Institution: | aInstitute of Low Temperature and Structure Research, Polish Academy of Sciences, PL-50 422 Wrocław, Poland bDepartment of Physics, Technical University of Denmark, DK-2800 Lyngby, Denmark cNiels Bohr Institute, Oersted Laboratory, University of Copenhagen, DK-2100 Copenhagen, Denmark dInstitute of Physics, Wrocław University of Technology, Wybrzeże Wyspiańskiego 27, PL 50-370 Wrocław, Poland eDepartment of Chemistry, Aarhus University, DK-8000 Aarhus C, Denmark fc/o DESY/HASYLAB, D-22603 Hamburg, Germany |
Abstract: | The temperature evolution of the lattice parameters measured from 295 to 125 K exhibits a small instability below Tc≈278 K, indicating ferroelastic properties of Na2TiGeO5. The behavior is related to the specific crystal structure built of polyhedral layers with shared TiO5 pyramids and GeO4 tetrahedra, alternating with layers of Na+ cations. Antiparallel alignment of the short apical titanyl bond in adjacent rows of the polyhedral layer gives rise to spontaneous strain, when a distortion of the TiO5 groups occurs. Single-crystal structures determined at room temperature and 120 K suggest that {1 1 0} domains, developing below Tc, entail a tetragonal-to-orthorhombic symmetry change. The mechanism is attributed to a shortening of the O–O distance between the polyhedral layers, and to minor shifts of the positions of the Ti atoms and the correlated oxygen atoms along the c-axis. The structure distortion, however, is too small to allow any unambiguous determination of the symmetry-breaking effects. The bulk modulus and its pressure derivative have been determined as B0=89(2) GPa and . A pressure-induced phase transformation takes place at Pc≈12.5 GPa, presumably to an orthorhombic structure. The pressure effect on the transition temperature is given by ΔTc/ΔP≈1.76 K/GPa. |