2018
DOI: 10.1364/ol.43.004312
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Laser performance of a 966  nm LD side-pumped Er,Pr:GYSGG laser crystal operated at 279  μm

Abstract: We demonstrate a 966 nm laser diode (LD) side-pumped Er,Pr:GYSGG laser crystal operated at 2.79 μm under a high repetition rate. The lifetimes of the upper level I4 and lower level I4 are 0.66 and 0.85 ms, respectively. The laser performance under different repetition rates and pulse widths is experimentally studied with the optimal cavity structure. A maximum output power of 8.86 W is achieved at 125 Hz and 200 μs pulse widths, corresponding to the slope efficiency of 14.8% and electrical-to-optical efficienc… Show more

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Cited by 21 publications
(12 citation statements)
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“…8. The beam quality factor M 2 is calculated from the following equation: 26 where ω is the beam waist diameter, Θ is the far-field divergence, and λ is the laser wavelength. The laser beam quality M 2 factors in the x and y directions are fitted to be 7.04 and 7.12.…”
Section: Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…8. The beam quality factor M 2 is calculated from the following equation: 26 where ω is the beam waist diameter, Θ is the far-field divergence, and λ is the laser wavelength. The laser beam quality M 2 factors in the x and y directions are fitted to be 7.04 and 7.12.…”
Section: Resultsmentioning
confidence: 99%
“…Thus, more pump power may be consumed to compensate for these losses. 26 The longer duration of a single pump pulse is beneficial to the accumulation of upper particles. However, in the highfrequency pump mode, the longer pulse width corresponds to the higher duty cycle, and more waste heat is accumulated in the crystal rod, resulting in the increase of the thermal lensing effect and limiting the enhancement of output power.…”
Section: Crystengcommmentioning
confidence: 99%
See 1 more Smart Citation
“…Recently, Zhao et al adopted the diode side-pumping scheme to pump Er,Pr:GYSGG, and realized a maximum output power of 8.66 W with a slope efficiency of 14.8% at a repetition rate of 125 Hz and pulse width of 200 µs. These impressive results indicate that Er,Pr:GYSGG crystals have great potential in high-power 2.79 µm laser generation by deactivation and LD side-pumping [48]. successfully grew high-quality Er,Pr:GYSGG crystals with the Czochralski method [9].…”
Section: Laser Performance Of Erpr:gysgg Using Cr 3+ As the Deactivatormentioning
confidence: 93%
“…By far, various Er 3+ -doped gain materials had been reported, such as the garnet (crystals and ceramics) YAG [5], GGG [6], LuGG [7], YGG [8], YSGG [9][10][11][12], GSGG [13,14], the sesquioxide (crystals and ceramics) Y 2 O 3 [15,16], Lu 2 O 3 [17], and the fluoride (crystals, ceramics, and fibers) CaF 2 [18,19], SrF 2 [20], LiYF 4 [21], ZBLAN [22]. However, the fluorescence lifetime of the upper laser level 4 I 11/2 is much shorter than that of the lower laser level 4 I 13/2 , which is considered to be self-terminating, making the population inversion difficult and impeding laser oscillations.…”
Section: Introductionmentioning
confidence: 99%