to BCPs (i.e., homopolymers can undergo INCP), the resulting nano-objects have semiconducting properties, and more diverse nanostructures can be achieved (such as nanocaterpillars, nanostars, fractals, etc.).
Conjugated polymer nanoparticles are generally prepared by post-polymerization treatment and have been targeted for various applications including sensors, imaging agents, photovoltaics, light-emitting diodes, and catalysts.18–21In situ nanoparticlization can also be achieved with the aid of surfactants or stabilizers using miniemulsion or dispersion polymerizations (techniques that are mostly limited to producing spherical nanoparticles),22–25 but these methods are beyond the scope of this Perspective. In contrast, INCP does not require any stabilizers and various 1D, 2D, or 3D nano-objects can be obtained. With a few exceptions, INCP has been performed using ring-opening metathesis polymerization (ROMP),26–28 cyclopolymerization (CP),29–31 and catalyst-transfer polycondensation (CTP).32–34 In this Perspective, we will discuss the development of INCP, including synthetic methods, nano-object morphologies, and mechanisms of nano-object formation (organized by the polymerization type).
Fig. 2 (A) Synthesis of PA-based BCPs. (B) DLS measurements of aliquots from the polymerization solution of PNB150-b-PAn. Times are after COT addition. Numbers above the peaks correspond to the average hydrodynamic diameter (Dh, with units of nm). Adapted from ref. 37 with permission from the Royal Society of Chemistry, copyright 2014. (C) DLS measurements of aliquots from the polymerization solution of PTD150-b-PAn. Adapted from ref. 38 with permission from John Wiley and Sons, copyright 2015. (D) AFM (on mica) images of nanospheres from PNB150-b-PA40. Adapted from ref. 16 with permission from American Chemical Society, copyright 2012. (E) AFM (on mica) and TEM (on a carbon-coated copper grid) images of nanocaterpillars from PNB150-b-PA208. Adapted from ref. 37 with permission from the Royal Society of Chemistry, copyright 2014. (F) AFM (on mica) images of the nano/micro-object morphologies for PTD150-b-PAn. Adapted from ref. 38 with permission from John Wiley and Sons, copyright 2015. |
To determine the morphology of the nanoparticles, dilute solutions of BCPs were spin-coated on mica surfaces and imaged with atomic force microscopy (AFM). For PNB150-b-PA40, nanospheres were observed (Fig. 2D).16 As the length of the PA block was increased, a morphological transition from nanospheres to 1D nano-objects was observed (Fig. 2E). High resolution AFM and transmission electron microscopy (TEM) images revealed undulated linear nanostructures, termed nanocaterpillars, which were also confirmed to exist in solution using cryogenic TEM (cryo-TEM). Defect- (i.e., nanosphere) free nanocaterpillars were obtained by enhancing the stereo-purity of the PA block (cis-PA was favored when polymerizations were conducted at 0 °C) and decreasing the molecular weight dispersity.37 Importantly, the highly stable nature of the nano-objects was supported by DLS experiments, as nanoparticle size distributions remained constant in solution after heating at 90 °C or sonicating for 30 min.16
We envisioned that we might be able to obtain higher-order nanostructures (i.e., 3D nano-objects) by using a more rigid shell-block, which would promote stronger PA block interactions.38 Thus, we switched from NB1 to an endo-tricyclo[4.2.2.0]deca-3,9-diene (TD) monomer (TD1) to achieve BCPs with a rigid poly(TD) (PTD) shell-block (Fig. 2A). While polymerizations were slower with TD1, PTD150-b-PAn with PA DPs up to 156 were still obtainable. The formation of nanoparticles during the polymerization was again supported by DLS measurements (Fig. 2C). The structural evolution from nanospheres to nanocaterpillars, with increasing PA block length, was also still observed (Fig. 2F). This transition, however, appeared to occur at much shorter PA block lengths for PTD150-b-PAn (nanocaterpillars were observed with a PA DP of 34) than for PNB150-b-PAn (nanocaterpillars were observed with PA DPs of 80 or higher). Further increasing the PA block length for PTD150-b-PAn resulted in the formation of 3D nano- and then micro-objects. DLS and cryo-TEM were used to confirm that the nanostructures did not form as a result of aggregation during drying for AFM/TEM imaging. Of note, the INCP process could also be achieved in a one-shot manner (without sequential monomer addition) due to the disparity between the polymerization rates of NB1 or TD1 and COT.39 The use of the one-shot process did not disrupt or alter the nano-object formation processes, thereby making the one-shot INCP one of the simplest method for preparing nano-objects.
Based on these results, we proposed a model (Fig. 3) for the self-assembly and morphological transition of nanospheres to nanocaterpillars and 3D micro-objects.38 As the PA block grows during the polymerization, the BCPs spontaneously self-assemble into micelle-like nanospheres due to strong π–π interactions of the PA blocks (the propagating carbenes remain active in the core). COT diffuses into the PA core and propagation continues. Eventually, the PA core-blocks become elongated enough that they are exposed to solvent. Solvophobic and π–π interactions promote the spontaneous assembly of the nanospheres into nanocaterpillar morphologies. Due to the relatively flexible nature of PNB, the PA core is well-shielded from solvent and other nanospheres or nanocaterpillars, such that they do not assemble into higher-order morphologies (even as the PA core continues to grow). The rigid nature of PTD,40 however, prohibits adequate shielding of the PA core. Thus, as the PA blocks of the PTD-based nanocaterpillars grow, the PA core-blocks become exposed, leading to aggregation of the nanocaterpillars into 3D nano- and then micro-objects.
Fig. 3 Proposed model for the formation of nanocaterpillars from PNB-based BCPs and 3D nano-objects from PTD-based BCPs via INCP. |
Poly(p-phenylenevinylene)s (PPVs) are highly fluorescent semiconducting polymers used in various optoelectronic applications and devices.41 A facile method of preparing PPVs is the ROMP of [2.2]paracyclophane-1,9-diene (PD). We envisioned conducting INCP with BCPs having PNB shell- and PVP core-blocks.42 Due to the disparate reactivity between NB1 and PD, one-shot polymerizations were achieved with G3-Cl, yielding PNB150-b-PPVn with PPV DPs up to 60 (Fig. 4A). Aliquots were removed from the polymerization and were characterized by DLS, AFM, and TEM, without termination or purification, to support in situ nanoparticlization. AFM and TEM images revealed a morphological transition from nanospheres to nanocaterpillars with increasing PPV block length (analogous to that described above for PA), followed by a transition from nanocaterpillar to nanostar morphologies (Fig. 4B). Water-dispersible nanocaterpillars were also prepared using NB2 (Fig. 4A). The nanocaterpillars were stable in tetrahydrofuran (THF), chloroform, and water, which highlights one of the advantages of preparing nanoparticles with INCP. The nanocaterpillars were also shown to undergo fluorescence quenching in the presence of trace amounts of nitroaromatics, including 2,4,6-trinitrotoluene (TNT), supporting their potential use in explosive sensing applications.
Fig. 4 (A) Synthesis of PPV-based BCPs. (B) AFM (on mica) and TEM (on a carbon-coated copper grid) images of the nano-object morphologies for PNB150-b-PPVn. Adapted from ref. 42 with permission from the Royal Society of Chemistry, copyright 2017. (C) AFM (on mica) images of the nanoparticle morphologies for PTD1200-b-PPVn. Adapted ref. 43 with permission from American Chemical Society, copyright 2018. (D) Proposed mechanism for fractal nano-object formation via INCP. (E) TEM (on a carbon-coated copper grid) images of PTD2200-b-PPV15-based nanostructures prepared with or without 3,5-DCP as an additive to tune the polymerization kinetics. Adapted from ref. 43 with permission from American Chemical Society, copyright 2018. |
We also explored the INCP of PPV-based BCPs having a PTD shell-block.43 The self-assembly behavior of PTD-b-PPVs was quite different from their PNB-based counterparts. In situ formation of nanospheres was still observed during the one-shot polymerization of PTD1200-b-PVPn. However, instead of forming uniform nanocaterpillars, rod-like and branched morphologies were formed with increasing polymerization time, then unexpected and unique fractal nano-objects were produced (Fig. 4C). To explain the origin of these unprecedented nano-fractal structures, kinetics studies were conducted. We observed slow initiation of PD from the living PTD blocks, followed by fast propagation, and thus, low initiation-to-propagation rate ratios (ki/kp). This implied that the polymerization was uncontrolled, leading to the gradual generation of BCPs and then micellar nanostructures (instead of simultaneous self-assembly). We proposed a model in which this gradual generation of nanospheres would maintain a sufficiently low nanoparticle concentration such that a diffusion limited aggregation mechanism would be operative (Fig. 4D).44–46 We imagined that if we could tune the polymerization kinetics to improve control of the polymerization, we would achieve uniform generation of nanospheres and observe the formation of nanocaterpillars (following the mechanism shown in Fig. 3). Switching to TD2 (which forms a shell-block with decreased steric bulk, enabling faster initiation of PD), fractal nano-objects were still observed (Fig. 4E). With the use of 3,5-dichloropyridine (3,5-DCP) as an additive (which reversibly binds to the propagating Ru species and slows PD propagation), a 13.5 times larger ki/kp value was obtained for PD (compared to polymerizations using TD1 without an additive). As expected, this resulted in a well-controlled block copolymerization, more uniform nanosphere formation, and the formation of nanocaterpillars (Fig. 4E). Therefore, we demonstrated that tuning the polymerization kinetics was a useful strategy to prepare unique nano-objects that would otherwise be challenging to accomplish via conventional equilibrium-driven self-assembly processes.
Fig. 5 (A) Synthesis of PCPV-based BCPs. (B) Structural evolution of PNB450-b-PCPV194-based nanospheres (which were prepared via INCP) to nanocaterpillars and branched nanocaterpillars with aging (a non-INCP process), and (C) structural evolution of PTD150-b-PCPV130-based nanospheres (which were prepared via INCP) to 3D micro-objects with aging under light irradiation (another non-INCP process). Adapted from ref. 47 with permission from John Wiley and Sons, copyright 2017. |
To produce fully conjugated nano-objects without insulating shell blocks, we prepared BCPs using a soluble 1,6-heptadiyne monomer (HD2) and a fluorene-based monomer (HD3) (Fig. 6A).48 We found that the resulting PCPV250-b-PCPV3n underwent INCP, and self-assembled into long nanofibers (Fig. 6B) without going through an intermediate nanostructure (such as nanospheres). We attributed this difference in self-assembly behavior to the higher solubility of the PCPV3 block, compared to unfunctionalized PA blocks which underwent rapid nanoparticlization (as they were completely insoluble). Instead, the PCPV3 block underwent crystallization, forming well-defined cores for the nanofibers, with the PCPV2 block acting as a solubilizing shell (Fig. 6B). Remarkably, we also observed direct formation of higher-order nano-objects via INCP for PCPV3 homopolymers.49 Specifically, 2D leaf structures (Fig. 6C and D) were observed with in situ sampling during the polymerization of HD3 in THF. This result highlights one of the primary features that differentiates INCP from conventional PISA; that INCP is not limited to BCPs. Interestingly, when the leaf nano-objects were dispersed in chloroform, a morphological transition from leaf to rectangle morphologies was observed (Fig. 6D). Comparison of the diffraction patterns by fast Fourier transform (FFT) analysis of high-resolution TEM images for the two different morphologies provided insight into the self-assembly mechanism (Fig. 6E). The diffraction patterns suggested the presence of defects in chain packing for the leaf nano-objects and more ordered packing for the rectangular nano-objects. Specifically, the latter supported an orthorhombic crystal lattice and an interdigitated slip-stack packing of the polymer chains, without chain folding, leading to strong van der Waals and CH–π interactions serving as the driving force for self-assembly.
Fig. 6 (A) Synthesis of PCPV-based BCPs and homopolymers. (B) TEM (on a carbon-coated copper grid) and AFM (on mica) images of the nanofibers for PCPV250-b-PCPV3n. Adapted from ref. 48 with permission from the Royal Society of Chemistry, copyright 2020. (C) Proposed mechanism for 2D leaf nano-object formation via INCP. (D) TEM (on a carbon-coated copper grid) images of PCPV3n-based 2D leaf nano-objects (via INCP) and rectangular nano-objects (after a non-INCP process), and (E) corresponding FFT electron diffraction patterns of each morphology. The highly ordered pattern from 2D rectangles in chloroform corresponded to the orthorhombic crystalline lattice with three main d-spacing values of 10.3, 16.1, and 18.5 Å. Adapted from ref. 49 with permission from American Chemical Society, copyright 2017. |
Xie, Sun, and coworkers observed micellular or aggregated structures from various PNB-b-PCPVs via INCP (Fig. 7A).50,51 These polymers showed good potential for obtaining unique, higher-order morphologies. For instance, PNB575-b-PCPV450 formed vesicles upon evaporating the polymerization solvent (increasing the nano-object concentration in THF, Fig. 7B). It was unclear if vesicles were formed during the polymerization as well, or only after the post-treatment. PNB675-b-PCPV425 formed nanotubes after changing from the polymerization solvent (THF) to chloroform (Fig. 7C). Direct formation of nanotubes, by conducting the polymerization in chloroform, was not explored. Li, Xie, and coworkers also demonstrated the formation of irregularly aggregated micellular structures from PNB6-b-PCPV5via INCP in chloroform.52 More uniform structures could be achieved by re-dispersing the nanostructures in THF, suggesting that more uniform nanospheres might have been achieved if THF was used as a polymerization solvent. Xie, Liao, and coworkers also observed self-assembly of PCPV homopolymers into unique structures.53PCPV7316 formed (concentration-dependent) nanospheres and hollow cylindrical structures in THF. PCPV629 formed (concentration-dependent) solid or hollow cylindrical structures in THF or chloroform, respectively (Fig. 7D). It was unclear if the cylindrical nano-objects were generated by INCP or were only a result of the solvent evaporation process in preparation for imaging. Regardless, these polymers represent promising candidates for further study.
Fig. 7 (A) Synthesis of PCPV-based BCPs and homopolymers. (B) TEM (on a carbon-coated copper grid) image of PNB575-b-PCPV450-based vesicles formed by changing solvent concentration. Adapted from ref. 50 with permission from the Royal Society of Chemistry, copyright 2015. (C) TEM (on a carbon-coated copper grid) image of PNB675-b-PCPV425-based nanotubes formed by changing the dispersion solvent. Adapted from ref. 51 with permission from the Royal Society of Chemistry, copyright 2017. (D) 3D AFM (on mica) images of cylindrical nano-objects from PCPV6. Adapted from ref. 53 with permission from American Chemical Society, copyright 2015. |
Fig. 8 (A) Synthesis of PT-based BCPs. (B) AFM images of the nanostar to branched network evolution for PT1100-b-PT2n with increasing PT2 block length. Adapted from ref. 56 with permission from American Chemical Society, copyright 2013. (C) AFM image of nanocaterpillars from PPP170-b-PT2n. Adapted from ref. 63 with permission from the Royal Society of Chemistry, copyright 2014. (D) TEM images of P3HT50-b-PT240-based nano-objects using conventional or externally initiated KCTP. Adapted from ref. 64 with permission from the Royal Society of Chemistry, copyright 2016. (E) Schematic and TEM images for the generation of multi-line nanocaterpillars from PPP170-b-PT3n. Adapted from ref. 65 with permission from the Royal Society of Chemistry, copyright 2016. |
We next explored the influence of two different shell blocks on the PT-based nanoparticle morphology. We first looked at switching the first block to a dihexyloxy substituted poly(p-phenylene) (PPP1), which was expected to have a larger hydrodynamic radius than PT1 and would enable better shielding of the PT2 core-block.63 The resulting PPP170-b-PT2n formed well-defined nanocaterpillar structures (Fig. 8C), which still showed good stability to elevated temperatures and sonication. The second shell block we studied was poly(3-hexylthiophene) (P3HT), which we initially found to generate irregular aggregated nanostructures using conventional KCTP conditions (Fig. 8D).64 To improve the control of the nanoparticle morphology, we implemented an externally initiated KCTP method.66–69 The conventional KCTP leads to the production of triblock-impurities, whereas externally initiated KCTP gives clean diblock structures due to unidirectional polymerization from the o-tolyl-based Ni initiator/catalyst.
Specifically, defect-free o-tolyl-P3HT50-b-PT2n generated nanocaterpillars (with a PT2 DP of 40) and branched nanocaterpillars at higher PT2 block lengths (Fig. 8D).
Unique nano-object morphologies were observed by switching the core-block (from PT2 to PT3) for PPP1-based BCPs.65PT3 and PT2 undergo different types of crystalline packing. Specifically, PT3 and PT2 undergo staggered π-stacking (forming a face-centered lattice) and edge-to-face (herringbone) stacking, respectively.70 A consequence of the differences in packing is that PT3 has weaker π–π interactions. Interestingly, this led to the formation of multi-line nanostructures at higher PT3 DPs. Specifically, we observed the morphological evolution of nanospheres to nanocaterpillars to multi-line nanocaterpillars to branched multi-line nanocaterpillar structures (Fig. 8E). However, the weaker interactions came at the cost of decreased nano-object stability. While multi-line nanocaterpillars were robust to elevated temperatures, sonication resulted in their fragmentation into shorter multi-line structures. Very long nanocaterpillars (over 2 μm) could also be achieved by changing the PPP1 block to the more soluble PPP2, with branched 2-ethylhexyl side chains, without disrupting the ability to form multi-line nanocaterpillars.
Fig. 9 (A) Synthesis of functional PA BCPs (PPAX) and homopolymers (PPGA). (B) TEM images of the vesicle to helical ribbon evolution for PPA180-b-PPA2n with increasing PPA2 block length. Adapted from ref. 71 with permission from American Chemical Society, copyright 2020. (C) Proposed mechanism for nano-object formation from PPAX-based BCPs. (D) TEM images of the micellular, nanostar, and network nanostructures from PPGAvia INCP in different solvents. Adapted from ref. 72 with permission from Springer Nature, copyright 2018. |
We can also look to other self-assembly methods for inspiration. Various conjugated polymers (homopolymers or within BCPs) have been shown to undergo self-assembly using methods such as CDSA or self-seeding. While some of those polymers have already been explored in INCP, they have been shown to produce different nano-objects morphologies (than INCP), such as nanowires from oligo(p-phenylenevinylene)82,83 and 2D squares from PPV.84 Some of these polymers may be well suited for INCP, such as oligo(p-phenylene ethynylene) (which forms nanowires)85 and poly(9,9-dihexylfluorene) (which forms spherical nanoparticles and nanowires).86–89 Other polymers may be more challenging to adapt to INCP, such as P3HT (which was previously utilized as the soluble block in INCP), despite its ability to form nanofibers and 2D-rectangles using other methods.61,62,90–95 Similarly, poly(3-octylthiophene) (which forms nanowires)96 and poly[3-(2,5,8,11-tetraoxatridecanyl)thiophene] (which forms nanoribbons)97 would also be challenging due to their side chains which provide good solubility.
Other self-assembly methods can also provide insight into new nano-object morphologies that might be obtained with INCP (if proper polymers and polymerization conditions were used). For instance, higher-order morphological structures such as “octopi” or “jellyfish” were obtained by conventional PISA with the addition of a small amount of solvophilic comonomer into the insoluble block of a BCP.98 The use of copolymer core-blocks in PISA has also enabled inverse morphologies such as compound vesicles, sponges, and cubosomes.99 Specific examples, based on CDSA, which might be adaptable to INCP include the formation of diamond or hexagonal 2D nano-objects.100,101 One distinct advantage of CDSA over INCP is the ability to precisely control the structural dimensions of nano-objects.101,102 Further exploration of such control should done for INCP. Furthermore, even more complex structures can be achieved with CDSA due to the use of multi-polymer systems.103,104 Conducting INCP in the presence of other polymers could be an interesting area of exploration to generate novel nano-objects.
To date, the majority of INCP examples have focused on expanding the scope of polymers and nano-object morphologies, as well as understanding the mechanisms of self-assembly. More thorough characterization of nano-object properties (and perhaps morphology-dependent properties) will be important to identifying potential applications for which they would be best suited. Furthermore, despite the use of semiconducting polymers, the optoelectronic properties of the nano-objects have not been well characterized. As described above, semiconducting nanoparticles generally have a broad range of applications (sensors, imaging agents, photovoltaics, light-emitting diodes, and catalysts),105 and given that unique morphologies can be obtained with INCP, there is good reason to explore these applications in detail.
Footnote |
† These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2021 |