Department of Materials Science & Engineering, University of Texas at Dallas, Richardson, Texas 75080, USA.
J Am Chem Soc. 2010 Feb 10;132(5):1654-64. doi: 10.1021/ja908817n.
Infrared (IR) absorption spectroscopy measurements, performed at 300 K and high pressures (27-55 bar) on several prototypes of metal organic framework (MOF) materials, reveal that the MOF ligands are weakly perturbed upon incorporation of guest molecules and that the molecular hydrogen (H(2)) stretch mode is red-shifted (30-40 cm(-1)) from its unperturbed value (4155 cm(-1) for ortho H(2)). For MOFs of the form M(bdc)(ted)(0.5) (bdc = 1,4-benzenedicarboxylate; ted = triethylenediamine), H(2) molecules interact with the organic ligands instead of the saturated metal centers located at the corners of the unit cell. First-principles van der Waals density functional calculations identify the binding sites and further show that the induced dipole associated with the trapped H(2) depends sensitively on these sites. For M(bdc)(ted)(0.5) systems, the strongest dipole moment is of the site that is in the corner of the unit cell and is dominated by the interaction with the benzene ligand and not by the metal center. For MOFs of the M(3)HCOO type with relatively short ligands (i.e., formate) and 1-D pore structures, there is a weak dependence of H(2) vibrational frequency on the cations, due to a small change in the unit cell dimension. Furthermore, translational states of approximately +/-100 cm(-1) are clearly observed as side bands on the H(2) stretch mode in these 1-D channels interconnected by very small apertures. The H(2) stretch IR integrated areas in all the MOFs considered in this work increase linearly with H(2) pressure, consistent with isotherm measurements performed in similar conditions. However, the IR intensity varies substantially, depending on the number of benzene rings interacting with the H(2) molecules. Finally, there is no correlation between H(2) binding energies (determined by isotherm measurements) and the magnitude of the H(2) stretch shift, indicating that IR shifts are dominated by the environment (organic ligand, metal center, and structure) rather than the strength of the interaction. These results highlight the relevance of IR spectroscopy to determine the type and arrangement of ligands in the structure of MOFs.
在 300 K 和高压(27-55 巴)下对几种金属有机骨架(MOF)材料的原型进行了红外(IR)吸收光谱测量,结果表明,当引入客体分子时,MOF 配体受到的干扰很微弱,并且氢气(H(2))的伸缩模式从其未受干扰的(对于正 H(2)为 4155 cm(-1))值红移(30-40 cm(-1))。对于形式为 M(bdc)(ted)(0.5)的 MOF(bdc = 1,4-苯二甲酸酯;ted = 三乙二胺),H(2)分子与有机配体相互作用,而不是与位于单元胞角的饱和金属中心相互作用。第一性原理范德华密度泛函计算确定了结合位点,并进一步表明与捕获的 H(2)相关的诱导偶极子对这些位点敏感。对于 M(bdc)(ted)(0.5)系统,最强的偶极矩是位于单元胞角的位点,主要由与苯配体的相互作用决定,而不是由金属中心决定。对于具有相对较短配体(即甲酸盐)和 1-D 孔结构的 M(3)[HCOO](6)类型的 MOF,由于单元胞尺寸的微小变化,H(2)振动频率对阳离子的依赖性较弱。此外,在这些由非常小的孔径互连的 1-D 通道中,H(2)伸缩模式的侧带可以清楚地观察到大约正负 100 cm(-1)的平移状态。在这项工作中考虑的所有 MOF 中,H(2)拉伸 IR 积分面积随 H(2)压力线性增加,与在类似条件下进行的等温测量一致。然而,IR 强度变化很大,取决于与 H(2)分子相互作用的苯环数量。最后,H(2)结合能(由等温测量确定)与 H(2)伸缩位移的大小之间没有相关性,这表明 IR 位移主要由环境(有机配体、金属中心和结构)决定,而不是由相互作用的强度决定。这些结果强调了红外光谱对于确定 MOF 结构中配体的类型和排列的重要性。