2019
DOI: 10.1016/j.apradiso.2019.108815
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Luminescent behavior of Eu3+ doped BaHfO3 perovskite ceramic under UV radiation

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Cited by 7 publications
(8 citation statements)
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“…Some authors have proposed theoretical models for the observed 5 D 0 → 7 F 0 transition, including the breakdown of the closure approximation in the Judd–Ofelt theory and third order perturbation theory [ 1 , 32 , 33 ]. The most obvious explanation assumes that this transition is due to J-mixing or to the mixing of low-lying charge-transfer states into the wave functions of the 4f 6 configuration.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Some authors have proposed theoretical models for the observed 5 D 0 → 7 F 0 transition, including the breakdown of the closure approximation in the Judd–Ofelt theory and third order perturbation theory [ 1 , 32 , 33 ]. The most obvious explanation assumes that this transition is due to J-mixing or to the mixing of low-lying charge-transfer states into the wave functions of the 4f 6 configuration.…”
Section: Resultsmentioning
confidence: 99%
“…Furthermore, even though the induced electric dipole (ED) 5 D 0 → 7 F 0 transition is strictly forbidden by the ΔJ selection rule of the Judd–Ofelt theory, there are reported occurrences of it as a well-known example of the breakdown of the selection rules of the Judd–Ofelt theory [ 1 ]. For example, Guzmán-Olguín et al showed an unusual great intensity of the 5 D 0 → 7 F 0 transition centered at 580 nm when they excited their Eu 3+ -doped BaHfO 3 perovskite ceramic under UV radiation with the wavelength associated with the charge transfer band (272 nm), while this transition was very weak when the sample was excited at 396 or 466 nm wavelengths [ 32 ]. One of the co-authors of this manuscript, Gupta, with his co-workers, reported the presence of two Stark components in the 5 D 0 → 7 F 0 transition from their Nd 2 Zr 2 O 7 :Eu phosphor when excited at 256 nm [ 33 ].…”
Section: Introductionmentioning
confidence: 99%
“…Perovskite structures in general have demonstrated excellent ability to host rare earth ions for light-emitting applications. Barium hafnium oxide (BHO) with the formula BaHfO 3 represents a very interesting class of nonpolar perovskite materials with superlative properties such as a large band gap ∼6 eV, high dielectric constant, low phonon frequency <700 cm –1 , high transparency in UV–visible region, which makes it an ideal host for rare earth-doped photoluminescence (PL). BHO also has very high density (8.5 g/cc) and high effective atomic number ( Z eff = 64.6), making it an ideal host for scintillators and X-ray phosphors . In fact, the BHO sample itself demonstrated broad RL at around 410 nm, which disappears on doping, though .…”
Section: Introductionmentioning
confidence: 99%
“…In one of the works, the authors have stabilized both Eu 3+ and Eu 2+ to produce white light emission . Guzman–Olguin also discussed about PL of BHOE under UV excitation but did not give any information on the role of defects, local dopant structure and host–dopant energy transfer efficacy . Drag–Jarzabek also explored PL of BHOE, but their work was more focused on designing the same using a single molecular precursor rather than photophysical aspects .…”
Section: Introductionmentioning
confidence: 99%
“…BaHfO 3 (BHO) is an interesting class of non‐polar perovskite materials with favorable properties including wide band gap∼ 6 eV, high dielectric constant, ability to accommodate large concentration of dopant ion at both A and B‐site, high radiation stability, low phonon energy (<700 cm −1 ), high UV‐visible transparency, and so forth. which makes it an ideal host lattice for actinide (An) and lanthanide (Ln) doping 16–18 …”
Section: Introductionmentioning
confidence: 99%