A pulsed master oscillator power amplifier system is constructed using a double-cladding polarized Ybdoped fiber and an all-fiber Q-switched narrow-linewidth pulsed laser used as seed laser. This system has a high repetition rate and provides a nanosecond pulsed laser with a narrow linewidth and linear polarization. Moreover, it generates amplified radiation with up to 14 W of average power, narrow linewidth (full-width at half-maximum is smaller than 0.12 nm), linear polarization at 1 080-nm wavelength, repetition rate of 51 kHz, and pulse duration of approximately 50 ns. Based on this pulsed amplified radiation, 3.5 W of green laser, with an optical-to-optical efficiency of 27.3%, is obtained via single-pass frequency doubling using a noncritical phase matching KTP crystal.OCIS High-power green lasers are applied in material processing, medical treatments, laser projection, and pumping optical parametric amplifiers [1] . Green lasers with more than 100 W have been produced from solid-state lasers. However, these lasers have beam quality of M 2 >10 [2] . Fiber lasers have drawn much attention because of their high beam quality, conversion efficiency, high stability, and high heat dissipation. High-powered, narrowlinewidth, and linearly polarized pulse lasers have been widely applied in laser radars, spectrography, and precision measurements [3−6] . Recently, with the emergence of the cladding pump, high-powered double-cladding fiber lasers and amplifiers have been rapidly developed. Therefore, because of the advantages in the volume, efficiency, and beam quality of Yb 3+ -doped fiber lasers, researchers tend to adopt narrow-linewidth fiber lasers to obtain a second-harmonic generation (SHG) output and thus realize miniature and highly efficient short-wave lasers [7−10] , particularly those from green sources. The application of narrow-linewidth fiber lasers, particularly those achieved via the frequency-doubling technique [11,12] , often has high laser polarization requirements. Currently, many research groups have studied linearly polarized pulsed fiber lasers [13−16] . However, considering that the peak power of the pulsed laser is several orders of magnitude higher than the output power of the continuous-wave laser, the pulsed laser is much easily affected by the nonlinear efficiency of stimulated Raman scattering (SRS) and stimulated Brillouin scattering (SBS), preventing the improvement of its output power [16,17] . Nevertheless, in fiber lasers, the frequency doubling of quasi-phase-matched ferroelectric materials is the most commonly used method. Aculight Company has employed a high-power 1 080-nm pulsed laser via using two LBO crystals to realize the average power of a green-source output of 60 W [18] with a conversion efficiency of 54.5%, the highest reported power achieved by green-source fiber lasers. As a frequency-doubling crystal, KTP has a higher nonlinear coefficient than LBO and a stronger damage threshold than PPKTP [19] . However, reports on green lasers produced from fiber laser using the...