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Spin resolved electron density study of YTiO(3) in its ferromagnetic phase: signature of orbital ordering

The present work reports on the charge and spin density modelling of YTiO(3) in its ferromagnetic state (T (C) = 27 K). Accurate polarized neutron diffraction and high-resolution X-ray diffraction (XRD) experiments were carried out on a single crystal at the ORPHÉE reactor (LLB) and SPRING8 synchrot...

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Detalles Bibliográficos
Autores principales: Voufack, Ariste Bolivard, Kibalin, Iurii, Yan, Zeyin, Claiser, Nicolas, Gueddida, Saber, Gillon, Béatrice, Porcher, Florence, Gukasov, Arsen, Sugimoto, Kunishisa, Lecomte, Claude, Dahaoui, Slimane, Gillet, Jean-Michel, Souhassou, Mohamed
Formato: Online Artículo Texto
Lenguaje:English
Publicado: International Union of Crystallography 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6760435/
https://www.ncbi.nlm.nih.gov/pubmed/31576221
http://dx.doi.org/10.1107/S2052252519009230
Descripción
Sumario:The present work reports on the charge and spin density modelling of YTiO(3) in its ferromagnetic state (T (C) = 27 K). Accurate polarized neutron diffraction and high-resolution X-ray diffraction (XRD) experiments were carried out on a single crystal at the ORPHÉE reactor (LLB) and SPRING8 synchrotron source. The experimental data are modelled by the spin resolved pseudo-atomic multipolar model (Deutsch et al., 2012 ▸). The refinement strategy is discussed and the result of this electron density modelling is compared with that from XRD measured at 100 K and with density functional theory calculations. The results show that the spin and charge densities around the Ti atom have lobes directed away from the O atoms, confirming the filling of the t (2g) orbitals of the Ti atom. The d (xy) orbital is less populated than d (xz) and d (yz), which is a sign of a partial lift of degeneracy of the t (2g) orbitals. This study confirms the orbital ordering at low temperature (20 K), which is already present in the paramagnetic state above the ferromagnetic transition (100 K).