Chiang Ming-Hsi, Antonio Mark R, Williams Clayton W, Soderholm L
Chemistry Division, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, IL 60439-4831, USA.
Dalton Trans. 2004 Mar 7(5):801-6. doi: 10.1039/b315334g. Epub 2004 Jan 30.
X-Ray absorption spectroscopy was used to probe the coordination of different encrypted cations in the Preyssler anions M(n+)P5W(30)O(110)(M(n+)= Sr2+, Am3+, Eu3+, Sm3+, Y3+, Th4+, U4+ in decreasing order of ionic radius, IR), hereafter abbreviated M(n+)PA-. The increase of the M-W distance and the decrease of the M-P distance with increasing M ionic radius reveal that the M cation is displaced along the C5 axis within the Preyssler cavity. The slight change (0.07 A) of the M-O distance that does not correspond to the IR difference of 0.27 A confirms that the cavity retains its rigidity upon cation substitution. Geometric modeling of the encapsulated cation in the channel was performed for comparison to the EXAFS results. The position of the cation in the cavity was calculated as well as the M-O10, -W5 and -P5 distances. This modeling confirms the cation displacement toward the center of the Preyssler anion as the cation size increases, which is understood in terms of the non-homogenous electrostatic potential present within the cavity. The bond valence model approach was applied to obtain experimental bond valences. Only the bond valence sum (BVS) of Am3+ is close to its actual charge. Sums smaller than the actual valences of the +3 and +4 ions (2.39-2.63 for +3 cations, Y, Sm, Eu; 3.17 and 3.38 for +4 cations, U and Th, respectively) were obtained, and a larger sum (2.89) was obtained for Sr2+. The deviations from the formal M sums of the encapsulated ions are attributed to the rigidity of the Preyssler framework. The tendency toward coordinative unsaturation for electroactive cations, such as Eu3+, is thought to be the driving force for facile reduction. Unlike other inorganic chelating ligands, the Preyssler anion provides a unique redox system to stabilize an electroactive cation in a low oxidation state.
利用X射线吸收光谱法探究了普雷斯勒阴离子[M(n+)P5W(30)O(110)]((15 - n)-)(M(n+)= Sr2+、Am3+、Eu3+、Sm3+、Y3+、Th4+、U4+,按离子半径减小顺序排列,即IR)中不同加密阳离子的配位情况,以下简称为[M(n+)PA](15 - n)-。随着M离子半径增大,M - W距离增加而M - P距离减小,这表明M阳离子在普雷斯勒空腔内沿C5轴发生位移。M - O距离的微小变化(0.07 Å)与0.27 Å的离子半径差异不对应,这证实了空腔在阳离子取代后保持其刚性。对通道中封装阳离子进行几何建模,以便与扩展X射线吸收精细结构(EXAFS)结果进行比较。计算了阳离子在空腔中的位置以及M - O10、 - W5和 - P5距离。该建模证实随着阳离子尺寸增加,阳离子向普雷斯勒阴离子中心位移,这可根据空腔内存在的非均匀静电势来理解。应用键价模型方法来获得实验键价。只有Am3+的键价和(BVS)接近其实际电荷。得到的值小于 +3和 +4离子的实际价态(+3阳离子Y、Sm、Eu为2.39 - 2.63;+4阳离子U和Th分别为3.17和3.38),而Sr2+得到的值更大(2.89)。封装离子与形式上M的和值存在偏差归因于普雷斯勒骨架的刚性。对于电活性阳离子如Eu3+,配位不饱和的趋势被认为是易于还原的驱动力。与其他无机螯合配体不同,普雷斯勒阴离子提供了一个独特的氧化还原体系来稳定处于低氧化态的电活性阳离子。