AbstractThe atomic relaxations near the (111) 1 × 1 covalent semiconductor (C, Si, and Ge) surfaces are calculated using a tight‐binding Green's function approach and compared with the results of LEED experiments as well as those of other theoretical calculations. The present calculation takes into account the repulsive interaction energies between adjacent atomic sites and uses a total energy minimization procedure. It is shown that the change in the topmost interlayer spacing δ0 depends strongly on the material and subsurface relaxation is unimportant. The value of δ0 increases rapidly as going C(≈︁ 1%) → Si(≈︁ 5%) → Ge(≈︁ 13%). Simple physical interpretation for this behaviour is also given.
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