Page 492 - Tunable Lasers Handbook
P. 492

452      Stephen Vincent Benson

                  energies. A  taper in the undulator cannot be  used to recover the power in this
                  case  since  the  deceleration  leg  has  a  limited  energy  aperture  that  would  be
                  exceeded for tapered operation.


                  2.2 Wiggler Tuning
                      The wiggler parameter can be varied by changing the magnetic field. If the
                  wiggler parameter is approximately equal to or greater than unity. this can lead
                  to  large changes  in  the  wavelength. In  permanent  magnet  undulators  one  can
                  vary the gap of the wiggler in order to vary the magnetic field strength. Electro-
                  magnetic wigglers can be varied by changing the energizing current. The group
                  at Orsay pioneered gap tuning on the ACO storage-ring-based laser [24]. Contin-
                  uous tuning was demonstrated over the bandwidth of  the mirrors. The VEPP-3
                  project at Novosibirsk demonstrated continuous tunability over the range of sev-
                  eral sets of mirrors by varying the current of their electromagnetic wiggler [25].
                  Both the Mark I11 FEL  and the Rockwell FEL at Stanford used gap tuning to
                  tune over a large wavelength range  123,261. The Mark I11 could tune continu-
                  ously over a 70% change in wavelength in a matter of seconds. This technique is
                  also used at Vanderbilt [27], the CLIO project at Orsay [28] and the FELIX proj-
                  ect at the FOM institute at Rinhuizen. The Netherlands [29]. The latter two sys-
                  tems  have  demonstrated  two  to  one  tuning  range  at  a  single  electron-beam
                  energy.
                      The advantages and disadvantages of this approach are opposite to those of
                  the energy tuning  approach. The power  output  is  fairly  independent  of  wave-
                  length over a large range. Tuning the laser  is quite  simple. It  is quite easy to
                  design for single-knob tuning by a factor of 2 to 4. This can be quite convenient
                  in a user facility, since no understanding of the computer control system is nec-
                  essary for the user. The tuning control can even be isolated so that it does not
                  interfere with the accelerator control system. The tuning cannot be carried out as
                  quickly as energy tuning in a mechanically tuned wiggler but might be quite fast
                  in a properly designed electromagnetic wiggler (especially a pulsed electromag-
                  netic undulator).
                      The largest disadvantage is  in  the constraints  placed  on the  wiggler con-
                  struction. Wiggler tuning is only useful when one has  a high K  wiggler. Great
                  care must be taken in the construction of the wiggler so that the input and output
                   steering is independent of  the magnetic field  strength. The field quality of  the
                  wiggler must remain high as the wiggler is tuned. All these constraints are most
                   easily satisfied for an electromagnet. There is more interest these days in using
                   electromagnets in future user facilities. The proposed high-average-power facil-
                   ity at CEBAF uses an electromagnet to tune over a range of 4 to  1 [30]. A new
                   facility at Princeton University will use a superconducting wiggler in a compact
                   infrared FEL (CIRFEL) [31] built by Northrop-Grumman.
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