title: Crystal structures and phase transition in (Sr(0.8)Ce(0.2))(Mn(1-y)Co(y))O(3) (y = 0 and 0.2): the influence of Jahn-Teller distortion.
abstract: We have studied the crystal structures of (Sr(0.8)Ce(0.2))(Mn(1-y)Co(y))O(3) (y = 0 and 0.2) using neutron diffraction. Both (Sr(0.8)Ce(0.2))MnO(3) and (Sr(0.8)Ce(0.2))(Mn(0.8)Co(0.2))O(3) have a tetragonal structure in space group I4/mcm at room temperature, and the octahedral tilt angle around the c-axis is nearly the same. The only significant difference is the shape of the Mn(Co)O(6) octahedron: it is elongated in (Sr(0.8)Ce(0.2))MnO(3) due to the cooperative Jahn-Teller (JT) effect, but essentially regular in (Sr(0.8)Ce(0.2))(Mn(0.8)Co(0.2))O(3) due to the absence of JT-active Mn(3+) ions. With increasing temperature, both compounds undergo a continuous phase transition at around 400 °C to a cubic structure in [Formula: see text], with no indication of a distinct transition in (Sr(0.8)Ce(0.2))MnO(3) from the removal of the static JT distortion. In addition, the temperature dependence of the octahedral tilt angle is very similar in the two samples, implying that the JT distortion has minimal effect on the octahedral tilting and the phase transition to cubic. X-ray absorption near-edge structure (XANES) analysis indicates that the Ce oxidation state is predominantly 4+ in both samples. The electrical conductivity is higher in (Sr(0.8)Ce(0.2))MnO(3) than in (Sr(0.8)Ce(0.2))(Mn(0.8)Co(0.2))O(3) in the temperature range studied (100-900 °C).
authors.affiliation: Institute of Materials Engineering, Australian Nuclear Science and Technology Organisation, Lucas Heights, NSW 2234, Australia.
authors.forename: Zhaoming
authors.initials: Z
authors.lastname: Zhang
authors.forename: Christopher J
authors.initials: CJ
authors.lastname: Howard
authors.forename: Brendan J
authors.initials: BJ
authors.lastname: Kennedy
authors.forename: Motohide
authors.initials: M
authors.lastname: Matsuda
authors.forename: Michihiro
authors.initials: M
authors.lastname: Miyake