Abstract: Gas laser comprising a flat electric energizing line consisting of an insulating layer inserted between two metallic layers brought to different potentials, one of whose edges is cut out in the shape of a parabola, one slot being provided in one of the layers, an active gaseous medium flowing in the slot, a circuit for setting up a substantially punctiform discharge between the metallic layers at the level of the focus of the parabolas. The electric line is arranged on a massive plate comprising on the one hand a cut provided in its lower face substantially opposite the slot and communicating with the latter and on the other hand two grooves provided on its upper face each having fitted in it a flexible seal and arranged opposite the walls of the slot.

Abstract: A molecular gas laser capable of operating at or near atmospheric pressure in which electrical energy is coupled into an active molecular gas medium comprising molecules having vibrational rotational energy levels by means of an electric field transverse to the lasing axis. By applying an impulse voltage to the electrode configuration, high current glow discharges can be created. The pulse discharge takes place between electrodes having parallel planar surfaces facing each other. The lateral edges of these faces are suitably profiled to avoid field concentrations and thus provide a diffused glow discharge in a uniform electric field transverse to the lasing axis. Initiatory electrons required to produce the high current diffused glow are provided by generating an intense burst of corona in the gap between spacer members having very high dielectric constants which are interposed between the electrodes.

Abstract: A laser featuring, in one aspect, a volume of gas having a lasing constituent, a light source arranged to emit light having ionizing photons for ionizing the gas, the effective photon energy spectrum of the ionizing photons lying below the ionization potential of the lasing constituent and below the level of photon absorption bands of the gas, the spectrum being selected to provide an average penetration depth of the ionizing photons into the gas of at least 1 cm. and to photoionize the gas predominantly by a multiple step process involving absorption of successive photons at least the first of which has a photon energy less than the ionization potential of said lasing constituent, and an electric field source for applying to the gas a voltage sufficient to produce an avalanche breakdown in the gas to effectively raise the lasing constituent to its lasing level; and in another aspect a seed gas comprising an amine having the structure ##EQU1## where R.sub.1, R.sub.2, and R.sub.

Abstract: The invention is directed to a method for obtaining pulsed metal vapor laser transitions. The method comprises placing a metal halide of the desired metal within an enclosure and vaporizing the metal halide to provide a metal halide vapor. The metal halide vapor is thereafter dissociated to provide ground state metal atoms of sufficient number density to create a condition for resonance trapping and, substantially simultaneously therewith, ground state metal atoms are excited to an upper laser level, while maintaining a sufficient number in the ground state to preserve said resonance radiation trapping condition, with electrons sufficiently energized to create a population inversion between the upper and lower laser level. The excited metal atom is permitted to emit laser radiation by stimulated emission to a lower laser level and the emission is resonated, preferably between a pair of externally mounted mirrors.

Abstract: An improved ion-laser system utilizing a cold, perforated-wall hollow-cate electron-beam discharge to produce a high energy, high intensity self-collimated electron-beam to provide a high efficiency, high power continuous wave or pulsed ion-laser oscillations in both visible and ultra-violet ranges.

Abstract: A laser gyroscope is disclosed wherein a polarization dispersive structure, disposed in the path of the laser beam, includes an anisotropic crystal as a half-wave retarder. The crystallographic axes of such crystal are oriented with respect to the plane of the path to produce different delays to oppositely polarized waves passing through the crystal structure.