CEA, Nuclear Energy Division, RadioChemistry & Processes Department, F-30207 Bagnols sur Cèze, France.
J Phys Chem A. 2013 May 30;117(21):4500-5. doi: 10.1021/jp401875f. Epub 2013 May 10.
The measured redox potential of an actinide at an electrode surface involves the transfer of a single electron from the electrode surface on to the actinide center. Before electron transfer takes place, the complexing ligands and molecules of solvation need to become structurally arranged such that the electron transfer is at its most favorable. Following the electron transfer, there is further rearrangement to obtain the minimum energy structure for the reduced state. As such, there are three parts to the total energy cycle required to take the complex from its ground state oxidized form to its ground state reduced form. The first part of the energy comes from the structural rearrangement and solvation energies of the actinide species before the electron transfer or charge transfer process; the second part, the energy of the electron transfer; the third part, the energy required to reorganize the ligands and molecules of solvation around the reduced species. The time resolution of electrochemical techniques such as cyclic voltammetry is inadequate to determine to what extent bond and solvation rearrangement occurs before or after electron transfer; only for a couple to be classed as reversible is it fast in terms of the experimental time. Consequently, the partitioning of the energy theoretically is of importance to obtain good experimental agreement. Here we investigate the magnitude of the instantaneous charge transfer through calculating the fast one electron reduction energies of AnO2(H2O)n(2+), where An = U, Np, and Pu, for n = 4-6, in solution without inclusion of the structural optimization energy of the reduced form. These calculations have been performed using a number of DFT functionals, including the recently developed functionals of Zhao and Truhlar. The results obtained for calculated electron affinities in the aqueous phase for the AnO2(H2O)5(2+/+) couples are within 0.04 V of accepted experimental redox potentials, nearly an order of magnitude improvement on previous calculated standard potentials E(0) values, obtained using both DFT and high level multireference approaches.
在电极表面测量锕系元素的氧化还原电位涉及从电极表面向锕系元素中心转移单个电子。在电子转移发生之前,需要对配位体和溶剂分子进行结构排列,以使电子转移处于最有利的状态。电子转移后,需要进一步重排以获得还原态的最低能量结构。因此,从复合物的基态氧化形式到基态还原形式,需要经历三个部分的总能量循环。第一部分能量来自电子转移或电荷转移过程之前的锕系物种的结构重排和溶剂化能;第二部分能量是电子转移的能量;第三部分能量是围绕还原物种重新排列配位体和溶剂分子所需的能量。电化学技术(如循环伏安法)的时间分辨率不足以确定电子转移前后键和溶剂化重排的程度;只有当一对被归类为可逆时,从实验时间的角度来看,它才是快速的。因此,理论上能量的分配对于获得良好的实验一致性很重要。在这里,我们通过计算 AnO2(H2O)n(2+)(其中 An = U、Np 和 Pu,n = 4-6)在溶液中的快速单电子还原能来研究瞬时电荷转移的幅度,而不包括还原形式的结构优化能。这些计算是使用几种 DFT 泛函进行的,包括最近由 Zhao 和 Truhlar 开发的泛函。对于 AnO2(H2O)5(2+/+)偶对在水相中的计算电子亲和能,得到的结果与公认的实验氧化还原电位相差 0.04 V,与之前使用 DFT 和高精度多参考方法获得的标准电位 E(0)值相比,有近一个数量级的改进。