We report on room temperature operation of blue-green ZnSe-based electron-beam pumped semiconductor lasers grown by molecular beam epitaxy. The lowest ever reported values of threshold current density in transverse excitation geometry (3-3.5 A/cm 2 ), which is independent of the electron beam energy in the 15-35 kV range, have been obtained. Possible ways to improve the electron-beam pumped laser characteristics are discussed.Although important steps have been made towards realization of II-VI laser diodes, reliable long-living devices operating in cw mode at room temperature (RT) are not yet available. The main reasons of the "slow" degradation are assumed to be a metastable nature of N-acceptors [1] and electrical instability of N-related shallow donors [2]. The electron beam pumped lasers known for many years [3] are, in principle, beyond this problem, but their practical applications [4] are strongly restricted by both a relatively high threshold current density at RT and high voltages needed for laser generation.The first ZnSe-based electron beam pumped laser was demonstrated in 1967 [5]. The threshold current density J th as high as 20 A/cm 2 was obtained at 77 K and electron beam energy E e = 45 keV. Electron beams with E e = 30-70 keV, commonly used in laser screen applications, have a penetration depth of a few microns. This makes difficult using bulk semiconductor crystals as the active elements, especially for lasers with longitudinal excitation, due to a rather complicated procedure of fabrication of relatively thin (10-50 mm) defect-free layers by mechanical treatment of the crystals [6,7]. Employing of epitaxial growth technologies for the active layer fabrication immediately resulted in a decrease of the threshold current density. The first electron beam pumped laser based on the ZnSe film grown on a ZnS substrate exhibited J th = 4.5 A/cm 2 and J th = 42 A/cm 2 at T 80 K and 300 K, respectively, in transverse pumping geometry with E e = 50 keV [8].Further efforts to reduce the threshold were addressed to the improvement of both structural quality of the films and heterostructure design to decrease optical losses in a laser cavity and to enhance carrier confinement. Laser generation with J th as low as 3.5 A/cm 2 (E e = 30-45 keV, T = 80 K, transverse excitation geometry) has been achieved on the ZnSe/GaAs films grown by metal-organic chemical vapor deposition 1 ) Corresponding