Correlated electronic structure and optical response of rare-earth based semiconductors
BIERMANN, Silke
Centre de Physique Théorique [CPHT]
Skane University Hospital [Lund]
European Theoretical Spectroscopy Facility
Collège de France - Chaire Physique de la matière condensée (A. Georges)
Centre de Physique Théorique [CPHT]
Skane University Hospital [Lund]
European Theoretical Spectroscopy Facility
Collège de France - Chaire Physique de la matière condensée (A. Georges)
POUROVSKII, Leonid
Centre de Physique Théorique [CPHT]
Collège de France - Chaire Physique de la matière condensée (A. Georges)
< Réduire
Centre de Physique Théorique [CPHT]
Collège de France - Chaire Physique de la matière condensée (A. Georges)
Langue
en
Article de revue
Ce document a été publié dans
Physical Review B. 2021-06-09, vol. 103, n° 24, p. L241105 (6 p.)
American Physical Society
Résumé en anglais
The coexistence of Mott localized f states with wide conduction and valence bands in f-electron semiconductors results, quite generically, in a complex optical response with the nature of the absorption edge difficult to ...Lire la suite >
The coexistence of Mott localized f states with wide conduction and valence bands in f-electron semiconductors results, quite generically, in a complex optical response with the nature of the absorption edge difficult to resolve both experimentally and theoretically. Here, we combine a dynamical mean-field theory approach to localized 4f shells with an improved description of band gaps by a semilocal exchange-correlation potential to calculate the optical properties of the light rare-earth fluorosulfides LnSF (Ln=Pr, Nd, Sm, Gd) from first principles. In agreement with experiment, we find the absorption edge in SmSF to stem from S−3p to Sm−4f transitions, while the Gd compound behaves as an ordinary p−d gap semiconductor. In the unexplored PrSF and NdSF systems we predict a rather unique occurrence of strongly hybridized 4f−5d states at the bottom of the conduction band. The nature of the absorption edge results in a characteristic anisotropy of the optical conductivity in each system, which may be used as a fingerprint of the relative energetic positions of different states.< Réduire
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