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254    So l i d - S t at e   La s e r s                                                                                              Thin-Disc Lasers     255


                      laser power levels with nearly fundamental mode properties will be
                      possible in future.
                         With the potential of very high output power levels for the funda-
                      mental mode, it is possible to operate thin-disc lasers also in single
                      frequency operation. 43,44  To achieve this, it is necessary to use a birefrin-
                      gent filter and one or two uncoated etalons inside the fundamental
                      mode resonator. With such resonators, up to 98-W single frequency
                                                43
                      power has been demonstrated.  In addition, the laser’s wavelength
                      can be tuned over a wide spectral range (1000–1060 nm for Yb:YAG) by
                      tuning the birefringent filter. 5,43–46
                         Another interesting feature is resonator’s internal doubling of the
                      laser  frequency  for  covering  the  visible  spectral  range  with  high
                      efficiency. This can be successfully demonstrated with different laser
                      materials. With Yb:YAG the wavelength tunability between 500 and
                      530  nm,  maximum  power  around  515  nm  could  be  shown;  50-W
                      green output power is commercially available. For Nd:YVO 4 18,19  more
                      than 12 W can be demonstrated at 532-nm wavelength and more than
                      3 W can be demonstrated at 457 nm (doubling of the quasi-three-level
                      transition at 914 nm). For Nd:YAG more than 1 W at 660 nm was
                      achieved when doubling the 1320 nm transition.


                 10.7  Thin-Disc Laser in Pulsed Operation
                      In  addition  to  the  outstanding  properties  of  the  thin-disc  laser’s
                      design for CW operation, it is also well suited for pulsed laser sys-
                      tems,  especially  if  high  average  output  power  is  demanded.  Until
                      recently,  pulsed  thin-disc  laser  systems  had  been  developed  and
                      demonstrated for the nanosecond-, picosecond-, and femtosecond-
                      pulse duration regime. All systems showed an excellent beam quality
                      and a high efficiency.
                         In Ursula Keller’s group at the ETH Zurich high average power
                      fs-oscillators  have  been  developed,  which  are  described  in  more
                      detail in Chap. 13. 47–51  It has been demonstrated that with the thin-
                      disc  laser  design,  high  output  powers  are  possible  down  to  pulse
                                                                          52
                      durations  of  220  fs,  especially  with  the  use  of  Yb:Lu O   and
                                                                       2
                                                                         3
                                53
                      Yb:LuScO .  An exhaustive overview of possible laser materials and
                              3
                      the achieved results with mode-locked thin-disc lasers can be found
                      in a recent paper.  The mode locking of thin-disc lasers with semi-
                                     54
                      conductor saturable absorbers (SESAM) is a very elegant approach to
                      exploit the scaling behavior of both concepts, as the SESAM concept
                      also can be scaled by increasing the active area. This advantage is
                      already transformed to an industrial product, a mode-locked thin-disc
                      laser with 800 fs pulse duration and 50 W output power available
                      from Time–Bandwidth products.
                         In the following sections the results for q-switched lasers, cavity
                      dumped lasers and for pulse laser amplifiers are discussed in more
                      detail.
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