2004
DOI: 10.1063/1.1823577
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Downconversion and upconversion dynamics in Pr-doped Y3Al5O12 crystals

Abstract: We have investigated the spectroscopic properties of praseodymium ion in a Y3Al5O12 sample. We obtained the luminescence spectra by exciting selectively the sample at 460 and 599nm, resulting in the excitation of the P03 and D21 levels, respectively. With excitation in the P03 level we obtained emission from this level and from the D21 level. We used time resolved spectra and decay pattern inspection to assign spectral lines to specific radiative transitions. With excitation in the D21 level we observed lumine… Show more

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Cited by 39 publications
(13 citation statements)
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“…The values obtained from this analysis are plotted in Figure 4( decay time of 1 D 2 , which is much more strongly affected by complicated quenching processes than 1 P 0 , is about one order of magnitude shorter than for the corresponding single crystal. 18 This suggests, that radiative and nonradiative relaxation processes, due to surface effects and structural distortions present in the nanoparticles, 19 are generally much stronger for nanosized grains compared to the single crystals doped with the same Pr 3+ content. As it can be seen in Figure 4( relatively stronger with increasing pressure, compared to 3 P 0 → 3 H 4 .…”
Section: Resultsmentioning
confidence: 98%
“…The values obtained from this analysis are plotted in Figure 4( decay time of 1 D 2 , which is much more strongly affected by complicated quenching processes than 1 P 0 , is about one order of magnitude shorter than for the corresponding single crystal. 18 This suggests, that radiative and nonradiative relaxation processes, due to surface effects and structural distortions present in the nanoparticles, 19 are generally much stronger for nanosized grains compared to the single crystals doped with the same Pr 3+ content. As it can be seen in Figure 4( relatively stronger with increasing pressure, compared to 3 P 0 → 3 H 4 .…”
Section: Resultsmentioning
confidence: 98%
“…And the lifetime the 1 D 2 manifold is estimated to be 118.4 s by using = (B 1 1 2 + B 2 2 2 )/(B 1 1 + B 2 2 ) [29], which is much longer than that of 3 P 0 level. The experimental lifetime value of the 1 D 2 level can be compared to that of 1 mol%Pr:GGG nanocrystalline: 110s [25], 0.5% Pr 3+ :YAG: 110s [45] and of 1% Pr 3+ :YAP: 28s [43]. It is interesting to point that at 4 K the decay 1 D 2 → 3 H 4 profile of Pr:GGG is exponential with a lifetime of 260 s [23], as in contrast with the above results of this job.…”
Section: Fluorescence Lifetimes and Quantum Efficiencymentioning
confidence: 99%
“…1. No emission from 4f5d was detected, although it was expected as reported in [5,9]. As previously, the dynamics of 1 D 2 and upconverted 3 P 0 emission was recorded.…”
Section: Orange Excitationmentioning
confidence: 81%
“…Despite this, some processes taking place within Pr ions in YAG matrix are still unexplored or need clarification. This could explain the renewed interest in investigations of Pr:YAG optical properties [9,10]. Moreover, all the experimental data available up-to-now referred to relatively lightly doped, bulk materials.…”
Section: Introductionmentioning
confidence: 95%