Long-Range Beam-Beam Compensation in RHIC
2010
https://doi.org/10.18429/JACOW-IPAC2010-TUPD065…
3 pages
1 file
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Abstract
In order to avoid the effects of long-range beam-beam interactions which produce beam blow-up and deteriorate beam life time, a compensation scheme with current carrying wires has been proposed. Two long-range beam-beam compensators were installed in RHIC rings in 2006. The effects of the compensators have been experimentally investigated. An indication was observed that the compensators are beneficial to beam life time in measurements performed in RHIC during 2009. In this paper, we report the effects of wire compensator on beam loss and emittance for proton-proton beams at collision energy.
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References (3)
- J.P. Koutchouk, LHC Project Note 223, CERN (2000).
- R. Calaga et al, http://www.c-ad.bnl.gov/APEX/APEX2009 (2009).
- H.J. Kim et al., PRSTAB 12, 031001 (2009).