Phase diagram of LaTiO x : from 2D layered ferroelectric insulator to 3D weak ferromagnetic semiconductor

TLDR: In this article, a phase diagram is established which displays the following physical and structural properties of the LaTiO x compounds: a structural phase boundary atx=3.20 separates a new series of 2D layered structures from the 3D orthorhombic one, and a phase boundary exists between a metallic and a weak ferromagnetic state where the magnetic transition temperature can be sensitively tuned by the oxygen stoichiometry.

Abstract: LaTiO x compounds are structurally related to perovskites and there are two known phases. The first,x=3.50, is a 2D layered-type ferroelectric. The second,x=3.00, is a weak ferromagnet with a 3D orthorhombic distorted perovskite structure. 20 samples with varying oxygen stoichiometry between these end members were prepared by floating zone melting, and then characterized by means of X-ray powder diffraction, electron microscopy, thermogravimetric analysis, resistivity and magnetic measurement. A phase diagram is established which displays the following physical and structural properties. A structural phase boundary atx=3.20 separates a new series of 2D layered structures from the 3D orthorhombic one. The former series represents the first conducting titanium oxides with a 2D layered structure to be reported. Atx=3.10 a phase boundary exists between a metallic and a weak ferromagnetic state where the magnetic transition temperatureT c can be sensitively tuned by the oxygen stoichiometryx. Samples withT c between 100 K and 130 K exhibit a metal-semiconductor transition whereas samples with higherT c , up to 149 K, are semiconductors between room temperature and 4.2 K.