Thermal Hall Effect of Spin Excitations in a Kagome Magnet

At low temperatures, the thermal conductivity of spin excitations in a magnetic insulator can exceed that of phonons. However, because they are charge neutral, the spin waves are not expected to display a thermal Hall effect. However, in the kagome lattice, theory predicts that the Berry curvature l...

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Bibliographic Details
Main Authors: Hirschberger, Max (Author), Chisnell, Robin (Contributor), Lee, Young S. (Contributor), Ong, N. P (Author)
Other Authors: Massachusetts Institute of Technology. Department of Physics (Contributor)
Format: Article
Language:English
Published: American Physical Society, 2015-09-08T12:54:14Z.
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Online Access:Get fulltext
LEADER 01634 am a22002293u 4500
001 98381
042 |a dc 
100 1 0 |a Hirschberger, Max  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Physics  |e contributor 
100 1 0 |a Chisnell, Robin  |e contributor 
100 1 0 |a Lee, Young S.  |e contributor 
700 1 0 |a Chisnell, Robin  |e author 
700 1 0 |a Lee, Young S.  |e author 
700 1 0 |a Ong, N. P.  |e author 
245 0 0 |a Thermal Hall Effect of Spin Excitations in a Kagome Magnet 
260 |b American Physical Society,   |c 2015-09-08T12:54:14Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/98381 
520 |a At low temperatures, the thermal conductivity of spin excitations in a magnetic insulator can exceed that of phonons. However, because they are charge neutral, the spin waves are not expected to display a thermal Hall effect. However, in the kagome lattice, theory predicts that the Berry curvature leads to a thermal Hall conductivity κ[subscript xy]. Here we report observation of a large κ[subscript xy] in the kagome magnet Cu(1-3, bdc) which orders magnetically at 1.8 K. The observed κ[subscript xy] undergoes a remarkable sign reversal with changes in temperature or magnetic field, associated with sign alternation of the Chern flux between magnon bands. The close correlation between κ[subscript xy] and κ[subscript xx] firmly precludes a phonon origin for the thermal Hall effect. 
520 |a National Science Foundation (U.S.). Materials Research Science and Engineering Centers (Program) (Grant DMR 1420541) 
546 |a en 
655 7 |a Article 
773 |t Physical Review Letters