Monolithically integrated multimode interference coupler-based master oscillator power amplifier with dual-wavelength emission around 830 nm

• Published in: Journal of physics communications 2024-04, Vol.8 (4), p.45002
• Main Authors: Müller, André, Koester, Jan-Philipp, Theurer, Lara Sophie, Fricke, Jörg, Wenzel, Hans, Knigge, Andrea, Sumpf, Bernd
• Format: Article
• Language: English
• Subjects: distributed Bragg reflector; dual-wavelength; master oscillator power amplifier; multimode interference; ridge waveguide
• ISSN: 2399-6528; 2399-6528
• DOI: 10.1088/2399-6528/ad37ef

A monolithically integrated dual-wavelength multimode interference coupler-based master oscillator power amplifier is presented. It consists of two shallowly etched, laterally separated ridge waveguide laser cavities as master oscillators with individual distributed Bragg reflector gratings as cavity mirrors. A deeply etched coupling section containing S-bend shaped waveguides and a multimode interference coupler is used to couple the laser emission of the master oscillators into a shallowly etched single waveguide serving as power amplifier. Changing the etch depth for the coupling section enables a compact device layout. In addition, increased radiation angles of modes not coupled into the power amplifier help to suppress beam steering, otherwise indicated by laterally separated far-field intensity distributions. The device provides 0.5 W of dual-wavelength emission around 830 nm in individual and common operation. As designed, both emission wavelengths are separated by 0.5 nm with spectral widths below 20 pm, limited by the spectral resolution of the spectrometer. Both peak wavelengths remain within spectral windows of 50 pm within the available power range. This enables full flexibility selecting operating points for applications such as shifted excitation Raman difference spectroscopy and the generation of THz emission by photomixing. The emission wavelengths can additionally be non-continuously tuned by applying a heater current to resistors implemented next to the distributed Bragg reflector gratings. As an example, selected spectral distances of 0.5 nm, 1.0 nm, 1.5 nm, and 2.0 nm are demonstrated. Near field widths of 5 μ m and far field angles of 17° result in beam propagation ratios of 1.4 (1/e 2 ) in all operation modes and enable easy beam shaping or optical single-mode fiber coupling.