Abstract
We propose a new mechanism for the thermal Hall effect in exchange spin-wave systems, which is induced by the magnon-phonon interaction. Using symmetry arguments, we first show that this effect is quite general, and exists whenever the mirror symmetry in the direction of the magnetization is broken. We then demonstrate our result in a collinear ferromagnet on a square lattice, with perpendicular easy-axis anisotropy and Dzyaloshinskii-Moriya interaction from mirror symmetry breaking. We show that the thermal Hall conductivity is controlled by the resonant contribution from the anticrossing points between the magnon and phonon branches, and estimate its size to be comparable to that of the magnon-mediated thermal Hall effect.
Original language | English |
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Article number | 167202 |
Journal | Physical Review Letters |
Volume | 123 |
Issue number | 16 |
DOIs | |
State | Published - Oct 15 2019 |
Funding
We acknowledge useful discussions with Ran Cheng, Matthew W. Daniels, Tao Qin, and Junren Shi. Work at CMU is supported by the U.S. Department of Energy, Basic Energy Science, Pro-QM EFRC No. DE-SC0019443 (X. Z.) and No. DE-SC0012509 (Y. Z. and D. X.). S. O. acknowledges support by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences, and Engineering Division. D. X. also acknowledges support from a Research Corporation for Science Advancement Cottrell Scholar Grant.
Funders | Funder number |
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U.S. Department of Energy | |
Carnegie Mellon University | |
Division of Materials Sciences and Engineering | |
Basic Energy Sciences | |
Office of Science | |
Basic Energy Sciences | DE-SC0019443, DE-SC0012509 |