Abstract

Wavelengths around 1.15 &#956;m, 1.3 &#956;m and 1.7 &#956;m can be used to pump Dy-doped ZBLAN fibre in order to generate ~3 &#956;m with high efficiency. Previously the generation of 2.9 &#956;m from the Dy-ZBLAN fibre was demonstrated by pumping with 1.1 &#956;m Yb-silica fibre laser sources. The laser slope efficiency and lasing threshold demonstrated was about ~5% and ~1.78 W. In this investigation, the longer wavelength absorption band (<sup>6</sup>H<sub>9/2</sub> , <sup>6</sup>F<sub>11/2</sub>) centred at 1.3 &#956;m of Dy<sup>3+</sup>-doped ZBLAN is utilised and the lasing transition around ~3 &#956;m takes places from <sup>6</sup>H<sub>13/2</sub> &#8594; <sup>6</sup>H<sub>15/2</sub>. With this pumping scheme the Stokes' efficiency is expected to be up to ~45%. A quasi-continuous wave Dy<sup>3+</sup>-ZBLAN fibre laser pumped by a ~1.3 &#956;m Nd:YAG laser and operating at 2.96 &#956;m with a bandwidth (FWHM) of ~14 nm has been demonstrated. For a 60cm fibre length, a threshold of 0.5W and a slope efficiency of ~20% with respect to the absorbed pump power was observed. The overall pump absorption in the fibre was around 84%. The cavity reflectivities at 2.9 &#956;m were 99% and 50%. The demonstrated slope efficiency was 45% of the Stokes' limit. The slope efficiency was around four times higher and the threshold around 3.6 times lower than the previous performance demonstrated by using the 1.1 &#956;m Yb fibre laser pumping scheme. The higher performance achieved compared to the 1.1 &#956;m pump scheme is due to the higher Stokes' limit, lower pump ESA losses and higher cavity reflectivity. About 590 cm<sup>-1</sup> Raman Stokes shift has also detected by using 514.5 nm and 488 nm Ar ion laser as excitation pump sources.

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