I. Introduction
High power semiconductor lasers are the most efficient narrow-band light sources for the pumping of solid-state and fiber lasers. The constant demand for cost reduction in terms of dollar per Watt forced the development of laser bars and single emitters with higher output powers and maximum wall-plug efficiencies. The easiest approach to achieve this goal was an increase of the cavity length up to 6 mm. The accompanied loss of power conversion efficiency (PCE) was compensated by a lowered reflectivity of the antireflection (AR) coating on the outcoupling facet down to 1% for an operation even without volume Bragg gratings. This led to a significantly increased susceptibility of several electro-optical diode laser parameters to external optical feedback (EOF) including the risk of feedback induced accelerated gradual or sudden degradation and catastrophic optical (mirror) damage [CO(M)D] [1]–[2].