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低氧化还原电位下紫色细菌的细菌叶绿素荧光。反应中心三线态产率与发射产率之间的关系。

Bacteriochlorophyll fluorescence of purple bacteria at low redox potentials. The relationship between reaction center triplet yield and the emission yield.

作者信息

van Grondelle R, Holmes N G, Rademaker H, Duysens L N

出版信息

Biochim Biophys Acta. 1978 Jul 6;503(1):10-25. doi: 10.1016/0005-2728(78)90158-5.

Abstract

This work describes fluorescence yield measurements in suspensions of strains of Rhodospirillum rubrum and Rhodopseudomonas sphaeroides in which the iron . quinone complex (X) was chemically reduced (state [PIX-]; P is the reaction center bacteriochlorophyll dimer, I is the long wavelength bacteriopheophytin), and compares these with the fluorescence observed when all the traps are open (state [PIX]) and with the fluorescence observed when all the traps are closed (state [P+IX]). At 77 K the amplitude and the shape of the fluorescence emission spectrum in [PIX-] are identical to those observed in [PIX]. This is a strong indication that all the extra fluorescence observed at room temperature in [PIX-] is, in fact, caused by an efficient back reaction [P+I-X-] leads to [PIX-]. Using an equation similar to the original Vredenberg-Duysens relationship (Vredenburg, W.J. and Duysens, L.N.M. (1963) Nature 197, 355-357) but now assuming that a single reaction center has a probability pt of trapping an excitation and (1--pt) of re-emitting it to the surroundings, we are able to calculate pt as a function of the temperature by measuring the fluorescence in [PIX], [PIX-] and [P+IX] as a function of the temperature. The calculated pt values agree reasonably well with triplet yields measured in isolated reaction centers. Finally, we have measured the reaction center triplet yield (PTR) in intact systems and we have shown that the sum of the triplet yield and the remaining loss processes (PL) in the antenna bacteriochlorophyll including the bacteriochlorophyll dimer (such as fluorescence, internal conversion or direct triplet formation) is approximately constant; if we assume that at 77 K the only process which occurs in the reaction center is the formation of a reaction center triplet, than PTR + PL=1. The energy barrier between [PIX-] and [P+I-X-] was estimated to be 0.11--0.15 eV for a set of preparations.

摘要

这项工作描述了在红螺菌和球形红假单胞菌菌株悬浮液中的荧光产率测量,其中铁 - 醌复合物(X)被化学还原(状态[PIX-];P是反应中心细菌叶绿素二聚体,I是长波长细菌脱镁叶绿素),并将这些结果与所有陷阱开放时观察到的荧光(状态[PIX])以及所有陷阱关闭时观察到的荧光(状态[P+IX])进行比较。在77K时,[PIX-]中荧光发射光谱的幅度和形状与[PIX]中观察到的相同。这有力地表明,在室温下[PIX-]中观察到的所有额外荧光实际上是由有效的逆反应[P+I-X-]导致[PIX-]引起的。使用一个类似于原始弗雷登伯格 - 杜伊斯恩斯关系的方程(弗雷登伯格,W.J.和杜伊斯恩斯,L.N.M.(1963年)《自然》197,355 - 357),但现在假设单个反应中心捕获激发的概率为pt,将其重新发射到周围环境的概率为(1 - pt),我们能够通过测量[PIX]、[PIX-]和[P+IX]中作为温度函数的荧光来计算pt作为温度的函数。计算得到的pt值与在分离的反应中心中测量的三重态产率相当吻合。最后,我们测量了完整系统中的反应中心三重态产率(PTR),并且我们已经表明,三重态产率与包括细菌叶绿素二聚体在内的天线细菌叶绿素中的剩余损失过程(PL)(如荧光、内转换或直接三重态形成)的总和大致恒定;如果我们假设在77K时反应中心中发生的唯一过程是反应中心三重态的形成,那么PTR + PL = 1。对于一组制剂,估计[PIX-]和[P+I-X-]之间的能垒为0.11 - 0.15eV。

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