Autor: |
Wen X; Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, New Jersey 08544-5263, United States., Boyn JN; Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, New Jersey 08544-5263, United States., Martirez JMP; Princeton Plasma Physics Laboratory, Princeton, New Jersey 08540-6655, United States., Zhao Q; Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, New Jersey 08544-5263, United States., Carter EA; Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, New Jersey 08544-5263, United States.; Princeton Plasma Physics Laboratory, Princeton, New Jersey 08540-6655, United States.; Andlinger Center for Energy and the Environment, Princeton University, Princeton, New Jersey 08544-5263, United States. |
Abstrakt: |
Embedded correlated wavefunction (ECW) theory is a powerful tool for studying ground- and excited-state reaction mechanisms and associated energetics in heterogeneous catalysis. Several factors are important to obtaining reliable ECW energies, critically the construction of consistent active spaces (ASs) along reaction pathways when using a multireference correlated wavefunction (CW) method that relies on a subset of orbital spaces in the configuration interaction expansion to account for static electron correlation, e.g., complete AS self-consistent field theory, in addition to the adequate partitioning of the system into a cluster and environment, as well as the choice of a suitable basis set and number of states included in excited-state simulations. Here, we conducted a series of systematic studies to develop best-practice guidelines for ground- and excited-state ECW theory simulations, utilizing the decomposition of NH 3 on Pd(111) as an example. We determine that ECW theory results are relatively insensitive to cluster size, the aug-cc-pVDZ basis set provides an adequate compromise between computational complexity and accuracy, and that a fixed-clean-surface approximation holds well for the derivation of the embedding potential. Additionally, we demonstrate that a merging approach, which involves generating ASs from the molecular fragments at each configuration, is preferable to a creeping approach, which utilizes ASs from adjacent structures as an initial guess, for the generation of consistent potential energy curves involving open-d-shell metal surfaces, and, finally, we show that it is essential to include bands of excited states in their entirety when simulating excited-state reaction pathways. |