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Simulation of the S2 state multiline electron paramagnetic resonance signal of photosystem II: a multifrequency approach.

机译:光系统II的S2状态多线电子顺磁共振信号的仿真:多频方法。

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摘要

The S2 state electron paramagnetic resonance (EPR) multiline signal of Photosystem II has been simulated at Q-band (35 Ghz), X-band (9 GHz) and S-band (4 GHz) frequencies. The model used for the simulation assumes that the signal arises from an essentially magnetically isolated MnIII-MnIV dimer, with a ground state electronic spin ST = 1/2. The spectra are generated from exact numerical solution of a general spin Hamiltonian containing anisotropic hyperfine and quadrupolar interactions at both Mn nuclei. The features that distinguish the multiline from the EPR spectra of model manganese dimer complexes (additional width of the spectrum (195 mT), additional peaks (22), internal "superhyperfine" structure) are plausibly explained assuming an unusual ligand geometry at both Mn nuclei, giving rise to normally forbidden transitions from quadrupole interactions as well as hyperfine anisotropy. The fitted parameters indicate that the hyperfine and quadrupole interactions arise from Mn ions in low symmetry environments, corresponding approximately to the removal of one ligand from an octahedral geometry in both cases. For a quadrupole interaction of the magnitude indicated here to be present, the MnIII ion must be 5-coordinate and the MnIV 5-coordinate or possibly have a sixth, weakly bound ligand. The hyperfine parameters indicate a quasi-axial anisotropy at MnIII, which while consistent with Jahn-Teller distortion as expected for a d4 ion, corresponds here to the unpaired spin being in the ligand deficient, z direction of the molecular reference axis. The fitted parameters for MnIV are very unusual, showing a high degree of anisotropy not expected in a d3 ion. This degree of anisotropy could be qualitatively accounted for by a histidine ligand providing pi backbonding into the metal dxy orbital, together with a weakly bound or absent ligand in the x direction.
机译:已在Q波段(35 Ghz),X波段(9 GHz)和S波段(4 GHz)频率上模拟了Photosystem II的S2状态电子顺磁共振(EPR)多线信号。用于仿真的模型假设信号来自基本磁隔离的MnIII-MnIV二聚体,基态电子自旋ST = 1/2。光谱是从一般的自旋哈密顿量的精确数值解生成的,该自旋哈密顿量在两个Mn核上都包含各向异性的超精细和四极相互作用。假设在两个锰原子核上都有异常的配体几何构型,可以合理地解释将多线与模型锰二聚体配合物的EPR光谱区分开的特征(光谱的附加宽度(195 mT),附加峰(22),内部“超高精细”结构)。 ,会引起四极子相互作用中通常禁止的跃迁以及超精细各向异性。拟合的参数表明,超对称和四极相互作用是在低对称性环境中由Mn离子引起的,在两种情况下,大约对应于从八面体几何结构中除去一个配体。对于此处显示的大小的四极相互作用,MnIII离子必须为5配位且MnIV离子为5配位或可能具有第六个弱结合配体。超精细参数表明MnIII处的准轴各向异性,尽管与d4离子所预期的Jahn-Teller变形相一致,但此处对应于未配位的自旋在分子参考轴的配体缺陷z方向上。 MnIV的拟合参数非常不寻常,显示出在d3离子中无法预期的高度各向异性。这种各向异性程度可以通过组氨酸配体定性地解释,该组氨酸配体在金属dxy轨道上提供pi反向键合,并在x方向上弱结合或不存在配体。

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