首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Spectral Distributions of 'Trap' Pigments in the RC, CP47, and CP47-RC Complexes of PhotosystemⅡat Low Temperature: A Fluorescence Line-Narrowing and Hole-Burning Study
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Spectral Distributions of 'Trap' Pigments in the RC, CP47, and CP47-RC Complexes of PhotosystemⅡat Low Temperature: A Fluorescence Line-Narrowing and Hole-Burning Study

机译:低温下光系统ⅡRC,CP47和CP47-RC配合物中“诱捕”颜料的光谱分布:荧光变窄和烧孔研究

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摘要

Broad-band absorption and fluorescence, fluorescence line-narrowing (FLN), and spectral hole-burning experiments have been performed on the Q↓(y)-band of three subcore reaction-center complexes of photosystem II between 1.2 and 4.2 K: the isolated reaction center (RC), the inner core antenna CP47, and the CP47-RC complex. In the RC, fluorescence line-narrowing (FLN) is observed for excitation wavelengths λ↓(exc) ≥ 676 nm, whereas in CP47, this occurs for λ↓(exc)≥680 nm. The FLN spectra of CP47-RC appear to be the sum of the individual spectra of the RC and CP47, an indication that this complex has two "traps". This has been confirmed from the spectral distributions obtained by measuring the hole depth (at constant hole width) as a function of λ↓(exc) previously done for the RC [Groot, M. L., et al. J. Phys. Chem. 100, 1996, 11488]. The maxima of these distributions are at ~682 nm for the RC "trap" and at ~690 nm for the CP47 "trap" within the CP47-RC complex. Further support that the two distributions of pigments in CP47-RC belong indeed to "trap" pigments is provided by the "effective" homogeneous line width Γ'↓(hom)determined as a function of temperature for various excitation and detection wavelengths.
机译:已经在1.2和4.2 K之间的光系统II的三个子核心反应中心复合物的Q↓(y)带上进行了宽带吸收和荧光,荧光线变窄(FLN)和光谱烧孔实验:隔离反应中心(RC),内芯天线CP47和CP47-RC复合体。在RC中,对于激发波长λ↓(exc)≥676 nm,观察到荧光线变窄(FLN),而在CP47中,对于λ↓(exc)≥680nm发生荧光变窄。 CP47-RC的FLN谱图似乎是RC和CP47的各个谱图的总和,表明该络合物具有两个“陷阱”。从通过测量孔深度(在恒定孔宽度下)得到的光谱分布可以证实这一点,该光谱深度是先前对RC所做的λ↓(exc)的函数[Groot,M. L.,et al。 J.物理化学100,1996,11488]。对于CP“陷阱”,这些分布的最大值在〜682 nm处,对于CP47-RC复合物中的CP47“陷阱”,在〜690 nm处。 CP47-RC中颜料的两种分布确实属于“捕获”颜料的进一步支持是由“有效”均匀线宽Γ'↓(hom)决定的,该线宽是各种激发和检测波长的温度函数。

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