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Picosecond kinetics of fluorescence and absorbance changes in photosystem II particles excited at low photon density

机译:在低光子密度下激发的光系统II粒子的荧光和吸收率变化的皮秒动力学

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摘要

Oxygen-evolving photosystem II particles (from Synechococcus) with about 80 chlorophyll molecules per primary electron donor (P680) were used for a correlated study of picosecond kinetics of fluorescence and absorbance changes, detected by the single-photon-timing technique and by a pump-probe apparatus, respectively. Chlorophyll fluorescence decays were biexponential with lifetimes τ1 = 80 ± 20 ps and τ2 = 520 ± 120 ps in open reaction centers and τ1 = 220 ± 30 ps and τ2 = 1.3 ± 0.15 ns in closed reaction centers. The corresponding fluorescence yield ratio Fmax/Fo was 3-4. Absorbance changes were monitored in the spectral range of 620-700 nm after excitation at 675 nm with 10-ps pulses sufficiently weak (<7 × 1012 photons/cm2 per pulse) to avoid singlet-singlet annihilation. With open reaction centers, the absorbance changes could be fit to the sum of three exponentials. The associated absorbance difference spectra were attributed to (i) exciton trapping and charge separation (τ = 100 ± 20 ps), (ii) the electron-transfer step P680+ I- QA → P680+ I QA- (where I is the primary electron acceptor and QA is the first quinone acceptor) (τ = 510 ± 50 ps), and (iii) the reduction of P680+ by the intact donor side (τ > 10 ns). With closed reaction centers, the absorbance changes were biexponential with lifetimes τ1 = 170-260 ps and τ2 = 1.6-1.75 ns. The results are explained in terms of a kinetic model that assumes P680 to constitute a shallow trap. The results show that QA reduction in these photosystem II particles decreases both the apparent rate and the yield of the primary charge separation by a factor of 2-3 and increases the mean lifetime of excitons in the antenna by a factor of 3-4. Thus, we conclude that the long-lived, nanosecond chlorophyll fluorescence is not charge-recombination luminescence but rather emission from equilibrated excited states of antenna chlorophylls.
机译:每个初级电子供体(P680)大约有80个叶绿素分子的放氧光系统II颗粒(来自Synechococcus)被用于通过单光子定时技术和泵检测的皮秒动力学荧光和吸光度变化的相关研究。 -探头设备。叶绿素荧光衰减是双指数的,在开放反应中心的寿命为τ1= 80±20 ps和τ2= 520±120 ps,在封闭反应中心的寿命为τ1= 220±30 ps和τ2= 1.3±0.15 ns。相应的荧光产率比Fmax / Fo为3-4。在675 nm激发后,在10-ps脉冲足够弱的情况下(<7×10 12 光子/ cm 2 每秒)在620-700 nm光谱范围内监测吸光度变化。脉冲),以避免单重态ing灭。在开放反应中心的情况下,吸光度变化可能适合三个指数的总和。相关的吸光度差异光谱归因于(i)激子俘获和电荷分离(τ= 100±20 ps),(ii)电子转移步骤P680 + I - QA→P680 + I QA -(其中I是主要电子受体,QA是第一个醌受体)(τ= 510±50 ps),和(iii )通过完整的供体侧(τ> 10 ns)还原P680 + 。在封闭的反应中心,吸收率的变化是双指数的,寿命τ1= 170-260 ps,τ2= 1.6-1.75 ns。根据动力学模型解释了结果,该动力学模型假定P680构成浅陷阱。结果表明,这些光系统II粒子的Q A 减少将表观速率和一次电荷分离的产率降低了2-3倍,并通过以下方式延长了天线中激子的平均寿命: 3-4倍。因此,我们得出结论,长寿命的纳秒级叶绿素荧光不是电荷重组发光,而是天线叶绿素平衡激发态的发射。

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