“…Momentum slip-stacking [15] consists of capturing two trains of bunches with independent beam controls, and by detuning them in momentum, bringing them closer together. Those gymnastics, originally proposed to increase bunch densities [16], can be applied in our case to interleave the bunches, as sketched in Fig. 3:…”
Section: Momentum Slip-stacking In the Spsmentioning
We review the performance of the ion injector chain in the light of the improvements which will take place in the near future, and we derive the expected luminosity gain for Pb-Pb collisions in the collider during the HL-LHC era.
“…Momentum slip-stacking [15] consists of capturing two trains of bunches with independent beam controls, and by detuning them in momentum, bringing them closer together. Those gymnastics, originally proposed to increase bunch densities [16], can be applied in our case to interleave the bunches, as sketched in Fig. 3:…”
Section: Momentum Slip-stacking In the Spsmentioning
We review the performance of the ion injector chain in the light of the improvements which will take place in the near future, and we derive the expected luminosity gain for Pb-Pb collisions in the collider during the HL-LHC era.
“…One possibility that has been studied is a technique called "slip stacking" [5]. This technique, which was first demonstrated at CERN in the 1970s [6], involves stacking beams in longitudinal phase space. Two subsequent Booster batches are injected into the Main Injector and captured at different energies (different radial positions) by subsets of the rf cavities running one harmonic number above and below the nominal harmonic number of the accelerator (h=588).…”
“…The slipping of bunched beams was first demonstrated at the CERN Super Proton Synchrotron (SPS) [6] but the emittance growth led to unacceptable particle losses. Fermilab has subsequently implemented slip stacking operationally since 2004 [4,7,8].…”
We study the stability of particles in slip-stacking configuration, used to nearly double proton beam intensity at Fermilab. We introduce universal area factors to calculate the available phase space area for any set of beam parameters without individual simulation. We find perturbative solutions for stable particle trajectories. We establish Booster beam quality requirements to achieve 97% slip-stacking efficiency. We show that slip-stacking dynamics directly correspond to the driven pendulum and to the system of two standing-wave traps moving with respect to each other.
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