1991
DOI: 10.1117/12.46043
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<title>Spectroscopic properties of Er3+-doped glasses for the realization of active waveguides by ion-exchange technique</title>

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Cited by 4 publications
(3 citation statements)
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“…where hn p is the pump photon energy, s a and s e are the absorption and emission cross sections at 1.48 mm, 17 and I p is the pump intensity, which is estimated by use of an average mode diameter of ϳ10 mm. 13 Note that the stimulated emission term R # n 2 of pump light has to be included because the pump laser spectrum partly overlaps with the 4 I 13/2 !…”
Section: Cooperative Upconversion a Results And Analysismentioning
confidence: 99%
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“…where hn p is the pump photon energy, s a and s e are the absorption and emission cross sections at 1.48 mm, 17 and I p is the pump intensity, which is estimated by use of an average mode diameter of ϳ10 mm. 13 Note that the stimulated emission term R # n 2 of pump light has to be included because the pump laser spectrum partly overlaps with the 4 I 13/2 !…”
Section: Cooperative Upconversion a Results And Analysismentioning
confidence: 99%
“…Cross sections for absorption and emission at pump and signal wavelengths were taken from Ref. 17, and a typical value of 1.0 dB͞cm was assumed for the intrinsic waveguide loss. 9 Excited-state absorption was neglected.…”
Section: Optical Amplification a Results And Analysismentioning
confidence: 99%
“…These results show that phosphorous is not the best material to be used to improve the spectroscopic properties of the silica/titania matrix, as for erbium doping level as small as 0.25 mole%, the lifetime in an Er doped silicate glass should be between 5 and 10 ms [8]. The low fluorescence lifetime can be also explained by non-radiative deexcitations due to high phonon energy corresponding to the P---O bond.…”
Section: Erbium Doped Planar Waveguidesmentioning
confidence: 91%