Walla P J, Linden P A, Hsu C P, Scholes G D, Fleming G R
Department of Chemistry, University of California, and Physical Biosciences Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720-1460, USA.
Proc Natl Acad Sci U S A. 2000 Sep 26;97(20):10808-13. doi: 10.1073/pnas.190230097.
Time-resolved excited-state absorption intensities after direct two-photon excitation of the carotenoid S(1) state are reported for light-harvesting complexes of purple bacteria. Direct excitation of the carotenoid S(1) state enables the measurement of subsequent dynamics on a fs time scale without interference from higher excited states, such as the optically allowed S(2) state or the recently discovered dark state situated between S(1) and S(2). The lifetimes of the carotenoid S(1) states in the B800-B850 complex and B800-B820 complex of Rhodopseudomonas acidophila are 7+/-0.5 ps and 6+/-0.5 ps, respectively, and in the light-harvesting complex 2 of Rhodobacter sphaeroides approximately 1.9+/-0.5 ps. These results explain the differences in the carotenoid to bacteriochlorophyll energy transfer efficiency after S(2) excitation. In Rps. acidophila the carotenoid S(1) to bacteriochlorophyll energy transfer is found to be quite inefficient (phi(ET1) <28%) whereas in Rb. sphaeroides this energy transfer is very efficient (phi(ET1) approximately 80%). The results are rationalized by calculations of the ensemble averaged time constants. We find that the Car S(1) --> B800 electronic energy transfer (EET) pathway ( approximately 85%) dominates over Car S(1) --> B850 EET ( approximately 15%) in Rb. sphaeroides, whereas in Rps. acidophila the Car S(1) --> B850 EET ( approximately 60%) is more efficient than the Car S(1) --> B800 EET ( approximately 40%). The individual electronic couplings for the Car S(1) --> BChl energy transfer are estimated to be approximately 5-26 cm(-1). A major contribution to the difference between the energy transfer efficiencies can be explained by different Car S(1) energy gaps in the two species.
报道了紫色细菌捕光复合物在类胡萝卜素S(1)态直接双光子激发后的时间分辨激发态吸收强度。类胡萝卜素S(1)态的直接激发能够在飞秒时间尺度上测量后续动力学,而不受更高激发态的干扰,如光学允许的S(2)态或最近发现的位于S(1)和S(2)之间的暗态。嗜酸性红假单胞菌的B800 - B850复合物和B800 - B820复合物中类胡萝卜素S(1)态的寿命分别为7±0.5皮秒和6±0.5皮秒,而在球形红杆菌的捕光复合物2中约为1.9±0.5皮秒。这些结果解释了S(2)激发后类胡萝卜素向细菌叶绿素能量转移效率的差异。在嗜酸性红假单胞菌中,发现类胡萝卜素S(1)向细菌叶绿素的能量转移效率相当低(φ(ET1)<28%),而在球形红杆菌中这种能量转移非常高效(φ(ET1)约为80%)。通过系综平均时间常数的计算使结果合理化。我们发现,在球形红杆菌中,Car S(1)→B800电子能量转移(EET)途径(约85%)比Car S(1)→B850 EET(约15%)占主导,而在嗜酸性红假单胞菌中,Car S(1)→B850 EET(约60%)比Car S(1)→B800 EET(约40%)更有效。类胡萝卜素S(1)→细菌叶绿素能量转移的单个电子耦合估计约为5 - 26厘米(-1)。两种物种之间能量转移效率差异的主要原因可以用不同的类胡萝卜素S(1)能隙来解释。