<?xml version="1.0" encoding="UTF-8"?>
<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Marqversen, O.</author>
             <author>Alves, D.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Beam Intensity Measurement in ELENA Using Orbit Pick-Ups
          </title>
       </titles>
       <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>2673-5350</isbn>
		 <isbn>978-3-95450-241-7</isbn>
		 <electronic-resource-num>10.18429/JACoW-IBIC2022-TUP30</electronic-resource-num>
		 <language>English</language>
		 <pages>296-299</pages>
       <keywords>
          <keyword>proton</keyword>
          <keyword>simulation</keyword>
          <keyword>feedback</keyword>
          <keyword>antiproton</keyword>
          <keyword>pick-up</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2022</year>
          <pub-dates>
             <date>2022-12</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-IBIC2022-TUP30</url>
              <url>https://jacow.org/ibic2022/papers/tup30.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          A bunched beam intensity measurement system for the CERN Extra Low ENergy Antiproton (ELENA) ring, using a cylindrical shoe-box electrostatic pick-up from the existing orbit system [1], is presented. The system has been developed to measure very challenging beam cur-rents, as low as 200nA corresponding to intensities of the order of 10⁷ antiprotons circulating with a relativistic beta of the order of 10-2. In this work we derive and show that the turn-by-turn beam intensity is proportional to the baseline of the sum signal and that, despite the AC-coupling of the system, the installed front-end electronics, based on a charge amplifier, not only guarantees the preservation of the bunch shape (up to a few tens of MHz), but also allows for an absolute calibration of the system. In addition, the linearity of the intensity measurements and their inde-pendence with respect to average beam position is evalu-ated using a standard electromagnetic simulation tool. Finally, experimental measurements throughout typical antiproton deceleration cycles are presented and their accuracy and precision are discussed.
       </abstract>
    </record>
  </records>
</xml>
