Precision Epitaxy for Aqueous 1D and 2D Poly(ε-caprolactone) Assemblies
- Maria C. Arno ,
- Maria Inam ,
- Zachary Coe ,
- Graeme Cambridge ,
- Laura J. Macdougall ,
- Robert Keogh ,
- Andrew P. Dove
- Rachel K. O’Reilly
Abstract

The fabrication of monodisperse nanostructures of highly controlled size and morphology with spatially distinct functional regions is a current area of high interest in materials science. Achieving this control directly in a biologically relevant solvent, without affecting cell viability, opens the door to a wide range of biomedical applications, yet this remains a significant challenge. Herein, we report the preparation of biocompatible and biodegradable poly(ε-caprolactone) 1D (cylindrical) and 2D (platelet) micelles in water and alcoholic solvents via crystallization-driven self-assembly. Using epitaxial growth in an alcoholic solvent, we show exquisite control over the dimensions and dispersity of these nanostructures, allowing access to uniform morphologies and predictable dimensions based on the unimer-to-seed ratio. Furthermore, for the first time, we report epitaxial growth in aqueous solvent, achieving precise control over 1D nanostructures in water, an essential feature for any relevant biological application. Exploiting this further, a strong, biocompatible and fluorescent hydrogel was obtained as a result of living epitaxial growth in aqueous solvent and cell culture medium. MC3T3 and A549 cells were successfully encapsulated, demonstrating high viability (>95% after 4 days) in these novel hydrogel materials.
Introduction
Results and Discussion
Synthesis and Preparation of PCL Crystalline Seeds
Figure 1

Figure 1. (a) Schematic of self-nucleation of PCL50-b-PDMA180 diblock copolymer followed by sonication of polydisperse cylinders to form uniform seed micelles, TEM micrographs of (b) polydisperse cylinders and (c) seed micelles, and (d) length distribution of seed micelles. Uranyl acetate (1%) was used as a negative stain. Scale bar = 1000 nm.
Epitaxial Growth of PCL Cylinders in an Alcoholic Solvent
Figure 2

Figure 2. (a) Schematic of epitaxial growth of PCL50-b-PDMA180 cylindrical micelles in ethanol from 50 nm seeds. TEM micrographs of cylindrical micelles epitaxially grown from seed micelles with a unimer/seed ratio of (b) 1, (c) 2, (d) 3, (e) 5, (f) 7, and (g) 9. Uranyl acetate (1%) was used as a negative stain. Scale bar = 1000 nm. (h) Length dispersity of cylindrical micelles. (i) Plot showing a linear epitaxial growth regime of cylinders with narrow length dispersities (error bars represent the standard deviation, σ, of the length distribution) in comparison to the theoretical length (dashed line).
Controlled Epitaxial Growth in Water
Figure 3

Figure 3. (a) Schematic representation of epitaxial growth in water using PCL50-b-PMMA20-b-PDMA200 triblock copolymer. TEM micrographs of cylindrical micelles epitaxially grown from 40 nm seed micelles in water with a unimer/seed ratio of (b) 1, (c) 5, (d) 9, and (e) 15, using graphene oxide TEM grids. (44) Scale bar = 1000 nm. (f) TEM micrograph (scale bar = 1000 nm) and (g) confocal microscopy image (scale bar = 20 μm) of fluorescently labeled cylindrical micelles epitaxially grown from seed micelles in water with a unimer/seed ratio of 15. Scale bar = 20 μm. (h) Length dispersity of cylindrical micelles. (i) Plot showing a linear epitaxial growth regime of cylinders with narrow length dispersities (error bars represent the standard deviation, σ, of the length distribution) in comparison to the theoretical length (dashed line).
Epitaxy in Water to Form Hydrogel Materials
Figure 4

Figure 4. (a) Schematic of hydrogel formation via direct epitaxial growth of PCL50-b-PMMA20-b-PDMA200 cylinders in water. (b) TEM micrograph of PCL50-b-PMMA20-b-PDMA200 hydrogel freeze-dried on a TEM grid. Scale bar = 1000 nm. (c) Cryo-SEM image of the cylinder hydrogel (scale bar = 2 μm) with photographs of the hydrogel using BODIPY-tagged (inset, left) and untagged cylinders (inset, right). (d) Step-strain measurements of cylinder hydrogel over three cycles (ω = 10 rad s–1) with (e) enlargement of the recovery of the material properties after each cycle. (f) Strain-dependent oscillatory rheology of the cylinder hydrogel at 293 K and a constant frequency of 10 rad s–1.
Supporting Information
The Supporting Information is available free of charge on the ACS Publications website at DOI: 10.1021/jacs.7b10199.
Experimental details and additional results (PDF)
Terms & Conditions
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Acknowledgment
Zachary P. L. Laker and Neil. R. Wilson are acknowledged for SAED measurements. Nicole Kelly is acknowledged for running WAXD of the samples. Wei Yu is acknowledged for running MALDI-ToF of PCL. Prof. Matthew Gibson is thanked for access to his cell lab facilities. The University of Warwick Advanced BioImaging Research Technology Platform, BBSRC ALERT14 award BB/M01228X/1, is thanked for confocal fluorescence microscopy analysis. The University of Warwick and EPSRC are thanked for the award of a Warwick Chancellors Scholarship (R.K.) and a DTP studentship (M.I. and L.J.M., respectively). ERC is acknowledged for support to M.C.A., A.P.D. (Grant Number 681559), G.C., and R.O.R. (Grant Number 615142).
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Abstract
Figure 1
Figure 1. (a) Schematic of self-nucleation of PCL50-b-PDMA180 diblock copolymer followed by sonication of polydisperse cylinders to form uniform seed micelles, TEM micrographs of (b) polydisperse cylinders and (c) seed micelles, and (d) length distribution of seed micelles. Uranyl acetate (1%) was used as a negative stain. Scale bar = 1000 nm.
Figure 2
Figure 2. (a) Schematic of epitaxial growth of PCL50-b-PDMA180 cylindrical micelles in ethanol from 50 nm seeds. TEM micrographs of cylindrical micelles epitaxially grown from seed micelles with a unimer/seed ratio of (b) 1, (c) 2, (d) 3, (e) 5, (f) 7, and (g) 9. Uranyl acetate (1%) was used as a negative stain. Scale bar = 1000 nm. (h) Length dispersity of cylindrical micelles. (i) Plot showing a linear epitaxial growth regime of cylinders with narrow length dispersities (error bars represent the standard deviation, σ, of the length distribution) in comparison to the theoretical length (dashed line).
Figure 3
Figure 3. (a) Schematic representation of epitaxial growth in water using PCL50-b-PMMA20-b-PDMA200 triblock copolymer. TEM micrographs of cylindrical micelles epitaxially grown from 40 nm seed micelles in water with a unimer/seed ratio of (b) 1, (c) 5, (d) 9, and (e) 15, using graphene oxide TEM grids. (44) Scale bar = 1000 nm. (f) TEM micrograph (scale bar = 1000 nm) and (g) confocal microscopy image (scale bar = 20 μm) of fluorescently labeled cylindrical micelles epitaxially grown from seed micelles in water with a unimer/seed ratio of 15. Scale bar = 20 μm. (h) Length dispersity of cylindrical micelles. (i) Plot showing a linear epitaxial growth regime of cylinders with narrow length dispersities (error bars represent the standard deviation, σ, of the length distribution) in comparison to the theoretical length (dashed line).
Figure 4
Figure 4. (a) Schematic of hydrogel formation via direct epitaxial growth of PCL50-b-PMMA20-b-PDMA200 cylinders in water. (b) TEM micrograph of PCL50-b-PMMA20-b-PDMA200 hydrogel freeze-dried on a TEM grid. Scale bar = 1000 nm. (c) Cryo-SEM image of the cylinder hydrogel (scale bar = 2 μm) with photographs of the hydrogel using BODIPY-tagged (inset, left) and untagged cylinders (inset, right). (d) Step-strain measurements of cylinder hydrogel over three cycles (ω = 10 rad s–1) with (e) enlargement of the recovery of the material properties after each cycle. (f) Strain-dependent oscillatory rheology of the cylinder hydrogel at 293 K and a constant frequency of 10 rad s–1.
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- 10Geng, Y.; Dalhaimer, P.; Cai, S.; Tsai, R.; Tewari, M.; Minko, T.; Discher, D. E. Nat. Nanotechnol. 2007, 2, 249– 255 DOI: 10.1038/nnano.2007.70[Crossref], [PubMed], [CAS], Google Scholar10https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BD1cXktVGgsbs%253D&md5=e93d8a9b11bf2a6cc2c5e970aa37a433Shape effects of filaments versus spherical particles in flow and drug deliveryGeng, Yan; Dalhaimer, Paul; Cai, Shenshen; Tsai, Richard; Tewari, Manorama; Minko, Tamara; Discher, Dennis E.Nature Nanotechnology (2007), 2 (4), 249-255CODEN: NNAABX; ISSN:1748-3387. (Nature Publishing Group)Interaction of spherical particles with cells and within animals was studied extensively, but the effects of shape have received little attention. Here the authors use highly stable, polymer micelle assemblies known as filomicelles to compare the transport and trafficking of flexible filaments with spheres of similar chem. In rodents, filomicelles persisted in the circulation up to one week after i.v. injection. This is about ten times longer than their spherical counterparts and is more persistent than any known synthetic nanoparticle. Under fluid flow conditions, spheres and short filomicelles are taken up by cells more readily than longer filaments because the latter are extended by the flow. Preliminary results further demonstrate that filomicelles can effectively deliver the anticancer drug paclitaxel and shrink human-derived tumors in mice. Although these findings show that long-circulating vehicles need not be nanospheres, they also lead insight into possible shape effects of natural filamentous viruses.
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- 27Inam, M.; Cambridge, G.; Pitto-Barry, A.; Laker, Z. P. L.; Wilson, N. R.; Mathers, R. T.; Dove, A. P.; O’Reilly, R. K. Chem. Sci. 2017, 8, 4223– 4230 DOI: 10.1039/C7SC00641A[Crossref], [PubMed], [CAS], Google Scholar27https://chemport.cas.org/services/resolver?origin=ACS&resolution=options&coi=1%3ACAS%3A528%3ADC%252BC2sXmtVeqtLo%253D&md5=7bf2d5494c613d5ceb273d98fba3feba1D vs. 2D shape selectivity in the crystallization-driven self-assembly of polylactide block copolymersInam, Maria; Cambridge, Graeme; Pitto-Barry, Anais; Laker, Zachary P. L.; Wilson, Neil R.; Mathers, Robert T.; Dove, Andrew P.; O'Reilly, Rachel K.Chemical Science (2017), 8 (6), 4223-4230CODEN: CSHCCN; ISSN:2041-6520. (Royal Society of Chemistry)The 2D materials such as graphene, LAPONITE clays or molybdenum disulfide nanosheets are of extremely high interest to the materials community as a result of their high surface area and controllable surface properties. While several methods to access 2D inorg. materials are known, the investigation of 2D org. nanomaterials is less well developed on account of the lack of ready synthetic accessibility. Crystn.-driven self-assembly (CDSA) has become a powerful method to access a wide range of complex but precisely-defined nanostructures. The prepn. of 2D structures, however, particularly those aimed towards biomedical applications, is limited, with few offering biocompatible and biodegradable characteristics as well as control over self-assembly in two dimensions. Herein, in contrast to conventional self-assembly rules, we show that the soly. of polylactide (PLLA)-based amphiphiles in alcs. results in unprecedented shape selectivity based on unimer soly. We use log Poct anal. to drive solvent selection for the formation of large uniform 2D diamond-shaped platelets, up to several microns in size, using long, sol. coronal blocks. By contrast, less sol. PLLA-contg. block copolymers yield cylindrical micelles and mixed morphologies. The methods developed in this work provide a simple and consistently reproducible protocol for the prepn. of well-defined 2D org. nanomaterials, whose size and morphol. are expected to facilitate potential applications in drug delivery, tissue engineering and in nanocomposites.
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