Page 397 - High Power Laser Handbook
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366     So l i d - S t at e   La s e r s                                                                          The National Ignition Facility Laser    367


                      through the PA and TSF. After the TSF, a beam splitter reflects a small
                      sample of the output pulse back to the central TSF area, where it is
                      collimated and directed to an output sensor package (OSP) located
                      under  the  TSF.  OSP  diagnostics  record  the  beam  energy,  temporal
                      pulse shape, and near-field profiles.  The main pulse proceeds to the
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                      switchyard, where four or five transport mirrors direct it to one of a
                      number  of  final  optics  assemblies  (FOAs)  symmetrically  located
                      about and mounted on the target chamber. Each FOA contains a 1ω
                      vacuum window, focal spot beam-conditioning optics, two frequency-
                      conversion crystals to reach 351-nm wavelength, a focusing lens, a
                      main debris shield that also serves as a beam diagnostic pickoff to mea-
                      sure energy and power, and a 3-mm-thick disposable debris shield.
                      The debris shields protect the upstream optics from target debris.
                         For the experiments reported in Secs. 14.4 to 14.6, the beam was
                      not  transported  to  the  target  chamber.  Instead,  an  array  of  either
                      seven or eight calorimeters was inserted at the TSF output to both
                      measure and absorb the 1ω laser energy. When the eighth calorimeter
                      was absent, it was replaced by a pickoff that routed that beam to an
                      extensive suite of diagnostics for 1ω, 2ω, and 3ω light called the preci-
                      sion diagnostic system (PDS). The PDS instruments can diagnose one
                      beamline in great detail, whereas the OSP diagnostics can acquire 1ω
                      data on all 192 beams during a shot. In PDS, the laser was frequency
                      converted  to  the  second  or  third  harmonic  using  typical  NIF  final
                      optics, and detailed studies of the 1ω beam entering the FOA, as well
                      as the 1ω, 2ω, and 3ω beams exiting it were performed. 1
                         The MA contains eleven Nd:glass laser slabs. The PA is configured
                      to have as many as seven slabs, though it typically contains only five.
                      Some NIF shots have had one, three, or seven slabs in the PA to explore
                      the full range of operating conditions. As an indication of scale, the CSF
                      is 22 m long, the TSF is 60 m, the path length from the TSF output to the
                      target chamber is 60 to 75 m, and the target chamber is 5 m in radius.


                 14.4   1v Bundle Performance and 1v/3v NIF
                         Operating Envelopes
                      Each of NIF’s eight-beam laser bundles undergoes 1ω operational and
                      performance  qualification  (OQ  and  PQ)  before  being  used  in  any
                      experiments. The OQ-PQ consists of firing 8 to 10 shots, using all 8 beams,
                      into a bank of full-aperture calorimeters. These calorimeters measure
                      absolute beam energy and calibrate a system of diodes in the OSP that
                      serve as energy diagnostics during routine operations. Beam energies
                      at 1ω for these shots range from 1 to 19 kJ, and pulse shapes are either
                      flat in time (FIT) at the output or shaped to match user specifications.
                      In addition to verifying the bundle performance, these shots are used
                      to  calibrate  and  validate  the  laser  performance  operations  model
                      (LPOM) description of these beamlines. LPOM is then used to predict
                      laser performance and to set up the ILS for all NIF shots.
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