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arxiv: 1410.5315 · v1 · pith:2GLVP6ACnew · submitted 2014-10-20 · ⚛️ physics.acc-ph

Status of head-on beam-beam compensation in RHIC

W. Fischer (Brookhaven) , Z. Altinbas (Brookhaven) , M. Anerella (Brookhaven) , M. Blaskiewicz (Brookhaven) , D. Bruno (Brookhaven) , M. Costanzo (Brookhaven) , W.C. Dawson (Brookhaven) , D.M. Gassner (Brookhaven)
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X. Gu (Brookhaven) R.C. Gupta (Brookhaven) K. Hamdi (Brookhaven) J. Hock (Brookhaven) L.T. Hoff (Brookhaven) R. Hulsart (Brookhaven) A.K. Jain (Brookhaven) R. Lambiase (Brookhaven) Y. Luo (Brookhaven) M. Mapes (Brookhaven) A. Marone (Brookhaven) R. Michnoff (Brookhaven) T.A. Miller (Brookhaven) M. Minty (Brookhaven) C. Montag (Brookhaven) J. Muratore (Brookhaven) S. Nemesure (Brookhaven) D. Phillips (Brookhaven) A.I. Pikin (Brookhaven) S.R. Plate (Brookhaven) P. Rosas (Brookhaven) L. Snydstrup (Brookhaven) Y. Tan (Brookhaven) C. Theisen (Brookhaven) P. Thieberger (Brookhaven) J. Tuozzolo (Brookhaven) P. Wanderer (Brookhaven) S.M. White (Brookhaven) W. Zhang (Brookhaven)
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classification ⚛️ physics.acc-ph
keywords beam-beamhead-onrhiccommissioningcompensationelectronlensesstatus
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In polarized proton operation, the performance of the Relativistic Heavy Ion Collider (RHIC) is limited by the head-on beam-beam effect. To overcome this limitation, two electron lenses are under commissioning. We give an overview of head-on beam-beam compensation in general and in the specific design for RHIC, which is based on electron lenses. The status of installation and commissioning are presented along with plans for the future.

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