Doped manganite perovskites AMnO3 exhibit a rich variety of electronic properties, resulting from the interplay of charge (Mn3+/Mn4+), spin (Mn magnetic moment) and orbital (Mn3+ Jahn–Teller distortion) degrees of freedom. Magnetisation measurements and ESR spectra have been used to study a series of eight AMnO3 perovskites, in which the A cation sites are occupied by a distribution of 70% trivalent lanthanide and 30% divalent Ca, Sr or Ba ions. These all have a mean A cation radius of 1.20 Å but different values of the cation size variance σ2. A change from orbital disorder to order (cooperative Jahn–Teller distortions) was previously found in the insulating regime at σ2
≈ 0.005 Å2. This work has shown that co-existence of the orbitally ordered and disordered phases is found in σ2
= 0.0016–0.0040 Å2 samples, with a difference of 40 K between their Curie temperatures. This is ascribed to competition between orbital ordering and microstructural lattice strains. At larger σ2 > 0.005 Å2, the orbital ordering strains are dominant and only this phase is observed. This intermediate temperature phase segregation is one of many strain-driven separation phenomena in manganites.
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