Crystalline and magnetic structures, magnetization, heat capacity and anisotropic magnetostriction effect in a yttrium-chromium oxide
arXiv:2007.08985 · doi:10.1103/PhysRevMaterials.4.094409
Abstract
We have studied a nearly stoichiometric insulating YCrO single crystal by performing measurements of magnetization, heat capacity, and neutron diffraction. Albeit that the YCrO compound behaviors like a soft ferromagnet with a coersive force of 0.05 T, there exist strong antiferromagnetic (AFM) interactions between Cr spins due to a strongly negative paramagnetic Curie-Weiss temperature, i.e., -433.2(6) K. The coexistence of ferromagnetism and antiferromagnetism may indicate a canted AFM structure. The AFM phase transition occurs at 141.5(1) K, which increases to (5T) = 144.5(1) K at 5 T. Within the accuracy of the present neuron-diffraction studies, we determine a G-type AFM structure with a propagation vector \textbf{k} = (1 1 0) and Cr spin directions along the crystallographic \emph{c} axis of the orthorhombic structure with space group \emph{Pnma} below . At 12 K, the refined moment size is 2.45(6) , 82\% of the theoretical saturation value 3 . The Cr spin interactions are probably two-dimensional Ising like within the reciprocal (1 1 0) scattering plane. Below , the lattice configuration (\emph{a}, \emph{b}, \emph{c}, and \emph{V}) deviates largely downward from the Grneisen law, displaying an anisotropic magnetostriction effect and a magnetoelastic effect. Especially, the sample contraction upon cooling is enhanced below the AFM transition temperature. There is evidence to suggest that the actual crystalline symmetry of YCrO compound is probably lower than the currently assumed one. Additionally, we compared the YCrO and the LaSrMnO single crystals for a further understanding of the reason for the possible symmetry lowering.
13 pages, 13 figures
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