Page 264 - Tunable Lasers Handbook
P. 264

224     Norman P. Barnes

                   transition  metal  solid-state  lasers.  Basic  material  properties  and  laser  perfor-
                   mance details are given for each laser material. Oscillator performance, as well
                   as amplifier performance where appropriate, is also presented.
                      Laser performance will be characterized by a threshold and slope efficiency.
                   If  the laser output energy is plotted versus the pump energy, very often a linear
                   relationship  can be  obtained. That  is, the  laser  output  energy ELo is  approxi-
                   mately related to the pump energy, Ep, by a relationship of the form






                   where os is the  slope efficiency  and EPrh is the threshold  energy. Pumping  of
                   the transition metal solid-state lasers can be accomplished using either a flash-
                   lamp or another laser. In  either case.  the linear relationship  is approximately
                   true. For some laser materials, both types  of optical pumping  have been  suc-
                   cessfully  employed. Furthermore.  this  approximate  relation  is true  for either
                   normal mode or Q-switched operation of the laser. Thus, rather than presenting
                   typical  laser output energy versus pump energy  data. the threshold  and slope
                   efficiency are given.
                      When selecting a laser for a particular application, several factors need to be
                   considered including tuning range, threshold, slope efficiency, energy per pulse,
                   and average power. Tuning range is often the first selection criterion, that is, the
                   laser must be able to produce the desired wavelength. Toward this end, the emis-
                   sion spectra for the various laser materials are given.
                      A low threshold is necessary to efficient laser operation, particularly if  cw
                   operation is desired. A primary consideration is whether the laser operates as a
                   three- or four-level laser, the latter being vastly preferred. Threshold depends on
                   the  absorption efficiency of  the laser  material and the product of  the effective
                   stimulated  emission  cross  section  and  the  lifetime.  Absorption  efficiency
                   depends on the characteristics of the optical pump and the absorption properties
                   of the laser material. If  a narrow spectral bandwidth optical pump is used, such
                   as  a laser  diode or  another laser, relatively narrow  absorption features  can be
                   used to advantage. However, if a broad spectral bandwidth pump is used, such as
                   a  flashlamp,  broad  absorption  features  become  advantageous.  To  assess  the
                   absorption  efficiency,  absorption  spectra  have  been  included.  Threshold  is
                   roughly inversely proportional  to the product of  the effective stimulated emis-
                   sion cross section and the upper laser level lifetime. Both parameters are given
                   in this chapter for the various laser materials.
                       Slope efficiency depends on the absorption efficiency, as does the threshold,
                   and on the overlap of the laser mode volume with the pumped volume as well as
                   the losses. Overlap of the laser mode volume and the pumped volume is particu-
                   larly important if  good beam quality is also important. Good overlap is depen-
                   dent on the particular laser design but as a general rule is easier to achieve when
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