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紫色细菌非均匀展宽核心天线中的能量转移:低强度皮秒吸收和荧光动力学的同时拟合

Energy transfer in the inhomogeneously broadened core antenna of purple bacteria: a simultaneous fit of low-intensity picosecond absorption and fluorescence kinetics.

作者信息

Pullerits T, Visscher K J, Hess S, Sundström V, Freiberg A, Timpmann K, van Grondelle R

机构信息

Department of Physical Chemistry, University of Umeå, Sweden.

出版信息

Biophys J. 1994 Jan;66(1):236-48. doi: 10.1016/S0006-3495(94)80770-2.

Abstract

The excited state decay kinetics of chromatophores of the purple photosynthetic bacterium Rhodospirillum rubrum have been recorded at 77 K using picosecond absorption difference spectroscopy under strict annihilation free conditions. The kinetics are shown to be strongly detection wavelength dependent. A simultaneous kinetic modeling of these experiments together with earlier fluorescence kinetics by numerical integration of the appropriate master equation is performed. This model, which accounts for the spectral inhomogeneity of the core light-harvesting antenna of photosynthetic purple bacteria, reveals three qualitatively distinct stages of excitation transfer with different time scales. At first a fast transfer to a local energy minimum takes place (approximately 1 ps). This is followed by a much slower transfer between different energy minima (10-30 ps). The third component corresponds to the excitation transfer to the reaction center, which depends on its state (60 and 200 ps for open and closed, respectively) and seems also to be the bottleneck in the overall trapping time. An acceptable correspondence between theoretical and experimental decay kinetics is achieved at 77 K and at room temperature by assuming that the width of the inhomogeneous broadening is 10-15 nm and the mean residence time of the excitation in the antenna lattice site is 2-3 ps.

摘要

利用皮秒吸收差光谱法,在严格无湮灭条件下,于77K记录了红色光合细菌红螺菌的色素小体的激发态衰减动力学。结果表明,动力学强烈依赖于检测波长。通过对适当的主方程进行数值积分,对这些实验以及早期的荧光动力学进行了同步动力学建模。该模型考虑了光合紫色细菌核心光捕获天线的光谱不均匀性,揭示了激发转移的三个定性不同阶段,具有不同的时间尺度。首先,快速转移到局部能量最小值(约1皮秒)。随后是在不同能量最小值之间的慢得多的转移(10 - 30皮秒)。第三个成分对应于激发转移到反应中心,这取决于其状态(开放和关闭状态分别为60和200皮秒),并且似乎也是整体捕获时间的瓶颈。通过假设非均匀展宽的宽度为10 - 15纳米,激发在天线晶格位点的平均停留时间为2 - 3皮秒,在77K和室温下实现了理论和实验衰减动力学之间的可接受对应关系。

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