<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Mulyani, E.</author>
             <author>Flanagan, J.W.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Design of Coded Aperture Optical Elements  for SuperKEKB X-ray Beam Size Monitors
          </title>
       </titles>
		 <publisher>JACoW</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>978-3-95450-176-2</isbn>
		 <electronic-resource-num>10.18429/JACoW-IBIC2015-TUPB025</electronic-resource-num>
		 <language>English</language>
		 <pages>377-380</pages>
       <pages>TUPB025</pages>
       <keywords>
          <keyword>detector</keyword>
          <keyword>photon</keyword>
          <keyword>optics</keyword>
          <keyword>electron</keyword>
          <keyword>emittance</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2016</year>
          <pub-dates>
             <date>2016-01</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>http://dx.doi.org/10.18429/JACoW-IBIC2015-TUPB025</url>
              <url>http://accelconf.web.cern.ch/AccelConf/IBIC2015/papers/tupb025.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          We describe the design of coded aperture optical elements for the SuperKEKB x-ray beam size monitors. X-ray beam profile monitor are being installed in each ring of SuperKEKB (LER and HER) to provide high resolution bunch-by-bunch, turn-by-turn measurement capability for low emittance tuning, collision tuning and instability measurements. We use two types of optical elements, single-slit (pinhole) and multi-slit optical elements (coded apertures, CA). CA imaging offers greater open aperture than a single pinhole, for greater photon throughput and better statistical resolution for single-shot measurements. X-rays produced by a hard-bend magnet pass through a pinhole or CA optical element onto a detector. The resolution is obtained by calculating the differences between the images recorded by the detector for various simulated beam sizes, for a given number of photons. The CA elements that we have designed for use at SuperKEKB are estimated to provide 1.25-2.25 microns resolution for 10-25 microns of vertical beam sizes at 1 mA bunches. We present the design principle and optimizing process used to optimize the resolution at various beam sizes for SuperKEKB.
       </abstract>
    </record>
  </records>
</xml>
