2005
DOI: 10.1016/j.jcrysgro.2004.10.077
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Highly Yb-doped oxides for thin-disc lasers

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Cited by 124 publications
(65 citation statements)
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“…In the model, a value for the emission and absorption cross-sections was utilized that employed the values reported in the literature for KGd(WO 4 at other pump powers were investigated. A fraction of incident signal light remains uncoupled during the measurements, being neither amplified nor attenuated.…”
Section: Discussionmentioning
confidence: 99%
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“…In the model, a value for the emission and absorption cross-sections was utilized that employed the values reported in the literature for KGd(WO 4 at other pump powers were investigated. A fraction of incident signal light remains uncoupled during the measurements, being neither amplified nor attenuated.…”
Section: Discussionmentioning
confidence: 99%
“…The long excited-state lifetime of RE ions, typically in the millisecond range, permits amplification without distortion of high-rate signals. The large inter-atomic distance of ~0.5 nm permits high RE dopant concentration without significant lifetime quenching [4]. Finally, these host materials provide very high absorption and emission cross-sections to the RE ions doped into them [5].…”
Section: Introduction (Heading 1)mentioning
confidence: 99%
“…The radiation trapping effect, which is also known as reabsorption effect, is illustrated in Figure 4 In the absence of strong lifetime quenching effect, as in the case of KRE(WO4)2:Yb 3+ [83], a higher concentration of active ions in the material increases the occurrence of the reabsorption process and leads to the observation of longer measured lifetimes [92]. Contrarily, with the presence of strong quenching, the lifetime initially increases with the increasing active ions concentration, after which it sharply decreases with the further increase of active ion concentration [27,83] [126]. This approach requires extensive sample preparation which is destructive in nature.…”
Section: Radiation Trappingmentioning
confidence: 99%
“…Besides, the total population within each manifold will be distributed among the Stark levels. Assuming that rapid thermalisation takes place within the manifold, the fractional population at the i-th Stark level within the lower state can be deduced with the Boltzmann distribution 0 0 0 0 Similarly, the fractional population at the j-th Stark level within the upper state can be calculated using Therefore, it is often assumed that the measured luminescent lifetime represents the radiative lifetime τrad [82,83]. There are, however, a number of experimental results [77] indicating that small amount of non-radiative relaxation may occur in Yb 3+ -doped media.…”
Section: Lifetime and Effective Cross-sectionsmentioning
confidence: 99%
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