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Benedikt, M.

Paper Title Page
TU6PFP055 An RF Scenario for Protons and Ions in the PS2 1406
 
  • S. Hancock, M. Benedikt, C. Carli
    CERN, Geneva
 
 

The PS2 is proposed as a replacement for the ageing PS and will provide proton beams with kinetic energies up to 50 GeV. It must also deliver Pb54+ ions, for which the revolution frequency swing will be more than a factor of two. The favoured rf scenario considers a 40 MHz accelerating system and is motivated by the possibility of chopping at up to 40 MHz in the SPL, the proposed proton injector. Using the same principal rf system for ions implies pushing for an unprecedented tuning range and the introduction of a new rf system in LEIR, the existing ion source. We present a solution to the disparate requirements of protons and ions based on a 40 MHz rf system with switchable tuning ranges to cover the large frequency swing required.

 
TU6PFP056 Longitudinal Painting Schemes for H- Charge Exchange Injection into the PS2 1409
 
  • C. Carli, M. Benedikt, S. Hancock
    CERN, Geneva
  • V. Knuenz, I. Vonderhaid
    TU Vienna, Wien
 
 

Minimization of direct space charge tune shift at injection into the PS2 is important for the reduction of beam losses. A determining parameter for the tune shift is the bunching factor, defined as mean current over peak current for one RF period. Various longitudinal painting schemes for PS2 injection, all based on synchrotron motion, have been studied with respect to the resulting bunching factors. In particular, schemes using the SPL high-frequency chopper and different energy-spreads and offsets of the incoming beam as well as SPL beam energy modulations on have been simulated with the ESME code.

 
TU6RFP027 Resonant Third-Integer Extraction from the PS2 1593
 
  • M. Gyr, W. Bartmann, M. Benedikt, B. Goddard, M. Meddahi
    CERN, Geneva
  • A. Koschik
    ETH, Zürich
  • D. Mayani Parás
    UNAM, México, D.F.
 
 

For the proposed PS2 accelerator several extraction systems are needed, including a slow third-integer resonant extraction. The requirements are presented together with the conceptual considerations for the sextupole locations and strengths, the separatrices at the extraction elements and the aperture implications for the overall machine. Calculations of the phase space separatrices have been computed with a new code for the physics of slow resonant extraction, which is briefly reviewed. Implications for the extraction equipment design and for the injection-extraction straight section optics are discussed.

 
WE1GRI03 Design Optimization of PS2 1828
 
  • M. Benedikt, B. Goddard
    CERN, Geneva
 
 

The PS2 will replace the present CERN-PS as the LHC pre-injector. It will have twice the PS energy and twice the circumference. Extensive design optimization is presently ongoing with the aim of starting the PS2 construction around 2011 and delivering beams for physics in 2017. The talk describes the various PS2 design constraints, the optimization steps, and the path towards the final design.

 

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Slides

 
WE6RFP017 Collimation Considerations for PS2 2817
 
  • J. Barranco
    UPC, Barcelona
  • W. Bartmann, M. Benedikt, Y. Papaphilippou
    CERN, Geneva
 
 

A main concern in high intensity rings is the evaluation of uncontrolled losses and their minimization using collimation systems. A two-stage systemis foreseen for the PS2. The fundamental design strategy for the collimation design is presented, including machine apertures and collimator materials. The dependence of the collimator system efficiency on the primary scraper length and the impact parameter of the particle is evaluated for different collimator locations. Beam loss maps are finally produced displaying the detailed power load deposited around the ring.

 
TH6PFP039 Beam Loss Control for the Unstripped Ions from the PS2 Charge Exchange Injection 3790
 
  • W. Bartmann, J. Barranco, M. Benedikt, B. Goddard, T. Kramer, Y. Papaphilippou, H. Vincke
    CERN, Geneva
 
 

Control of beam losses is an important aspect of the H- injection system for the PS2, a proposed replacement of the CPS in the CERN injector complex. H- ions may pass the foil unstripped or be partially stripped to excited H0 states which may be stripped in the subsequent strong-field chicane magnet. Depending on the choice of the magnetic field, atoms in the ground and first excited states can be extracted and dumped. The conceptual design of the waste beam handling is presented, including local collimation and the dump line, both of which must take into account the divergence of the beam from stripping in fringe fields. Beam load estimates and activation related requirements of the local collimators and dump are briefly discussed.

 
TH6PFP043 Orbit, Optics and Chromaticity Correction for PS2 Negative Momentum Compaction Lattices 3802
 
  • Y. Papaphilippou, J. Barranco, W. Bartmann, M. Benedikt, C. Carli
    CERN, Geneva
  • R. De Maria, S. Peggs, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

The effect of magnet misalignments in the beam orbit and linear optics functions are reviewed and correction schemes are applied to the negative momentum compaction lattices of PS2. Chromaticity correction schemes are also proposed and tested with respect to off-momentum optics properties. The impact of the correction schemes in the dynamic aperture of the different lattices is finally evaluated.

 
TH6PFP044 Linear Optics Design of Negative Momentum Compaction Lattices for PS2 3805
 
  • Y. Papaphilippou, J. Barranco, W. Bartmann, M. Benedikt, C. Carli, B. Goddard
    CERN, Geneva
  • R. De Maria, S. Peggs, D. Trbojevic
    BNL, Upton, Long Island, New York
 
 

In view of the CERN Proton Synchrotron proposed replacement with a new ring (PS2), a detailed optics design as been undertaken following the evaluation of several lattice options. The basic arc module consists of cells providing negative momentum compaction. The straight section is formed with a combination of FODO and quadrupole triplet cells, to accommodate the injection and extraction systems, in particular the H- injection elements. The arc is matched to the straight section with a dispersion suppressor and matching module. Different lattices are compared with respect to their linear optics functions, tuning flexibility and geometrical acceptance properties.