Page 496 - High Power Laser Handbook
P. 496

464     Fi b er   L a s er s                                                                                                       Pulsed Fiber Lasers     465


                      bear the promise of ultimate compactness and ruggedness, mainly
                      due  to  the  minimization  of  free-space  alignment-sensitive  optical
                      paths  and  the  potential  for  transition  from  the  traditional  optical
                      bench concept toward distributed architectures of fluid, application-
                      tailored form factor.
                         However, traditional pulsed fiber laser (PFL) systems have been
                      confined to relatively low values of pulse energy and peak power,
                      which only suit optical telecommunications and other niche applica-
                      tions. The primary obstacle to overcoming this limitation has been
                      the  onset  of  unwanted  nonlinear  optical  effects,  which  stem  from
                      high in-fiber irradiance × length products and which result in spectral
                      broadening.  This  issue  directly  impairs  the  PFL’s  ability  to  serve
                      applications that require high spectral brightness, such as laser fre-
                      quency tuning to material resonances, return signal discrimination
                      against a broadband background, or optical efficiency maximization
                      in nonlinear wavelength conversion. Indirectly, spectral broadening
                      precludes ultimate power scaling through beam combining schemes
                      that  preserve  spatial  brightness—namely,  coherent  phasing  and
                      wavelength multiplexing. Other important challenges to overcome in
                      pulse power scaling in the kilohertz PRF regime are energy storage
                      limitations due to amplified spontaneous emission (ASE) and optical
                      damage.
                         This chapter details the nature and extent of such challenges,
                      with an emphasis on the specific cases of nanosecond pulse widths
                      and high in-fiber pulse energy and peak power generation. It then
                      reviews key enabling solutions that have permitted, in recent years,
                      substantial  power  scaling  for  fiber-based  lasers  and  amplifiers
                      operating in this regime. This review focuses entirely on ~1-μm-
                      wavelength Yb-doped fiber technologies, which dominate the high-
                      power  fiber  laser  scene  in  both  the  continuous  wave  and  pulsed
                      regimes. An  outlook  toward  near-future  developments  concludes
                      the analysis.


                 16.2  Challenges to Pulse Power Scaling

                      This section provides an overview of the issues that must be faced in
                      order to boost the performance of PFLs and pulsed fiber amplifiers
                      and to meet the requirements of demanding nontelecommunications
                      applications. Three key problem areas are identified and discussed:
                      nonlinear optical effects, amplified spontaneous emission, and opti-
                      cal damage.

                      16.2.1  Nonlinear Optical Effects
                      Nonlinear effects (NLEs) represent the principal limitation for in-fiber
                      pulse peak power. This situation is a direct consequence of the tight
   491   492   493   494   495   496   497   498   499   500   501