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Current advances in synthesizing and characterizing atomically precise monodisperse metal clusters (AMCs) at the subnanometer scale have opened up new possibilities in quantum materials research. Their quantizied “molecule‐like” electronic structure showcases unique stability, and physical and chemical properties differentiate them from larger nanoparticles. When integrated into inorganic materials that interact with the environment and sunlight, AMCs serve to enhance their (photo)catalytic activity and optoelectronic properties. Their tiny size makes AMCs isolated in the gas phase amenable to atom‐scale modeling using either density functional theory (DFT) or methods at a high level of ab initio theory, even addressing nonadiabatic (e.g., Jahn–Teller) effects. Surface‐supported AMCs can be routinely modeled using DFT, enabling long real‐time molecular dynamics simulations. Their optical properties can also be addressed using time‐dependent DFT or reduced density matrix (RDM) theory. These theoretical–computational efforts aim to achieve predictability and molecular‐level understanding of the stability and properties of AMCs as function of their composition, size, and structural fluxionality in different thermodynamical conditions (temperature and pressure). In this perspective, the potential of ab initio and DFT‐based modeling is illustrated through recent studies of unsupported and surface‐supported AMCs. Future directions of research are also discussed, including applications and methodological enhancements beyond the state‐of‐the‐art.
Current advances in synthesizing and characterizing atomically precise monodisperse metal clusters (AMCs) at the subnanometer scale have opened up new possibilities in quantum materials research. Their quantizied “molecule‐like” electronic structure showcases unique stability, and physical and chemical properties differentiate them from larger nanoparticles. When integrated into inorganic materials that interact with the environment and sunlight, AMCs serve to enhance their (photo)catalytic activity and optoelectronic properties. Their tiny size makes AMCs isolated in the gas phase amenable to atom‐scale modeling using either density functional theory (DFT) or methods at a high level of ab initio theory, even addressing nonadiabatic (e.g., Jahn–Teller) effects. Surface‐supported AMCs can be routinely modeled using DFT, enabling long real‐time molecular dynamics simulations. Their optical properties can also be addressed using time‐dependent DFT or reduced density matrix (RDM) theory. These theoretical–computational efforts aim to achieve predictability and molecular‐level understanding of the stability and properties of AMCs as function of their composition, size, and structural fluxionality in different thermodynamical conditions (temperature and pressure). In this perspective, the potential of ab initio and DFT‐based modeling is illustrated through recent studies of unsupported and surface‐supported AMCs. Future directions of research are also discussed, including applications and methodological enhancements beyond the state‐of‐the‐art.
The dissociative chemisorption (DC) of O 2 on Cu(111) has been extensively studied by both theory and experimentation. Different experiments disagree on the underlying mechanisms (direct or indirect) for the sticking of O 2 . Thus far, studies based on density functional theory (DFT) favor the indirect mechanism. However, DFT has not fully resolved the discussion as DFT based on the generalized gradient approximation (GGA) has always substantially overestimated the reactivity and sticking probabilities of O 2 on Cu(111) and other Cu surfaces. Recent work indicated that this overestimation is due to the failure of GGA DFT to describe molecule−metal systems where the charge transfer energy (E CT ), i.e., the work function of the metal surface minus the electron affinity of the molecule, is below 7 eV. O 2 + Cu( 111) is one such system. This work presents computed sticking probabilities for O 2 + Cu(111) based on the HSE06-1/2x-VdWDF2 screened hybrid van der Waals density functional (DF), which is applied self-consistently. A six-dimensional static potential energy surface (PES) was constructed using the corrugation-reducing procedure, keeping the surface atoms fixed. This PES was used to perform quasi-classical trajectory calculations to compute the sticking probabilities of O 2 + Cu(111). For the first time, we present DFT-based sticking probabilities that underestimate the experimental sticking probabilities. While reproducing the experimental results would have been even more desirable, the fact that we found a DF which underestimates the measured sticking probabilities means that a DF using a lower fraction of exact exchange will most likely describe the O 2 + Cu(111) system with high accuracy. Furthermore, our work shows evidence for the presence of both indirect and direct dissociative chemisorptions. The indirect precursor-mediated mechanism occurs for low-incidence energy O 2 . The mechanism is supplanted by a direct dissociative mechanism at higher incidence energies. Lastly, our work suggests that the Cu surface temperature may also affect the dissociation mechanism, but this still needs further verification with a different theoretical framework that allows for the simulation of surface temperature.
We report high-resolution angular diffraction measurements of CH 4 and Ne from Ni(111) and from a graphene (Gr) layer grown on Ni(111), whose effective atomic mass is enhanced by the strong Gr−Ni interaction. The incident energies are between 43 and 68 meV for Ne, and between 62 and 108 meV for CH 4 beams. Sharp diffraction features are observed with Ne beams from both Ni(111) and Gr/Ni(111) surfaces. However, using methane beams, clear diffraction peaks are observed only from Ni(111), with broad angular distributions measured from Gr/Ni(111), as expected for classical particles, with no quantum features. This is surprising, since Ne and methane have similar masses and therefore a comparable quantum behavior is expected for the same incident energy. This effect is mainly due to the larger physisorption well of CH 4 on Gr/Ni(111), as shown by DFT calculations, in addition to the larger corrugation of the potential energy surface and the excitation of phonon modes of the graphene overlayer.
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