A   B   C   D   E   F   G   H   I   K   L   M   N   O   P   Q   R   S   T   U   V   W  

beam-beam-effects

Paper Title Other Keywords Page
TUPEB021 Conceptual Design of the Muon Collider Ring Lattice sextupole, collider, lattice, dynamic-aperture 1563
 
  • Y. Alexahin, E. Gianfelice-Wendt, A.V. Netepenko
    Fermilab, Batavia
 
 

Muon collider is a promising candidate for the next energy frontier machine. However, in order to obtain peak luminosity in the 1035/cm2/s range the collider lattice design must satisfy a number of stringent requirements, such as low beta at IP (beta*<1 cm), large momentum acceptance and dynamic aperture and small value of the momentum compaction factor. Here we present a particular solution for the interaction region optics whose distinctive feature is a three-sextupole local chromatic correction scheme. Together with a new flexible momentum compaction arc cell design this scheme allows to satisfy all the above-mentioned requirements and is relatively insensitive to the beam-beam effect.

 
TUPD068 Simulations of Head-on Beam-Beam Compensation at RHIC and LHC simulation, electron, luminosity, betatron 2081
 
  • A. Valishev
    Fermilab, Batavia
 
 

Electron lenses are proposed as a way to mitigate head-on beam-beam effects for the LHC upgrade. An extensive effort was put together within the US LARP in order to develop numerical simulations of beam-beam effects in the presence of electron lenses. In this report the results of beam-beam simulations for RHIC and LHC are presented. The effect of electron lenses is demonstrated and sensitivity of beam-beam compensation to imperfections is discussed.

 
THPE100 Bunch Length Effects in the Beam-beam Compensation with an Electron Lens electron, proton, heavy-ion, collider 4755
 
  • W. Fischer, Y. Luo, C. Montag
    BNL, Upton, Long Island, New York
 
 

Electron lenses for the head-on beam-beam compensation are under construction at the Relativistic Heavy Ion Collider. The bunch length is of the same order as the beta-function at the interaction point, and a proton passing through another proton bunch experiences a substantial phase shift which modifies the beam-beam interaction. We review the effect of the bunch length in the single pass beam-beam interaction, apply the same analysis to a proton passing through a long electron lens, and study the single pass beam-beam compensation with long bunches.