| Literature DB >> 35127391 |
Lei Fang1,2, Zitong Zhao2, Jue Wang2, Ping Xiao2, Xiangshi Sun2, Yaping Ding1, Pengcheng Zhang2,3, Dangge Wang2,4,3, Yaping Li2,4,3.
Abstract
Nucleic acid drugs are highly applicable for cancer immunotherapy with promising therapeutic effects, while targeting delivery of these drugs to disease lesions remains challenging. Cationic polymeric nanoparticles have paved the way for efficient delivery of nucleic acid drugs, and achieved stimuli-responsive disassembly in tumor microenvironment (TME). However, TME is highly heterogeneous between individuals, and most nanocarriers lack active-control over the release of loaded nucleic acid drugs, which will definitely reduce the therapeutic efficacy. Herein, we have developed a light-controllable charge-reversal nanoparticle (LCCN) with controlled release of polyinosinic-polycytidylic acid [Poly(I:C)] to treat triple negative breast cancer (TNBC) by enhanced photodynamic immunotherapy. The nanoparticles keep suitably positive charge for stable loading of Poly(I:C), while rapidly reverse to negative charge after near-infrared light irradiation to release Poly(I:C). LCCN-Poly(I:C) nanoparticles trigger effective phototoxicity and immunogenic cell death on 4T1 tumor cells, elevate antitumor immune responses and inhibit the growth of primary and abscopal 4T1 tumors in mice. The approach provides a promising strategy for controlled release of various nucleic acid-based immune modulators, which may enhance the efficacy of photodynamic immunotherapy against TNBC.Entities:
Keywords: Cancer immunotherapy; Charge-reversal; Nanoparticles; Photodynamic therapy; Polyinosinic-polycytidylic acid; ROS-responsive; Triple negative breast cancer; Tumor microenvironment
Year: 2021 PMID: 35127391 PMCID: PMC8800000 DOI: 10.1016/j.apsb.2021.06.006
Source DB: PubMed Journal: Acta Pharm Sin B ISSN: 2211-3835 Impact factor: 11.413
Scheme 1Schematic illustration of the LCCN and its mechanisms for enhanced photodynamic immunotherapy against TNBC. (A) Design of LCCN-Poly(I:C). Briefly, FK-PBA, PVA and PEI-Ce6 are self-assembled into nanoparticles and then load Poly(I:C) via electrostatic interactions. The release of Poly(I:C) is actively controlled by NIR light via a charge-reversal process. LCCN-triggered ROS promote the cleavage of phenylboronic ester between PBA and PVA, and then lead to the variation of surface charge. The nanoparticles are totally disassembled in reduction microenvironment owing to the break of disulfide bond in FK-PBA. (B) The nanoparticles distribute into tumors after intravenous injection. Poly(I:C) is released from the nanoparticles once irradiated by 655 nm NIR light. When combined with PDT-induced ICD, the nanoparticles efficiently prime antitumor immune responses and inhibit the growth of 4T1 tumors in mice.
Figure 1Preparation and characterization of LCCN and LCCN-Poly(I:C). (A) Diameter and PDI of LCCN as a fucntion of FK-PBA to diols in PVA mole ratio. (B) Diameter and PDI of LCCN when fabricated by using 47, 67 and 125 kDa of PVA. (C) TEM images of LCCN fabricated by using 47, 67 and 125 kDa of PVA. Scale bar = 500 nm. (D) TEM images of LCCN with NIR light irradiation (left) and GSH (right) treated. Scale bar = 500 nm. (E) DLS examination of LCCN with NIR light irradiation (left) and GSH (right) treated. (F) ζ-potential variation of LCCN-Poly(I:C) at different Poly(I:C) to LCCN weight ratios. (G) ζ-potential variation of LCCN-Poly(I:C) nanoparticles after NIR light irradiation at a power density of 300 mW/cm2 for 5 min. (H) Agarose gel electrophoresis of LCCN-Poly(I:C) without NIR light treatment. (I) Agarose gel electrophoresis of LCCN-Poly(I:C) post NIR light treatment. Data are presented as mean ± SD (n = 3).
Figure 2LCCN-induced PDT and ICD in vitro. (A) Intracellular uptake of LCCN after incubated with 4T1 tumor cells for 0.5, 1, 2, 4 and 6 h, respectively. (B) NIR light (655 nm) power density-dependent phototoxicity of LCCN on 4T1 tumor cells. (C) LCCN-triggered ROS prodution in 4T1 cells by using ROS probe DCFH-DA. Scale bar = 20 μm. (D) Analysis of PDT-induced apoptosis/necrosis in 4T1 tumor cells by Annexin V-FITC/PI apoptosis detection kit. (E) CRT exposure induced by LCCN-based PDT. Scale bar = 20 μm. (F) Leakage of HMGB1 from cell nucleus induced by LCCN-based PDT. Scale bar = 20 μm. (G) Extracellular secretion of ATP induced by LCCN-induced PDT at 0.25 or 2.0 μg/mL of Ce6. (H) 4T1 cells were treated with LCCN and NIR light to induce ICD. Percentage of CD11c+CD80+ BMDCs and (I) CD11c+CD86+ BMDCs was examined by flow cytometry. Data are presented as mean ± SD (n = 3). ∗P < 0.05, ∗∗P < 0.01.
Figure 3LCCN-Poly(I:C) effectively distributed into tumors and induced antitumor immunity in 4T1 tumor model. (A) Fluorescent imaging of LCCN and LCCN-Poly(I:C) intravenously treated mice at equal 1.0 mg/kg of Ce6. (B) Biodistribution of LCCN and LCCN-Poly(I:C) ex vivo at 12 h and (C) 24 h. (D) CLSM images of FAM-NC distribution in tumor sections 4 h post-injection. Scale bar = 50 μm. (E) Frequency of CD11c+CD80+CD86+ DCs in tumors. (F) Frequency of CD3+CD4+, CD3+CD8+ T cells in lymphocytes harvested from tumors in control and treated groups. (G) Frequency of Tregs in tumors with different treatments. Data are presented as mean ± SD (n = 3).
Figure 4Growth inhibition of primary and abscopal 4T1 tumors by LCCN-Poly(I:C). (A) Average growth kinetics of primary tumors after treatments (n = 6). (B) Individual growth kinetics of tumors in mice. (C) Body weight (n = 6). (D) Survival percentage in control and treated groups (n = 6). (E) Abscopal tumor free percentage of mice with various treatments (n = 5). (F) H&E assessment of primary tumors. Scale bar = 200 μm. (G) TUNEL staining of primary tumor sections. Scale bar = 100 μm. (H) Fluorescent staining of CD8+ T cells in tumor slice. Scale bar = 100 μm. (I) Histochemistry staining of IFN-γ+ cells in tumor slice. Scale bar = 100 μm. Data are presented as mean ± SD. ∗P < 0.05, ∗∗P < 0.01, ∗∗∗P < 0.001.