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Successive Magnetic-Field-Induced Transitions and Colossal Magnetoelectric Effect in Ni_{3}TeO_{6}.
Kim, Jae Wook; Artyukhin, S; Mun, E D; Jaime, M; Harrison, N; Hansen, A; Yang, J J; Oh, Y S; Vanderbilt, D; Zapf, V S; Cheong, S-W.
Afiliação
  • Kim JW; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Artyukhin S; Rutgers Center for Emergent Materials and Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA.
  • Mun ED; IAMDN and Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA.
  • Jaime M; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Harrison N; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Hansen A; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Yang JJ; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
  • Oh YS; Rutgers Center for Emergent Materials and Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA.
  • Vanderbilt D; Rutgers Center for Emergent Materials and Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA.
  • Zapf VS; IAMDN and Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA.
  • Cheong SW; Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
Phys Rev Lett ; 115(13): 137201, 2015 Sep 25.
Article em En | MEDLINE | ID: mdl-26451580
ABSTRACT
We report the discovery of a metamagnetic phase transition in a polar antiferromagnet Ni_{3}TeO_{6} that occurs at 52 T. The new phase transition accompanies a colossal magnetoelectric effect, with a magnetic-field-induced polarization change of 0.3 µC/cm^{2}, a value that is 4 times larger than for the spin-flop transition at 9 T in the same material, and also comparable to the largest magnetically induced polarization changes observed to date. Via density-functional calculations we construct a full microscopic model that describes the data. We model the spin structures in all fields and clarify the physics behind the 52 T transition. The high-field transition involves a competition between multiple different exchange interactions which drives the polarization change through the exchange-striction mechanism. The resultant spin structure is rather counterintuitive and complex, thus providing new insights on design principles for materials with strong magnetoelectric coupling.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2015 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2015 Tipo de documento: Article