Superorders and terahertz acoustic modes in multiferroic BiFeO<sub>3</sub>/LaFeO<sub>3</sub> superlattices - Archive ouverte HAL
Article Dans Une Revue Applied Physics Reviews Année : 2024

Superorders and terahertz acoustic modes in multiferroic BiFeO3/LaFeO3 superlattices

N. Jaouen
  • Fonction : Auteur
P. Manuel
  • Fonction : Auteur

Résumé

Superlattices are materials created by the alternating growth of two chemically different materials. The direct consequence of creating a superlattice is the folding of the Brillouin zone, which gives rise to additional electronic bands and phonon modes. This phenomenon has been successfully exploited to achieve new transport and optical properties in semiconductor superlattices. Here, we show that multiferroic BiFeO3/LaFeO3 superlattices exhibit several structural orders parallel and perpendicular to the growth direction, not existing in individual bulk materials. Using transmission electron microscopy, x-ray diffraction, and first-principles calculations, we reveal in particular a new long-range order of tilted FeO6 octahedra, with a period along the growth direction about twice that of the chemical supercell, i.e., a superorder. The effect of this new structural order on the phonon dynamics is studied with ultrafast optical pump-probe experiments. While a folded-mode at 1.2 THz is attributed solely to the chemical modulation of the superlattice, the existence of another 0.7 THz mode seems to be explained only by a double Brillouin zone folding in agreement with the structural out-of-plane superorder. Our work shows that multiferroic BiFeO3/LaFeO3 superlattices can be used to tune the spectrum of coherent THz phonons, and potentially that of magnons or electromagnons.

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Dates et versions

hal-04747723 , version 1 (22-10-2024)

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R. Gu, R. Xu, Francesco Delodovici, B. Carcan, M. Khiari, et al.. Superorders and terahertz acoustic modes in multiferroic BiFeO3/LaFeO3 superlattices. Applied Physics Reviews, 2024, 11, pp.041415 (article number). ⟨10.1063/5.0203076⟩. ⟨hal-04747723⟩
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