2013
DOI: 10.1088/1054-660x/23/9/095101
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A high average power single-stage picosecond double-clad fiber amplifier

et al.

Abstract: In this paper, we report 38.8 W average power output through a single-stage fiber amplifier, with emission of 1064 nm wavelength with 80 MHz repetition and 35 ps pulse width amplified from a 2.15 W SESAM passively mode-locked Nd:YVO 4 laser oscillator. The high power fiber amplification is through a coupled 60.8 W 976 nm backward unidirectional pump power into a 2 m long 30/250 µm Yb-doped inner cladding. No obvious nonlinear effects arise in the high power output. To our knowledge this is the highest average … Show more

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Cited by 4 publications
(4 citation statements)
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“…High energy and high peak power femtosecond pulses have numerous practically important applications [3]. In addition to the well-known applications of femtosecond lasers in areas such as nonlinear optics, metrology, and spectroscopy, the femtosecond lasers can also be an advanced tool for material processing or imaging [4,5].…”
Section: Introductionmentioning
confidence: 99%
“…High energy and high peak power femtosecond pulses have numerous practically important applications [3]. In addition to the well-known applications of femtosecond lasers in areas such as nonlinear optics, metrology, and spectroscopy, the femtosecond lasers can also be an advanced tool for material processing or imaging [4,5].…”
Section: Introductionmentioning
confidence: 99%
“…Double-clad rare-earth doped fiber structures were developed in order to overcome the limitations in the output power level imposed by the difficulty of pumping the doped core of single mode fiber structures [1][2][3]. After reaching significant power levels, in the level of tens of watts [1][2][3], nonlinear effects start to play a significant role.…”
Section: Introductionmentioning
confidence: 99%
“…Double-clad rare-earth doped fiber structures were developed in order to overcome the limitations in the output power level imposed by the difficulty of pumping the doped core of single mode fiber structures [1][2][3]. After reaching significant power levels, in the level of tens of watts [1][2][3], nonlinear effects start to play a significant role. Since the strength of the nonlinear effects depends inversely on the doped core area, additional scaling of the output power level required the design of large mode area (LMA) structures [4], which increases the threshold for the stimulated Raman scattering, for example, and allows increasing of the dopant concentration.…”
Section: Introductionmentioning
confidence: 99%
“…In our earlier work, Sun et al achieved 38.8 W average power output through a single-stage 2 m 30∕250 μm Ybdoped fiber (YDF) amplifier with 80 MHz repetition and 35 ps pulse width. 7 In 2015, we also utilized this scheme to achieve 85 W burst mode picosecond pulses based on a Q-switched and mode-locked laser with output energy of 0.5 mJ per burst pulse. 8 Thus, the picosecond-pulse fiber amplifier based on the CWML solid-state laser can be a highly efficient and appropriate candidate for delivering high average power, high peak power, narrow-linewidth picosecond pulses.…”
mentioning
confidence: 99%