首页> 外文期刊>Journal of the American Chemical Society >ELECTRONIC STRUCTURE OF THE REDUCED BLUE COPPER ACTIVE SITE - CONTRIBUTIONS TO REDUCTION POTENTIALS AND GEOMETRY
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ELECTRONIC STRUCTURE OF THE REDUCED BLUE COPPER ACTIVE SITE - CONTRIBUTIONS TO REDUCTION POTENTIALS AND GEOMETRY

机译:还原的蓝铜活性部位的电子结构-对还原电位和几何形状的贡献

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A detailed electronic structure description of the reduced blue copper active site has now been developed. To date, the Cu(I) 3d(10) oxidation state of this site has been generally inaccessible to the spectroscopic techniques commonly employed in the extensive studies of the open shell, oxidized blue copper active site. Photoelectron spectroscopy (PES) of imidazole, dimethyl sulfide, and methanethiolate bound to Cu(I) sites at single crystal surfaces has been used to define normal Cu(I) bonding to ligands relevant to the blue copper site. Variable photon energy PES has been used to assign valence band spectra, assess metal-ligand covalency, and probe specific orbital contributions to Cu(I) bonding. Self Consistent Field-Xa-Scattered Wave (SCF-X alpha-SW) molecular orbital calculations calibrated to the photoelectron spectra have been performed to quantitatively complement the experimental bonding descriptions. These calculations have been extended to the reduced blue copper active site in plastocyanin, the prototypical blue copper protein, to detail the electronic structure changes that occur relative to normal Cu(I) bonding and upon oxidation. It is found that the weakened axial interaction associated with the elongated Cu-thioether bond is compensated by a strong Cu-thiolate equatorial pi bond, which activates the cysteine residue as an effective superexchange pathway for electron transfer. The metal-ligand bonding at the reduced blue copper site is found to be dominated by ligand p --> Cu(I) 4p charge transfer. Upon oxidation new Cu 3d bonding contributions arise as a result of the hole created in the Cu(II) 3d(x)(2)-(2)(y) orbital. In particular, the thiolate S pi orbital exhibits significant overlap with the d(x)(2)-(2)(y) orbital, which leads to a considerable increase in the thiolate pi donor strength of the Cu-S(thiolate) bond. Ionization energies have been used to estimate the electronic structure contributions to the reduction potential. The long Cu-thioether axial bond present at the active site destabilizes the oxidized state and is therefore a key determining factor in the high reduction potentials generally observed for blue copper proteins. Linear coupling terms have been evaluated for the distortions of a blue copper site unconstrained by the protein backbone. The geometry changes which occur in the blue copper site upon oxidation are found to be consistent with the changes in the electronic structure. Therefore, the reduced Cu(I) geometry is not imposed on the oxidized site by the protein environment. Rather, the structural constraints due to the protein matrix are present in the reduced site, where the long Cu-thioether bond lowers the site symmetry and eliminates the electronic degeneracy of the ground state and, thus, the Jahn-Teller distortion that would normally occur upon oxidation. As a result the geometric changes are small, giving rise to a low Franck-Condon barrier to electron transfer. [References: 95]
机译:现在已经开发了还原的蓝铜活性部位的详细电子结构描述。迄今为止,该位点的Cu(I)3d(10)氧化态通常对于在开放壳,氧化的蓝铜活性位点的广泛研究中通常使用的光谱技术来说是不可访问的。咪唑,二甲基硫醚和甲烷硫醇盐与单晶表面上的Cu(I)位键合的光电子能谱(PES)已用于定义正常Cu(I)与与蓝铜位点有关的配体的键合。可变光子能量PES已被用于分配价带谱,评估金属配体价和探测对Cu(I)键合的特定轨道贡献。已对光电子光谱进行了校准的自洽场Xa散射波(SCF-X alpha-SW)分子轨道计算,以定量补充实验性的键合描述。这些计算已扩展至原型蓝铜蛋​​白plastocyanin中还原的蓝铜活性位,以详细说明相对于正常Cu(I)结合和氧化时发生的电子结构变化。发现与拉长的Cu-硫醚键相关联的减弱的轴向相互作用被强的Cu-硫醇盐赤道π键补偿,其激活半胱氨酸残基作为电子转移的有效超交换途径。发现在还原的蓝铜位点处的金属-配体键主要由配体p-> Cu(I)4p电荷转移控制。在氧化时,由于在Cu(II)3d(x)(2)-(2)(y)轨道上形成的空穴而产生了新的Cu 3d键合贡献。特别是,硫醇盐S pi轨道与d(x)(2)-(2)(y)轨道表现出明显的重叠,这导致Cu-S(硫醇盐)键的硫醇盐pi供体强度显着增加。 。电离能已被用于估计电子结构对还原电势的贡献。活性位点上存在的长的Cu-硫醚轴向键使氧化态不稳定,因此是蓝色铜蛋白通常具有高还原电位的关键决定因素。线性耦合项已经评估了不受蛋白质主链约束的蓝色铜位点的变形。发现在氧化时在蓝铜部位发生的几何形状变化与电子结构的变化一致。因此,降低的Cu(I)几何形状不会被蛋白质环境强加在氧化位点上。相反,归因于蛋白质基质的结构限制存在于还原位点中,其中长的Cu-硫醚键降低了位点对称性并消除了基态的电子简并性,因此消除了通常会发生的Jahn-Teller变形在氧化时。结果,几何变化很小,对电子转移产生了低的弗兰克-康登势垒。 [参考:95]

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