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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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Gomes, Laércio
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (5/5 displayed)
- 2014Spectroscopy of mid-infrared (2.9 μm) fluorescence and energy transfer in Dy3+-doped tellurite glassescitations
- 2012Numerical modeling of holmium-doped fluoride fiber laserscitations
- 2012Energy transfer and energy level decay processes in Tm 3-doped tellurite glasscitations
- 2011Energy level decay and excited state absorption processes in erbium-doped tellurite glasscitations
- 2011Energy level decay processes in Ho3-doped tellurite glass relevant to the 3 μm transitioncitations
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article
Energy transfer and energy level decay processes in Tm 3-doped tellurite glass
Abstract
<p>The primary excited state decay and energy transfer processes in singly Tm <sup>3</sup>-doped TeO <sub>2</sub>:ZnO:Bi <sub>2</sub>O <sub>3</sub>:GeO <sub>2</sub> (TZBG) glass relating to the <sup>3</sup>F <sub>4</sub> → <sup>3</sup>H <sub>6</sub> ∼1.85 m laser transition have been investigated in detail using time-resolved fluorescence spectroscopy. Selective laser excitation of the <sup>3</sup>H <sub>4</sub> manifold at 794 nm, the <sup>3</sup>H <sub>5</sub> manifold at 1220 nm, and <sup>3</sup>F <sub>4</sub> manifold at 1760 nm has established that the <sup>3</sup>H <sub>5</sub> manifold is entirely quenched by multiphonon relaxation in tellurite glass. The luminescence from the <sup>3</sup>H <sub>4</sub> manifold with an emission peak at 1465 nm suffers strong suppression due to cross relaxation that populates the <sup>3</sup>F <sub>4</sub> level with a near quadratic dependence on the Tm <sup>3</sup> concentration. The <sup>3</sup>F <sub>4</sub> lifetime becomes longer as the Tm <sup>3</sup> concentration increases due to energy migration and decreases to 2.92 ms when Tm <sup>3</sup> 4 mol. as a result of quasi-resonant energy transfer to free OH <sup>-</sup> radicals present in the glass at concentrations between 1 10 <sup>18</sup> cm <sup>-3</sup> and 2 10 <sup>18</sup> cm <sup>-3</sup>. Judd-Ofelt theory in conjunction with absorption measurements were used to obtain the radiative lifetimes and branching ratios of the energy levels located below 25 000 cm <sup>-1</sup>. The spectroscopic parameters, the cross relaxation and Tm <sup>3</sup>( <sup>3</sup>F <sub>4</sub>) → OH <sup>-</sup> energy transfer rates were used in a numerical model for laser transitions emitting at 2335 nm and 1865 nm.</p>