Momentum slip-stacking of the nominal I-LHC beam in the SPS Particle simulations (preliminary) T. Argyropoulos, E. Shaposhnikova LIU-SPS BD WG 30/01/2014.

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Presentation transcript:

Momentum slip-stacking of the nominal I-LHC beam in the SPS Particle simulations (preliminary) T. Argyropoulos, E. Shaposhnikova LIU-SPS BD WG 30/01/2014

History Previous studies in the SPS to increase bunch intensity: – Protons: D. Boussard and Y. Mizumachi. Production of beams with high line-density by azimuthal combination of bunches in a synchrotron. IEEE Trans. Nucl. Sci. Vol. NS-26 No. 3, 3623, June – Ions: T. Linnecar. Azimuthal combination - slip stacking. Slides, SLI Meeting , CERN proposal (R. Garoby): Interpose two super batches of the nominal I-LHC Beam (100 ns bunch spacing)  beam of 50 ns bunch spacing. Same way of implementation

Slip-stacking procedure

Buckets do not interact in that case In reality we need α>5 for both batches to slide without emittance blow- up Simulations are focused on the last part – recapture of the batches

Slip-stacking parameters Based on: T. Bohl, Note Flat bottom: not studied here – large recapture voltage needed – influence of RF noise, IBS and space charge (observed under present operational conditions)

Slip-stacking parameters Flat top (450 GeV/c): – Longitudinal emittance: ε L = eVs/A – Initial RF Voltage: VRF = MV (filling factor of 0.9) – momentum separation: dp/p=2x10 -3 – min. dist. of mean radial pos: ΔR = 6.8 mm Simulations were performed for the last part  bring the batches back starting from the maximum distance from the central orbit

Designed RF programs Programs calculated for a single RF for constant bucket area

Varying parameters Δf RF Time of the cycle, T cycle Time of recapture V RF recapture T cycle Δf RF

Example Δf RF = 4f s Initial losses (~2 %) can be possibly eliminated

Example Δf RF = 4f s ε L = 0.3 eVs/A Losses = 10 % Decreasing VRF = 0.7 MV ε L = 0.29 eVs/A Losses = 15 %

Δf RF < 4f s ε L = 0.3 eVs/A Losses = 7 % Decreasing VRF = 0.7 MV ε L = 0.28 eVs/A Losses = % For Δf RF > 4f s we don’t gain in intensity but more emittance blow-up

Increasing Tcycle Increasing the total time reduces the losses by ~ 20 % And also the final ε L can be reduced by a ~5% More time is still needed for fine tuning

Summury Time required for manipulations: ~ 1.0 s t tot = 0.45 s (slipping) s (up-down) s (filamentation) (maybe more time will be needed, +0.2 s ?) Beam parameters: losses >7%, emittance blow- up by ~ factor 2.5 => OK for extraction to LHC after 200 MHz upgrade in the SPS (or 200 MHz in LHC) Further optimization is needed!