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The CO2 Laser pp 138-194 | Cite as

Pulsed Systems

  • W. J. Witteman
Chapter
Part of the Springer Series in Optical Sciences book series (SSOS, volume 53)

Abstract

The major problem in increasing the output energy of a continuous CO2 laser system is the temperature rise with increased input energy. As discussed in Chaps. 3 and 4, the population density of the lower laser level and its depopulation rate to translational and rotational energies depend strongly on the gas temperature. The gas temperature, in turn, results from the balance between the input and the heat conduction energies. Since the heat conductivity is independent of the gas density, the heat transport by conduction is fixed for a given maximum gas temperature and hence is the limitation on the input energy. Higher output energies of cw systems can then only be obtained by also applying heat convection for cooling such as by rapidly moving the gas through the electric discharge region. For efficient operation of these systems, the discharge power input per unit mass flow rate does not exceed 600 J/g, as we have seen in Chap. 4.

Keywords

Corona Discharge Inelastic Collision Elastic Collision Laser Level Vibrational Excitation 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer-Verlag Berlin Heidelberg 1987

Authors and Affiliations

  • W. J. Witteman
    • 1
  1. 1.Department of Applied PhysicsTwente University of TechnologyEnschedeNetherlands

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