Croce R, Müller M G, Bassi R, Holzwarth A R
Max-Planck-Institut für Strahlenchemie, D-45470 Mülheim/Ruhr, Germany.
Biophys J. 2001 Feb;80(2):901-15. doi: 10.1016/S0006-3495(01)76069-9.
The energy transfer kinetics from carotenoids to chlorophylls and among chlorophylls has been measured by femtosecond transient absorption kinetics in a monomeric unit of the major light-harvesting complex (LHCII) from higher plants. The samples were reconstituted complexes with different carotenoid contents. The kinetics was measured both in the carotenoid absorption region and in the chlorophyll Q(y) region using two different excitation wavelengths suitable for selective excitation of the carotenoids. Analysis of the data shows that the overwhelming part of the energy transfer from the carotenoids occurs directly from the initially excited S(2) state of the carotenoids. Only a small part (<20%) may possibly take an S(1) pathway. All the S(2) energy transfer from carotenoids to chlorophylls occurs with time constants <100 fs. We have been able to differentiate among the three carotenoids, two luteins and neoxanthin, which have transfer times of approximately 50 and 75 fs for the two luteins, and approximately 90 fs for neoxanthin. About 50% of the energy absorbed by carotenoids is initially transferred directly to chlorophyll b (Chl b), while the rest is transferred to Chl a. Neoxanthin almost exclusively transfers to Chl b. Due to various complex effects discussed in the paper, such as a specific coupling of Chl b and Chl a excited states, the percentage of direct Chl b transfer thus is somewhat lower than estimated by us previously for LHCII from Arabidopsis thaliana. (Connelly, J. P., M. G. Müller, R. Bassi, R. Croce, and A. R. Holzwarth. 1997. Biochemistry. 36:281). We can distinguish three different Chls b receiving energy directly from carotenoids. We propose as a new mechanism that the carotenoid-to-Chl b transfer occurs to a large part via the B(x) state of Chl b and to the Q(x) state, while the transfer to Chl a occurs only via the Q(x) state. We find no compelling evidence in favor of a substantial S(1) transfer path of the carotenoids, although some transfer via the S(1) state of neoxanthin can not be entirely excluded. The S(1) lifetimes of the two luteins were determined to be 15 ps and 3.9 ps. A detailed quantitative analysis and kinetic model of the processes described here will be presented in a separate paper.
通过飞秒瞬态吸收动力学,在高等植物主要捕光复合物(LHCII)的单体单元中测量了从类胡萝卜素到叶绿素以及叶绿素之间的能量转移动力学。样品是具有不同类胡萝卜素含量的重组复合物。使用适合选择性激发类胡萝卜素的两种不同激发波长,在类胡萝卜素吸收区域和叶绿素Q(y)区域测量了动力学。数据分析表明,从类胡萝卜素的能量转移的绝大部分直接来自类胡萝卜素最初激发的S(2)态。只有一小部分(<20%)可能走S(1)途径。从类胡萝卜素到叶绿素的所有S(2)能量转移都以<100 fs的时间常数发生。我们能够区分三种类胡萝卜素,即两种叶黄素和新黄质,两种叶黄素的转移时间约为50 fs和75 fs,新黄质约为90 fs。类胡萝卜素吸收的能量约50%最初直接转移到叶绿素b(Chl b),其余转移到Chl a。新黄质几乎只转移到Chl b。由于本文讨论的各种复杂效应,如Chl b和Chl a激发态的特定耦合,因此直接Chl b转移的百分比略低于我们先前对拟南芥LHCII的估计。(康奈利,J.P.,M.G.米勒,R.巴西,R.克罗切,和A.R.霍尔兹瓦特。1997.生物化学。36:281)。我们可以区分三种直接从类胡萝卜素接收能量的不同Chls b。我们提出一种新机制,即类胡萝卜素到Chl b的转移很大一部分通过Chl b的B(x)态发生并转移到Q(x)态,而到Chl a的转移仅通过Q(x)态发生。我们没有找到支持类胡萝卜素大量S(1)转移路径的有力证据,尽管不能完全排除通过新黄质的S(1)态的一些转移。两种叶黄素的S(1)寿命测定为15 ps和3.9 ps。本文所述过程的详细定量分析和动力学模型将在另一篇论文中给出。