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IPAC'23 - 14th International Particle Accelerator Conference

7–12 May 2023
Venice, Italy
Europe/Zurich timezone

IPAC'23

Session

MC04.1 - Hadron Accelerators (Contributed)

TUOGA
9 May 2023, 09:30
Venice, Italy

Venice, Italy

Lungomare Marconi 1861 30126 Lido di Venezia Italy

Conveners

MC04.1 - Hadron Accelerators (Contributed)

  • Yoichi Sato (Japan Proton Accelerator Research Complex)

Presentation materials

There are no materials yet.

  1. 1192. Laser assisted charge exchange injection into the ring at the SNS (TUOGA1)
    Timofey Gorlov (Oak Ridge National Laboratory)
    09/05/2023, 09:30
    MC4.T12: Beam Injection/Extraction and Transport
    Contributed Oral Presentation

    A realistic laser assisted charge exchange (LACE) scheme for 1.3~GeV H- beam injection into the Ring for Spallation Neutron Source is under development. The design considered here is supposed to demonstrate the possibility of H$^-$ charge exchange injection into the SNS ring as an alternative to carbon foil stripping. A realistic stripping magnet design is considered as an integrated part of...

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  2. 1014. Laser cooling taken to the extreme: cold relativistic intense beams of highly-charged heavy ions (TUOGA2)
    Dr Danyal Winters (GSI Helmholtz Centre for Heavy Ion Research)
    09/05/2023, 09:50
    MC4.A11: Beam Cooling
    Contributed Oral Presentation

    Recent storage ring experiments have demonstrated the power and the potential of laser cooling of bunched relativistic ion beams. Encouraged by this, the heavy-ion synchrotron SIS100 at FAIR (Darmstadt, Germany) will be equipped with a truly unique laser cooling facility. A sophisticated combination of 3 newly developed UV (257 nm) laser systems and modest rf-bunching will allow for fast...

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  3. 1864. Experimental measuremnet of quadrupole beam oscillating frequency at CSNS RCS (TUOGA3)
    Yue Yuan (Institute of High Energy Physics)
    09/05/2023, 10:10
    MC4.A04: Circular Accelerators
    Contributed Oral Presentation

    In high intensity proton synchrotrons, space charges effects will cause tune shift of the beam. When the betatron tune spreads over a resonance line, the betatron oscillation amplitude will get larger, causing large beam loss. Through the quadrupolar beam transfer function, the coherent space-charge tune shift of quadrupolar beam oscillations can be derived with quadrupole oscillating...

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