Pressure broadening effects on the output of a gas laser.
Gas laser oscillator model allowing atomic collisions, noting pressure effects on output intensity profile when tuning cavity frequency through atomic resonance
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Gas laser oscillator model allowing atomic collisions, noting pressure effects on output intensity profile when tuning cavity frequency through atomic resonance
Gas lasers pumping by nuclear energy, discussing heavy particle interactions, threshold densities, population inversion, etc
Molecular gas laser Q-switching techniques, determining rotational collision sections for carbon dioxide and cross sections for vibrational relaxation
For use in a waveguide gas laser, a capillary tube of glass or ceramic has an inner surface defining a longitudinal capillary opening through which the laser gas flows. At least a portion of the inner surface is corrugated with corrugations or channels with a periodicity Lambda where Lambda = 1/2 Lambda, Lambda being the laser gas wavelength. The tube includes a diffused region extending outwardly from the opening. The diffused region of a depth d on the order of 1 Lambda to 3 Lambda acts as a waveguide for the waves, with the corrugations producing distributed feedback. The evanescent component of the waves traveling in the diffused region interact with the laser gas in the opening, gaining energy, and thereby amplifying the waves travelling in the diffused region, which exit the diffused region, surrounding the opening, as a beam of wavelength Lambda.
IR gas pulsed lasers continuous self mode locking, observing optical spectra with scanning Fabry-Perot interferometer
Single mode gas laser theory for arbitrary field intensities in terms of ensemble averaged form of density-matrix equations of motion
High power gas laser concepts are discussed with emphasis on the role that fluid mechanics has played in their development. Consideration is given to three types of systems: gasdynamic lasers, HF supersonic diffusion lasers, and electric discharge lasers. Flow effects and aerodynamic windows in such lasers are briefly described. Future directions of research are outlined.
Frequency measurement of gas laser transitions in heavy water and acetylene discharges
Carbon dioxide dissociation in gas discharge, water vapor and xenon effects on dissociation, and electrode material influence on clean-up rate related to nonflowing sealed gas laser
Inexpensive carbon dioxide molecular gas laser using plano-concave eyeglass lenses
A brief review of laser elements is given. Flowing gas lasers are represented to have the best potential for high average power. The background of shock-tube researchers and the shock tube itself are alleged to be ideally suited for the development of such lasers. Three types - the electric discharge, the gasdynamic, and the chemical laser - are discussed briefly. A legion number of possible gas lasers is enumerated. With the development of their potential for higher power and efficiency, many additional and important uses of lasers are predicted, even beaming power through space for long distances, up to 1 AU. A few details of some current high-power gasdynamic laser devices are given.
A multiple pulse electric discharge gas laser system is described in which a plurality of pulsed electric discharge gas lasers are supported in a common housing. Each laser is supplied with excitation pulses from a separate power supply. A controller, which may be a microprocessor, is connected to each power supply for controlling the application of excitation pulses to each laser so that the lasers can be fired simultaneously or in any desired sequence. The output light beams from the individual lasers may be combined or utilized independently, depending on the desired application. The individual lasers may include multiple pairs of discharge electrodes with a separate power supply connected across each electrode pair so that multiple light output beams can be generated from a single laser tube and combined or utilized separately.
Efficient impedance-matched gas laser excitation circuits integrally employ prepulse power generators. Magnetic switches are employed to both generate the prepulse and switch the prepulse onto the laser electrodes.
Pressure effects in Fabry-Perot lossy-cavity gas laser output
Aluminum cold cathodes for single mode helium neon gas lasers
Gas laser application to magnetospectroscopy of graphite, Bi, As and pyrolytic graphite single crystals
Quantum phase fluctuations in IR gas lasers, noting nearly Lorentzian power spectrum with bandwidth inversely proportional to output power
Discharge tube dimensions, flow rate, wall temperature, and gas mixtures defined for carbon dioxide gas laser