<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Divall, M.C.</author>
             <author>Hauri, C.P.</author>
             <author>Hunziker, S.</author>
             <author>Romann, A.</author>
             <author>Trisorio, A.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Laser Arrival Time Measurement and Correction for the SwissFEL Lasers
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-177-9</isbn>
		 <electronic-resource-num>10.18429/JACoW-IBIC2016-WEPG52</electronic-resource-num>
		 <language>English</language>
		 <pages>764-767</pages>
       <pages>WEPG52</pages>
       <keywords>
          <keyword>laser</keyword>
          <keyword>timing</keyword>
          <keyword>gun</keyword>
          <keyword>FEL</keyword>
          <keyword>experiment</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2017</year>
          <pub-dates>
             <date>2017-02</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-IBIC2016-WEPG52</url>
              <url>http://jacow.org/ibic2016/papers/wepg52.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          SwissFEL will ultimately produce sub-fs X-ray pulses. Both the photo-injector laser and the pump lasers used for the experimental end stations therefore have tight requirements for relative arrival time to the machine and the X-rays. The gun laser oscillator delivers excellent jitter performance at ~20fs integrated from 10Hz-10MHz. The Yb:CaF2 regenerative amplifier, with an over 1km total propagation path, calls for active control of the laser arrival time. This is achieved by balanced cross-correlation against the oscillator pulses and a translation stage before amplification. The experimental laser, based on Ti:sapphire laser technology will use a spectrally resolved cross-correlator to determine relative jitter between the optical reference and the laser, with fs resolution. To be able to perform fs resolution pump-probe measurements the laser has to be timed with the X-rays with &lt;10fs accuracy. These systems will be integrated into the machine timing and complemented by electron bunch and X-ray timing tools. Here we present the overall concept and the first results obtained on the existing laser systems.
       </abstract>
    </record>
  </records>
</xml>
