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Spin-Reorientation-Driven Linear Magnetoelectric Effect in Topological Antiferromagnet Cu_{3}TeO_{6}.
Kisicek, Virna; Dominko, Damir; Culo, Matija; Rapljenovic, Zeljko; Kuvezdic, Marko; Dragicevic, Martina; Berger, Helmuth; Rocquefelte, Xavier; Herak, Mirta; Ivek, Tomislav.
Afiliação
  • Kisicek V; Institute of Physics, Bijenicka cesta 46, 10 000 Zagreb, Croatia.
  • Dominko D; Faculty of Physics, University of Rijeka, Radmile Matejcic 2, 51 000 Rijeka, Croatia.
  • Culo M; Institute of Physics, Bijenicka cesta 46, 10 000 Zagreb, Croatia.
  • Rapljenovic Z; Institute of Physics, Bijenicka cesta 46, 10 000 Zagreb, Croatia.
  • Kuvezdic M; Institute of Physics, Bijenicka cesta 46, 10 000 Zagreb, Croatia.
  • Dragicevic M; Department of Physics, Faculty of Science, University of Zagreb, Bijenicka cesta 32, 10 000 Zagreb, Croatia.
  • Berger H; Institute of Physics, Bijenicka cesta 46, 10 000 Zagreb, Croatia.
  • Rocquefelte X; Institute of Physics, Ecole Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne, Switzerland.
  • Herak M; Univ Rennes, CNRS, ISCR (Institut des Sciences Chimiques de Rennes) UMR 6226, F-35000 Rennes, France.
  • Ivek T; Institute of Physics, Bijenicka cesta 46, 10 000 Zagreb, Croatia.
Phys Rev Lett ; 132(9): 096701, 2024 Mar 01.
Article em En | MEDLINE | ID: mdl-38489626
ABSTRACT
The search for new materials for energy-efficient electronic devices has gained unprecedented importance. Among the various classes of magnetic materials driving this search are antiferromagnets, magnetoelectrics, and systems with topological spin excitations. Cu_{3}TeO_{6} is a material that belongs to all three of these classes. Combining static electric polarization and magnetic torque measurements with phenomenological simulations we demonstrate that magnetic-field-induced spin reorientation needs to be taken into account to understand the linear magnetoelectric effect in Cu_{3}TeO_{6}. Our calculations reveal that the magnetic field pushes the system from the nonpolar ground state to the polar magnetic structures. However, nonpolar structures only weakly differing from the obtained polar ones exist due to the weak effect that the field-induced breaking of some symmetries has on the calculated structures. Among those symmetries is the PT (1[over ¯]^{'}) symmetry, preserved for Dirac points found in Cu_{3}TeO_{6}. Our findings establish Cu_{3}TeO_{6} as a promising playground to study the interplay of spintronics-related phenomena.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2024 Tipo de documento: Article País de afiliação: Croácia

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: Phys Rev Lett Ano de publicação: 2024 Tipo de documento: Article País de afiliação: Croácia