Atomic and electronic structures of ternary iron arsenides $A$Fe${}_2$As${}_2$(001) surfaces ($A$=Ba, Sr, or Ca)

By the first-principles electronic structure calculations, we find that energetically the most favorable cleaved $A$Fe${}_2$As${}_2$(001) surface ($A$=Ba, Sr, or Ca) is $A$-terminated with a $(\sqrt{2}\times \sqrt{2})R{45}^{\circ }$ or $(1\times 2)$ order. The $(1\times 2)$ ordered structure yields a $(1\times 2)$ dimerized STM image, in agreement with the experimental observation. The $A$ atoms are found to diffuse on the surface with a small energy barrier so that the cleaving process may destroy the $A$ atoms ordering. At the very low temperatures this may result in an As-terminated surface with the $A$ atoms in randomly assembling. The As-terminated BaFe${}_2$As${}_2$ surface in orthorhombic phase is $(\sqrt{2}\times \sqrt{2})R{45}^{\circ }$ buckled, giving rise to a switchable $(\sqrt{2}\times \sqrt{2})R{45}^{\circ }$ STM pattern upon varying the applied bias. No any reconstruction is found for the other As-terminated surfaces. There are surface states crossing or nearby the Fermi energy in the As-terminated and $(1\times 2)$ $A$-terminated surfaces. A unified physical picture is thus established to help understand the cleaved $A$Fe${}_2$As${}_2$(001) surfaces.