Abstract

Polar surfaces are known to be unstable due to the divergence of the surface electrostatic energy. Here we report on the experimental determination, by grazing incidence x-ray diffraction, of the surface structure of polar Ti-terminated (111) ${\mathrm{SrTiO}}_{3}$ single crystals. We find that the polar instability of the $1\ifmmode\times\else\texttimes\fi{}1$ surface is solved by a pure electronic reconstruction mechanism, which induces out-of-plane ionic displacements typical of the polar response of ${\mathrm{SrTiO}}_{3}$ layers to an electron confining potential. On the other hand, the surface instability can be also eliminated by a structural reconstruction driven by a change in the surface stoichiometry, which induces a variety of $3\ifmmode\times\else\texttimes\fi{}3$ (111) ${\mathrm{SrTiO}}_{3}$ surfaces consisting in an incomplete Ti (surface)--${\mathrm{O}}_{2}$ (subsurface) layer covering the $1\ifmmode\times\else\texttimes\fi{}1$ Ti-terminated (111) ${\mathrm{SrTiO}}_{3}$ truncated crystal. In both cases, the ${\mathrm{TiO}}_{6}$ octahedra are characterized by trigonal distortions affecting the structural and the electronic symmetry of several unit cells from the surface. These findings show that the stabilization of the polar (111) ${\mathrm{SrTiO}}_{3}$ surface can lead to the formation of quasi-two-dimensional electron systems characterized by radically different ground states which depend on the surface reconstructions.

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