Abstract

In this work, X-ray diffraction data taken on Bi 1− x La x FeO 3 solid solutions are used to verify the following structural phase transitions: “polar rhombohedral–antipolar orthorhombic” at x ≈ 0.16 and “commensurate–incommensurate” within the orthorhombic phase at x ≈ 0.18 . In contrast, in the Bi 1− x Pr x FeO 3 series, the polar rhombohedral phase transforms into an antipolar orthorhombic one at x ≥ 0.13 . The polar rhombohedral phase near the morphotropic phase boundary exhibits an isothermal transformation into an antipolar orthorhombic phase, though the transformation occurs much faster in the case of La-doped compounds. The incommensurate structural phase was not detected in Bi 1− x Pr x FeO 3 solid solutions. The ternary structural phase diagram is constructed for (Bi,La,Pr)FeO 3 systems. In addition, the polar rhombohedral phase exhibits a magnetic field-induced transition from the modulated antiferromagnetic state into a homogeneous weak ferromagnetic state whereas the antipolar phase is a weak ferromagnetic state in the absence of an external field.

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