<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Garolfi, L.</author>
             <author>Bruni, C.</author>
             <author>El Khaldi, M.</author>
             <author>Vallerand, C.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Beam Dynamics for the ThomX Linac
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-182-3</isbn>
		 <electronic-resource-num>10.18429/JACoW-IPAC2017-THPIK008</electronic-resource-num>
		 <language>English</language>
		 <pages>4121-4123</pages>
       <pages>THPIK008</pages>
       <keywords>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-05</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-IPAC2017-THPIK008</url>
              <url>http://jacow.org/ipac2017/papers/thpik008.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          We report the results of a recent beam dynamics study that has led to promising working points for the split ThomX photoinjector. ThomX is a back-scattering Thomson light source that will use S-band electron Linac with an energy of 50 MeV to produce 45 keV high X-rays flux (10¹¹ - 10¹³ ph/s), by means of collision between electron bunches and laser pulses, in the energy range from 45 keV to 90 keV. Since Thomx has been conceived to maximise the average X-rays flux in a fixed bandwidth, the high rate electron-photon collisions impose a linear accelerator combined with a storage ring. The high performances of the accelerator are largely affected by the high quality of the electron beam at the interaction point in the ring. Beam specifications should be achieved at the interaction point to the extent that 1 nC, 50 nA average current per bunch with normalised rms transverse emittance less than 5 mm and around 0.3% energy spread, at the end of the linac. The beam dynamics along the linac has been studied to demonstrate the capability of the accelerator to meet the requirements for the high brightness electron beam using an RF photoinjector configuration.
       </abstract>
    </record>
  </records>
</xml>
