<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Gadjev, I.I.</author>
             <author>Emma, C.</author>
             <author>Nause, A.</author>
             <author>Rosenzweig, J.B.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             High-Gain FEL in the Space-Charge Dominated Raman Limit
          </title>
       </titles>
       <pages>TUP008</pages>
       <keywords>
          <keyword>FEL</keyword>
          <keyword>space-charge</keyword>
          <keyword>undulator</keyword>
          <keyword>electron</keyword>
          <keyword>simulation</keyword>
       </keywords>
       <dates>
          <year>2015</year>
          <pub-dates>
             <date>2015-12</date>
          </pub-dates>
       </dates>
       <abstract>
          While FEL technology has reached the EUV and X-ray regime at existing machines such as LCLS and SACLA, the scale of these projects is often impractical for research and industrial applications. Sub-millimeter period undulators can reduce the size of a high-gain EUV FEL, but will impose stringent conditions on the electron beam. In particular, a high-gain EUV FEL based on undulators with a sub-millimeter period will require electron beam currents upwards of 1 kA at energies below 100 MeV. Coupled with the small gap of such undulators and their low undulator strengths, K &lt; 0.1, these beam parameters bring longitudinal space-charge effects to the foreground of the FEL process. When the wavelength of plasma oscillations in the electron beam becomes comparable to the gain-length, the 1D theoretical FEL model transitions from the Compton to the Raman limit. In this work, we investigate the behavior of the FEL's gain-length and efficiency in these two limits. The starting point for the analysis was the one-dimensional FEL theory including space-charge forces. The derived results were compared to numerical results of Genesis 1.3 simulations. This theoretical model predicts that in the Raman limit, the gain-length scales as the beam current to the -1/4th power while the efficiency plateaus to a constant.
       </abstract>
    </record>
  </records>
</xml>
