Kenneth S. Pitzer Center for Theoretical Chemistry, Department of Chemistry, University of California, Berkeley, California 94720, USA.
J Chem Phys. 2019 Mar 7;150(9):094115. doi: 10.1063/1.5080122.
Unrestricted density functional theory (DFT) methods are typically expected to describe the homolytic dissociation of nonpolar single bonds in neutral species with qualitative accuracy, due to the lack of significant delocalization error. We however find that many widely used density functional approximations fail to describe features along the dissociation curve of the simple H molecule. This is not a universal failure of DFT in the sense that many classic functionals like PBE and B3LYP give very reasonable results, as do some more modern methods like MS2. However, some other widely used functionals like B97-D (empirically fitted) and TPSS (non-empirically constrained) predict qualitatively wrong static polarizabilities, force constants, and some even introduce an artificial barrier against association of independent H atoms to form H. The polarizability and force constant prediction failures appear to stem from incomplete spin localization into individual H atoms beyond the Coulson-Fischer point, resulting in "fractionally bonded" species where the ionic contributions to the Slater determinant are not completely eliminated, unlike the case of unrestricted Hartree-Fock. These errors therefore appear to be a consequence of poor self-consistent density prediction by the problematic functional. The same reasons could potentially lead to spurious barriers toward H atom association, indirectly also leading to incorrect forces. These unphysicalities suggest that the use of problematic functionals is probably unwise in ab initio dynamics calculations, especially if strong electrostatic interactions are possible.
无限制密度泛函理论 (DFT) 方法通常被期望能够定性准确地描述中性物种中非极性单键的均裂离解,因为不存在显著的离域误差。然而,我们发现许多广泛使用的密度泛函近似不能描述简单 H 分子离解曲线上的特征。这并不是 DFT 的普遍失败,因为许多经典泛函,如 PBE 和 B3LYP,以及一些更现代的方法,如 MS2,给出了非常合理的结果。然而,一些其他广泛使用的泛函,如 B97-D(经验拟合)和 TPSS(非经验约束),则预测出了错误的静态极化率、力常数,甚至有些方法引入了人为的障碍,阻止独立的 H 原子形成 H。这些极化率和力常数预测失败似乎源于在考尔森-菲舍尔点之外,单个 H 原子的自旋局域化不完全,导致“部分键合”物种,其中斯莱特行列式的离子贡献没有完全消除,这与无限制哈特利-福克的情况不同。因此,这些误差似乎是有问题的泛函在自洽密度预测方面的不良结果。同样的原因可能会导致 H 原子缔合的虚假障碍,间接地导致力的不正确。这些非物理性质表明,在从头动力学计算中使用有问题的泛函可能是不明智的,特别是如果存在强静电相互作用的话。