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.
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.
Block copolymer nanostructures
have received an increasing amount
of interest in the nanomedical field.[1,2] The ability
to obtain different morphologies with controlled dimensions, from
spherical micelles to rods, platelets, vesicles, and more complex
structures, opens a wide range of possibilities for potential applications.[3] For example, it has been reported that elongated
morphologies, such as rod-like particles, not only exhibit better
cell uptake rates in comparison to their spherical counterparts[4−9] but also show increased blood circulation times on increasing cylindrical
micelle length.[10]Precise control
over the formation of anisotropic materials with
biocompatible and biodegradable properties, however, represents a
key challenge in enabling their use in nanomedicine. Recent advances
in the solution crystallization of polymers have allowed access to
a wide range of complex hierarchical structures,[11] where the presence of a crystalline core-forming block
promotes the formation of morphologies with low interfacial curvature,
such as cylinders,[12−15] ribbons,[16] and platelet micelles.[17−21] Despite recent advances in precision design, in particular those
using poly(ferrocenyldimethylsilane) (PFS)[15,21] and poly(ε-caprolactone) (PCL)[22−26] block copolymers, few size-controlled assemblies
can be retained in aqueous media, with no reports of direct epitaxial
crystallization in water to date. Thus, previously reported controlled
crystallization methods are limited by the lack of translation toward
simple crystalline growth in aqueous media. Therefore, given the importance
of life-essential aqueous environments, the formation of precision
nanostructures directly in a biologically relevant solvent remains
a key challenge in opening new frontiers for biological applications.Of the previously reported micelles that can be dispersed in water,
few show significant control over dimensions and dispersity. Recently,
Manners and co-workers reported that cylindrical micelles could be
obtained from PFS-b-poly(allyl glycidyl ether), and
grafting modifications to form water-stable micelles via a postpolymerization
modification step allowed the micelles to be successfully dialyzed
from DMF into water.[15] To date, however,
such precise control over biologically relevant and degradable polymers
has not yet been achieved despite the enhanced micellar stability
offered by the crystalline core, the narrow width and length dispersity,
and the ability to modulate shape and surface chemistry through living
growth, which provides significant potential in advancing a wide range
of biomedical applications, from drug delivery to tissue engineering.
Furthermore, growth without the need for such postmodification and
solvent transfer steps would greatly simplify access to these nanostructures.
Previous reports using biocompatible polymers such as polyethylene
(PE), poly(ethylene oxide) (PEO), PCL, and poly(l-lactide)
(PLLA) have shown that these polymers can form both 1D and 2D assemblies
by crystallization-driven self-assembly (CDSA)[27−35] and undergo controlled growth from single crystals.[36−38] For example, Eisenberg and co-workers reported the formation of
cylindrical micelles using CDSA with a PCL core-forming block and
a PEO corona.[39] The cylindrical micelle
formation was ascribed to a crystallinity-driven ripening process
of spherical micelles in water, yielding micrometer long cylinders
after 2 weeks. However, no control was shown over the cylinders’
growth, and samples aged 3 months or longer were observed to undergo
further morphological changes into ribbon-like particles and lamellae.
Fan and co-workers also demonstrated that PEO-b-PCL
seeds can be elongated into longer fibers via two simultaneous growth
regimes, addition of unimers or end-to-end coupling of preformed cylinders.
In this example, however, conditions that are not ideal when applied
in a biological environment, including H2O/DMF or DMSO
assembly solvents, and extended time periods for micellar growth at
4 °C were required.[40] Furthermore,
PEO-b-PCL copolymers have not enabled full control
over particle morphology (a mixture of spheres and cylinders are observed
during the formation of short seeds) or precision controlled growth
that could be predicted based on the polymer-to-seed ratio.[40] An alternative approach of fragmentation and
growth of cylinders has also been reported, where the use of small
molecule hydrogen-bond donors induce fragmentation (by creating stress
in the corona) or dynamic cross-linking of the corona to allow growth.[42] However, this method is inherently limited by
the demands of the coronal chemistry and provides only moderate length
control. To date, only one example of CDSA in aqueous media has been
reported using polymers with a poly(2-isopropyl-2-oxazoline) core.[41] However, no control over growth has been achieved.Herein, we present the precise formation of biocompatible PCL block
copolymers assembled into cylindrical micelles with unprecedented
control over morphology and dimensions in both alcoholic and, for
the first time, aqueous media. We report direct epitaxial crystallization
in water without the need for postmodification or solvent transfer
steps, leading to the formation of strong, biocompatible hydrogel
materials capable of >95% cell viability. Furthermore, in contrast
to previous work, where changes in block length were necessary to
induce transitions from 1D to 2D materials,[17,18] we show that block copolymers of the same block lengths but different
coronal chemistry can be used to determine different morphologies,
including platelet-forming unimers with larger corona blocks.
Results
and Discussion
Synthesis and Preparation of PCL Crystalline
Seeds
PCL block copolymers were synthesized using a combination
of ring-opening
polymerization (ROP) and reversible addition–fragmentation
chain transfer (RAFT) polymerization (Table S1). Synthesis can be carried out on a large scale with predictable
molecular weights and narrow dispersities as determined by NMR spectroscopic
and SEC analyses (Figures S1–S5).
Polydisperse cylinders of several micrometers in length were prepared
by spontaneous nucleation in ethanol, a selective solvent for the
corona block,[27] at a concentration of 5 mg/mL,
when heated at 70 °C for 3 h and subsequently cooled down to
room temperature (Figures and S6). Self-assembly was monitored
via transmission electron microscopy (TEM), and samples were aged
for 5 days to reach well-defined structures. In order to achieve precise
control over cylinder length, sonication of the aged micelles was
carried out under controlled temperature (0 °C) using a sonication
probe. Sonication kinetics revealed controlled fracture of the micelles
according to a Gaussian scission model (Figure S7 and Table S2), where preferential
fracture occurs toward the center of cylindrical micelles with no
recombination of the fragments.[43] Uniform
crystalline seeds ca. 50 nm in length were obtained as observed by
TEM and selected area electron diffraction (SAED) (Figures and S8). Importantly, no side reactions were observed after the heating
process in ethanol or after sonication of the crystalline micelles
(Figure S9).
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.
(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
A living CDSA process was
observed, where the 50 nm crystalline
seeds serve as initiation sites for micelle growth on addition of
polymer unimers prepared by dissolving the PCL50-b-PDMA180 block copolymer in a miscible solvent,
such as tetrahydrofuran (THF). Controlled linear epitaxial growth
showed the formation of nearly monodisperse cylindrical micelles up
to several micrometers long (Figure S10), where the micelle length was found to be proportional to the amount
of unimer added (Figure ) (Lw/Ln ≤
1.1 where Ln = number-average length and Lw = weight-average length). In contrast, the
addition of PCL50-b-PDMAEMA170 unimers in THF to previously prepared PCL50-b-PDMA180 seeds resulted in the formation of platelet micelles
(Figures S11–S14). This can be explained
using a unimer solubility approach, as reported previously,[27] where more soluble unimers lead to a preference
for the crystallization of plates as opposed to an initial aggregation
step to form cylinders.
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).
(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
A key challenge
in the field of CDSA that currently limits the translation of these
methodologies more rapidly into biomedical studies is the inability
to apply commonly studied biodegradable polymer-based micelles of
controlled length in a biologically relevant solvent. Several methods
were attempted to achieve this with our PCL50-b-PDMA180 system, including dialysis of the micelles against
water (both directly into pure water and using an ethanol/water gradient,
from 9:1 to 1:9), slow addition of water, or fast removal of organic
solvent using N2 flow and resuspension in water. However,
the structures disassembled in all attempts, leading to rapid polymer
precipitation (Figure S15). We attributed
this phenomenon to the swelling of the corona block when transferring
into water, causing stress to the crystalline structure and subsequent
fracture. As such, we concluded that protecting the PCL core with
a short block of a glassy, highly hydrophobic polymer would be more
efficient in preventing disassembly. Following this strategy, micrometer-long
cylindrical micelles were prepared from PCL50-b-PMMA20-b-PDMA200 triblock
copolymers (Figures S16–19) using
the same methodology described above (ethanol at 70 °C for 3
h and subsequent cooling to room temperature). Similarly to the diblock
copolymer system, cylindrical micelles of controlled length were isolated
by sonication and subsequent epitaxial growth in ethanol (Figure S20). Notably, the addition of the glassy,
hydrophobic midblock enabled the successful transfer of these micellar
structures into water by dialysis. We confirmed our methodology by
also successfully preparing cylinders of controlled length using an
alternative PCL50-b-PS10-b-PDMA200 triblock copolymer (Figures S21–S24).These polymers show the first
example of water-stable precision nanostructures of controllable morphology
and dimensions in water using a biocompatible and biodegradable crystalline
domain. To simplify our methods further, as well as seek to obtain
control directly in aqueous media for the first time, we investigated
the self-nucleation, sonication, and epitaxial growth in water. Self-nucleation
was carried out in water at room temperature by dissolution of the
polymer in a small amount of THF (50 mg/mL), followed by evaporation
of the organic solvent to obtain long, polydisperse cylinders (Figure S25). Sonication of the self-nucleated
cylinders in water resulted in seeds in a much shorter time scale
(ca. 5 min), while still producing a controlled seed length of ca.
40 nm, (Figures S26 and S27). Importantly,
the crystalline structure typical of PCL[45] was maintained in aqueous media, with the first strongest (110)
diffraction at 2θ = 21.41° and the second strongest (200)
diffraction at 2θ = 23.76° (Figure S27). Furthermore, the diameter of the cylinders remained constant
(ca. 12 nm) for both the long and short micelles, as confirmed by
cryogenic-TEM analysis (Figure S28), which
is indicative of the controlled nature of this process. Controlled
epitaxy was successfully achieved by adding different concentrations
of unimers in acetone (a more volatile solvent than THF) to these
seeds, followed by fast solvent evaporation to obtain stable structures
in aqueous media (Figures , S29, and S30), achieving linear
epitaxy with a micellar length that is predictable based on the unimer-to-seed
ratio. In contrast to other CDSA-formed micelles, these cylinders
represent the first example of directly preparing cylindrical micelles
of controlled dimensions in water, thus paving the way for their utility
in biological applications.
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).
(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).With the success of the above approach to prepare precisely
defined
cylindrical micelles directly in water, we sought to demonstrate the
biorelevance of our cylindrical micelles by investigating cell viability
(using cylinders ca. 50 nm in length, as these represent an ideal
size for drug delivery purposes).[46] MC3T3
(murine preosteoblasts) and A549 (humanlung cancer fibroblasts) were
treated with increasing concentrations of polymer in water, from 0
to 5 mg/mL. Cell viability was found to be higher than 95% even with
the highest concentration of polymer used (Figure S31), suggesting our PCL system is highly biocompatible and
can therefore find potential applications as a drug delivery carrier.Furthermore, labeling of such micellar constructs with functional
handles such as fluorescent molecules or radiolabels provides a simple
method by which to readily track and image the particles within biological
systems. As such, we sought to demonstrate that our water-dispersed
cylindrical micelles were easily labeled while retaining the ability
to undergo controlled living epitaxial growth in aqueous media. To
this end, we took advantage of the ease of postpolymerization modification
of the trithiocarbonate RAFT group to attach BODIPY-FL-C5-maleimide by a simple aminolysis and subsequent click reaction (Figures , S32, and S33). As expected, the living growth characteristics
were retained, demonstrating their utility for further study in this
field.
Epitaxy in Water to Form Hydrogel Materials
In order
to fully take advantage of the unprecedented control in dimensions
achieved in water, we then exploited the triblock copolymer micelle
system to create biologically relevant hydrogel materials. Using sequential
unimer additions with dye-labeled unimers, a strong hydrogel was obtained
upon fast evaporation of acetone, with an overall solid content of
15 wt % (Figure a).
Interestingly, it was observed that a minimum length of 2 μm
was necessary to obtain a hydrogel by living CDSA. Targeting shorter
lengths induced a gradual increase in viscosity, until hydrogel formation
occurred when enough unimers were added to target the 2 μm length.
Oscillatory rheology confirmed the gel-like nature of the material
with a storage modulus (G′) of 4 kPa (Figure f), around 10 times
higher than previously reported worm gels with a similar solid content.[47,48] On applied strain (300%), the loss modulus (G″)
was measured as greater than G′, indicating
that the gel structure had been destroyed; however, the G′ was recovered at rest (0.1% strain) as the gel reformed
(Figure d,e). The
pore structure of the hydrogel was confirmed by cryogenic-scanning
electron microscopy (cryo-SEM) analysis (Figure c) and, as expected, long, uniform cylinders
could be observed by TEM upon freeze-drying a small amount of sample
on the grid (Figure b).
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.
(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.Surprisingly, the hydrogel
did not swell and could not be redissolved
upon addition of water despite the absence of any cross-linking or
stabilization by chemical interactions. While the worm-gels as prepared
were stable for extended time periods (at least 2 months) in aqueous
media, the gel sheared into smaller fragments upon the addition of
a larger amount of water, most likely as a consequence of the increasing
osmotic pressure leading to fragmentation. This can be supported by
TEM analysis of the residual water after fragmentation, where several
shorter cylinders were observed (Figure S34).Finally, the cell viability, using both previously mentioned
cell
lines, was assessed in 3D by preparing a hydrogel by living CDSA in
cell-culture medium (MEM-α with addition of 10% fetal bovine
serum and 1% penicillin/streptomycin). Cells were added by injection
into the preformed gel and viability was assessed over 4 days. At
each time point, high biocompatibility (>95%) was observed in the
3D matrix (Figure S35), opening the door
to a new method for biorelevant hydrogel formation. Such systems,
already loaded with the desired concentration of a therapeutic agent,
would avoid the need for subsequent incorporation of potential drugs
after gelation, increasing the control over dose and drug release.In conclusion, we report the successful formation of crystalline
poly(ε-caprolactone)-core 1D and 2D assemblies, achieving unprecedented
control in morphology and dimension dispersities by direct epitaxial
crystallization in aqueous media for the first time. This critical
advance in the preparation of precision nanostructures is crucial
to their translation into biological applications, providing a simplified
method without the need for postpolymerization or postassembly modifications
and solvent transfer steps. Furthermore, the ability to epitaxially
grow a strong, biocompatible hydrogel from living CDSA of a biodegradable
polymer and encapsulate living cells in its matrix demonstrates the
versatility of this technique and opens vast avenues for future biorelevant
applications.
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