Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1811233 | Physica B: Condensed Matter | 2012 | 6 Pages |
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 O2pâTi3d transition in CaTiO3 host corresponds to the centered 330Â nm excitation spectra. The gap states above the valence band of â¼1.30Â eV and â¼2.06Â 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 614Â nm due to 1D2â3H4 transition of Pr3+ activator. The latter is related to the excitation spectra centered at 380Â nm due to the low-lying Pr-to-mental intervalence charge transfer transitions (Pr3+-O2â-Ti4+âPr4+-O2â-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
Authors
Ailing Zhu, Jianchuan Wang, Yong Du, Dongdong Zhao, Qiannan Gao,