Butler W F, Calvo R, Fredkin D R, Isaacson R A, Okamura M Y, Feher G
Biophys J. 1984 May;45(5):947-73. doi: 10.1016/S0006-3495(84)84241-1.
Electron paramagnetic resonance (EPR) spectra of the reduced quinone-iron acceptor complex in reaction centers were measured in a variety of environments and compared with spectra calculated from a theoretical model. Spectra were obtained at microwave frequencies of 1, 9, and 35 GHz and at temperatures from 1.4 to 30 K. The spectra are characterized by a broad absorption peak centered at g = 1.8 with wings extending from g approximately equal to 5 to g less than 0.8. The peak is split with the low-field component increasing in amplitude with temperature. The theoretical model is based on a spin Hamiltonian, in which the reduced quinone, Q-, interacts magnetically with Fe2+. In this model the ground manifold of the interacting Q-Fe2+ system has two lowest doublets that are separated by approximately 3 K. Both perturbation analyses and exact numerical calculations were used to show how the observed spectrum arises from these two doublets. The following spin Hamiltonian parameters optimized the agreement between simulated and observed spectra: the electronic g tensor gFe, x = 2.16, gFe, y = 2.27, gFez = 2.04, the crystal field parameters D = 7.60 K and E/D = 0.25, and the antiferromagnetic magnetic interaction tensor, Jx = -0.13 K, Jy = -0.58 K, Jz = -0.58 K. The model accounts well for the g value (1.8) of the broad peak, the observed splitting of the peak, the high and low g value wings, and the observed temperature dependence of the shape of the spectra. The structural implications of the value of the magnetic interaction, J, and the influence of the environment on the spin Hamiltonian parameters are discussed. The similarity of spectra and relaxation times observed from the primary and secondary acceptor complexes Q-AFe2+ and Fe2+Q-B leads to the conclusion that the Fe2+ is approximately equidistant from QA and QB.
在各种环境中测量了反应中心中还原醌 - 铁受体复合物的电子顺磁共振(EPR)光谱,并与根据理论模型计算的光谱进行了比较。在1、9和35 GHz的微波频率以及1.4至30 K的温度下获得了光谱。这些光谱的特征是在g = 1.8处有一个宽吸收峰,其侧翼从g约等于5延伸到g小于0.8。该峰被分裂,低场分量的幅度随温度增加。理论模型基于一个自旋哈密顿量,其中还原醌Q-与Fe2+发生磁相互作用。在该模型中,相互作用的Q-Fe2+系统的基态流形有两个最低的双重态,它们之间的间隔约为3 K。使用微扰分析和精确数值计算来展示观察到的光谱是如何由这两个双重态产生的。以下自旋哈密顿量参数优化了模拟光谱与观察光谱之间的一致性:电子g张量gFe,x = 2.16,gFe,y = 2.27,gFe,z = 2.04,晶体场参数D = 7.60 K且E/D = 0.25,以及反铁磁相互作用张量Jx = -0.13 K,Jy = -0.58 K,Jz = -0.58 K。该模型很好地解释了宽峰的g值(1.8)、观察到的峰分裂、高g值和低g值侧翼以及观察到的光谱形状的温度依赖性。讨论了磁相互作用值J的结构含义以及环境对自旋哈密顿量参数的影响。从初级和次级受体复合物Q-AFe2+和Fe2+Q-B观察到的光谱和弛豫时间的相似性得出结论,Fe2+与QA和QB的距离大致相等。