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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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Taccardi, Nicola |
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Petrov, R. H. | Madrid |
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Azam, Siraj |
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Ali, M. A. |
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Rančić, M. |
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Azevedo, Nuno Monteiro |
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Oermann, Michael
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article
Energy level decay and excited state absorption processes in erbium-doped tellurite glass
Abstract
<p>The fundamental excited state decay processes relating to the <sup>4</sup>I<sub>11/2</sub> → <sup>4</sup>I<sub>13/2</sub> transition in singly Er<sup>3+</sup>-doped tellurite (TZNL) glass have been investigated in detail using time-resolved fluorescence spectroscopy. Selective laser excitation of the <sup>4</sup>I<sub>11/2</sub> energy level at 970 nm and selective laser excitation of the <sup>4</sup>I<sub>13/2</sub> energy level at 1485 nm has established that energy transfer upconversion by way of a dipole-dipole interaction between two excited erbium ions in the <sup>4</sup>I<sub>13/2</sub> level populates the <sup>4</sup>I<sub>11/2</sub> upper laser level of the 3 m transition. This upconversion has been analyzed for Er<sub>2</sub>O<sub>3</sub> concentrations between 0.5 mol. and 2.2 mol. . The <sup>4</sup>I<sub>13/2</sub> and <sup>4</sup>I<sub>11/2</sub> energy levels emit luminescence with peaks located at 1532 nm and 2734 nm, respectively, with radiative decay efficiencies of 65 and 6.8 for the higher (2.2 mol. ) concentration sample. The low 2.7 m emission efficiency is due to the non-radiative decay bridging the <sup>4</sup>I<sub>11/2</sub> → <sup>4</sup>I<sub>13/2</sub> transition and energy transfer to the OH<sup>-</sup> groups in the glass. Excited state absorption was observed to occur from the <sup>4</sup>I<sub>13/2</sub> and <sup>4</sup>I<sub>11/2</sub> levels with peak absorptions occurring at 1550 nm and 971 nm, respectively. The decay time of the <sup>4</sup>I<sub>11/2</sub> excited state decreased with an increase in the Er<sup>3+</sup> concentration, which related to energy transfer to OH<sup>-</sup> ions that had a measured concentration of 6.6 10<sup>18</sup> cm<sup>-3</sup>. Results from numerical simulations showed that a population inversion is reached at a threshold pumping intensity of ∼80 kW cm<sup>-2</sup> for a cw laser pump at 976 nm if [Er<sup>3+</sup>] ≥ 1.2 × 10<sup>21</sup> cm<sup>-3</sup> (or [Er <sub>2</sub>O<sub>3</sub>] ≥ 2.65 mol. ) without OH<sup>-</sup> impurities being present.</p>