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<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Pires, A.</author>
             <author>Delerue, N.</author>
             <author>Le Flanchec, V.</author>
             <author>Rosch, R.</author>
             <author>Touguet, J.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Evolution of the Inverse Compton Scattering X-ray Source of the ELSA Accelerator
          </title>
       </titles>
       <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>2673-7035</isbn>
		 <isbn>978-3-95450-224-0</isbn>
		 <electronic-resource-num>10.18429/JACoW-FLS2023-TU1C2</electronic-resource-num>
		 <language>English</language>
		 <pages>50-53</pages>
       <keywords>
          <keyword>laser</keyword>
          <keyword>electron</keyword>
          <keyword>alignment</keyword>
          <keyword>scattering</keyword>
          <keyword>cavity</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2024</year>
          <pub-dates>
             <date>2024-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-FLS2023-TU1C2</url>
              <url>http://jacow.org/fls2023/papers/tu1c2.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The Inverse Compton Scattering (ICS) X-ray source of ELSA accelerator at CEA-DAM, presents an efficient approach for generating X-rays with a compact linac. The source consists of a 30 MeV, 15 ps rms, up to 3 nC electron beam; and a table-top Nd:YAG laser. X-rays are produced in the 10-80 keV range, higher X-ray energies achieved with frequency doubling of the laser. The yield is increased by a factor of 8 thanks to an optical mirror system developed at CEA, folding the laser beam path and accumulating successive laser pulses. We present a new version of the device, with improvement of mechanical constraints management, adjunction of motorized mirrors, and a new imaging system. A Chirped Pulse Amplification (CPA) system was also designed, enabling higher amplification levels without exceeding laser damage threshold. The uniqueness of this CPA system lies in its use of a short wavelength bandwidth, ±250 pm after Self-Phase Modulation (SPM) broadening, and a line density of 1850 lines/mm for the gratings of the compressor. The pulse is stretched with a chirped fiber Bragg grating (CFBG) before amplification in Nd:YAG amplifiers, and compressed by a double pass grating compressor.
       </abstract>
    </record>
  </records>
</xml>
