Page 325 - High Power Laser Handbook
P. 325

294    So l i d - S t at e   La s e r s                                                                                         Heat-Capacity Lasers      295
























                      Figure 11.30  The front face of the intracavity deformable mirror. The
                      actuators can be seen through the front faceplate.


                         The main source of phase distortions is pump-induced thermal gra-
                      dients in the gain medium (see Fig. 11.18 for the calculated temperature
                      distribution in the slab). The source of these gradients is primarily non-
                      uniform pump-light deposition on the face of the slab. These nonunifor-
                      mities get directly imprinted on the wavefront.
                         Even though pump nonuniformities produce the greatest effect on
                      wavefront, other effects, such as heating of optics or thermally induced
                      air currents, also play a role. For example, the window on the face of
                      the DM was initially BK7 glass in which there was unacceptable absorp-
                      tion of the laser light by the window, causing large amounts of distor-
                      tion. These distortions were sufficient to be visible in the near-field
                      intensity pattern. We also detected the presence of convection cells via
                      the AO control loop. These cells resulted in large tilts that had to be
                      applied to the rear mirror for mitigation. Operating the laser in a helium
                      atmosphere would be one way to reduce the impact of these cells.
                         Because of pump nonuniformities and absorption by the DM
                      window, the laser’s initial runtime was limited to about 1 s before
                      the level of aberrations was too large to be corrected by the DM.
                      Note this runtime is in good agreement with the calculations pre-
                      sented  earlier.  By  replacing  the  DM  window  and  using  a  holo-
                      graphic diffuser to homogenize the pump arrays, the runtime was
                      extended to 5 s at less than two times the diffraction limit, as shown
                      in Fig. 11.31. The “Early fall 2005” graph represents the laser’s ini-
                      tial condition. In late fall 2005, the BK7 window in front of the DM
                      was  replaced  with  a  fused-silica  version.  In  spring  2006,  holo-
                      graphic diffusers were added to the pump arrays. The final result
                      was a beam quality of no more than two times the diffraction limit
                      at the end of the 5-s run.
   320   321   322   323   324   325   326   327   328   329   330