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含锌细菌叶绿素的球形红杆菌反应中心中的电子转移:光穴烧蚀研究。

Electron transfer in Rhodobacter sphaeroides reaction centers containing Zn-bacteriochlorophylls: a hole-burning study.

机构信息

Department of Chemistry, Kansas State University, Manhattan, Kansas 66506, USA.

出版信息

J Phys Chem B. 2012 Mar 15;116(10):3457-66. doi: 10.1021/jp300304r. Epub 2012 Feb 29.

Abstract

Nonresonant and resonant transient, photochemical hole-burned (HB) spectra are presented for primary electron donor states of a novel bacterial reaction center (Zn-RC) of Rhodobacter sphaeroides, containing six Zn-bacteriochlorophylls (Zn-BChls). A "Zn-β-RC" in which the Zn-BChl in the bacteriopheophytin (BPhe)-binding site on the A side (H(A)) has the Zn penta-coordinated, was also studied. The fifth ligand comes from a histidine introduced by site-directed mutagenesis. Formation of the P(+)Q(A)(-) state was observed in both types of RC, although under identical experimental conditions a significantly deeper P(-) band (corresponding to the lower-energy, special pair, excitonic component) was revealed in the Zn-RC. Assuming a similar lifetime of the P(+)Q(A)(-) state, the quantum yield of P(+)Q(A)(-) formation decreased by ~60% in the Zn-β-RC (compared to the Zn-RC), as was seen in a comparison of analogous (Mg) BChl-containing wild type and β-RCs of Rb. sphaeroides [Kirmaier et al. Science1991, 251, 922]. However, the average (weakly frequency-dependent) low-temperature electron transfer (ET) rates of the Zn-RC and Zn-β-RC (measured from zero phonon holes in resonant transient HB spectra) were both ~1 ps and similar to a rate previously measured in the Rb. sphaeroides native RC [Johnson et al. J. Phys. Chem. 1989, 93, 5953]. Electron transfer rates observed in this work on the Zn-RC yielded a P870* decay rate in good agreement with recent room-temperature, time-domain data [Lin et al. Proc. Natl. Acad. Sci. 2009, 106, 8537]. A lack of correlation observed between the holes near 810 and 883 nm, accounting for electrochromically induced shifts of the Zn-BChl transitions in the B(A,B) and H(A,B) binding sites, produced by formation of the P(+)BHQ(A)(-) state, indicates that the 810 nm bleach does not correspond to the P(+) (upper excitonic component of the dimer) band and is mostly contributed to by a shift of the B(B) absorption band. ZPH-action spectra indicated inhomogeneous broadening (Γ(inh)) of ~110 cm(-1) (Zn-RC) and ~130 cm(-1) (Zn-β-RC). Experimentally determined Γ(inh) decreased the number of variables in theoretical fits of the absorption and frequency-dependent shapes of resonant HB spectra, leading to more reliable Huang-Rhys factors for both low-frequency phonons and a pseudolocalized phonon, ω(SP), often referred to as the special pair marker mode.

摘要

非共振和共振瞬态、光化学空穴烧蚀(HB)光谱被呈现为一种新型细菌反应中心(Zn-RC)的初级电子供体状态,该反应中心含有六个锌细菌叶绿素(Zn-BChls)。还研究了在 A 侧(H(A))上结合位的细菌叶绿素(BPhe)结合位含有 Zn 五配位的“Zn-β-RC”,第五个配体来自通过定点突变引入的组氨酸。在这两种类型的 RC 中都观察到了 P(+)Q(A)(-)状态的形成,尽管在相同的实验条件下,在 Zn-RC 中揭示了明显更深的 P(-)带(对应于较低能量的特殊对激子分量)。假设 P(+)Q(A)(-)状态的寿命相似,与 Zn-RC 相比,Zn-β-RC 中 P(+)Q(A)(-)形成的量子产率降低了约 60%(与 Zn-RC 相比),这与在 Rb.sphaeroides 的类似(Mg)BChl 野生型和β-RC 中观察到的情况相似[Kirmaier 等人,科学 1991,251,922]。然而,Zn-RC 和 Zn-β-RC 的平均(弱频率依赖)低温电子转移(ET)速率(从共振瞬态 HB 光谱中的零声子孔测量)均为~1 ps,与先前在 Rb.sphaeroides 天然 RC 中测量的速率相似[Johnson 等人,J.Phys.Chem.1989,93,5953]。在这项关于 Zn-RC 的工作中观察到的电子转移速率产生了与最近室温、时域数据[Lin 等人,Proc.Natl.Acad.Sci.2009,106,8537]很好吻合的 P870*衰减速率。在 P(+)BHQ(A)(-)状态形成时,观察到近 810nm 和 883nm 处的孔之间缺乏相关性,这解释了在 B(A,B)和 H(A,B)结合位中 Zn-BChl 跃迁的电致变色诱导位移,表明 810nm 漂白不对应于 P(+)(二聚体的上激子分量)带,主要由 B(B)吸收带的位移引起。ZPH 作用谱表明不均匀展宽(Γ(inh))约为 110cm(-1)(Zn-RC)和约 130cm(-1)(Zn-β-RC)。实验确定的 Γ(inh)减少了理论拟合吸收和频率相关 HB 光谱形状的变量数量,从而为低频声子和伪局域声子(ω(SP))获得更可靠的黄-瑞利因子,ω(SP)通常被称为特殊对标记模式。

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