Page 209 - High Power Laser Handbook
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178    So l i d - S t at e   La s e r s                                                                Intr oduction to High-Power Solid-State Lasers      179


                                   Primary mirror
                                 λL
                                                               Secondary
                                                                 mirror
                               Fresnel
                                core





                      Figure 7.8  Unstable resonator cavity.



                      at the edges. This latter configuration is widely used in present-day
                      unstable  resonators  to  eliminate  diffraction  from  the  hard-edged
                      aperture.  For  nonspatially  varying  reflectivities,  the  outcoupling
                                                   2
                      fraction is approximately 1 – 1/M .
                         Whereas unstable resonators provide large mode volumes, they
                      also impose some challenges when used to extract high-power SSL
                      gain materials. To maintain good wavefront control and single-mode
                      output, any OPD imposed by the gain material must be small enough
                      that  it  is  overwhelmed  by  the  mirror  curvatures.  Otherwise,  OPD
                      from the gain module can effectively form a lens over a small aper-
                      ture that can drive the resonator over the stability boundary, hence
                      forming a locally stable resonator. This, in turn, causes “filamenta-
                      tion” of the unstable resonator mode, in which multiple independent
                      output  beams  with  uncorrelated  wavefronts  colase  over  different
                      subapertures of the gain medium.
                         To avoid such an event and to provide some robustness against
                      thermal  OPD,  unstable  resonators  for  SSLs  are  typically  designed
                      with high-curvature mirrors, leading to short resonator lengths and
                      large  magnifications.  However,  high  M  leads  to  large  outcoupling
                      fractions and, thus, to a requirement for correspondingly high laser
                      gain to make up for the loss on each round trip to maintain laser oscil-
                      lation. Hence, unstable resonators tend to achieve the most success
                      with high gain materials, such as Nd, or with geometries that provide
                      a long gain path for the extracting beam (e.g., zigzag slabs). To further
                      increase laser gain, the modules are often operated in a pulsed or
                      quasi-CW format, even when the goal is high average, rather than
                      peak, power. 22
                         This is not to say that unstable resonators cannot be made to work
                      with low gain materials and module architectures such as Yb:YAG
                      thin  disks.  Even  with  a  low-gain  SSL  medium,  unstable  resonator
                      extraction has been demonstrated successfully by combining multiple
                      gain modules, or gain module passes, per resonator round trip, often
                      with  the  use  of  image-relay  optics  to  accommodate  long  physical
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