1983
DOI: 10.1103/physrevb.27.6635
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Optical transitions ofEr3+ions in fluorozirconate glass

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Cited by 577 publications
(198 citation statements)
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“…8, a change in the relative intensity of the 530 nm ( 2 Hn/2 -^-4 Iis/2) and 550 nm ( 4 S3/2 -^-4 Iis/2 ) bands can be observed. These effects have been previously observed in a variety of host materials and attributed to a poor thermal contact between the nanoparticles, which favors a local temperature increase during optical excitation [29][30][31]. Since the energy gap between both emitting multiplets is relatively low (around 800 cm _1 ), they are thermally coupled at ordinary temperatures following a Boltzmann distribution.…”
Section: J ^7/2mentioning
confidence: 98%
“…8, a change in the relative intensity of the 530 nm ( 2 Hn/2 -^-4 Iis/2) and 550 nm ( 4 S3/2 -^-4 Iis/2 ) bands can be observed. These effects have been previously observed in a variety of host materials and attributed to a poor thermal contact between the nanoparticles, which favors a local temperature increase during optical excitation [29][30][31]. Since the energy gap between both emitting multiplets is relatively low (around 800 cm _1 ), they are thermally coupled at ordinary temperatures following a Boltzmann distribution.…”
Section: J ^7/2mentioning
confidence: 98%
“…We have used value S = 0.1, which is in accordance with experimental values obtained for Er ions fluorozirconate glasses. 30 The influence of the value of Huang-Rhys parameter is shortly discussed in Ref. 31.…”
Section: ͑8͒mentioning
confidence: 99%
“…24), and fluoride glass (80 C) (Ref. 25). Since~T has been frequently used as a rough estimate of the glass formation ability or glass stability against crystallization, a large~T is beneficial to the fiber drawing.…”
Section: Resultsmentioning
confidence: 99%