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 800–4000- region—a broad band at 1016 at T=100 K for H on Mo(100) and at 1069 at T=300 K for H on W(100), corresponding to the symmetric stretch (), and a narrow derivative-like feature at 1302 on Mo(100) and at 1269 on W(100), identified as the first overtone of the wag motion (2). The physical origin of the line shapes, as well as the larger intensity of the 2 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 and 2 linewidths. The most distinctive feature of the spectra, the derivative or ‘‘Fano shape’’ of 2, arises from a nonadiabatic coupling between the sharp 2 vibration and the continuum absorption due to surface electronic transitions. The asymmetry parameter ντ̃, which gauges the 2-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 2 on both surfaces at T=100 K, 12.2 on Mo(100) and 18.5 on W(100), set a limit on the lifetime of these vibrational levels at ≥0.9 ps and ≥0.6 ps, respectively.
Direct evidence for the electronic excitation continuum that interacts with 2 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 2 intensity upon CO co-adsorption.
- Received 26 April 1988
DOI:https://doi.org/10.1103/PhysRevB.38.3112
©1988 American Physical Society