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

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${}_5$.

arXiv comment9 pages, 8 figures, accepted for publication in Phys. Rev. B

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