The c(6×2) is a reconstruction of the SrTiO3(001) surface that is formed between 1050 and 1100 °C in oxidizing annealing conditions. This work proposes a model for the atomic structure for the c(6×2) obtained through a combination of results from transmission electron diffraction, surface x-ray diffraction, direct methods analysis, computational combinational screening, and density functional theory. As it is formed at high temperatures, the surface is complex and can be described as a short-range-ordered phase featuring microscopic domains composed of four main structural motifs. Additionally, nonperiodic TiO2 units are present on the surface. Simulated scanning tunneling microscopy images based on the electronic structure calculations are...
SrTiO3(111) samples, doped with Nb, are Ar+ ion sputtered and annealed in ultrahigh vacuum (UHV) and...
An extensive surface characterization of hydrofluoric acid (HF) etched and annealed SrTiO3 single cr...
AbstractControlling the surface structure on the atomic scale is a major difficulty for most transit...
The c(6x2) is a reconstruction of the SrTiO3(001) surface that is formed between 1050 and 1100 degre...
SrTi03 is a metal oxide with a perovskite structure which can support numerous surface reconstructio...
This contribution presents a study of the atomic and electronic structure of the (√5×√5)R26.6° surfa...
The structure of SrTiO3 (100) (STO) single crystal surfaces has been investigated by grazing inciden...
The structure of SrTiO3 (100) (STO) single crystal surfaces has been investigated by grazing inciden...
Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)The atomic surface structure of SrTiO3(...
The structure of SrTiO3 (100) (STO) single crystal surfaces has been investigated by grazing inciden...
s131d and s231d reconstructions of the (001) SrTiO3 surface were studied using the first-principles ...
Using the B3PW hybrid exchange-correlation functional within density-functional theory and employing...
Using the B3PW hybrid exchange-correlation functional within density-functional theory and employing...
The atomic structures of two reconstructions, (√7 × √7)R19.1° and (√13 × √13)R13.9°, on the SrTiO3 (...
The atomic surface structure of single terminated SrTiO3(0 0 1) (1 × 1) is investigated employing su...
SrTiO3(111) samples, doped with Nb, are Ar+ ion sputtered and annealed in ultrahigh vacuum (UHV) and...
An extensive surface characterization of hydrofluoric acid (HF) etched and annealed SrTiO3 single cr...
AbstractControlling the surface structure on the atomic scale is a major difficulty for most transit...
The c(6x2) is a reconstruction of the SrTiO3(001) surface that is formed between 1050 and 1100 degre...
SrTi03 is a metal oxide with a perovskite structure which can support numerous surface reconstructio...
This contribution presents a study of the atomic and electronic structure of the (√5×√5)R26.6° surfa...
The structure of SrTiO3 (100) (STO) single crystal surfaces has been investigated by grazing inciden...
The structure of SrTiO3 (100) (STO) single crystal surfaces has been investigated by grazing inciden...
Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)The atomic surface structure of SrTiO3(...
The structure of SrTiO3 (100) (STO) single crystal surfaces has been investigated by grazing inciden...
s131d and s231d reconstructions of the (001) SrTiO3 surface were studied using the first-principles ...
Using the B3PW hybrid exchange-correlation functional within density-functional theory and employing...
Using the B3PW hybrid exchange-correlation functional within density-functional theory and employing...
The atomic structures of two reconstructions, (√7 × √7)R19.1° and (√13 × √13)R13.9°, on the SrTiO3 (...
The atomic surface structure of single terminated SrTiO3(0 0 1) (1 × 1) is investigated employing su...
SrTiO3(111) samples, doped with Nb, are Ar+ ion sputtered and annealed in ultrahigh vacuum (UHV) and...
An extensive surface characterization of hydrofluoric acid (HF) etched and annealed SrTiO3 single cr...
AbstractControlling the surface structure on the atomic scale is a major difficulty for most transit...