Bulletin of the American Physical Society
2024 APS March Meeting
Monday–Friday, March 4–8, 2024; Minneapolis & Virtual
Session K03: Magnetic Topological Materials I
3:00 PM–6:00 PM,
Tuesday, March 5, 2024
Room: L100C
Sponsoring
Unit:
DMP
Chair: Weiwei Xie, Michigan State University
Abstract: K03.00004 : Weyl metallic state induced by helical magnetic order.*
4:24 PM–4:36 PM
Presenter:
Irián Sánchez Ramírez
(Donostia International Physics Center)
Authors:
Irián Sánchez Ramírez
(Donostia International Physics Center)
Jian-Rui Soh
(EPFL)
Xupeng Yang
(EPFL)
jinzhao sun
(University of Oxford)
Ivica Živković
(EPFL)
Alberto Rodríguez-Velamazán
(Institut Laue-Langevin)
Oscar Fabelo
(Institut Laue-Langevin)
Anne Stunault
(Institut Laue-Langevin)
Alessandro Bombardi
(Diamond)
Christian Balz
(Oak Ridge National Lab)
Manh Duc Le
(Science and Technology Facilities Council)
Helen C Walker
(Rutherford Appleton Lab)
J. Hugo Dil
(EPFL)
Dharmalingam Prabhakaran
(Oxford)
Henrik M. Rønnow
(EPFL)
Fernando De Juan
(Donostia International Physics Center)
Maia G Vergniory
(DIPC / MPI CPfS)
Andrew T Boothroyd
(Oxford)
In the rapidly expanding field of topological materials there is growing interest in systems whose topological electronic band features can be induced or controlled by magnetism. Magnetic Weyl semimetals, which contain linear band crossings near the Fermi level, are of particular interest owing to their exotic charge and spin transport properties. Up to now, the majority of magnetic Weyl semimetals have been realized in ferro or ferrimagnetically ordered compounds, but a disadvantage of these materials for practical use is their stray magnetic field which limits the minimum size of devices. Here we show that a Weyl state can be induced by a helical spin configuration, in which the magnetization is fully compensated. Using a combination of neutron diffraction and resonant elastic x-ray scattering, we find that below T_N = 14.5 K the Eu spins in EuCuAs develop a planar helical structure which induces two quadratic Weyl nodes with Chern numbers C = ± 2 at the A point in the Brillouin zone. In this talk we will cover maily the theoretical aspects of this project.
*D.P. and A.T.B. acknowledge support from the Oxford–ShanghaiTech collaboration project. This work was supported by the U.K. Engineering and Physical Sciences Research Council, grant no. EP/M020517/1. J.-R.S. acknowledges support from the Singapore National Sci- ence Scholarship, Agency for Science Technology and Re- search and the European Research Council (HERO, Grant No. 810451).
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