4.6 Article

Potential-dependent chemisorption of carbon monoxide on platinum electrodes: new insight from quantum-chemical calculations combined with vibrational spectroscopy

Journal

JOURNAL OF ELECTROANALYTICAL CHEMISTRY
Volume 500, Issue 1-2, Pages 344-355

Publisher

ELSEVIER SCIENCE SA
DOI: 10.1016/S0022-0728(00)00420-4

Keywords

density functional theory; CO adsorption at a Pt cluster; electrochemical stark effect

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Density functional theory (DFT) using the finite cluster approach is utilized to compute binding energies, bond geometries, and vibrational properties of carbon monoxide adsorbed on Pt(111) as a function of the external interfacial field, focusing attention on the metal-CO bond itself. Comparison with electrode potential-dependent frequencies for the metal-CO (nu (M-CO)) as well as the much-studied intramolecular C-O (vco) vibration, as measured by in-situ Raman and infrared spectroscopy, facilitate their interpretation in terms of metal-chemisorbate bonding for this archetypal electrochemical system. Decomposing the calculated metal-CO binding energy and vibrational frequencies into individual orbital and steric repulsion components enables the role of such quantum-chemical interactions to the field- (and hence potential-) dependent bonding to be assessed. No simple relationship between the field(F)-dependent binding energies and the nu (M-CO) frequencies is evident. While the DFT nu (M-CO)-F slopes are negative at positive and small-moderate negative fields, reflecting the prevailing influence of back-donation, a nu (M-CO)-F maximum is obtained at larger negative fields for atop CO, and a plateau for hollow-site CO. This Stark-tuning behavior reflects largely offsetting field-dependent contributions from pi and sigma surface bonding, and can also be rationalized on the basis of changes in the electrostatic component of nu (M-CO) from increasing M-CO charge polarization. A rough correlation between the held-dependent nu (M-CO) frequencies and the corresponding bond distances, r(M-CO), is observed for hollow and atop CO in that r(M-CO) shortens towards less positive fields, but becomes near-constant at moderate-large negative fields. A more quantitative correlation between the field-dependent C-O frequencies and bond lengths is also evident. In harmony with earlier findings (and unlike the nu (M-CO)-F behavior), the nu (CO)-F dependence is due chiefly to changes in the back-donation bonding component. The overall vibrational frequency-field behavior predicted by DFT is also in semi-quantitative concordance with experimental potential-dependent spectra. (C) 2001 Elsevier Science B.V. All rights reserved.

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