Page 234 - High Power Laser Handbook
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202   So l i d - S t at e   La s e r s                   Zigzag Slab Lasers    203


                                                              Piston sensor
                   Master  YDFA       Frequency-shifted reference beam
                  oscillator    AOM
                                             Power amplifier chains
                            PM  YDFA  PA
                                                                      Tiled, high-power
                                                                       output beam


                               Adaptive
                                optics
                                                     Wavefront
                                                     sensors
                          Phase control
                          electronics
                                                            Heterodyne detectors
                 Figure 8.18  Schematic of the laser system. The grayed-out components indicate
                 hardware duplication to scale past two chains. YDFA: Yb-doped fiber amplifier; PM:
                 phase modulator; AOM: acousto-optic modulator; PA: preamplifier.






                 Gain module
                 w/shroud                                               Module
                                                                        diagnostic
                                                                        bench
                     Relay
                     telescope
                     w/shroud



                 Figure 8.19  One of the JHPSSL MOPA chains.

                      via  angular  multiplexing  enables  good  staturation  and  30  percent
                      optical extraction efficiency. Angular multiplexing of the slabs is made
                      straightforward  by  choosing  different  integral  numbers  of  zigzag
                                           15
                      reflections  on  each  pass.   After  all  eight  amplification  passes,  the
                      beamlet powers are amplified to their final levels of 15 kW.
                         The slab amplifiers impose multiple waves of OPD on each beam-
                      let, due to thermo-optic effects in the slabs that arise from spatial inho-
                      mogeneities in the heat deposition and removal and which are thus not
                      removed by zigzagging. Figure 8.20 shows OPD imposed by a pass







                      Figure 8.20  Typical 4-kW slab gain module OPD meausured using a Mach-
                      Zehnder inteferometer operating at 658 nm. The zigzag axis is vertical, and
                      the non-zigzag axis is horizontal.
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