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Sensitizing effect of Ho3+ on the Er3+: 2.7μm-emission in fluoride glass
•The fluorescence properties of 2.7μm emission and energy transfer mechanism are investigated.•The optimized concentration ratio of Er3+ to Ho3+ is found to be 1:1.•The sample possesses large emission cross section and radiative transition probability.•The energy transfer microparameters are calcula...
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Published in: | Optical materials 2014-03, Vol.36 (5), p.921-925 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | •The fluorescence properties of 2.7μm emission and energy transfer mechanism are investigated.•The optimized concentration ratio of Er3+ to Ho3+ is found to be 1:1.•The sample possesses large emission cross section and radiative transition probability.•The energy transfer microparameters are calculated and discussed.
The fluorescence properties of 2.7μm emission and energy transfer mechanism of Ho3+/Er3+ co-doped fluoride glass (ZBYA) have been investigated in the present paper. Ho3+ strengthens the Er3+: 2.7μm emission in the ZBYA glasses due to the energy transfer from Er3+ to Ho3+, while the 1.5μm emission decreases dramatically. The optimized concentration ratio of Er3+ to Ho3+ is found to be 1:1 in our glass system. The absorption and emission spectra are tested and the sample possesses large emission cross section (16.5×10−21cm2) around 2.7μm along with larger radiative transition probability (25.11S−1) on the basis of Judd–Ofelt and Fuchtbauer–Ladenburg theories. Additionally, the energy transfer microparameters are calculated using Förster–Dexter theory and the result shows the energy transfer coefficient of Er3+:4I13/2→Ho3+:5I7 is 24 times larger than that of Er3+:4I11/2→Ho3+:5I6. Our results show that Er3+: 2.7μm emission can be sensitized by Ho3+ efficiently, and this Er3+/Ho3+-codoped fluoride glasses might have potential application in mid-infrared lasers. |
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ISSN: | 0925-3467 1873-1252 |
DOI: | 10.1016/j.optmat.2013.12.031 |