Abstract: In this paper, we will review the recent developments of high-power continuous-wave (CW) Er-Yb codoped fi-ber amplifiers (EYDFAs). Several related patents and a couple of methods of improving the performance of high-power EYDFAs are reviewed. Current research results show that the Yb-band amplified spontaneous emission (Yb-ASE) is the main reason that limits the efficiency and stability of an EYDFA at high pump power. Several methods and experimental results dedicated to suppress the Yb-ASE are introduced. Current and potential future developments of high-power EYD-FAs are summarized in the last part of this paper. Keywords: Erbium, fiber amplifiers, fiber lasers, MOPA, ytterbium 1. INTRODUCTION High-power fiber laser sources in the 1.5-μm band have made a great progress in recent years. Due to their many advantages, such as relatively eye-safe nature, low atmos-phere transmission loss, light weight, low loss in communi-cation fibers, and readily available reliable and cost-effective fiber communication components, they are of great potential for both military and civilian applications, such as laser in-frared radars (LIDARs), free-space communications, mate-rial processing and so on [1-3]. To flexibly control the linewidth, wavelength, and beam quality of a high-power fiber laser source, a master-oscillator power-amplifier (MOPA) configuration is commonly used. In this configuration, the master-oscillator generates a low-power high beam quality seed, and then the seed is amplified through several stages of power-amplifier until the desired output power is achieved. Apparently, the available power and performance of a MOPA system is largely determined by the performance of the power-amplifier(s). The details of the MOPA configuration will be introduced in the next sec-tion. In the 1.5-μm band high-power MOPAs, double-clad erbium-ytterbium codoped fibers (EYDFs) are usually used as the gain media of the power-amplifier. This fiber has an inner cladding surrounding the core and its refractive index is lower than the core but larger than the outer cladding [4]. The cross-sectional shape of the inner cladding is usually non-circular, which can enhance the mode mixing to pro-mote the pump absorption [5].
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