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ABSTRACT Objective Methods Results Conclusion The lipid‐lowering simvastatin (SIM) has been shown to be an effective inhibitor of keloid proliferation. However, due to its low water solubility and short half‐life, simvastatin aggregates to the liver and does not reach the skin lesions after oral administration, which restricts its widespread clinical use. The development of nanomedicine provides the possibility for us to break through this bottleneck problem clinically. The objective of this study was to investigate the feasibility of using complex nanocontrolled delivery system (CNDS), simvastatin‐loaded polyethylene glycol‐poly lactic‐co‐glycolic acid (PEG‐PLGA), in the treatment of keloids.In the in vitro study, the release of simvastatin in fibroblasts by CNDS@Simvastatin and its effect on inhibition of the proliferation of fibroblasts, Col Ι, and CTGF by the slow release of simvastatin were assessed. The efficacy of CNDS@Simvastatin in improving keloids and the biocompatibility and safety of CNDS@Simvastatin were examined in vivo by establishing a murine ear keloid model.CNDS@Simvastatin showed sustained and uniform inhibition of the proliferation of fibroblasts, Col Ι, and CTGF via the gradual release of simvastatin over 72 h. It was efficient in the treatment of the murine ear keloid with no observable toxic side effects on various organs.Simvastatin‐loaded copolymer acid‐sensitive nanocarriers, CNDS@Simvastatin nanospheres, were successfully developed in this study, and these were characterized by favorable physicochemical properties and biocompatibility. [ABSTRACT FROM AUTHOR]

Defect engineering is of great interest to the two-dimensional (2D) materials community. If nonmagnetic transition-metal dichalcogenides can possess room-temperature ferromagnetism (RTFM) induced by defects, then they will be ideal for application as spintronic materials and also for studying the relation between electronic and magnetic properties of quantum-confined structures. Thus, in this work, we aimed to study gamma-ray irradiation effects on MoS 2 , which is diamagnetic in nature. We found that gamma-ray exposure up to 9 kGy on few-layered (3.5 nm) MoS 2 films induces an ultrahigh saturation magnetization of around 610 emu/cm 3 at RT, whereas no significant changes were observed in the structure and magnetism of bulk MoS 2 (40 nm) films even after gamma-ray irradiation. The RTFM in a few-layered gamma-ray irradiated sample is most likely due to the bound magnetic polaron created by the spin interaction of Mo 4d ions with trapped electrons present at sulfur vacancies. In addition, density functional theory (DFT) calculations suggest that the defect containing one Mo and two S vacancies is the dominant defect inducing the RTFM in MoS 2 . These DFT results are consistent with Raman, X-ray photoelectron spectroscopy, and ESR spectroscopy results, and they confirm the breakage of Mo and S bonds and the existence of vacancies after gamma-ray irradiation. Overall, this study suggests that the occurrence of magnetism in gamma-ray irradiated MoS 2 few-layered films could be attributed to the synergistic effects of magnetic moments arising from the existence of both Mo and S vacancies as well as lattice distortion of the MoS 2 structure.