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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Boetti, Nadia
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Publications (4/4 displayed)
- 2017Highly Doped Phosphate Glass Fibers for Compact Lasers and Amplifiers: A Reviewcitations
- 2017Effect of Partial Crystallization on the Structural and Luminescence Properties of Er3$-Doped Phosphate Glassescitations
- 2017Hollow resorbable fiber for combined light and drug delivery: fiber development and analysis of release kinetics
- 2011Energy level decay processes in Ho3-doped tellurite glass relevant to the 3 μm transitioncitations
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article
Energy level decay processes in Ho3-doped tellurite glass relevant to the 3 μm transition
Abstract
<p>The primary excited state decay processes relating to the<sup>5</sup>I<sub>6</sub>→<sup>5</sup>I<sub>7</sub>∼ 2.9 m laser transition in singly Ho<sup>3</sup>-doped tellurite (TZBG) glass have been investigated in detail using time-resolved fluorescence spectroscopy. Selective laser excitation of the<sup>5</sup>I<sub>6</sub>energy level at 1151 nm and<sup>5</sup>I<sub>7</sub>energy level at 1958 nm has established that the rate of energy transfer up-conversion between holmium ions excited to the<sup>5</sup>I<sub>7</sub>level is negligible for Ho<sup>3</sup>concentrations up to 4 mol. Excited state absorption was not observed from either the<sup>5</sup>I<sub>7</sub>or<sup>5</sup>I<sub>6</sub>levels and the luminescence from the<sup>5</sup>I<sub>7</sub>and<sup>5</sup>I<sub>6</sub>energy levels was measured to peak at ∼2050 nm and ∼2930 nm, respectively. The<sup>5</sup>I<sub>6</sub>level has a low luminescence efficiency of ∼8.9 due to strong nonradiative multiphonon relaxation. In contrast, decay from the<sup>5</sup>I<sub>7</sub>level is essentially fully radiative. A linear decrease in the decay time of the<sup>5</sup>I<sub>6</sub>level with Ho<sup>3</sup>concentration augmentation results from energy transfer to OH<sup>-</sup>ions in the glass (with N<sub>OH</sub>∼ 8.2 10<sup>17</sup>ions cm<sup>-3</sup>) and reduces the luminescence efficiency of the<sup>5</sup>I<sub>6</sub>level to 8 for [Ho<sup>3</sup>] 4 mol. Numerical simulation of a fiber laser incorporating 4 mol. Ho<sup>3</sup>showed that a population inversion of ∼7.8 is reached for square pulses of 100 s duration and a repetition frequency of 20 Hz at a moderate pump intensity of 418 kW cm<sup>-2</sup>if energy transfer to OH<sup>-</sup>radicals is neglected.</p>