Faculty of Sciences, Department of Physics and Astronomy, Vrije Universiteit Amsterdam, De Boelelaan 1081, 1081 HV Amsterdam, The Netherlands.
Phys Chem Chem Phys. 2010 Mar 20;12(11):2693-705. doi: 10.1039/b905934b. Epub 2010 Jan 28.
Energy and electron transfer in a tyrosine M210 to tryptophan (YM210W) mutant of the Rhodobacter sphaeroides reaction center (RC) were investigated through time-resolved visible pump/mid-infrared (mid-IR) probe spectroscopy at room temperature, with the aim to further characterize the primary charge separated states in the RC. This mutant is known to display slow and multi-exponential charge separation, and was used in earlier work to prove the existence of an alternative route for charge separation starting from the accessory bacteriochlorophyll in the active branch, B(L). The mutant RCs were excited at 860 nm (direct excitation of the primary donor (P) BChls (P(L)/P(M))), 600 nm (unselective excitation), 805 nm (direct excitation of both accessory bacteriochlorophyll cofactors B(L) and B(M)) and 795 nm (direct excitation of B(L)). Absorption changes associated with carbonyl (C=O) stretch vibrational modes of the cofactors and protein were recorded in the region between 1600 and 1775 cm(-1), and both a sequential analysis and simultaneous target analysis of the data were performed. The decay of P* in the YM210W mutant was multi-exponential with lifetimes of 29 and 63.5 ps. The decay of P(+)B(L)(-) state was approximately 10 times longer in the YM210W RC than in the R-26 RC (approximately 7 ps vs. approximately 0.7 ps), and in the mid-IR difference absorption spectrum of P(+)B(L)(-) the stretching frequency of the 9-keto C=O group of B(L) in the ground state was located around 1675-1680 cm(-1), consistent with the presence of a hydrogen bond donated by an adjacent water molecule. Excitation at 795 nm produced a small amount of B(L)*-driven charge separation, as assessed from the excitation wavelength dependence of the raw difference spectra recorded during the first few ps after excitation. This process led to the formation of P(+)B(L)(-). Only the relaxed form of the P(+)H(L)(-) radical pair was observed in the YM210W mutant, and the mid-IR difference absorption spectra of P(+)H(L)(-) and P(+)B(L)(-) showed a change in the relative amplitude of the P(L)(+) and P(M)(+) bands when compared to equivalent spectra for the R-26 RC. This indicates that the YM210W mutation causes an increased localization of the electron hole on the P(M) half of the dimer. The absorbance difference spectrum of P(+)H(L)(-) in the R-26 RC contains a feature attributable to a Stark shift of one or more amide C=O oscillators. This feature was shifted to lower frequency by approximately 5 cm(-1) in the YM210W RC, and consideration of the limited structural changes in this RC indicates that this feature arises from an amide C=O group in the immediate vicinity of the M210 residue, most probably that of the adjacent M209 amino acid.
在室温下通过时间分辨可见泵/中红外(mid-IR)探针光谱研究了反应中心(RC)中酪氨酸 M210 到色氨酸(YM210W)突变体的能量和电子转移,目的是进一步表征 RC 中的初始电荷分离态。已知该突变体显示出缓慢和多指数电荷分离,并且在早期工作中用于证明从活性分支中的辅助细菌叶绿素 B(L)开始存在替代的电荷分离途径。突变体 RC 在 860nm(直接激发初级供体(P)细菌叶绿素(P(L)/P(M)))、600nm(非选择性激发)、805nm(直接激发辅助细菌叶绿素 cofactors B(L)和 B(M))和 795nm(直接激发 B(L))。在 1600 和 1775cm(-1)之间的区域记录了与辅助因子和蛋白质的羰基(C=O)伸缩振动模式相关的吸收变化,并对数据进行了顺序分析和同时目标分析。在 YM210W 突变体中,P*的衰减是多指数的,寿命为 29 和 63.5ps。在 YM210W RC 中,P(+)B(L)(-)态的衰减比 R-26 RC 长约 10 倍(约 7ps 对约 0.7ps),并且在 P(+)B(L)(-)的中红外差吸收光谱中,B(L)的 9-酮 C=O 基团在基态下的伸缩频率约为 1675-1680cm(-1),这与相邻水分子提供的氢键一致。在 795nm 处的激发产生了少量由 B(L)*驱动的电荷分离,这可以从激发后最初几 ps 期间记录的原始差光谱的激发波长依赖性来评估。这个过程导致了 P(+)B(L)(-)的形成。在 YM210W 突变体中仅观察到 P(+)H(L)(-)自由基对的弛豫形式,并且 P(+)H(L)(-)和 P(+)B(L)(-)的中红外差吸收光谱显示当与 R-26 RC 的等效光谱相比时,P(L)(+)和 P(M)(+)带的相对幅度发生变化。这表明 YM210W 突变导致电子空穴在二聚体的 P(M)半部分上的定位增加。R-26 RC 中 P(+)H(L)(-)的吸收差光谱包含归因于一个或多个酰胺 C=O 振荡器的斯塔克位移的特征。在 YM210W RC 中,该特征向低频移动了约 5cm(-1),并且对该 RC 中有限的结构变化的考虑表明,该特征来自于 M210 残基附近的酰胺 C=O 基团,很可能是相邻 M209 氨基酸的酰胺 C=O 基团。