Article ID Journal Published Year Pages File Type
1811233 Physica B: Condensed Matter 2012 6 Pages PDF
Abstract
Microcosmic investigations of weak red-emitting materials are crucial for their further development and application. In this work, we have focused on the band structures and electronic properties of Pr mono- and (Zn, Pr) co-doped CaTiO3 using density functional theory. Zn substitution for Ca or Ti tends to form clusters energetically with Pr substituting for Ca in CaTiO3. In Pr mono-doped CaTiO3, the O2p→Ti3d transition in CaTiO3 host corresponds to the centered 330 nm excitation spectra. The gap states above the valence band of ∼1.30 eV and ∼2.06 eV are hybridized by Pr4f, O2p and Ti3d orbitals. They are mainly due to Pr4f orbitals in CaTiO3:Pr. The former gap level is related to red emission at 614 nm due to 1D2→3H4 transition of Pr3+ activator. The latter is related to the excitation spectra centered at 380 nm due to the low-lying Pr-to-mental intervalence charge transfer transitions (Pr3+-O2−-Ti4+⇌Pr4+-O2−-Ti3+). The band structures of (Zn, Pr) co-doped CaTiO3 keep the similar gap levels to those in Pr mono-doped CaTiO3. The incorporation of Zn brings out the two stronger localized gap states, which are hybridized by Pr4f, O2p and Ti3d orbitals, in comparison with those in Pr mono-doped CaTiO3. Therefore, when Zn impurities are added into Pr doped CaTiO3, the present calculations visualize the two enhanced levels and the distorted structures around Pr.
Related Topics
Physical Sciences and Engineering Physics and Astronomy Condensed Matter Physics
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