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能量如何在隐藻红藻CS24细胞中从藻红蛋白天线复合体传递到光系统I和光系统II。

How energy funnels from the phycoerythrin antenna complex to photosystem I and photosystem II in cryptophyte Rhodomonas CS24 cells.

作者信息

van der Weij-De Wit Chantal D, Doust Alexander B, van Stokkum Ivo H M, Dekker Jan P, Wilk Krystyna E, Curmi Paul M G, Scholes Gregory D, van Grondelle Rienk

机构信息

Department of Physics and Astronomy, Faculty of Sciences, Vrije Universiteit, De Boelelaan 1081, 1081 HV Amsterdam, The Netherlands.

出版信息

J Phys Chem B. 2006 Dec 14;110(49):25066-73. doi: 10.1021/jp061546w.

Abstract

We report an investigation of energy migration dynamics in intact cells of the photosynthetic cryptophyte Rhodomonas CS24 using analyses of steady-state and time-resolved fluorescence anisotropy measurements. By fitting a specific model to the fluorescence data, we obtain three time scales (17, 58, and 113 ps) by which the energy is transferred from phycoerythrin 545 (PE545) to the membrane-associated chlorophylls (Chls). We propose that these time scales reflect both an angular distribution of PE545 around the photosystems and the relative orientations of the donor dihydrobiliverdin (DBV) bilin and the acceptor Chl. Contrary to investigations of the isolated antenna complex, it is demonstrated that energy transfer from PE545 does not occur from a single-emitting bilin, but rather both the peripheral dihydrobiliverdin (DBV) chromophores in PE545 appear to be viable donors of excitation energy to the membrane-bound proteins. The model shows an almost equal distribution of excitation energy from PE545 to both photosystem I (PSI) and photosystem II (PSII), whose trap times correspond well to those obtained from experiments on isolated photosystems.

摘要

我们报告了一项利用稳态和时间分辨荧光各向异性测量分析,对光合隐藻红胞藻CS24完整细胞中能量迁移动力学进行的研究。通过将一个特定模型拟合到荧光数据,我们获得了三个时间尺度(17、58和113皮秒),能量通过这些时间尺度从藻红蛋白545(PE545)转移到与膜相关的叶绿素(Chls)。我们提出,这些时间尺度既反映了PE545在光系统周围的角分布,也反映了供体二氢胆绿素(DBV)胆素和受体叶绿素的相对取向。与对分离的天线复合体的研究相反,结果表明,来自PE545的能量转移并非来自单个发射胆素,而是PE545中的两个外周二氢胆绿素(DBV)发色团似乎都是向膜结合蛋白传递激发能的可行供体。该模型显示,从PE545到光系统I(PSI)和光系统II(PSII)的激发能分布几乎相等,其捕获时间与从分离光系统的实验中获得的时间相当吻合。

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