Poulsen Rasmus D, Jørgensen Mads R V, Overgaard Jacob, Larsen Finn K, Morgenroth Wolfgang, Graber Timothy, Chen Yu-Sheng, Iversen Bo B
Department of Chemistry, University of Aarhus, 8000 Arhus C, Denmark.
Chemistry. 2007;13(35):9775-90. doi: 10.1002/chem.200700756.
Three high-quality single-crystal X-ray diffraction data sets have been measured under very different conditions on a structurally simple, but magnetically complex, coordination polymer, Mn(HCOO)(2)(H(2)O)(2) (1). The first data set is a conventional 100(2) K Mo(Kalpha) data set, the second is a very high resolution 100(2) K data set measured on a second-generation synchrotron source, while the third data set was measured with a tiny crystal on a high brilliance third-generation synchrotron source at 16(2) K. Furthermore, the magnetic susceptibility (chi) and the heat capacity (C(p)) have been measured from 2 to 300 K on pressed powder. The charge density of 1 was determined from multipole modeling of the experimental structure factors, and overall there is good agreement between the densities obtained separately from the three data sets. When considering the fine density features, the two 100 K data sets agree well with each other, but show small differences to the 16 K data set. Comparison with ab initio theory suggests that the 16 K APS data set provides the most accurate density. Topological analysis of the metal-ligand bonding, experimental 3d orbital populations on the Mn atoms, and Bader atomic charges indicate quite ionic, high-spin metal atoms. This picture is supported by the effective moment estimated from the magnetization measurements (5.840(2) mu(B)), but it is at variance with earlier spin density measurements from polarized neutron diffraction. The magnetic ordering originates from superexchange involving covalent interactions with the ligands, and non-ionic effects are observed in the static deformation density maps as well as in plots of the valence shell charge concentrations. Overall, the present study provides a benchmark charge density that can be used in comparison with future metal formate dihydrate charge densities.
在非常不同的条件下,对一种结构简单但磁性复杂的配位聚合物[Mn(HCOO)₂(H₂O)₂]∞ (1)测量了三个高质量的单晶X射线衍射数据集。第一个数据集是常规的100(2) K钼(Kα)数据集,第二个是在第二代同步辐射源上测量的非常高分辨率的100(2) K数据集,而第三个数据集是在16(2) K下用微小晶体在高亮度第三代同步辐射源上测量的。此外,还对压制粉末在2至300 K范围内测量了磁化率(χ)和热容(Cp)。通过对实验结构因子的多极建模确定了1的电荷密度,总体而言,从三个数据集分别获得的密度之间有很好的一致性。在考虑精细密度特征时,两个100 K数据集彼此吻合良好,但与16 K数据集存在细微差异。与从头算理论的比较表明,16 K APS数据集提供了最准确的密度。对金属-配体键合的拓扑分析、Mn原子上的实验3d轨道占据数和巴德原子电荷表明金属原子具有相当离子性的高自旋态。这一图景得到了磁化测量估计的有效磁矩(5.840(2) μB)的支持,但与早期极化中子衍射的自旋密度测量结果不一致。磁有序源于涉及与配体共价相互作用的超交换,在静态变形密度图以及价壳层电荷浓度图中观察到了非离子效应。总体而言,本研究提供了一个基准电荷密度,可用于与未来的金属甲酸盐二水合物电荷密度进行比较。