Wasileski Sally A, Koper Marc T M, Weaver Michael J
Department of Chemistry, Purdue University, West Lafayette, Indiana 47907, USA.
J Am Chem Soc. 2002 Mar 20;124(11):2796-805. doi: 10.1021/ja012200w.
Illustrative quantum-chemical calculations for selected atomic and molecular chemisorbates on Pt(111) (modeled as a finite cluster) are undertaken as a function of external field, F, by using Density Functional Theory (DFT) with the aim of ascertaining the sensitivity of the field-dependent metal-adsorbate binding energetics and vibrational frequencies (i.e., the vibrational Stark effect) to the nature of the surface coordination in electrochemical systems. The adsorbates selected--Cl, I, O, N, Na, NH(3), and CO--include chemically important examples featuring both electron-withdrawing and -donating characteristics. The direction of metal-adsorbate charge polarization, characterized by the static dipole moment, mu(S), determines the binding energy-field (E(b-F) slopes, while the corresponding Stark-tuning behavior is controlled primarily by the dynamic dipole moment, mu(D). Significantly, analysis of the F-dependent sensitivity of mu(S) and mu(D) leads to a general adsorbate classification. For electronegative adsorbates, such as O and Cl, both mu(S) and mu(D) are negative, the opposite being the case for electropositive adsorbates. However, for systems forming dative-covalent rather than ionic bonds, as exemplified here by NH(3) and CO, mu(S) and mu(D) have opposite signs. The latter behavior, including electron-donating and -withdrawing categories, arises from diminishing metal-chemisorbate orbital overlap, and hence the extent of charge polarization, as the bond is stretched. A clear-cut distinction between these different types of surface bonding is therefore obtainable by combining vibrational Stark-tuning and E(b)-F slopes, as extracted from experimental data and/or DFT calculations. The former behavior is illustrated by means of potential-dependent Raman spectral data obtained in our laboratory.
通过使用密度泛函理论(DFT),针对Pt(111)(建模为有限簇)上选定的原子和分子化学吸附物进行了说明性量子化学计算,该计算是作为外部场F的函数进行的,目的是确定场依赖的金属 - 吸附物结合能和振动频率(即振动斯塔克效应)对电化学系统中表面配位性质的敏感性。所选的吸附物——Cl、I、O、N、Na、NH₃和CO——包括具有吸电子和供电子特性的重要化学实例。以静态偶极矩μ(S)为特征的金属 - 吸附物电荷极化方向决定了结合能 - 场(E(b - F)斜率,而相应的斯塔克调谐行为主要由动态偶极矩μ(D)控制。值得注意的是,对μ(S)和μ(D)的F依赖性敏感性分析导致了一种通用的吸附物分类。对于电负性吸附物,如O和Cl,μ(S)和μ(D)均为负,而对于电正性吸附物则相反。然而,对于形成配位共价而非离子键的系统,如这里以NH₃和CO为例,μ(S)和μ(D)具有相反的符号。后一种行为,包括供电子和吸电子类别,是由于随着键的拉伸,金属 - 化学吸附物轨道重叠减少,从而电荷极化程度降低而产生的。因此,通过结合从实验数据和/或DFT计算中提取的振动斯塔克调谐和E(b) - F斜率,可以清楚地区分这些不同类型的表面键合。前一种行为通过我们实验室获得的电位依赖拉曼光谱数据进行了说明。