<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Lumpkin, A.H.</author>
             <author>Edstrom, D.R.</author>
             <author>Ruan, J.</author>
             <author>Santucci, J.K.</author>
             <author>Thurman-Keup, R.M.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Initial Observations of Micropulse  Elongation of Electron Beams in a SCRF Accelerator*
          </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-TUPOA26</electronic-resource-num>
		 <language>English</language>
		 <pages>337-340</pages>
       <pages>TUPOA26</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>electron</keyword>
          <keyword>laser</keyword>
          <keyword>gun</keyword>
          <keyword>MMI</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-TUPOA26</url>
              <url>https://jacow.org/napac2016/papers/tupoa26.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Commissioning at the SCRF accelerator at the Fermilab Accelerator Science and Technology (FAST) Facility has included the implementation of a versatile bunch-length monitor located after the 4-dipole chicane bunch compressor for electron beam energies of 20-50 MeV and integrated charges in excess of 10 nC. The team has initially used a Hamamatsu C5680 synchroscan streak camera. An Al-coated Si screen was used to generate optical transition radiation (OTR) resulting from the beam's interaction with the screen. The chicane bypass beamline allowed the measurements of the bunch length without the compression stage at the downstream beamline location using OTR and the streak camera. The UV component of the drive laser had previously been characterized with a Gaussian fit σ of 3.5-3.7 ps**. However, the uncompressed electron beam is expected to elongate due to space charge forces in an initial 1.5-m drift from the gun to the first SCRF accelerator cavity. We have observed electron beam bunch lengths from 5 to 14 ps (σ) for micropulse charges of 60 pC to 800 pC, respectively. Commissioning of the system and initial results with uncompressed and compressed beam will be presented.
       </abstract>
    </record>
  </records>
</xml>
