2012
DOI: 10.3788/col201210.101401
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Ytterbium-sensitized thulium-doped f iber laser with a single-mode output operating at 1 900-nm region

Abstract: A single-mode laser is demonstrated using a newly developed double-clad thulium-ytterbium-doped fiber (TYDF) in a linear cavity formed by two fiber Bragg gratings (FBGs). The YTF used is drawn from a D-shape preform fabricated using the modified chemical vapor deposition and solution doping technique. The laser is operated at 1 901.6 nm via the transition of thulium ions from 3 F4 to 3 H6 with the assistance of ytterbium to thulium ion energy transfer. The efficiencies of the laser are 0.71% and 0.75% at 927an… Show more

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Cited by 8 publications
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“…Generally, Tm 3+ -doped active media can be used for direct diode pumping at 785 nm and the quantum efficiency can reach 2 because two Tm ions are raised to the upper laser level by one absorbed pump photon [9]. However, as a quasithree level system, the laser emission near 1.9 µm is difficult to obtain because of the reabsorption effect of the Tm ions.…”
Section: Introductionmentioning
confidence: 99%
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“…Generally, Tm 3+ -doped active media can be used for direct diode pumping at 785 nm and the quantum efficiency can reach 2 because two Tm ions are raised to the upper laser level by one absorbed pump photon [9]. However, as a quasithree level system, the laser emission near 1.9 µm is difficult to obtain because of the reabsorption effect of the Tm ions.…”
Section: Introductionmentioning
confidence: 99%
“…However, as a quasithree level system, the laser emission near 1.9 µm is difficult to obtain because of the reabsorption effect of the Tm ions. Although many Tm 3+ -doped crystals (YAG, YAP, YLF and LLF) [10][11][12][13][14][15][16][17][18][19][20] were studied in the past (shown in table 1) and several of them have shown good laser performance, only the Tm:YLF crystal [9] achieves efficient laser operation with a center wavelength near 1.9 µm. Compared with oxide crystals, fluoride crystals are interesting because of their lowphonon energy reducing non-radiative relaxation and making them particularly suitable for infrared (IR) transitions, lower refractive index limiting non-linear effects, high transparency within a wide wavelength region from the vacuum ultraviolet to the IR and longer fluorescence lifetime for improving energy storage [21][22][23][24].…”
Section: Introductionmentioning
confidence: 99%