We demonstrate continuous-wave dual-wavelength operation of a broad-area distributed feedback (DFB) laser diode with a single external-cavity configuration. This high-power DFB laser has a narrow bandwidth (<0.29 nm) and was used as a single-wavelength source. A volume Bragg grating was used as an output coupler for the external-cavity DFB laser to output another stable wavelength beam with a narrow bandwidth of 0.27 nm. A frequency difference for dual-wavelength operation of 0.88 THz was achieved and an output power of up to 415 mW was obtained. The external-cavity DFB laser showed a stable dual-wavelength operation over the practical current and temperature ranges.© 2018 The Japan Society of Applied Physics H igh-power broad-area laser diodes (LDs) are the most commonly used optical sources in a wide range of applications because of their compact size, high efficiency, and low cost. However, the spectral linewidths of Fabry-Perot LDs are typically in the 2-4 nm range, which is too wide for some of the more demanding LD applications, including solid-state laser pumping, 1,2) alkalivapor laser pumping, [3][4][5][6] and spin-exchange optical pumping. 7,8) Spectrum narrowing has been achieved in high-power LDs using both internal and external techniques. Externalcavity techniques using volume Bragg gratings (VBGs) [9][10][11][12] have been used to narrow the spectral linewidths of these LDs to the 0.014-0.4 nm range. In 2011, Vijayakumar et al. reported an output power of 5 W with a narrow linewidth of 0.2 nm from a VBG-coupled tapered LD bar.13) We have recently a reported reduction in the spectral bandwidth of spatial beam-combining high-power LD stacks to 0.31 nm, with a 581 W peak power output for quasicontinuous wave operation when using a single VBG.14) However, complete locking of the wavelength for continuous-wave broad-area LDs is difficult in the practical current and temperature ranges because of the wavelength thermal shift of high-power LDs. 1,9,12) Another potential linewidth reduction measure involves direct integration of a Bragg grating into the internal laser cavity. An output power of 1.1 W with a spectral width of 90 pm has been reported for continuous-wave 893 nm distributed feedback (DFB) lasers.15) In 2013, Garrod et al. reported high-efficiency 1 W output continuous-wave DFB lasers that operated at 1.4 µm with a linewidth of 0.5 nm, and the wavelength thermal shift of the DFB lasers (0.1 nm=°C) was much smaller than that of the broad-area LDs (0.45 nm=°C) in a temperature range of 10 to 30°C.16) Recently, we have reported a stable-spectrum DFB LD with a narrow linewidth of 33 pm that used a VBG.
17)Dual-wavelength lasers have also been rapidly developed for a wide variety of applications, including THz-wave generation, interferometry, and imaging systems. Dual-wavelength operation has also been achieved in LDs using external techniques. Dual-wavelength generation was reported with a maximum output power of 186 mW and a stable spectral separation of 0.62 THz from a quantum-dot-based medium t...