<?xml version="1.0" encoding="UTF-8"?>
<xml>
  <records>
    <record>
       <contributors>
          <authors>
             <author>Bruchon, N.</author>
             <author>Karpov, I.</author>
             <author>Madysa, N.</author>
             <author>Papotti, G.</author>
             <author>Quartullo, D.</author>
          </authors>
       </contributors>
       <titles>
          <title>
             Operational Tool for Automatic Setup of Controlled Longitudinal Emittance Blow-Up in the CERN SPS
          </title>
       </titles>
       <publisher>JACoW Publishing</publisher>
       <pub-location>Geneva, Switzerland</pub-location>
		 <isbn>2226-0358</isbn>
		 <isbn>978-3-95450-238-7</isbn>
		 <electronic-resource-num>10.18429/JACoW-ICALEPCS2023-TUPDP086</electronic-resource-num>
		 <language>English</language>
		 <pages>723-728</pages>
       <keywords>
          <keyword>controls</keyword>
          <keyword>emittance</keyword>
          <keyword>operation</keyword>
          <keyword>target</keyword>
          <keyword>software</keyword>
       </keywords>
       <work-type>Contribution to a conference proceedings</work-type>
       <dates>
          <year>2024</year>
          <pub-dates>
             <date>2024-02</date>
          </pub-dates>
       </dates>
       <urls>
          <related-urls>
              <url>https://doi.org/10.18429/JACoW-ICALEPCS2023-TUPDP086</url>
              <url>https://jacow.org/icalepcs2023/papers/tupdp086.pdf</url>
          </related-urls>
       </urls>
       <abstract>
          The controlled longitudinal emittance blow-up is necessary to ensure the stability of high-intensity LHC-type beams in the CERN SPS. It consists of diffusing the particles in the bunch core by injecting a bandwidth-limited noise into the beam phase loop of the main 200 MHz RF system. Obtaining the correct amplitude and bandwidth of this noise signal is non-trivial, and it may be tedious and time-demanding if done manually. An automatic approach was developed to speed up the determination of optimal settings. The problem complexity is reduced by splitting the blow-up into multiple sub-intervals for which the noise parameters are optimized by observing the longitudinal profiles at the end of each sub-interval. The derived bunch lengths are used to determine the objective function which measures the error with respect to the requirements. The sub-intervals are tackled sequentially. The optimization moves to the next one only when the previous sub-interval is completed. The proposed tool is integrated into the CERN generic optimization framework that features pre-implemented optimization algorithms. Both single- and multi-bunch high-intensity beams are quickly and efficiently stabilized by the optimizer, used so far in high-intensity studies. A possible extension to Bayesian optimization is being investigated. 
       </abstract>
    </record>
  </records>
</xml>
