4.6 Article

DFT-Based Method for More Accurate Adsorption Energies: An Adaptive Sum of Energies from RPBE and vdW Density Functionals

期刊

JOURNAL OF PHYSICAL CHEMISTRY C
卷 121, 期 9, 页码 4937-4945

出版社

AMER CHEMICAL SOC
DOI: 10.1021/acs.jpcc.6b10187

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资金

  1. U.S. Department of Energy, Office of Basic Energy Sciences, Division of Chemical Sciences, Biosciences and Geosciences [DE-SC0014560]
  2. Federal Republic of Germany through the Federal Ministry of Education and Research
  3. U.S. National Science Foundation [CHE-1361939]
  4. Office of Science of the U.S. Department of Energy [DE-AC02-05CH11231]
  5. U.S. Department of Energy (DOE) [DE-SC0014560] Funding Source: U.S. Department of Energy (DOE)
  6. Direct For Mathematical & Physical Scien
  7. Division Of Chemistry [1361939] Funding Source: National Science Foundation

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In recent years, the popularity of density functional theory with periodic boundary conditions (DFT) has surged for the design and optimization of functional materials. However, no single DFT exchange-correlation functional currently available gives accurate adsorption energies on transition metals both when bonding to the surface is dominated by strong covalent or ionic bonding and when it has strong contributions from van der Waals interactions (i.e., dispersion forces). Here we present a new, simple method for accurately predicting adsorption energies, on transition-metal surfaces based on DFT calculations, using an adaptively weighted sum of energies from RPBE and optB86b-vdW (or optB88-vdW) density functionals. This method has been benchmarked against a set of 39 reliable experimental energies for adsorption reactions. Our results show that this method has a mean absolute error and root mean squared error relative to experiments of 13.4 and 19.3 kJ/mol, respectively, compared to 20.4 and 26.4 kJ/mol for the BEEF-vdW functional. For systems with large van der Waals contributions, this method decreases these errors to 11.6 and 17.5 kJ/mol. Thus, this method provides predictions of adsorption energies both for processes dominated by strong covalent or ionic bonding and for those dominated by dispersion forces that are more accurate than those of any current standard DFT functional alone.

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