【JACS】山西医科大学张瑞平|单线态氧提升27.8倍!HLCT近红外二区光敏剂实现12天肿瘤滞留与99.01%抑瘤率
【JACS】山西医科大学张瑞平|单线态氧提升27.8倍!HLCT近红外二区光敏剂实现12天肿瘤滞留与99.01%抑瘤率
文章标题:Molecular Engineering of Asymmetric Cyanines with Hybridized Local and Charge-Transfer Characteristics for NIR-II Imaging-Guided Type I/II Photodynamic Therapy
文章作者:Ruixue Yang, Yating Wen, Tingran Wang, Runyu Gao, Huixia Xu, Runfeng Chen, Hua Wang, Liping Li, Ruiping Zhang
文章概要
山西医科大学张瑞平教授团队通过分子工程策略设计并合成了一类具有非对称D-π-A-D’结构的杂化局部与电荷转移(HLCT)特性的近红外二区(NIR-II)花菁染料。该类光敏剂有效克服了传统花菁类分子系间跨越效率低、缺氧微环境不敏感以及肿瘤滞留时间短等瓶颈,实现了高度协同的Ⅰ型与Ⅱ型光动力治疗(PDT) 以及高对比度近红外二区荧光成像。其中代表性分子CyTY-3制备成纳米颗粒后,单线态氧产生效率达到临床常用吲哚氰绿(ICG)的27.8倍,近红外二区荧光量子产率高达11.4%,并在无外源靶向配体的情况下实现了长达12天的肿瘤靶向滞留,在体内光动力治疗中达到了99.01%的肿瘤抑制率,为高效精准诊疗缺氧肿瘤提供了全新的分子设计思路。

引言
癌症是严重威胁人类健康的重大疾病,开发兼具高时空分辨率和低侵入性的诊疗一体化策略具有重要科学意义。以吲哚氰绿(ICG)为代表的近红外花菁染料因吸收系数高和生物相容性好而广受关注,然而传统花菁分子由于第一单线态到第一三线态的系间跨越速率较慢,导致活性氧生成效率低下。虽然通过重原子效应或引入强吸电子基团能够增强Ⅱ型光动力过程,但这些方法难以产生超氧阴离子自由基与羟基自由基,在缺氧肿瘤微环境中疗效受到严重制约。热激活延迟荧光型光敏剂虽然可以促进Ⅰ型光动力途径,但过窄的能级差极易引发三线态-三线态湮灭效应并导致荧光猝灭。针对上述多重矛盾,设计一种能够平衡近红外二区高荧光量子产率、多途径活性氧生成以及肿瘤高效蓄积的新型分子体系,成为光医学领域迫切需要解决的核心难题。

(a) Schematic Illustration of the Photophysical and Photodynamic Mechanisms of Different Photosensitizers (PSs); (b) Molecular Structures and Photophysical/Photodynamic Properties of the HLCT-Type Cyanine Dyes (CyTY-1, CyTY-2, CyTY-3); (c) The Unique Charge-Separated Structure of CyTY-3 and Its Long-Term Tumor Retention Performance In Vivo
主要实验及结论
研究团队提出了利用杂化局部与电荷转移(HLCT)态调控三重态激子动力学的分子设计新策略。如图1所示,团队以四甲基吲哚盐为主要给体,二氧硼杂环为受体,三苯胺为辅助给体,通过延长共轭链长度精准合成了CyTY-1、CyTY-2和CyTY-3三种非对称花菁分子。吸收与发射光谱表明,共轭链的延伸使最大发射波长显著红移至856 nm,且尾部延伸至近红外二区,其中CyTY-3展现出高达2.53 × 10⁵ M⁻¹cm⁻¹的摩尔消光系数与140 nm的大斯托克斯位移。飞秒瞬态吸收光谱与时间分辨光谱进一步证实,CyTY-3在光激发后呈现出快速的局部激发态向电荷转移态的弛豫过程,并在连续激光照射10分钟后保持84.2%的吸光度,稳定性显著优于ICG。

Fig.1 Evaluation of the synthesis and photophysical properties of three CyTY dyes: (a) Chemical structures; (b) UV–vis absorption spectra in dimethyl sulfoxide (DMSO); (c) PL spectra in DMSO; (d) transient PL decay spectra; (e) linear fitting of the Lippert–Mataga model; (f) transient absorption (TA) spectra and corresponding kinetic decay curves of CyTY-3 in DCM.
为了深入探索分子的激发态演化机制,研究团队进行了理论计算与光谱验证。如图2所示,时间依赖密度泛函理论计算揭示了分子最高占据分子轨道与最低未占分子轨道的空间有效分离,证实了典型的HLCT特征。能级图分析显示,CyTY-3具有极小的S₁-T₂能级差(0.08 eV)和较大的T₂-T₁能级差(0.76 eV),大幅提升了单线态到高阶三重态的系间跨越速率(3.8 × 10⁷ s⁻¹)。在此基础上,局部激发态特性保障了高荧光发光效率并抑制了三线态湮灭,而电荷转移态特性则驱动了电子转移过程,从而同时激活了产生单线态氧的Ⅱ型途径以及产生超氧阴离子和羟基自由基的Ⅰ型途径。

Fig.2 (a) Frontier molecular orbitals from TDDFT calculations of CyTY in the ground state. (b) Singlet–triplet energy-level diagrams and spin–orbit coupling matrix element (SOCMe) values of CyTY and ICG. (c) Photoinduced ROS generation and photosensitization mechanism of CyTY-3.
活性氧检测实验全面验证了分子的光动力性能。如图3所示,利用DPBF、DHR123和HPF等探针评估发现,CyTY-2和CyTY-3的单线态氧生成能力显著优于对照组。电子自旋共振光谱配合猝灭剂实验明确捕获到了单线态氧、超氧阴离子和羟基自由基的特征信号,证实了CyTY-3具备出色的Ⅰ/Ⅱ型协同光动力活性。如图4所示,光热性能与能量跃迁测试表明,CyTY-3较大的构象柔性促进了非辐射跃迁,使其兼具19.0%的光热转换效率。

Fig.3 (a) Kinetic curve of 1O2 generation derived from the decomposition rate of DPBF. (b) Graph of relative fluorescence intensity (I/_I_0) of DHR123 solution containing CyTY dyes as a function of irradiation time. (c) Graph of relative fluorescence intensity (I/_I_0) of HPF solution containing CyTY dyes as a function of irradiation time. (d) Fluorescence kinetic curves of DCFH for verifying the total ROS production of CyTY-3, together with the control groups pretreated with FFA (1O2) and TBA + SOD (O2–• and •OH). (e) EPR spectra of TEMP and DMPO spin-trapping adducts, confirming the production of 1O2, O2–•, and •OH upon white light irradiation for 5 min in the presence of 5 μM CyTY-3. (f) Photostability comparison of CyTY-3 and commercial ICG monitored by the absorbance retention ratio (A/_A_0) within 10 min of continuous light irradiation.

Fig.4 (a) Temperature elevation profiles of CyTY-2 and (b) CyTY-3 aqueous solutions with different concentrations under 808 nm laser irradiation (1.5 W·cm–2, 600 s). (c) Photothermal stability tests of CyTY-2, CyTY-3, and ICG over three heating–cooling cycles. (d) Decomposition of reorganization energy into contributions from bond angles, dihedral angles, and bond lengths for CyTY-2 and (e) CyTY-3. (f) RMSD comparison between the optimized ground- and excited-state conformations of CyTY-2 and CyTY-3.
在细胞与动物水平的生物学效应评价中,HLCT光敏剂展现出了突出的诊疗潜能。如图5所示,激光共聚焦显微镜观察到CyTY-3能在60分钟内被4T1乳腺癌细胞高效摄取。在常氧及1%氧气的缺氧条件下,结合808 nm激光照射,CyTY-3处理组的细胞存活率均显著下降至18%左右,证实其克服缺氧微环境的能力。如图6所示,将CyTY-3封装为纳米颗粒后,其平均粒径约为60 nm。借助于电荷分布带来的自靶向效应以及高局部正电荷与肿瘤细胞膜负电荷的静电作用,CyTY-3纳米颗粒在小鼠肿瘤部位的积累荧光强度达到ICG的15倍,且肿瘤滞留时间长达12天。如图7所示,在体内抑瘤实验中,经808 nm激光照射治疗14天后,CyTY-3纳米颗粒组的肿瘤完全消退,抑瘤率达到99.01%,且小鼠血生化指标与主要器官组织切片均未见明显毒副作用,表现出极佳的体内生物安全性。

Fig.5 (a) Fluorescence staining images of incubated 4T1 cells with CyTY dyes (λex: 580/640/640 nm, λem: 650–900 nm, scale bars: 50 μm). (b) ROS generation image of CyTY-3 dye after light irradiation (scale bars: 100 μm). (c) Survival rate of 4T1 cells treated with various concentrations of CyTY dyes under normoxia, hypoxia, light-irradiated, and nonirradiated conditions. Data are representative of n = 5 independent experiments. (d) Live/Dead cell costaining images of CyTY-3 treated groups under normoxic and hypoxic conditions with Calcein-AM and Propidium Iodide (PI) as markers (scale bars: 100 μm). (e) DHE and HPF staining images of ROS for CyTY dyes under hypoxic conditions (scale bars: 50 μm).

Fig.6 (a) Schematic illustration of the preparation process of CyTY-3 NPs. (b) Particle size distribution of CyTY-3 NPs detected by DLS (inset: typical TEM images of CyTY-3 NPs. Scale bars: 100 nm). (c) NIR-II emission spectrum and NIR-II fluorescence images of CyTY-3 NPs. (d) NIR-II fluorescence images of heart, liver, spleen, lung, kidney, and tumor tissues from tumor-bearing mice at 72 h postintravenous injection of CyTY-3 NPs (after dissection). (e) Comparison of NIR-II fluorescence imaging between ICG and CyTY-3 NPs. The illustration includes: After intravenous injection of ICG and CyTY-3 NPs into tumor-bearing mice, respectively, tumor photographs and NIR-II fluorescence images were acquired at different time points (excitation wavelength λex = 808 nm, long-pass filter 880 nm, exposure time 100 ms). (f) Comparison of intratumoral fluorescence intensity between ICG NPs and CyTY-3 NPs. (g) CyTY-3 NPs zeta potential plot and surface electrostatic potential distribution of CyTY-3 and ICG within different electrostatic potential intervals.

Fig.7 (a) Schematic diagram of the photodynamic antitumor therapy process. (b) Images of mice and tumors with different treatments 14 days post-treatment. (c) Relative tumor volume of mice after treatments. (d) Body weights of the mice after different treatments. (e) Photographs of tumors dissected from 4T1 tumor-bearing mice after 14 days of treatment. (f) H&E-stained tumor sections from different treatment groups. Scale bar = 100 μm. (g) Liver function indicators: detection levels of Alanine Aminotransferase (ALT). (h) Liver function indicators: detection levels of Aspartate Aminotransferase (AST). (i) Renal function indicators: detection levels of Creatinine (CREA). The results are representative of n = 3 independent experiments.
总结及展望
本研究成功构筑了首例基于HLCT特性的非对称近红外二区花菁光敏剂,通过精确调控高阶三重态能级与激子跃迁动力学,一举打破了传统花菁分子在荧光亮度和光动力活性之间的博弈。CyTY-3纳米颗粒兼具出色的近红外二区荧光成像能力、高效的Ⅰ/Ⅱ型协同光动力疗效以及长效的电荷介导肿瘤蓄积特性,显著改善了缺氧肿瘤的诊疗瓶颈。这一分子工程策略不仅为下一代高性能近红外光诊疗剂的开发提供了普适性的理论指导,也为推动缺氧肿瘤精准光化学治疗的临床转化奠定了坚实的科学基础。
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