“…In addition, the coincidence with one of the atmospheric spectral transmission window from 3 to 4 µm, allows also interesting applications in remote sensing and free-space optical communications [2], [3]. Conventional single-frequency sources directly emitting in this spectral region are based on semiconductor lasers, such as intercascade quantum laser [4]- [6] and lead-salt lasers [7], [8], solid-state Cr-doped chalcogenide lasers [9], and non-linear parametric sources such as optical parametric oscillators (OPOs) [10], [11] and difference frequency generation (DFG) schemes between near-infrared laser sources [12], [13]. Each of these technologies has advantages and disadvantages: the compact and robust semiconductor lasers have reduced tunability ranges and poor beam spatial qualities, the broadly tunable and narrow emission linewidth OPOs require rather complex architectures, while the simplest DFG sources have low output powers requiring high-power singlefrequency pump lasers.…”