Proportionality between the magnetic exchange energy and Néel temperature in pyrochlore ruthenates
ORAL
Abstract
Pyrochlore oxides provide a rich platform for exploring diverse states of matter due to the unique crystal structure and chemical versatility. They are one of the most widely known systems to inherently host magnetic frustrations, setting the ground for exotic quantum states and diverse magnetic structures. Specifically, pyrochlore ruthenates, a family of strongly correlated 4d materials, houses a wide range of interaction between orbital, spin, and lattice degrees of freedom. Rare earth pyrochlore ruthenates are generally known to be spin-1 Mott insulators that display antiferromagnetic ordering of Ru ions below the Néel temperature (TN), with TN strongly depending on the size of the rare earth ions. Also, they have a linear relation between rare earth ionic radii, lattice constant, Ru-O-Ru bond angle, bond length, and Ru 4d t2g bandwidth which is believed to be the origin of the systematic metal to insulator transition shown throughout these compounds.
In our study, a series of polycrystalline pyrochlore powder samples RE2Ru2O7 (RE= Y, Nd, Sm, Eu, Ho, and Er) was synthesized and temperature dependent Raman spectroscopy measurements were performed. Our results concisely show a linear correlation between the one-magnon excitation energy within range of 15 - 35 meV and TN of each compound, varying from TN = 80K - 150 K. This strongly suggests the system is predominantly dependent on the superexchange interaction. This indicates that we have found a family of compounds in which we can freely tune the magnon energy. Therefore, changing the A site components only tunes the magnetic exchange energies while everything else is the same.
In our study, a series of polycrystalline pyrochlore powder samples RE2Ru2O7 (RE= Y, Nd, Sm, Eu, Ho, and Er) was synthesized and temperature dependent Raman spectroscopy measurements were performed. Our results concisely show a linear correlation between the one-magnon excitation energy within range of 15 - 35 meV and TN of each compound, varying from TN = 80K - 150 K. This strongly suggests the system is predominantly dependent on the superexchange interaction. This indicates that we have found a family of compounds in which we can freely tune the magnon energy. Therefore, changing the A site components only tunes the magnetic exchange energies while everything else is the same.
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Presenters
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Jae Hyuck Lee
Seoul National University
Authors
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Jae Hyuck Lee
Seoul National University
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Dirk Wulferding
Department of Physics and Astronomy, Seoul National University
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Dongjoon Song
National Institute of Advanced Industrial Science and Technology, Department of Physics and Astronomy and Quantum Matter Institute, University of British Columbia
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Junkyoung Kim
Department of Physics, Incheon National University
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Seungryung Park
Department of Physics, Incheon National University
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Changyoung Kim
Seoul Natl Univ, Seoul National University, Department of Physics and Astronomy, Seoul National University, Center for Correlated Electron Systems, Institute for Basic Science (IBS), Seoul 08826, Republic of Korea, Seoul national university