9–11 Nov 2017
CERN
Europe/Zurich timezone

Session

Session 3: Beam quality and improving spill structure

10 Nov 2017, 08:45
6/2-024 - BE Auditorium Meyrin (CERN)

6/2-024 - BE Auditorium Meyrin

CERN

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Conveners

Session 3: Beam quality and improving spill structure

  • Verena Kain (CERN)
  • Sergey Ivanov (Institute for High Energy Physics (IHEP))

Presentation materials

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  1. Johannes Bernhard (CERN)
    10/11/2017, 08:45

    We will present a short overview of the experimental requirements on the spill quality with an emphasis on the CERN North Area experiments. Together with a short introduction of categories of users at CERN, the main characteristics of the experiments concerning instantaneous intensity, monitoring and impact of non-flat spill structures will be discussed. Finally, a list of possible...

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  2. Dr Peter Schmid
    10/11/2017, 09:05
  3. Dr Bernd Alfred Lorentz (Forschungszentrum Jülich)
    10/11/2017, 09:25
  4. Dr Claude Krantz (Marburger Ionenstrahl-Therapiezentrum)
    10/11/2017, 09:45

    At the p/12C6+ synchrotron of the Marburg Ion-Beam Therapy Centre we use slow extraction by transverse noise (KO-) excitation. The system is equipped with a Dynamic Intensity Control (DIC) loop allowing fast modulation of the spill rate during extraction. By careful adjustment of the exciter noise spectrum relative to the small-amplitude particle tune and the extraction tune, it is possible to...

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  5. Masahito Tomizawa (masahito.tomizawa@kek.jp)
    10/11/2017, 10:05
  6. Francesco Maria Velotti (CERN)
    10/11/2017, 10:25
  7. Peter Forck (GSI)
    10/11/2017, 11:15
  8. Stefan Sorge
    10/11/2017, 11:35
  9. Jean-Paul Burnet (CERN)
    10/11/2017, 11:55
  10. Kevin Brown (Brookhaven National Laboratory)
    10/11/2017, 12:15
  11. L. Falbo
    10/11/2017, 12:35

    After a short overview of CNAO machine, the presentation shows how the spill is controlled during extraction:
    momentum-amplitude extraction, HEBT chopper, RF phase jump, Empty bucket channelling, Empty sweeping Bucket channelling, Air core quad feedback.
    Each topic is first presented under the theoretical point of view, then the results in CNAO machine are shown.

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