Adsorption of Benzene on Copper, Silver, and Gold Surfaces

The adsorption of benzene on the Cu(111), Ag(111), Au(111), and Cu(110) surfaces at low coverage is modeled using density-functional theory (DFT) using periodic-slab models of the surfaces as well as using both DFT and complete-active-space self-consistent field theory with second-order M-r-Plesset...

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Main Authors: Bilic, Ante, Reimers, J., Hush, N., Hoft, R., Ford, M.
Format: Journal Article
Published: American Chemical Society 2006
Online Access:http://pubs.acs.org/journals/jctcce/index.html
http://hdl.handle.net/20.500.11937/9502
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author Bilic, Ante
Reimers, J.
Hush, N.
Hoft, R.
Ford, M.
author_facet Bilic, Ante
Reimers, J.
Hush, N.
Hoft, R.
Ford, M.
author_sort Bilic, Ante
building Curtin Institutional Repository
collection Online Access
description The adsorption of benzene on the Cu(111), Ag(111), Au(111), and Cu(110) surfaces at low coverage is modeled using density-functional theory (DFT) using periodic-slab models of the surfaces as well as using both DFT and complete-active-space self-consistent field theory with second-order M-r-Plesset perturbation corrections (CASPT2) for the interaction of benzene with a Cu13 cluster model for the Cu(110) surface. For the binding to the (111) surfaces, key qualitative features of the results such as weak physisorption, the relative orientation of the adsorbate on the surface, and surface potential changes are in good agreement with experimental findings. Also, the binding to Cu(110) is predicted to be much stronger than that to Cu(111) and much weaker than that seen in previous calculations for Ni(110), as observed. However, a range of physisorptive-like and chemisorptive-like structures are found for benzene on Cu(110) that are roughly consistent with observed spectroscopic data, with these structures differing dramatically in geometry but trivially in energy. For all systems, the bonding is found to be purely dispersive in nature with minimal covalent character. As dispersive energies are reproduced very poorly by DFT, the calculated binding energies are found to dramatically underestimate the observed ones, while CASPT2 calculations indicate that there is no binding at the Hartree- Fock level and demonstrate that the expected intermolecular correlation (dispersive) energy is of the correct order to explain the experimental binding-energy data. DFT calculations performed for benzene on Cu(110) and for benzene on the model cluster indicate that this cluster is actually too reactive and provides a poor chemical model for the system.
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publishDate 2006
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spelling curtin-20.500.11937-95022017-01-30T11:13:03Z Adsorption of Benzene on Copper, Silver, and Gold Surfaces Bilic, Ante Reimers, J. Hush, N. Hoft, R. Ford, M. The adsorption of benzene on the Cu(111), Ag(111), Au(111), and Cu(110) surfaces at low coverage is modeled using density-functional theory (DFT) using periodic-slab models of the surfaces as well as using both DFT and complete-active-space self-consistent field theory with second-order M-r-Plesset perturbation corrections (CASPT2) for the interaction of benzene with a Cu13 cluster model for the Cu(110) surface. For the binding to the (111) surfaces, key qualitative features of the results such as weak physisorption, the relative orientation of the adsorbate on the surface, and surface potential changes are in good agreement with experimental findings. Also, the binding to Cu(110) is predicted to be much stronger than that to Cu(111) and much weaker than that seen in previous calculations for Ni(110), as observed. However, a range of physisorptive-like and chemisorptive-like structures are found for benzene on Cu(110) that are roughly consistent with observed spectroscopic data, with these structures differing dramatically in geometry but trivially in energy. For all systems, the bonding is found to be purely dispersive in nature with minimal covalent character. As dispersive energies are reproduced very poorly by DFT, the calculated binding energies are found to dramatically underestimate the observed ones, while CASPT2 calculations indicate that there is no binding at the Hartree- Fock level and demonstrate that the expected intermolecular correlation (dispersive) energy is of the correct order to explain the experimental binding-energy data. DFT calculations performed for benzene on Cu(110) and for benzene on the model cluster indicate that this cluster is actually too reactive and provides a poor chemical model for the system. 2006 Journal Article http://hdl.handle.net/20.500.11937/9502 http://pubs.acs.org/journals/jctcce/index.html http://pubs.acs.org/cgi-bin/article.cgi/jctcce/2006/2/i04/pdf/ct050237r.pdf American Chemical Society restricted
spellingShingle Bilic, Ante
Reimers, J.
Hush, N.
Hoft, R.
Ford, M.
Adsorption of Benzene on Copper, Silver, and Gold Surfaces
title Adsorption of Benzene on Copper, Silver, and Gold Surfaces
title_full Adsorption of Benzene on Copper, Silver, and Gold Surfaces
title_fullStr Adsorption of Benzene on Copper, Silver, and Gold Surfaces
title_full_unstemmed Adsorption of Benzene on Copper, Silver, and Gold Surfaces
title_short Adsorption of Benzene on Copper, Silver, and Gold Surfaces
title_sort adsorption of benzene on copper, silver, and gold surfaces
url http://pubs.acs.org/journals/jctcce/index.html
http://pubs.acs.org/journals/jctcce/index.html
http://hdl.handle.net/20.500.11937/9502