2017
DOI: 10.1364/optica.4.000235
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Diode-pumped mid-infrared fiber laser with 50% slope efficiency

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Cited by 89 publications
(21 citation statements)
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“…It had a reflectivity of ∼30% at 3.552 μm, a bandwidth of about 5 nm with similar loss values as compared to the high-reflective grating. Enabled by the ability to inscribe tailored FBGs into various erbiumdoped ZBLAN fibers, Aydin et al also demonstrated that the slope efficiency for emission at 2.8 μm can exceed the Stokes limit and can reach values of up to 50% if the two adjacent transitions of the erbium ion that correspond to emission at 2.8 μm and 1.6 μm, respectively, are cascaded [41]. To achieve this, the erbium fluoride fiber laser cavity consisted of a highly reflective input FBG with a reflectivity of ࣙ99.5% centered at 2.825 μm and Fresnel reflection on the opposite side was utilized to couple the mid-infrared light out.…”
Section: Phase Mask Techniquementioning
confidence: 99%
“…It had a reflectivity of ∼30% at 3.552 μm, a bandwidth of about 5 nm with similar loss values as compared to the high-reflective grating. Enabled by the ability to inscribe tailored FBGs into various erbiumdoped ZBLAN fibers, Aydin et al also demonstrated that the slope efficiency for emission at 2.8 μm can exceed the Stokes limit and can reach values of up to 50% if the two adjacent transitions of the erbium ion that correspond to emission at 2.8 μm and 1.6 μm, respectively, are cascaded [41]. To achieve this, the erbium fluoride fiber laser cavity consisted of a highly reflective input FBG with a reflectivity of ࣙ99.5% centered at 2.825 μm and Fresnel reflection on the opposite side was utilized to couple the mid-infrared light out.…”
Section: Phase Mask Techniquementioning
confidence: 99%
“…Owing to their compact structure, high conversion efficiency and robust operation, high-power fiber lasers have attracted much research interest and have been widely employed in many fields [1][2][3][4] . Rare-earth-doped fiber lasers, as a significant mainstay of high-power fiber lasers [5][6][7][8][9] , however, are challenged by waste heat accumulation in the active fiber [10] , especially with the power increasing beyond kilowatt level [11][12][13][14][15] . The quantum defect (QD) is one of the most important heat sources in the gain fiber, which could result in serious thermal effects on fiber lasers, such as the thermal lens effect, thermal mode instability and additional noise [16][17][18] .…”
Section: Introductionmentioning
confidence: 99%
“…In 2015, a 30-W Er 3+ -doped all-fiber laser operating at 2938 nm was demonstrated by using ZBLAN fiber Bragg gratings to form the all-fiber laser cavity and combining several high power laser diodes near 980 nm to provide a total pump power of 188 W [17]. The stokes limit has been exceeded in a 2.8 µm cascaded laser with 50% efficiency in 2017, which paves the way to 100-W-level mid-infrared fiber laser [18]. In 2018, a 2824 nm passive cooled Er 3+ -doped fluoride fiber approaches an average output power of 41.6 W, which is the highest output average power achieved with the mid-infrared fiber laser [19].…”
Section: Introductionmentioning
confidence: 99%