Coupling of H vibration to substrate electronic states in Mo(100)-p(1×1)H and W(100)-p(1×1)H: Example of strong breakdown of adiabaticity

J. E. Reutt, Y. J. Chabal, and S. B. Christman
Phys. Rev. B 38, 3112 – Published 15 August 1988
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Abstract

The surface infrared reflectance spectra of Mo(100)-p(1×1)H and W(100)-p(1×1)H are both characterized by two vibrational absorptions in the 8004000-cm1 regiona broad band at 1016 cm1 at T=100 K for H on Mo(100) and at 1069 cm1 at T=300 K for H on W(100), corresponding to the symmetric stretch (ν1), and a narrow derivative-like feature at 1302 cm1 on Mo(100) and at 1269 cm1 on W(100), identified as the first overtone of the wag motion (2ν2). The physical origin of the line shapes, as well as the larger intensity of the 2ν2 than expected from adiabatic considerations, were investigated through phenomenological line-shape analysis of data obtained as a function of temperature and relative H/D and H/CO coadsorption concentrations. Inhomogeneous broadening is negligible, and dephasing processes contribute weakly to both ν1 and 2ν2 linewidths. The most distinctive feature of the spectra, the derivative or ‘‘Fano shape’’ of 2ν2, arises from a nonadiabatic coupling between the sharp 2ν2 vibration and the continuum absorption due to surface electronic transitions. The asymmetry parameter ν̃0τ̃, which gauges the 2ν2-continuum coupling strength, is temperature insensitive and does not exhibit an isotopic dependence, as predicted for a strong breakdown of adiabaticity. The narrow linewidths observed for 2ν2 on both surfaces at T=100 K, 12.2 cm1 on Mo(100) and 18.5 cm1 on W(100), set a limit on the lifetime of these vibrational levels at T1≥0.9 ps and T1≥0.6 ps, respectively.

Direct evidence for the electronic excitation continuum that interacts with 2ν2 is obtained by analyzing changes in broadband reflectivity measurements on W(100)/H and Mo(100)/H as a function of coverage. Both H-saturated surfaces exhibit a strong absorption with x-y symmetry that can be related to optical excitation of surface states. Further support for surface-state participation in the nonadiabatic process is inferred from the strong attenuation of the 2ν2 intensity upon CO co-adsorption.

  • Received 26 April 1988

DOI:https://doi.org/10.1103/PhysRevB.38.3112

©1988 American Physical Society

Authors & Affiliations

J. E. Reutt, Y. J. Chabal, and S. B. Christman

  • AT&T Bell Laboratories, Murray Hill, New Jersey 07974-2070

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Issue

Vol. 38, Iss. 5 — 15 August 1988

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