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216   So l i d - S t at e   La s e r s     Nd:YAG Ceramic ThinZag® High-Power Laser Development     217
























                      Figure 9.13  The three ThinZag modules: TZ-1, TZ-2, and TZ-3 (from left to
                      right). Interestingly, there is not a significant size change in the modules as
                      the power increases from about 1 kW laser output (TZ-1) to more than 15 kW
                      laser output (TZ-3).



                      the height of the Nd:YAG slabs. The TZ-2 device uses 1-cm-high slabs,
                      while the TZ-3 uses 3-cm-high slabs. Because the pump intensity in
                      both devices is the same, the output from the TZ-3 module, compared
                      with the TZ-2 module, is expected to be greater by a factor of 3. Since
                      the TZ-2 module produced about 5.6 kW, the TZ-3 is expected to pro-
                      duce  about  16.8  kW.  Figure  9.13  shows  the  TZ-1,  TZ-2,  and  TZ-3
                      lasers.  Note  the  small  change  in  the  devices’  overall  dimensions,
                      which  produces  more  than  an  order  of  magnitude  higher  power
                      when scaling from the TZ-1 to the TZ-3. Initial short-pulse measure-
                      ments performed on the TZ-3 demonstrated outputs to 16.8 kW out-
                      put using a stable cavity, as shown in Fig. 9.14.
                         The TZ-3 laser module operates, as did all the previous ThinZag
                      laser  modules,  with  laser  medium  distortions  that  are  low  order
                      (mainly cylinder) and slowly varying (time scales of seconds). Modi-
                      fications to the laser module continue to improve the device’s ther-
                      mal control, which in turn influences the medium quality when under
                      full-power extraction.
                      9.1.4  Coupling Three TZ-3 Modules
                      Three  TZ-3  modules  were  coupled  in  series  as  a  single-aperture
                      power oscillator. (Three is the minimum number of modules needed
                      to operate with an unstable cavity for good beam quality.) The laser
                      model calculations shown in Fig. 9.15 indicate that with three mod-
                      ules, optimum feedback for good extraction occurs at a little over
                      40  percent  reflectivity.  For  graded  reflectivity  output  couplers,  the
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