Fig. 1: Ferroelectric and magnetic ground state of La substituted BiFeO3.
From: Non-volatile magnon transport in a single domain multiferroic

Effective Hamiltonian calculated (a) magnetic ground state energy of the spin cycloid and G-type antiferromagnetic phase in BiFeO3 and Bi0.85La0.15FeO3. R3c represents uniform, and M1 and M2 represent modulated polar configurations (“Methods”). A spin cycloid exists in the ground state of BiFeO3 whereas a complex mixed state becomes increasingly stable in Bi0.85La0.15FeO3 thin films due to the decreasing energy difference between the two magnetic configurations. Complex state (shaded area) is defined as the mixed state of the spin cycloid and G-type canted antiferromagnetic phase. The dotted lines represent the average energy of the two systems in the complex state configuration. b Schematic of the energy landscape of the BiFeO3 and Bi0.85La0.15FeO3 where the ground state of magnetic textures such as G-type antiferromagnet and spin cycloid phases in the two systems is described. Red arrows form the spin cycloid in the ground state of BiFeO3 with the ΔU energy barrier, whereas the complex state is formed in Bi0.85La0.15FeO3 due to the reduced energy barrier on La substitution. Green up/down arrows represent the polarization in the double well structure. c, d High angle annular dark field (HAADF) scanning transmission electron microscopy (STEM) images and polar vector mapping in BiFeO3 and Bi0.85La0.15FeO3. Insets are the schematics of the estimated polarization direction in the unit cell of BiFeO3 and Bi0.85La0.15FeO3. Colored arrows indicate the direction as well as the magnitude of the atomic displacement vector vis-à-vis polarization. The average polarization is no longer along [111] after La-substitution. The scale bar is 1 nm. e–h Ferroelectric domain (PFM) and corresponding magnetic texture (iso-B NV images) of BiFeO3/Bi0.85La0.15FeO3 in the pristine state. In (h), two types of contrast are visible: the stripe-like contrast from the spin cycloid phase, and the more uniform contrast from a canted antiferromagnetic (AFM) phase.