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Pump excited state absorption in holmium-doped fluoride glass

机译:掺fluoride氟化物玻璃的泵浦激发态吸收

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摘要

The primary excited state absorption processes relating to the ⁵I₆ → ⁵I₇ 3 μm laser transition in singly Ho³⁺-doped fluoride glass have been investigated in detail using time-resolved fluorescence spectroscopy. Selective laser excitation of the ⁵I₆ and ⁵I₇ energy levels established the occurrence of two excited state absorption transitions from these energy levels that compete with previously described energy transfer upconversion processes. The ⁵I₇ → ⁵I₄ excited state absorption transition has peak cross sections at 1216 nm (σesa =2.8x10⁻²¹ cm²), 1174 nm (σesa =1x10⁻²¹ cm²), and 1134 nm (σesa =7.4x10⁻²² cm²) which have a strong overlap with the ⁵I₈ → ⁵I₆ ground state absorption. On the other hand, it was established that the excited state absorption transition ⁵I₆ → ⁵S₂ had a weak overlap with ground state absorption. Using numerical solution of the rate equations, we show that Ho³⁺-doped fluoride fiber lasers employing pumping at 1100 nm rely on excited state absorption from the lowest excited state of Ho³⁺ to maintain a population inversion and that energy transfer upconversion processes compete detrimentally with the excited state absorption processes in concentrated Ho³⁺-doped fluoride glass.
机译:使用时间分辨荧光光谱法详细研究了单掺Ho 3+氟化物玻璃中与⁵I⁵→⁵I₇3μm激光跃迁有关的一次激发态吸收过程。 laserI₆和⁵I₇能级的选择性激光激发建立了从这些能级与先前描述的能量转移上转换过程竞争的两个激发态吸收跃迁的发生。 ₄I₇→⁵I₄激发态吸收跃迁的峰值横截面分别为1216 nm(σesa=2.8x10⁻cm·cm²),1174 nm(σesa=1x10⁻²¹cm cm)和1134 nm(σesa=7.4x10⁻²²cm cm)与⁵I₈→⁵I₆基态吸收强烈重叠。另一方面,可以确定,激发态吸收跃迁⁵I₆→⁵S2与基态吸收具有弱的重叠。使用速率方程的数值解,我们表明采用1100 nm抽运的掺Ho3 +氟化物光纤激光器依赖于Ho3⁺最低激发态的激发态吸收来维持粒子数反转,并且能量转移上转换过程与在掺Ho 3+的氟化物玻璃中的激发态吸收过程。

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