<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Sergeeva, D.Yu.</author>
             <author>Strikhanov, M.N.</author>
             <author>Tishchenko, A.A.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Incoherent and Coherent Polarization Radiation as Instrument of the Transversal Beam Size Diagnostics
          </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-WEPG62</electronic-resource-num>
		 <language>English</language>
		 <pages>793-795</pages>
       <pages>WEPG62</pages>
       <keywords>
          <keyword>radiation</keyword>
          <keyword>polarization</keyword>
          <keyword>factory</keyword>
          <keyword>target</keyword>
          <keyword>diagnostics</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-WEPG62</url>
              <url>http://jacow.org/ibic2016/papers/wepg62.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Polarization radiation, which includes diffraction radiation (DR), transition radiation (TR), Smith-Purcell radiation, and others, can be a good instrument for beam diagnostics. All information about the beam size is contained in the so-called form-factor of the beam. The form-factor represents the sum of two parts corresponding to the coherent and incoherent radiation*. Contrary to the general opinion the incoherent part does not always equal unity*, **. In this report we give theoretical description of the incoherent and coherent parts of the form-factor both for Gaussian and uniform distribution of the ultrarelativistic particles in the bunch*, ***. The theory constructed describes also the case of beam skimming the target, which leads to mixing of DR and TR***. We show that the incoherent part depends on the transversal size of the beam, and dependence differs for different distributions. The role of the incoherent part of the form-factor of the bunch for different parameters is discussed.
       </abstract>
    </record>
  </records>
</xml>
