Page 50 - High Power Laser Handbook
P. 50

22    G a s , C h e m i c a l , a n d F r e e - E l e c t r o n L a s e r s                                                           Excimer Lasers     23




                       Reset
                  Power              TR 1
                  supply                       L 1   L     L            C  R
                                                      2    3             c  c
                                 C 0       C 1    C 2    C  3
                                                               C  p  D   L  5
                  Trigger
                                     IGBT

                        IGBT                    Solid state pulser  Discharge
                        driver
                 Figure 2.3  Example of a discharge circuit with a solid-state pulser and multistage
                 compression. C : storage capacitor; IGBT (insulated gate bipolar transistor): solid-
                            0
                 state switch; TR : transformer; C –C : magnetic compression circuit capacitors;
                                         1
                                            3
                             1
                 L – L : magnetic compression inductors; Rc, Cc: circuit of corona preionizer;
                     3
                  1
                 D: discharge electrodes (in laser tube); Cp: peaking capacitor, L : discharge coil.
                                                                5
                      beam’s spatial uniformity. To obtain the required peak currents and
                      voltage rise times, high-power excimer lasers use multistage pulse
                      compression techniques and all-solid-state switching through mod-
                      ern semiconductor switches, such as thyristors, gate turn-offs (GTOs),
                      or  insulated  gate  bipolar  transistors  (IGBTs).  Magnetic  pulse  com-
                      pression  circuits  deliver  the  electrical  energy  to  the  laser  cavity  in
                      multiple steps, as is done in a basic capacitor transfer (C-C transfer)
                      circuit.
                         The primary solid-state switching circuit transfers the energy
                      on a slow timescale from the primary energy store (C ) to interme-
                                                                    0
                      diate energy stores (C , C , C ) in a multistage magnetic compres-
                                               3
                                            2
                                         1
                      sion circuit. From there, the energy is rapidly transferred into the
                      laser cavity for the discharge. The transformation of the pulse from
                      a low-peak power to the fast high-peak power pulse required by
                      the discharge is schematically shown in Fig. 2.4. The transfer from
                      C  to C  uses a step-up transformer, which converts the primary
                             1
                       0
                      charging voltage of C  to the required high voltage level of 20
                                          0
                      to  40  kV  in  the  secondary  circuit.  From  C   to  the  final  peaking
                                                            0
                      capacitors (C ), the pulse is typically compressed by a factor 50 to
                                 p
                      100. The inductors L , L , and L  saturate after their hold-off time
                                           2
                                        1
                                                  3
                      and then rapidly transfer the energy to the next stage. The satura-
                      ble inductors are then reset to the original unsaturated state by the
                      reset current that is actively supplied. An all-solid-state switching
                      technology  constitutes  a  major  advancement  toward  highly  reli-
                      able industrial excimer laser systems, because solid-state switches
                      are maintenance free and have demonstrated a practically unlim-
                      ited lifetime. Today all high-power industrial excimer lasers and
                      high-repetition-rate  lasers  for  microlithography  applications  use
                      solid-state  switching  technology  and  routinely  achieve  mainte-
                      nance-free operating times of several 10,000 hours.
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