Elastic softness of low-symmetry frustrated $A$Ti$_2$O$_5$ ($A$ = Co, Fe)

TL;DR

This study investigates the elastic properties of low-symmetry frustrated $A$Ti$_2$O$_5$ compounds, revealing unusual elastic softness in CoTi$_2$O$_5$ above its magnetic transition, indicating complex spin-lattice interactions.

Contribution

It uncovers the presence of magnetostructural fluctuations and differing spin-lattice coupling strengths in CoTi$_2$O$_5$ and FeTi$_2$O$_5$, highlighting their unique frustrated magnetic systems.

Findings

CoTi$_2$O$_5$ shows elastic softness above $T_N$ in $ac$-plane shear mode.

FeTi$_2$O$_5$ exhibits negligible elastic softness, indicating weaker spin-lattice coupling.

CoTi$_2$O$_5$ has stronger three-dimensional spin-lattice coupling than FeTi$_2$O$_5$.

Abstract

Orthorhombic pseudobrookites CoTi$_2$O$_5$ and FeTi$_2$O$_5$ have a low-symmetry crystal structure comprising magnetic Co$^{2+}$/Fe$^{2+}$ ions and nonmagnetic Ti$^{4+}$ ions, where the orbital-nondegenerate Co$^{2+}$/Fe$^{2+}$ ions form one-dimensional chains running along the orthorhombic $a$ axis. These compounds undergo an antiferromagnetic phase transition at $T_N \sim$ 26 K for CoTi$_2$O$_5$ and $T_N \sim$ 40 K for FeTi$_2$O$_5$. Ultrasound velocity measurements on single crystals of CoTi$_2$O$_5$ and FeTi$_2$O$_5$ reveal that CoTi$_2$O$_5$ exhibits unusual elastic softness above $T_N$ in the symmetry-lowering elastic mode of $ac$-plane shear elastic modulus, inconsistent with the structural symmetry breaking caused by antiferromagnetic ordering at $T_N$. This suggests the presence of two distinct types of magnetostructural fluctuations above $T_N$ that should be a precursor to the symmetry-lowering lattice distortion at $T_N$. In contrast, FeTi$_2$O$_5$ exhibits either negligible or smaller elastic softness, indicating weaker spin-lattice coupling. These findings highlight CoTi$_2$O$_5$ and FeTi$_2$O$_5$ as unique spin-latticed-coupled frustrated systems with low crystal symmetry, where, while the exchange interactions are quasi-one-dimensional in nature, the frustration is released by further lowering the crystal symmetry through three-dimensional spin-lattice coupling, which is stronger in CoTi$_2$O$_5$ than in FeTi$_2$O$_5$.