Page 370 - High Power Laser Handbook
P. 370

338   So l i d - S t at e   La s e r s     Ultrafast Lasers in Thin-Disk Geometry    339


                      other  mode-locked  laser  oscillator  technology.  Because  the  average
                      power is the product of the pulse energy and the repetition rate, decreas-
                      ing the repetition rate at constant pulse duration leads to higher pulse
                      energy and peak power. Ultrafast TDLs can generate greater than 10-mJ
                      pulses directly out of the oscillator, which makes them highly attractive
                      for applications in material structuring and high-field science. On the
                      other  hand,  semiconductor  lasers  are  ideally  suited  for  cost-efficient
                      mass production due to their epitaxial growth on wafers. Therefore,
                      they are attractive for such applications as telecommunication or optical
                      clocking  and  interconnects,  in  which  a  high  repetition  rate  is  more
                      important than high pulse energy. Furthermore, mode-locked VECSELs
                      cover a wide range of the infrared spectral range—between 0.95 mm and
                                                                    7
                      2.01 mm, depending on the semiconductor gain material.  This range is
                      in strong contrast to that of mode-locked solid-state TDLs, which up to
                                                     3+
                      now were only demonstrated with Yb -doped gain materials at a laser
                      wavelength around (1035 ± 10) nm. This section highlights the funda-
                      mental  reasons  for  the  different  operation  regimes  of  VECSELs  and
                      TDLs, which are clearly distinguishable in Fig. 13.6.

                      Average Power
                      The upper limit for the average power in mode-locked operation is
                      the maximum fundamental  mode output  power  in  CW  operation.
                      The presence of higher-order modes tends to introduce destabilizing


                         100 µJ
                          10 µJ
                                     TDL
                           1 µJ                        1 kW
                                                     100 W
                         100 nJ                     10 W
                        Pulse energy  10 nJ      100 mW
                                                   1 W
                           1 nJ
                         100 pJ                 10 mW
                                                                  VECSEL
                          10 pJ                1 mW

                           1 pJ
                         100 fJ
                             1 MHz   10 MHz   100 MHz   1 GHz    10 GHz  100 GHz
                                               Pulse repetition rate

                      Figure 13.6  Graphical representation of the different output parameter
                      regimes for SESAM mode-locked VECSELs and TDLs. The diagonal lines
                      correspond to constant average output power. The data for the TDL results
                      were taken from Refs. 12, 14, 33, 43, 58–67; the VECSEL results were
                      published in Refs. 21, 38, 68–83.
   365   366   367   368   369   370   371   372   373   374   375