Answers are grounded in this paper and cite their sources.
Tight-binding calculations of the surface-phonon dispersion curves for unreconstructed p(1×{}1) W(001) reveal a whole region of soft surface modes at the boundary of the surface Brillouin zone, caused by interactions with electronic surface states around EF. An interplay of Fermi-surface nesting features and real-space d-orbital interactions leads to the maximum instability of the M₅ phonons, the basis of the observed c(2×{}2) reconstruction patterns. For small H coverages the electronic surface states are not removed but modified, probably in such a way as to produce incommensurate reconstructions.
No takes yet. Share an insight, caveat, or question.
Wang et al. (1987) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: