Extensive first-principles calculations of the H-Be interaction reveal that novel H-surface vacancy structures dominate the high-coverage regime, from 2/3 to 1 monolayer (ML). At 1 ML the low-energy structure is a honeycomb of Be vacancies each decorated by three bridge-bonded H's tilting inward. At 2/3 ML the H's tilt in toward linear trenches organized in a 3×{}1 structure. At low coverages H prefers ordinary hcp threefold sites. A combination of the three structural models explains most of the experimental results. The adsorption of H in subsurface sites is shown to be unlikely.
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Stumpf et al. (1995) studied this question.
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