Page 257 - High Power Laser Handbook
P. 257

226    So l i d - S t at e   La s e r s                                                                                              Thin-Disc Lasers     227


                         In November 1991, during the Lasers and Electro-Optics Society
                      (LEOS)  conference,  Adolf  Giesen  listened  to  a  talk  about  diode
                      pumped Yb:YAG lasers given by T. Y. Fan of the Massachusetts Insti-
                      tute of Technology (MIT). Fan explained the advantages of Yb:YAG
                      for diode laser pumping in detail, but he also stated that it would be
                      very  difficult  to  build  a  high-power  Yb:YAG  laser  using  classical
                      designs due to Yb:YAG’s quasi-three-level nature. At that time, the
                      laser output power was only a few watts.
                         After  this  talk,  Giesen  made  some  initial  calculations,  which
                      showed that it would be possible to power scale Yb:YAG if the mate-
                      rial were simply a very thin sheet of material cooled from one or two
                      sides, so that the heat flux length to the cooling device were mini-
                      mum. At the University of Stuttgart in Germany, Giesen convinced
                      his colleagues of his idea. In January 1992, a small group (Uwe Brauch
                      from the German Aerospace Center [DLR], Adolf Giesen, Klaus Wit-
                      tig and Andreas Voss from the University of Stuttgart [IFSW]) started
                      to develop the details of such a laser design, using a thin sheet of laser
                      active material. The primary thin-disc laser design was developed at
                      the end of March 1992, and in late spring 1993, the first demonstra-
                                                                              3, 4
                      tion was realized—first with 2 W output power and later with 4 W.
                      Also in 1993, the group applied for the first patent for this design,
                      which has since been successfully licensed to more than 20 compa-
                      nies. During the following years, Giesen’s group demonstrated power
                      scaling of thin-disc lasers, pulsed operation also with subpicosecond
                      pulse  duration,  and  the  applicability  of  this  design  to  many  other
                      laser active materials.
                         Fortunately,  during  the  1980s  the  German  federal  ministry  of
                      Research and Technology (BMFT) identified laser technology as a
                      key technology for materials processing. Consequently, during these
                      years,  many  projects  were  initiated  and  funded  between  research
                      institutes and companies, which led to increased funds for thin-disc
                      laser  work.  Later,  companies  like  Trumpf  Laser,  Rofin-Sinar  and
                      Jenoptik started working on thin-disc lasers, generously supporting
                      the  institute’s  work. As  a  result,  within  just  one  decade,  German
                      companies became very strong in the field of laser technology for
                      materials  processing,  eventually  taking  the  leadership  role  in  this
                      industrial area.

                 10.3  Principles of Thin-Disc Lasers

                      The core concept of the principle behind thin-disc lasers is the use of
                      a thin, disc-shaped active medium that is cooled through one of the
                      flat faces of the disc; simultaneously, the cooled face is used as a fold-
                      ing or end mirror of the resonator. This face cooling minimizes the
                      transversal  temperature  gradient,  as  well  as  the  phase  distortion
                      transversal to the direction of the beam propagation, and it accounts
   252   253   254   255   256   257   258   259   260   261   262