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174    So l i d - S t at e   La s e r s                                                                Intr oduction to  h igh-Power Solid-State Lasers      175


                      structure  to  match  any  desired  absorption  feature  in  the  near  IR.
                      Selecting a diode wavelength close to the laser emission wavelength
                      reduces  the  quantum  defect  and  thus  minimizes  waste  heat.  For
                      Nd:YAG, the most common band for diode pumping is the absorp-
                      tion feature centered at 808 nm, which boasts a high absorption cross
                      section and a fairly broad line width.
                         The narrow, engineerable emission spectrum of diodes has enabled
                      use of SSL gain materials that simply could not be pumped effectively
                      with  lamps.  The  most  prominent  of  these  is  Yb:YAG.  Owing  to
                      Yb:YAG’s simple energy-level structure, it is almost completely trans-
                      parent except in the 900 to 1100 nm range (Fig. 7.4). Yet this makes
                      Yb:YAG an ideal candidate for diode pumping, most commonly at the
                      ∼10-nm broad absorption line near 940 nm. Yb-doped materials can
                      also be pumped at the narrower ∼980-nm, zero-phonon line to mini-
                      mize the quantum defect.
                         Another advantage of diode pumping is its highly directional (i.e.,
                      bright) emission. Although high-power diode emitters are multimode
                      lasers,  their  beam  quality  is  nevertheless  sufficient  to  enable  beam
                      shaping  using  conventional  optics  or  lens  ducts.  Hence,  the  pump
                      intensity distribution within the SSL gain medium can be tailored to
                      generate smooth excitation profiles to minimize thermal nonuniformi-
                      ties  across  the  lasing  aperture.  Another  advantage  of  high  diode
                      brightness is that the pump light can be focused to very high intensi-
                      ties, easily surpassing the tens of kW/cm  needed for efficient pump-
                                                        2
                      ing  of  the  quasi-three-level  Yb  transition.  Diode  focusability  also
                      eliminates the need for the SSL gain material to have a large surface
                      area devoted to receiving pump light. With the use of focused diodes,
                      pump light can be coupled into the gain medium through a relatively
                      thin edge or tip, allowing large-area faces to be devoted to heat removal
                      or laser extraction, with the corresponding thermal advantages.
                         Diodes have numerous other practical advantages as SSL pump
                      sources. They may be scaled nearly arbitrarily in power (although not
                      in brightness) by incoherently stacking multiple emitters or bars to
                      form large arrays, with multikilowatt modules commonplace. They
                      have benefited from years of investment in reliability engineering to
                      achieve lifetimes typically measured in tens of thousands of hours.
                      Finally, diodes are relatively compact and enable packaging of SSLs
                      for platforms and environments (such as space), where lamp-pumped
                      systems simply would not be feasible. In particular, fiber delivery of
                      diode light allows unprecedented design flexibility and packaging
                      convenience.


                      7.3.2  Laser Extraction and Heat Removal
                      Removal of heat through the laser material’s surface creates thermal
                      gradients that can aberrate the extracting laser beam and thus limit the
                      output BQ, or even lead to catastrophic failure due to stress fracture.
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