Page 352 - High Power Laser Handbook
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320   So l i d - S t at e   La s e r s         Ultrafast Solid-State Lasers    321


                      by  light-induced  polymerization,  because  two-photon  absorption
                      may be used to initiate the polymerization reaction. As in their use for
                      micromachining,  femtosecond  laser  pulses  allow  significant  two-
                      photon absorption in localized volumes and can produce small, high-
                      resolution spatial features.
                      12.6.3  Laser-Based Photon and Particle Sources
                      Recent experiments have demonstrated that an intense femtosecond
                      laser pulse focused into a gas-puff target can drive a strong plasma wake
                      field, which can accelerate electrons to tens of mega-electronvolt
                      energy in a propagation distance of just a few millimeters. Recent
                      experiments have shown that under the right conditions, the emitted
                      electron bunch can be monochromatic, with an energy bandwidth of a
                                                                  45
                      few percent at electron energies as high as 80 MeV.  In this recent
                      work, ultrafast laser pulses of peak power ~1 to 10 TW are needed to
                      effect relativistic self-focusing of the pulse at intensities greater than
                        18
                               2
                      10  W/cm , which is required to generate the wake field. Further
                      work in ultrafast laser development, as well as continued progress in
                      optimizing parameters for plasma generation, will allow this type of
                      electron accelerator to work reliably at higher 100 to 1000 Hz repeti-
                      tion  rates.  This  would  make  laser-plasma-based  electron  sources
                      practical for such applications as radioisotope production and, even-
                      tually,  for  use  as  much-brighter  photoinjector  electron  sources  for
                      compact free-electron lasers.
                         An  important  set  of  new,  high-resolution  radiological  applica-
                      tions may soon be possible using these intense lasers. It is well known
                      that such intense laser pulses can produce copious amounts of radia-
                      tion  of  various  sorts.  These  radiation  sources  range  from  photons
                      with energy of 10 eV to greater than 1 MeV to a host of particles,
                      including neutrons, protons, and electrons. Moreover, the fluxes of
                      these radiation sources can be quite substantial, even though their
                      source sizes are small (microns to tens of microns). Therefore, these
                      new photon and particle radiation sources would have unique appli-
                      cations  in  high-resolution  probing  of  materials—for  example,  to
                      detect buried voids and cracks in aircraft surfaces or to understand
                      fuel flow and combustion. Thus, this field has the potential for these
                      sources of extreme photons and particles to be combined with novel
                      diagnostic techniques to realize enabling technologies that will have
                      a major impact on diverse areas of the defense, manufacturing, envi-
                      ronmental and medical industries.

                      12.6.4  High Harmonic Generation
                      One of the major thrusts in modern science and technology has been
                      to  understand  and  make  use  of  electromagnetic  (EM)  radiation.
                      Understanding the interaction of EM radiation with matter led to the
                      development  of  quantum  theory  and,  subsequently,  of  solid-state
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