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. 2022 Nov 17;27(22):7981.
doi: 10.3390/molecules27227981.

Tricyano-Methylene-Pyridine Based High-Performance Aggregation-Induced Emission Photosensitizer for Imaging and Photodynamic Therapy

Affiliations

Tricyano-Methylene-Pyridine Based High-Performance Aggregation-Induced Emission Photosensitizer for Imaging and Photodynamic Therapy

Xupeng Wu et al. Molecules. .

Abstract

Photosensitizers equipped with high reactive oxygen species (ROS) generation capability and bright emission are essential for accurate tumor imaging and precise photodynamic therapy (PDT). However, traditional aggregation-caused quenching (ACQ) photosensitizers cannot simultaneously produce desirable ROS and bright fluorescence, resulting in poor image-guided therapy effect. Herein, we report an aggregation-induced emission (AIE) photosensitizer TCM-Ph with a strong donor-π-acceptor (D-π-A) structure, which greatly separates the HOMO-LUMO distribution and reduces the ΔEST, thereby increasing the number of triplet excitons and producing more ROS. The AIE photosensitizer TCM-Ph has bright near-infrared emission, as well as a higher ROS generation capacity than the commercial photosensitizers Bengal Rose (RB) and Chlorine e6 (Ce6), and can effectively eliminate cancer cells under image guidance. Therefore, the AIE photosensitizer TCM-Ph has great potential to replace the commercial photosensitizers.

Keywords: ROS generation; aggregation-induced emission; bioimaging; photosensitizer.

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Conflict of interest statement

The authors declare no conflict of interest.

Figures

Figure 1
Figure 1
Design of the high-performance aggregation-induced emission photosensitizer TCM-Ph for imaging and photodynamic therapy. (A) Rational design of the AIE photosensitizer TCM-Ph; (B) TCM-Ph nanoparticles (TCM-Ph NPs) could image cancer cells and produce ROS upon light irradiation to kill cancer cells.
Figure 2
Figure 2
Photophysical properties of TCM-Et and TCM-Ph. (A) Absorption spectra of TCM-Et in 99% water; (B) Fluorescence spectra and (C) I/I0 plots of TCM-Et in THF/water mixtures with different water fractions (fw), λex = 511 nm. Inset: photographs of TCM-Et in 0% and 80% water under UV lamp (365 nm). I0 is the maximum fluorescence intensity of TCM-Et in THF. (D) Size distribution of TCM-Et in 99% water; (E) Absorption spectra of TCM-Ph in 99% water; (F) Fluorescence spectra and (G) I/I0 plots of TCM-Ph in THF/water mixtures with different fw, λex = 510 nm. Inset: photographs of TCM-Ph in 0% and 70% water under UV lamp (365 nm). I0 is the maximum fluorescence intensity of TCM-Ph in THF. (H) Size distribution of TCM-Ph in 99% water.
Figure 3
Figure 3
High ROS generation of TCM-Ph. (A) Light-induced total ROS generation of Ce6, RB, TCM-Et and TCM-Ph (10 μM) with DCFH (40 μM) as indicator. The plot of relative PL intensity (I-I0)/I0 at 525 nm versus the different irradiation times, where I0 is the fluorescence value of the mixture at 525 nm before illumination, and I is the fluorescence value of the mixture at 525 nm after illumination; excitation wavelength is 488 nm. (B) Light-induced 1O2 generation of Ce6, RB, TCM-Et and TCM-Ph (10 μM), evaluated by ABDA (50 μM). The relationship between A/A0 of ABDA at 378 nm versus the different irradiation times. (C) The relationship between ln(A0/A) and the light irradiation times, where A0 is the absorbance of ABDA at 378 nm before light irradiation, and A is the absorbance of ABDA at 378 nm after light irradiation. (D) Molecular orbital amplitude plots of HOMO and LUMO. (E) The energy levels of TCM-Et and TCM-Ph. The well vibration-resolved profiles allow accurate energy level abstractions based on the 0–0 peaks for solution samples in 2-methyl-tetrahydrofuran at 77 K.
Figure 4
Figure 4
Efficient cell penetrating and tumor cell ablation of TCM-Ph NPs. (A) Size distribution of TCM-Ph NPs in water. (B) Absorbance and fluorescence spectra of TCM-Ph NPs in water, λex = 497 nm. (C) Light-induced total ROS generation of Ce6, RB, and TCM-Ph NPs, evaluated by DCFH (40 μM). The plot of relative PL intensity (I-I0)/I0 at 525 nm versus the different irradiation times, where I0 is the fluorescence value of the mixture at 525 nm before illumination and I is the fluorescence value of the mixture at 525 nm after illumination, respectively, λex = 488 nm. (D) CLSM of HeLa cells incubated with TCM-Ph NPs (10 μM based on TCM-Ph) for different times. Red channel from TCM-Ph NPs: λex = 514 nm, λem = 550–700 nm. Scale bar: 25 μm. (E) Average fluorescence intensity of cells incubated with TCM-Ph NPs (10 μM based on TCM-Ph) for different times from Figure (D) (down). Data are shown as mean ± s.d., with n = 3, **** p < 0.0001. (F) Intracellular ROS level in HeLa cells under various treatments detected by reaction between DCFH and ROS. Green channel from DCFH: λex = 488 nm, λem = 505–560 nm. Scale bar: 50 μm. (G) In vitro cytotoxicity of different concentrations of TCM-Ph NPs under dark, 10 min and 20 min white-light irradiation. Light: 50 mW cm−2, > 400 nm. Data are shown as mean ± s.d., with n = 3, **** p < 0.0001, ** p < 0.01.

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