The potential for power scaling and wavelength scalability of semiconductor disk lasers (SDLs) makes them attractive for high-power single-frequency operation with numerous applications. In particular, single-frequency operation at 1.55 μm has been demonstrated with a monolithically grown InP-based SDL with 170 mW of output power at room temperature [1].The performance of monolithically grown InP-based SDLs, however, suffers from the low quality of distributed Bragg reflectors (DBRs), because the available compounds lattice-matched to InP offer low of refractive index contrast and poor thermal conductivity. This matter has been settled using wafer fusion that allows the integration of InP-based active regions with high quality GaAs-based DBRs. Consequently, multiwatt output powers in the wavelength range 1.3-1.6 μm have been demonstrated [2,3]. In the present work, we demonstrate a wafer-fused single-frequency SDL emitting at 1.56 μm with watt-level output power. The result represents the highest output power obtained from a single-frequency SDL at this wavelength range.The thermal management of the gain chip was achieved by capillary bonding it onto a 300 μm thick intracavity diamond heat spreader. The optical pumping was performed with a 980 nm fiber-coupled diode laser that was focused onto a spot with a diameter of 300 μm at the gain element. The arm lengths of the laser Vcavity were 12 cm and 20 cm. Two fused silica etalons with thicknesses of 500 μm and 750 μm were inserted into the cavity to facilitate the single frequency operation.The output power for a single-frequency regime as a function of pump power is shown in Fig. 1(a). The single-frequency operation was validated using a scanning Fabry-Perot interferometer (FPI) with a free spectral range of 1.5 GHz. The observed linewidth of 18 MHz was instrument resolution limited. The spectral linewidth was further studied using a delayed self-heterodyne interferometer (DSHI) with a 25 μs delay and 100 MHz acousto-optic modulator [4]. The DSHI output shown in Fig. 1(b) reveals 40 kHz oscillations in the wings of the signal. These oscillations correspond to the inverse of the DSHI delay time and indicate that the coherence length of the laser is longer than the 5 km DSHI fiber delay line [5]. Fig. 1(b) also shows a Lorentzian fit to the experimental signal, neglecting the central peak [5]. Fig. 1 (a): The output power for single-frequency operation as a function of pump power. The output beam and the spectrum of the laser are shown in the inset. (b): The DSHI signal at 600 mW of output power. Lorentzian fit is shown in red.