Woodbury N W, Parson W W
Biochim Biophys Acta. 1986 Jul 2;850(2):197-210. doi: 10.1016/0005-2728(86)90174-x.
Single-photon counting techniques were used to measure the fluorescence decay from Rhodopseudomonas sphaeroides and Rhodospirillum rubrum chromatophores after excitation with a 25-ps, 600-nm laser pulse. Electron transfer was blocked beyond the initial radical-pair state (PF) by chemical reduction of the quinone that serves as the next electron acceptor. Under these conditions, the fluorescence decays with multiphasic kinetics and at least three exponential decay components are required to describe the delayed fluorescence. Weak magnetic fields cause a small increase in the decay time of the longest component. The components of the delayed fluorescence are similar to those found previously with isolated reaction centers. We interpret the multi-exponential decay in terms of two small (0.01-0.02 eV) relaxations in the free energy of PF, as suggested previously for reaction centers. From the initial amplitudes of the delayed fluorescence, it is possible to calculate the standard free-energy difference between the earliest resolved form of PF and the excited singlet state of the antenna complexes in R. rubrum strains S1 and G9. The free-energy gap is found to be about 0.10 eV. It also is possible to calculate the standard free-energy difference between PF and the excited singlet state of the reaction center bacteriochlorophyll dimer (P). Values of 0.17 to 0.19 eV were found in both R. rubrum strains and also in Rps. sphaeroides strain 2.4.1. This free-energy gap agrees well with the standard free-energy difference between PF and P determined previously for reaction centers isolated from Rps. sphaeroides strain R26. The temperature dependence of the delayed fluorescence amplitudes between 180 K and 295 K is qualitatively different in isolated reaction centers and chromatophores. However, the temperature dependence of the calculated standard free-energy difference between P* and PF is similar in reaction centers and chromatophores of Rps. sphaeroides. The different temperature dependence of the fluorescence amplitudes in reaction centers and chromatophores arises because the free-energy difference between P* and the excited antenna is dominated by the entropy change associated with delocalization of the excitation in the antenna. We conclude that the state PF is similar in isolated reaction centers and in the intact photosynthetic membrane. Chromatophores from Rps. sphaeroides strain R-26 exhibit an anomalous fluorescence component that could reflect heterogeneity in their antenna.
采用单光子计数技术,在25皮秒、600纳米激光脉冲激发后,测量球形红假单胞菌和深红红螺菌载色体的荧光衰减。通过化学还原作为下一个电子受体的醌,电子转移在初始自由基对状态(PF)之后被阻断。在这些条件下,荧光以多相动力学衰减,并且至少需要三个指数衰减分量来描述延迟荧光。弱磁场会使最长分量的衰减时间略有增加。延迟荧光的分量与先前在分离的反应中心中发现的分量相似。正如先前对反应中心所建议的那样,我们根据PF自由能中的两个小(0.01 - 0.02电子伏特)弛豫来解释多指数衰减。从延迟荧光的初始振幅,可以计算出深红红螺菌菌株S1和G9中PF最早分辨形式与天线复合物激发单重态之间的标准自由能差。发现自由能隙约为0.10电子伏特。还可以计算出PF与反应中心细菌叶绿素二聚体(P)激发单重态之间的标准自由能差。在深红红螺菌的两个菌株以及球形红假单胞菌菌株2.4.1中都发现其值为0.17至0.19电子伏特。这个自由能隙与先前为从球形红假单胞菌菌株R26分离的反应中心确定的PF和P之间的标准自由能差非常吻合。在180 K至295 K之间,分离的反应中心和载色体中延迟荧光振幅的温度依赖性在定性上有所不同。然而,在球形红假单胞菌的反应中心和载色体中,计算出的P和PF之间的标准自由能差的温度依赖性是相似的。反应中心和载色体中荧光振幅不同的温度依赖性是因为P与激发天线之间的自由能差主要由与天线中激发离域相关的熵变决定。我们得出结论,PF状态在分离的反应中心和完整的光合膜中是相似的。球形红假单胞菌菌株R - 26的载色体表现出一种异常的荧光成分,这可能反映了其天线中的异质性。