Poly[(9,9-dioctylfluorenyl-2,7-diyl)-alt-(benzo[2,1,3]thiadiazol-4,7-diyl)] (PFBT) and Roxadustat were self-assembled into liposomal nanoparticles (PFBT@Rox Lip)
via nanoprecipitation using cholesterol, lecithin and 1,2-distearoyl-sn-glycero-3-phosphoethanolamine-poly(ethylene glycol)-2000 as surfactants (
Fig. 1A). PFBT@Rox Lip nanoparticles had a uniform and transparent appearance in aqueous solutions. Transmission electron microscopy (TEM) analysis demonstrated that PFBT@Rox Lip nanoparticles were round in shape and ∼50 nm in diameter (
Fig. 1B). The hydrodynamic diameter of a PFBT@Rox Lip nanoparticle was 56 nm, as measured using dynamic light scattering (
Fig. 1C). PFBT@Rox Lip nanoparticles were dispersed in water, phosphate-buffered saline (PBS), and Dulbecco's modified Eagle medium. The stability examination of PFBT@Rox Lip nanoparticles suggested no obvious aggregation was observed in various aqueous solutions within 14 days, implying good stability for PFBT@Rox Lip nanoparticles (
Fig. 1D and Supporting Information Fig. S1). The encapsulation rates of Roxadustat and PFBT were calculated to be 70 % and 95 % respectively from established standard curves by measuring absorbance values. The loading rates of Roxadustat and PFBT were determined to be 15% and 64% respectively (Supporting Information Fig. S2). We also investigated the Roxadustat release
in vitro from PFBT@Rox Lip nanoparticles. The results showed that abundant PFBT and Roxadustat were released from PFBT@Rox Lip upon incubating PFBT@Rox Lip in PBS containing H
2O
2 (pH 7.4) (Supporting Information Fig. S3). A slower release of drug behavior was observed at the condition without irradiation, suggesting 39% and 19.8% of PFBT and Roxadustat release after 24 h incubation, respectively. However, upon light irradiation for 1h, a marked increase in the release of PFBT and Roxadustat was detected with a cumulative drug release of 98% and 48.8% for PFBT and Roxadustat, respectively after 24 h (Fig. S3). Next, the zeta potential of PFBT@Rox Lip nanoparticles was determined to be −12.3 mV, which is conducive to maintaining nanoparticle stability in the bloodstream (
Fig. 1E). In addition, the ultraviolet–visible–near infrared absorption and emission spectra were analyzed and showed that PFBT@Rox Lip nanoparticles had an absorption peak at ∼470 nm and an emission peak at ∼540 nm (
Fig. 1F). To gain a deeper understanding of the excitation properties of PFBT-conjugated polymers, we performed theoretical calculations to reveal the process of
in situ self-assembling coating and photophysical properties of the obtained nanoparticles. As shown in
Fig. 1G and H, the density functional theory calculations demonstrated that the PFBT ΔE
S1-T1 value was 0.26 eV. Such a low ΔE
S1-T1 value is beneficial for the energy transfer from S
1 to T
1 and generates a sensitized T
1 state, and it enables the energy transfer to the adjacent O
2 for
1O
2 generation efficiency. In addition, the energy gap between the highest occupied molecular orbital and the lowest unoccupied molecular orbital (HOMO–LUMO) for the PFBT-conjugated polymer was calculated to be 3.2 eV. Full separation of the HOMO and LUMO is beneficial for the
in situ self-assembling coating and promotes the generation of type II ROS. Because the PFBT-conjugated polymer possesses a
π‒electronic backbone structure, the excited PFBT∗ further transfers electrons to the surrounding O
2 or H
2O to produce superoxide radicals (O
2·
−) and hydroxyl radicals (·OH) (Supporting Information Fig. S4). In addition, PFBT energy levels measured using an ultraviolet photoelectron spectrometer showed an energy tendency similar to the calculated one for the conjugated polymer (
Fig. 1G). Total ROS production by PFBT@Rox Lip nanoparticles was determined using the ROS probe 2,7-dichlorofluorescein diacetate (DCFH-DA). In the presence of ROS, DCFH-DA is oxidized to 2,7-dichlorofluorescin (DCF), which emits bright fluorescence at 525 nm. As shown in
Fig. 1I, upon white light irradiation with a direct current for 6 min, the fluorescence intensity of DCF increased over time. However, there was no significant change in the fluorescence of DCFH without PFBT@Rox Lip nanoparticles, indicating that the latter sensitized the surrounding oxygen or water molecules to produce ROS. The identities of ROS (
1O
2, ·OH and O
2·
−) were experimentally evaluated using electron paramagnetic resonance. Established methods typically use 2,2,6,6-tetramethylpiperidine (TEMP) as a probe for
1O
2, and 5,5-dimethyl-1-pyrroline-
N-oxide (DMPO) as a spin-trap to detect O
2·
− and ·OH. The hyperfine splitting constants (aN, aH) and g factor for the spin adducts were used to examine the presence of each ROS. As shown in
Fig. 1J, triplet peaks corresponding to typical TEMPO signals were observed for white light irradiation (aN = 16.5 G,
g = 2.0058), suggesting the appearance of
1O
2, in sharp contrast to the silent spectra for the untreated sample. The signals of the DMPO/O
2− adduct were also observed under the experimental conditions (
Fig. 1K). In addition, as shown in
Fig. 1L, OH formation was also evidenced by the electron paramagnetic resonance signals of the DMPO/·OH adduct (aN = aH = 14.8 G,
g = 2.0031). Additionally, the frequently used photosensitizer Hematoporphyrin monomethyl ether (HMME), was also employed as a control to compare its capability of ROS generation with that of PFBT. We found that PFBT showed a more efficient capability of ROS generation when compared with HMME, indicating that PFBT is an excellent photosensitizer. (Supporting Information Fig. S5). Together, these results indicated that PFBT@Rox Lip nanoparticles showed excellent Type I and Type II ROS generation capacities.