We have developed a Watt-level single-frequency tunable fiber laser in the 915-937 nm spectral window. The laser is based on a neodymium-doped fiber master oscillator power amplifier architecture, with two amplification stages using a 20 mW extended cavity diode laser as seed. The system output power is higher than 2 W from 921 to 933 nm, with a stability better than 1.4% and a low relative intensity noise.Watt-level Single-Frequency (SF) lasers have been thoroughly investigated due to their widespread applications ranging from atom cooling [1], to coherent LIDAR [2], and laser spectroscopy [3], among others. However, to date there are still uncovered wavelength domains due to technological challenges, especially in the 900-940 nm window, as well as the corresponding frequency-doubled 450-470 nm spectral domain, for applications such as laser-cooling of atoms [4], high resolution 3D lithography [5], and underwater communications [6]. Recently, neodymium (Nd) doped fiber operating on the 4 F3/2-4 I9/2 transition have attracted high interest for the development of high-power lasers operating in the 900-940 nm spectral window. However, this type of lasers has only been demonstrated in longitudinal multimode operation, by using resonant cavity configurations combined with wavelength selection elements [7][8][9] or with photonic crystal fiber [10], in order to increase the gain at 910-940 nm and suppress the 1060 nm emission. In this Letter, we report for the first time to the best of our knowledge a Watt-level single-frequency all-fiber laser, tunable in the 915-937 nm window, with an output power in excess of 2 W from 921 to 933 nm.The Master Oscillator Power Amplifier (MOPA) Nd-doped fiber laser is composed of two amplification stages, a preamplifier and a booster amplifier (see Fig. 1), seeded by a low power (20mW) SF narrow linewidth (<100 kHz) Extended Cavity Diode Laser (ECDL, Toptica DL Pro 940). This double stage configuration is compatible with low-power sources (<5 mW), like fiber-based sources based on distributed Bragg reflector (DBR) lasers [11].The gain medium is based on a special designed Nd-doped double-clad fiber with core/cladding diameters of 5m/125 m, NA=0.12 and clad absorption of 0.8 dB/m at =808 nm (iXblue Photonics). Standard Nd-doped fibers usually present a very high gain on the 4 F3/2-4 I11/2 transition (near 1060 nm) due to its true four-level nature, which prevents laser operation near 900 nm. The fiber we adopted is designed with a W-type core refractive index profile in order to suppress the stimulated emission at 1060 nm by bending induced losses. Two Nd-fiber sections of 5m, coiled with a diameter of 6 cm, were used to implement the preamplifier and the booster amplifier. The preamplifier was pumped with a 4W laser diode at 808 nm via a multimode (MM) combiner. The booster amplifier was instead pumped with a 25 W pump laser diode at 808 nm through a high-power (HP) MM combiner. To avoid stray reflections and achieve stable operation of the amplification stages, three polarizatio...