Teschner Thomas, Yatsunyk Liliya, Schünemann Volker, Paulsen Hauke, Winkler Heiner, Hu Chuanjiang, Scheidt W Robert, Walker F Ann, Trautwein Alfred X
Institut für Physik, Universität zu Lübeck, Germany
J Am Chem Soc. 2006 Feb 1;128(4):1379-89. doi: 10.1021/ja056343k.
Crystalline samples of four low-spin Fe(III) octaalkyltetraphenylporphyrinate and two low-spin Fe(III) tetramesitylporphyrinate complexes, all of which are models of the bis-histidine-coordinated cytochromes of mitochondrial complexes II, III, and IV and chloroplast complex b(6)f, and whose molecular structures and EPR spectra have been reported previously, have been investigated in detail by Mössbauer spectroscopy. The six complexes and the dihedral angles between axial ligand planes of each are [(TMP)Fe(1-MeIm)(2)]ClO(4) (0 degree), paral-[(OMTPP)Fe(1-MeIm)(2)]Cl (19.5 degrees), paral-[(TMP)Fe(5-MeHIm)(2)]ClO(4) (26 degrees, 30 degrees for two molecules in the unit cell whose EPR spectra overlap), [(OETPP)Fe(4-Me(2)NPy)(2)]Cl (70 degrees), perp-[(OETPP)Fe(1-MeIm)(2)]Cl (73 degrees), and perp-[(OMTPP)Fe(1-MeIm)(2)]Cl (90 degrees). Of these, the first three have been shown to exhibit normal rhombic EPR spectra, each with three clearly resolved g-values, while the last three have been shown to exhibit "large g(max)" EPR spectra at 4.2 K. It is found that the hyperfine coupling constants of the complexes are consistent with those reported previously for low-spin ferriheme systems, with the largest-magnitude hyperfine coupling constant, A(zz), being considerably smaller for the "parallel" complexes (400-540 kG) than for the strictly perpendicular complex (902 kG), A(xx) being negative for all six complexes, and A(zz) and A(xx) being of similar magnitude for the "parallel" complexes (for example, for [(TMP)Fe(1-MeIm)(2)]Cl, A(zz) = 400 kG, A(xx) = -400 kG). In all cases, A(yy) is small but difficult to estimate with accuracy. With results for six structurally characterized model systems, we find for the first time qualitative correlations of g(zz), A(zz), and DeltaE(Q) with axial ligand plane dihedral angle Deltavarphi.
四种低自旋八烷基四苯基卟啉铁(III)和两种低自旋四甲基卟啉铁(III)配合物的晶体样品,所有这些都是线粒体复合物II、III和IV以及叶绿体复合物b(6)f中双组氨酸配位细胞色素的模型,并且其分子结构和电子顺磁共振光谱先前已被报道,已经通过穆斯堡尔光谱进行了详细研究。这六种配合物以及每种配合物轴向配体平面之间的二面角分别为[(TMP)Fe(1-MeIm)(2)]ClO(4)(0度)、顺式-[(OMTPP)Fe(1-MeIm)(2)]Cl(19.5度)、顺式-[(TMP)Fe(5-MeHIm)(2)]ClO(4)(26度,晶胞中两个分子的二面角为30度,其电子顺磁共振光谱重叠)、[(OETPP)Fe(4-Me(2)NPy)(2)]Cl(70度)、反式-[(OETPP)Fe(1-MeIm)(2)]Cl(73度)和反式-[(OMTPP)Fe(1-MeIm)(2)]Cl(90度)。其中,前三种已被证明表现出正常的菱形电子顺磁共振光谱,每种光谱都有三个清晰分辨的g值,而后三种已被证明在4.2 K时表现出“大g(max)”电子顺磁共振光谱。研究发现,这些配合物的超精细耦合常数与先前报道的低自旋高铁血红素系统的常数一致,“平行”配合物(400 - 540 kG)的最大超精细耦合常数A(zz)比严格垂直的配合物(902 kG)小得多,所有六种配合物的A(xx)均为负,并且“平行”配合物的A(zz)和A(xx)大小相似(例如,对于[(TMP)Fe(1-MeIm)(2)]Cl,A(zz) = 400 kG,A(xx) = -400 kG)。在所有情况下,A(yy)都很小但难以准确估计。通过六个结构表征的模型系统的结果,我们首次发现g(zz)、A(zz)和DeltaE(Q)与轴向配体平面二面角Deltavarphi之间的定性相关性。