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首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >The Radical Pair State PA in PhotosystemⅠ Single Crystals: Orientation Dependence of the Transient Spin-Polarized EPR Spectra
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The Radical Pair State PA in PhotosystemⅠ Single Crystals: Orientation Dependence of the Transient Spin-Polarized EPR Spectra

机译:光系统Ⅰ单晶中的自由基对态PA:瞬态自旋极化EPR谱的取向依赖性

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The light-induced, charge-separated state P↑(·+)↓(700)A↑(·-)↓(1) in single crystals of PhotosystemⅠ (PSI) from the cyanobacterium Synechococcus elongatus is investigated with transient, direct-detection EPR spectroscopy. The orientation of the phylloquinone head group of A↓(1) within the PSI reaction center is determined from the orientation dependence of the spin-polarized X-band EPR spectrum of the radical pair P↑(·+)↓(700)A↑(·-)↓(l) made up of the primary donor, P↓(700), and the acceptor, A↓(l). From the angular dependence of the overall spin-polarization pattern an upper limit ∠(c, Z↓(d)) ≤30° is evaluated for the angle between the crystallographic c-axis, collinear with the membrane normal, and the dipolar axis, Zd, connecting the electron spin density centers of P↑(·+)↓(700) and A↑(·-)↓(1). A partially resolved hyperfine coupling (hfc) is assigned to the hfc tensor of the 2-methyl group of A↓(1) Its A↓(‖) principal axis encloses an angle of β= 35°--55° with c. Simulations of the rotation patterns support a lower limit for the angle ∠(c, Zd) ≥ 25° with a larger error than for the upper limit. Zd is confirmed to be parallel to both the g↓(xx) principal axis of g(A↑(·-)↓(1)) and to the C=O carbonyl bonds within ±5° With respect to rotation around the g↓(xx) axis, the angle between the (c, Zd) plane and the quinone plane of the A↑(·-)↓(1) head group can only be specified within an upper limit of 60°. Together with independent knowledge about the location of A↓(1) within the PSI reaction center, a nearly complete structural model for the head group of the functional A↓(1) cofactor is achieved.
机译:采用瞬时,直接检测技术研究了蓝藻集球菌的光系统Ⅰ(PSI)单晶中光诱导的电荷分离状态P↑(·+)↓(700)A↑(·-)↓(1) EPR光谱。根据自由基对P↑(·+)↓(700)A↑的自旋极化X波段EPR光谱的取向依赖性确定PSI反应中心内A↓(1)的叶醌基团的取向(·-)↓(l)由主要供体P↓(700)和受体A↓(l)组成。根据整个自旋极化图的角度依赖性,计算出与薄膜法线共线的结晶c轴与偶极轴之间的夹角上限∠(c,Z↓(d))≤30°, Zd,连接P↑(·+)↓(700)和A↑(·-)↓(1)的电子自旋密度中心。将部分解析的超精细耦合(hfc)分配给A↓(1)的2-甲基基团的hfc张量,其A↓(‖)主轴线与c围成β= 35°--55°的角。旋转模式的仿真支持角度∠(c,Zd)≥25°的下限,其误差大于上限。确认Zd与g(A↑(·-)↓(1))的g↓(xx)主轴和围绕g↓旋转的±5°内的C = O羰基键平行在(xx)轴上,A↑(·-)↓(1)头组的(c,Zd)平面和醌平面之间的角度只能在60°的上限内指定。加上关于A↓(1)在PSI反应中心内位置的独立知识,可以得到功能性A↓(1)辅因子的头基的几乎完整的结构模型。

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