Abstract:We report a high power, single frequency, linearly polarized master oscillator power amplifier emitting 110 ns, 1 kW peak power pulses at 2050 nm. A 20% slope efficiency and a beam quality of M2=1.21 are achieved with three-stage double-clad Tm(3+)-doped fiber architecture. Various pump schemes are compared leading to the conclusion that 793 nm pump wavelength is the most efficient for amplification at 2050 nm. Based on numerical simulations, the Brillouin gain coefficient around 2 μm in Tm(3+) highly doped si… Show more
“…It is known that the central frequency of the lorentzian Brillouin gain curve can be shifted by applying strain to the fiber. Applying an optimal strain distribution for a given signal distribution in the fiber will result in a flat Brillouin spectrum and a larger threshold [6]. We have shown that a triangular distribution can be used.…”
Section: Preliminary Version Of the High Power Fiber Transmittermentioning
“…It is known that the central frequency of the lorentzian Brillouin gain curve can be shifted by applying strain to the fiber. Applying an optimal strain distribution for a given signal distribution in the fiber will result in a flat Brillouin spectrum and a larger threshold [6]. We have shown that a triangular distribution can be used.…”
Section: Preliminary Version Of the High Power Fiber Transmittermentioning
“…We developed a high power single-frequency laser source at 2050 nm using strain gradient to mitigate SBS [25]. The pumping scheme selected for the amplifier is clad pumping using 793 nm laser diodes.…”
Section: High Peak Power Narrow Linewidth Mopfa Emitting At 2050 Nmmentioning
confidence: 99%
“…The value of the Brillouin gain that we have discussed so far is the Brillouin gain value obtained for a homogenous fiber length L. Among the various methods used to increase the Brillouin threshold several are based on strain [15,25] or temperature [40][41][42] change along the fiber. The principle is to shift the Brillouin gain maximum along the fiber.…”
Section: Comparison Of Brillouin Propertiesmentioning
a b s t r a c tWe present design and performances of several eye-safe high peak power fiber lasers operating either around 1550 nm or 2000 nm. They share the limitations by nonlinear effects either Stimulated Brillouin Scattering for single frequency lasers or Kerr related effects for short pulse amplifiers. Performances above 1 kW peak power for single frequency lasers and 26 nJ for short pulse fiber lasers are reported. The influence of the saturation power of the fibers on the non-linearity is discussed and applied to a comparison between Erbium and Ytterbium co-doped fibers and Thulium doped fibers. The Brillouin gain properties in these fibers are also compared.
“…A careful comparison of experiment and theory is important both for basic research and systematic engineering design of Thulium fiber amplifiers operating in the 2 µm region. Applications include LIDAR or spectroscopy, such as CO2 atmospheric absorption at 2051.4 nm 1 . Currently the state of modeling for Tm-doped fiber (TDF) amplifiers is not nearly as advanced as the state of modeling for Erbium-doped fiber amplifiers [2][3][4][5] .…”
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