<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Gupta, L.</author>
             <author>Kim, K.-J.</author>
             <author>Lindberg, R.R.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Performance of a Combined System Using an X-Ray FEL Oscillator and a High-Gain FEL Amplifier
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-180-9</isbn>
		 <electronic-resource-num>10.18429/JACoW-NAPAC2016-WEPOB32</electronic-resource-num>
		 <language>English</language>
		 <pages>974-976</pages>
       <pages>WEPOB32</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>FEL</keyword>
          <keyword>radiation</keyword>
          <keyword>simulation</keyword>
          <keyword>laser</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-NAPAC2016-WEPOB32</url>
              <url>https://jacow.org/napac2016/papers/wepob32.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The LCLS-II at SLAC will feature a 4 GeV CW superconducting (SC) RF linac [1] that can potentially drive a 5th harmonic X-Ray FEL Oscillator to produce fully coherent, 1 MW photon pulses with a 5 meV bandwidth at 14.4 keV [2]. The XFELO output can serve as the input seed signal for a high-gain FEL amplifier employing fs electron beams from the normal conducting SLAC linac, thereby generating coherent, fs x-ray pulses with ~TW peak powers using a tapered undulator after saturation [3]. Coherent, intense output at several tens of keV will also be feasible if one considers a harmonic generation scheme. Thus, one can potentially reach the 42 keV photon energy required for the MaRIE project [4] by beginning with an XFELO operating at the 5th harmonic to produce 8.4 keV photons using a 3.1 GeV SCRF linac, and then subsequently using the high-gain harmonic generation scheme to generate and amplify the 5th harmonic at 42 keV [5]. We report extensive GINGER simulations that determine an optimized parameter set for the combined system. [1] "Linac Coherent Light Source-II Conceptual Design Report," SLAC-R-978 (2011)
       </abstract>
    </record>
  </records>
</xml>
