Thermal Transport Properties of Ho<sub>2</sub>RhIn<sub>8</sub>
ORAL
Abstract
The arrangement of the rare-earth atoms in the tetragonal structure of R2TX8 (R = rare earth, T = transition metal, X = In, Ga) takes a quasi two dimensional (2D) character. All of these compounds order antiferromagnetically with Neel temperatures (TN) ranging between 4 – 45 K. Ho2RhIn8 is one of the most interesting compounds among this very large family of closely related materials.
It shows two successive metamagnetic transitions at 2 K, when an external magnetic field is applied along the c axis. Its magnetic properties are driven mainly by crystalline electric effects and the RKKY interactions. We have grown single crystals of Ho2RhIn8 and have studied these metamagnetic transitions through thermal and electrical transport properties. These transitions are absent in the Hall resistivity but they appear around the same fields in the thermal conductivity, thermal Hall conductivity, and the longitudinal electrical resistivity. We discuss these metamagnetic transitions and their relations to the possibility of the Ho2RhIn8 compound being a magnetic topological candidate.
It shows two successive metamagnetic transitions at 2 K, when an external magnetic field is applied along the c axis. Its magnetic properties are driven mainly by crystalline electric effects and the RKKY interactions. We have grown single crystals of Ho2RhIn8 and have studied these metamagnetic transitions through thermal and electrical transport properties. These transitions are absent in the Hall resistivity but they appear around the same fields in the thermal conductivity, thermal Hall conductivity, and the longitudinal electrical resistivity. We discuss these metamagnetic transitions and their relations to the possibility of the Ho2RhIn8 compound being a magnetic topological candidate.
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Presenters
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Shirin Mozaffari
University of Tennessee
Authors
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Shirin Mozaffari
University of Tennessee
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Eun Sang Choi
National High Magnetic Field Laboratory, National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA, National High Magnetic Field Laboratory and Department of Physics, Florida State University
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David G Mandrus
University of Tennessee, Department of Materials Science and Engineering, University of Tennessee, Knoxville, TN, 37916, USA