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182    So l i d - S t at e   La s e r s                                                                Intr oduction to  h igh-Power Solid-State Lasers      183




                                                            SBS cell
                             MO            Amplifiers
                                  Polarizer         λ/4 plate


                              Clean        Aberrated             Hypersonic wave
                              input         input
                                                                   caused by
                                                                  electrostriction
                                    Aberrations


                                                                   Focal region
                         Clean        Invetred                    in SBS liquid
                         output       output

                      Figure 7.10  SBS-based phase conjugate mirror configured with a MOPA.



                      that upon the return transmission through the aberrated PA, the orig-
                      inal planar wavefront is recovered at the MOPA output port.
                         PCMs can be formed using a variety of linear and nonlinear phys-
                      ical  mechanisms  and  materials.  Although  SBS  works  particularly
                      well with pulsed, high-peak-intensity SSLs, lower-threshold PCMs
                      have been demonstrated using SBS in multimode fibers  and in free
                                                                     30
                      space using photorefractive or thermal gratings. 31
                         Despite the attractive simplicity of a PCM, they are not always
                      feasible to implement on an HP SSL. Each PCM mechanism, whether
                      SBS, thermal, or photorefractive, constrains the incident laser’s oper-
                      ating regime. For example, SBS in Freon has a high threshold and
                      requires a long interaction length to build up sufficient reflectivity
                      from the acoustic grating; thus, it does not work well with anything
                      other  than  pulsed,  single-frequency  lasers  with  long  coherence
                      lengths. The dynamic range in power of most thermal PCM configu-
                      rations is also limited. Typically the reflection from a PCM is signifi-
                      cantly  less  than  unity,  requiring  a  high-gain  geometry  to  avoid
                      substantial  loss  of  efficiency.  Finally,  the  conjugation  range  of  any
                      PCM  will  be  limited—essentially,  the  input  wavefront  aberrations
                      must be of sufficiently low amplitude and spatial frequency such that
                      the beam does not break into separate spots near the focus. This yields
                      a set of conjugate returns from each spot with uncorrelated phases
                      that will not yield planar output after the second PA pass.
                      7.5.3  Adaptive Optics
                      Adaptive  optics  (AO)  provides  a  more  flexible  and  engineerable
                      means of wavefront control than phase conjugation.  This capability
                                                                  32
                      comes at the cost of added complexity in the form of active control
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