Takizawa Shin-ya, Breitenbach Thomas, Westberg Michael, Holmegaard Lotte, Gollmer Anita, Jensen Rasmus L, Murata Shigeru, Ogilby Peter R
Department of Basic Science, Graduate School of Arts and Sciences, The University of Tokyo, Meguro-ku, Tokyo, 153-8902, Japan.
Photochem Photobiol Sci. 2015 Oct;14(10):1831-43. doi: 10.1039/c5pp00230c.
A cationic cyclometallated Ir(III) complex with 1,10-phenanthroline and 2-phenylpyridine ligands photosensitizes the production of singlet oxygen, O2(a(1)Δ(g)), with yields that depend appreciably on the solvent. In water, the quantum yield of photosensitized O2(a(1)Δ(g)) production is small (ϕ(Δ) = 0.036 ± 0.008), whereas in less polar solvents, the quantum yield is much larger (ϕ(Δ) = 0.54 ± 0.05 in octan-1-ol). A solvent effect on ϕ(Δ) of this magnitude is rarely observed and, in this case, is attributed to charge-transfer-mediated processes of non-radiative excited state deactivation that are more pronounced in polar solvents and that kinetically compete with energy transfer to produce O2(a(1)Δ(g)). A key component of this non-radiative deactivation process, electronic-to-vibrational energy transfer, is also manifested in pronounced H2O/D2O isotope effects that indicate appreciable coupling between the Ir(III) complex and water. This Ir(III) complex is readily incorporated into HeLa cells and, upon irradiation, is cytotoxic as a consequence of the O2(a(1)Δ(g)) thus produced. The data reported herein point to a pervasive problem in mechanistic studies of photosensitized O2(a(1)Δ(g))-mediated cell death: care must be exercised when interpreting the effective cytotoxicity of O2(a(1)Δ(g)) photosensitizers whose photophysical properties depend strongly on the local environment. Specifically, the photophysics of the sensitizer in bulk solutions may not accurately reflect its intracellular behavior, and the control and quantification of the O2(a(1)Δ(g)) "dose" can be difficult in vivo.
一种含有1,10 - 菲咯啉和2 - 苯基吡啶配体的阳离子环金属化铱(III)配合物可光敏化单线态氧O₂(a¹Δg)的产生,其产率在很大程度上取决于溶剂。在水中,光敏化产生O₂(a¹Δg)的量子产率较小(ϕ(Δ)= 0.036 ± 0.008),而在极性较小的溶剂中,量子产率要大得多(在1 - 辛醇中ϕ(Δ)= 0.54 ± 0.05)。如此大的溶剂对ϕ(Δ)的影响很少被观察到,在这种情况下,这归因于电荷转移介导的非辐射激发态失活过程,该过程在极性溶剂中更为明显,并且在动力学上与能量转移竞争以产生O₂(a¹Δg)。这种非辐射失活过程的一个关键组成部分,即电子 - 振动能量转移,也表现为明显的H₂O/D₂O同位素效应,这表明铱(III)配合物与水之间存在明显的耦合。这种铱(III)配合物很容易被整合到HeLa细胞中,并且在照射后,由于产生的O₂(a¹Δg)而具有细胞毒性。本文报道的数据指出了光敏化O₂(a¹Δg)介导的细胞死亡机制研究中的一个普遍问题:在解释光物理性质强烈依赖于局部环境的O₂(a¹Δg)光敏剂的有效细胞毒性时必须谨慎。具体而言,主体溶液中敏化剂的光物理性质可能无法准确反映其细胞内行为,并且在体内很难控制和定量O₂(a¹Δg)的“剂量”。