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226   So l i d - S t at e   La s e r s                     Thin-Disc Lasers    227


                                                   Laser beam

                                                             Pump power



                              Pumped area
                                                            AR coating
                                                            Laser active material
                                                            HR coating
                                      Heat flow

                                                     Heat sink



                                          Surface cooling

                      Figure 10.1  Thin-disc laser design. AR: antireflective; HR: highly reflective.
                      (Courtesy of Dausinger und Giesen GmbH)

                      for one of the outstanding features of the thin-disc laser—that is, its
                      excellent beam quality.
                         Figure 10.1 shows the principle of the thin-disc laser design.
                                                                              3-8
                      The laser crystal has a diameter of several millimeters (depending on
                      the output power or energy) and a thickness of 100 to 200 mm (depend-
                      ing on the laser active material, the doping concentration, and the
                      pump design). The disc has a highly reflective (HR) coating on its
                      back side for both the laser and the pump wavelengths and an antire-
                      flective (AR) coating on the front side for both wavelengths. This disc
                      is mounted with its back on a water-cooled heat sink, using indium-
                      tin or gold-tin solder, which allows for a very stiff fixation of the disc
                      to the heat sink without disc deformation. To reduce the stress during
                      and after the soldering process as much as possible, the heat sink is
                      made from a heat-expansion-matched material (e.g., copper-tungsten
                      metal  matrix  material  [CuW]).  The  heat  sink  is  water  cooled  by
                      impingement cooling using several nozzles inside the heat sink.
                         As mentioned earlier, the temperature gradients inside the laser
                      crystal are mainly coaxial to the disc axis and the laser beam axis due
                      to this mounting and cooling technique. The temperature in the radial
                      direction is nearly uniform within the disc’s homogeneously pumped
                      central  area.  Therefore,  these  temperature  gradients  only  slightly
                      influence the laser beam propagation through the disc. All the ther-
                      mal lens effects and aspherical parts of the index of refraction profile
                      are reduced by more than 1 order of magnitude as compared with rod
                      laser systems. The stress-induced birefringence is even more reduced
                      and can be neglected for real laser systems. In addition, due to the
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