2014
DOI: 10.1016/j.ceramint.2014.01.063
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Optical influence of annealing in nano- and submicron-scale ZrO2 powders

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Cited by 29 publications
(23 citation statements)
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“…A prominent peak is observed at 499 nm and less intense peaks are observed at 533, 568, and 604 nm. There are two arguments given in the literature for the emission peak at 499 nm in ZrO 2 . , According to the first one, the emission peak at 499 nm is caused by electron transitions (e g → t 2g ) in impurity ions of titanium (Ti 3+ ). ,,, Another point of view is that the luminescence at 499 nm is caused by intrinsic defects that are related to oxygen vacancies. ,,, However, in the present work, the results of the EPR and EDX exclude the existence of Ti 3+ ions in the samples. Other emission peaks observed at 568 and 605 nm are the related surface trap defects …”
Section: Resultsmentioning
confidence: 55%
See 1 more Smart Citation
“…A prominent peak is observed at 499 nm and less intense peaks are observed at 533, 568, and 604 nm. There are two arguments given in the literature for the emission peak at 499 nm in ZrO 2 . , According to the first one, the emission peak at 499 nm is caused by electron transitions (e g → t 2g ) in impurity ions of titanium (Ti 3+ ). ,,, Another point of view is that the luminescence at 499 nm is caused by intrinsic defects that are related to oxygen vacancies. ,,, However, in the present work, the results of the EPR and EDX exclude the existence of Ti 3+ ions in the samples. Other emission peaks observed at 568 and 605 nm are the related surface trap defects …”
Section: Resultsmentioning
confidence: 55%
“…The XRD results of the ZrO 2 sample annealed at ≤500 °C show a tetragonal phase and it transforms into monoclinic when ZrO 2 was annealed at a higher temperature, that is, ≥1000 ο C. Meanwhile, the PL emission peak position changed with the crystalline phase of ZrO 2 . Typically, the synthesized ZrO 2 sample exhibits 5–10% of the tetragonal phase along with the monoclinic phase. According to the literature, a prominent PL peak appears in the range 390–425 nm for a pure tetragonal structure , with a lifetime decay smaller than 10 ns. ,, A PL peak is reported between 475 and 500 nm for monoclinic ZrO 2 , with a corresponding lifetime decay of up to a few μs (<20 μs). , As far as monoclinic ZrO 2 is concerned, the origin of the prominent emission band (expected in the range 475–500 nm) is still a matter of debate. Several reports attribute this band to the inherent presence of impurity titanium ions (Ti 3+ ) ,,, and this hypothesis is supported by density functional theory (DFT) calculations .…”
Section: Introductionmentioning
confidence: 97%
“…[ 79 ] However, emission of 2.6 eV also has been reported in m ‐ZrO 2 powders by Ashraf et al., proposing an origin to electronic transitions between the levels generated by the excited F +* and F + states. [ 85 ] Finally, the component of 2.3 eV could correspond with the emission of 2.2 eV for t ‐ZrO 2 nanoparticles reported by Zhang et al. They attribute it to the presence of carbon impurities (C i ), demonstrating that the emission is tuned in energy with the amount of carbon incorporated in such nanostructures.…”
Section: Resultsmentioning
confidence: 75%
“…The components calculated by the deconvolution of the CL spectra using Gaussian curves are centered at 1.65, 2.3, 2.6, 2.9, 3.2, and 3.5 eV for ZrO 2 annealed at 600 °C and centered at 2.3, 2.6, and 2.9 eV for ZrO 2 buckyballs annealed at 1200 °C, to match the energy of defects-related emissions reported by other authors. [79,[83][84][85][86] The full width at half maximum (FWHM) of these components is adjusted to obtain a fitting value for the coefficient of determination nearest to unity. The values obtained for this parameter are 0.995 and 0.997 after fitting the CL spectra of ZrO 2 buckyballs annealed at 600 and 1200 °C by assigning an FWHM of 0.35 eV to each Gaussian component.…”
Section: Additive Manufacturing Of T-zro 2 and M-zro 2 Microarchitect...mentioning
confidence: 99%
“…Moreover, another green-colored down-conversion emission is observed with a series of bands at 493, 510, 531, and 554 nm. This is ascribed to the electron transition from the excited state to the ground state of F þ centers located above the valence band due to the singly ionized oxygen-vacancy defects [48]. It was reported that the crystalline ZrO 2 with both monoclinic and tetragonal phases could create new color centers in the presence of the oxygen vacancies.…”
Section: Fluorescent Characteristicsmentioning
confidence: 99%