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9 Tunable Free-Electron Lasers   46%
                     range of wavelength coverage as possible. This section describes the major facil-
                     ities available now  and one facility that  is  scheduled to  come on line  shortly.
                     More  detailed  information  can  be  obtained  from  the  individual  institutions.
                     Interested readers can contact the institution which seems to have the best match
                     of  capabilities  and  submit  a  proposal  to  use  their  facility. Each  facility  has
                     strengths and weaknesses and is best matched to a given range of  experiments.
                     For each laboratory. I will describe the  available wavelength range, the power
                     available over the wavelength range. the temporal and spectral structure, and any
                     unique features of  the facility. Most of  the facilities are driven by  rf  linacs and
                     therefore have a micropulse/macropulse structure. so the power quoted in the lit-
                     erature  may  be  peak  power  during the  micropulse,  average  power  during the
                     macropulse,  or,  rarely,  the  long-term  average  power.  One  can  also  quote
                     micropulse energy or macropulse energy. For most research applications average
                     power is unimportant. The energy per macropulse and micropulse and the pulse
                     lengths are usually the most important quantities. For all the facilities, the mode
                     quality is nearly diffraction limited, so that feature will not be  discussed here.
                     Another common feature is that the lasers are generally  locked to the a-c line
                     frequency for stability purposes. Some of the properties of the facilities are listed
                     in Table 2. Note that only ranges of power and pulse lengths can be giwn since
                     they often vary by  as much as a factor of  10 as the wavelength is changed. The
                     power, microbunch length, and spectral bandwidth in rf  linear accelerator-based
                     devices can be strongly dependent on the cavity length, sometimes varying by as
                     much as a factor of  10. It is therefore useful for the user to have control of  the
                     cavity length to optimize the power, bunch length, or spectral width. Note that



                     TABLE 2  Properties of User Facilities around the World"

                                          IValelength  Micropulse  Macropulse  Micropulse  Macropulse
                                          range    frequency   frequency   power   power
                     Location of facility   (pm)   (MHz)    tHz)     (MW)     (kW)

                     CLIO. Orsaj. France   2-17.5   31-250   1-50    1-10     1-6
                     Mark 111. Duke University   3-9   2857   1-30   0.5-3    2-30
                     FELIX. FOM, Netherlands   6-100   1000   3      0.1-3    1-10
                     CIRFEL, Princeton
                       Universityb        5-15     142.8    10       1-5      1-7
                     SCAFEL, Stanford University  3-61   11.82   1-120   0.1-1   0.001-0.01
                     CFELS. UCSB          62-2500   /'      0.25-4            1-27
                     Vanderbilt University   2-7.7   2857   1-30     1-10     2-30
                     aFor more details. see the texr descriptions. Third harmonic lasing is not included in the wavelength
                      range whez available.
                     bSystem being commissioned.
                     'This  accelerator has no micropulse structure.
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