SUBSTRATE AND HYDROGEN PHONONS OF THE ORDERED P(2X1) AND (2X2) PHASE AND OF THE ANOMALOUS (1X1) PHASE OF HYDROGEN ON W(110)

Citation
M. Balden et al., SUBSTRATE AND HYDROGEN PHONONS OF THE ORDERED P(2X1) AND (2X2) PHASE AND OF THE ANOMALOUS (1X1) PHASE OF HYDROGEN ON W(110), Physical review. B, Condensed matter, 53(11), 1996, pp. 7479-7491
Citations number
74
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
53
Issue
11
Year of publication
1996
Pages
7479 - 7491
Database
ISI
SICI code
0163-1829(1996)53:11<7479:SAHPOT>2.0.ZU;2-X
Abstract
The adsorbate and substrate phonons of the hydrogen- and deuterium-cov ered W(110) surface were investigated using electron-energy-loss spect roscopy (EELS). For coverages below saturation, the measured substrate phonon dispersion curves show a continuous change of the Rayleigh wav e frequency around the (S) over bar and (N) over bar points with incre asing coverage. No effect of the suggested reconstruction could be obs erved. For the saturated (1 x 1) phase the frequency of the Rayleigh w ave (RW) in the shallow dip of the phonon anomaly depends on coverage and temperature. In addition we found a shallow dip also for the longi tudinal tungsten surface phonon at the same incommensurate wave vector along <(Gamma)over bar>(H) over bar. The frequency always stays above the RW. The deep dip, which has recently been interpreted as due to e lectron-hole pair excitations, has not been detected up to now with EE LS at all accessible scattering conditions. At the wave vector of the anomalies along <(Gamma)over bar>(H) over bar we observed a small peak in the elastic diffuse intensity. For the ordered p(2 x 1) phase thre e H modes are resolved (550, 770, and 1250 cm(-1)); at least two of th em are dipole active. The ordered (2 x 2) phase shows six sharp H mode s. The linewidth of the modes depends on the order of the overlayer, t he coverage, and the adsorbate isotope. The (triply coordinated) hollo w site could be determined as the adsorption site starting from low co verages up to about 0.75 ML. The H modes of the (1 x 1 ) phase show an anomalous behavior: they create in specular a continuum and a single sharp loss in the EELS spectra. Additional structures in the frequency range of the continuum develop with increasing coverage and decreasin g temperature.