<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Krishnan, M.</author>
             <author>Chapman, S.F.</author>
             <author>Irfan, I.</author>
             <author>Spradlin, J.K.</author>
             <author>Tian, H.</author>
             <author>Velas, K.M.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Bulk Niobium Polishing and Electropolishing Steps for Thinfilm Coated Copper SRF Cavities
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-178-6</isbn>
		 <electronic-resource-num>10.18429/JACoW-SRF2015-TUPB034</electronic-resource-num>
		 <language>English</language>
		 <pages>633-637</pages>
       <pages>TUPB034</pages>
       <keywords>
          <keyword>cavity</keyword>
          <keyword>SRF</keyword>
          <keyword>ion</keyword>
          <keyword>plasma</keyword>
          <keyword>cathode</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2015</year>
          <pub-dates>
             <date>2015-12</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-SRF2015-TUPB034</url>
              <url>http://srf2015.vrws.de/papers/tupb034.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          Alameda Applied Sciences Corporation (AASC) grows Nb thin films via Coaxial Energetic Deposition (CED) from a cathodic arc plasma. The plasma consists of 60-120eV Nb ions (Nb+ and Nb++) [1] that penetrate a few monolayers into the substrate [2] and enable sufficient surface mobility to ensure that the lowest energy state (crystalline structure with minimal defects) is accessible to the film [3]. One limitation of CED thinfilms is the presence of Nb macroparticles (~0.1-10 microns) that could be deleterious to high field performance of the SRF cavity. One way to remove such macroparticles [4] is to grow a thick film (~3-5 microns), followed by mechanical polishing (MP) using the finest media as might be applied in Centrifugal Barrel Polishing (CBP) to achieve a 0.4 micron surface figure, and an electropolishing (EP) step to remove ~1 micron of Nb that also removes all traces of embedded media in the film. The residual 2-4 micron Nb film should more nearly resemble the surface of a bulk Nb cavity that has been subjected to the same steps. This paper describes experiments conducted on Cu coupons as a prelude to an SRF Cu cavity coating.
       </abstract>
    </record>
  </records>
</xml>
