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Monte Carlo simulations of excitation and electron transfer in grana membranes

机译:格兰纳膜中激发和电子转移的蒙特卡洛模拟

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摘要

Time-resolved fluorescence measurements on grana membranes with instrumental response function of 3 ps reveal faster excitation dynamics (120 ps) than those reported previously. A possible reason for the faster decay may be a relatively low amount of "extra" LHCII trimers per reaction center of Photosystem II. Monte Carlo modeling of excitation dynamics in CSM form of PSII-LHCII supercomplexes has been performed using a coarse grained model of this complex, constituting a large majority of proteins in grana membranes. The main factor responsible for the fast fluorescence decay reported in this work was the deep trap constituted by the primary charge separated state in the reaction center (950-1090 cm- 1). This value is critical for a good fit, whereas typical hopping times between antenna polypeptides (from ~ 4.5 to ~ 10.5 ps) and reversible primary charge separation times (from ~ 4 to ~ 1.5 ps, respectively) are less critical. Consequently, respective mean migration times of excitation from anywhere in the PSII-LHCII supercomplexes to reaction center range from ~ 30 to ~ 80 ps. Thus 1/4-2/3 of the ~ 120-ps average excitation lifetime is necessary for the diffusion of excitation to reaction center, whereas the remaining time is due to the bottle-neck effect of the trap. Removal of 27% of the Lhcb6 apoprotein pool by mutagenesis of DEG5 gene caused the acceleration of the excitation decay from ~ 120 to ~ 100 ps. This effect may be due to the detachment of LHCII-M trimers from PSII-LHCII supercomplexes, accompanied by deepening of the reaction center trap.
机译:在具有3 ps的仪器响应功能的格拉纳膜上进行时间分辨的荧光测量显示,激发动力学(120 ps)比以前报道的要快。更快衰减的可能原因可能是光系统II的每个反应中心的“额外” LHCII三聚体相对较少。已经使用该复合物的粗粒模型对CII形式的PSII-LHCII超复合物的激发动力学进行了蒙特卡洛建模,该模型构成了颗粒膜中的大部分蛋白质。在这项工作中报道的导致快速荧光衰减的主要因素是由反应中心的主电荷分离状态(950-1090 cm-1)构成的深陷阱。该值对于良好的拟合至关重要,而天线多肽之间的典型跳变时间(从〜4.5到〜10.5 ps)和可逆的一次电荷分离时间(分别从〜4到〜1.5 ps)则不那么关键。因此,从PSII-LHCII超复合物中任何地方到反应中心的激发的平均迁移时间分别为〜30 ps〜〜80 ps。因此,约120ps的平均激发寿命的1 / 4-2 / 3是激发扩散到反应中心所必需的,而剩余时间则是由于阱的瓶颈效应所致。通过诱变DEG5基因去除了27%的Lhcb6载脂蛋白池,导致激发衰减从〜120 ps加速到〜100 ps。这种作用可能是由于LHCII-M三聚体从PSII-LHCII超复合物中分离出来,同时伴随着反应中心阱的加深。

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