Theoretische Organische Chemie, Organisch-Chemisches Institut der Universität Münster, Corrensstrasse 40, 48149 Münster, Germany.
Chemphyschem. 2011 Dec 9;12(17):3414-20. doi: 10.1002/cphc.201100521. Epub 2011 Oct 19.
Dispersion-corrected density functional theory calculations (DFT-D3) were performed for the adsorption of CO on MgO and C(2) H(2) on NaCl surfaces. An extension of our non-empirical scheme for the computation of atom-in-molecules dispersion coefficients is proposed. It is based on electrostatically embedded M(4)X(4) (M=Na, Mg) clusters that are used in TDDFT calculations of dynamic dipole polarizabilities. We find that the C(MM)(6) dispersion coefficients for bulk NaCl and MgO are reduced by factors of about 100 and 35 for Na and Mg, respectively, compared to the values of the free atoms. These are used in periodic DFT calculations with the revPBE semi-local density functional. As demonstrated by calculations of adsorption potential energy curves, the new C(6) coefficients lead to much more accurate energies (E(ads)) and molecule-surface distances than with previous DFT-D schemes. For NaCl/C(2) H(2) we obtained at the revPBE-D3(BJ) level a value of E(ads) =-7.4 kcal mol(-1) in good agreement with experimental data (-5.7 to -7.1 kcal mol(-1)). Dispersion-uncorrected DFT yields an unbound surface state. For the MgO/CO system, the computed revPBE-D3(BJ) value of E(ads) =-4.1 kcal mol(-1) is also in reasonable agreement with experimental results (-3.0 kcal mol(-1)) when thermal corrections are taken into account. Our new dispersion correction also improves computed lattice constants of the bulk systems significantly compared to plain DFT or previous DFT-D results. The extended DFT-D3 scheme also provides accurate non-covalent interactions for ionic systems without empirical adjustments and is suggested as a general tool in surface science.
对 CO 在 MgO 上的吸附和 C(2)H(2)在 NaCl 表面上的吸附进行了弥散修正密度泛函理论计算(DFT-D3)。提出了一种扩展我们非经验原子分子弥散系数计算方案。它基于静电嵌入 M(4)X(4)(M=Na,Mg)簇,这些簇用于动态偶极极化率的 TDDFT 计算。我们发现,与自由原子相比,NaCl 和 MgO 体相的 C(MM)(6)弥散系数分别降低了约 100 和 35 倍,对于 Na 和 Mg。这些在使用 revPBE 半局域密度泛函的周期性 DFT 计算中使用。正如吸附势能曲线的计算所证明的那样,新的 C(6)系数导致比以前的 DFT-D 方案更准确的能量(E(ads))和分子-表面距离。对于 NaCl/C(2)H(2),我们在 revPBE-D3(BJ)水平上得到了 E(ads)=-7.4 kcal mol(-1)的值,与实验数据(-5.7 至-7.1 kcal mol(-1))吻合良好。未弥散修正的 DFT 给出了未结合的表面态。对于 MgO/CO 体系,计算得到的 revPBE-D3(BJ)值 E(ads)=-4.1 kcal mol(-1)在考虑热修正时也与实验结果(-3.0 kcal mol(-1))相当吻合。与纯 DFT 或以前的 DFT-D 结果相比,我们的新弥散修正也显著提高了体相系统的计算晶格常数。扩展的 DFT-D3 方案还为离子体系提供了准确的非共价相互作用,而无需经验调整,并被建议作为表面科学的通用工具。