Abstract:Although polymeric single crystals fabricated from self‐assembly of block copolymers are reported, preparation of single crystals with different aspect ratios still remains a major challenge. In this work, a facile way is demonstrated to prepare poly(ε‐caprolactone) based single crystals with tunable aspect ratios through simple counterion exchange on the basis of the Hofmeister series. Briefly, after ion exchange from Brˉ (an ion‐containing triblock copolymer, poly(ethylene oxide)‐b‐poly(ε‐caprolactone)‐b‐pol… Show more
“…51 Through counterion exchange, various counterions with different hydrophilicity, such as Br À , I À , SCN À , PF 6 À and OTf À , were introduced into the amorphous block, thus the aspect ratio of BCPSCs could be easily controlled. 51 They also prepared lozenge BCPSCs of PCL-b-qPDM containing liquid crystal (LC) AOT anions in the corona. 52,53 The soluble qPDM chains prefer to arrange parallel due to the directional arrangement of the LC AOT.…”
Section: Single Crystals Of Bcps With Single Crystalline Block 21 | M...mentioning
confidence: 99%
“…25,[44][45][46][47][48][49][50] Tong et al prepared BCPSCs of PEO-b-PCL-b-qPDM. 51 Through counterion exchange, various counterions with different hydrophilicity, such as Br À , I À , SCN À , PF 6 À and OTf À , were introduced into the amorphous block, thus the aspect ratio of BCPSCs could be easily controlled. 51 They also prepared lozenge BCPSCs of PCL-b-qPDM containing liquid crystal (LC) AOT anions in the corona.…”
Section: Single Crystals Of Bcps With Single Crystalline Block 21 | M...mentioning
Block copolymer single crystals (BCPSCs) have attracted widespread attentions due to their unique two-dimensional (2D) structure, good controllability, and great potential applications in recent years. In this paper, the morphology, surface structure of BCPSCs and the related influencing factors are reviewed. We also summarize the studies of 2D crystalline assemblies of block copolymers (BCPs) driven by crystallization and intermolecular π-π interaction. Moreover, the functionalization and properties of BCPSCs and 2D crystalline assemblies of BCPs are introduced. Finally, we put forward some unsolved problems in this field.
“…51 Through counterion exchange, various counterions with different hydrophilicity, such as Br À , I À , SCN À , PF 6 À and OTf À , were introduced into the amorphous block, thus the aspect ratio of BCPSCs could be easily controlled. 51 They also prepared lozenge BCPSCs of PCL-b-qPDM containing liquid crystal (LC) AOT anions in the corona. 52,53 The soluble qPDM chains prefer to arrange parallel due to the directional arrangement of the LC AOT.…”
Section: Single Crystals Of Bcps With Single Crystalline Block 21 | M...mentioning
confidence: 99%
“…25,[44][45][46][47][48][49][50] Tong et al prepared BCPSCs of PEO-b-PCL-b-qPDM. 51 Through counterion exchange, various counterions with different hydrophilicity, such as Br À , I À , SCN À , PF 6 À and OTf À , were introduced into the amorphous block, thus the aspect ratio of BCPSCs could be easily controlled. 51 They also prepared lozenge BCPSCs of PCL-b-qPDM containing liquid crystal (LC) AOT anions in the corona.…”
Section: Single Crystals Of Bcps With Single Crystalline Block 21 | M...mentioning
Block copolymer single crystals (BCPSCs) have attracted widespread attentions due to their unique two-dimensional (2D) structure, good controllability, and great potential applications in recent years. In this paper, the morphology, surface structure of BCPSCs and the related influencing factors are reviewed. We also summarize the studies of 2D crystalline assemblies of block copolymers (BCPs) driven by crystallization and intermolecular π-π interaction. Moreover, the functionalization and properties of BCPSCs and 2D crystalline assemblies of BCPs are introduced. Finally, we put forward some unsolved problems in this field.
“…In recent years, breakthroughs have been achieved by introducing uniform assembly units, specific crystallizable blocks, or directional noncovalent interactions. − For instance, the self-assembly of quasi-monodisperse polymers or nanoparticles has been utilized to generate 2D nanosheets with ordered structures . Crystallization-driven self-assembly (CDSA) has facilitated arrangements in crystallizable segments, − resulting in uniform 2D structures. − Among directional noncovalent interactions, π–π stacking has proven effective for constructing 2D structures. − In addition to traditional block copolymers, emerging alternating copolymers show promising potential for constructing materials with an ultrasmall or thin dimension, leveraging their consistently small and uniformly distributed repeating subunits. − These advancements have promoted the development of ordered 2D nanomaterials with improved properties and functionalities.…”
The pursuit of ordered two-dimensional (2D) materials with customized properties has fueled extensive research. While many established fabrication methods rely on substrates, solution-based polymer self-assembly processes remain much unexplored. Here, by manipulating the delicate balance between dominating and competing forces, we demonstrate how polymer chains fold, self-adjust, and self-assemble into diverse ordered 2D nanostructures in solution guided by an energy landscape, especially highly ordered crystalline structures, which are of great challenge to realize by polymers. An alternating copolymer initially self-assembled into 2D planar flakes via a kinetic pathway, lacking crystallinity. Through thermal annealing, they overcame a local kinetic barrier, in situ transforming into 2D circular crystalline clusters. Furthermore, by facilely replacing alkenyl linkers with triazoles in the alternating copolymers, additional tunable competing interactions were introduced, enabling the system to take thermodynamically favored pathways from the beginning and form 2D crystalline spindles directly. Besides, both the systems exhibited reversible self-assembly behavior and remote-controllable merit under light irradiation, forming 2D crystalline structures including flowers and spindles, respectively, highlighting the systems' responsiveness and versatility. This study offers diverse and facile strategies for constructing and fine-tuning tailorable nanostructures, suggesting promising applications in precision engineering and biomedical technologies.
Hybrid single crystals (HSCs) of different poly(ε‐caprolactone) (PCL) homopolymers with a poly(ε‐caprolactone)‐b‐poly(ethylene oxide) (PCL‐b‐PEO) block copolymer (BCP) were prepared. The effects of PCL length, PCL/PCL‐b‐PEO molar ratio, crystallization temperature (Tc) and solvent on crystal morphology were investigated. The optimal Tc for the formation of more perfect HSCs is between those for homo‐crystals of individual PCL and PCL‐b‐PEO and roughly increases with the length of PCL and PCL/PCL‐b‐PEO molar ratio. The chain folding in the HSCs was studied by comparing the experimentally measured heights obtained by atomic force microscopy (AFM) and theoretically calculated ones based on a sandwich structure model. Under most situations, the PCL homopolymers adopt a larger chain folding number in the HSCs than that in their homo‐crystals, while the chain folding of BCP remains unaltered. However, when both PCL homopolymer and PCL‐b‐PEO BCP crystallize slowly and the overcrowding of the PEO is effectively alleviated, thicker HSCs can be formed, in which the PCL homopolymer preserves the chain folding in its homo‐crystals but the BCP adopts a reduced chain folding number as compared with that in its homo‐crystals. The relative crystallization rate of PCL homopolymer versus BCP also affects the real composition and overall height of the HSCs.This article is protected by copyright. All rights reserved
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