Large Room Temperature Anomalous Transverse Thermoelectric Effect in Kagome Antiferromagnet YMn<sub>6</sub>Sn<sub>6</sub>

ORAL

Abstract

Kagome magnets possess several novel nontrivial topological features owing to the strong correlation between topology and magnetism that extends to their applications in the field of thermoelectricity. Conventional thermoelectric (TE) devices use the Seebeck effect to convert heat into electrical energy. In contrast, transverse thermoelectric devices based on the Nernst effect are attracting recent attention due to their unique transverse geometry, which uses a single material to eliminate the need for a multitude of electrical connections compared to conventional TE devices. Here, a large anomalous transverse thermoelectric effect of ≈2 µV K−1 at room temperature in a kagome antiferromagnet YMn6Sn6 single crystal is obtained. The obtained value is larger than that of state-of-the-art canted antiferromagnetic (AFM) materials and comparable with ferromagnetic systems. The large anomalous Nernst effect (ANE) can be attributed to the net Berry curvature near the Fermi level. Furthermore, the ANE of the AFM YMn6Sn6 exceeds the magnetization scaling relationship of conventional ferromagnets. The results clearly illustrate that AFM material YMn6Sn6 is an ideal topological material for room-temperature transverse thermoelectric applications.

*Alexander von Humboldt Foundation; Deutsche Forschungsgemeinschaft (DFG) under SFB1143; the European Research Council (ERC)

Publication: S. Roychowdhury, A. M. Ochs, S. N. Guin, K. Samanta, J. Noky, C. Shekhar, M. G Vergniory, J. E. Goldberger, C. Felser, Large Room Temperature Anomalous Transverse Thermoelectric Effect in Kagome Antiferromagnet YMn6Sn6, Adv. Mater., 2022, 34, 2201350.

Presenters

  • Subhajit Roychowdhury

    • Max Planck Institute for Chemical Physic
    • Max Planck Institute for Chemical Physics of Solids

Authors

  • Subhajit Roychowdhury

    • Max Planck Institute for Chemical Physic
    • Max Planck Institute for Chemical Physics of Solids
  • Andrew M Ochs

    • The Ohio State University
  • Satya N Guin

    • Max Planck Institute for Chemical Physics of Solids
  • Kartik Samanta

    • Max Planck Institute for Chemical Physics of Solids
    • Max Plank Institute for Chemical Physics of Solids
  • Jonathan Noky

    • Max Planck Institute for Chemical Physics of Solids
  • Chandra Shekhar

    • Max Planck Institute for Chemical Physics of Solids
  • Maia Garcia Vergniory

    • Max Planck Institute for Chemical Physics of Solids, Dresden, Germany
    • Donostia International Physics Center, P. Manuel de Lardizabal 4, 20018 Donostia-San Sebastian, Spain
    • Donostia International Physics Center and Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute for Chemical Physics of Solids
    • Max Planck Institute CPFS
    • Donostia International Physics Center
  • Joshua E Goldberger

    • The Ohio State University
    • Department of Chemistry, University of Ohio
  • Claudia Felser

    • Max Planck Institute for Chemical Physic
    • Max Planck Institute for Chemical Physics of Solids