Zan Hua1, Robert Keogh1, Zhen Li2, Thomas R Wilks1, Guosong Chen2, Rachel K O'Reilly1. 1. Department of Chemistry, University of Warwick, Gibbet Hill Road, Coventry CV4 7AL, U.K. 2. The State Key Laboratory of Molecular Engineering of Polymers and Department of Macromolecular Science, Fudan University, Shanghai 200433, China.
Abstract
"Grafting to" polymeric nanostructures or surfaces is a simple and versatile approach to achieve functionalization. Herein, we describe the formation of mixed polymer-grafted nanoparticles through a supramolecular "grafting to" method that exploits multiple hydrogen-bonding interactions between the thymine (T)-containing cores of preformed micelles and the complementary nucleobase adenine (A) of added diblock copolymers. To demonstrate this new "grafting to" approach, mixed-corona polymeric nanoparticles with different sizes were prepared by the addition of a series of complementary diblock copolymers containing thermoresponsive poly(N-isopropylacrylamide) (PNIPAM) to a preformed micelle with a different coronal forming block, poly(4-acryloylmorpholine) (PNAM). PNIPAM chains were distributed throughout the corona and facilitated a fast and fully reversible size change of the resulting mixed-corona micelles upon heating. Through the introduction of an environmentally sensitive fluorophore, the reversible changes in nanoparticle size and coronal composition could be easily probed. Furthermore, preparation of mixed-corona micelles also enabled ligands, such as d-mannose, to be concealed and displayed on the micelle surface. This supramolecular "grafting to" approach provides a straightforward route to fabricate highly functionalized mixed polymeric nanostructures or surfaces with potential applications in targeted diagnosis or therapy and responsive surfaces.
"Grafting to" polymeric nanostructures or surfaces is a simple and versatile approach to achieve functionalization. Herein, we describe the formation of mixed polymer-grafted nanoparticles through a supramolecular "grafting to" method that exploits multiple hydrogen-bonding interactions between the thymine (T)-containing cores of preformed micelles and the complementary nucleobase adenine (A) of added diblock copolymers. To demonstrate this new "grafting to" approach, mixed-corona polymeric nanoparticles with different sizes were prepared by the addition of a series of complementary diblock copolymers containing thermoresponsive poly(N-isopropylacrylamide) (PNIPAM) to a preformed micelle with a different coronal forming block, poly(4-acryloylmorpholine) (PNAM). PNIPAM chains were distributed throughout the corona and facilitated a fast and fully reversible size change of the resulting mixed-corona micelles upon heating. Through the introduction of an environmentally sensitive fluorophore, the reversible changes in nanoparticle size and coronal composition could be easily probed. Furthermore, preparation of mixed-corona micelles also enabled ligands, such as d-mannose, to be concealed and displayed on the micelle surface. This supramolecular "grafting to" approach provides a straightforward route to fabricate highly functionalized mixed polymeric nanostructures or surfaces with potential applications in targeted diagnosis or therapy and responsive surfaces.
Hydrogen-bonding (H-bonding)
mediated assemblies have for many
decades been employed as surrogates to mimic the nanostructures formed
as a result of nucleobase pairing within RNA and DNA.[1−9] Hydrogen bonds are normally weaker than covalent and ionic bonds,
with an energy typically between 5 and 30 kJ mol–1. Importantly, although a single hydrogen bond is weak, controlled
display of multiple H-bonding groups can result in strong, specific
interactions. Synthetic chemists inspired by Nature have widely utilized
complementary H-bonding interactions to achieve templated polymerization,[10−14] mediate polymer tacticity,[15] and tune
nanoparticle morphologies.[16−18] Selective recognition of nucleobase
functionalities has also provided a new route to modify and functionalize
nucleobase- or DNA-containing nanomaterials.[19−23]Mixed polymer-grafted nanostructures and surfaces,
consisting of
two distinct polymers in the outer layer, enable various applications
such as smart wetting surfaces,[24,25] controllable oil/water
separation,[26] and cancer diagnostics.[27] Generally, mixed-corona polymeric nanostructures
are made using cooperative self-assembly of two distinct diblock copolymers
in a common selective solvent, and then microphase separation can
occur due to differences in the properties of the two diblock copolymers.[28,29] Alternatively, two “grafting” strategies can be exploited
to attach polymer chains to the surface of a nanostructure: (i) “grafting
from” and (ii) “grafting to” approaches.[30] In the “grafting from” approach,
polymer chains are formed from initiator-functionalized nanostructures/surfaces,
which can produce thick and very dense polymer layers.[31] However, stringent reaction conditions and complicated
purification steps often limit potential applications. On the other
hand, the relatively simple “grafting to” strategy involves
the attachment of prefabricated polymers via either physisorption[32] or covalent bond formation.[30,33−36] Typically, the “grafting to” strategy suffers from
several limitations. With increasing polymer molecular weight, the
reaction efficiency between the end-group and the reactive group on
the surface significantly decreases.[37] Furthermore,
steric repulsion between polymer chains is expected to hinder the
successful fabrication of novel polymeric materials due to relatively
low grafting densities.The “grafting to” strategy
also has some undoubted
advantages. Tethered polymers can be thoroughly characterized prior
to conjugation, which allows the fabrication of tailor-made nanostructures
or surfaces.[38,39] Furthermore, the “grafting
to” approach is experimentally very straightforward, unlike
the “grafting from” approach. Since the development
of “click” chemistry in the past decade, a range of
modular conjugation strategies have breathed new life into “grafting
to” approaches.[40,41] However, the relatively small
and mostly buried reactive groups of long polymer chains often result
in moderate grafting densities and require high reactant concentrations.[42,43]Stimuli-responsive polymers represent a growing cadre of materials
that support various applications such as responsive coatings and
controlled release agents.[44] Many smart
polymers have been developed to switch their various functions via
external stimuli such as pH, light, temperature, etc.[45−50] Such switching behavior has been utilized to turn off/on activity
or interaction of functional groups within the material. For example,
switching of a cationic N,N-dimethyl-2-morpholinone
(CD-Ring) film between attacking and defending against bacteria, through
a change in solution pH, has been achieved in a controlled manner.[45] Furthermore, light-responsive azobenzene[46] and thermoresponsive PNIPAM[49,50] have been utilized to reversibly conceal and expose ligand for biospecific
cell adhesion or targeting.Recent work in our group has highlighted
the effect of complementary
multiple H-bonding interactions within the core of self-assembled
nanostructures on their self-assembly behavior.[17] Indeed, the utilization of specific complementary A–T
interactions within the micelle cores enabled the progressive modulation
of nanostructure morphology. At high dilution (0.5 mg mL–1), efficient complementary interactions allowed for control over
nanostructure morphology. To expand on the utility and application
of these discoveries, we aimed to exploit the complementary interactions
within the nanostructure cores to allow for the preparation of responsive
mixed-corona micelles. Our previous work employed PNAM as the sole
hydrophilic block and thus generated micelles with a homogeneous and
non-responsive corona. In contrast, our new system uses both hydrophilic
PNAM and PNIPAM in different diblock copolymers, thus forming a mixed
corona micelle. Mixed-corona micelles containing both thermoresponsive
PNIPAM, which can reversibly manipulate the micelle surface functionality,
and a permanently hydrophilic, non-responsive PNAM, which was able
to stabilize the nanoparticles above the characteristic cloud point
of PNIPAM,[51] were prepared using a “grafting
to” approach. This approach allowed facile control of nanostructure
size through the introduction of complementary diblock copolymers,
poly(N-isopropylacrylamide)-b-poly(3-(adenine-9-yl)propylacrylamide) (PNIPAM-b-PAAm) with different chain lengths, to preformed micelles with thymine-functionalized
cores. Interestingly, the thermoresponsive polymeric micelles exhibited
behavior consistent with single particle collapse/swelling, and the
transition was fully reversible. Introduction of an environmentally
sensitive fluorophore at the chain ends of the hydrophilic blocks
using a “grafting to” approach allowed the hydrophobicity
of the corona domain of the micelles to be probed at different temperatures.
Having confirmed the reversible collapse/swelling of the thermoresponsive
chains of the corona, it was then demonstrated that it was possible
to selectively display or conceal a protein ligand using temperature
as a responsive trigger. This work demonstrates that a “grafting
to” approach, mediated by complementary nucleobase interactions,
allows for the efficient functionalization of polymeric nanostructures/surfaces
and represents an efficient route to fabricate tailor-made nanomaterials.
Experimental Section
Materials
2,2′-Azobis(isobutyronitrile)
(AIBN)
was obtained from Molekula and recrystallized from methanol. 2,2′-Azobis[2-(2-imidazolin-2-yl)propane]
dihydrochloride (VA-044, Wako) was used without further purification.
Concanavalin A (Con A) was used as purchased from Sigma-Aldrich. 4-Acryloylmorpholine
(NAM) was bought from Sigma-Aldrich and was purified by vacuum distillation. N-Isopropylacrylamide (NIPAM) was purchased from Sigma-Aldrich
and recrystallized from a toluene–hexane mixture prior to use.
3-(Adenine-9-yl)propylacrylamide (AAm), 3-(thymin-1-yl)propylacrylamide
(TAm), 2-(((butylthio)carbonothiolyl)thio)propanoic acid,
and micelle M1 were synthesized as described previously[17] and stored at 4 °C. DMF, DMSO, and other
chemicals were obtained from Fisher Chemicals and used without further
purification. Dry solvents were obtained by passing over a column
of activated alumina using an Innovative Technologies solvent purification
system. Dialysis membranes (MWCO = 3.5 kDa) were purchased from Spectra/Por.
Instrumentation
1H NMR and 13C NMR
spectra were recorded on a Bruker DPX-300, DPX-400, or HD500
spectrometer with DMSO-d6 or CDCl3 as the solvent. The chemical shifts of protons were relative
to tetramethylsilane (TMS) at δ = 0 ppm when using CDCl3 or solvent residues (DMSO 2.50 ppm). UV–vis spectra
were recorded on a PerkinElmer Lambda 35 UV–vis instrument.
Turbidimetry assays were performed as described in a previous publication.[52] Fluorescence spectra were recorded using an
Agilent Cary Eclipse fluorescence spectrophotometer. The samples were
incubated at the relevant temperatures for at least 2 min and then
measured immediately. High-resolution mass spectrometry (HR-MS) was
conducted on a Bruker UHR-Q-TOF MaXis with electrospray ionization
(ESI). Size exclusion chromatography (SEC) data were obtained in HPLC
grade DMF containing 5 mM NH4BF4 at 50 °C,
with a flow rate of 1.0 mL min–1, on a set of two
PLgel 5 μm Mixed-D columns and a guard column. SEC data were
analyzed with Cirrus SEC software calibrated using poly(methyl methacrylate)
(PMMA) standards.Hydrodynamic diameters (Dh) and size distributions of the self-assemblies were
determined by dynamic light scattering (DLS). The DLS instrumentation
consisted of a Malvern Zetasizer NanoS instrument with a 4 mW He–Ne
633 nm laser module. Measurements were made at a detection angle of
173°, and Malvern DTS 7.03 software was used to analyze the data. Dh was calculated by fitting the apparent diffusion
coefficient in the Stokes–Einstein equation Dh = kT/(3πηDapp), where k, T, and
η are the Boltzmann constant, the temperature, and the viscosity
of the solvent, respectively. As the measured sample is a solution
of monodispersed spherical micelles, Dh coincides to the real hydrodynamic diameter as Dapp is equal to the translational diffusion coefficient
(Dt). For thermoresponsive size change,
all measurements were run at least three times with a minimum of 10
runs per measurement for every temperature point. For reversible size
change, the samples were incubated at the relevant temperature for
2 min before measurement. Static light scattering (SLS) measurements
were conducted with an ALV CGS3 (λ = 632 nm) at different temperatures.
The data were collected from 50°
to 150° with an interval of 10° against a toluene standard.
The self-assembled solutions were filtered through 0.45 μm nylon
filters prior to analysis.TEM observations were performed on
a JEOL 2000FX electron microscope
at an acceleration voltage of 200 kV. TEM samples were prepared by
drop deposition of an aqueous solution onto a copper grid coated with
Formvar. Generally, a drop of sample (10 μL) was pipetted on
a grid, left for several minutes, and then blotted away. Uranyl acetate
(UA, 1%) was used for the staining of TEM samples. TEM images were
analyzed using the ImageJ software package, and over 100 particles
were counted for each sample to obtain number-average diameter Dn (for spherical micelles).
Synthesis of
Poly(N-isopropylacrylamide) (PNIPAM)
Macro-CTA via RAFT Polymerization
The typical procedure was
as follows: a 10 mL ampule was charged with NIPAM (339.5 mg, 3.0 mmol), 2-(((butylthio)carbonothiolyl)thio)propanoic
acid (2.4 mg, 0.01 mmol), AIBN (0.16 mg, 0.001 mmol), and 1,4-dioxane (0.68 mL). The mixture was thoroughly
degassed via
four freeze–pump–thaw cycles, filled with nitrogen,
and then immersed in an oil bath at 70 °C for 2 h. The conversion
was determined by 1H NMR spectroscopy. The polymerization
solution was then precipitated three times from cold diethyl ether.
The light yellow polymer was dried in a vacuum oven overnight at room
temperature and analyzed by 1H NMR spectroscopy and DMF
SEC.
Synthesis of PNIPAM-b-PAAm Diblock Copolymers
The
typical procedure was as follows. For PNIPAM262-b-PAAm20: PNIPAM262 (75 mg, 0.0025
mmol), AAm (15.4 mg, 0.0625 mmol), and AIBN (0.04 mg, 0.00025 mmol)
were dissolved in DMSO (0.3 mL). The
mixture was thoroughly degassed via four freeze–pump–thaw
cycles, filled with nitrogen, and then immersed in an oil bath at
70 °C overnight. An aliquot of the crude product was taken and
analyzed by 1H NMR spectroscopy to calculate the conversion.
The residual solution was precipitated three times from cold CH3OH. The light yellow polymer was dried in a vacuum oven overnight
at room temperature and analyzed by 1H NMR spectroscopy
and DMF SEC. The synthetic details and characterization of the fluorescent
ABM and d-mannose containing CTAs can be found in the Supporting Information (Figures S1–S4,
Schemes S1 and S2).
Self-Assembly of PNAM98-b-PTAm302P10 Diblock Copolymer
in Water
The
diblock PNAM98-b-PTAm302P10 was synthesized using a d-mannose containing
CTA (Figure S4). For the self-assembly
of P10, a solvent switch method was used. Specifically,
the diblock copolymer was dissolved in DMF (at 8 mg mL–1) and stirred for 2 h. Then an excess
of 18.2 MΩ·cm water was added via a syringe pump at a rate
of 1 mL h–1. The final volume ratio between water
and organic solvent was 8:1. The solution was then dialyzed against 18.2 MΩ·cm water (MWCO
= 3.5 kDa), incorporating
at least six water changes, to afford self-assemblies (M10) at a concentration of ca. 1 mg mL–1.
Preparation
of Mixed-Corona Micelles Containing PNIPAM-b-PAAm
and PNAM-b-PTAm
Diblockcopolymers PNIPAM-b-PAAmP2–P9 were
dissolved in H2O at 10 mg mL–1. This
was then added to the micellar solution of M1 or M10 (0.5 mg mL–1) dropwise with stirring.
The molar ratios were calculated according to the Mn determined from 1H NMR spectroscopic analyses
and the polymer mass concentration. The mixture was then sealed and
allowed to stir at room temperature for at least 2 h. The solutions
were then analyzed by DLS, TEM, and SLS.
Results and Discussion
Synthesis
of Mixed-Corona Micelles through a Supramolecular
“Grafting To” Approach
A diblock copolymer, P1, with a permanently hydrophilic domain and a thymine functional
hydrophobic block was prepared by RAFT polymerization. The self-assembly
of this diblock copolymer was achieved via a solvent switch method
as reported previously to afford micelle M1 (Dh = 69 nm, PD = 0.058) at ca. 1 mg mL–1. In order to fabricate mixed-corona micelles using a “grafting
to” approach a series of PNIPAM-b-PAAmdiblockcopolymers with various hydrophilic block lengths were also prepared
via RAFT polymerization (Table , P2–P5, Figures S5 and S6). Subsequently, 1 mol equiv. of complementary
diblock copolymers P2–P5 in water
was added to the solution of micelle M1 with stirring
at room temperature and left for at least 2 h. In agreement with our
previous work, no morphology transition or disassembly occurred when
only 1 mol equiv. of complementary diblock copolymers was added to
the preformed micelles.[17] Using this approach,
well-defined mixed-corona micelles M2–M5 were formed through multiple H-bonding interactions between the
thymine-containing micelle core of M1 and complementary
adenine-containing diblock copolymers P2–P5 (Scheme and Figures S7a–S10a).
Table 1
Characterization Data of Polymers P1–P10
Polymer
Structure
Mn,NMRa (kDa)
Mn,SECb (kDa)
ĐMb
P1
PNAM96-b-PTAm301
85.1
68.4
1.29
P2
PNIPAM96-b-PAAm20
15.5
17.8
1.05
P3
PNIPAM176-b-PAAm20
25.3
23.9
1.10
P4
PNIPAM262-b-PAAm20
35.3
34.1
1.13
P5
PNIPAM438-b-PAAm20
56.7
52.9
1.18
P6
PNIPAM262
29.9
31.6
1.09
P7
PNAM295-b-PAAm20
47.0
36.8
1.17
P8
PNIPAM237-b-PAAm20c
33.0
32.8
1.17
P9
PNAM244-b-PAAm20c
40.5
33.0
1.25
P10
PNAM98-b-PTAm302d
85.8
64.2
1.32
Determined by 1H NMR
spectroscopy (400 MHz) in deuterated DMSO.
Determined by DMF SEC, with poly(methyl
methacrylate) (PMMA) standards.
Aminobromomaleimide-containing chain
transfer agent (CTA) was used.
d-mannose containing CTA
was used.
Scheme 1
Syntheses of Mixed-Corona
Polymeric Nanostructures M2–M7 through
a Supramolecular “Grafting
To” Approach Mediated by Complementary Nucleobase Interactions
Determined by 1H NMR
spectroscopy (400 MHz) in deuterated DMSO.Determined by DMF SEC, with poly(methyl
methacrylate) (PMMA) standards.Aminobromomaleimide-containing chain
transfer agent (CTA) was used.d-mannose containing CTA
was used.Mixed-corona micelles generally
inherit the solution properties
of both corona-forming blocks. Indeed, dynamic light scattering (DLS)
analysis indicated that the PNIPAM chains in the mixed-corona micelles
collapsed, and no aggregation between self-assembled nanostructures
was observed at 60 °C (see Figures S7b–S10b). For example, Figure a shows the heating process for M4 and the resulting
hydrodynamic diameter of the mixed-corona micelles, which decreased
from ca. 89 to ca. 70 nm upon heating from 15 to 60 °C. Meanwhile,
the polydispersity values of the mixed-corona micelles were determined
to lie in a range of 0.02–0.08 during this heating process.
Micelle M4 solution was dried and stained with uranyl
acetate at 20 and 60 °C for TEM imaging (Figures b and 1c, respectively).
TEM images further suggested that no aggregation was observed at 60
°C. Meanwhile, smaller spherical nanoparticles with diameter
ca. 61 nm were observed at 60 °C compared with spherical nanoparticles
with diameter ca. 70 nm at 20 °C. This further suggested that
these “grafting to” mixed-corona micelles underwent
intraparticle chain collapse without interparticle aggregation. In
stark contrast, upon addition of 1 mol equiv. of PNIPAM P6 without a complementary nucleobase block to preformed micelle M1, large aggregates and much higher dispersity values were
observed by DLS for the resultant micelle, M6, above
the cloud point of the PNIPAM block (Scheme and Figure S11a). Notably, complementary diblock copolymers P2–P5 with small anchoring groups avoided the formation of frozen
aggregates and facilitated efficient incorporation of the complementary
diblock copolymers. Static light scattering (SLS) analyses of micelle M4 also indicated no appreciable change in the apparent molecular
weight by light scattering (Mw) and aggregation
number (Nagg) of the respective micelles
at 15, 35, and 50 °C (Figure S12).[53] On the basis of these initial results, we proposed
that the size change of the mixed-corona micelle upon heating was
a result of PNIPAM collapse with retention of the micellar structure
rather than disassembly and re-formation of the micellar aggregates
(Scheme ). As expected,
the hydrophilic PNAM chains were still capable of stabilizing mixed-corona
micelles even when the PNIPAM chains were fully collapsed at elevated
temperatures.
Figure 1
(a) Variation of the hydrodynamic diameter (Dh) of the mixed-corona micelles M4 with temperature
as determined by DLS; TEM images (stained with uranyl acetate) and
histograms of number-average diameter distribution of M4 at (b, c) 20 °C and (d, e) 60 °C. Scale bar: 200 nm.
(a) Variation of the hydrodynamic diameter (Dh) of the mixed-corona micelles M4 with temperature
as determined by DLS; TEM images (stained with uranyl acetate) and
histograms of number-average diameter distribution of M4 at (b, c) 20 °C and (d, e) 60 °C. Scale bar: 200 nm.Given that H-bonding interactions
are known to be disrupted at
elevated temperatures, we next investigated the effect of temperature
on PNAM corona micelles prepared by a “grafting to”
approach through the addition of a non-responsive diblock copolymer, P7 (PNAM295-b-PAAm20), to the preformed micelle M1 (Scheme ). The resultant micelle M7 was
investigated by temperature-dependent DLS, and no appreciable size
change was observed at elevated temperatures, which demonstrated the
stability of the H-bonding interactions in the micellar core up to
60 °C (Figure S11b). This result also
suggested that the size decrease observed in the mixed-corona micelles M2–M5 were solely caused by the intraparticle
PNIPAM chain collapsing rather than the separation of complementary
polymer chains at elevated temperatures.
Reversible Alteration of
the Sizes of Mixed-Corona Nanoparticles
The size of a nanoparticle
is an important parameter that affects
the majority of applications but perhaps most notably their application
in nanomedicine. In biomedical delivery applications, nanoparticle
sizes greatly influence their circulation time, rate of clearance,
selective tissue distribution, and intracellular fate.[54] To circumvent the need for laborious syntheses
to access nanoparticles of a particular size, the “grafting
to” strategy described here provides a facile method to prepare
nanoparticles of controlled sizes. Indeed, we have demonstrated that
a series of nanoparticles with different sizes (75–110 nm)
could be easily produced by adding complementary diblock copolymers
with different chain lengths to a single preformed micelle (M1 of a small size 69 nm). Moreover, the composition and properties
of the newly formed nanoparticles could be adjusted by changing the
chemistry of the added complementary block copolymers.To demonstrate
this approach, 1 mol equiv. of complementary diblock copolymers P2–P5 was added to separate solutions
of preformed micelle M1. Hydrodynamic diameters of the
resultant nanoparticles were observed to increase stepwise from ca.
69 nm for M1 to ca. 75 nm for M2 and then
to ca. 110 nm for M5. We propose that this increase was
due to the increase in PNIPAM chain lengths in the added complementary
diblock copolymers. Upon heating of the mixed-corona micelle solutions,
the PNIPAM chains appeared to gradually collapse up to their cloud
point at 32 °C (Figure a). Above 40 °C, there was no further size alteration
observed by DLS analysis. It is notable that mixed-corona micelles M2–M5 all collapsed to micelles of similar
sizes (70–74 nm in hydrodynamic diameter) at 60 °C. We
presumed that this was because the collapsed PNIPAM chains at elevated
temperatures resided at the core–corona interface and therefore
played a negligible role in determining the mixed-corona micelles’
hydrodynamic diameters.
Figure 2
(a) DLS analyses of the mixed-corona micelles M2–M5 with different PNIPAM chain lengths
heated from 15 to 60
°C. (b) Reversible size change (Dh) of mixed-corona micelles M2–M5 at both 15 and 60 °C. Error bars show size dispersity (PD).
(a) DLS analyses of the mixed-corona micelles M2–M5 with different PNIPAM chain lengths
heated from 15 to 60
°C. (b) Reversible size change (Dh) of mixed-corona micelles M2–M5 at both 15 and 60 °C. Error bars show size dispersity (PD).For thermoresponsive nanoparticles,
fast and fully reversible switching
behavior is of great importance.[55−57] As shown in Figure b, size switching
of the mixed-corona micelles could be performed for at least five
heating and cooling cycles, highlighting that this transition was
fully reversible. More importantly, the transition could be achieved
in just 2 min as determined by DLS analysis. We propose that the distribution
of both thermoresponsive PNIPAM chains and non-responsive PNAM chains
in the mixed micelle corona led to less chain entanglement and as
a result a faster transition compared with micelles which have only
a PNIPAM corona domain.[55,56] Therefore, the “grafting
to” mixed nature of the micelle coronas resulted in cooperative
effects—nanoparticles were stabilized and the speed of the
coronal collapse increased. The dispersity of the nanoparticles at
both high and low temperatures remained below 0.1 throughout the five
cycles. Hence, we propose that at low temperatures the elongated PNIPAM
chains served as the outer corona and stabilized the large mixed micelles.
Then at high temperatures, the smaller mixed micelles remained stabilized
by the hydrophilic PNAM chains, which were revealed as a result of
the collapse of PNIPAM chains to the core–corona interface.
Altering the Coronas and Surfaces of Mixed-Corona Nanoparticles
Changes in the surface chemistry of nanostructures can be used
to modulate hydrophilicity, cellular uptake, and endocytosis.[49] However, it is difficult to probe a nanoparticle
surface’s chemistry and local environment. Recent work in our
group has reported the development of aminobromomaleimide (ABM)
and dithiolmalemide (DTM) fluorophores.[58,59] These are
a new class of highly emissive compounds which can be readily incorporated
into micellar constructs without noticeable effects on the particle
size or dynamics.[60,61] Interestingly, these fluorophores
show much lower emission in water compared with more hydrophobic environments
and a concentration independent emission maximum.[62] We therefore proposed that ABMs could be used as a probe
to provide a fluorescence read-out of the hydrophobicity of the fluorophore’s
local environment.[63] In the present case,
it was envisaged that ABMs could be used to reveal the hydration state
of the coronal domain of the mixed-corona micelles.Fluorescent
diblock copolymerPNIPAM237-b-PAAm20P8 was synthesized (as described for P2–P5) and added to preformed micelle M1 to yield the mixed-corona micelle M8 (Scheme and Table ). A clear fluorescence emission
peak at 488 nm (λex = 350 nm) was observed at 40
°C (when the PNIPAM coronal chain was collapsed and hydrophobic
in nature), which was attributed to the fluorescence emission of the
ABM fluorophore in a hydrophobic environment (Figure a). This fluorescence emission peak was no
longer present at 25 °C as the elongated PNIPAM resulted in ABM
being brought into a more hydrophilic environment, which led to fluorescence
quenching. Note that the shoulder peak at 430 nm (in Figure a) appeared as a result of
scattering of the micelle solution. A control experiment using micelle M4 (which did not contain the ABM functionality) displayed
a slight decrease in the shoulder peak at 40 °C (Figure S13a), which can be rationalized by assuming
that the collapsing nanostructures at 40 °C contributed to less
scattering due to their smaller size. Moreover, the non-responsive
corona micelle M9 consisting of preformed micelle M1 and ABM-functionalized PNAM244-b-PAAm20P9 exhibited no appreciable fluorescence
change at 25 and 40 °C, as the fluorophore did not undergo any
significant microenvironment change as the hydrophobicity of the coronal
block did not change at elevated temperature (Figure S13b). A similar fluorescence read-out response was
observed for the mixed micelle consisting of micelle M1 and ABM-attached PNIPAM40-b-PAAm20 (see Figure S13c). Hence, the
fluorescence read-out of the ABM mixed micelles was proposed to be
determined by the hydrophobic microenvironment where the dye lies
and hence is independent of PNIPAM corona block length. We concluded
that the fluorescence ON/OFF switch was triggered by changes in the
microenvironment surrounding the ABM fluorophore upon collapse of
the responsive block—this enabled a read-out of the surface
state of the mixed corona micelles. Again, as suggested by DLS analysis
and as shown in Figure b, the temperature-dependent fluorescence switch was fully reversible.
The intensity of the fluorescence emission peak at 488 nm at 40 °C
did not decrease, even after five cycles of heating and cooling, which
indicated that collapse and expansion of the PNIPAM did not lead to
any loss of micelle structure and confirmed the integrity of the nucleobase
interactions within the core domain during these heat–cool
cycles.
Scheme 2
Syntheses of ABM-Functionalized PNIPAM237-b-PAAm20 [P8] and Subsequent Addition
to M1 To Afford Mixed Micelles M8, and d-Mannose-Functionalized PNAM98-b-PTAm302 [P10] and Subsequent Assembly To
Afford Micelles M10 and Mixed Micelles, M11
Figure 3
Demonstration of a reversible fluorescence
ON/OFF switch using
ABM-tagged mixed-corona nanoparticles. (a) Fluorescence spectra (λex = 350 nm) of mixed-corona micelle M8 at 25
(black) and 40 °C (red). (b) Fluorescence emission intensity
of M8 at 488 nm at 25 and 40 °C for five consecutive
heating and cooling cycles (λex = 350 nm).
Demonstration of a reversible fluorescence
ON/OFF switch using
ABM-tagged mixed-corona nanoparticles. (a) Fluorescence spectra (λex = 350 nm) of mixed-corona micelle M8 at 25
(black) and 40 °C (red). (b) Fluorescence emission intensity
of M8 at 488 nm at 25 and 40 °C for five consecutive
heating and cooling cycles (λex = 350 nm).We next explored the utility of
this “grafted to”
system in controlling protein ligand display on the mixed micelle
surface using changes in temperature. To achieve this, we utilized
Concanavalin A (Con A), a tetrameric mannose-binding plant lectin,
which can effectively bind to the ligand d-mannose with moderate
binding constants.[64] This type of specific
recognition between carbohydrates and proteins is involved in many
complex cellular events, including cell adhesion, pathogen invasion,
and cancer metastasis, to name but a few.[65]d-Mannose-functionalized PNAM98-b-PTAm302P10 was synthesized and self-assembled
to form non-responsive micelle M10 as an experimental
control (Scheme and Figure S14a). In addition, d-mannose
containing mixed-corona micelles M11 were prepared by
adding diblock copolymer P8 to preformed micelle M10 (Scheme and Figure S14b) as described for the
previous mixed micellar systems. This afforded a micelle M11 with a mixed-corona domain, which consisted of a responsive PNIPAM
block bearing the ABM probe and a non-responsive PNAM block bearing
the ligand, which we proposed could be selectively revealed and buried
depending on the state of the responsive block (i.e. the temperature
of the system). To explore this, a Con A agglutination assay was used
to measure the extent of binding between Con A and M11.[52] At 25 °C, the d-mannose
ligands were expected to be fully concealed by the extended PNIPAM
chains, and indeed no agglutination was observed at this temperature
(Figure a). In contrast,
at 40 °C significant agglutination was observed—at this
temperature the PNIPAM chains were expected to collapse, revealing
the ligands for binding with the Con A receptors. Notably, the binding
between the receptor d-mannose and Con A is not reversible,
and the formed aggregates precipitated out after longer time periods.
Further analysis of the ABM-tagged mixed-corona micelle M11 using fluorescence spectroscopy confirmed the collapse of the PNIPAM
above 40 °C, with the characteristic change in the emission spectrum
of ABM again observed (Figure b).
Figure 4
Controlled ligand display on the mixed-corona micelle surface.
(a) Agglutination assay of mixed-corona micelle M11 with
Con A at 25 and 40 °C. (b) Fluorescence spectra of M11 at 25 and 40 °C (λex = 350 nm).
Controlled ligand display on the mixed-corona micelle surface.
(a) Agglutination assay of mixed-corona micelle M11 with
Con A at 25 and 40 °C. (b) Fluorescence spectra of M11 at 25 and 40 °C (λex = 350 nm).
Conclusions
In summary, a novel
supramolecular “grafting to”
strategy for the formation of well-defined mixed-corona micelles has
been demonstrated. This strategy involved the exploitation of multiple
complementary H-bonding interactions between thymine-containing cores
of preformed micelles and added adenine-containing diblock copolymers.
Polymeric micelles with different sizes were easily prepared by changing
the chain lengths of the added complementary diblock copolymers. Intraparticle
chain collapse allowed micelle size and coronal state to be reversibly
altered in response to an external stimulus—in this case temperature—and
this could be coupled to the reversible display/concealment of protein
ligands at the nanoparticle surface. While in this work a temperature
responsive block was utilized to showcase the viability of this approach
for achieving the reversible presentation of functionality at the
surface of a nanoparticle, other stimuli responses could be easily
utilized such as pH, light, etc. Indeed, through the synthesis of
the appropriate complementary diblock copolymers, the incorporation
of a diverse range of functionalities at the nanoparticle surface
can be envisaged using this supramolecular “grafting to”
approach. This work provides a new route and platform to fabricate
mixed polymer-grafted nanostructures and surfaces, which may find
potential applications as smart materials for utilization in a range
of areas such as nanomedicine.
Authors: Mathew P Robin; Paul Wilson; Anne B Mabire; Jenny K Kiviaho; Jeffery E Raymond; David M Haddleton; Rachel K O'Reilly Journal: J Am Chem Soc Date: 2013-02-13 Impact factor: 15.419
Authors: Anne B Mabire; Mathew P Robin; Wen-Dong Quan; Helen Willcock; Vasilios G Stavros; Rachel K O'Reilly Journal: Chem Commun (Camb) Date: 2015-06-14 Impact factor: 6.222