A gas laser oscillator includes laser gas circulation paths including first and second paths; a first discharge tube provided in the first path; a second discharge tube provided in the second path; a laser power supply for supplying a first high frequency power to the first discharge tube and supplying a second high frequency power having a different phase from the first high frequency power to the second discharge tube; and a matching unit including a first coil and a first capacitor, and a second coil and a second capacitor. Each value of the first coil, the first capacitor, the second coil, and the second capacitor is determined such that the difference between the peak value of a voltage applied to the first discharge tube and the peak value of a voltage applied to the second discharge tube falls within a predetermined range.

An intracavity plasma solid state laser with an emission line radiation source of determined wavelength seeding a semiconductor laser gain medium providing a high power laser beam of the determined wavelength. A plasma cell generates a determined wavelength based on an atomic emission line that is received by the semiconductor laser or laser diode having a broadband output encompassing the determined wavelength received from the plasma cell. The laser diode locks on to the determined wavelength and emits a high powered laser beam of the determined wavelength. The intracavity plasma solid state laser creates a laser beam of narrow linewidth comparable to the natural Voight or Doppler linewidth of atomic transition and higher power in a smaller size than previously possible. The intracavity plasma solid state laser is easily manufactured and suitable for placement in an array for targeting a predetermined area.

A laser and methods for providing a continuous wave output beam. The laser and method includes positioning a micro-plasma chip capable of creating micro-plasmas within a resonant cavity. A gas is input into the resonant cavity and flows around the micro-plasma chip. Micro-plasmas ignite and excite the gas to create metastables. The metastables are further excited by an optical pump having an energy sufficient to cause the metastables to lase.

A gas laser oscillation apparatus of orthogonal excitation type includes an electric discharge region having a pair of electric discharge electrodes, an axial flow blower having a plurality of rotor vanes and working by a permanent magnet motor, a first heat exchanger having a plurality of cooling fins, the cooling fins arranged on a plane perpendicular to an optical axis, a second heat exchanger having a plurality of cooling fins, the cooling fins arranged on a plane perpendicular to the optical axis, a gas duct having a gas passageway and arranged between the electric discharge region and the first heat exchanger, the axial flow blower being arranged on the gas passageway. The axial flow blower is arranged on a windward side of the first heat exchanger. The second heat exchanger is arranged on a windward side of the axial flow blower.

A gas laser oscillator includes laser gas circulation paths including first and second paths; a first discharge tube provided in the first path; a second discharge tube provided in the second path; a laser power supply for supplying a first high frequency power to the first discharge tube and supplying a second high frequency power having a different phase from the first high frequency power to the second discharge tube; and a matching unit including a first coil and a first capacitor, and a second coil and a second capacitor. Each value of the first coil, the first capacitor, the second coil, and the second capacitor is determined such that the difference between the peak value of a voltage applied to the first discharge tube and the peak value of a voltage applied to the second discharge tube falls within a predetermined range.