<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Edelen, J.P.</author>
             <author>Chase, B.E.</author>
             <author>Cullerton, E.</author>
             <author>Einstein, J.</author>
             <author>Varghese, P.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Low Level RF Control for the PIP-II Injector Test RFQ
          </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-TUPOA18</electronic-resource-num>
		 <language>English</language>
		 <pages>323-325</pages>
       <pages>TUPOA18</pages>
       <keywords>
          <keyword>ion</keyword>
          <keyword>rfq</keyword>
          <keyword>controls</keyword>
          <keyword>LLRF</keyword>
          <keyword>cavity</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-TUPOA18</url>
              <url>https://jacow.org/napac2016/papers/tupoa18.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The PIP-II injector test radio frequency quadrupole (RFQ) arrived at Fermilab in the fall of 2015. The RFQ is a 162.5MHz H⁻ accelerator with a nominal drive power of 100kW, which produces a bunched H⁻ beam at 2.1MeV. In this paper we discuss commissioning, operational performance, and improvements to the low level RF (LLRF) control system for the RFQ. We begin by describing the general system configuration and initial simulation results. We will then highlight temperature related issues in the high power RF system, which necessitate active control over the phase balance of the two amplifiers. Finally we demonstrate performance of the RF feedback and feed-forward compensation needed to meet specification during a 20-microsecond beam pulse.
       </abstract>
    </record>
  </records>
</xml>
