A‐site order in rhombohedral perovskite‐like oxides La2−xSrxCoTiO6 (0.6 ≤ x ≤ 1.0). (22nd January 2016)

• Record Type: Journal Article
• Authors: Gómez-Pérez, Alejandro; Ritter, Clemens; Boulahya, Khalid; Muñoz-Noval, Alvaro; García-Alvarado, Flaviano; Amador, Ulises
• Is Part Of: Journal of applied crystallography. Volume 49:Part 1(2016:Feb.)
• Page Start: 31
• Page End: 39
• Publication Date: 2016-01-22
• Subjects: perovskites -- phase transitions -- neutron diffraction -- synchrotron X‐ray diffraction -- AMPLIMODES -- cobaltite; Crystallography -- Periodicals; 548.05
• DOI: 10.1107/S1600576715022566
• Languages: English
• ISSNs: 0021-8898

Abstract

Abstract : Two composition‐driven phase transitions are observed in the series La2− x Sr x CoTiO6 (0.0 ≤ x ≤ 1.0), which can be discussed on the basis of the internal pressure associated with Sr doping using the symmetry‐adapted modes formalism. Abstract : The evolution of the room‐temperature structure of the oxide series La2− x Sr x CoTiO6 (0.6 ≤ x ≤ 1.0) was studied as a function of the Sr content using different diffraction techniques and applying the symmetry‐adapted modes formalism ( AMPLIMODES ). The title compounds adopt perovskite‐like structures of rhombohedral symmetry with an octahedral tilting scheme ( a − a − a − ) with either space group or R 32. The latter symmetry is observed in those cases (for x ≃ 0.6) where additional rock‐salt‐like ordering of La and Sr is produced in the perovskite A sites. Two composition‐driven phase transitions are observed in the whole series La2− x Sr x CoTiO6 (0.0 ≤ x ≤ 1.0). Using the concept of internal pressure, the effect of doping with Sr on the structure can be properly discussed. Both phase transitions seem to be of first order since they can be associated with discontinuities either in the entropy or in the structure. The first transition ( P 21 / n → Pnma ) occurs as the B cations become totally disordered. Along the whole compositional range the modes responsible for the out‐of‐phase tilting of B O6 octahedra remain active, but those associated with the in‐phase octahedral tilting vanish for x ≥ 0.6, this being associated with the second transition ( Pnma → ). Finally, for x = 1.0 the three pseudo‐cubic cell parameters become very similar, pointing to a transition to a cubic structure which could be obtained by applying pressure or raising the temperature.