pH- and Thermo-Responsive Water-Soluble Smart Polyion Complex (PIC) Vesicle with Polyampholyte Shells

Abstract

A diblock copolymer (P(VBTAC/NaSS)₁₇-b-PAPTAC₅₀; P(VS)₁₇A₅₀) composed of amphoteric random copolymer, poly(vinylbenzyl trimethylammonium chloride-co-sodium p-styrensunfonate) (P(VBTAC/NaSS); P(VS)) and cationic poly(3-(acrylamidopropyl) trimethylammonium chloride) (PAPTAC; A) block, and poly(acrylic acid) (PAAc₄₉) were prepared via a reversible addition−fragmentation chain transfer radical polymerization. Scrips V, S, and A represent VBTAC, NaSS, and PAPTAC blocks, respectively. Water-soluble polyion complex (PIC) vesicles were formed by mixing P(VS)₁₇A₅₀ and PAAc₄₉ in water under basic conditions through electrostatic interactions between the cationic PAPTAC block and PAA_c49 with the deprotonated pendant carboxylate anions. The PIC vesicle collapsed under an acidic medium because the pendant carboxylate anions in PAAc₄₉ were protonated to delete the anionic charges. The PIC vesicle comprises an ionic PAPTAC/PAAc membrane coated with amphoteric random copolymer P(VS)₁₇ shells. The PIC vesicle showed upper critical solution temperature (UCST) behavior in aqueous solutions because of the P(VS)₁₇ shells. The pH- and thermo-responsive behavior of the PIC vesicle were studied using ¹H NMR, static and dynamic light scattering, and percent transmittance measurements. When the ratio of the oppositely charged polymers in PAPTAC/PAAc was equal, the size and light scattering intensity of the PIC vesicle reached maximum values. The hydrophilic guest molecules can be encapsulated into the PIC vesicle at the base medium and released under acidic conditions. It is expected that the PIC vesicles will be applied as a smart drug delivery system.

1. Introduction

Owing to electrostatic interactions between cationic and anionic units, oppositely charged polyelectrolytes in water form a polyion complex (PIC) or polyelectrolytes complex [1,2]. Furthermore, PIC micelles with a PIC core and hydrophilic noncharged shells can be prepared without using an organic solvent in water [3,4]. Smart PIC aggregates have single- or multi-responsive properties against external stimuli, such as pH, temperature, and light irradiation. They show substantial changes in their properties with a slight change in the surrounding environments [5]. The PIC aggregates have attracted huge interest from many researchers because of their advantages. The PIC aggregates are expected to meet some drug delivery system (DDS) assignments, such as the targeted and controlled release of the drug. The pH of the medium is an important factor in the controlled release of a DDS. The microenvironment of cancer tumors is acidic, whereas it is nearly neutral for normal cells [6]. The change in the pH of the environment results in an ideal pH-responsive DDS carrier, which can be applied in cancer treatments. Therefore, many PIC aggregate systems, which target the release of drugs in response to the acidity of the surroundings, have been reported [7,8,9,10,11,12]. Water-soluble pH-responsive PIC vesicles covered with biocompatible poly(2-(methacryloyloxy)ethyl phosphorylcholine) (PMPC) shells have also been reported [3]. The PIC vesicle was coassembled via electrostatic interactions between PMAPTAC and ionized PAaH under a basic medium by mixing oppositely charged diblock copolymers consisting of PMPC and cationic poly(3-(methacrylamidopropyl) trimethylammonium chloride) (PMAPTAC), or anionic poly(sodium 6-acrylamidohexanoate) (PAaH) blocks. The hydrophilic guest molecule, Texas red-labeled dextran, was encapsulated into the inner water phase of the PIC vesicle. Under the acidic medium, PAaH was protonated to become noncharged resulting in a dissociation of the PIC vesicle, where the guest molecule was released. Therefore, the PIC vesicle is expected to effectively target the drug in the cytoplasm.

Similarly, the environment’s temperature is a widely used parameter in the controlled release of drugs [13,14,15,16,17]. Matsuoka et al. [13] reported on thermo-responsive PIC aggregates. Diblock copolymers composed of poly(sulfopropyl dimethylammonium propylacrylamide) (PSPP) and cationic PMAPTAC or anionic poly(sodium p-styrenesulfonate) (PNaSS) were mixed in water to form PIC micelles with a PMAPTAC/PNaSS core and PSPP shells. The PIC micelles showed an upper critical solution temperature (UCST) caused by the PSPP shells. They formed large aggregates of micelles below the phase transition temperature of the PSPP shells owing to the PSPP chain shrinkage. The UCST behavior of the PIC aggregates can be controlled using the polymer concentration and the degree of polymerization (DP) of the PSPP chains. Furthermore, some other PIC systems have been fabricated with the target to release a drug in response to environments containing glucose to deal with diabetes [18,19] or to use light irradiation to control the release of the drug [20,21].

These single stimulus-responsive PIC aggregates have been studied and applied. Besides stimuli response, PIC aggregates have shown other outstanding advantages [22,23,24,25,26,27]. For instance, dual pH- and thermo-responsive PIC micelles were prepared from a co-assembly of oppositely charged diblock copolymers, poly(N-methyl-2-vinyl pyridinium iodide)-block-poly(ethylene oxide) (P2MVP-b-PEO) and poly(acrylic acid)-block-poly(isopropyl acrylamide) (PAAc-b-PNIPAM) in water [27]. Under a basic medium at 25 °C, the PIC micelles were formed owing to the electrostatic interaction between the PAAc and P2MPV blocks with the PAAc/P2MVP core and hydrophilic mixed PNIPAM/PEG shells. However, under an acidic medium, the size of the aggregates increased, which can be attributed to the aggregation formed by hydrogen bonding between PAAc and PNIPAM/PEO. At high concentrations, the core–shell structure of PIC micelles switches to core–shell–corona (onion type) with a PNIPAM core, covered with a mixed P2MVP/PAAc shell, and a PEO outer corona at 60 °C.

Polyampholytes or amphoteric random copolymers are polymers that consist of cationic and anionic units in their structure [28,29,30]. Amphoteric random copolymers have no charge, which is comparable to the balance between oppositely charged groups since they contain both pendant cationic and anionic groups [31,32]. Therefore, to avoid complex precipitation, the polyampholytes can be used as a hydrophilic nonionic block. Furthermore, some amphoteric polymers show thermo-responsive and protein antifouling properties. Yusa et al. [28] reported that amphoteric diblock copolymers from poly(2-acrylamido-2-methylpropanesulfonic acid sodium salt) (PAMPS) and poly(3-(acrylamido)propyl trimethylammonium chloride) (PAPTAC) synthesized via a reversible addition−fragmentation chain transfer (RAFT) radical polymerization. The polymer exhibited a lower critical solution temperature (LCST) behavior due to the hydrogen-bonding interactions of the pendant amide groups and water molecules. The thermo-responsive behavior of the polymers can be controlled by adjusting the NaCl concentration. Meanwhile, P(APMPS/APTAC), a random copolymer prepared by RAFT with the same content as APMPS and APTAC, showed an ability in protein antifouling [33]. The PIC micelle consists of amphoteric random copolymer P(AMPS/APTAC) shells that show no interaction with proteins. Furthermore, a UCST-type thermo-responsive amphoteric random copolymer (P(VBTAC/NaSS)) composed of the pendant quaternary ammonium group in vinylbenzyl trimethylammonium chloride (VBTAC) and pendant sulfonate in NaSS with the same content of each monomer, was prepared via RAFT polymerization [34]. P(VBTAC/NaSS) showed the UCST behavior caused by electrostatic interactions between PVBTAC and PNaSS. The UCST behavior was affected by DP and concentrations of P(VBTAC/NaSS).

Based on prior studies, we designed pH- and thermos-responsive PIC micelles. The interaction of the PIC vesicle with the hydrophobic surface may be controlled by temperature if the PIC vesicle surface hydrophobicity is changed by heating. For example, if the PIC vesicle surface changes to be hydrophobic with cooling, the interactions increase between the PIC vesicle and cell. Furthermore, if the PIC vesicle is dissociated in response to pH, the encapsulated guest molecules are released by pH change. Particularly, cancer tissue is more acidic than healthy tissue, so designing a pH-responsive PIC vesicle is useful for cancer treatment. In this study, we have prepared a diblock copolymer (P(VS)₁₇A₅₀) consisting of polyampholyte (P(VBTAC/NaSS)₁₇; P(VS)₁₇) block and a cationic PAPTAC₅₀ (A₅₀) block (Scheme 1). Furthermore, the PIC aggregates were prepared by mixing P(VS)₁₇A₅₀ and polyacrylic acid (PAAc₄₉) in a basic medium because of electrostatic interactions between the cationic PAPTAC block and deprotonated anionic PAAc₄₉. The PIC aggregate had a vesicle structure, which confirmed that the PIC aggregate could encapsulate a hydrophilic guest molecule into the hollow core. PAAc indicated pH-responsive behavior caused by protonation and the pendant carboxyl groups [35,36,37]. The PAAc pendant carboxyl groups are protonated and neutralized under acidic conditions, leading to the dissociation of the PIC vesicles. The PIC vesicle was formed from the PAPTAC/PAAc membrane, covered with the amphoteric random copolymer P(VS)₁₇ shells. In this study, to synthesize P(VS)₁₇, equimolar amounts of styrene-type cationic VBTAC and anionic NaSS were randomly copolymerized via RAFT. Then, the cationic APTAC monomer was polymerized to synthesize P(SV)₁₇A₅₀. Furthermore, PAAc₄₉ was also synthesized via RAFT. Polymers were characterized with NMR and gel-permeation chromatography (GPC) measurements. The pH- and thermo-responsive properties of the PIC vesicle were studied with percent transmittance, dynamic and static light scattering, zeta-potential, and NMR measurements. Additionally, since the P(SV)₁₇ polyampholyte shells exhibited the UCST behavior, controlling the interaction with proteins and cells in response to temperature may be possible. Furthermore, the P(SV)₁₇ polyampholyte can suppress protein adsorption. Therefore, the PIC vesicles are expected to modify the surfaces of medical devices.

2. Materials and Methods

2.1. Materials

Vinylbenzyl trimethylammonium chloride (VBTAC, 99%) methoxy poly(ethylene glycol) labeled pyrene (PEG-Py, M_n = 2000 g/mol) was purchased from Sigma-Aldrich (St. Louis, MO, USA), sodium p-styrenesulfonate (NaSS, 98%) from Tokyo Chemical Industry (Tokyo, Japan), and 4,4-azobis(4-cyanopentanoic acid) (V-501, 98%) and 2,2-azobisisobutyronitrile (AIBN, 98%) from Wako Pure Chemical (Osaka, Japan) were used without further purification. Acrylic acid (AAc, 98%) from Wako Pure Chemical (Osaka, Japan) was distilled under reduced pressure. 4-Cyanopentanoic acid dithiobenzoate (CPD) was synthesized using the previously reported method [38]. The water was purified using an ion-exchange column system.

2.2. Synthesis of P(VS)₁₇ Random Copolymer

First, amphoteric random copolymer (P(VS)₁₇) was prepared via RAFT polymerization in accordance with the previous report [34]. VTBAC (3.18 g, 15.0 mmol), NaSS (3.09 g, 15.0 mmol), CPD (419 mg, 1.50 mmol), and V-501 (210 mg, 0.749 mmol) were dissolved in 30 mL of mixed solvent of 1.2 M NaCl aqueous solution and MeOH (9/1, v/v) with the feed molar ratio of [VBTAC]/[NaSS]/[CPD]/[V-501] = 10/10/1/0.5. The mixture was then, degassed by purging with Ar gas for 30 min. Polymerization occurred at 70 °C for 5 h. After polymerization, ¹H NMR spectra were used to calculate the polymerization conversion of VBTAC and NaSS (conversion = 84.5%). The reaction mixture was dialyzed against 1.2-M NaCl aqueous solution for two days and pure water for one day and collected using a freeze-drying method (4.69 g, 67.9%). The theoretical DP(theo)) and number-average molecular weight (M_n(theo)) were 17 and 3.83 × 10³ g/mol. The VBTAC and NaSS contents were determined using ¹H NMR spectra of P(VS)₁₇ and found to be 51.9 and 48.1 mol%, respectively.

2.3. P(VBTAC/NaSS)₁₇-b-PAPTAC₅₀

The diblock copolymer was prepared via RAFT polymerization using P(VS)₁₇ as a macro-CTA. P(VS)₁₇ (539 mg, 0.141 mmol), APTAC (1.46 g, 7.06 mmol), and V-501 (15.7 mg, 0.06 mmol) with a feed molar ratio of [P(VS)₁₇]/[APTAC]/[AIBN] = 1/50/0.4 were dissolved in water (7.0 mL). The mixture was degassed by purging with Ar gas for 30 min. Polymerization occurred at 70 °C for 24 h. The polymerization conversion was calculated from ¹H NMR integral intensity ratio of the vinyl protons and phenyl protons to 5.6 and 6.4–7.6 ppm, respectively, (conversion = 98.4%). Then, the reaction mixture was dialyzed against pure water for 5 days and collected using a freeze-drying method (1.55 g, 77.5%). From ¹H NMR measurement, the DP(NMR)) of the APTAC block was estimated to be 50. The number-average molecular weight (M_n(GPC)) and polydispersity index (M_w/M_n) of P(VS)₁₇A₅₀ were estimated to be 5.70 × 10⁴ g/mol and 1.04, respectively, based on the GPC measurement.

2.4. Synthesis of PAAc₄₉

RAFT polymerization was used to prepare poly(acrylic acid) (PAAc₄₉). AAc (7.20 g, 100 mmol), CPD (280 mg, 0.99 mg), and AIBN (65.7 mg, 0.40 mmol) with a feed molar ratio of [AAc]/[CPD]/[AIBN] = 100/1/0.4 were dissolved in methanol (100 mL). The mixture was degassed by purging with Ar gas for 30 min. Polymerization occurred at 60 °C for 47 h. From the ¹H NMR integral intensity ratio, the polymerization conversion of the vinyl proton signal at 5.8 ppm and terminal phenyl group protons at 7.3–7.9 ppm (conversion = 36.3%) was estimated. Then, the reaction mixture was dialyzed against pure water for one week and collected using a freeze-drying method (0.97 g, 12.9%). From ¹H NMR measurement the DP(NMR) of PAAc₄₉ was calculated to be 49. From GPC measurement, the M_n(GPC) and M_w/M_n of P(VS)₁₇A₅₀ were 1.46 × 10⁴ g/mol and 1.07, respectively.

2.5. Preparation of PIC Vesicles

P(VS)₁₇A₅₀ and PAAc₄₉ were individually dissolved in water at C_p = 1.0 g/L as stock solutions to prepare the PIC vesicles. The PIC vesicles were fabricated by mixing the cationic P(VS)₁₇A₅₀ solution with the anionic PAAc₄₉ solution while stirring for 5 min at room temperature. The pH of the mixed solution was adjusted using 0.1-M NaOH and 0.1-M HCl aqueous solutions, then left for one day to obtain an equilibrium state. The mole fraction of positively charged (f⁺ = [APTAC]/([APTAC] + [PAAc]) in the PIC vesicle solution corresponds to the mixing ratio of the opposite polymers

2.6. Encapsulation of PEG-Py

PEG-Py (0.01 g/L) aqueous solution was prepared. Then, P(VS)₁₇A₅₀ (0.1 g/L) and PAAc₄₉ (0.1 g/L) were separately dissolved in the PEG-Py aqueous solution. Subsequently, the P(VS)₁₇A₅₀ aqueous solution was added to the PAAc₄₉ aqueous solution with f⁺ = 0.5 and stirred for 5 min at room temperature. The mixed solution was adjusted to pH 10 using NaOH solution and then dialyzed for 20 days against an aqueous solution at pH 10 using a Harvard Apparatus (Holliston, MA, USA) polycarbonate membrane with 10-nm pores. The solvent was replaced every 12 h to remove the unbound PEG-Py molecules. A PEG-Py aqueous solution (0.01 g/L) without a PIC vesicle was dialyzed with the same procedure. Fluorescence spectroscopy measurements for PEG-Py in the presence and absence of the PIC vesicles were performed to detect PEG-Py content in the solution after dialysis. The loading capacity (LC) and loading efficiency (LE) were calculated according to the following Equations [39]:

$$\mathrm{LE} (\%)=\frac{\mathrm{Weight} \mathrm{of} \mathrm{encapsulated} \mathrm{PEG}-\mathrm{Py}}{\mathrm{Weight} \mathrm{of} \mathrm{total} \mathrm{PEG}-\mathrm{Py}} \times 100,$$

(1)

$$\mathrm{LC} (\%)=\frac{\mathrm{Weight} \mathrm{of} \mathrm{encapsulated} \mathrm{PEG}-\mathrm{Py}}{\mathrm{Weight} \mathrm{of} \mathrm{the} \mathrm{PIC} \mathrm{aggregate}} \times 100.$$

(2)

2.7. Measurements

¹H NMR measurements were performed to determine the complex characteristics of the polymer and polyion complex using a JEOL (Tokyo, Japan) JNM-ECZ 400 MHz NMR. The sample solutions were prepared in D₂O and adjusted with NaOD or DCl solutions to desired pH. The standard pulse program, stebpgp1s19, used a stimulated echo, bipolar gradient pulse, and one spoil gradient with 3-9-19 pulse sequence (WATERGATE) solvent suppression of the water signal. The GPC measurements were used to determine the number-average molecular weight (M_n(GPC)) and polydispersity index (M_w/M_n). For cationic polymer, P(VS)₁₇A₅₀, a mixture of Na₂SO₄ (0.3 M) and CH₃COOH (0.5 M) aqueous solution was used as a cationic eluent. P(VS)₁₇A₅₀ signal was detected using Jasco (Tokyo, Japan) RI-2031 Plus refractive index (RI) detector equipped with a PU-2080 Plus column operating at 40 °C. Using a calibrated curve of standard poly(2-vinylpyridine), the values of M_n(GPC) and M_w/M_n for P(VS)₁₇A₅₀ were estimated. For anionic homopolymer PAAc₄₉, GPC spectra were obtained from Tosoh RI-8020 RI working at 40 °C with a Shodex (Tokyo, Japan) GF-7M column, Tosoh (Yamaguchi, Japan) DP-8020 pump and a mixture of phosphate buffer (50 mM) at pH 9 and acetonitrile (9/1, v/v) as an anionic eluent. Using a calibration made from standard PNaSS, the values of M_n and M_w/M_n for polymers were estimated. Fourier transform infrared (FTIR) spectra were obtained using a Jasco FT/IR-4200 spectrometer. The PIC vesicle structure was confirmed via transmission electron microscopy (TEM) observation using a JEOL (Tokyo, Japan) JEM-2100. The PIC vesicle aqueous solutions with f⁺ = 0.5 and C_p = 0.1 g/L at pH 10 were prepared. Then, a drop of the sample solution was put on a copper grid coated with thin films of Formvar. The oversupply sample solution was filtered using filter paper. The next step was to stain with sodium phosphotungstate and dry under a vacuum for one night. The hydrodynamic radius (R_h), light scattering intensity (LSI), and zeta-potential of polymers and PIC vesicles were calculated using a Malvern Nano ZS with He–Ne laser (4 mW at 632.8 nm) from Malvern (Kobe, Japan). Before taking the measurements, the sample solutions were filtered using a 0.45-μm pore size membrane filter. Furthermore, to estimate the weight-average molecular weight (M_w), a z-average radius of gyration (R_g), and the second viral coefficient (A₂) values of the polymers and PIC, SLS measurements were performed using the Otsuka Electronics Photal (Osaka, Japan) SLS-6500 with a He–Ne laser (4 mW at 632.8 nm) as a light source working at 25 °C. An Otsuka Electronics Photal DRM-3000 (Osaka, Japan) differential refract meter was used to calculate dn/dC_p values at 633 nm. Percentage transmittance (%T) was measured on a Jasco (Tokyo, Japan) V-730 UV-vis spectrophotometer equipped with a temperature control system. Fluorescence spectra for PEG-Py were measured using a Hitachi (Tokyo, Japan) F-2500 fluorescence spectrometer. The excitation and emission slit widths were kept constantly at 20 and 2.5 nm, respectively.

3. Results

3.1. Preparation of P(VS)₁₇A₅₀ and PAAc₄₉

All polymers in this study were prepared via normal RAFT polymerization. An amphoteric random copolymer comprising cationic VBVTAC and anionic NaSS was prepared via RAFT radical polymerization. According to ¹H NMR, the total conversion (p) of VBTAC and NaSS was estimated to be 84.5%. The theoretical DP(theo) and theoretical number-average molecular weight (M_n(theo)) of P(VS)₁₇ were calculated using p and the following equation:

$$\mathrm{DP}\left(\mathrm{theo}\right)=\frac{{\left[\mathrm{M}\right]}_0}{{\left[\mathrm{CTA}\right]}_0} \times \frac{p}{100 }$$

(3)

$$M_{\mathrm{n}}{\left(\mathrm{theo}\right)=\mathrm{DP}}_{\mathrm{theo}}{ \times \mathrm{M}}_{\mathrm{m}}{+\mathrm{M}}_{\mathrm{CTA}}$$

(4)

where, [M]₀ and [CTA]₀ are the initial concentrations of the monomer and CTA, respectively, and M_m and M_CTA are the molecular weights of the monomer and CTA, respectively. The DP(theo) and M_n(theo) for P(VS)₁₇ were calculated to be 17 and 3.83 × 10³ g/mol, respectively. The composition of P(VS)₁₇ was estimated from ¹H NMR in D₂O containing 1.2 M NaCl at 70 °C (Figure S1). The main chain proton signals were observed at 1.5–2.1 ppm. The pendent methyl protons of the VTBAC unit were observed at 2.9 ppm. The pendant phenyl protons of the VBTAC and NaSS units are presented as 6.4–7.6 ppm. The VBTAC content in the P(VS)₁₇ block was calculated to be 51.9 mol% based on the integral intensities between the pendant phenyl and VBTAC methyl protons. The DP(NMR) for the PAPTAC block in P(VS)₁₇A₅₀ was 50, as estimated from the integral intensity of the methylene proton from the PAPTAC unit at 1.6 ppm compared with that for the phenyl protons of VBTAC and NaSS at 6.4–7.6 ppm (Figure 1a). PAAc₄₉ has a DP(NMR) of 49, estimated from the ratio of integral intensities between main chain protons at 1.5–2.3 ppm and terminal phenyl protons at 7.3–7.9 ppm, derived from the CTA fragment (Figure 1b). The M_n(NMR) and M_n(theo) values for P(VS)₁₇A₅₀ were close. The M_w/M_n values estimated from GPC for P(VS)₁₇A₅₀ and PAAc₄₉ (Figure S2) were 1.04 and 1.07, respectively, indicating that the polymers showed well-controlled structures. The DP, M_n, and M_w/M_n values for all polymers are summarized in

Table 1. Degree of polymerization (DP), number-average molecular weight (M_n), and polydispersity index (M_w/M_n).

Sample	DP (theo)	DP (NMR)	Mn(theo) 1 × 10−4 (g/mol)	Mn(NMR) 2 × 10−4 (g/mol)	Mn(GPC) 3 × 10−4 (g/mol)	Mw/Mn
P(VS)17	17	-	0.38	-	-	-
P(VS)17A50	49	50	1.40	1.41	5.70	1.04
PAAc49	36	49	0.26	0.34	1.40	1.07

¹ Calculated from Equation (4) ² Obtained from ¹H NMR ³ Obtained from GPC.

. P(VS)₁₇ could not be measured using GPC because it cannot dissolve in the eluent. FTIR spectrum was measured for P(VS)₁₇A₅₀. The pendant carbonyl signal can be seen at 1700 cm⁻¹ (Figure S3).

3.2. Preparation and Characterization of PIC Vesicles

The PIC vesicle was prepared by mixing P(VS)₁₇A₅₀ and PAAc₄₉ with f⁺ = 0.5 at C_p = 2.0 g/L in D₂O at pH 10 for the ¹H NMR measurement (Figure 1c). For DLS measurements, the PIC vesicle was prepared at 0.1 g/L; however, the C_p was too low for NMR measurements so the PIC vesicle was prepared at C_p = 2.0 g/L. After mixing, the signals from the PAPTAC₅₀ block and PAAc₄₉ disappeared. The VBTAC unit’s methylene proton signal remained at 2.9 ppm, showing that the PAPTAC block and PAA_c49 interacted to create the vesicle structure’s membrane and P(VS)₁₇ produced shells.

TEM was conducted to confirm the PIC aggregate shape. The TEM image was obtained for the stoichiometrically charge neutralized mixture of P(VS)₁₇A₅₀ and PAAc₄₉ at pH 10 (Figure 2). The particles had a spherical shape with a contrasting white center and black edge, indicating a vesicle structure in the PIC aggregates. The average radius obtained from the TEM observations was 86.2 ± 17.3 nm, close to the hydrodynamic radius (R_h) estimated from the dynamic light scattering measurements (R_h = 86.6 nm). During TEM observation, the sample shrank due to the high vacuum conditions. The PIC vesicles collapsed as they shrank and stuck to the TEM grid membrane. At that time, the PIC vesicles expanded. Therefore, the size obtained from the TEM observation did not decrease much compared to the R_h value.

The mixing ratio of the oppositely charged polymers determines the development of the PIC vesicle [40,41]. The plots of R_h, LSI, and zeta-potential with f⁺ at pH 10 were prepared (Figure 3). The C_p values in the PIC vesicle solutions were kept at 0.1 g/L. However, samples at f⁺ = 0 and 1 attributed to anionic PAAc₄₉ and cationic P(VS)₁₇A₅₀, respectively, were prepared at C_p = 2.0 g/L because R_h and zeta-potential values could not be obtained because of very low LSI at C_p = 0.1 g/L. The R_h and LSI values of the PIC vesicle reached maximum values at f⁺ = 0.5, and then the zeta-potential reached 0 mV, suggesting the neutralization of the oppositely charged PAPTAC₅₀ block and PAAc₄₉. Meanwhile, the zeta-potential values of PAAc₄₉ and the PAPTAC₅₀ block at f⁺ = 0 and 1 were −27.7 and 23.8 mV, respectively, indicating negative and positive charges.

The critical micelle concentration (CMC) of the PIC vesicle was determined to certify the thermodynamic equilibrium properties. The LSI of the PIC vesicle aqueous solutions was measured as a function of C_p. The PIC vesicle aqueous solution was prepared by mixing P(VS)₁₇A₅₀ and PAAc₄₉ in water at pH 10 with f⁺ = 0.5 at C_p = 0.1 g/L; the solution was diluted to the desired C_p using water at pH 10. The CMC for the PIC vesicle in water was determined from the relationship between the LSI ratio (I/I₀) and C_p (Figure 4). I and I₀ correspond to the LSIs of the PIC vesicle aqueous solution and water at pH 10, respectively. The crossing point of the linear portions in the low and high C_p regions was defined as the CMC value, which was 2.47 × 10⁻³ g/L. The defined CMC value implies that the PIC vesicle is in a dynamic equilibrium state. The PIC vesicle is stable above the CMC. The PIC vesicle, however, can disintegrate below the CMC into a small assembly of P(VS)₁₇A₅₀/PAAc₄₉ because of strong electrostatic interactions between them [33,42].

We studied the concentration dependence of the PIC vesicle because the SLS should be measured at different C_p values to perform the SLS measurements. The P(VS)₁₇A₅₀ and PAAc₄₉ aqueous solutions were separately prepared at C_p = 0.1, 0.08, and 0.05 g/L. Then, P(VS)₁₇A₅₀ and PAAc₄₉ C_p were mixed to form the PIC vesicle. The pH value of the aqueous solution was adjusted to 10 and left for one day to obtain an equilibrium state. Subsequently, the PIC vesicle aqueous solutions were diluted by water at pH 10 to adjust the target C_p. The R_h and LSI for the PIC vesicle were plotted as a function of the C_p after mixing (Figure 5). The R_h values for the PIC vesicles at C_p = 0.1, 0.08, and 0.05 g/L before mixing were 86.6, 71.2, and 67.8 nm, respectively. This indicated that the size of the PIC vesicles increased with an increasing C_p before mixing since the aggregation number (N_agg) of the PIC vesicle depends on the C_p. When the C_p increases, the N_agg increases to increase the size of the PIC vesicle [42]. Furthermore, the increase in the N_agg was confirmed by of the increase in the LSI value from 1.55 to 3.25 Mcps at C_p = 0.05 and 0.1 g/L, respectively (Figure S4). When the PIC vesicle was diluted with water at pH 10, the R_h values remained nearly constant, independent of the C_p. These findings suggest that the size of the PIC vesicle can be controlled by adjusting the C_p before mixing, and after the PIC vesicleformation they were stable against dilution.

SLS measurements at 25 °C were used to determine further properties of the polymers and PIC vesicle, such as evident weight-average molecular weight (M_w(SLS)), and radius of gyration (R_g) (Figure S5). The RI increment (dn/dC_p) values for all samples were also separately estimated. N_agg is the number of polymer chains required to form a PIC vesicle. The PIC vesicle was prepared by mixing P(VS)₁₇A₅₀ and PAAc₄₉ at C_p = 0.1 g/L with f⁺ = 0.5 at pH 10 then the solution was diluted to 0.025 g/L by water at pH 10.

Table 2. Dynamic and static light scattering data for P(VS)₁₇A₅₀, PAAc₄₉, and the P(VS)₁₇A₅₀/PAAc₄₉ PIC vesicle.

Sample	Mw(SLS) × 10−4 (g/mol)	Nagg	Rg (nm)	Rh (nm)	Rg/Rh	dn/dCp	d1 (g/cm3)
P(VS)17A50	1.55	1	-	5.7	-	0.1323	0.033
PAAc49	0.33	1	-	5.3	-	0.2278	0.028
PIC vesicle	10,600	5640	101	86.6	1.17	0.0736	0.064

¹ Calculated from Equation (5).

indicates the value of M_w(SLS), N_agg, R_g, and R_h for all samples. The values of M_w(SLS) for P(VS)₁₇A₅₀ and PAAc₄₉ were 1.55 × 10⁴ g/mol and 0.33 × 10⁴ g/mol, respectively, which were close to the M_n(NMR) values estimated from the ¹H NMR measurements. P(VS)₁₇A₅₀ and PAAc₄₉ had M_n(NMR) values of 1.42 × 10⁴ and 0.35 × 10⁴ g/mol, respectively. The M_w(SLS) for the PIC vesicle was 1.06 × 10⁸ g/mol. The value of N_agg for the PIC vesicle was estimated by dividing the M_w(SLS) of the PIC vesicle by that of the unimers and was found to be 5640. The R_g/R_h value for the PIC vesicle was calculated as 1.17, indicating a spherical shape [3,43,44]. The following equation can be used to calculate the density (d) of the polymers and PIC vesicles:

$$d=\frac{M_w\left(\mathrm{SLS}\right)}{\frac{4}{3}{\pi \mathrm{N}}_{\mathrm{A}}{R}_{\mathrm{h}}^3}$$

(5)

The d values for P(VS)₁₇A₅₀, PAAc₄₉, and the PIC vesicle were calculated to be 0.033, 0.028, and 0.064 g/cm³, respectively. The d value for the PIC vesicle was larger than those for P(VS)₁₇A₅₀ and PAAc₄₉, suggesting that the polymer chains in the PIC vesicle are more densely packed than those of the unimers.

The pendant carboxylic groups in PAAc₄₉ are deprotonated under basic conditions. Therefore, the pH of the solution is an important factor in the PIC vesicle formation. To understand the effect of the pH value on the PIC vesicle, the R_h and LSI were measured as a function of the pH values. Initially, the PIC vesicle aqueous solution was prepared in water at C_p = 0.1 g/L with f⁺ = 0.5, then adjusted to the appropriate pH using NaOH and HCl aqueous solutions. The R_h, LSI, and zeta-potential values were plotted against the pH. By increasing pH from 3 to 5, the R_h of the PIC vesicle increased from 60.9 to 85.5 nm, then remained at ca. 86 nm above pH 5 (Figure 6a). The LSI value of the PIC vesicle showed the same tendency as that of the R_h. The acid dissociation constant (pK_a) of PAAc is about 4.5 [45,46,47]. At pH above 4.5 of the PAAc₄₉ aqueous solutions, the pendant carboxyl groups were deprotonated to generate anionic charges. The anionic PAAc₄₉ with pendant carboxylate anions can interact with the cationic PAPTAC block in P(VS)₁₇A₅₀ to form the PIC vesicle through electrostatic interactions. This was supported by the zeta-potential value of the PIC vesicle aqueous solutions. At pH < 5, the zeta-potential of the PIC vesicle showed a positive value which can be attributed to a charge of the cationic PAPTAC block in P(VS)₁₇A₅₀ with protonated PAAc₄₉ (Figure 6b). After increasing the pH value, at 5 ≤ pH the zeta-potential reached nearly 0 mV. It implied that the PIC vesicle formation was affected by the pH value, which means that the PIC vesicle can be formed above pH 5 and collapse below pH 5. The pH influence on the association behavior of the PIC vesicle is attributed to the pH-responsive property of PAAc₄₉. The conformation of PAAc in water was reported, and a reversible transition from the coil to the globule dependence of the pH was caused by deprotonation of the carboxylic group. At low pH, PAAc was a compact globular shape. When the media of the solution became baser, PAAc expanded into an open coil shape [47,48]. Furthermore, the R_h and LSI values for P(VS)₁₇A₅₀ were constant at ca. 6 nm and 70 kcps, respectively, at all pH values ranging from 3 to 10 (Figure S6), suggesting that P(VS)₁₇A₅₀ was not affected by pH. The small R_h and LSI values indicated that the polymer was in the unimer state. The zeta-potential values of P(VS)₁₇A₅₀ and PAAc₄₉ were measured as a function of pH (Figure S7). The zeta-potential for P(VS)₁₇A₅₀ stayed constant at ca. 17 mV, indicating that the polymer always gives a positive charge independent of the solution’s pH. However, the zeta-potential of PAAc₄₉ decreased from pH 3 to 5, then remained constant from pH 6. The pK_a for PAAc₄₉ was 4.5; therefore, from pH 5, the PAAc₄₉ deprotonated and indicated a negative charge.

The ¹H NMR spectra for the PIC vesicle suggested the A₅₀/PAAc₄₉ PIC membrane was covered with P(VS)₁₇ amphoteric random copolymer shells. P(VS)₁₇ showed the UCST behavior in aqueous solutions (Figure S8). Therefore, the PIC vesicle was expected to exhibit the UCST behavior owing to the P(VS)₁₇ shells. The percentage transmittance (%T) of the PIC vesicle was plotted against temperature upon the cooling process indicating the UCST behavior of the PIC vesicle. The temperature dependences investigated the effect of pH on the UCST behavior on %T at different pH conditions ranging from pH 3 to 10 (Figure 7). The PIC vesicle was disrupted below pH 5 owing to protonation of the pendant carboxyl groups in PAAc₄₉ (Figure 6). However, the aqueous solutions showed the UCST behavior excepted at pH 3. The phase transition temperature (T_p) of the PIC vesicle decreased from pH 4 to 6, then remained at 15 °C from pH 6. The UCST behavior of the PIC vesicle was affected by pH.

We have studied incorporating a hydrophilic noncharged guest molecule, PEG-Py, into the PIC vesicles. The hydrophilic drugs can be encapsulated inside the PIC vesicle thanks to the inner water phase. Herein, P(VS)₁₇A₅₀ and PAAc₄₉ solutions containing PEG-Py were mixed to form the PIC vesicle. The PEG-Py molecules which could not be incorporated into the PIC vesicle were removed by dialysis against pure water at pH 10. In comparison, a blank experiment was conducted, and the PEG-Py aqueous solution in the absence of the PIC vesicle was dialyzed with the same procedure. After dialysis for 20 days, fluorescence spectroscopy for PEG-Py in the presence and absence of the PIC aggregate was measured (Figure 8). The maximum emission wavelengths at 376 and 397 nm for PEG-Py were observed in the PIC vesicle solution, suggesting that the PIC vesicles can encapsulate PEG-Py. Hydrophobic pyrene molecules associate to produce excimer emission with a peak at 480 nm. PEG-Py can dissolve in water without interpolymer association in this study because no excimer emission was observed from PEG-Py fluorescence. In contrast, no signal of PEG-Py was detected from the reference solution in the absence of the PIC vesicle owing to the removal of the small PEG-Py molecules after dialysis membrane with a pore size of 10 nm. These findings suggested the PIC aggregate might be a vesicle structure because it can encapsulate hydrophilic PEG-Py. From the calibration curve of PEG-Py (Figure S9) and the fluorescence intensity, the weight of PEG-Py encapsulated into a PIC vesicle was estimated to be 0.0012 g. The LE and LC were calculated to be 12% and 1.2%, respectively, from Equations (1) and (2).

Using an HCl aqueous solution, the PIC vesicle encapsulating PEG-Py at pH 10 was adjusted to pH 3. A dialysis bag with a 10-nm pore size was used to dialyze the solution with an aqueous solution at pH 3. The solution sample inside the dialysis bag was taken out at varying times to measure the fluorescence intensities to calculate the release rate of the encapsulated PEG-Py from the PIC vesicle (Figure 9). After 24 h, the release amount of PEG-Py at pH 3 was 86.2%. Noncharged hydrophilic guest molecules can be encapsulated into the PIC vesicle at pH 10 and released at pH 3 owing to the PIC vesicle’s disruption. The release rate of the encapsulated guest molecule may be changed above and below the UCST of the P(VS)₁₇ shell.

4. Conclusions

P(VS)₁₇A₅₀, a cationic diblock copolymer, and an anionic homopolymer, PAAc₄₉, were successfully synthesized via a RAFT polymerization with a well-controlled structure. The pH- and thermo-responsive P(VS)₁₇A₅₀/PAAc₄₉ PIC vesicle was prepared by mixing P(VS)₁₇A₅₀ and PAAc₄₉ in basic aqueous solutions at room temperature due to electrostatic interactions. The R_h and LSI values of the PIC vesicle showed maximum values at f⁺ = 0.5, whereas the zeta-potential was near 0 mV. At low pH, the PIC vesicle disintegrated. The spherical shape with a vesicle structure was confirmed by TEM. The R_g/R_h ratio obtained from SLS and DLS measurements showed a value close to 1, indicating the spherical shape of the PIC vesicle. The thermo-responsive P(VS)₁₇ shells caused UCST behavior in the PIC vesicle. The thermo-responsive behavior of the PIC vesicle was affected by the pH of the solution. The PIC vesicle can encapsulate water-soluble nonionic guest molecules at a high pH and release them under acidic conditions, implying that it could be used as a DDS material. The interaction of the PIC vesicle with the cell can be controlled by temperature because the surface hydrophobicity increases with decreasing temperature. Therefore, it is expected that the PIC vesicle can be taken in the cell at a low temperature below the UCS of the P(VS)₁₇ shells. It is known that the pH around the cancer tissue is low. The encapsulated hydrophilic anticancer drugs can be released under acidic conditions from the P(VS)₁₇A₅₀/PAAc₄₉ PIC vesicle.