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172   So l i d - S t at e   La s e r s     Intr oduction to  h igh-Power Solid-State Lasers      173




                            Xenonlamp  emission



                                      Wasted flashlamp power



                            Nd:YAG  absorption




                                    300  400  500   600  700  800   900
                                               Wavelength (nm)
                      Figure 7.5  (top) Emission spectrum of a xenon-filled flash lamp. The shaded
                      regions of the spectrum represent wasted energy that is not absorbed by
                      Nd:YAG (bottom).

                      laser’s efficiency. Even if a lamp photon happens to be at a favorable
                      wavelength for absorption, it will most likely be at a transition to an
                      energy level high above the upper laser level, leading to a large quan-
                      tum defect and thus a large amount of heat deposited in the gain
                      material for every emitted laser photon. From the standpoint of per-
                      formance, this excess heat is the primary disadvantage of lamp pump-
                      ing in comparison to the modern standard of diode pumping.
                         One final difficulty with lamp pumping is that lamps emit in all
                      directions, with low spatial brightness, which severely constrains the
                      geometric choices for optical coupling of the pump source into the
                      gain medium. The most common choices are either to simply close-
                      couple the lamp(s) against the gain medium, typically with a reflector
                      to capture light emitted away from the desired direction, or to embed
                      both the lamp and the gain medium (typically in the form of a rod) at
                      the foci of an elliptical reflecting cavity, so that the lamp light is reim-
                      aged onto the rod. Neither of these geometries is advantageous for
                      scaling to higher power, because they both constrain the geometries
                      for laser beam extraction and heat removal.
                      Diode Pumping
                      The development of efficient, high-power laser diodes for pumping
                      SSLs has revolutionized the development of HAP SSLs over the past
                      15  years.  Owing  to  the  importance  of  diode  lasers  both  as  pump
                      sources  and  as  high-power  lasers  in  their  own  right,  they  are  dis-
                      cussed in detail in Chaps. 5 and 6.
                         Diodes  make  ideal  excitation  sources  for  SSLs.  Their  emission
                      spectrum can be engineered through choice of material and epitaxial
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