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Surface Adsorption from the Exchange-Hole Dipole Moment Dispersion Model

机译:交换孔偶极矩扩散模型的表面吸附

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The accurate calculation of intermolecular interaction energies with density functional theory requires methods that include a treatment of long-range, nonlocal dispersion correlation. In this work, we explore the ability of the exchange-hole dipole moment (XDM) dispersion correction to model molecular surface adsorption. Adsorption energies are calculated for six small aromatic molecules (benzene, furan, pyridine, thiophene, thiophenol, and benzenediamine) and the four DNA nucleobases (adenine, thymine, guanine, and cytosine) on the (111) surfaces of the three coinage metals (copper, silver, and gold). For benzene, where the experimental reference data is most precise, the mean absolute error in the computed absorption energies is 0.04 eV. For the other aromatic molecules, the computed binding energies are found to be within 0.09 eV of the available reference data, on average, which is well below the expected experimental uncertainties for temperature-programmed desorption measurements. Unlike other dispersion-corrected functionals, adequate performance does not require changes to the canonical XDM implementation, and the good performance of XDM is explained in terms of the behavior of the exchange hole. Additionally, the base functional employed (B86bPBE) is also optimal for molecular studies, making B86bPBE-XDM an excellent candidate for studying chemistry on material surfaces. Finally, the noncovalent interaction (NCI) plot technique is shown to detect adsorption effects in real space on the order of tenths of an eV.
机译:用密度泛函理论准确地计算分子间相互作用能需要使用包括处理长距离,非局部色散相关性的方法。在这项工作中,我们探索了交换孔偶极矩(XDM)色散校正模型分子表面吸附的能力。计算了三种造币金属(111)表面上六个芳香族小分子(苯,呋喃,吡啶,噻吩,噻吩和苯二胺)和四个DNA核碱基(腺嘌呤,胸腺嘧啶,鸟嘌呤和胞嘧啶)的吸附能。铜,银和金)。对于最精确的实验参考数据的苯,计算出的吸收能的平均绝对误差为0.04 eV。对于其他芳族分子,发现计算得出的结合能平均在可用参考数据的0.09 eV范围内,远低于程序升温脱附测量的预期实验不确定性。与其他色散校正功能不同,适当的性能不需要更改规范的XDM实现,并且根据交换孔的行为来说明XDM的良好性能。此外,所采用的基本功能(B86bPBE)也是分子研究的最佳选择,使B86bPBE-XDM成为研究材料表面化学的绝佳候选者。最后,非共价相互作用(NCI)绘图技术显示可检测到真实空间中吸附效应的十分之一eV。

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