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Strong interband Faraday rotation in 3D topological insulator Bi(2)Se(3)

The Faraday effect is a representative magneto-optical phenomenon, resulting from the transfer of angular momentum between interacting light and matter in which time-reversal symmetry has been broken by an externally applied magnetic field. Here we report on the Faraday rotation induced in the promi...

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Detalles Bibliográficos
Autores principales: Ohnoutek, L., Hakl, M., Veis, M., Piot, B. A., Faugeras, C., Martinez, G., Yakushev, M. V., Martin, R. W., Drašar, Č., Materna, A., Strzelecka, G., Hruban, A., Potemski, M., Orlita, M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4707504/
https://www.ncbi.nlm.nih.gov/pubmed/26750455
http://dx.doi.org/10.1038/srep19087
Descripción
Sumario:The Faraday effect is a representative magneto-optical phenomenon, resulting from the transfer of angular momentum between interacting light and matter in which time-reversal symmetry has been broken by an externally applied magnetic field. Here we report on the Faraday rotation induced in the prominent 3D topological insulator Bi(2)Se(3) due to bulk interband excitations. The origin of this non-resonant effect, extraordinarily strong among other non-magnetic materials, is traced back to the specific Dirac-type Hamiltonian for Bi(2)Se(3), which implies that electrons and holes in this material closely resemble relativistic particles with a non-zero rest mass.