Breathing Pyrochlore Lattice Realized in the A-Site Ordered Spinel Oxides LiGaCr$_{4}$O$_{8}$ and LiInCr$_{4}$O$_{8}$
COFFEE_KLATCH · Invited
Abstract
A Cr spinel oxide ACr$_{2}$O$_{4}$ with a nonmagnetic A$^{2+}$ ion at the tetrahedral site provides an interesting playground for studying magnetic frustration in a pyrochlore lattice made of Cr$^{3+}$ ions with an $S =$ 3/2 spin. We found a novel type of frustrated lattice called ``breathing'' pyrochlore lattice, which is made of Cr$^{3+}$ ions in two A-site ordered spinel oxides, LiGaCr$_{4}$O$_{8}$ and LiInCr$_{4}$O$_{8}$ [1]. Because of the large size mismatch between Li$^{+}$ and Ga$^{3+}$/In$^{3+}$ ions, they alternately occupy the tetrahedral sites so as to form a Zinc Blende lattice. This transforms the conventional pyrochlore lattice into an alternating array of small and large tetrahedra, while keeping their shapes regular. LiGaCr$_{4}$O$_{8}$, with a lesser degree of alternation, shows similar magnetic properties to the conventional Cr spinel oxides such as ZnCr$_{2}$O$_{4}$. In contrast, LiInCr$_{4}$O$_{8}$ shows a spin-gap behavior in its magnetic susceptibility caused by a large alternation of magnetic interaction in the more breathing pyrochlore lattice. This suggests that LiInCr$_{4}$O$_{8}$ exists in a proximity to an exotic singlet ground state based on a tetramer singlet formed in the smaller tetrahedron, although it finally goes to a magnetically ordered state below 13 K, which may be triggered by a structural transition. We will also present NMR and neutron scattering measurements carried out to elucidate the nature of these compounds, and our recent results on solid solutions between the two compounds.\\[4pt]The work has been done in collaboration with T. Nakazono, Z. Hiroi, Y. Tanaka, M. Yoshida, M. Takigawa, T. Masuda (ISSP, Univ. of Tokyo), G. J. Nilsen, H. Mutka, T. Hansen (ILL), and J. P. Attfield (Univ. of Edinburgh). \\[4pt] [1] Y. Okamoto, G. J. Nilsen, J. P. Attfield, and Z. Hiroi, Phys. Rev. Lett. 110, 097203 (2013).
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Authors
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Yoshihiko Okamoto
Institute for Solid State Physics, University of Tokyo