Electronic structure of clean and carbon-covered closed-packed rhodium and ruthenium surfaces

Peter J. Feibelman
Phys. Rev. B 26, 5347 – Published 15 November 1982
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Abstract

In order to determine the nature of the active species which several groups have found to be important in catalytic carbon hydrogenation reactions, self-consistent linear combination of atomic orbitals (LCAO) calculations have been performed of the electronic structure of clean and C-covered Rh(111) and Ru(0001) surfaces. Apart from the shift of the Fermi level to higher energy to accomodate an extra electron per atom in Rh, the results are quite similar for the two metals. A (1×1) layer of C's, occupying threefold-coordination sites binds by forming tetrahedral bonds with its neighbors, leaving a nonbonding pz band at the Fermi energy. Thus the model C species examined here should be very reactive. Additionally, the C 2sC 2pz binding-energy difference is about 10 eV, in accord with the Augerpeak separation seen by Goodman et al. for a reactive carbidic layer on Ni. Partial local density of states (LDOS) and energy-band dispersion curves are presented to permit the verification of the model carbidic overlayer. Results presented for the clean surfaces include work functions that are in excellent accord with the measured values, and band dispersions, notably a surface resonance band that has been observed on Ru, by Himpsel et al. Finally, surface-bulk core-level binding-energy shifts have been calculated. For the clean surfaces, they are in reasonable agreement with empirical heats of segregation. For the C-covered surfaces, they indicate that C binds most strongly to Ru, followed by Rh and Pd.

  • Received 17 May 1982

DOI:https://doi.org/10.1103/PhysRevB.26.5347

©1982 American Physical Society

Authors & Affiliations

Peter J. Feibelman

  • Sandia National Laboratories, Albuquerque, New Mexico 87185

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Issue

Vol. 26, Iss. 10 — 15 November 1982

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