Optimization of the LHC Beam Cleaning System With Respect to Beam Losses in the High Luminosity Insertions

The LHC design performance is achievable only with a dedicated beam cleaning embedded in the lattice. The effect of the system on the beam loss distribution in the entire machine is studied with emphasis on the two high luminosity insertions. Realistic Monte-Carlo simulations are described, which include a model for beam halo interactions with collimators and other components, multi-turn particle tracking in the lattice, hadronic and electromagnetic shower simulations, and thermal and stress analyses. Methods to mitigate beam-induced effects in the interactions regions at operational and accidental beam loss are proposed, both for injection and collision conditions

Development of hollow electron beams for proton and ion collimation

Magnetically confined hollow electron beams for controlled halo removal in high-energy colliders such as the Tevatron or the LHC may extend traditional collimation systems beyond the intensity limits imposed by tolerable material damage. They may also improve collimation performance by suppressing loss spikes due to beam jitter and by increasing capture efficiency. A hollow electron gun was designed and built. Its performance and stability were measured at the Fermilab test stand. The gun will be installed in one of the existing Tevatron electron lenses for preliminary tests of the hollow-beam collimator concept, addressing critical issues such as alignment and instabilities of the overlapping proton and electron beams.Comment: 3 pp. 1st International Particle Accelerator Conference: IPAC'10, 23-28 May 2010: Kyoto, Japa

Protecting LHC Components Against Radiation Resulting From an Unsynchronized Beam Abort

The effect of possible accidental beam loss in the LHC on the IP5 and IP6 insertion elements is studied via realistic Monte Carlo simulations. The scenario studied is beam loss due to unsynchronized abort at an accidental prefire of one of the abort kicker modules. Simulations show that this beam loss would result in severe heating of the IP5 and IP6 superconducting (SC) quadrupoles. Contrary to the previous considerations with a stationary set of collimators in IP5, collimators in IP6 close to the cause are proposed: a movable collimator upstream of the Q4 quadrupole and a stationary one upstream of the extraction septum MSD. The calculated temperature rise in the optimal set of collimators is quite acceptable. All SC magnets are protected by these collimators against damage